000833 Handbook of X-ray Photoelectron Spectroscopy AReference Book of Standard Spectra for Identification and Interpretation of XPS Data by , Jolm F. Moulder William F. Stickle Peter E.'Sobol Kennetlf D. Bomben Edited by Jill Chastain Published by Perkin-Elmer Corporation Physical Electronics Division 6509 Flying Cloud Drive Eden Prairie, MinnCSOla 55344 United Stales of America £55f 'lOr 0£ Preface X-ray Photoelectron Spectroscopy (XPS), also known as Electron Spectroscopy for Chem.ical Analysis (ESCA), is widely used LO investigate the chemical composition of surfaces. The usc of XPS in analytical laboratories throughout the world attests to the problem-solving capability of this technique. The ability to explore the first few atomic layers and assign chemical states to the detected atoms has shown XPS to be a powerful addition to any analytical laboratory. A great deal of information has been published on the principles of the technique and the diverse range of applications for which it is used. Volumes of XPS speclra exisl in the scientific literature, and international committees are establishing databases with reference spectra that will be made available to the geneml public. It is nOi the authors' intent to exclude these specua or to ignore these databases. Rather the intent is to assemble a concise volume of standard spectra to aid in the identification of XPS data. " The prevIous version of this handbook, published in 1918, ~ontained data acquired with a cylindrical mirror analyzer (CMA). Since that time, our XPS hardware has evolved., We currently use a spherical capacitance analyzer (SCA) in conjunction with improved detector technology and the choice of either a high-perfonnance AI x-ray monochromator or an achromatic Mg/AI dual anode x-ray source. This handbook is an update of the previous handbook with data acquired using our currenl SeA, which has a transmission function different from thai of a CMA, and both monochromatic and achromatic x-ray sources. In addition, data are included from several elements not contained in the previous handbook. This handbook is meant to selVe as a guide and reference work for the identification, quantification, calibration and interpretation of XPS spectra for users of Perkin-Elmer XPS systems equipped with SCAs and Omni FOCUS™ lenses. It is the authors' hope thai this handbook will playa useful role in the practice of XPS. Perkin-Elmer Corporation Physical Electronics Division Oc.ober 1992 Acknowledgments: The authors and editor would like to thank the following individuals for their contributions to the completion of this handbook: Dr. Charles Wagner, Surfex, for his contributions to the chemical states database; Dr. Albert Bevolo, Iowa Stale University, Ames Laboratory (USDOE), for providing the rare eaI1h samples; Linda Wirtjes, Physical Electronics Laboratory; Teresa Salvati; Dr. Douglas Stickle; and Dr. Michael Burrell, General Electric Company. The National Museum of Natural History - Smithsonian Institution provided the cinnabar sample (NMNH R630) used for the mercury dala. Wc also gratefully acknowledge the authors of the previous handbook. Table of Contents I. X-ray Photoelectron Spectroscopy A. Introduction 9 B. Principles of the Technique........................................................................................................................•.... 10 C. Preparing and Mounting Samples I. Removing Volatile Material 2. Removing Nonvolatile Organic Contaminants 3. Surface Etching 4. Abrasion 5.. Fracturing and Scraping 6. Grinding to Powder 7. Mounting Powders for Analysis 12 D. Experimental Procedure : I. Technique for Obtaining Spectra 2. Instrument Calibration 3. Programming Scans for an Unknown Sample a. Survey Scans b. Detail Scans 14 E. Data Interpretation I. The Nature of the Spectrum a. General Features b. Types of Lines 2. Line Identification 3. Chemical State Identification a. Determining Static Charge on Insulators b. Photoelectron Line Chemical Shifts and Separations c. Auger Line Chemical Shifts and Auger Parameter d. Chemical Information from Satellite Lines and Peak Shapes 16 4. Quantitative Analysis 5. Detennining Element Location a. Depth b. Surface Distribution c. Insulating Domains on a Conduclor F. Hnw to Use this Handbook 29 II. Standard XPS Spectra of the Elements III. Appendix A. Auger Parametm 198 B. Chemical States Tables 213 C. Chemical States Tables References , 243 D. Valence Band Spectra 250 E. Atomic Sensitivity Factors for X-ray Sources at 90' 252 F. Atomic Sensitivity Factors for X-ray Sources at 54.7' 253 G. Line Positions by Element for AI Ka X-rays 254 H. Line Positions by Element for Mg Ka X-rays 256 J. Line Positions in Numerical Order 258 K. Periodic Table 261 I. X-ray Photoelectron Spectroscopy Handbook of X-ray Photoelectron Spectroscopy A. Introduction A. Introduction X-ray Photoelectron Spectroscopy (XPS) was developed in the mid-l960s by Kai Siegbahn and his research group at the University of Uppsala, Sweden. The technique was first known by the acronym ESCA (Electron Spectroscopy for Chemical Analysis). The advent of commercial manufacturing of surface analysis equipment in the early 19705 enabled the placement of equipment in laboratories throughout the world. In 1981, Siegbahn was -awarded !.he Nobel Prize for Physics for his wotk with XPS. This handbook is meant to furnish the user with much of lhe information necessary to use XPS for diverse types of surface analysis. Information is provided on methods of sample preparation, data gathering, elemental identification, chemical stale identification, quantitative calculation and elemental distribution. Surface analysis by XPS involves irradiating a solid in vacuo with monoenergeLic soft x-rays and analyzing the emitted electrons by energy. The spectrum is obtained as a plot of the number of detected electrons per energy interval versus their kinetic energy. Each element has a unique SpecUliffi. The spectrum from a mixture of elements is approximately the sum of the peaks of the individual constituents. Because the ,mean free path of electrons in solids is very small, the , detected electrons originate from only the top few atOlruc layers, making XPS a unique surface~sensitive technique for chemical analysis. Quantitative data can be obtained from peak heights or peak areas, and identification of chemical states often can be made from exact measurement of peak positions and separations, as well as from certain spectral features. Included in this handbook are survey spectra, strong line spectra and x-ray excited Auger spectra for most of the elements and some of their complunds, in addition to plOIS and tables of energy shift data which aid in the identirlCation of chemical states. m Perkin-Elmer Corporation Physical Electronics Division "-' 9 Handbook of X-ray Phnloelectron Spectroscopy B. Principles of the Technique B. Principles of the Technique ' r . : : - - - - - - - - - - - - - - - - Fonli Levtl ~ Surface analysis by XPS is accomplished by irradiating a sample with monocnergetic soft x-rays and analyzing the energy of the detected electrons. Mg Ka (1253.6 eV) or Al K~ (1486.6 eV) x-rays are usually used. These photons have limited penctrating power in a solid on the order of 1-10 micrometers. Thcy interact with alOms in the surfacc region, causing electrons to be emitted by the photoelectric effect. The emitted electrons have measured kinetic energies givcn by: KE =hv - BE - Ii. • I==-~~ "'" >, ... <oolo=========~ ~;;_- 4Fm (I) where hv is the energy of the pholon, BE is the binding energy of the atomic orbital from which the electron originates, and f, is the spectrometer work function. The binding energy may be regarded as the energy difference between the initial and final states after the photoelectron has left the atom. Because there is a variety of possible final states of the ions from each type of atom, there is a corresppnding variety of kinetic energies of the emilie<! electrons. Moreover, there is a different probability or cross-section for each final state. Relative binding energies and ionization cross-sections for an atom are shown schematically in Figure 1. The Fenni level corresponds 10 zero binding energy (by definition), and the deplh beneaLh the Femli level in the figure indicates the relative energy of the ion remaining after electron emission, or the binding energy of the electron. The line lengths indicate the relative probabilities of the various ionization processes. The p, d and f levels become split upon ionization, leading to vacancies in the Plfl, Pm, dlfl, dsn , f.'i12 and (1/2. The spin-orbit splitting ratio is 1:2 for p levels, 2:3 for d levels and 3:4 for f levels. As an example, the spin-orbit splitting of the Si 2p is shown in Figure 2. .. • > , , • •, 1 " • 4d~ "m '00 100) r---''''' IlOO 1<00 Because each element has a unique set of binding energies, XPS can be used to identify and determine the concentration of the elements in the surface. Variations in the elemental binding energies (the chemical shifts) arise from differences in the chemical potential and polarizability of compounds. These 10 Figure I. Relati~e binding mergies lmd iO/Jization CroSNecliQlU for U. The binding energy is jlroporriolla/lo llle distance below tile li,le illl/icating tile Fenni level, and the ioniWlion cross-section is pro/JOrtionalto tile length of the line. if\. W Perkin-Elmer Corporation Physical Electronics Division B. Principles of the Technique Handbook of X-ray Photoelectron Spectroscopy 2p~ - - e - e - e - e - e - e - - L2,)or2p Si 2p e e'----- L,oc2s Phoroelectron " / - - - 0 - -••1 - - - - - Kor Is os ,0> BindiD& Energy (tV) Auger electron • Fi,Wft 2. High-tuolUliOll sptetrum If sillg/~·<:I'ptalSi slwwing 1M spin-orbil spUrling of the 2p lt~L /~ • chemical shifts can be used to identify the chemical state of the materials being analyzed. In addition to photoeleclfons emitted in the photoelectric process, Auger electrons may be emitted because of relaxation I of the excited ions remaining after photoemission. This Auger electron emission occurs roughly I(}"I. seconds after the photoelectric event. The competing emission of a fluorescent x.- ray photon is a minor process in this energy range. In the Auger process (Figure 3), an ouler electron falls into the inner orbital vacancy, and a second electron is simultaneously emitted, carry· iog off the excess energy. The Auger electron possesses kinetic energy equal to the difference between the energy of the initial ion and the doubly charged fmal ion, and is independent of the mode of the initial ionization. Thus, photoiol)ization normally leads to two emitted electrons - a photoelectron and an Auger electron. The sum of the kinetic energies of the electrons emilie<! cannot exceed the energy of the ionizing photons. Probabilities of electron interaction with matter far exceed those of the photons, so while the path length of the photons is of the order of micrometers, that of the electrons is of the order of tens of angstroms. Thus, while ionization occurs to a depth of a few micrometers, only those electrons that originate within tens of Perkin-Elmer Corporation Physical Electronics Division e~L2)OC2p " Llor2s e• e Kor Is Figure 3. The XPS emissiOll process (top) for 0 model atom. An incoming photon COUstS the ejection of the photoelectron. The relaxation process (bol· tom) for 0 model atom I't:su/ting in Ik emission of a Kf...uLzJ eleclron. The simullo~ous fWO-eleclron cou./ombic reomlllgemenl mulJs in a [mal Slate with two elte/TOII varoneia angstroms below the solid surface can leave the surface without energy loss. These electrons which leave the surface without energy loss produce the peaks in the spectra and are the most useful. The electrons that undergo inelastic loss processes before emerging form the background. Calculations of the inelastic mean free paths of electrons in various materials are shown in Figure 4. 11 Handbook orx·ray Photoe)ec)ron Spectroscopy C. Preparing and Mounting Samples The electrons leaving the sample are detected by an electron spectrometer according to their kinetic energy. The analyzer is usually operated as an energy window, referred to as the pass energy, accepting only those electrons having an energy within the range of Ihis window. To maintain a constant energy resolution, the pass energy is fixed. Incoming electrons are adjusted to the pass energy before entering the energy analyzer. Scanning for different energies is accomplished by applying a variable electrostatic field before the analyzer. This retardation vollage may be varied from zero up to and beyond the photon energy. Electrons are detected as discrete events, and the number of electrons for a given detection time and energy is stored and displayed. .,',---------------------, • " AI " figure 4. Calculated inelastic elec/ron mean free paths in various me/als from {he me/hod of S. Tanuma, C.J. Powell and D.R. Penn, Sr/rf. brrerjace Anal. 17,911 (l99ll C. Preparing and Mounting Samples In the majority of XPS applications, sample preparation and mounting are not critical. Typically, the sample is mechanically attached to the specimen mount, and analysis is begun wiltJ the sample in the aNeceived condition. Additional sample preparation is discouraged in many cases because any preparation might modify the surface composition. For those samples where special preparation or mounting cannot be avoided, the following techniques are recommended. 1. Removing Volatile Material Ordinarily, volatile material is removed from the sample before analysis. In exceptional cases, when Ihe volatile layer is of interest, lhe sample may be cooled for analysis. The cooling must be to a sufficiently low temperatufC to guarantee that the volatile element is not warmed to evaporation by any heat load thaI the analysis conditions may impan. Removal of unwanted volatile materials is usually accomplished by long-term pumping in a separate vacuum system or by washing with a suitable solvent. Use freshly distilled solvent to avoid contamination by high boiling point impurities within the solvent. Choice of the solvent can be critical. Hexane or other light hydrocarbon solvents are probably least likely to alter the surface, providing the solvent properties are satisfactory. Samples may also be washed efficiently in a Soxhleu extractor using a suitable solvent. 2. Removing Nonvolatile Organic Contaminants When the nature of an organic contaminant is not of interest or when a contaminant obscures underlying material that is of interest, the contaminant may be removed with appropriate organic solvents. As with volatile materials, the choice of solvent can be critical. m 1? Perkin-Elmer Corporation \ j ! Ph.ysical Electronics Division Handbook of X-ray Photoelectron Spectroscopy C. Preparing and Mounting Samples 3. Surface Etching 6. Grinding to Powder Ion sputter-etching or other erosion techniques, such as the use of an oxygen plasma on organic materials (see Section E.5.a.(J), p. 27), may be used to remove surface contaminants. This technique is particularly useful when removing adventitious hydrocarbons from the sample or when the native oxides, formed by exposure to the atmosphere, are not of interest. If spectra charactcristic of bulk composition are desired, samples may be ground to a powder in a mortar. Protection of the fresh surfaces from the atmosphere is required. When grinding samples, localized high temperatures can be produced, so grinding should be done slowly to minimize heat-induced chemical changes at the newly created surfaces. The mortar should be well cleaned before reuse. Argon ion etching is commonly used to obtain information on composition as a function of the exposure time to ion etching. Calibration of the spuller rates can be used to convert spuner timc to infonnation on depth into the specimen. Because sputtering may cause changes in the surface chemistry, identification of the changes in chemical stales with depth may not reflect the true composition. 4. Abrasion Abrasion of a surface can be done without signiflCaI1t contamination by using a laboratory wipe, a cork, a file or a knife blade. This may cause local heating, and reaction with environmental gases may occur (e.g., oxidation in air and formation of nitrides in nitrogen). To prevent oxidation of more active materials, perform abrasion in an inell atmosphere such as a glove box. The abraded material should then be transferred to the ultra-high vacuum (UHV) chamber in a sealed vessel to preserve the clean surface. 5. Fracturing and Scraping With proper equipmen~ many materials can be fractured or scraped within the test chamber under UHV conditions. While this obviates contamination by reaction with atmospheric gases, allention must be given to unexpected results which might occur. Fracturing might occur along the grain boundaries which may not be representalive of the bulk material. Scraping can cover hard material with soft material whcn the sample is lllultiphase. Perkin-Elmer Corporation Physical Electronics Division 7. Mounting Powders for Analysis There are a number of methods which can be used to mount powders for analysis. Perhaps the most widely used method is dusting the powder onto a polymer-based adhesive tape with a camel-hair brush. The powder mUSl be dusled across the surface carefully and lightly, with no wiping strokes. Some researchers shun organic tape " for UHV work, but others have successfully used certain types of tape in the 10. 10 Torr range. Alternative methods for mounting powders include pressing (he powder into indium or other soft foils, supporting the powder on a metallic mesh, pressing the powder into pellets or simply depositing (he powder by gravity. With the foil method, the powder is pressed between two pieces of pure foil. The pieces arc then separated, and one of them is mounted for analysis. Success with this techntque has been varied. Sometimes bare foil remains exposed and, if lhe sample is an insulator, pans of the powder can charge differently. Differential charging can also be a problem when a metallic mesh is used to suppon (he powder. If a press is used to form the powder into a pellet of workable dimensions, a press with hard and extremely clean working surfaces should be used. Gravity can effectively hold some materials in place, particularly if a shallo.w well or depression is cuI in the surface of tht sample mount. Allowing a liquid suspension of the powder to dry on the specimen holder is an effective way of producing a D. Experimental Procedure unifonJl lflyer. With the.~ methods, care must be taken in pump-down to ensure that gas evolution does not disturb Handbook or X-ray Photoelectron Spectroscopy the sample. A throttled roughing valve is especially effcctive. D. Experimental Procedure 1. Technique for Ohtaining Spectra All spectra in this handbook were obtained using a PHI Mooel 5600 MultiTcchnique system. A schematic diagram of the apparatus (Figure 5) illustrates the relationship of major components, including the electron energy analy:r.er, the x-ray source, and the ion gun used ror sputter-etching_ The Model !(}.J60 Electron Energy Analyzer incorporated into the 5600 is an SeA, and the input lens to the analyzer is an Omni Focus JII lens. The excitation sources used were a Model 10.550 x-ray .source with a Model 10-410 monochromator and a Model 04-548 dual-anode source which was used with 'a magnesium anode. All of the spectra in the handbook were taken with the x·ray source operating at 400 W(15 kV - 27 rnA). The specimens were analyzed at an electron take·off angle of 70', measured with respect to the surface plane. The monochromatic x-ray source is located perpendicular to the analyzer axis, and the standard x-ray source is located at 54.7' relative to the analyzer axis. In the PHI Model 5600 MultiTechnique system, energy distribution, energy resolution and analysis area are all a function of the analyzer. For all of the spectra in this handbook, the spectrometer was operated in a standard mode. The Omni Focus III lens was used to scan the spectrum while Ihe SeA was operated at a constant pass energy. This resulted in constant resolution (.6.£) across lhe entire energy spectrum. The size of the analysis area was defined by the aperture selection of the Omni Focus III lens. Analyzer energy resolution (6EJE) was determined by the choice of pass energy and the seiected J4 aperture. AU of the spectra in this handbook were 00. tained using an 800 11m diameter analysis area. All of the spectra in lhis handbook were recorded and stored using the PHI ACCESSfM data system. The instrument was calibrated daily, and the calibration was checked several times each day during data acquisition. The analyzer work. function was determined assuming the binding eocrgy or the Au 4rm peak to be 84_0 eV. All survey spectra scans were taken at a pass energy of 58.7 eV. The narrow scans of strong lines were, in most cases, just wide enough to encompass the peak(s) of interest and were obtained with a pass energy of 23.5 eV. A lower pass energy may show more structure for some materials. The narrow spectra were necessary to accurately determine the energy, shape and spin-orbit split. ting of the strong lines. On insulating samples, a highresolution spectrum was taken of the adventitious hydrocarbon on the surface of the sample to use as a reference for charge correction. The generally accepted binding energy for adventiLious carbon is 284.8 eV. The samples analyzed to obtain the spectra in this handbook are standard materials of known composition. Metal foils and polycrystalline materials with large sur· face areas were mechanically fastened to the specimen mount. Powder samples were ground with a mortar and pestle to expose fresh surfaces and were dusted onto adhesive tape. Most elemental standards were sputteretched immediately prior to analysis to remove surfn contamination. Most compounds, however, were ground or cleaved, and lhe freshly exposed surface was analyzed m \lI Perkin-Elmer Corporation Physical Electronics Division , Handbook of X-ray Photoelectron Spectroscopy D. Experimental Procedure a pass energy of 23.5 eV or less (corresponding to the pass energy nonnally used for high resolution scans) should be used. There is general agreement 011 accurate values of Cu, Au and Ag standard line energies. The values in Table I are recommended for clean Au, Ag and Cu: Table 1. Referellce Billdillg Energies (eV) Cu 3p Au4fm Ag3d~ AIKa MgKa 75.14 8198 361.26 75.13 84.00 361.27 334.94 932.66 895.75 Cu L~lM 561.96 93167 Cu 2Pl'2 A, M,NN 1128.78 fran M. P. Seah Swf/fIlu/QaAnoJ. 14,488 (1989) Because tbe 2Pl'l and JPl'l photoelectron peak ,n''Eies of Cu are widely separated in energy, measurement of Figuft 5. A sclllrnOlic diagram of the PHI MOtkI 5600 Mul1l7lChniqul sysrem. without etching in order to avoid possible changes in surface chemistI)'. Ne, Xe and Kr were implanted in graphite and Ar ill silicon via ion implantation to unknown concentrations prior to analysis. 2. Instrument Calibralion To ensure the accuracy of the data presented in this handbook, the instrument used 10 obtain the data was calibrated regularly throughout the data-gathering process. The best way to check calibration, and the method used here, is to record suitable lines from a known, Conducting specimen. Typically, the Au 4f or Cu 2p and 3p lines are used. The lines should be recorded with a narrow sweep width in thc range of 5-10 cV, and Perkin-Elmer Corporation Physical Electronics Division these peak binding energies provides a quick and simple means of checking the accuracy of the binding energy scale. Utilizing all of the above standard energies establishes the linearity of the energy scale and its position, i.e., the location of the Fermi level. 3. Programming Scans for an Unknown Sample For a typical XPS investigation where the surface composition is unknown, a broad scan survey spectrum should be obtained flrst to identify the elements present. Once the elemental composition has been detennined, narrower detailed scans of selected peaks can be used for a more comprehensive picture of the chemical composition. This is the procedure that has been followed in compiling data for this handbook, even though specimen composition was known prior to analysis. a. Survey Scans. Most elements have major photoelectron peaks below 1100 eV, and a scan range from 1100-0 eV binding energy is usually sufficient to 15 E. Data Interpretation identify all detectable elements. The spectra in this handbook were recorded with a scan range of 1400-0 eV (AI excit3tton) or 1200.0 eV (Mg excitation) binding energy. In an unknown sample, if specific elements are suspected at low concentrations, their standard s~ctra should be consulted before programming the survey scan. If the strongest line occurs above 1100 eV binding energy, the scan range can be morlificd accordingly. An analy-ar pass energy of 187 eV, in conjunction with the appropriate apenure, is recommended for survey scans with the PHI Model 5600 MultiTechnique system. These settings result in adequate resolution for elemental identification and produce very high signal intensities, minimizing data acquisition time ,md maximizing elemental delectability. b. Detail Scans. For purposes of chemical state iden: litication, for quantitative analysis of minor components and for peak deconvolution or other mathematical manipulations of the data, detail scans must be obtainetl for precise peak location and for accurate registration of line shapes. There arc some logical rules for this programmmg. Handbook of X·ray Photoelectron Spectroscopy terest, yet with small enough step sizes 10 permit determination of the exact peak position. Sufficient scanning must be done within the time limits of the analysis in order to obtain good counting statistics. (2) Peaks from any species thought to be radiation-sensitive or transient should be run first. Otherwise, any convenient order may be chosen. (3) No clear guidelines can be given on the maximum duration of data gathering on anyone sample. It should be recognized, however, that chemical states have vastly varying degrees of radiation sensitivity and that for anyone set of irradiation conditions, there exists for many samples a condition beyond which it is impraclical to attempt gathering data. (I) Scans should be wide enough to encompass (4) With the PHI Model 5600 MultiTechnique system, an analyzer pass energy of 23 eV is nonnally used for mutine detail scans. Where higher energy resolution is needed, lower pass energies can be utilized. For example, the sputter-cleaned Si 2p on p. 56, taken at 23 eV pass energy, can be compared to the chemically etched Si 2p shown in Figure 2 the background on both sides of the region of in- (p. II) E. Data Interpretation 1. The Nature of the Spectrum a. Gencr<ll Features. The spectrum is displayed as a plot of the number of electrons versus electron binding energy in II fixed, small energy interval. The position on the kinetic energy scale equal to the photon excitation energy minus the spectrometer work function cor- responds 10 a binding energy of 0 eV with reference to the Fermi level (Equation I, p. 10). Therefore, a binding energy scale with 0 at that point arKI increasing to the left is customarily used. The speclra in this handbook are typical for the various elements. The well-defined peaks are due to electrons tf'\ 16 \lI Perkin-Elmer Corporation ))hysical Electronics Division E. Data Interpretation Handbook of X-ray Photoelectron Spectroscopy strumental contribution to the observed line width. Less intense photoelectron lines at higher binding energies are usually wider by 1-4 eV than the lines at lower binding energies. All of the photoelectron lines of insulating solids are of the order of 0.5 eV wider than photoelectron lines of conductors. The approximate hinding energies of all photoelectron lines detectable by AI or Mg radiation are cataloged in Appendices Gand H. which have not suffered an inelastic energy loss emerging from the sample. Electrons that have lost energy inCTCase the level of the background at binding energies higher than the peak energy. The background is continuous because the energy Joss processes are random and multiple. The background in the Mg Ka induced spectra is larger than the background in the monochromalcd Al Ka induced spectra because of excitation by Bremsstrahlung radiation of the nonmonochromated light. (2) Auger Lines. These are groups of lines in The "noise" in the spectrum is not instrumental in origin but is the consequence of the collection of single electrons as counts randomly spaced in time. The standard deviation for counts collected in any channel is equal to the square root of the counts SO thaI the percent standard deviation is lOO/(counts)1f2. The signal-to-noise ratio is then proportional to the square root of the counting time. The background level upon which the peak is superimposed is a characteristic of the specimen, the excitation source and lhe transmission characteristics of the instrument. b. Types of Lines. Several types of peaks are observed in XPS spectra. Some are fundamental to lhe technique' and are always observed. Others are dependent upon the exact physical and chemical nature of the sample. A third type is the result of instrumental effects. The following describes the various spectral features that are likely to be encountered: Photoelectron Lines. The most intense photoelectron lines are relatively symmetrical and are typically the narrowest lines observed in the spectra. Photoelectron lines of pure metals can, however, exhibit considerable asymmetry due 10 coupling with conduction electrons. Peak width is a convolution of the natural line width (the lifetime of lhe "hole" resulting from the photoionization process), the width of the x-ray line which created the photclectron line and the in- (1) Perkin-Elmer Corporation Physical Electronics Division tT\ \II .' rather complex patterns. There are four main Auger series observable in XPS. They arc the KLL, LMM, MNN and NOO series, identified by specifying the initial and final vacancies in the Auger transition. The KLL series, for example, includes those processes with an initial vacancy in the Kshell and final double vacancy in the Lshell. The symbol V (e.g., KVV) iodieates that the final vacancies are in valence levels. The KLL series has, theoretically, nine lines, and others have still more. Because Auger lines have kinetic energies which are indePendent of the ionizing radiation, they appear on a binding energy plot to be in different positions when ionizing photons of different energies (i.e., different x-ray sources) are used. Core-type Auger lincs (with final vacancies deeper than the valence levels) usually have at least one COOlponent of intensity similar to the most intense photoelectron line. Positions of the more prominent Auger components are cataloged along with the photoelectron peaks in Appendices G and H. (3) X-ray Satelliles. The x-ray emission spectrum from a nonmonochromatic source used for irradiation exhibits not only the characteristic x-ray but also some minor x-ray components at higher photon energies. For each photoelectron peak that results from the routinely used Mg and AI Kn x- 17 E. Data Interpretation Handbook of X-ray Photoelectron Spectroscopy ray photons, there is a family of minor peaks at lower binding energies, with intensity and spacing characteristic of the x-ray anode material. The pattern of such satellites for Mg and AI is shown in Table 2. A resultant spectrum using Mg x-rays is shown in Figure 6. 48.7 0.5 generation of x-rays within the sample itself. This last possibility is rare because the probability of x-ray emission is low relative to Auger electron emission. Nevertheless, such minor lines can be puuling. Table 3 indicates where such peaks are most likely to occur relative to the most intense photoelectron lines. Because such ghost lines rarely appear with nonmonochromatic x-ray sources and are not possible with monochromatic x-ray sources, .they should not be considered in line identification until all other possibilities are excluded. 69.7 0.6 Table 3. Displactlllent of X-ray GIIOSI lilies (eV) Tobie 2. X-m] SaUllile Ellergits (l.IId In/lnsiJies a" Mg displacemcnl, eV 0 relative height 100 AI displacement, eV relative height 0 100 "8.' 10.1'" 17.6" 20.6"' 8.0 • .1 0.6 OJ 9.8 6.4 11.8 J.2 20.1 0.4 23.4 OJ P Contaminating Radiation ." .' o(K.) c, (La) Mg (Ka) AI (K.I '" JOO FiglUt 6. Mg x-roy SQuf/it~s obs~1Vtd in tht C Is sp«1nun of graplUrt. (4) X-ray Ghost Lines. Occasionally, x-radiation from an element other than the x-ray source anode material impinges upon the sample, resulting in small peaks corresponding to the most intense spectral peaks but displaced by a characteristic energy interval. These lines may result from Mg impurity in the Al anode or vice versa, eu from the aoode base structure, oxidation of the anode, or generation of x-ray photons in the AI foil x-ray window. On occasion, such lines can originate via 18 (5) Shake-Up Lines. Not all photoelectric proces- 210 Binding Energy (eV) Anode Material Mg AI 728.7 961.7 323.9 556.9 233.0 ·233.0 ses are simple ones which lead to the fonnation of ions in the ground state. but there is a finite probability that the ion will be left in an excited state a few electron volts above the ground state. In this event, the kinetic energy of the emitted photoelectron is reduced, with the difference corresponding to the energy difference between the ground state and the excited state. This results in the foonation of a satellite peak: a few electron volts lower in kinetic energy (higher in binding energy) than the main peak. For example, the characteristic shake-up line for carbon in aromatic compounds, a shake-up process involving the ener· gy of the 1t -? 1t* transition, is shown in Figure 7. In some cases, most often with paramagnetic com· pounds, the intensity of the shake-up satellite may Perkin-Elmer Corporation (J) Physical Electronics Division Handbook of X-ray Photoete<lron Spectroscopy E. Data Interpretation C I' C" ) \ 280 Bindint Fllergy (eV) Figure 7. The 11 bond shflke.up salel/ile for C 1£ in polystyrene. The peak is aboul6.7 eV higher ihan/he main photopeak. approach that of the main line. More than one satellite of a principal photoelectron line can also be observed, as shown in Figure 8. The occunence of such lines is sometimes also apparent in Auger spectral contours (Figure 9). The displacements and relative intensities of shake.up satellites can sometimes be useful in identifying the chemical stale of an element, as discussed in Section EJ.d. ""0 . (p.24). (6) Mulliplet Splitting. Emission of an electron from a core level of an atom that itself has a spin (unpaired electrons in valence levels) can create a vacancy in two or more ways. The coupling of the new unpaired eleclTOn left after photoemission from an s-type orbital with orner unpaired electrons in the alOm can create an ion with several possible final state configurations and as many energies. This results in a photoelectron line which is split asymmelricaJly into several components similar to the one s~own in Figure 10. MUltiplet splitting also occurs in the ionization of p levels, but the result is more complex and subtle. In favorable cases, it results in an apparent slight Perkin-Elmer Corporation Physical Electronics Division 970 925 Binding Energy (eV) Figurr 8. &amp/a of shoU-up lintS (s) of Ihe c~r 2p obstmd in cop- fJlr c<mpOunds. increase in the spin doublet separation, evidenced in the separation of the 2pln and 2P3r2 lines in first-row transition metals. and in the generation of a less easily noticed asymmetry in the line shape of the components. Often such effects on the p double! are obscured by shake-up lines. Energy Loss Lines. With some materials, there is an enhanced probability for loss of a specific (7) cD 19 Handbook of X-ray Photoelectron Spectroscopy Ii:. Oa1.1 InteqJrelation Ni (C2HJOm' 4Hi) ""L_~_ _~--~--~--'~600 M, \ BlIldiD& Encrzy (eV) Figure 9. Examplts of tht tJJtclS of chemical stalts OR Augtr lint shopts in nickel compounds. : amount of energy due 10 interaction between the photoelectron and other electrons in the surface region of the sample (Figure 11), The energy loh phenomenon produces a distinct and rather sharp hump 20-25 eV above the binding energy of the parent line. Under certain conditions of spectral display, energy loss lines can cause confusion. Such phenomena in insulators are rarely sharper than that shown in Figure II and arc usually much more muted. They are different in each solid medium. With metals, the effect is often much more dramatic, as indicated by the loss lines for aluminum shown in Figure 12. Energy loss to the conduction electrons occurs in well-defined quanta characteristic of each metal. These plasmons arise from group oscillations of the conduction electrons. The photoelectron line, or the Auger line, is successively mirrored at intervals of higher binding energy with reduced intensity. The energy '''' 80 Binding EncItY (eV) Figurr: 10. Multiplet splitting of t~ Mn Js. interval between the primary peak and the loss peak is called the plasmon energy_ The so-called bulk plasmons are the more prominent of these lines. Asecond series, the surface plasmons, exists at energy intervals detennined approximately by dividing the bulk plasmon energy by the square root of two. The effect is not easily observed in nonconductors, nor is it prominent in all conductors. Plasmon lines are especially prominent in the Groups 13 and lIa metal spectra in Ihis handbook. (8) Valence lines atuf Bands. Lines of low inten- sity occur in the low binding energy region of the m W Perkin-Elmer Corporation I)hysical Electronics Division E. Dala Interpretation Handbook or X-ray Photoelectron Spectroscopy tween insulators and conductors are especially notcd by the absence or presence of electrons from conduction bands at thc Fermi level. Valcnce bands may also be used to distinguish between materials where the core level XPS photoelectron lines arc quite similar in shape and position. Appendix 0 contains valence band spectra of several materials. 0" 2, Line Identification 520 "" Binding Energy (eV) Figuft II. Enff8Y loss tRW:/opt from Iht 0 Is line in AllYl (sopphire). In general, interpretation of the XPS spectrum is most readily accomplished first by identifying the lines that are almost always present (specifically those of C and 0), then by identifying major lines and associated weaker lines, and lastly by identifying the remaining weak lines. Most modem, commercially available 5peClrOmetcTS have peak identification algorithms within " their data reduction packages. Poor signal-to-noise of the data or database limitations may require manual identification of some peaks. The following step-by-step procedure simplifies the data interpretation task and minimizes data ambiguities. Step I, The Cis, 0 • NornW • • b """" '~ \'--'--- 190 11O Binding Energy (eV) FigUft 11 Sutface (s) and bulJ: (b) Jiasmotlli1ltS assockl/td wi/It the AI 2s at IIOnMI and gmting IQu-<Jff OIIglts. spectrum between the Fermi level and 10-20 eV binding energy_ These lines are produced by photoelectron emission from molecular orbitals and from solid state energy bands. Differences be- Perkin-Elmer Corporation Physical Electronics Division I~ C (KLL) and 0 (KLL) lines are usually prominent in any spectrum. Identify these lines first along with all derived x-ray satellites and energy loss envelopes. Step 2. Identify other intense lines (Appendix J) present in the spectrum, then label any related satellites and other less intense spectral lines associated with those elements. The energy positions of the less intense lines are noted in the line position table with the spectra. Keep in mind that some lines may be interfered with by more intense, overlapping Jines from other elements, The most serious interferences by the C and 0 lines, for example, are Ru 3d hy C Is, V 2p and Sb 3d by 0 Is, I (MNN) and Cr (LMM) by 0 (KLL), and Ru (MNN) by C (KLL). E. Data Interpretation Step 3. Identify any remaining minor Jines. In doing this, assume they are the most intense lines of an unknown clement. If not, they should already have been identified in the previous steps. Again, keep in mind possible line interferences. Small lines that seem unidentifiable can be ghost lines. Use Table J (p. 18) to check for the more intense parent photoeleclron lines. Step 4. Check the conclusions by noting the spin doublets for p, d and f lines. They should have the right separation (cf. spin orbit splitting for individual elemenls and Appendices G and H) and should be in the correct intensity ratio. The ratio for p lines should be about 1:2, d lines 2:3 and f lines 3:4. P jines, especially 4p lines, may be less than 1:2. Handbook of X-ray Photoelectron Spectroscopy electrons and tends to make the peaks appear at higher binding energies, whereas excessive charge compensation can makc thc peaks shift to lower binding energies. The following are four methods which are usually valid for charge correction on insulating samples: (/) Measurement of the position of the C Is line from adventitious hydrocarbon nearly always present on samples introduced from the laboratory environment or from the glove box. This line, on unspullered inen metals such as Au or Cu, appears at 284.8 eV, so any shift from this value can be taken as a measure of the stalic charge. At this time, it is not known whether a reproducible line position exists for C remaining on the surface after ion beam ctching. 3. Chemical State Identification The identification of chemical Slates primarily depends: on the accurate deternlination of line energies. To determine line energies accuralely, the voltage scale of Ihe instrumenl must be precisely calibrated (cf. Section 0.2., p. 15), a line with a narrow sweep range m~st be recorded wilh good statistics (of lhe order of several thousand counts-per-channel above background), and accurate correction must be made for SIalic charge if the sample is an insulator. (2) The use of an internal standard, such as a hydrocarbon moiety of a polymer sample. For the study of supported catalysts or similar materials, one can adopt a suitable value for a constituent of the support and use that to interrelate binding energies of different samples. One must be certain that treatments of the various samples are not so different that the inherent binding energies of support constituents are changed. a. Determining Static Charge on Insulators. During analysis, insulating samples tend to acquire a steadystate charge of as much as several volts. This steadystate charge is a balance between electron loss from the surface by emission and electron gain by conduction or by acquisition of slow or thermal eleclrons from the vacuum. The steady-slale charge, usually positive, can be minimized with an adjacent neutralizer or flood gun. It is often advantageous to do this to reduce differential charging and sharpen the spectral lines. (3) The use of a normally insulating sample so thin that it effectively does not insulate. This can be assumed if the spectrum of the underlying conductor appears in good intensity and if line positions are flOt affected by changes in electron flux from the charge neutralizer. A serious problem is exactly determining the extent of charging. Any positive charging retards outgoing (4) For the study of insulating polymer films, binding energies of the C functional groups may also be determined by applying a small amount of poly(dimethyl siloxane) solution (10.6 M) 10 the sample surface and chargc reference to the Si 2p of the silicone (at about 102.1 eV). iI'\ W l)erkin·Elmer Corporati( Physical Electronics Divisil Handbook of X-ray Pholoeleclron Speclroscopy SOffie precautions should be kept in mind. If the sample is heterogeneous on even a micrometer scale, particles of different materials can be charged to different extents, and interpretation of the spectrum is complicated accordingly. One cannol physically mix a conducting standard like Au or graphite of micron dimensions with a powder and validly use the Au or graphite line in order to COfrect for static charge. Differential charging can be minimized to a great extent by using a flood source of lowenergy electrons. b. Photoelectron Line Chemical Shifts and Separations. An imponant advantage of XPS is its ability to obtain information on chemical stales from the variations in binding energies, or chemical shifts, of the photoelectron lines. While many auempts have been made to calculate chemical shifts and absolute binding energies, the factors involved (especially in the solid Slate) are imperfectly understood, and one must rely on experimental data from standard materials. The tables accompanying the spectra in this handbook record considerable data from the literature as well as data obtained specifically for this handbook. All literature data have been carefully evaluated to the instrumental calibration and static charge reference values given above and are, therefore, directly comparable. Because occasional line interferences do occur, it is sometimes necessary to use a line other than the most intense one in the spectrum. Chemical shifts of a minor line are within 0.2 eV of the chemical shift of the primary line. However, exceptional separations can occur in paramagnetic materials because of multiplet splitting. Separations of photoelectron lines can be determined approximately from the line position tables in Appendices G and H. c. Auger Line Chemical Shifts and the Auger Parameter. Core-type Auger lines (transitions ending with double vacancies below the valence levels) usually have at least one component that is narrow and intense, Perkin-Elmer Corporation Physical Electronics Division E. Data Interpretation often nearly as intense as the strongest photoelectron line (cr. spec", for F, Na, As, In, Te and Ph). There are four core Auger groups that can be generated by Mg or Al ,-mys: the KLL (Na, Mg); the LMM (Cu, Zo, Ga, Ge, As, Se); the MNN (Ag, Cd, 10, So, Sb, Te, I, Xc, Cs, Ba); and NOO (Th, U).. The MNN lines in the rare earlhs, while accessible, are very broad because of multiplet splitting and shake-up phenomena with most of the compounds. Valence-type Auger lines (final states with vacancies in valence levels) - such as those for 0 and F (KLL); Mo, Fe, Co and Ni (LMM); and Rn, Rh aod Pd (MNN) - can be intense and are, therefore, also useful. Chemical shifts occur with Auger lines as well as with photoelectron lines. The chemical shifts are different from those of the photoelectron lines, but they are often more pronounced. This can be very useful for identifying chemical states, especially in combination : with photoelectron chemical shift data. If data for the various chemical Slates of an element are plotted with the binding energy of the photoelectron line on the abscissa and the kinetic energy of the Auger line on the ordinate, a two-dimensional chemical slate plot can be obtained. Such plotS are in Appendix A for F, Na, AI, Si, 5, Cu, ?n, As, Se, Ag, Cd, In, So and Te. With chemical states displayed in two dimensions, the Auger parameter method becomes more powerful as a tool for identifying the chemical components than using photoelectron chemical shifts alone. In the (annat adopted for this handbook, the kinetic energy of the Auger line is plotted against the binding energy of the photoelectron line, with the latter plotted in the ·x direction (kinetic energy is still, implicitly, +x). The kinetic energy of the Auger electron, referred \0 the Fermi level, is easily calculated by subtracting from the photon energy the position of the Auger line on the binding energy scale. With this arrangement, each diagonal line represents all values of equal sums of Auger kinetic energy and 21 E. Data InterpreL'ltioll Handbook of X-ray Photoelectron Spectroscopy photoelectron binding energy. The Auger parameter, a, is defined as, or as the difference in binding energy between the photoelectron and Auger lines. This difference can be accurately determined because static charge corrections cancel. With all kinetic and binding energies referenced to the Fermi level, and recalling that KE =hv - BE (3) MuJtip/~1 spliJlillg and slulU-up Jillts art generally aptettd ill/he pammaglittle SIales btlow: Atomic No. 22 23 2' 25 26 27 28 29 .2 then... KE A + BEp :::hv +a 1i1blc 4. Gcneral Guilfe 10 I'aramugllelic Species (4) or the sum of the kinetic energy of the Auger line and the binding energy of lhe photoelectric line equals the .Auger parameter plus the photon energy. A plot showing Auger kinetic energy versus photoelectron binding energy then becomes independent of the photon energy. I In general, polari7.able materials, especially conductive material~, have a high Auger parameter, while insulating compounds have a lower Auger parameter. d. Chemical information from Satellite Lines and Peak Shapes (I) Shakt-up Unts. These satellite lines have in· tensities and separations from the parent photoelectron line that are unique to each chemical state (Figure 8, p. 19). Some Auger lines also exhibit radical changes with chemical stale that reflect these processes (Figure 9, p. 20). With transition clements and fare earths, the absence of shake-up satellites is usually characteristic of the elemental or diamagnetic slates. Prominent shakeup patterns typically occur with paramagnetic stales. Table 4 is a guide 10 some expected paramagnetic states. 44 .7 58 59,70 7. 75 76 77 92 Pammagrctic States Diamagnetic States 11(/1)11(111) 1i{lV) V(/I, V(III), V(IV) V(V) C«II), C«III), C«IV), C«V) C«VI) Mn(l!). Mn(ltI). Mn(IV), Mn(V) Mn(VII) F,(II), F.III1 "'Fo(CNI6. Fo(CO)dlo Co(/I, Co(lII) Coli, Co(No,hNHllJ, KJCo(CNI6. Co(NHl)oO: Ni(lI) K1Ni(CN)4, square planar complexes C,(lI) CuO) Mo(IV), Mo(V) M"VI, MoS" "'Mo(t} R»(III), R,(lV), R»(V) R.(II) Ag(lI) Ag(1I Co(III) Co(IV) Pr. Nd, Sm. Eu, Gd, Tb, Dy. Ho, Er. Tm, Yb compoollds W(lV), W(V) W(VI), W02. WCI4, WC, "'W(CN), Ro(Il), R.III), Re(IV), Re(VII). Re03 R«V), Ro(VI) Os(III), Os(IV), Os(V) Os(lIl, Os(VI), 0s(V1II) )«IVI 1«11I) . U(III), U(IV) U(VI) (2) Multiplet Splitting. On occasion, the multiplet splitling phenomenon can also be helpful in identifying chemical states. The 3s lines in the first series of transition metals, for example, exhibit separations characteristic of each paramagnetic chemical state. The 3s line, however, is weak and therefore is not oflen useful analytically. The 2p doublet separation is also affected by multiplet splitting, and the lines are more intense. The effect becomes very evident with Co compounds where the separation varies up 10 I eV. When first·row transition metal compounds are under study, it is m l4 Perkin·Elmer COfl>oration ' " Physical Electronics Division E. Data Interpretation Handbook of X-ray Pbotoelectron Spectroscopy useful 10 accurately record these linc separations and make comparisons with model compounds. (3) Auger line Shape. Valence-type Auger transitions (onn final-state ions with vacancies in molecular orbitals. The distribution of the group of lines is strongly affected, therefore, by the nature of the molecular orbitals in the different chemical states. Although little has yet been tabulated on this subject, the spectroscopist should bear in mind the possible utility of Auger line shapes. 4. Quantitative Analysis -For many XPS investigations, it is important LO determine the relative concentrations of the various constituents. Methods have been developed for quantifying the XPS measurement utilizing peak area and peak height sensitivity factors. The method which utilizes peak area sensitivity factors typically is the more accurate and is discussed below. This approach is satisfactory for quantitative work. For transition metal spectra with prominent shake·up lines, it i.s best to include the entire 2p region when measuring peak area. For a sample that is homogeneous in the analysis volume, the number of photoelectrons per second in a specific spectra peak is given by: are detected, and T is the detection efficiency for electrons emitted from the sample. From Equation 5: n ~ UfoGyl.AT (6) The denominillor in Equation 6 can be defined as the atomic sensitivity factor, S. If we conr;idcr a strong line from each of two elements, then: nJ (7) n, This expression may be used for all homogeneous samples if the ratio SdS2 is matrix-independent for all materials. It is certainly true that such quantities as (J and A. vary somewhat from material to material (especially A), but the ratio of each of the two quantities 01/02 and llA.2 remains nearly constant. Thus, for any " spectrometer, it is possible to develop a set of relative values of S for all of the elements. Multiple sets of values may be necessary for instruments with multiple x-ray sources at different angles relative to the analyzer. A general expression for determining the atom fraction of any constituent in a sample, C1 , can be written as an extension of Equation 7: ~ t ~ nfoGyl.AT (5) where n is the number of atoms of the element per cm3 of the sample, f is the x-ray flux in photons/cm2-sec, 0" is the photoelectric cross-section for the atomic orbital of interest in cm2, e is an angular efficiency factor for the instrumental arrangement based on the angle between the photon path and detected electron, y js the efficiency in the photoelectric process for formation of photoelectrons of the normal photoelectron energy, A. is the mean free path of the photoelectrons in the sample, A is the area of the sample from which photoelectrons Perkin-Elmer Corporation I~hysical Electronics Division (8) Values of S based on peak area measurements are indicated in Appendices E and F. The values of S in the appendices are based on empirical data (CD. Wagner et al. Surf Inierface Anal. 3, 211 (1981)) which have been corrected for the transmission function of the spectrometer. The values in the appendix are only valid for and should only be applied when the electron energy analyzer used has the transmission characteristics of the SCA supplied by Perkin-Elmer. An example of the application of Equation 8 to analysis of a sample of E. D3ta Interpretation Handbook of X-ray Photoelectron Spectroscopy b. Transition metals, especially of the first series, have widely varying and low values of y, whereas y for the other elements is rather unifonn at about 0.8 eV. Thus, a value of S detennined on olle chemical state for a transition metal may not be valid for another chemical state. This effect can be minimized by including shake-up peaks in the area measurement. F Is Atomic Concentration Theoretical C 33 F Experimental 33 67 67 c. When peak imerferences occur, alternative lines must sometimes'be used. The ratios of spin doublets (except 4p) are rather uniform, and the weaker of the pair can often be substituted. The spectra of the elements should be consulted, but caution must be exercised because the spectra of the elements themselves can be different from the spectra of their compounds. F Cis .' F • 1100 o d. Occasionally, an x-ray satellite from an intense photoelectron line interferes with measurement of a weak component. A mathematical approach can then be used to subtract the x-ray satellite before the measurement. Biooing f.Jlergy (tV) Figuft /3. Quamiwlive analysis ofpoI)(lelrajluorotlhylene). known composition, poly(telrafluoroohylene), is shown in Figure 13. The use of atomic senSItiVity factors in the manner described will nonnally furnish semiquantitative results (within 10-20%), except in the following situations: The technique cannot be applied rigorously to heterogeneous samples. It can be useful with heterogeneous samples in measuring the relative number of atoms detected, but one must be conscious that the microscopic character of the heterogeneous system influences the quantitative results. Moreover, an overlying contamination layer has the effect of diminishing the in~ tensity of high binding energy peaks more than that of low binding energy peaks. 3. For quantitative work, check the spectrometer operation frequenlly to ensure that analyzer response is constant and optimum. Auseful test is the recording of the three widely spaced spectral lines from Cu. Measurement of the peak height in counts-per-second should be made on 2o-voh-wide scans of the 2p312. LMM Auger and 3p lines. Maintenance of such records makes it easy to notice if an instrument change occurs that would affect quantitative analysis. 5. Determining Element Location Depth. There are four methods of Obtaining information on the depth of an element in the sample. The first two methods described below utilize the characteristics of the spectrum itself but provide limited infonnation. The third provides more detailed information but is attcnded by cenain problems. The founh utilizes measurements at two or more electron escape angles. 3. Perkin-li:lmer Corporatio Physical Electronics Oivisio E. Data Interpretation HandbOOk of X-ray Photoelectron Spectroscopy (I) The presence or absence of an energy loss peak (3) Depth profiling can be accomplished using controlled erosion of the surface by ion sputtering. Table 5 lists some data on sputter rates as a general guide. One can use this technique on organic materials, but few data are available for calibration. Chemical states are often changed by the sputter technique, but useful infonnation on elemental distribution can slill be obtained. or envelope indicates whether the emitting atoms are in the bulk or at the surface. Because electrons from sUlface atoms do not traverse the bulk, peaks from the surface atoms are symmetrical above level baselines on both sides, and the energy loss peak is absent. For a homogeneous sample, peaks from all elements will have similar inelastic loss structures. (2) Elements whose spectra exhibit photoelectron lines widely spaced in kinetic energy can be approximately located by noting the intensity ratio of the lines. In the energy range above approximately 100 eV, electrons moving through a solid with lower kinetic energy are attenuated more strongly than those with higher kinetic energy. Thus, for a surface species, the low kinetic energy component will be relatively stronger than the high kinetic energy component, compared to that observed in the pure material. The data for homogeneous bulk solids can be compared with intensity ratios observed on unknowns to determine qualitatively the distribution of the elemen! in the sample. Suitable elemen~ include Na and Mg (Is and 15); In, Ga, Ge and As (2pll1 and 3d); and Cd, In, Sn, Sb, Te, I, Cs and Ba (3p," and 4d or 3d512 and 4d). When the element is in a bulk homogeneous layer beneath a thin contaminating layer, the characteristic intensity ratio is modified in the opposite direction. Thus, for a pair of lines from subsurface species, the low kinetic energy line will be attenuated more than the high kinetic energy line, distorting the characteristic intensity ratio. By 0bserving such intensity ratios and comparing them with the pure bulk elements, it is possible to deduce whether the observed lines are from predominantly sUlface-, subsurface- or homogeneously distributed material. Table 5. Rtfative SpIltler Rala aI4,tV. Ia:get Si02 1.00 O!Xl 0.85 ~ 120 C, 1.<0 0.95 4.10 Tat.05 S; : Spu!lCT Rale Al A' Another useful method of controlled erosion, especially of organic materials, is reaction with oxygen atoms from a plasma. This tcchnique may also change the chemical states in the affected surface. Further, because the elements differ in their rates of reaction with oxygen atoms, the rate of removal of surface materials will be sample dependent. (4) In XPS studies, the sample-mounting angle is nOl usually critical, though it does have some effeci on the spectra. Very shallow electron take-off angles accentuate lhe spectrum of any component scgregated on the surface, whereas a sample mounted al an angle normal to the analyzer axis minimizes the contribulion from such a component. This effect can be used to esJ.imate lhe depth of layers on or in the surface. This effect is not limited to flat surfaces, because angular dependence is even observed with powders, though the effects are muted. The spectrometer used to oblain the spectra presented in this handbook in- m Perkin-Elmer Corporation Physical Electronics Division ' " 27 E. Data Interpretation Handbook of X·ray Photoelectron SpectrosCOI»)' tegrates the signal over only a narrow range of take-off angles. It is possible to cbange the angle between the plane of tbe sample surface and the angle of entrance to the analyzer. AI 90" with respect to the surface plane, the signal from the bulk is maximized relalive to that from the surface layer. At small angles, the signal from me surface becomes greatly enhanced, relative to that from me bulk. The location of an element can thus be deduced by noting how me magnitude of its spectral peaks changes with sample orientation in relation to those from other elements. The analysis depth may be estimated by d =Asine, where d is the analysis depth of the overlayer, Ais the inelastic mean free path, and e is the take-off angle of the analyzed electrons. Perkin-Elmer SCAs permit angle-dependent studies by simply varying the angle of the sample surface with respect to the input lens of the analyzer. The magnification of the lens detennines the half-angle acceptance of the analyzer. An example of the information that can be gained through the use of this capability is shown in Figure 14. Data were obtained at normal (near 90') and grazing (near 15') take-off angles from a silicon sample with a thin silicon oxide overlayer. The observed intensity ratio of oxidized to elemental Si is much greater at the low take-off angle. b. Surface Distribution. Many current XPS systems have the capability (0 obtain data from areas as small as 30 IJI11 in diameter. This relatively high lateral resolution allows for the acquisition of XPS maps which show both elemental and chemical state information. Si 2p "'" Si Gnu,. ,.,., : \ /\ 110 96 BindiDg Energy (eV) "'igurt 14. All Uilmpf~ of /he ~nhanctd surfaee sensilivity achkvtd by va,)'ing /he elte/ron take·offangle. A thin oxidt on silicon is enhallctd at the low lakt-off(lllgit. c. Insulating Domains on a Conductor. The occurrence of steady-state charging of an insulator during analysis sometimes has useful consequences. Microscopic insulating domains on a conductor reach their own steady-state charge, while the conductor remains at spectrometer potential. Thus, an element in the same chemical state in both phases will exhibit two peaks. If a change is made in the supply of low-energy electrons which stabilize the charge (as from the neutralizer filament) or if a bias is applied to the conductor, the spectral peaks from the insulating phase will move relative to those from the conducting phase. For such heterogeneous systems, this can be an extremely useful technique. It makes it possible to determine whether the elements that contribute to the overall spectrum arc in the conducting phase, the insulating phase or both. m 28 /1 Perkin-Elmer Corporation \j!' Physical Electronics Dil'isioll F. How to Use this Handbook Handbook or X·ray Photoelectron Spectroscopy F. How to Use this Handbook gies by comparing the binding energy to the charts with the standard spectra and with the tabulated data in Appendix B. 1. Qualitative Analysis Elemental and chemical identification of sample constituents can be perlormed by combining the infonnation in the survey spectra with the binding energy tables of Appendices G, Hand J. (3) As suggested above, much about the chemical state can be learned frol11 the magnitude and posi· tion of shake-up lines as well as from the energy and shape of valence Auger lines. a. Identify all major photoelectron peaks by using the line position tables in Appendix J. b. Compare the elemental identifications with the elemental survey spectra to see that line positions and relative intensities are consistent. Also note the positions of the Auger electron peaks. Review Section E (pp. 16-28) to account for fine structures such as energy loss lines, shake-up peaks, satellite lines, etc., not identified in the handbook spectra or energy tables. Co d, Identify any remaining peaks assuming lhey are intense photoelectron or Auger lines using Appendices G or H. e. Chemical stale identification can be determined from high resolution spectra of the strongest photoelectron and sharpest Auger lines. (I) Correct binding energies for slatic charging of insulators. When applicable, charge reference the binding energy scale to the C Is phOioelectron peak at 284.8 eV. (2) Deteffiline the chemical state from the measured shifts in the photoelectron binding ener- Perkin-Elmer Corporation Physical Electronics Division " (4) For the elemell~ F, Na, AI, SI, S, Cu, Zn, As, Se, Ag, Cd, In, Sn and Te, the Auger parameter tables in Appendix Amay prove useful. The Auger line positions may be convened to kinetic energy by sublracting from the pboton energy (AI = 1486.6 'V, Mg = 1253.6 eV). Note the locatiou of the points for Auger kinetic energy and photoelectron binding energy on the respective elemental piaL. Proximity of the experimental points to those of recorded chemical slates should be considered probable identification. Note that experimental error is much greater along the Auger parameter grid than normal to the grid lines. 2, Quantification The atomic sensitivity factors presented in Appendices E and F are applicable to the Perkiu-Elmer Model 10-360 SCA and the Omni Focus III lens. A simp~fied expression to determine the atomic concentration of any element is given by Equation 8 (p. 25). However, the accuracy is limited by the assumptions made in Section E.4 (p.25). 29 II. Standard XPS Spectra of the Elements : Standard Spectra of the Elements This ste1iOll if I~ hnndbooi eM/aillS SUM)' spectra of 8/ elemellfs. high ~solufion spectra of the mo.ll ustful photot/Utfrlll lints, a d1alt of binding tntrgies for each of Ihe oostrvtd plrmotlettmn and major Auger electron peaks, alld a phol«ItclrfJn chemicoI Slalt binding tntrgy CNIf/ jor tacit oj Ille eJemtlJ/s. Used i'l combinatioll willi the appendices, Ihe survey spectra Oil! ill elemellIal idelllijicalion, while lire high-resolutiOil sl,eerra Gnd binding trltrgy daln aid in Ihe idelJ/ijicalioJJ ofchemical Slale5. Survey Spectra Tk survey data include all of the lines which are normally useful. For most elements, the survey data wele acquired with both a mmochromatic Al x-I3Y source and a nonmooochromatic Mg Hay source. WIlen survey sptCtlt for two compoonds are presented, the monochromatic SOIJrce is used for both. The photon soorce fa each survey is noted on the survey. TIle photoelectron and Auger lines for the element of interest are identified. lines which occur d~ to olber elements are only designated by the elemental symbol, and x-ray S3lClliles and energy loss lines are not noted. Fa many elemenlS, tile Auger peaks are presented in expanded form. lk ordinate is left undesignated, bm the general conlours and intensilY ratios of the sJX=ctra are lypical of measuremenlS made using a Perkin-Elmer ModellD-360 SeA with an Omni r"OCus lens. : High-Resolution Spectra The high-resolution SJX=ctra of the most useful photoelectron peaks are !X"tsented Unless otherwise nored, the high-resolution data were acquired using the same photon soorct as the survey on the sarrc page. The binding energy of the main line is Jl)te<! and when awrc¥iate, !he spin 0Tbi1 separation (&) is given. The lino from insulators were charge-corrected to adventitioos hydrocarbon 3t284.8 eV. The spectra of the inert gas atoms implanted in graphite or silicon deserve special mcntiolL The high-resolution data often show an asymmetric peak shape or a secord resolvable peak when a single sytlll'OOric peak is expwell. The intensity of the second, high binding energy peak is dcpeOOenl 00 the implantation energy and is diminished at lower eneTgies. The spcctI3 are of inert gas atoms implanted at 4 kV. Photoelectron and Auger Electron Line Position Tables 'J'b; photoclectron and Auger line position tables reflect the energies reduced species, the measured values may differ by a few electron valls. of the elemental peaks observed in this handbook. For oxidized or Chemical State Binding Energy Tables The binding energy tables hnve been constructed to renecl the general chnnges in binding energy with change in oxidation state or chemical environment. A more eXlensive listing wilh specific binding me'!)' values for more than 1500 compounds is presented in Appendix B. Perkin-Elmer Corporation Physical Electronics Division Abbreviations in the chemical slale database are as follows: acac = acetyl acetonate; metallocene metal (C)H1h; Bu butyl; Et ethyl; Me methyl; Ph phenyl; OAc acetate. = = = = = = Lithium Handbook or X·ray I)hotoelectron Spectroscopy Li Atomic Number 3 F Li in LiF Monochromated Al Ka. F : ·1 r'--1400 F , A F '; I 1000 1200 800 600 Binding Energy (eV) 400 200 o Line Positions (eV) Is =55.6 eV Is Pholoclccuoo Lines j 60 Binding Energy (eV) lQ m 'II Perkin-Ehner Corporation Physical Electronics Division HandbOOk of X-ray Photoelectron Spectroscopy Lithium Atomic Number Li 3 F Li in LiF MgKa '. F F F : A " . j , 1000 1200 800 F 1: I 600 Binding Energy (eV) Is Binding Energy (eV) Compound Ty~ 54 55 56 400 Is =55.6 eV 51 o 200 Is U LiBr UC1 uF LhO LOH UzCOJ t.;,ro. -- u.P,Q, ~ LiNbOJ 10 Perkin-Elmer Corporation Physical Electronics Division 60 Binding Energy (tV) ~ 50 Beryllium Handbook of X-ray Photoelectron Spectroscopy Be Atomic Number 4 Monochromatcd Al Ka. /~ 1391l 1410 " KVV 1370 Binding Energy (eV) Ac Ac / KVV Ac 1400 0 1200 I 1000 800 .11 0 I Fe , 600 ,j .,~ 400 200 " o Binding EnelgY (eV) Line Positions (eV) Is=111.8eV Is PbotoekctronLines I, 112 Auger Lim KVV 1384 1151 \ 125 '" (AI) (Mg) 105 Bindins F.nergy (cV) m \M Perkin-Elmer Corporation Physical Electronics Division J Handbook of X~ray Photoelectron Spectroscopy Beryllium Be Atomic Number 4 Is Mg KlX KVV 1175 N 1155 Binding Enelgy (eV) 1135 Ar F, 0 1200 1000 800 600 400 o 200 Binding Energy (eV) I, Binding Energy (eV) Compoundl'ype III 112 113 )[4 JJS 116 1,= 1I1.8eV 117 I, Ik BoO BeMo(1 BeRhtO. 1kF, NaBeFl Na2BeF4 \ '" Perkin~Elmer Corporation Physical Electronics Division 115 BiOOin& Energy (eV) lOS Boron Handbook of X-ray Photoelectron Spectroscopy B Atomic Number 5 Is Monochromated Al Ko. KLL \. N, 1J>J BilXlint &Iergy (eV) 1350 KLL : 120) N' c o 1400 1000 1200 800 600 Binding EneIg)' (eV) N, 400 200 o Line Positions (eV) Is =189.4 eV Is f\ Photoelectron Lines Is 189 Auger Lines KLL \ 200 190 Binding Energy (tV) 1310 (AI) Ion (Mg) 180 m 1ft \II Perkin-Elmer Corporation Ilhysical Electronics Division HandbOOk or X-ray Photoelectron Spectroscopy \ B Atomic Number 5 I, /,\ MgKa Boron KLL KLL No \. ~ 1Il0 Ill<! BiDding Energy (eV) No ~ ., ~ ., C JJ , No • 1200 1000 800 600 Binding Energy (eV) L 400 200 o Is Binding Energy (eV) ComlXlund Type , Ilorido 'N '>0, 186 188 I~ NaBF4 NaBH, H,ao, Na 2B..{h. IOH,o B1OH14 190 • • 192 19' 1% Is =189.4 eV Is (\ III • '" IOJ Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 39 Handbook of X-ray Phntoelectron Spectroscopy C Carbon Atomic Number 6 Is C as graphite Monochromalcd AI Ka ''''' / KVV 1200 BiDdiaS Energy (eV) " . KVV 1400 , 1000 1200 . 800 -4 600 400 200 o· Binding EneJgy (eV) Is =284.5 eV Line Positions (eV) Is Photoelectron Lines Is 285 Auger Lines KVV '95 122J (AI) 990 (Mg) '85 Binding Entrgy (eV) '" 40 'II' Perkin-Elmer Corporation Physical Electronics Division Handtwok of X-ray Photoelectron Spectroscopy Carbon C Atomic Number 6 Is C as graphite Mg Ka ~ KVV 1m 91<1 BiOOillg f.Dc:rgy (tV) KVV .r : "V , , 1200 1000 800 600 Binding Energy (eV) 400 200 o Is Binding Energy (eV) Compound Type Carbide 280 282 284 286 288 290 292 Is = 284.5 eV 294 Is eMboo C with N Cwith S Cwith 0 ,- K,.,,,,,,,,,,,,,,, """ """"'" """""" C with 0 C with F CHF a; a; 29l "5 215 Bildill& Eatrzy (tV) Perkin-Elmer Corporation Physical Electronics Division 41 Nitrogen Handbook of X-ra)' Photoelectron Spectroscopy N Atomic Number 7 Is N in BN KLL Monochromated Al Ka. \ 1120 Binding Encrv (eV) 1160 lOW' B : KLL B 0 , ~ 1400 1200 1000 800 600 Binding Energy (eV) "\ c 400 200 0 Line Positions (eV) Is =398.1 eV Is Pholoelectron Lines Is 398 Auger Lines KLL ) "0 \ 1107 874 (AI) (Mg) 400 Binding Enetgy (eV) m 42 W I Perkin-Elmer Corporntion Physical Electronics Division 1 HandbOOk of X-ray Photoelectroo Spectroscopy Nitrogen N Atomic Number Nin BN I' J\ MgKa 910 B 7 KLL • \ B90 BilldiDg Energy (tV) "" KLL B ftI f) . I J. C • 1200 I()()() 800 600 400 200 Binding Energy (eV) o Is Binding Energy (eV) CO~nd Type 396 398 400 402 404 406 408 Is =398.1 eV 410 NHl Nitride Is BN ~'"' Cy",,,,, Nitrites Ammooium Sail AZidt{N*NN*) Azide (NN*N) Nitrates /' Organic MatriJ: 410 Perkin·Elmer Corporation Physical Electronics Division m \lI 400 Binding Eqy (tV) 390 Oxygen Handbook of X-ray Photoelectron Spectroscopy 0 Atomic Number 8 o in Al203 (sapphire) I' Monochromaled AI Ka KlL ~ 990 Bindin& Energy (cV) 1030 \ KlL 9,. . ~ IZOO . Al .. , 14110 , Al " .-J " cI 2s I 8110 600 Binding Energy (eV) 1000 L- zoo 400 a o Line Positions (eV) Is =531.0 eV Is f\ Pb~oeIeclron Lines 531 2s 23 KLILI KL1L23 1Ol3 999 7M I' Auger Lines ) 545 535 \ m KLnL23 978 (AI) 745 (M81 S2S Binding Energy (tV) m 44 W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Oxygen Atomic Number 0 8 Is o in AI203 (sapphire) KLL Mg Ka ~ \ ,., KLL 120 Binding EncIIY (eV) fi AI Al ~, N , N , IIXKJ 1200 800 • 600 Bindiog Energy (eV) 400 C 2s "" 200 Is Bioding Energy (eV) Compoulld Type S28 529 530 53] Is 532 533 • o A 534 Metal Oxides "'0, S;o, HyIloX~ Phosphates Nitrates Sulfates c.mooates Odorates ) AI,o, Silicones Perkin.Elmer Corporation Physical Electronics Division '45 m Binding Emgy (eV) \ 525 Fluorine Hanlbook of X-ray Photoelectron Spectroscopy F Atomic Number 9 I, Fin LiF Monochromated AI Ka Kil. \ '45 '" "" Binding Energy (tV) KLL .. .1 . A '-. 1400 Is = 684.9 eV 1200 1000 ~r 800 600 Binding Energy (eV) 400 200 o Line Positions (eV) Is Photoelectron Lines I, 685 h 30 Auger Lines KLILn .58 \ 700 625 KLn L23 832 599 (AI) (Mg) 680 m Perkin-Elmer Corporation \j! Physical Electronics Division I Han dl.""k or X-ray Photoelectron Spectroscopy IJ\}\I Fluorine F Atomic Number 9 's Fin llF MgKa Kll " KLL 615 595 575 Binding EllCrgy (eV) : ~ . j , 1000 1200 800 600 Binding Energy (eV) Is Binding Enelgy (eV) C'_"IT,," 6IJ 684 615 686 617 Li" d 688 689 400 Is =684.9 eV o 200 Is KF UF N,F &F, MgJ; AIF)·3H1O NaBF4 NaN iF6 P{C"~F,) EJ.NHillF) Ph)PI3F) Perkin-Elmer Corporation Physical Electronics Division ,. Neon Handbook of X-ray Photoelectron SpectroscoPJ Ne Atomic Number 10 c Ne implanted in graphite Momx:hromated AI Ka KlL ~~j no Binding Energy (eV) "" Is .' . C KlL .--J\. v1 , ~C , 1400 1000 1200 800 600 Binding Energy (eV) 4110 Is Is =863.1 eV o 200 Line Positions (eV) Photoelectron Lines Is 2s 863 41 2p 14 KLILI KL]L2J KLnLn Auger Unes ns 492 \. 875 865 702 (ffJ (AI) 469 436 (Mg) 855 Binding Eottgy (eV) .. m Perkin-Elmer Corporation \j! Physical Electronics Division Han dl.n"k uvu or X-ray Photoelectron Spectroscopy Neon Ne Atomic Number 10 c Ne implanted in graphite KlL MgKa '\. ~N ><Xl 'll Bindillg Encq;y (eV) C .f1 Is KLL : -'\ , , 1200 800 1000 ac 600 Binding Energy (eV) 400 200 o Is Binding Energy (eV) Compound Type Ne in Ag Ne in Au Ne in Cu Ne in Fe Ne in gnphile 861 862 863 - - Is=86J.leV 864 Is / j '" Perkin.Elmer Corporation PhYSical Electronics Division .., Binding Enttty (eV) 49 Sodium Handbook of X-ray Photoelectron Spectroscopy Na Atomic Number 11 MonochromaLed AI Ka KU. Is ~ ,.. 53. Bindinz Etcrgr (e V) - ... KU. : 2s , 2, • 1400 1200 1000 .I 800 600 400 lA 200 o Binding EneIgy (eV) Line Positions (eV) Is Photoeleclron Lines Is 1012 2, 2s 64 31 AUger Lines KLIL23 '32 299 108' so 1075 Binding &le:IxY (eV) KLnLn 493 (AI) 260 (Mg) 1065 If' W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Sodium Atomic Number Na in NaCI Monochmmaled AI Ka Na II Is KIl. ./' --JV ,'" '- "" BilWilll Enqy.(eV) CI KIl. a a L/ ~ , ~L-J , '- , 1400 1200 1000 800 600 Binding Energy (eV) 400 1070 1071 2p 200 Is Binding Energy (eV) ComlXlund Type 2s l1 o Is 1072 Na in NaCI 1073 N. Is= 1072.1 cV N.I NoB, N.a No!' No,cQ, Na2S2OJ Na,sQ, ....p,o, NaHzP'Ch Mol Sieve tOO 11m Bindill& Energy (eV) Perkin·ELmer Corp<lration Physical Electronia Division \ tOO Magnesium Mg Atomic umber 12 Is Handbook of X-ray Photoelectron Spectroscopy Monochromated Al Ka KLL KU J'~ A 340 Binding Energy (eV) 390 ~ , J 290 , 1400 1200 I(XX) 2s 2, ~ 800 600 400 .>! .I o 200 Binding Energy (eV) Line Positions (eV) 2p=49.8eV 2p Photoelectron Lines Is 1303 2s 89 2, 50 Auger Lines KLnL2l 301 (AQ \ 68 60 50 Binding Energy (eV) (Mg) 40 m Perkin-Elmer Corporation ' " Physical Eledronics Division l..n"k of X-ray Photoelectron Spectroscopy »an d~ Magnesium Mg Atomic Number 12 Mg Ka KLL "'-on from 2p KLL 2p o " 1000 1200 800 600 Binding Energy (eY) 2p Binding Energy (eY) Compound Type 48 Mg Mg,C, M&JBh MgF, Mg(OHn MgAhO. 49 50 51 zoo 400 2p =49.8 eY 2p • .... -- \ so Binding Enero' (tV) Perkin·Elmer Corporation Physical Electronics Division o .. 53 Handbook of X-ray Photoelectron Spectroscopy Aluminum AI Atomic Number 13 " Monochromaled AI Kn 2p At : At I , • )~ • 1400 1200 1000 800 600 Binding EneJgy (eV) 400 o Line Positions (eV) 2p 2p = 72.9 eV 200 Photoelectron Unes " 118 2p 73 Auger lines LnMlMn 1419 (AI) 1186 8l 71 (M&> 65 Binding EncliY (tV) m 54 W Perkin-Elmer Corporation Physical Electronics Division HandbOOk 01' X-ray Photoelectron Spectroscopy Aluminum AI Atomic Number 13 MgKa 2s .1 ) _~ .. 2p i\J\ 1200 1000 800 600 Binding Energy (eV) 400 200 o 2p Binding Energy (eV) COmpound Type AI AlAs AIGaAs "Alii, Halides 72 73 74 75 16 AI in A1J:0) (sap~rt) Mooochromated AI Ka 11 •• All; 2p =74.4 eV • Oxides AlA Apphrro AIA~ph. Ali>J, gamma AIDOH, boehmite ) 85 75 Binding Energy (eV) m Perkin·Elmer Corporation Physical Electronics Division \jl 65 Silicon Si Atomic Number 14 Handbook or X·ray Pholoelectron Spectroscopy 2s 2p MOllochromated AI Ka , . " LMM .___ 1' -Al) ¥~I : , d t400 1000 1200 800 600 Binding EnelEY (eV) 400 200 o Line Positions (eV) 2p : 99.3 eV 2p Photoelectron Lines 2s 2p 151 99 Auger Lines L2JM23M23 1394 1161 110 56 (AI) (Mg) 100 Binding Energy (tV) Perkin-Elmer Corporation (J) Physical Electronics Division Handbook nr X·",y Photoelettron Spetlros",py Silicon Si Atomic Number 14 2, MgKa II., IMM 1000 1200 800 600 400 200 o Binding Energy (eV) 2p Binding Energy (eV) Compoo.. Tl'P' SilicKles smcoll 98 101 10< Si in SiCh Monochrornaled Al Ka. 2p • 2p = IOJ.J eV Carbides Nitrides S~~ (Silanes) S~icates • smca Perkin-Elmer Corporation Physical Electronics Division m \M ) II' \ 100 Binding Ene!gy (tV) 90 Handbook of X-ray Photoelectron Spectroscopy Phosphorus P Atomic Number 15 2p LMM Monochromated Al Ka \ 1340 1310 1400 Binding Energy (eV) LMM 1400 1200 1000 800 600 400 o 200 Binding Energy (eV) Line Positions (eV) 2pll2 2plI2 =129.9 eV A=O.84eV 2s 188 2p112 2P3t2 3s 131 130 14 Auger Lines L,JMnM2J 1367 1134 140 130 (AI) (Mg) 120 Binding EneJgy (tV) if\. W l)erkin·Elmer Corporation Physical Electronics Division of X·ray Photoelectron Spectroscopy Ban dl.""k IJVV Phosphorus P Atomic Number 15 MgKa 2p LMM .15 LMM \ 1170 1200 1140 Birding Energy (eV) 1000 800 1110 600 Binding Energy (eV) 2p Binding Energy (eV) Comr-ound Type 128 129 130 131 132 133 134 400 200 2Plil = 129.9 eV 135 o 2Plll 6=O.84eV P P(rod) GoP loP PIospha" 1'yrophospM" M~aph0sph3te • PcOlo Ph,p Ph,PSH (PhOJ,PO / 140 \ 130 120 Binding Energy (eV) Perkin-Elmer Corporation PhYsical Electronics Division <n Sulfur Han~book S of X-ray Photoelectron Spectroscopy Atomic Number 16 J\ Monochromated AI Ko: '" LMM , 2s \ 1370 1310 '340 Binding EnertY (tV) LMM / f-.rJ 0 , , 1400 1200 1000 800 600 Binding Energy (eV) ~w o 200 400 Line Positions (eV) 2plIl' 164.0 eV 2plll !J.= Ll8eV Photoelectron Lines 2s 228 2plfl 165 2PY2 164 3s 18 Auger Lines L2JM23 MU I7S ,. '65 Binding Enetgy (eV) IJJ6 (AI) 1I0J (Mg) '55 m W Perkin-Elmer Corporation Physical Electronics Division HandbOok of X~ray Photoelectron Spectroscopy Sulfur S Atomic Number 16 1200 1000 800 600 Binding Energy (eV) 400 o 200 2p312 Binding Energy (eV) Compound Type 160 163 166 S Sulfide Sulfite SulFate SF, SO, Thiophene Mercaptan Cysteine SulFone I • 169 172 175 2p312 = 164.0 eV 118 6= 1.18eV • \ 175 16' 1S5 Binding Energy (eV) Perkin.Elmer Corporation Physical Electronics Division m 'II 61 Chlorine Handbook of X-ray Photoeleclron Spectroscopy CI Atomic Number 17 K Clin KCI Mooochromated AI Ka LMM (V , 2, 11JlO 1330 BindingEMgy(eV) K 2s LMM ~ K / W,.J 1400 ~l--AJ 1000 1200 ~ v, , 800 600 200 400 3, o Binding EneJgy (eV) Line Positions (eV) 2pYl =198.5 eV 2p,. A=L60eV Photoele<:tron Lines 2s 271 lpln 20t 2p,. 199 j, 11 3, 6 Auger Lines L23 M23M23 1304 1071 \ 21l WI (AI) (Mg) 191 Billding FJJergy (eV) Perkin-Elmer Corporation (J) Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Chlorine Cl Atomic Number 17 CI in KCI MgKa Compound Type Alkali Chloride C"Ch Ni01 PdCh KllrC" Pt{NHJhCh I'trchlorate KCIQ, "'00. 4Ii,Q ~CH,'£Hal K IMM 2plI2 Binding Energy (eV) 202 204 2M 198 200 -.• ~ • 2pll2 210 2pll2 =198.5 eV !J.=J.60eV • •• r Perkin-Elmer Corporation PhvsiC3\ Rlectmnics Division 208 ) 2lS "" Binding Enttgy (eV) (I) \ I" Argon Handbook of X-ray Photoelectron Spectroscopy Ar Atomic Number 18 51 Ar implanted in Si Monochromaled AI Ka 51 . 2p 51 2s , I , ) lMM 1400 3, 1000 1200 800 600 Binding Eoogy (eV) 400 o 200 Line Positions (eV) 2P31l = 241.9 eV 6=2.12eV PhOl:oelectron Lines 2s 320 2pIIZ 2PJn 35 244 242 24 Auger Lines LnM,)M13 1272 1039 ) 215 '45 (AI) (Mg) 235 Binding fJlergy (eV) m. Perkin-Elmer Corporation \jI Physical Electronics Division Han dbo ok of X-ray Photoelectron SpectroscollY Argon Ar Atomic Number s; 18 s; Ar implanted in Si s; Mg Ko: 1\ 2p 2, I 'lJ 3, 1200 1000 800 600 Binding Energy CeV) 2p3I1 Binding Energy CeV) Compound Type Ar in Ag Ar in Au Ar in eu Ar in PI Ar in graphite Ar inSi 240 241 2pll2 242 400 o 200 =241.9 eV fl:;;2.12eV -- P1n 2 A \ J 2.\5 245 ~ 235 Binding EneJgy (eV) Perkin-Eitner Corporation Physical Electronics Division 65 Potassium Handbook oIX-ray Photoelectron Spectroscopy K Atomic Number 19 2p LMM Monochromated AI Ko: 124{} 1280 1100 Binding Energy leV) LMM 3p " 1400 1000 1200 800 600 Binding Energy (eV) 400 o 200 Line Posilions (eV) 2plI2 2Pl12 ~ 294.4 eV Ii = 2.80 eV Photoelectron Lines 2s 380 2PJn 2pln 297 294 3s 35 3p 19 Auger Lines LnM23M23 JIO 1239 (AI) 1006 (Mg) JOO Binding fJltlly (tV) m 66 \lI Perkin-Elmer Corporation Physical Electronics Division HandbOOk or X-ray Photoelectron Spectroscopy Potassium K Atomic Number 19 Kin KCI Monochromated Al Ka CI 2s a a LMM : L..,.,J 1400 , 1200 1000 3p j'V . ~ 800 600 Binding Energy (eV) 400 a :k B, I V 200 0 2p3I1 Binding Energy (eV) Compound Type 291 292 293 294 KinKO 295 2P3l1 2py, = 292.9 eV • K Halides KCN IJ. = 2.77 eV KNo, KCJo, KC1O< K}PO~ K.P,Q, K>OO, K,o,o, Perkin-Elmer Corporation Physical Electronics Division •m \lI ) JlO 300 Binding Energy (eV) v \ 290 Calcium Handbook or X-ray Photoelectron SpectroSCOP}' Ca Atomic Number 20 2, Monochromaled Al Kn LMM 2s 1175 1200 1225 Biodin! Energy (eV) LMM 3,3, a 1400 1000 1200 800 600 Binding Energy (e V) o· 200 400 Line Positions (eV) 2plIl = 346.7 eV 1I = 3.60eV 2plll Photoelecuoo Lines 2s 440 2p1l2 3S I 2p3ll 341 3s 45 3p 26 Auger lines L2J M23 M23 lt9) (AI) 964 351) 1M,) 340 Binding fJlerzy (cV) m 68 'II Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Calcium Ca Atomic Number 20 0 Ca in CaCO) Monochromated Al Ka 2PJn 2P1I2 . IMM 0 ---..A , 2s C . ---"'\ Jp 3s _I 1400 1000 1200 800 600 Binding Energy (eV) 2Pl1l Binding Energy (eV) Compound Type 345 c. CaS each CoF, 346 347 • 34a 349 400 o 200 Ca in CaffiJ 2Pl1l =346.6 eV A=3j5eV CaQ CaCOl C'NO,), C.c.o. ''''"''' CaMo04 C.so. CaJSi)O, \ 3JjJ Bindillg Enc:tu (tV) Perkin-Elmer Corporation Physical Electronics Division m W Scandium Handbook of X-ray Photoelectron Spectroscopy Sc Atomic Number 21 2p>2 Monochroma,oo Al Ka lMM 117<) 1100 Binding Energy (tV) lMM 2s 3p 3, 14110 1000 1200 2plI2 =398.6 eV 8110 600 Binding EnelgY (eV) 400 o 2110 Line Positions (eV) 2p>2 6 = 4.87 eV Photoelectron Lines 2s 499 u 2p312 399 3s 51 3p 29 Auger Lines \ 410 2pln 404 400 Binding Enagy (eV) LM23 M2) L,MnM<, I'P) 1149 1118 916 885 IA1) IMg) 390 '------ ----.J m W Perkin-Elmer Corporation Physical Electronics Division I I Handbook of X-ray Photoelectron Spectroscopy Scandium Sc Atomic Number 2] 2pyz lJ,iM MgKa . 2Pl12 2s ~ /~ I• ~\ LMM ) ... 1200 , '- '" • "BiDding En(flY (tV) I()()() 3. I .1. 870 600 800 3, A< 400 200 o Binding Energy (eV) 2plI2 Binding Energy (cV) Compound Type 398 399 5< 5<N &,0, <1S«C,",l> SqC,",XCoH,l 400 401 402 Sc in &203 Monochromaled AI Ka 2pll2 2pll2 = 401.8 eV A=4.4eV • 410 \ 400 390 Binding Energy (tV) Perkin-Elmer Corporation m Physical Electronics Division \.&I "' Titanium Handbook of X-ray Photoelectron Speclrnscop)' Ti Atomic Number 22 Monochromated AI Kll f\ IIlKI '. lMM 1050 1065 Binding Encrzy (cV) 2s LMM I 3p 3, " " 1400 1200 1000 2pll2 =454.1 eV 800 600 Binding Energy (eV) 400 200 0 Line Positions (eV) 2plI2 A =6.17 eV Photoelectron Lines 2s 561 1 ... Binding Enetgy (tV) 2p3J2 454 \ 4" LM2)Mn 11198 865 3p 33 L}fI-12JM~s (II') 1068 (AI) 83) (Mg) m. 72 3s 59 Auger Lines 1------470 2pln 460 'II Perkin-Elmer Corporation Physical Electronics Division HandboOk of X-ray Photoelectron SIJcctroscopy Titanium Ti Atomic Number 22 2Pl11 Mg Kll LMM 2pII2 , 2s A ~'/ 3p , 1000 1200 800 A, A, , 3, -.1 • 600 Binding Energy (eV) 400 o 200 2Pln Binding Energy (eV) Compound Type •• 453 454 TI liB~ TIN liCI4 no T~ BaTiOl (cubic. tetra. CaTIOl PbytOl 455 456 457 459 Ti in TIOz MonochrollUllcd AI Ka 460 2p3l.! 2pll1 • 458,& eV I • Metalloctne T (J) !J. = 5.54 eV • • • SmOl Perkin-Elmer Corporation Phvsical Electronics DiYision 458 T / <1. Bind:il~ ... \ E.iqy (eV) 450 Vanadium Handbook of X-ray Photoelectron Spectroscopy V Atomic Number 23 2plI2 Monochromated Al Ku '\ , LMM ~ lOIS 1030 2Pl12 1(0) Binding Energy (cV) LMM 1\ / 2, A ~t) 3p , , 1400 1000 1200 M 800 600 3s M , 400 j o 200 Binding Energy (eV) 2P312 =512.2 eV Line Positions (eV) 2plI2 !:.l.= 7.64 eV Photoelectron Lines 2s 627 2Pl12 520 2P3f2 512 3s 66 3p 37 Auger Lines 535 74 51S Binding l!nergy (eV) LlMnM4S (I p) 1014 L3 M4S M4S 977 (AI) 781 744 (Mg) 495 Perkin-Elmer Corporation (I) Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Vanadium V Atomic Number 23 2plIl MgKa \ LMM LMM ~ , ~ 795 2pln 185 Binding Fne~y (tV) 115 2s M-J / 3p , 1200 1000 600 800 3!' '" '" , 400 o 200 Binding Energy (eV) o Is 2pY2 Binding Energy (eV) Compound Type 512 513 V VB, VN Oxide VOCb VOS04 Vanadate K,VICN, V(acae)3 VO(acac)l Melallocene 514 515 516 517 Vin V1Js Monochromated AI Ka 518 2plll 2PJa=511.4eV • D.=7.6eV / 535 LA ~ \ 520 Binding Ene~y (eV) Perkin.Elmer Corporation Physical Electronics Division 505 Handbook or X-ray Photoelectron Spectroscopy Chromium Cr Atomic Number 24 2"", Monochromated AI Ka LMM '" ,,, "" BiOOing ~ (tV) LMM 2, I 3p 3, Ac 0 1400 1200 800 1000 600 Binding Energy (eV) Ac 400 200 0 Line Positions (eV) 2PJn =514.4 eV A=9.WeV Pholoelet\ron Lines 2s 696 2pln 583 2J>3I2 574 3s 75 3p '3 Auger Lines L3MnM4S ('P) 959 726 \ 5" L3~i45M.i5 917 684 (AI) (Mg) 510 Binding Energy (tV) m W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Chromium Cr Alomic Number 24 2P312 '\ MgKa LMM LMM 2pln '" \. 125 110 Rindilll F.nagy (eV) h tJ 3p 3, M 1200 I ()()() 800 600 400 Ac A o 200 Binding Energy (eV) 2p312 Binding Energy (eV) Compound Type C, 574 I Cr Nitride CtBrl 00, Oxide C,F, U(OH), CcOOH K,o,Q, I(,U(CN' Cr(acacb Perkin-Elmer Corporation Physical Electronics Division 576 578 Cr in Cr203 580 MonochromalCd AI Ka 582 2p312 2P3i2 = 576.9 eV I •1':'-. •• '•" A::: 9.8 eV I 595 570 Binding Energy (eV) 77 Manganese Handbook of X-ray Photoelectron Spectroscopy Mn Atomic Number 25 21'>2 LMM~~ Monochromated Al Ka \.. 2pII1 90S Bindint Enttgy (eV) "" "" LMM 1\ /\vU 3p Js J. fu 1400 800 1000 1200 600 400 o 200 Binding Energy (eV) Line Positions (eV) 2Pl11 2pll1 = 639.0 eV 6 = 11.05 eV Ptlotoeb:tronLines l' 2s 2Pll1 2m 7fB 650 639 3s 83 3p 48 Auger Lines \ 645 L23MnMn 944 L3M2}M4~ L3 M4S M45 900 JIl 667 852 619 (AI) (Mg) 630 Binding Enetgy (eV) It' 78 \J! Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Manganese Mn Atomic Number MgKa 25 U'M LMM 2pj \ 685 610 BiJdng fJlcqy (eV) 655 3, 3, 1200 1()()() 800 600 Binding Energy (eV) 2PlI2 Binding Energy (eV) Com",,,,,, 1)"" 638 639 Mn 640 641 642 643 644 645 400 200 o Mn in Mn02 Monochmmaled Al Ka 2plIl 2Plll = 642.1 eV MnS A=ll.1eV MnCh MnFJ MoO Mn,Q, MoJO. MnD, MnOOH MnSQ, M~C,J-t,n • Perkin-Elmer Corporation Physical Electronics Division '45 BindiDg E1q)' leV) 6JO Iron Handbook of X-ray Photoelectron Spectroscopy Fe Atomic Number 26 Monochromalcd Al Ka LMM 2plI2 770 LMM Ilinding Ellergy (eV) 3p 3s 1400 I()()() 1200 400 800 600 Binding Energy (eV) o 200 Line Positions (eV) 2PJn = 707.0 eV 2p3ll I:J. = 13.10 eV Photoelectron lines 2s 845 2Pln 12Q 2P3n 7tr1 3s 92 3p 53 Auger Lines lMuMn L3M.(sM45 784 (AI) 888 \. 740 1W 551 655 (Mg) 700 Binding fJlergy (eV) m RO W Perkin·Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Iron Fe Atomic Number 26 MgKa LMM 5" 565 Binding Energy (eV) 2, LMM Jp 1200 1000 800 600 400 200 o Binding Energy (eV) 2p312 Binding Energy (eV) CompoundTypc 706 707 708 709 710 711 712 Fe in FC20J Monochromalcd Al KCt 713 F, reS Fclh (markasile, pyr) FcCl, FeCl) • 2p", =710.9 eV FeO 6= 13.6eV • Fe,O) I FcOOH FeS04 • K3Fe(CNj(, K4fe(CNj(, Perkin-Elmer Corporation Phv~;"'!11 Ji'1"I'Io.... n;l'<' ni",<,i,," m. u.J • 740 120 Binding Energy (eV) 700 Cobalt Handbook nr X-ray Pboloeleclron Spectroscopy Co Atomic Number 27 Monochromated AI Ka '710 Binding Energy (tV) 735 685 LMM 3p A, 1400 1200 1000 800 600 Binding Energy (eV) o 200 400 Line Positions (eV) 2"", ; 778.3 eV Pbocoelectron Lines A= 14.97 eV 2s 925 2pln 793 2PJn 778 3s 101 3p 60 Auger Lines Ljt1nM23 838 605 815 710 L:zM23Mn 831 598 L)MnM45 (I P) m 544 LJMl]M" <'PI LJM<JM<, nt 538 698 465 (AI) (M8) (AI) (M8) Binding Energy (eV) m. W Pcrkin~Elmcr Corporation Physical Electronics Division Handbook nf X-ray Photoelectron Spectroscnpy Cobalt Co Atomic Number 27 2plI2 Mg Ka. \. 500 450 415 Binding Entl!y (eV) 2s \1>IM 3p Js 1200 600 Binding Energy (eV) 1000 o 200 400 Co in 00 Co Col', <:of, CoO • C",o. C",o. Mooochromated Al Ka • • CoOOH Co(OHh CoSo. - Co(NI'hhCh Perkin-Elmer COrtlOration Phv..i('!'I1 li'1Pl"trnniM: ni11;"inn IYo\. W 2p" 2plI2 = 780.4 eV 1i=ISleV l.~:;t 710 815 Binding Ene!gy (tV) Nickel Handbook of X-ray Photoelectron SpectroscoPJ Ni Atomic lumber 28 2pYl Monochromated AI Ka LMM 635 660 610 Binding Ene!gy(eV) LMM 3p 3, 1400 1200 woo 400 600 Binding Energy (eV) 800 o 200 Line Positions (eV) 2pYl =852.7 cV !J. = l7.27 eV 2pYl Photoelectron Lines 2s 1009 2P112 870 211312 853 35 III 3p 67 Auger Lines L3M23~5 (I p) 712 479 LIMnMn 772 539 LJM1JM4S ep) L2MnM45 (I p) 865 Binding Ene'&Y (eV) 840 7116 473 641 408 m. L3M4SM4S 624 391 (AI) (Mg) Perkin-Elmer Corporation \U Phvsical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Nickel Ni Atomic Number 28 2PJt2 Mg Ka LMM 430 405 Binding Enetgy (eV) 2s 380 LMM Jp 3, 1200 1000 800 600 400 o 200 Binding Energy (eV) 2P3a Binding Energy (eV) Compound Type 852 853 854 855 856 857 Ni in NiO 858 2plI1 2pll1 = 853.8 eV Ni Silicides !J. = 11.49 eV NiS !lalides NiQ Ni203 Ni(N03n Ni(acac)l Ni(OAcn·4Hi> Ni(dimclllylglyoxim)l • 890 865 Binding Enetgy (eV) 841) Copper Handbook of X-ray Photoelectron Spectroscopy Cu Atomic Number 29 2plI2 Monochromated Al Ka LMM lSO S60 570 Binding Energy (eV) LMM 3p 35 1400 1200 800 1000 a 200 400 600 3d Binding Ene<gy (eY) Line Positions (eV) 2pll2 =932.1 eY 2pll2 /1 = 19.80 eV Photoelectron Lines 28 1097 2PIn 953 2P312 933 35 123 3pll2 77 3p312 75 Auger Lines L3MnM4s t'P) 648 415 f------/ \..::=====~-"\~ 925 970 L3M23M45 ep) L2M23M4~ (Ip) 640 401 (AI) (MgI L2M4sM.ts 628 395 548 (AI) 315 (Mg) Binding Energy leV) it"'\. \.U Perkin-Elmer Corporation Phvdf'!ll trl.."t..... "i,..'" T'li"idnll Handbook of X-ray Pholo~edron SpeclroscoPl' Copper CD Atomic Number 29 2pyz MgKa LMM 2pln 32' JJI Binding Energy (eV) "" 2s LMM ~/" ~ 3p 3s ~ 1200 800 1000 2"", Binding Energy (eV) Compound Type 93 I C, CUlS C..s C..cl 932 933 •• 934 400 600 Binding Energy (eV) 935 936 I 200 fl 3d o Cu in CUO Monodlromated AI Ka 2pyz =933.6 eV A=19.geV C,o, C,lO C,O Cu(OHh C..so. C"OA," Cu(saHcylaldOJ:ime) 910 Binding Enagy (eV) Perkin-Elmer Corporation Physical Electronics Division m 'II .7 Zinc Handbook of X-ray Photoelectron Spectroscopy Zn Atomic Number 30 2m Monochromated Al Ka. LMM '\ 515 480 Binding Energy (tV) 2plI1 LMM 1\ 2s J. 1200 1400 ./ ~~ 1000 3p I 400 800 600 Binding Energy (eV) 3d 3, o 200 Line Positions (eV) 2PJn =1021.8 eV Photoelectroo Lines 2PJn 6 = 22.91 tV 2s 1195 2Plf2 2plI2 35 1045 1022 140' 91 3pln 3pYl: 3d 89 10 Auger Lines 2Plfl ~ L,M"M<> ('P) L,M""n 660 427 L,M""'5 <'PI L2Mnt-45 ( lp) '-./ 573 1010 1001 582 349 340 559 326 (AI) (Mg) LJM4""" L2~5M4S 495 262 239 4n (AI) (Mg) Binding EneJgy (tV) it\. W Perkin·Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Zinc Zn Atomic Number 30 2plI2 MgKa LMM 285 250 Binding Energy (eV) LMM 3p l' j !Ooo 1200 800 600 Binding Energy (eV) 400 3d o 200 2plI2 Binding Energy (eV) Compound Type 1020 1021 1022 1023 1024 2PJa' 1021.8 eV !J.:= 22.97 eV Phosphide Halides ",,0 Zn(acach 2p" • • (Me.NhZnBr~ Znso4 Zn 4Sb07(OHh . 2H20 ZnCf204 ZnRh204 11l6O 1010 Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 89 Gallium Handbook of X-ray Photoelectron Sp<etroscopy Ga Atomic Number 31 lpJ12 Monochromated AI Ka LMM 4!' 430 410 Bindllg F.neru (cV) LMM 2s 3d 3p 3s 1400 1200 1000 800 600 400 o 200 Binding Energy (eV) Line Positions (eV) 2pJl2= 1116.1 eV Pb:>toelecum Lines Ii =26.84 eV 2pII2 2s 2pln 2pYl 3s 3pln 3p312 3d 1301 1144 1117 160 107 104 19 Auger Unes L3Mn.\ti5 (Ip) 1110 1100 L3MnM45ep) 501 271 514 (AI) 281 (Mg) L~4S L1~sM4s 419 1116 392 159 (AI) (Mg) BilKling Ene'l)' (eV) m. 90 \II Perkin-Elmer Corporation Physical Eledronics Division Handbook of X-ray Photoelectron Spectroscopy Gallium Ga Atomic Number 31 Mg KCt LMM ~ LMM l&l 195 115 Bmilll EDergy (eV) 3p 1000 1200 2"", Binding EnelID' (eV) Compound Type 400 600 Binding Energy (eV) 1116 o 2plll' 1116.7 eV 1118 1117 200 3d A= 26.84 eV 3d Binding Energy (cV) CompoundType 18 19 20 21 G. ' GaAs GaP A1GaAs 1100 (;"oJ 1110 Binding &1ergy (eV) '·erkin-Elmer Corporation Physical Electronics Division m 'II n, Germanium Ge Atomic Number 32 Handbook of X-ray Photoelectron Spectroscopy LMM Monochromated Al Kex ~ 3SO lJO 340 Birdinc EneJgy (eV) LMM 3d 3p 3, 1400 1000 1200 800 400 600 o 200 Bin<ling Energy CeV) Line Positions (eV) 3d ~ 29.4 eV 3d Photoe\eclron Lines 2PI!2 [248 2PJ/2 1217 3, 181 3pll2 122 3Plfl 126 3d 29 Auger Lines LJMnM4, '" 2ll 433 200 LJMnMn LzMnMn L]M.'UM4S ep) 534 301 525 292 444 (AI) 211 (Mg) ('I» L2M~~, ('Pj L~14S 412 179 342 1119 L1M45M45 (AI) 310 (Mg) 77 Bindilll Encrzy (eV) if\. Perkin·Elmer Corporation ~ Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Germanium Ge Atomic Number 32 MgKo LMM LMM ~ 105 III 91 BiOOing Energy (eV) 3p 3d 600 Binding EnelJlY (eV) 800 1000 1200 3d Binding EnelJlY (eV) Compound Type 29 30 31 32 33 400 3d =29.4 eV 200 o 3d Go GeA" GeTelAs2 GeS2TeAS2 G<S,As GeTC:2 GoTe GeSe, G<Se Sulfides • aeo, Perkin-Elmer Corporation Physical Electronics Division ., \ 20 Binding EnetxY (eV) m \Jl 0' Arsenic Hand,book or X-ra.y Photoelectron Spectroscopy As Atomic Number 33 Monochromated Al Kll '00 270 '" Binding f.neJgy (eV) LMM 3d lp Js 1400 1200 1000 800 600 400 o 200 Binding Energy (eV) Line Positions (eV) 3d",: 41.6 eV tJ.=O.6geV 3d", Photoeleclron Lines 2Plf2 1359 2pll2 1324 3s 205 3pln 146 3p3f2 141 3dY.! 43 3d5,12 42 Auger Lines L,MnM.,('P) 360 '" (At) L2MnM45 ep) LJ~5M45 L2~5~5 lJ6 262 226 (At) 40 Biooing f.nef!)' (eV) Perkin-Elmer Corporation (I) Physical Electronics Division Handbook or X-ray Photoelectron Spectroscopy Arsenic As Atomic Number 33 3p MMN MgKa 3d 3s 1200 1000 800 600 Binding Energy (eV) 3d", Binding Energy (eV) Compound Type 40 41 AlGaAs GoA, IMs Sulfides Ash 43 44 45 46 47 • A, AlAs 42 400 200 3d", =41.6 eV !J. =0.69 eV 3d", 3d" • • I • "'Bo A,,,, "'''' Perkin-Elmer Corporation ir\. Ph,,~il'!ll Ji'1Pf'trnniN: n;"i"inn ~ f• . Bindilg Encfty (tV) o Selenium Handbook 01 X-ray Photoelectron Spectroscopy Se Atomic Number 34 Monochromated AJ Ko: LMM LMM 210 ISO 3s 150 3p Binding Energy (eV) 3d 1400 1200 1000 400 800 600 Binding Energy (eV) o 200 Line Positions (eV) 3d", = 55.6 eV 3d", A=O.86eV Photoelectron Lines 3s 3plI2 3p312 232 169 163 Jd]12 51 Jdsn 5<i Auger Lines 65 " L2MnM4~ (lp) L3~5M45 257 18\ 45 Binding Energy (eV) m. 96 W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Selenium Se Atomic Number 34 3d MgKa Jp MMN . 3> 1200 1000 Compound Type 800 58 600 Binding Energy (eV) 59 400 200 3d", = 55.6 cV 60 6=O.86eV So 3dll1 AS25eJ / o 3d", Ga2Sel G<S, G<S~ Selenides S<Q, • H>SeO, [B.c.H.hS~ (CI.H~n (c.H£OOHns<o Perkin-Elmer Corporation if\. Physical Electronics Division \jI • } " ~ " ~ 45 Binding Encqy (eV) 97 Bromine Handbook of X-ray Phntoelectron Spectroscopy Br Atomic Number 35 • Br in KBr Monochromated Al Ko: 3d 3, • 3, MMN • --J 1\ 1400 /'! • • LP 4d LAW 1000 1200 800 600 Binding EneIgy (eV) 400 o 200 Line Positions (eV) 3d", =68.8 eV 3d", 6,=I.05eV ~oelectron 35 256 Lifl(S 3pln 189 3p312 182 Jd312 70 3d512 69 45 15 4d 5 Auger Lines M,JM4"'" ) 80 \ 1390 1157 (AI) (Mg) JO Binding Energy (tV) m 98 W' Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Bromine Br Atomic Number 35 K Sr in KBr Mg Ku MMN 3d Jp K K 4d 1000 1200 600 800 400 o 200 Binding Energy (eV) 3dSll Binding Energy (eV) Compound Type CsBr RbBr KBr NaBr 68 •- 69 3dSll 3dSll = 68.8 eV 70 Ii= I.05eV 3d]12 ,J LiBr c,Bo PbBo Ni(NH))(,B11 Pt(NH)).Brl ~ K1PtBr4 K2PtBr6 SO \ 10 /' fIJ Binding Energy (eV) Perkin-Elmer Co~por~ti~~ Physical Electromcs DIVIsiOn if\ 'M' 99 Krypton Handbook or X-ray Photoelectron Spectroscopy Kr Atomic Number 36 c Kr implanted in graphite Monochromatcd Al Kn c 1400 ~ '" 1200 1000 3d 3p '-J 800 600 Binding Energy (eV) 200 400 0 Line Positions (eV) 3d", =87.0 eV 3d", Ii= l.23eV Photoelectron Lines 3d 312 35* 287 3pln 216 3pyz 2llI 3d312 88 3d~ 87 48 21 4p 8 ) 10l 90 Binding EneI1Y (tV) 7l m 100 W' Perkin-Elmer Corporation Physical Electrvnics Division Handbook of X-ray Photoelectron Spectroscopy Krypton Kr Atomic Number 36 c MgKa c .......r Fe 3p 3d 4, 1200 Com~und Type 1000 800 3d", Binding Energy (eV) 84 86 600 Binding Energy (eV) 3d", !:J.=1.23eV 3d" "" Perkin-Elmer Corporation· !)hysical Electronics Division o 200 3d", =87.0 eV 88 • Kr in graphite 400 '" 75 Binding EnertY (eV) m \Jl 101 Handbook of X-ray Photoelectron Spectroscopy Rubidium Rb Atomic Number 37 Jp 3d MOllochromated Al Ka MMN v 4p 4, 1400 1000 1200 800 400 600 o 200 Binding EnelID' (eY) une Positions (eY) Jdsn = 111.5 eY b. = 1.49 eV PhollX:lectron Lines 35 325 v ]PIn 249 3P312 240 3d312 113 3dsn III 4s 31 4p 16 Auger Lines \ '25 115 105 Birxling Energy (eV) m 102 'II l)erkin·Elmel' Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Rubidium Rb Atomic Number 37 3PJil Rb in RbCl Monochromated Al Ka 3d \3PII2 \ CI a 3s MMN I~ 1400 I 0 ~W 4p 4, 1000 1200 109 400 800 600 Binding Energy (eV) 3d", Binding Energy Compound Type "'VI II 0 o 200 Rb in Rl£I 110 111 Rb RbN3 Rbi RbBr - 3d", 3d", = 109.9 eV Ii= 1.48 eV 3d,. (\ RhO RbF Rbffi RboP,Q, - RbCIo. Perkin-Elmer Corporation . Physical Electronics Division m 'l' ) 12' "' 105 Binding Ene'!}' (cV) ,., Strontium Handbook or X-ray Photoelectron Spcctros<oPl' Sr Atomic Number 38 3d Monochromaloo Al Ka ls o \tJ\ 0 4p " .J 1400 1200 800 \000 600 200 400 0 Binding Enetgy (eV) Line Positions (eV) 3d", = 134.3 eV 3d", !1=1.7geV 3d3ll Photoelectron Lines 3:s 300 3Pl12 3PYl 3dyz 3d~ 4s 281 270 136 134 39 4p 2\ \ 150 140 130 Binding Energy (eV) m 104 I'erkin-Elmer Corpondion \j! Physical Electronics Division Handbook of X-ray Photoetectron Spectroscopy Strontium Sr Atomic Number 38 3d Mg Kll j, ~ 0 L 0 \V\ 4p 4, .11 1000 1200 800 600 Binding Energy (eV) 400 200 0 3d", Binding EnelID' (eV) Compound Type s, s,o Srl', SrCOl s,so. S«No,h SrMoO. SrRh204 133 134 135 -- - 3d", =134.3 eV 136 3dJ12 \ 150 Perkin-Elmer Corporation Physical Electronics Division IT' W 3d", 1:.= 1.7geV 1<0 Binding Energy (eV) 130 Yttrium Handbook or X-ray Photoeledron Spe<:troscopy Y Atomic Number 39 Monochromated AI Ka MNV 3P111 )P,. 1375 1360 1345 Bindil\& Energy (eV) 3, MNN 4p 4, 1400 1200 1000 800 600 Binding Energy (eV) o 200 400 Line Positions (eV) 3d.. ; 156.0 eV 3d,. lJ.=2.05eV Photoelectron Lilies 3dlll j, 3plfl 3PJn 3<>t 311 299 3dJn Jdsn 158 156 4, 45 4p 24 Auger Lines v M<"",V 1356 1123 170 160 Billdin& Energy (tV) (AI) 1M,) ISO m 106 Perkin·Elmer Corporation ' " Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Yttrium Y Atomic Number 39 3d", MgKa MNV 3pyz 3s MNN 1140 1125 Rinding Energy (cV) 1110 4p 4, 1200 1()()() 600 800 400 o 200 Binding Energy (eV) 3d", Binding Eoergy (eV) Compound Type 155 156 3d", =156.0 eV 157 !:J. = 2.05 eV v V,o, 110 I'" \ 150 Binding Eoogy (tV) Perkin-Elmer Corporation Physical Electronics Division '0' Handbook 01 X-ray Photoelectron Spe<:lroscopy Zirconium Zr Atomic Number 40 Monochromated AI Kex ,]SO 1320 1335 JP312 Binding Enttgy (eV) 3p1/2 MNN ~'-c ~ 4p 4, _/0 1400 3d", =178.9 eV 1000 1200 200· 400 800 600 Binding Energy (eV) 0 Line Positions (eV) 3d", 6. = 243 eV Photoelectron Lines 3s 3Pll2 3m 3d312 3d:rn 4s 430 343 330 181 179 51 4p 2& Auger Lines M4S N23 N2J v M4S N4S N45 1331 (AI) 1393 1160 '' t08 '80 1104 (Mg) 110 Binding £mru (eV) if\ W Perkin·Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Zirconium Zr Atomic Number 40 MgKa J\ MNN 1""- MNN 3dsn 3d", lp", 1120 1105 1ll9ll Bindillg F.nergy (tV) JplIl Js '\. ~ 'p 4.s 1200 1000 800 600 400 200 Binding Energy (eV) 3dsn Binding Energy (eV) Compound Type a z,o, 118 119 180 181 I a', K£lrFi K,z,n K2lF5' H2O 182 18l 18' 3dsn =178.9 eV 185 . . sn 3d", •• "" Perkin-Elmer Corporation ' " Physical Electronics Division 'II 3d !J. = 2.43 cV o 180 Bindin& 110 EM:rtY (cV) 109 i Handbook of X-ray Photoelectron Spectroscopy Nb Niobium Atomic Number 41 Monochromated Al Ka MNV 3dJ12 1305 1320 1335 3P312 Binding Enagy (eV) MNN Js 4p 4s 1400 1200 1000 800 600 400 o 200 Binding Energy (eV) Line Positions (eV) 3dll2 =202.4 eV 3d,n I!. = 2.72 eV Photoelectron Lines 3s 467 3pln JPJ12 376 J61 3dJ12 205 Jdll2 202 4s 56 4p JI Auger Lines M4SN2)V 1319 1086 v M4S VV 1287 (AI) 1054 (MgI \ 'IS 205 195 Binding Ellergy (eV) m. lIO l'erkill·Elmcr Corporation \ j / Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Niobium Nb Atomic Number 41 MgKa MNV ~ MNV \ 3dsn ) Jdjn JP3I1 1100 1085 1070 Binding Energy (eV) 3PIf2 Js \ ~ \t -J 4, 4, 1200 1000 800 600 Binding Energy (eV) 400 200 ! o 3d", Binding Energy (eV) Compound Type 201 202 20J 204 205 206 3d", =202.4 eV 207 208 3d," f1 = 2.72 eV Nb NbN NbO Nb;O, l1li • LiNb03 CaNtn06 Ca2NbJOJ Br6(Nb6Chl)(BlI4Nl2 C!2(Nb6ClJl)(Pf]P).l C!2(Nb6C1Il)(Mt1S0)4 Perkin-Elmer Corporation l)hysical Electronics Division •• • 215 205 195 Binding Energy (eV) '" Handbook of X-ray Pholoeleclroo SpeclroscoPJ' Molybdenum Mo Atomic Number 42 Monochromaled Al Ka. MNV \310 1280 1295 Binding Encrzy (eV) 3, 4p 4, 1400 1000 1200 400 800 600 Biodiog Eoergy (eV) o 200 Line Positions (eV) 3d", = 228.0 eV 3d", A=3.13eV POOtoelectron Lines 3< 506 3pln 412 3P1'2 394 3dJn 3d", 2JI 228 4, 63 4p 36 Auger Lines M<,N"V 1299 1066 M4jVV 1264 (AI) 1031 (Mg) \ '40 2JO Binding EneIgY (tV) m 112 Perkin-Elmer Corporation ' " Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Molybdenum Mo Atomic Number MgKa / MNV 42 3ds12 - 3d," 'Iv MNV lOW 1065 IOSO Binding Energy (eV) 3pli2 3p1I2 \ 3, 1l 'J d ~ 4p 4, ~ 1200 1000 800 600 Binding Energy (eV) 3ds" Binding Energy (cV) Compound Type 226 227 228 229 230 231 232 400 3d", = 228.0 eV 233 o 200 3dsr'2 IJ.:::3.13eV Mo Botide M~C MoS, MoCb MoCl. MoCI 5 3dli2 • MoO, MoO, (NH)4Mo04 (CO),Mo{Ph)Ply • Perkin-Elmer Corporation Physical Electronics Division • \ 240 230 220 Binding Energy (eV) 113 Ruthenium Ru Atomic Number 44 Handbook of X-ray Photoelectron Spectroscopy Monochromated Al Kex 3d," MNN Jdli2 1230 1215 Binding Energy (eV) IlOO MNN 4, 1400 114 1200 1000 800 600 Binding Energy (eV) 400 200 4p o Perkin-Elmer Corporation ([> Physical Electronics Division Hrmdbook or X-ray Photoelectron Spectroscopy MgKa Ruthenium Ru Atomic Number 44 3d512 MVV 3d", MNV ,., '" 965 BiDding Energy (eV) 3PlJl ~ 3PI12 V 3. \. -J .A .p 4p 4. A "\ 1000 1200 800 600 400 200 Binding Energy (eV) 3d512 Binding Energy (eV) Compoond Type T/6 271 R" R..a, R..o, RuO) RuO. Ru(NH3hNlh Ru(NH3l.sN1Br2 Ru(NH).sN1Q2 Perkin-Elmer Corporation l)hysical Electronics Division 278 279 280 281 3d", =280.1 eV 282 283 o 3d", Ii = 4.17 eV •• • • \ 290 210 ... Rhodium Handbook of X-ray Photoelectron SpectroscoPJ Rh Atomic Number 45 Monochromated AI Ka MVV 1110 1205 Binding Enel&Y (tV) 3PlIl MNV 3, 4p 4, 1400 1000 1200 800 600 o 200 400 Binding Energy (eV) 3d", = 301.2 eV Line Positions (eV) 3d", A:4.74eV Photoelectron Lines 3dm 3s 629 A 3ptn 521 3plll 497 3d", 312 3d", J01 4, 81 4p 48 Auger Lines \ J20 ." 310 Biodin& fnclJY (tV) M4SN2]V M.isVV 1234 1001 1185 952 (AI) (Mg) JOO m. W Perkin·Elmer Corporation Physical Electronics Division Handbook of X-ra)' Photoelectron Spectroscopy Rhodium Rh Atomic Number 45 \. MgKa MVV MNV Jdll1 ~ ",0 Jdll1 93' Binding Energy (tV) 3Pl11 3pln 3s \. J _I' 4s 4p • A 1000 1200 800 600 Binding Energy (eV) 400 o 200 3d", Binding Energy (eV) Compound Type 307 308 309 Rh I Halides •• Rhih CIRh(Ph,p), CbRh(Ph)p») CloRhlPh,Ph 310 3d," • 307.2 eV 311 3d," Ii = 4.74 eV 3dll1 f\ Br6Rh(Ph)Ph ClzRMcytlooctoo;e,," Rhz(OAc)4·2H:10 \ Rh(NH2CH2COOh . H20 320 m Perkin-Elmer Corporation Phvsical Electronics Divi.~ion \II 310 BiMinI Energy (tV) 300 Hand~ook of X-ray Palladium Pd Photoelectron Spedroscopy Atomic Number 46 Monochroma,ed AI Ka MVV 1170 1140 !ISS Bindi"& Energy (eV) 3P3Jl 3pln MNY 3s 4s As 1400 '" 1200 1000 600 Binding Energy (eV) 800 200 400 If\. W' 4p 4d 0 Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Palladium ._.~-_. Pd Atomic Number 46 JdSll MgKa MYY 940 925 Binding Energy (eV) MNY 910 4d 4s 4p 1200 1000 800 600 400 200 Binding Energy (eV) Pd Pd,Si PdJSi o 3dSll = 335.1 eV • A::: 5.26 eV 3d3i2 t Halides PdQ Pd02 K2Pd04 \J K1PdBr4 K,PdCI~ Pd(OAc)2 Pd(SPh)z Perkin·Elmer Corporation Physical Electronics DivisiOiI • 350 340 Binding Energy (eV) 330 Silver Handbook of X-ray Photoelectron Spectroscopy Ag Atomic Number 47 3d5ll Monochromatcd Al Ka ~ 1145 3d", 1120 BiDdi"l FJlergy (eV) 3"", MNV I~ 3PI(2 3s .JU " 4<1 / 4s 4p "' 1200 1400 800 600 Binding Encrgy (eV) 1000 400 o 200 Line Positions (eV) 3d5ll = 368.3 eV Ii = 6.00 eV PlllJloelectron Lines 3d", 3, )P,n 3"", 719 604 573 3d", 37. 3d5ll 368 4, 4p 98 60 AugerU~ \ J82 3n M.uNn V M5 VY 1191 958 1135 902 M4 VY 1129 (AI) 896 (Mg) J62 Bindin& Energy (eV) it'\. Perkin-Elmer Corporation W Ph.vsical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Silver Ag Atomic Number 47 MgKa MVV 910 885 Binding Energy (eV) MNV 3py, 3pln 3, 4d 4s 4p lZ00 800 !OOO 600 Binding Energy (eV) ZOO 400 0 3d", Binding Energy (eV) Compoooo Type 367 368 3d", =368.3 eV 369 3d", !J.=6.00eV A, Alloys A"s A~ AgF A,F, Oxides A"co, Sulfate AgOOCCFl Ag(OAc) 382 312 362 Binding Energy (eY) Perkin-Elmer Corporation Physical Electronics Division IZI Cadmium Handbook or X-ray Photoeletlron Spectroscnpy Cd Atomic Number 48 Mooochromated Al Ka MNN 3d", I~ 1120 3d., 1105 1090 Binding Entru (eV) 3"", MNN I~ 1400 3Plf2 4d 3s V /\/ A / 45 4p 1000 1200 800 600 Binding Energy (eV) 400 o 200 Line Positions (eV) 3dll1; 405.1 eV 3dll1 Ii = 6.74 eV Pholoelectron Lines 35 772 3Pl12 652 3P312 618 3d}'2 412 3d512 405 4s 110 4p 69 4d II Auger Lines ~N4SN45 "0 1103 (AI) 870 (Mg) 395 Binding EnerJy (eV) It' 122 \JI Perkin-Elmer Corporation Physical Electronics Division Handbook of X.ray Photoelectron Spectroscopy Cadmium Cd Atomic Number 48 MgKa 3d", f~ MNN 3d", I-----' \ 'v 8lO '" "" Dindin! Energy (eV) MNN 3p", ''0 3pln 3s A. -1\ , 4d J 4s 4p ~ 1200 1000 800 600 400 200 3d", ' 405.1 eV 3d", Binding Energy (eV) o 3d", Binding Energy (eV) COOIJXlUnd Type 404 405 406 407 6. = 6.74 eV Cd 3d", H8lU~.2Te 000 CelSe CdS Halides CdO CdO, Cd(OUh CdCO> 420 395 Biooiag Eoc:rtY (eV) Perkin-Elmer Corporation Physical Electronics Division if\. 'lI Indium Handbook of X-ray Photoelectron Spectroscopy In Atomic Number 49 Monochromated Al Ka 34jJ2 MNN ~ ~ 3d3l1 V\ 1060 1075 1100 Binding Energy (eV) 3p3I1 3.Pl/2 MNN 4d 3s I" V J; 4s 4p '1400 1200 1()()() 400 800 600 Binding Energy (eV) o 200 Line Positions (eV) Jd 5J2 =443.9 eV t:.=7.54eV Photoelectron Lines 3s 828 Jd m 3Pl12 703 3p312 665 3dJ12 452 3d512 444 4s 123 4p 78 44 17 Auger Lines M4 N4S N4S 1016 (A1) 843 (M,) 4Jj '60 Binding Energy (eV) 124 if\. W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Indium In Atomic Number 49 I~ MgKa f-/ 3d5!2 MNN 3dJ12 U\ 855 840 Binding Energy (eV) 825 MNN V'v . 3P3fl 3p1I2 3, j • 4d 4s 1200 woo 600 800 400 4p o 200 Binding Energy (eV) Compound Type 3d,n Binding Energy (eV) 443 444 445 446 447 3d,n = 443.9 eV C. = 7.54 eV 3dsn I" !nSb I"P IOlTe] InCh InCI ln203 In(OH)3 In(acac)J Br2InEl4N Br41nPr4N •• 3dJ12 ~ ~ 460 /' 43S Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 125 Tin Handbook of X-ray Photoelectron Spectroscopy Sn Atomic Number 50 Monochromated AI Ka. 3d", I~ MNN ~J nno 3d", 0\ 1040 1055 BiDding Energy (cV) . 3m MNN 3Pln I'" 3, V ~ 4d j 4, 4p -u 1000 1200 1400 800 600 o 200 400 Binding Energy (eV) ld",;485.0eV 6=8.41 eV Line Positions (eV) 3d", 3s 885 3p In 751 3p]n 715 JdYl 493 3dsn: 485 4s 137 .4p 4d 89 25 Auger Lines ~N45N.(5 \ 1049 816 (AI) (Mg) Binding fucJgY (eV) m 126 Perkin-Elmer Corporation \jI Ph)'sical Electronics Division Handbook of X-ray Photoelectron SllcctroSCO!>y Tin So Atomic Number 50 Mg Ka ~ MNN Jd", .. v\ 835 820 Jdll1 805 BilldiDg EntItY (tV) . MNN 'v 3Pl11 3pII2 J. ; 4d 4, 4p V 1200 1000 600 Binding Energy (eV) 800 3d", Binding Energy (eV) Compound Type 484 S, SOlS Halides SOO 485 486 487 400 3dll1 =485.0 eV 488 6=8.4IeV • o 200 3d", 3d", S..o, N32Sn(h PhiSn PluSn (Halide) Me3SnF \ Mt:!SnF2 BriSo(El.Nh 500 Binding Energy (tV) Perkin-Elmer Corporation Physical Electronics Division ''" Antimony Handbook of X-ray Photoelectron Spectroscopy Sb Atomic Number 51 3d", Monochromated Al Ka MNN ) . 3d3ll I~ \J\ 1040 . 1010 102.5 Binding Energy (e V) 3p3Il MNN I~ 3pII2 V 3, 4<l ) -l~ 4, 4p ....A 1200 1400 3d", 1000 400 800 600 Binding Enei&Y (eV) o 200 Line Positions (eV) =528.3 eV l'1 = 9.34 eV Photoelectron Lines 3d3ll 38 944 3pJn 813 3p312 767 3dJ12 537 3dYl 528 4s 153 lip 99 4<l 33 Auger Unes MtN4S N4S t022 (AI) 789 (Mg) 545 ... 520 m W Perkin-Elmer Corporation Physical Electronics Division Handbook of' X-ray Photoelectron Spectroscopy Antimony Sb Atomic Number 51 3ds12 MgKa (~ MNN Jd3i2 0\ 810 MNN 795 780 Binding Energy (eV) 3PI12 , V J~n !~ U \ 4d "0 1200 1000 800 600 Binding Energy (eV) 3d sn Binding Energy (eV) Compound Type 528 Sb AISb Sulfides Halides Sb,O, 529 530 531 532 3d", =528.3 eV 533 Il = 9.34 eV •• Ph3Sb BU3Sb a 200 3d", 3d3i2 ". Shi)5 KSbF6 NaSbF6 CsSbF4 400 • \ 545 / 520 Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 110 Tellurium Handbook of X-ray Photoelectron Spectroscopy Te Atomic Number 52 Monochromated AI Ka MNN 985 ''''' 1015 Binding Energy (eV) MNN 4d 4s 4p \400 \200 1000 800 600 400 o 200 Binding Energy (eY) Line Positions (eV) 3d,n = 573.\ eY 6= IO.3geV 3d1ll Photoelectron Lines 3d., )PIn 871 3"", 820 3d., 583 3d", 1009 4, 170 4, 4d., 4d", III 47 41 5, 12 j, 573 Auger Lines \ ~ \. MsN45 N45 ~N4514, 1005 995 762 772 'Ol (AI) (Mg) Bindilll f..Dc'IY (eV) rn. Perkin-Elmer Corporation \jI Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Tellurium Te Atomic Number 52 Mg Kll MNN MNN "" 765 Bindint FneJu (cV) 750 Js 4d 4s 1000 1200 800 600 Binding Energy (eVJ 400 4p o 200 3d", Binding Energy (eV) Compwnd Type 572 573 514 575 $76 577 Te 518 3d", = 573.1 eV A = 10.39 eV We GeTe Hgo.A2Te Tellurides Halides TeOz TeOz • T~OH' P!l2Te2 Br}TePh Perkin-Elmer Corporation Physical Electronics Division • m 'lI \ 16l Binding f.rJaD (cv) "' Iodine Handbook of X-ray Photoelectron Spectroscopy I Atomic Number 53 3dsn 1in KI Monochromated Al Ko: 3d., MNN IIA ~ ~ ~ \ 95JJ 1100 BiMing FMrgy (tV) ~J K ~ ........ J. K Jp3ll 4d 3plIl / K 4, I 4p ~ 1400 400 SOO 600 Binding Energy (eV) 1000 1200 ~l, o 200 Line Positions (eV) 3dsn 3d sn = 619.3 eV KK 55 V A=IJ.50eV 3d., PhoI:oelectron Lines 35 107) 3pln 930 3m 875 3d., 630 3dsn 619 45 187 4p 4dsn 4dS/1 ls 123 51 49 18 Allger Lines ~ / 640 \. 615 Binding ~y M5N45N45 M4N.o,N41 982 749 971 738 (tV) m 132 (AI) (Mg) W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Iodine I Atomic Number 53 3d512 I in KI MgKa MNN IIv\ 3dJi2 ~ ~ \J\ no MNN K 3,;" j 140 110 Binding E'nergy (eV) 3'lll ~ 'V LAI! K 4d K 4, A 4, KK cI 800 1000 1200 600 Binding Energy (eV) 400 200 , tJ o 3ds12 Binding Energy (eV) Compound Type 618 619 620 621 &22 623 3d,n= 619.3 eV 624 3d5l1 !:J=lI.5eV " Alkali iodides 3dJi2 Agi Nih Nih· 6H20 • Nal03 Nal04 H5J06 bOl lei leb Perkin-Eimer Corporation Physical Electronics Division •• \ 615 640 Binding Energy (eV) 133 Xenon Handbook of X-ray Photoelectron Spectroscopy Xe Atomic Number 54 C Xc implanled in graphite Monochromated AI Kll MNN M 3,312 fI i-'- 3d", ~ 970 '\ 3d1l2 ,.., 94' Binding Energy (eV) MNN C Jplll .3P1t'2 4d ~ "'1<\ 4p 4, I 1400 1000 1200 3d", = 669.7 eV 800 600 Binding Energy (eV) 400 o 200 Line Positions (eV) 3d", Photoelectron Lines 6= 12.67eV 3d1l2 . 3, Jp,n 3pll2 3d1l2 3d", 1141 996 934 683 670 4, 4, 4d1l2 4d", 2ff1 139 63 61 "17 Auger Lines MsN4SN45 955 \ 700 67' Bn.lirl& Erqy (tV) 722 M.iN4sN45 942 (AI) 709 (Mg) "" m 'II Perkin-Elmer Corporatiol Physical Electronics Dh'isioJ Handbook of X-ray Photoelectron Spectroscopy Xenon Xe Atomic Number 54 MNN C Mg Ka c 740 j1 115 Binding F1!cIgY (cV) 690 3dJ12 3pJ12 , MNN 3d5J2 ~ \ • '\, -1 4d 4, 1200 1000 800 600 Binding Energy (eV) 3dS/2 Binding Energy (eV) Compound Type Xc in Ag Xe in Au Xc in Cu Xe in Fe Xe in graphite N34XeQ, 668 669 610 • • • 611 672 673 400 200 3d512 =669.7 eV 614 4p 6 = 12.67 eV o 3d512 3dJ12 • 100 615 650 Binding Energy (cV) Pcrkin·Elmer Corporation Physical Electronics Division U5 , Handbook of X-ral' Photoelectron Spectroscopl' Cs Cesium Atomic Number 55 Monochromaled AI Ka. MNN 95. 920 890 BiJJlint Energy (eV) 3P1I2 3pYl MNN 3, 4d 4p 4, o 1400 1200 1000 400 800 600 Binding Energl' (eV) o 200 Line Positions (eV) 3d"," 726.4 eV 3d", Ii = 13.94 eV PhOloelectron Lines 3dJll 3s 1219 4, 234 3Plfl 1069 3Pl1l 1002 3dJll 740 3d", 726 4plfl 4Pl1l 161 4dJll 4d", 80 77 173 5, 25 Auger Lines 761 740 Bindilll FJlergy (tV) 115 MsN45N.ts 931 698 ~N45~S 918 685 m (AI) (Mg) Perkin-Elmer Corporaliol ' " I'hysical Electronics Divisiol Handbook or X-ray Phot""I'clron Spectroscopy Cesium Cs Atomic Number 5S Jdsn Mg Ka MNN 3dJll 710 Binding Energy (tV) MNN 4d 4p 4, 800 1000 1200 600 400 o 200 Binding Ene~y (eV) 3dsn Binding Compound Twe 723 Ene~y 724 (eV) 3dsn = 726.4 'V .725 3d sn fo"o:.l3.94eV 3dJll Cs Halides CsN, es,so. CSlPO. CS.P20J CsCl0~ CS1Cr04 CS£r-/h CsOU Perkin·Elmer Corporation Physical Electronics Division 765 740 Binding Enol)' (tV) 137 Barium Handbook of X-ray Photoelectron Spectroscop)' Ba Atomic Number 56 Monochromaled AI Ka. MNN 930 MNN 3p3/2 Binding Energy (cV) 4d 4p 4, 5s 1400 1200 3d", =780.6 eV 400 800 600 Binding Energy (cV) 1000 5 o 200 Line Positions (eV) 3d", 6= 15.33eV 3d3/2 Photoelectroo Lines 3, ~ 138 195 Jp3/2 1064 3d3/2 796 4, 254 4PII2 193 4pyz 4d3/2 93 4d", 90 179 78\ 5, 31 Sp 15 Auger Lines \. '" 3pII2 1138 3d", 1m no M5N.t5N.(s ~N45N'(5 900 886 667 653 (AI) (Mg) Binding Energy (eV) iY\ 'II Perkin-Elmer Corporation Physical Electronics Diyision Handbook of X·ray Photoelectron Spedroscopy Barium Ba Atomic Number 56 MgKn MNN OJ<} 700 Binding Energy (eV) MNN 4d 4p 4, S. 5p gOO 1000 1200 600 400 200 o Binding Energy (eV) 3dl/2 Binding Energy (eV) Compound Type 778 T19 ·780 - B, B'lS B,O Ba(NOlh BaCO) B'lSO. BaCr04 BaMo04 BaRh~ Perkin-Elmer Corporation Physical Electronics Division - 3d"" 780.6 eV 781 l!.=1533eV 810 795 710 BindillJ Energy (eV) 139 Lanthanum La Atomic Number 57 Handbook of X-ray Photoelectron Spectroscopy Monochromated AI Ka 3d1ll . MNN 4d MNN 4p 45 ~ 1400 1200 1000 V 400 &00 600 Binding EneTID' (eV) 55 200 5p 0 Line Positions (eV) 3d", =&35.& eV !J. = 16.78 tV Photoelectron Lines 3d1ll 3d", 1128 iS3 836 45 4Plfl 21J 41'312 4dlll 197 106 MsN4SN4:i 867 55 5p 34 IJ 820 634 M4N4S N45 854 621 m 140 4dlll 103 Auger lines \ 845 Binding EPe'l)' (tV) 3Pl1l 1208 27S ~ 87<1 3plI2 (AI) (Mg) Perkin. Elmer Corporation \j! Physical Electronics Division iandbook of X-ray Photoelectron Spectroscopy Lanthanum La Atomic Number 57 3d", MgKa Jdlll 3PlIl MNN '--'" , 4d 4, .A G "\ 1200 800 1IlOO 600 Binding EnelID' (eV) 3d", Binding Energy (eV) Co~ndType 833 834 835 Corporation 'hysical Electronics Division 400 5s 5p o 200 3d", = 835.8 eV 831 838 839 A= 16J8eV 3d", ~ u uH, u,o, 'erkill~Eliller 836 4p (]) 141 Handbook of X-ray Photoelectron Spectroscopy Ce Cerium Atomic Number 58 Monochromaled Al Ka 3dsn ld", / lPln \:V lJ MNN 4d 4p 4, 0 ""\. 1400 1200 !OOO 800 600 Binding Energy (eV) 400 5 Is, 200 0 Line Positions (eV) 3d", = 883.8 eV Photoelectron Lines 3d", 6= 18.10eV 3d", 3Plll 1m lPln Jd3ll liS< 902 3d", 814 4s 290 4pln 4P3ll 4d", 4d", 223 'If1I 112 109 5, 36 5p 18 Auger Lines M45N~5N45 \ 940 ... 900 Binding Fnergy (eV) 8ll Wl (AI) (Mg) "60 m 'lI Perkin-Elmer COl:poratioll Physical Electronics Division Handbook of X-raj' Photoelectron Spectroscopy Cerium Ce Atomic Number S8 3d", MgKa 3d", . . MNN 0 '- • 4d '--~ 4, 4p I '-- 1200 600 800 1000 Is o 200 400 5p Binding Energy (eV) 3d", Binding Ene~y (eV) Compou,d Type 881 882 883 884 885 886 3d", ~ 883.8 eV 3d", /::, = 18.10 eV 3d", Co etA. CePdl CoSe CeCU1:Sh c.o, • CoH, 900 Binding EMgy (eV) Corporation Physical Electronics Division l)erkin~Elmer 860 Handbook of X-ray I)hotoelcctron Spectroscopy Praseodymium Pr Atomic Number 59 Monochromated Al Ka 3d", Line Positions (eV) 3d," =931.8 eV !J. = 20.4 cV Photoelec!roll lines 3d312 3PI12 3plI2 3d312 3d", 1339 1242 952 932 4, 4Pln 4p1l2 4d 5, 305 234 218 115 38 5p 18 Aliger Lines 990 '50 910 M45 N4S N4S 797 (AI) 564 (Mg) BindiDg Erqy (cV) 144 Perkin-Elmer Corporation (J) Physical Electronics Division landbook of X-ray Photoelectron Spectroscopy Praseodymium Pr Atomic Number S9 3d", MgKa 3d", .• ~V MNN 4d ~ 1200 1000 4p I .--J ~ 400 600 800 4, 200 5.< 5, o Binding Energy (eV) 3d", Binding Energy (eV) Compound Type 931 932 • 93J 3d", =931.8 eV Ii:::: 20.4 eV 934 935 • 4d Binding Energy (eV) Compound Type liS 116 II? 99OL_~_ _-----C9C:C50::-------'"-=-;910 Bindin: Energy (tV) Perkin·Elmer Corporation Ilhysical Electronics Division 145 Handbook of X-ray Photoelectron Spectroscopy Neodymium Nd Atomic Number 60 3d", Monochromated Al Ka 3dJlJ 3pJIJ \.;\ MNN \ J 4d 4p 4s 0 14110 I zoo woo 800 600 Binding Energy leV) 6= 22.6eV 5s zoo 400 3d", 3d", =980.8 eV U 5p o Line Positions (eV) Photoelectron Lines 3pJlJ nOJ 3d", 1003 3d", 98J 4s 320 4PIf2 4P312 4d 245 228 J2J 5s 39 5p 19 Auger Lines M4S N45 N45 1040 100II 758 525 (AI) (M,) Binding Energy (eV) m 146 W Perkin-Elmer Corporation Physical Electronics Division iandbook of X-ray Photoelectron Spectroscopy Neodymium Nd Atomic Number 60 3dsn MgKa 3d", MNN 0 4d ~ 1200 1000 800 4s 400 600 4p 0 200 Is 5p o Binding EnelID' (eV) 3d", Binding EnelID' (eV) Compoond Type 9SO 981 3d",; 980.8 eV 982 !J. = 22.6 eV Nd Ndf)3 4d Binding EneIgy (eV) Compound Type 119 120 1040 )erkin-Elmer Corporation lhysical Electronics Division 1000 Binding Energy (eV) 147 Handbook or X-ray Photoelectron Spectroscop) Samarium Sm Atomic Number 62 3d3f2 3dS12 Monochromated AI Ka MNN 4d 4p 4s 5s 1200 1400 1000 400 800 600 Binding Energy (eV) , i' 3d"," 10Sl.1 eV A:; 26.8 eV Sp o 200 Line Positions (eV) 3d512 Photoelectron Lines 3d" 3d5n IOSl 3d312 1108 4s 349 4pJ/2 283 4p}(.I: 250 4d 129 5$ 41 Sp 19 Auger Lines M4S N4S N45 1140 1100 Binding fJlergy (eV) 682 (AI) 449 (Mg) 1060 m 148 \II Pcrkin~Elmcr Corporatiol IJhysic~d Electronics Divisiol Handbook nf X-ray Phnln<leclron Spectroscopy Samarium Sm Atomic Number 62 MgKa MNN 4d 4p 5, 1000 1200 600 800 200 400 5p o Binding Energy (eV) 3d", Binding Energy (eV) COlD;lOOnd Type Sm Sm203 .. 1081 1082 3d", = 1081.1 eV 100 1084 Ii = 26.8 eV - 3dJi2 "40 "00 1060 Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 149 Handbook of X-ray Photoelectron SpectroSCOJlY Europium Eu Atomic Number 63 Monochromaled Al Ka. MNN 4s 4p 5, 1400 1200 1000 400 800 600 Binding Energy (eV) o 200 Line Positions (eV) 3dlll =1125.6 eV 3d",· 3dlll t. = 29.8 eV Photoelretron Lines 3dYl 1155 Jd512 1126 4$ 363 4pln 289 4PY2 255 4d 128 55 39 5p 19 Auger lines M.(sN~sN.s 1190 ISO 1150 Binding Enc'!y (eV) 631 (AI) '04 (Mg) 1110 if\. W Perkin-Elmer Corporation Physical Electronics Oi.vision Handbook of X-ray Photoclectroo Spectroscopy Europium Eu Atomic Number 63 MNN Mg Ka 5p 1000 1200 800 600 Binding Energy (eV) 400 200 o 3d", Binding Energy (eV) Comp(xliKI Type 1123 1124 1125 1126 1121 4d = 128.2 eV 1128 1129 • Eu 4d Binding Energy (eV) Compound Type Eu EU20J 128 129 130 131 • Perkin-Elmer COr(JOration l)hysical Electronics Division 132 133 134 135 I' 180 150 120 Binding EIlerv (tV) if\ W 1'::;1 Gadolinium Gd Atomic Number 64 Handbook of X-ray Photoelectron Spectroscopy Monochromated AI Kn MNN 4d 4p 5p 5s 1400 1200 I()()() 800 400 600 o 200 Binding Energy (eV) Line Positions (eV) 4d. 140.4 eV 4d Photoelectroo Lines 3d", 1186 3dJn 1218 4s 31S 4Pln 291 4p1l2 m 4d 140 5s 43 5p 4f 21 S Auger Lines ~~ 602 180 130 369 (AI) IMS) Binding EnCl!Y (eV) m 1.1\1. Perkin-Elmer COrjlOration \jI Physical Electronics Division landbook of X-ray Photoelectron Spectroscopy Gadolinium Gd Atomic Number 64 Mg Kll MNN 4d ,[ 5p 1200 tooo 400 600 800 o 200 Binding Energy (eV) 4d Bindiog Energy (eV) Compound Type 140 141 142 143 4d 144 =140.4 eV 4d Gd Gd,o, 3d5ll Binding Energy (eV) Compound Type 1181 Gd Gd,o, 'erkin-Elmer Corporation 'hysical Electronics Division 1188 1189 ISO Birding EnettY (eV) '30 '" Terbium Handbook of X-ray J)hotoelectron SpectroscOIJ)' Tb Atomic Number 65 3d", ldyz Monochromated AI Kn MNN 4d 4f 5, 1400 1200 1000 800 600 Binding Enelty (eV) 400 5p o 200 Line Positions (eV) 4d = 146.0 eV 4d Pholoeleclr1:m Lines 3d", 1276 3d", 4, 396 'P,n 1241 322 4"", 285 4d Is 5p 146 45 22 " 8 Auger lines '' M4sN4sN45 M4SN 4sV MsVV M,VV 559 326 411 260 230 178 (AI) (Mg) '40 Binding Energy (eV) if\, W Perkin-Elmer Corporation Physical Electronics Division Handbook nf X-ray Phntoelectron Spectroscopy Terbium Tb Atomic Number 65 MgKa MNN 4f Sp ~ 1200 tOOO 800 600 400 200 o Binding Energy (eV) 4d Binding Energy (eV) Compoond Type Tb Tb,Q, ThO, 145 146 147 148 ~, 149 ~ 4d 4d =146.0 eV Jd 5ll Binding Energy (eV) Compound Type 1240 Tb Tl>,o, ThO, )Jerkin-Elmer Corporation Physical Electronics Division 1241 1242 -- 140 190 Binding Enesgy (eV) J55 Dysprosium Dy Atomic Number 66 Handbook of X-ray Photoelectron Spectroscopy 3d1ll Monochromatcd Al Ka 3d", MNN 4d 4p 4 5s 1400 JOOO J200 SIlO 600 Binding Energy (eV) 400 5p o 200 Line Positions (eV) 4d; 152.4 eV Photoelectron Unes 3d1ll 1333 3d", 4, 417 4Plf2 4P3n 4d j, 331 '!J1 152 48 1296 5p 23 4f 8 Auger Lines 200 170 ~sN4sN45 M45~5V 526 36ll (AI) 140 Binding &1ergy (eV) m W Perkin-Elmer Corporation Physical Electronics Division landbook of X-ray Photoelectron Spectroscopy Dysprosium Dy Atomic Number 66 4d MgKa 4f 5p 5, 1200 600 1000 400 200 o Binding Energy (eV) 4d Binding Energy (eV) Compoond Type 152 156 160 '164 4d = 152.4 eV 168 Dy 4d Drill 3d", Binding Energy (eV) Compoond Type 1287 Dy DnO) 1289 , 129\ 1293 1295 • 200 110 140 Binding Energy (eV) ~crkin·Elmer Corporation =-hysical Electronics Division 157 Holmium Handbook or X-ray Photoelectron Spectroscopy Ho Atomic Number 67 3dlll Monochromated AI Ka IV 3d", MNN 4d 4f 5 5p '.J 1400 1200 800 1000 600 400 o 200 Binding Energy <eV) Line Positions (eV) 4d ~ 159.6 eV 4d Pholoeleeuoo Lines 4PII2 4Pl1l 4d 1352 4, 435 353 309 160 50 SPin 5Pl1l 49 30 24 'f 9 3dlIl 3d", 1393 Auger Lines 100 M.1srt.5N4j ~sN4SV 488 31' ""VV 111 (AI) IlO BirKling Energy (eV) m. 158 'II Perkin-Elmer Corporation Physical Electronics Division Handbook nf X-ray Photoelectron Spectroscopy Holmium Ho Atomic Number 67 MgKa 4, 4Pi12 4f 5p 1200 1000 800 600 Binding Energy (eV) 400 o 200 4d Binding Energy CeV) Compoooo T"" 158 159 Hn - t60 4<1: 159.6eV 4d 200 Binding Energy (tV) Perkin-Elmer Corporation Physical Electronics Division m 'II ''0 Erbium Handbook or X-ray Photoelectron Spectroscopy Er Atomic Number 68 MNN Monochromated Al Ka 4PlIl 4d 4r 5p 1400 1200 1000 800 600 400 o 200 Binding EnclJiY (eV) Line Positions (eV) 4d =167.3 eV 4d Photoelectron Lines 4s 451 4plfl 368 4P312 321 4d 167 5s 52 5p1l2 31 5pY2 24 4f 9 Auger Lines MsVV M,VV 98 56 (AI) ,(;) 210 Binding &letu (eV) m 160 Perkin-Elmer Corporation \jI Physical Electronics Division Handbook of X-my Photoelectron Spedroscopy Erbium Er Atomic Number 68 Mg Ktt 'f 5, 1200 soo 1000 600 400 200 Binding Energy (eV) o 4d Binding Energy (eV) COffiJXlund Type 167 & & &,0, 168 4d = 167.3 eV 169 4d - 210 BiJldilll EaefD (cV) Perkin-Elmer Corporation if\, Physical Electronics Division W 160 161 Thulium Handbook of X-ray Photoelectron Spectroscopy Tm Atomic Number 69 MNN 'P3Il Monochromated AI Ka • J 1400 I()()() 1200 800 600 o 200 400 Binding Energy (eV) Line Positions (eV) 4d = 175.4 eV 4d Photoelcaroo Lines 4$ 4pJn 384 470 4Pl12 4d 5$ 5p1I2 5pYl 4f 333 175 53 32 25 8 Auger Lines M4S N4S N45 398 (AI) 220 190 160 Binding EPelgy (eV) m 162 W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Thulium Tm Atomic Number 69 4d 'f Sp 1200 gOO 1000 600 Binding Energy (eV) 4<1 Binding Energy (eV) Compound Type 175 11' Tm - 400 4<1 =175.4 eV 116 220 o 200 4<1 190 Binding Energy (tV) 160 m IJerkin-Elmer COfJlOration Physical Electronics Division \j! 163 Handbook of X-ray Photoelectron Spectroscopy Ytterbium Yb Atomic Number 70 \ Monochromated Al Kn 4d 41 4PlI2 4PJf2 5p 5, 1400 1200 800 600 Binding Energy (eV) 1000 400 o 200 Line Positions (eV) 4d =182.4 eV 4d Photoelectron Lines 4s <In 4Pln. 389 4PYl 341 4d 182 5s 51 5pln 30 5p3i2 24 4f 3 170 220 Binding Energy (eV) m. t64 W Pcrkill~Elmer Corporation Physical Electronics Division Handbook or X-ray Photoelectron Spectroscopy Ytterbium Yb Atomic Number 70 Mg Ko. 44 4f 4, 5p t200 1000 800 4d Binding Energy (eV) COOlp>Und Type Vb Yb,Q, 181 182 • 183 184 400 600 Binding Energy (eV) 185 186 o 200 4d; 182.4 eV 4d • 170 22Jl Binding Enogy (tV) Perkin·Elmer Corporation II\, Physical Electronics Division W 165 Lutetium Handbook of X-ray Photoelectron Spectroscopy Lu Atomic Number 71 Monochromatcd Al Ka 4d 'f 'PJn 4, 5p 5, 1400 1200 1000 800 600 o 200 400 Binding Energy (eV) Line Positions (eV) 41112 =7.3 eV .1.=1.5eV 41", Photoeleclroo Lines . 4, 509 55 57 20 10 4pln 413 'l'J/2 3!0 4dl12 206 4d", 1% SPIn 5pl12 4f", 4f7(2 34 T1 9 7 o Binding Energy (cV) if\ 166 Perkin-Elmer Corporation \j!' Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Lutetium Lu Atomic Number 71 4f Mg Ka 4d 4PlIl 5p 1000 1Z00 800 600 Binding Energy (eV) 4fln Binding Energy (eV) Compound Type 5 Lo 6 7 .. 8 9 400 zoo o 4fln =7.3 eV t::.=1.5eV 4flll 4f712 \ 10 ./ o Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 167 Handbook or X-ray Photoelectron Spectroscopy Hf Hafnium Atomic Number 72 4f Monochromated AI Ka NNN 1l4<l 1310 Binding Energy (tV) 1280 4PlI2 4s 5p 5s 1400 1200 1000 800 400 600 200 o Binding Energy (eV) Line Positions (eV) 4f712 41," = 14.3 eV t:. = 1.7J eV Photoelectron Lines 41", 4s 534 'PI" 4Pl12 4dll2 431 380 222 4dY2 211 5s lp," 5Pl12 41", 16 4f112 14 63 38 JO Auger Lines 2S " N~61N1 N4N~1N7 1311 1084 1306 1013 (AI) (Mg) 5 BiIldill& EaeW (tV) 168 m W l'erkin·Elmcr Corporation Physical Elettronics Division Handbook of X-ray Photoelectron Spectroscopy Hafnium Hf Atomic Number 72 'I NNN Mg Ka 'dl/1 1100 . ''''' " BMiDg Energy (tV) Sp 1200 1000 800 600 400 200 o Binding Energy (eV) 4fJn Binding Energy (eV) Compound Type HI HIO, I' - IS 4fJn =14.3 eV 16 !J = 1.71 tV 4dl/1 Binding Energy (eV) Compound Type HI HfO, 2lJ 212 ~ Perkin-Elmer Corporation Physical Electronics Division 214 " 15 Binding Encro (tV) 5 m W 169 Tantalum Handbook nf X-ray Photoelectron Spectroscopy Ta Atomic Number 73 Monochromated AI Ka NNN 4f 1J40 NNN 1280 1310 Biooing Energy (eV) 4pJll 4, 5p Is 1400 1200 1000 800 600 400 200 o Binding Energy (eY) m 170 W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Tantalum Ta Atomic Number 73 MgKa 4f NNN NNN 4dsn 'd312 1100 1050 Binding Energy (eV) 4, 5p 5, 1200 !OOO 800 600 Binding Energy (eV) 400 o 200 4f7n Binding Energy (eV) Compoulld Type T, T,S ToS, HaMes 21 22 • T,,o, Br6CT36CIn)(BILlNh Cr.cr..cI,>XE4Nh 23 2' 25 26 27 28 4fm =21.9 eV .1.= 1.91 eV --. -- 4fm 4f", " JLj_~_ _-~----'2::j-~--'~--~--:15 Bioding Energy (eV) I)crkill-Ebncr Corporation Physical Electronics Division ./ '" Thngsten Handbook of X-raj' Photoelectron Sptctroscopy W Atomic Number 74 Monochromated AI Ka NNN .1 1340 1310 Binding Energy (eV) 1280 NNN ''''' 4s 5s, 1400 1000 1200 800 600 200 400 o Bioding Energy (eV) Line Positions (eV) 4f7n = 31.4 eV 4f112 6=2.18eV Photoelectron Lines 4f., 's 594 4Pl12 '91 "'" 5s 75 5Plfl 41 5py> J7 .24 4dy> 4d", 256 2'3 .1., 4fm 13 31 Auger Lines .!'" V NsN61 Nl N4 N67N7 13~ 1307 101' 1087 45 15 Bioding Er.ergy (eV) " t1"\ 172 (AI) (Mg) W' Perkin-Elmer Corporation Ph)'sical ElectroniCs Dhrision Handbook of X-ray Photoelectron Spectroscopy Thngsten W Atomic Number 74 MgKa / NNN 4' NNN 1100 1050 4d,n Binding Energy (eV) 4dl/2 'Pl/2 4, 'PIn ~ J\ '--'\. ~ 1000 1200 600 800 400 o 200 Binding Energy (eV) 4fm Binding Energy (eV) Compound Type 31 32 33 34 35 36 37 4fm = 31.4 eV 38 4f712 A=2.18eV W we 4fSll WS, Halides WOC, Oxides Tungstate • • 'h,Wl\ a.W(E1,ph a,s,W(CO)](C>!ls) ""PWeCO. • • Perkin-Elmer Corporation Ph)'sical Electronics Division 5pl/2 " / II Binding Enc:rzy (eV) 25 m W 173" Rhenium Handbook or X-ray Photoelectron Spectroscopy Re Atomic Number 75 4fm Monochronlliled AI Ka NNN 4'", 1340 . 1310 881;Tl& Enqy (eV) 1280 NNN 1400 1200 1000 800 600 Binding Energy (eY) 400 o 200 Line Positions (eV) 41112 =40.3 eY lJ. = 2.43 eV Photoelectron Lines 4s 4PI12 625 518 4p)n 446 4dll2 4dstl 5$ 4f5(2 4fm 274 260 99 42 40 Allger Unes v 40 Binding Ene!Ey (eV) N>N6,N, N4N61N7 1122 1089 lJll9 1076 30 iY\ 174 (AI) (M,) Perkin-Elmer Corporation \jI Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Rhenium Re Atomic umber 7S Mg Kll 4fm NNN 4f", 1100 1050 NNN Binding EneTID' (eV) 4s 5s 1000 1200 800 600 Binding Energy (eV) Chemical State Database Compound Type 40 R, R<O, R<O, 41 • 42 K,..a. 43 • 45 • 46 47 200 4fm = 40.3 eV Ii = 2.43 eV o 4fm 4f", I CbReO(PhlP):l ChReN(PhlPh o,R«EtsPh C""~PM"Phh • ChRt(PMelPhh n~r fIi ChRc(PMe:2Ph).lttlrtS • CIReNiPMezPh4uallS 44 400 Perkin-Elmer Corporation Physical Electronics Division v "- ~ 5O.L~_~~-~-:::40---''''--''''---=~~30 Binding Energy (eV) (J) 175 Osmium Handbook or X·ra)' Photoelectron Spectroscopy Os Atomic Number 76 Monochromated Al Ka NNN 12911 . 1340 Binding Energy (eV) 5p 1400 1000 1200 800 600 Binding Energy (eV) 200 400 o Line Positions (eV) 4fm ; 50.7 eV 1J.=2.neV 4fm Pbotoclectroo Lines 4f5n 4, 658 4pw 548 4Pll2 471 5>* 41" 54 4rm 5p 51 44 89 4d3n 293 4d" 279 Auger Lines V \ OJ '" Binding F..llCIlY (eV) 5p N5N67 N7 N4N61N7 1326 1093 1078 J31l 40 'WilllalC if' 176 (AI) (M,) Ilerkin-Elmer Corporation \ j I Physical Electronics Division Handbook of X.ray Photoelectron Spectroscopy Osmium Os Atomic Number 76 4f712 MgKa 4fm NNN NNN 1110 11l8O Binding Energy (eV) 1050 4dJ12 5p 1000 1200 800 600 400 200 Binding Energy (eV) o 4fm Binding Energy (eV) Compound Type 50 51 52 53 4fm , 50.7 eV 4fm 54 1J.=2.72cV Os Oso, • K,Os~ K,OsBr6 K20SCI6 • OSC14(EIJPh OsClt(phPMC2h tfilns OsCl,(PhPMeVJ mer OSC!2(PhPMe,}l tr3ns Perkin-Elmer Corporation Physical Electronics Division • v 60 50 Binding Energy (eV) 40 177 Iridium Handbook of X-ray Photoelectron SpectroSCOlly Ir Atomic Number 77 Monochromated Al Kcr K. 4fm 7 NNN 4[5/1 \350 \290 1l2l1 Binding Encrgy (eV) 4d5/1 4d,n NNN 4PJn 4, \... 1400 1200 1000 4Plfl ~~ 800 600 Binding Energy (eV) " ~ 400 200 if\. 5p o Perkin-Elmer Corporation \j! Physical Electronics Division lfandbook of X·ray Photoelectron Spectroscopy Iridium Ir Atomic Number 77 4f712 MgKa NNN 41111 NNN . 1110 1060 Binding EDagy (eV) 4PII2 4, 5p lZoo 1000 BOO 600 Binding Energy (eV) 400 o ZOO 4f," Binding Energy (eV) Com(XlUnd Type 60 61 62 63 64 4f," = 60.9 eV 65 4f712 6=2.98eV Ir IrCb K2IrBr6 KJlrBr6 K2IJC16 K,lrC~ v (NH.»I~ (NH.lJ!~ KlrCI,NO K1n1CO)oCl. K,Ir,(COl<Cb Perkin-Elmer Corporation Physical Electronics Division \ " " Bindillg Enetu (eV) " m 'Ie' 179 Platinum ,. Handbook 01 X-ray Photoelectron Spectroscopy Pt Atomic Number 78 4f7ll Moncx:hromated AI Ka NNN l350 4f5J2 1300 Binding Energy (tV) 4<1512 NNN 4d1ll 4PlI2 A, 1400 HXX) 1200 800 600 200 400 o Binding Energy (eV) 41Jn = 71.2 eV Line Positions (eV) 41Jn A=3J3eV P~oelectron 41112 V 4s J25 4Pl12 (if) 4P311 520 4d)12 332 5s' 103 4fll2 14 4f712 71 5p 12 " Binding Energy (tV) " N.$N67N1 1114 N4N67Nl 1101 I~ 1317 (AI) (Mg) '''''''''' '" 180 4d", 315 Auger Lines \. Jj Lines W' Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Platinum Pt Atomic Number 78 r::::::: MgKa 4fm NNN 4f5f2 \ NNN 1OJ{) Binding Energy (eV) 1120 1ll6ll 4d", "'311 4P312 4, 4Pln ''.-- ~ 5p \ 1200 1000 800 600 Binding Energy (eV) 4fJn Binding Energy (eV) ComlXlund Type PI Pt$i Pt.2Si PtCI2 PtC]. Oxides Pt(OH)2 (IV) Halides ChP((PhlPh cis 7l 72 73 74 75 76 77 400 4f3l1 =71.2 eV 78 o 200 4fm !J.=3.33eV 4fsn •• • • \ bPt(MejPh cis bPt(MelPh (rans 85 15 65 Binding Energy (eV) Perkin-Elmer Corporation Physicall!:lectronics Division '01 Gold Handbook orx-ray Photoelectron Spectroscopy Au Atomic Number 79 4fm Monochromated AI Ka 4flll 4dsfl NNN 4dJ12 4p312 NNV 4, " 4Pln A /" 5p v... 1400 1200 800 600 Binding EneIgy (eV) 1000 41,. =84.0 eV o Line Positions (eV) 4fm !J.= 3.67 eV 200 400 Ptxltoclectron Lines 4111l 4, 4pln 4pl/2 76J 643 547 4dlfl 353 4d1ll 335 5,' 110 4f512 4f712 Spln 88 84 74 5plfl 57 AugCf Lines \, 100 9<l Biooing &erg)' (tV) N61O~5045 N,NoN67 [416 1183 1342 1109 1091 NsN61 V 1247 1014 (AI) (Mg) 80 'Ell'fIIale m 182 N<NoN61 1324 'lI Perkin.Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Gold Au Atomic Number 79 4fm MgKIl 41", NNN 4<1", 4dll2 NNV 41'>2 4PI12 4, A ~ 5p l-c 1000 1200 600 Binding Ene'tY (eV) 800 4fJn Binding Energy (eV) .Compound Type 83 Au AuSn AuSI\4 YbAu2 CIAuPhlP C1Aul!'bJPb ChAuPhlP (PhlP)AuNOl ClAu(P!lJAs) (-AuSPEl,s-l> 84 85 87 0 tJ. = 3.67 eV 4f", \ '00 if\. W 200 4fJn =84.0 eV 88 • •• • • (-AuCH2PEI2CH:rn l)erkin·Elmer COrj>oration Physical Electronics Division 86 400 90 Binding Ener!y (eV) 80 ,,, Mercury Hand,book of X-ray Photoelectron Spectroscopy Hg Atomic Number 80 4fm Hg in HgS l-J Monochromated AI Ko: NOO 4fll2 1380 1415 Binding Enagy (eV) 4dSf2 "'312 4plI2 I~v S , 4Pl12 4, " / c S 5d LA I J( 1400 1200 1000 800 600 Binding Energy (eV) 400 o 200 Line Positions (eV) 4fm 4fw = 101,0 eV Photoelectron Lines !'J=4.05eV 4f512 4s 805 4PIf2 'fill 105 4f712 682 \01 4p312 579 4d3fl 381 4dll2 361 5s' 125 5PIIl 85 5pll2 67 5d312 12 5d512 10 Auger Lines N704S045 V '15 184 105 Binding Energy (eV) 1412 1179 \ NsN70 1246 1013 N4 N60 1230 997 (AI) IMg) 95 *F.slimale if\. W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Mercury Hg Atomic Number 80 Hg in HgS 4[7/2 MgKa NOO 41", 1185 1165 Binding Energy (eV) 1145 S 4d,n 4dm 4pm NNV 4, S 4p1/2 C 5d 5p 1200 1000 800 600 400 200 0 Binding Energy (eV) 4fm Binding Energy (eV) Compound Type 99 100 101 4f712 4fm = 101.0 eV 102 L\ = 4,05 eV Hg 4f", Hgo.8C&12Te HgS Hgh HgBr1 HgCh HgF1 HgO Et2NCciH4HgOAc \ Hg(thiodibenzoylmeh (P~PI2Hg(SCN), Perkin-Elmer Corporation I'hysical Electronics Division 115 if\ \lI 105 Binding Energy (eV) 95 185 Thallium Handbook or X.ray. Photoelectron Spectroscopy TI Atomic Number 81 Monochromated Al Ko: NOO 41", 1400 1415 1385 Bindin& Energy (tV) 4dsa 4dll2 NNN 4Pln NMV 'PIa 45 Sd 0 Spin 1 5Pl12 1400 1000 1200 800 400 600 200 0 Binding Energy (eV) 4fm = 117.1 eV tJ.= 4.42 cy Line Positions (eV) 4fm Photoelectron Lines 4f", 4PlI2 4dll2 610 406 4d", 385 55' 133 4f712 5pln 95 5plI2 74 5dll2 IS Sd", 118 " 'PIn 847 no 4f", 122 13 Auger Lines U lJO 120 Binding Enttu (eV) "- N704so..s ..0.,0" 1401 1199 1166 1168 1008 ",".,0, 1m (AI) 989 (M,) 110 "Esti.lJe m 186 NsN,o, 1241 W Perkin-Elmer Corporation Physical Electronics Division Handbook of X~ray Photoelectron Spectroscopy Thallium TI Atomic Number 81 4f712 N()() Mg Ku 41", 1110 "65 1110 Binding Energy (eV) NNN 4<1", 44l/2 NNV 4Pl12 4, 4Pln 0 54 5p SOO 1000 1200 600 Binding Energy (eV) 41m Binding Energy (eV) Compound Type TI Til TIB, TIC1 TIP TI,s TIIS3 TI,o, . CbTl{pyridineh CI611z(PhPEtI)S 117 118 --- Perkin-Elmer Corporation Physical Electronics Division if\ '=II 119 400 200 41m =117.7 eV 120 li = 4.42 eV 0 4f712 41" \J no 120 Binding Energy (tV) 110 Lead Handbook of X-ray Photoelectron Spectroscopy Pb Atomic Number 82 Monochromaled Al Ka NOO 4fll2 13., 1<05 NOO 1375 Bjndin~ Energy (eV) 4d1l2 4dJl1 NNN 4"", NNV 4, 4Pln 5plI2 50 /5PJI1 1400 1200 1000 600 800 400 0 200 Binding Energy (eV) Line Positions (eV) 4rm 4f7n = 136.9 eV 1J.=4.86eV POOloelcdroo Lines 4fll2 4, 893 4pll2 4"", 644 4d)12 434 4d1l2 412 5s' 762 4f)12 142 4f1l2 Spin 5"", 107 84 5OJl1 21 5dl/2 1J7 ISO 18 Auger Lines U 150 1<0 Binding EntItY (eV) \. N7045 0 45 N6045045 1394 1J91 1158 1161 130 "Esti1lllle m 188 (All (Mg) W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spcttroscopy Lead Ph Atomic Number 82 00 MgKa NOO 4f", . 1110 NNN 1140 1155 Binding ElltID' (tV) 4<1", NNV 4<1312 4Pl12 4, 4Plf2 Sd Sp 1200 1000 800 400 600 200 0 Binding Energy (eV) 4fm Binding Energy (eV) ~C~om~poo~nd~T2ype~ _ _c.13~6 Pb PbT, PbSe Halides PbO PbA I'bO, Pb(OHn Pb(No,n 137 139 417n = 136.9 eV 140 A= 4.86 eV •• • m \M 4f7n 4f", •• PbSOl PbSO. Perkin-Elmer Corporation Physical Electronics Division 138 v 150 140 Bindill& F..nerty (tV) no Bismuth Handbook of X-ray Photoelectron Spectroscopy Bi Atomic Number 83 Monochromated AI Kn 4fm ) NOO 4f", 1390 1405 '1375 Binding Energy (eV) NOO 4d", 4dYl NNN ., NNV 4pYl 5d 4PII2 • Spin > 1400 1000 1200 800 600 400 o 200 Binding Eoergy (eV) 4f7fl Line Positions (eV) 4fm ; 157.0 eV 6=5.31 eV PIlotoeloctron Lines 4f", ., 4pl/2 4dy! 464 Is' 806 '''' 679 4d", 940 4Ml 161 'f", 4fm 5P1l2 162 157 119 5py! 93 5dYl 27 5d", 2' Auger Lines ...J 170 160 Billding EJJeTgy (eV) 190 N,o.,o., "- 1387 1154 150 N604S0 45 1383 (AI) 1150 (Mg) tE$limale m W Perkin-ELmer Corporation Physical Electronics Division Handbook of X-ray Photneletlron Spectroscnpy Bismuth Bi Atomic Number 83 41m Mg Ka NOO 41", NOO IISS ·1170 \140 Binding Energy (eV) NNN 44512 NNV 4pyz 4, 4Plf2 54 5p 1000 1200 800 400 600 200 0 Binding Energy (eV) 4fm Binding Energy (eV) Compound Type 156 157 ISS 159 160 161 4fm =157.0 eV 162 !J.=5.31eV Bi Bi2S) Bih BiF) 4f712 4f", Bi20J BiOCl NaBiCh BhMo06 BhTi107 (BiOhCr207 Bi,(SD.h· H,Q Perkin-Elmer Corporation Physical Electronics Division • '' 160 Binding Energy (tV) ISO '0' Thorium Handbook of X-ray Photoelectron Spectroscopy Th Atomic Number 90 Monochromated Al Ka. ,['" NOO 1415 14~ '<00 Binliog Energy (eV) NOO 4<l,n 'd312 'P312 4Pl12 5d", 5d312 AI 1400 1200 1000 4f7/2 4f", 6s6p 0 Photoelectroo Lines l/ 340 Binding Ene'!)' (eV) 'Pill 1170 'P312 4d1ll 4<l,n 4f1ll 4f7/2 1330 965 113 616 342 333 5s Spill 5P312 5d1ll 5d", 294 234 111 93 85 6s '2 6p,. 25 6p", 11 Auger Uncs N60n V N67045045 N70405 N67045 V 1419 1404 1335 1239 1186 1171 1'02 1006 (AI) (Mg) J25 -Estillllle m 192 \ / 200 400 ,,' ]55 5p Line Positions (eV) 4f,. = 333.2 eV A = 9.34 eV 800 600 Binding Ene~y (eV) 5, 'lI' Perkin.Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Thorium Th Atomic Number 90 MgKo NOV NOO "" 1200 Binding Energy (eV) 4d3J2 4dsn AT 1200 800 1000 600 Binding Energy (eV) 4fm Binding Energy (eV) ComJXlUnd Type Th ThO, -. 333 ThF, 334 3J6 335 400 'fm =333.2 eV 337 IJ.:=9.34eV 5s 5p o 200 4fm 4f512 • • 4d", Binding Encrgy (eV) Compound Type 675 67' ~ - Th 7,0, Perkin-Elmer Corporation Physical Electronics Division 676 if\ \II \ 315 340 325 Binding EoaJy (eV) ,., Uranium Handbook or X-ray Pholoeledron Spectroscopy U Atomic Number 92 Monochromated Al Ka 'fm NOV 1<00 BiOOing Energy (tV) 1430 1310 NOO 4dY2 ., .d312 'P312 0 5d~ ls C5Pu15py, 1400 1200 1000 800 600 400 200 5d", I 6s 6p 0 Binding Energy (eV) m 194 Perkin-Elmer CorporatiOi ' " Physical Electronics DivisiOl Handbook of X-ray Photoelectron Spectroscopy Uranium U Atomic Number 92 MgKn 4f", NOO -. NOO "'" 1140 Binding f.nefgy (eV) NOV jPlIl 1000 1200 800 600 Binding Energy (eV) 4fm Binding Energy (eV) eo"""""" Typ< 3n 378 379 380 381 382 400 4fm = 377.3 eV 383 6 = 10.89 eV U Tellurides o 200 4fm 4r '" Selenides Sulfides Halides lli;re, lliy Hal"" U(So.h U(aeoc~ \. CaU04 K2UF6 400 J8j 370 Binding Energy (eV) Perkin-Elmer Corporation Physical Electronies Division ([> 195 III. Appendix Appendix A. Auger Parameters The following Iables plot /he binding t:~'V of l~ mo51 illlt!1lSt phofotltclrtJfl liM WnrLS the kiMtic tntrg, of lht most inttrest Auger Irtmition. The Augtr fXJromtttr plOiS QIlIUt/ul for junher Sl!parotion ofthe chtmical stOIa 1344 662 Fluorine Compound Pis FKLL PbF, B>F, K}!'eF, NaF CdF, CuI', C,F, C,F, LaF, Zn F2 "'F, SmF) K,z,F, C>F, NdF, ThF, K21iF, Sd', NiF2 LiF btl', K2Ta fJ YF, N<l211F6 NaSnJ1 HIF, K2Nbry Na)A1F6 MgF, CaF N.,ad', N32S iF6 KSbF, NaBF~ NiOOCCF3 p-(Cr"l"CF,) 198 682.1 683.6 683.1 684.0 684.5 684.5 684.5 684.5 684.5 684.5 684.6 684.6 684.6 684.6 684.8 684.8 684.9 684.9 • 685.0 685.0 685.1 685.2 685.2 685.3 685.3 685.3 685.4 685.• 685.5 685.8 685.9 Ml.9 686.0 686.6 681.0 688.' 689.0 659.3 658.5 656.2 656.0 655.0 656.0 651.0 656.2 656.2 658.0 655.6 651.2 651.0 655.1 655.4 651.0 651.0 655.1 656.3 655.5 654.1 656.4 655.0 655.8 655.1 655.3 655.3 655.2 654.1 654.4 653.8 654.0 653.0 656.6 652.8 652.9 652.4 / 1/ i 1/ / r V I 1/ • 1/ V 1/ r 1/ ~ 1/ [Meta li 1/ I} II 1/ 1/ 1/ ~ I~ 1/ 1/ 1/ 1/ Ii 1/ 1/ 1/ 1/ 1/ 1/ > IlindiltEneltY(eVj KiRetJc&uvleVj ASF 1342 660 658 1340 \338 ~ • ~ I j 656 •• " ~ 654 I I 1336 I 1/ 1/ 1/ 1/ 1/ / 1/ CF 652 1/ / II '" 690 689 688 687 ." 686 685 684 683 682 68\ 680 Binding F..Iler&Y (tV) if\. Perkin·Elmer Corporation ' " Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Appendix A. Auger Parameters 1000 Sodium em-od Na2SeO) Na2Cil4 Nil2 Mo04 NaAs02 N.F Na:/OO. N:I)P04 NaH,PO, N"snOr 3H,o NaOAc NaP Na2S04 NaOOCCH2SH Na2SO:J N. N. Nail< NaNO:J Na,GO. NaCl Na,COJ Na2 HP0 4 Na2S20J N.ND, Na,Cr,o, N.I NaB, Na,Co, NaOAc N. NaCl NaCl Na20 Mol Sieve Y NaBF4 An rides , Na Is N. Kll Ilio&I &azr (eVI Kioeuc: FJqy (tV) 1070.8 1070.8 1070.9 1070.9 991.0 990.5 991.0 99o.J 1071.0 1071.0 1071.1 1071.1 1071.1 1071.1 1071.2 1071.2 1071.2 1071.3 1071.4 1071.4 '1071.4 1071.4 1071.4 10715 1071.5 I07l.S 1011.6 1071.6 1071.6 1071.7 1071.7 1071.7 1071.7 1071.8 1071.8 1072.5 1072.5 1072.6 1072.7 Perkin·Elmer Corporation Physical Electronics Division - 998.6 991.2 990.1 989.8 990.1 989.9 998.6 989.8 990A 990A 994.1 994.5 990.6 989.6 9912 990.1 989.8 989.1 990.1 989.8 990.6 998 / 996 994 99 V V /"" 2V 990 988 987.1 ~ Y V V V ./' 986L 1074 V ./' V ./' 991.2 990.6 9S9.8 9S9.9 994.1 990.1 990.0 989.8 981.8 V V V V V V V V II I V 2084 1072 ~ I a + ~ ~ V 2082 V V 2080 I Binding Energy (tV) > ~ I ,I" ./ V 'V l----< 1073 ~ I I V 2086 o I Vi V Is V , l--(' omc Compo nds" • V V 2088 1071 1070 ~ Appendix A. Auger Parameters Handbook or X-ray Photoelectron Spectroscopy 1395 Aluminum V 1394 Al2p ~ AI AlAs A1203, gamma A120), alpha AbO}, gamma Ai(OH)30 gibbsite AlzOJ, sapphire AIOOH, boehmile AI(OHh, hayerite A1203, gamma AI KLL &crzl'lcV) K-* "*'b' leV) n.8 73.6 73.7 73.9 74.0 74.0 742 74.2 74.2 V 1393 1393.3 1391,2 1387.8 1392 1388.2 1387.8 1387.4 1387.8 1387.6 74.3 1387.8 74.4 1389.0 Al:2SiOj, sillimanite 74.6 13&6.9 ~ ~ ••i ;; 1389 1388 ./ V- V /" V 1390 V./ VV V 1391 1387.7 AlN /" V ./ V- V V /' ./ V V V V 1387 1386 1385 75 V l-;) id~ .J V i? V- I ./ I V- /' V /" /' V /" V M V V /' ~i Ie A /" ? VV V V /" /" ./ V- VV- V V /" V /" V /" ~ /" /" /" V 1467 V 1466 V 1465 1464 V V /" /" V- :? V /" /" V V- V 1463 V 1462 V 1461 V /' V- '" 74 "" 73 72 BimJing Energy (cY) 200 m 'II Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Appendix A. Auger Parameters 1718 1618 Silicon Compound I Si 2p lWill& &qy (~V) s; MoSi:! PdSi Mol Sieve A Hydroxysodalite SiJN4 Mol Sieve X Natrolite Mica. muscovite Wollastooii, Capi:P9 jrMethylsiL (linear) LiAISi2~ spodumene NaAlSi30s. albite A1Si~ sillimanite , jrPhenylsil. (resin) Mol Sieve Y Pyrophyllite jrMelhylsi1. (resin) Kaolinite Talc, M&:jSi40"iOHh Si02, alpha cristobal HZeolon Si02, gel Si02,Vycor Si02 SiD:!, quartz 1716 , Metal ilie' Si (KLL) ,,-.: > c EMu leV) ~ ,• 1616 99.5 99.6 99.8 101.4 101.7 101.8 102.2 102.2 102.4 t02.4 102.4 1025 102.6 102.6 102.7 102.8 102.9 102.9 1010 lOll 103.3 1013 1014 103.5 1016 1017 1714 1616.6 ,~ , 1617.4 1610.0 1609.4 ~ 1614 1712 :; 1609.6 "t, 1609.2 .g l609j 1610.0 1608.7 1609.2 1608.8 1609.0 1608.9 1608.8 c w .' d 1612 1710 .•, ~ 1610 II 1608.4 1608.3 1608.5 1608.8 1608.6 I. 1608 " iL---=---1--....,IL::-.---+--t----t----1 1606 14-t-++f-+-t-H-++++-H-t++t+lH-+-H-t-H+l 104 103 102 101 Binding Energy (eV) Corporation 'IY\ Physical Electronics Division W ~ 3 1617.2 1610.1 1610.7 1612.6 1609.4 1609.6 1609.6 •• 100 99 98 Perkin~Elmer 201 ,~ ,m • ,~ Appendix A. Auger Parameters Handbook of X.ray Photoele<:lron Spe<:lrosOOp)' 2280 2118 Sulfur S 2116 Compouoo WS, NiS WS, Na2S03 Nlt2S 0 3 Nlt2S0J So, So, a,sO, SF, SF, S2p s..-, &aa:t '"' 162.1 162.2 163.0 165.6 . 166.6 167.2 167.4 168.1 1693 174.4 177.2 1/II 1/ 1/1/1/1/ 1/1/1/1/1/ 1/IIII I 1/ / 1/II71/ / / 1/1/1/ 1/ '/ / 1/1/ lLII ;;11/ IIII II II 2276 . S KIl. K-. &azy ~V) 2114 2115.6 2116.1 2115.6 2112 2108."5 21085 2108.5 21061 21061 2108.0 21005 21005 II~ / 2278 ~ > 2110 ~ , ~ •• .,, 2108 • " 2106 2104 2102 2100 2098 180 178 176 174 172 170 168 166 164 162 2274 2272 160 Binding Energy (tV) 202 m W Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Appendix A. Auger Parameters 921 1853 1852 r---,-,---,-,---,--'i-=---T-... 1851 Copper o,2p Compound o,LMM 920 B~ Enorl)' (eV) ki_ &laJ:J(eVJ Cu2MO)OlO Cu2Se CuAgSe CuSe o,S CuBr2 o"s CoC! C..cl 0.,0 0.,0 0.,0 a.,o 0, Ca c...zn" Ca Ca Ca CuCN o,ClCNlJ 0,0 o"M",o, CuMo04 CuCr204 CuSiO] c..co, Ca(OHh • 931.6 931.9 931.9 932.0 932.2 932.3 932.5 932.5 9325 932.5 932.5 932.5 932.5 932.6 932.6 932.6 932.6 932.6 932.7 914.5 935.1 OC" Cu(NO,h 935.2 CaSo, 935.5 935.5 Cal', Cal', CaF, 93H 936.8 937.0 Perkin-Elmer Corporation i'f\ Physical Electronics Division \j! 919 1849 • , ,• ~ , "m 917.4 914.5 918.1 916.6 916.6 918.0 915.2 916.3 916.2 9153 915.3 915.6 916.0 934.1 3 917.7 933.1 •, ~ 918.4 917.9 916.9 915.0 915.6 916.2 9161 916.6 9171 918.6 918.7 918.6 918.6 918.7 918.6 > c ~ •• 916.5 917.6 933.2 933.7 934.1 934.6 934.9 935.0 1850 > "~ , 918 1848 917 1847 c ., W • c 916 >! 915 I'-----f--f-----,l----f--f--I-:f----j---j 914 f'-----;/'---f--+-f--j'---+---j--t 913 R-r-t+i'+tt+f++tt-ft+++f+tt+t++ttt++++t++++l 938 937 936 935 934 933 932 931 930 Biming Energy (eV) 914.4 914.8 ••• ~ Appendix A. Auger Parameters Handbook of X·rny Photoelectron Spectroscopy 995 Zinc 994 Compound Zn 2p312 211 LM M Bm;" Entru (eV) Kllltllc l!nt:p (eV) 1021.4 1021.6 Zno 1021.75 In l()ll.!" In J()lI.!9 ZnClz 1021.9 Zn4siz07(OHn' 2Hj) 1021.96 z:,S J()l2 lnF, J()l2.2 lnO J()l2.5 lnF, J()l2.8 Znlz 1023 ZnBrz 1023.4 Zn(acacn Cu#nl6 993 981.7 I m.7 9885 m.1 m.1 989.4 981.3 989.7 986.2 981.7 986.7 988.7 981.3 992 99 I ~ j ., ~ " / 990 989 V / 8/ 98 987 / V / / / / V / / 1/ / 6/ 985~ " V / 1/ 1024 V 1/ 1/ V V V 1/ 1/ 1/ 1/ V V V / I V/ 98 1025 / ~ 1/ V V I / V 1023 V V V V / y Oxi 1/ / 1/ V Vlalide ,1/ V 1022 / V / / V 2014 2013 2012 2011 2010 2009 V 2008 V / 1021 1020 Binding Energy (cV) 204 m. W Perkin-Elmer CoqJoration Physical Electronics Division Handbook of X-ray Photoelectron SpectroscopJ' Appendix A. Auger Parameters 1228 1268 1226 1266 Arsenic Compoond As 3d As l.MM ~intF.nau (eV) Kindic '*'" NbAs GaAs 40.8 40.8 1226.0 1225.3 As 41.6 42.8 1224.8 1221.1 1222.3 Ph3As AS2Sc3 Asl) MeAsI2 Pb)AsS N.M>, Pls,AsO "'fiJ As&, NaH1AsO. "'fiJ KAsF, 42.9 43.5 43.5 44.1 44.2 44.3 44.9 45.3 455 46.2 48.0 (eVI 12195 1217.1 1217.5 1213.8 5 1264 I, 1222 1262 • •m • ~ ,• ", 1220 ,;;" 1260 1224 ~ § '> 0 0 ·is 0 ;l 1218 1216 V---¥------l----,V--*--+--+ 1214 V--+-----;j'~__c;ojL--+--+--+ 1212 I't-t+t-¥-r-H-t-f'+-+++-t+t+t-I--t-+l-+-f+-+-t-t-+ 52 so 48 46 44 42 40 Biooing t.:rzy (eV) Perkin-Elmer Corporation Phv<:i('~II?IM'Irt\n;M: ni"i~i .... n iI"\. u.J •, ~ 1222.9 12223 1220.0 12195 1218.8 1218.1 • ~ Appendix A. Auger J)arameters Handbook of X-ray Photoelectron Spectroscopy 1310 / Selenium Compound Se Se Ph2Se Pb,Se, I'h,SeO Cl2SePh2 12SePh 2 SeO, N"sea, H,SeO) H,SeO, Sc 3d ScLMM 1IiIIdiII&&oIv1ev} KiltticEtlcrs7(eV) 55.1 55.5 55.8 55.8 57.6 57.7 58.1 58.9 59.1 59.2 61.2 / 1308 1306 1301.9 1302.9 1302.1 1301.4 1301.2 ,- 1JOI).8 1297.9 ~, w "-, 1304 0 ·il, ;;; 1302 / , > ~ V / / / V V V Metal 1306.7 1307.0 1304.0. 1304.3 1364 1362 ~ "3 •• ,•• ,~ 1360 ,m 0 , " 1/ / V V V 1/ 1/ 1/ 1/ / 1/ V V 1/ 1/ 1/ V V 1358 • I Oxide 1300 1298 / 1296 / 62 • / 61 / 60 59 58 57 56 55 54 Binding Energy (tV) ?or. m W l)erkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Appendix A. Auger Parameters 360 Silver Metal Comp.,.,d AgF2 AgO AgF CuAgSe Ag,5o Ag,O A&2 S04 A~ A'IfJ A",S Ag Ag MgzlAg19 Ag,SO, A:f) M&JoA&so A""'88l Mg97Ag) AgOOCCF, A"jAg, Ag 3d Ag MNN ~&azy(eV' K___ !iazJleVI 367.3 367.4 367.7 367.8 367.8 367.8 367.8 368.0 368.0 368.1 368.2 368.2 368.3 368.3 368.4 368.7 368.8 368.8 368.8 369.0 349.6 355.5 349.3 351.3 351.4 356.6 354.2 350.1 350.6 351.2 358.2 357.9 352.1 354.7 350.6 351.9 351.7 3521 355.1 351.5 I 358 356 V ./ > ~ > ~ •, 354 w • 'is /' V , " 35 2/ / V ./ V 348 / 370 V V V /' ./ I I I I V /' V V ./ V /' I I I V Alloys V V y V V V I I• V 35 0 . / ./ /' V V I F1 u 726 V /' 724 / 722 V 720 / ' 718 rides I , 369 3611 367 366 Binding EneltY (tV) Perkin-Elmer Corporation Physical Electronics Division ?"? Appendix A. Auger Parameters Ha~dbook of X-ray Photoeledron Spectroscopy 386 Cadmium 385 f--+--+--+---"jL--,jL--~ Compound Cd 3~,V2 Cd MNN Kjodillg FJI<IV (eV) Ki. Eneru(eVj orr, Cd CdO CdS, CdS Cd!, CdI', 404.9 405.0 405.2 405.3 . 405.3 405.4 405.9 787 384 3814 383.8 382.2 383 381.. 381.1 381.0 382 378.8 ;;- ",t w .",, 381 > 380 ~ 379 I A ri e 378 m 376 375 408 407 406 405 404 403 402 Binding Energy (eV) 208 m Perkin-Elmer Corporation \jI Ph)'sical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Appendix A. Auger Parameters 856 412 854 Indium I Compound In 3d5J2 Binding Eo.~ (eV) 1095SnS I, JnSb 1020 3 hl,Te) luP I,P In,Se3 In,S) In(OH)] (NH4hlnF6 In!) hlBr] loCi] InF] InBr] 4436 4438 444.1 4443 444.5 444.6 444.6 444.8 444.8 Ki~li<: EntllY (eV) 408.3 4073 404.1 4058 404.8 404.6 403.1 404.8 . 446.6 ",, ,,•" I I Oxides 3 408 850 ,~ , ;; ", " m > 0 w 406 848 Halides .~ • 0 ;l 404 846 402 iL--+----,f"--+------+"--l---j 400 fLH-++-i+++-t-f'i-++-++++-t-HH-t-++++++t-I 448 447 446 445 444 443 442 Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division •• , • 411.0 445.6 446.4 852 > 0 401.6 406A 408.9 408.0 405.0 446.0 446.0 410 410.5 410.4 445.0 446.0 Metal InMNN 209 ~ Appendix A. Auger Parameters Handbook of X-ray Photoelectron Spectroscopy 440 Tin 439 Compound Sn Jdyz Sn MNN Binding 1::Io'D' (eV) Kinelic: So So So 485.0 SOS 485.6 . No,SoD, SoD, Na2Sn03 Na2SnOJ NaSnf) 486.2 484.9 485.1 486.7 486.7 481.2 481.4 ~ 437.4 437.4 437.4 435.7 431.7 432.7 431.1 431.7 430.8 1/ leV) 438 V V 1/ V V V / / 1/ l/'; 437 436 V V Mel~ V ~ V / 1/ / j 435 / / ., V V V i 1/ / 1/ 434 1/ V V V V / / 1/ 433 1/ V V ~ 1/ 1/ 432 1/ Vf Vi ~ 923 922 921 920 I ~ m 919 918 I I 431 / L 430 488 / / 487 486 485 " 484 Binding Energy (tV) 210 m 'lI ,> I ,! • l, 0\ Perkin-Elmer Corporation l)hysical Electronics Division ~ Handbook of X-ray Photoelectron Spectroscopy Appendix A. Auger Parameters 484 483 fL--.,IL---*--+'-------o¥--+----I 14--f-H-!4++-t+'f-H-+-f'+-+++t+!-H+t++t-+ 518 511 516 515 514 513 512 Binding Energy (eV) Perkin-Elmer Corporation Physical Electronics Division 211 Appendix B. Chemical States Tables . 11lis compilMioll of all Ihe elemtll/s, listed (llphaM/ical/y, provides specific binding energies of various compol/llds wId pl41't elements, alld a reference in abo breviated IIQ/ulioll. When Auger lines art listed, they are in k.ine/it tlU?rgy. For compounds with mort than ont chemical stalt, (Ill asterisk dtllotts rhe QlOm whose binding energy if listed. The rtftrtnces ort upandtd in Appendix C. An] listing with 0 ¢l refers /0 the wort cOnIaintd in this handbook. This apptndiJ:, most of which was compiled by Dr. Chtlrlu Wagner for Pt,*in-~r, is part if 1M d1emical $Ia~ itklllijiC1Jtioo algori/hIIl c{ the PHI Mftwart and is also lire basis for 1M XPS dalabast SRD·20 of lire NlJIionaf Ins/ilUle for Standards and Technology (NISI) Further reftrtnus may also be found in Iht journal Surface Science Spectra published by Ihe American Vacuum Society. AgJd Ag Ag Ag Ag A, A, Ag A, A, AgtsSns A""'.. Alw\~ M!2IAgl9 """'.. "g"A~ Ag:Yb CuAgSo Ag,& Ag,S Agi AgF Ag~ Ag,Q Ag,Q ApfJ ApfJ AgJOOl AgISO. AglSO. AgOOCCF) Ag(OAc) Ag(J.O.pyri<iohNo, Ag,& 368.3 368.2 368.2 368.1 368.2 368.2 368.2 368.2 368.2 368.0 368.' 369.0 368.3 368.1 368.' 368., 361.8 367.8 368.1 368.0 <I> At-~ """'16 BiSwSO BiSw80 BiSwSO nlBK73 .NyMaSO HOMS, Schon. WRDM79, Agi A,F 351.4 35L2 JlO.I 349.3 Ag~ 349.6 A,,o A,,o A,O AgO Ag,SO. Ag,SO. AgOOCCFJ 356.6 350.6 GaWi17, SFS71. Waga15 RRD18, Scho72 HSBSSI WeAn80 WeAn80 WeAn80 Al AlA. sapphire Al RRO" AlB} AIM WWCl1l 367.7 Gawm 367.3 367.8 368.' 361.4 368.0 367.5 367.8 368.3 368.' 368.' 368.6 Gawm 357.9 WRDM79 Wagn75 RRD 78, PWA 79 GaWi11 HGW75, GaWi77, Scho73 RRO" HGW75. GaWiTI. Sfbo13 WRDM79 HOW7S TMR80 Wagn7S Wago15 HHODSI SmWt77 Ag MNN Ag Ag Ag A, Ag A~Ag. 358.2 351.9 35\.6 "'.3 """", Mg9JA&l 351.7 351.5 352.1 351.9 352.2 CuAgS< 351.3 AIJ.&$ Mg11Agl' Perkin-Elmer Corporation Physical Electronics Division Al~s r'eJAI LiAu-t. AIN A!,S, All, AlB!] Ala, A1Fl AI2(MoO.)J Ah(W<hl) CoAJ,O, "gAlA NiAhOo AI"" AllOJ AI~Ol, sapphire Aho;' alplla Aho;' pmma AIApmma Schon. FKWFn AI~pmallI W<A"' " WeAo80 AIOtH, boehmite Al(OH»), bayerite AI(OH)), gibbsile W,,"'" WeAnS(} WeAnSO RRO" 354.2 "'.1 355.1 AI2p w,,"'" W,,"" RR07l RRD18 GaWm 355.5 350.6 AI1Si05> kyanile AI~iO" mullite AI~iOs, sillimanile AIbtte. NaAlSiJOa 72.9 14.4 12' RRD78 RRD7S Gowm Gowm GaWi71 Scho73 RRD78, GaWm WRDM79 GaWi17 Wagn1S TMRW WIgn1S • <I> 11.9 LMKJ7S. Tayl82, WPHK82. WRDM79, WtTaBO MOCC1J 136 73.6 Tayl82 Tayl82 73.4 ShTr75 MSC13 MSC1J MSC1J MSC1J MSC1J MSC13 MSC13 PCLH76 75.6 14.4 14.6 74.6 75.2 14.7 76.3 74.2 74.3 13.6 14.1 74.2 74.3 74.7 74.2 719 717 74.0 70 74.2 74.2 74.0 14.7 14.8 14.6 14.3 NgHc76 PCLH76 HNUW18 LFWS79, NgHe76 Nefe82, MSC13, NSLS71 KlIle83, t..'GDS7S Tay182, WPHK82 WPHK82 WP!-IK82 B..., NgHe76 Tayl82. WPHK82 Tay182, WPHK82 WPHK82 AnSw74 AnSw14 AnSw74, WPHK81 WPHK82 1.11 Appendix 8. Chemical States Tables Bentooite Kaolinite Mica, muscoyite Nalrolitc Pyrott!yUile """'- II """"" HydftUysOOalite Mol SicyeA A~aca:)J Handbook or X-ray PholoeJedron Spectroscopy 75.0 74.6 74.3 74.3 74.7 74.3 74.8 75.0 73.6 Ban!3. WPHK82 WPlIK&2 WPllK82 WPHK82 WPlIK82 WP'rlK82 WPIlK82 WPHK82, BarrS3 ",,s, ",,s, 72' "S03 KH2AsO. NaH)I\sO. NWO, ""'" AIKLL Al AlAs A'N AbOl, sapphire AhOJ.a~ AI,<>,. ,,,"'''' AlOOH AI(OHh, bayerite A~OH)}, gibbsite AhSiOj, sillimanite Abite, NaAISiA KlOIinite Mica, IT\USCOYite Nalrolite Pyro~ymle Spodumeoe II """"" Hydroxysoda61e Mol Sieye I I Ar2p AI inSi AI inA& ArinAg Ar inAu ArinAu AI in Cu AI ia PI AIintraphite Ar in graphile 1393.3 1391.2 1389.0 1387:8 1]88.2 1]87.8 1387.6 1387.7 1]87.4 1386.9 1386.5 1386.7 1387.1 1386.5 1386.8 1387.1 1l8S.5 1386.4 1386,9 241.9 241.2 241.9 240.3 240.7 241.1 240,4 241.8 241.5 WP'rlK82, WaTaSO Tayl82 TaRa81 Tay182. WPHK82 WPlIK82 WPHK82 WF'tIK82, Tay182 WPHK82, Tayl82 WPtlK82 WPHK82 WF'tIK82 WPHK82 WPHK82 WPHK82 WPHK82 WPHK82 wm"" WPHK82 WI'HK82 • CiHa74 KiWi75 CiHa74 KiWi75 CiHI74 Ki't'!'i.75 KiWi75 WRDM79 "'"" '" "'' .., AsBr} "'''' "'''' K""'" N.""", N34AstO! '"'" NbAs A'''' AlGoA. OW OW lnAs AS~l 214 41.6 4\.6 • Bert8I, BWWI76. MINN7&, SMAYn, UeOd8I 40.8 41.0 41.0 "'40.'.. 40.6 42.9 BWWI76 Tayl82 Tay182 LPMK74 GGVL79. WRDM79. Tayl82, MINN78. IMNN79 LPMK74 BWWI16,1JeOj82 46.7 45.5 44.2 44.' 44.' 45.4 KAsF. .<0 LiliF. 49.4 """, "",IuS "",,;'" 1'h,lAs{OHh MeAsl) """" I'l4IuB, ". 44.1 44.3 44.5 435 44.6 44.6 BWwn6 RWW176 SMAV12 BWW176 BWWI76 LPGC77, MINN78. Tayl82, WRDM79 Ben81, BWWI76, MINN78, SMAV72 SMAV72 WRDM79 T2)'I82, WRDM79 SMAV72 SMAV12 SMAV12 SMAV72, WRDM79 SMAV72 HVV79. SMAvn BWWl76. HVV79 BWWl76, SMAV12. HVV79 SMAV72 BWWI76 IIVV79 HVV79. SMAYn AsLMM '" NbA. OW As2Tel "'' ' AS2SJ Ash "'B" "'''' "'''' NaHIAsO. NaAsOl K1AsF, """" "",IuS ""MeAsh A,3d 43.4 44.' 43.5 45.3 44.' 1224,8 1226.0 1225.] 1225.0 [223.] 12221 1222.9 1218.1 121&.8 1217.5 [217.1 1219.5 1213.8 1221.1 1220.0 1219.5 12213 Au4f ""A. A. A. A. A. A. AoS, AuS", YbAul OAuPh,p 84.0 84.1 840 84.0 83.' 84.' 84.2 84.' 85.1 846 85" m. Wagn75, BWWI76 BWW176 T2)'I82, WROM79 BWWl76 .WWI76 BWWI76 BWW176 BWW176 Tlyl82, WRDM79, BWWl76 BWWI76 WRDM79 Tay182, WRDM79 WRDM79 BWWI76 BWW176 BWWl76 BWWl76 • Asam16 BiSwSO BiSw80 BiSwSO PEl" ALM"" FIIPW7J FIIPW7:l WWC78 BMCKn, VVSW77 Perkin-Elmer Corporation \ j ! Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy C1AlI(PhJ1'h 85.4 BMCK71 CbAlII'hlP (Ph)f')AlINOl C1AlI(PhlAs) (·AuSPEI1S·h (·AuCHlPEtjCHl-n 87.3 85.4 85.2 84.8 84.0 BMCK71 BMCK71 VVSW77 VVSW77 VVSW77 AuMNN A" A" A" 2015.8 2101.6 2015.7 rEm WaTa80 WaTa80 B Is B B B.C AlBl C",B CoB FelB FoB HfB, MnB 2 M02Bj MoB 2 TiBl VB, WjB j CrBl BN Na1806 B,o, B10) NaBF. NF4BP~ NaBH. H)BO) NaJB.Or . IOH l O BlOH I4 Me.NBlHI NaB~ NH)BFJ CsH~BF) EtNH1BF) McJNRFl NaBH(OMe)) PhIS!') Ph)POBF) PhlOBCb PhJPBCh CH)CNBf) CIC.H~B(OHh FCJl.B(OHh (EI)PhI'tBloH Il (PhJPhI'tB1oH 11 189.4 187.3 186.5 188.5 189.1 188.1 188.4 187.9 188.3 187.2 187.7 188.4 187.5 188.3 187.9 188.0 190.5 192.0 192.0 193.3 194.9 195.2 187.2 193.0 192.6 187.8 187.2 187.5 194.9 194.3 194.6 193.6 192,1 193.3 193.8 192,6 192.7 195.5 191.7 191.7 188.9 188.5 Perkin-Elmer Corporation Phvsical Electronics Division " HHJ70 HHJ70 MECC73 MECC73 MECC73 MECC73 MECC73 MECC73 MECC73 BrWh78 MECC73 MECC13 MECC73 MECC73 MECC73 HJGN70, KOK83, WRDM79 HHJ70 BrWh78 NGDS75 HHJ70, RNS73 RNS73 HHJ70 HHJ70 HHJ70 HHJ70 Hm70 HHJ70 BCGH73 BCGH73 BCGII73 Hm70 HflJ70 HHJ70 HHJ70 HHJ70 HHJ70 BCOH73 HHJ70 HHJ70 Rigg72 Rigg72 Appendix B. Chemical States Tables Ba 3d512 B. B. BaS BaD B,O BaD Ba(NOJh BaCOl BaSO~ BaS04 BaSO. BaCrO. BaMoO. BaRhJO. 780.6 779.3 779.8 779.9 779.6 779.1 780,7 779.9 780.8 780.4 779.9 778.9 779.1 779.6 VaVe80 SiWo8O WRDM79 SiWoBO VaVe80 CLSW83 CLSW83 Wagn77 CLSW83 SiW080 ACHT/3 NFS82 NFS82 602.B 597.5 598.4 596,1 VaVc80 WRDM79 VaVe80 Wago77 111.8 111.7 113.8 113.7 113.8 115.3 116.1 115.3 114.7 $ HJGN70, SMKM77, WRDM79 HJGN70, KOK83, NFS82 NFS82 NFS82 NKBP73 HJGN70 NKBP73 NKBP73 157.0 156.9 157.0 157.0 158.9 159.3 160.8 158.8 159.3 159,8 159.9 159.1 158.3 159.7 159.6 161.2 SFS77 LKMP73 WRDM79, MSV73 MSV73 MSV73 MSV73 NGDS75 MSV73 DSBG82 MSV73 MSV73 MaWo75 MSV73 MSV73 MSV73 $ Ba MNN B. B>O B.O BaSO. Be Is Bo Bo BoO BeMo04 BeRh1O. Bop, Bop, NaBeP) Na1BeF. Hi 4r B; B; B; B; BilS j Bih BiPj BhO) BhOj Bi 2O) BiOCI NaBiO) Bi 2Mo<\ Bh1hOr (RiOnerlOr Bi 2(S04h' H2O $ Br 3d KB' CsBr CsBr 68.8 68.1 69.6 $ MVS73 Shlq78 '" Appendix B. Chcmical States Tables RbBr KB' NaBr Lin, CdBr! CuBrz HgBl) PbBl) ""n,, Co(NH1)pbBr6 Ni(NHJk,Brl Pt(NHl)..Brl KIP1Br. K1Pl:Br. Cs~ln8r. RbJSblBr. Bromanil Pl4AsBr PhiSbBr ~NhZnBc. (E4NhMnBr. (EllNhNiBrl HY'OBBr) H)!'BBI) BnPt(CHJCONH). BI'LMM LiBr NoB' KB' KB.o, C~HJ1McJNBr 68.' 68.8 68.8 "'1 "'.2 68.9 69.0 68.1 10.0 68.9 68.1 68.4 693 69.2 '0.1 10.1 70.1 661 68.0 67.8 67.9 68.9 69.3 "'68.1., 1389.2 1"'3 13&8.0 1384,4 1390.1 CI4 Gnptile Gllphile CrlC1 F,,c Hie Mo,C NbC NilC r.e ToC VC WC z,c 28,. 2812 1818 KCN 281.1 286.1 N.eN "., K,e.,(CN), K,caiCNJ. K)r-e(CN;r. I(,""CN, KJMn(CNli 285.9 283.9 283.9 283.5 284.0 284.0 285.5 N"""CNJ. K.V{CN~ 216 2845 284.3 282.8 283.9 2808 2811 281.9 283.9 281.9 Handbook of X-ray Photoelectron Spectroscopy MVsn MVS73, WaTa80 MVS73, Shlq78 MVS13 SAT073 VWIISSI SAT073 Nefe82 SATD73 Tric74 NZB78 SNMK78 SNMK78 SNMK78 Tric74 Tric74 OYK74 HVV19 HVV19 EMGK74 EMGK74 EMGK74 HVV79 HVV19 NeSa78 .....,. Wagn78 WaTaSO Wagn73 Wagn78 • JHBK73 RHJF69 SbTr75 RHlF69 RlUF69 RHlF69 SiLe78 RIIJF69 RHJF69,IKlM73 RHJF69 RHJF69, CoRa76 RmF69 Vann76 Vann76 Vano76 Vann76, ZeHa71 Vann76, ZelIa71 Vann76 Vann76 Vann76 Vann76 Cr(COJ. 281.9 Co(CO))NO 288.2 ""CO, Fc(COb(NOh ,,<0 288.2 MniCO)11 Ni(CO)4 "7> 288.2 (M~CO)IBth 287.6 288.0 288.' 289.4 289.6 289.3 289.8 289.' 29Q0 289,5 287.0 291.9 29>4 293.9 296.7 285.2 2841 2841 285.1 285.0 2845 284.' BrMn(COh A"co, o.co, CaCOl CdCQl LiiXl) N.,co, NaHCOl S<CO, 05, co, co. COF, CF, Cyclohexaoe .""'" """'"II, 4!lsOh (c;.CH}) ~HICH) (C-·H) Pe(CsHln en""", CHJC%OH CHJCOO(.'4'H~h CoF, Inositol H~illOJle (C-HCOHh (CHCtOHh (CH)C%hO HCHO (CH)C-uOh C!!,C'OCl1, "'" "". "'" 2669 289.5 286.7 284.8 286.5 287.7 281.' 281.9 CFJCtQCth 28., C"FlCOCHl 292,6 288.3 289.3 288.2 28&.8 288.3 289.9 289.0 29Q. 2929 289.5 288.3 2921 288.9 281.4 (co. rn,c'OOH CHJC400Na CH~a CHlC'OOAg HOOCCOOH (COONah Cf,C'OOO C'F,CQ()EI CI)C·COONa CllCC'OONa FJC"COONa FJX:-QONa p-Benzoquinone m \Jl BCGHn, BC!l~1n, K1WY76, PF073 BCGH72 BCGHn BCGHn VWVBn BCGH72 VWVBn VWVBn HGW75 u.s"" CLSW83 HGW75 O5FG19 GHHL70. HHDDSI GHHL70 CLSW83 GHHL70 GHHL70 GIIHL70 GHHL70 GHHL10 GHHL70 GHHL7O, LaFo76, CKAMn CKM7I CKM11 CKM11 BCDII73 KTWY7' GHHL70 GHHL70 CKAMn GHHL70 OYK74 GHHL70 GHHL70 GHHL70, ClTh78 GHHL70 GHHL70 GHHL70 GHHL70 GHHL70 GHIlL70 GIIHL70 HHDDSI GHHL70 HHDD81 GHlIL70 GHHL70 GIIHL70 GIIHL70 GHIIL70 GIUlL70 GIlHL70 GHIIL70 OYK74 I)crkin-Elmcl' Corporation Physical Electronics Division Handbook or X-ray Photoelectron Spectroscopy O(""h CHCHtOCOCl E1OC'oa (PhOhCO HC'(OCH,h HCOONH.e OC'(OCH,h O(C'HJC(K)Hh O(cn~'OOUh CHJC'H~I CBIB!"! CHICb HCF) HCeh C6111CI (C'Cl) C6HJC1(C'U) C6II,Br C6HsF(C'F) C6HsF(C'II) c.Ha, C6HFslC'H) C.HFslC'f) "'" ChIUl'(l, C1JiC'(R], C'IIJCN CH""N CHJCONIIl E>NH, EtNli]BF, PhNH, ONHilia (CHl~' CsHsN PhCN C'HJCNBFl CHlC'NBFl TriaUJIe NC'N:C(NH,n NCN=C'(NHlh HINCHJC'OONa HlNCONHl H2NCSN~h H2NCQNHCONHl PhNo, I'hJ' ",po I'hJ'B< ""', ~CH~) ~CH~) ~HOCOCH<CHu ~No<lCOCMo<:Hu P(CtHJX.'OCIl=Old p(CHJOC'OCH=CH1) p(MeOCOCMe=CHv 286.0 287.' 290., 290.1 289.1 2884 2911 ZtHa1l GHHI.10 GHHL10 ClTh18 GHHL10 GHHL10 GHHL10 GHHL10 GHHL10 GHHL10 GHlIL10 GHHL10 GflllL10 GmU,10 CKM7l CKM71 l..IFo16 CKM71 CKM71 CKAM15 CKAMn "'" 289.5 "'281.1" 281.8 294.1 289.6 281.1 285.7 285.1 287.8 285.6 "'"'"" clWln 289.2 2881 291.7 GHIII.10 GHHL10 GIIIIL10 BOOH1] BOOH1] SNMK18 BOOH73, GIIHL70 8001173 UFo16 LtR.17 GIIHL70 BCGII13 Lar'076 BCGH13 BCGII73 GmlL70 LtRan LtRa17 GHHL10 GHHL70, LeRa77 teRa77, Srwan YYS78 LaFo16 "'-, 2B6J 2871 288.4 285.6 "'" 284.6 289.4 286.9 285.5 285.4 287.3 289.1 286.3 286.4 288.2 287.9 28&.1 2880 289.3 285.3 284.' 284.6 285.4 284.6 286J 286J 289.0 288' 286.4 288.6 289.0 Perkin-Elmer Corporation Ph\'.~i{,:ll Ji:1P.f'.tmnir<;: Oivi.<;:inn LMfOl LMfOl LMF80. LaFo16 BAlS76 PRcm PRcm HIIDDSI HI/DDS! ClTh18 ClTh18 HHDDSI if'\. W Appendix B. Chemical Stales Tables PVA ('(H£*HOH-)n "''''"'' !'EO (<:H,coli,<>. poly (<:H"",va.. CoH.lC'OOHh II~(CH!)£*OOH SociUIll Siearale Mylar PoIytSltt C'-H Mylar PoIytSlef C;--O MylM Polyeslef ~ PoIycarnooate-OCtDtTellon {-CF£F:!-)n (-C'FHCF!")n (-CA-lC'F!")n (-CHICFH.)n (-C%CF!") (-ClhC'Fr)n (.C%CFH-)n (-CHp'FH-)n PVC (.('HICHCI-) PVC (.(II£*IICI-) Ca 2p C. e.co, C. C. CallI c.s "'" c.a, C.~ 28., 286.2 "'" 281.4 288.' 288.9 28ll 284.85 2803 288.1 290.4 292.2 289.3 .291.6 288.4 286.3 290.8 285.9 2880 284.9 28., .. "6J " 345.9 346.8 ,,6.2 345.9 "., "8J 347.8 PRcvn COW81 COWSI COW8! COWSI COWSI COWSI JFM COW8l COW8] roW8l CFK13 CFK13 CFK13 CFK73 CFK73 CFK73 CFK13 CFK" PRcvn PRcvn $ $ V,VdIO SMKM77 FMUK77 FMUK77 FMUKl1 W""TI "., Wagn17, NSLS71 lnYa81 FMUKl1 VaVeSO Wagn77. CLSW83, WRDM19 CLSW83 ACHT73 NFS82 NFS82 CLSW83 Nefe82 WPHK82 V,V,", V,V,", c.~ 2982 292J 291.9 291.9 289.1 Cd 3d512 Cd Cd 405.1 405.0 C.O C.O C.O CaCOl Ca(NOln CaCrO. CaMoO. CaRhA C.so. CaW(h c.~;,o, CaLMM C. c.o e.co, c.a, C""". 346.1 341.3 346.9 348.1 346.3 341.2 345.7 348.0 3465 341.0 404.' WRDM19. Wagn77 WopTl WopTl $ GaWi17, HSBSSI,WRDM19. Wagn15 HSBSSI Appendix B. Chemical States Tables BgUCdo.lTe 00, CdS' CdS Cdb CdBrt CdCh CdF, CdO CdC, Cd(Ofib CdCO, CdRht04 CdMNN Cd 404.6 404,9 405.3 "".3 Handbook of X·ray Photoelectron Spectroscopy SBBSO SBB80. GaWi77 GaWi77 G:4Wi77 ""., ""-0 SATDn 406.1 405.9 40\.2 '03.6 "".0 405,1 404.7 SATD73 GaWi77,SATD13, Wagnn Gawm, NODS75, NFS82. SBB80 HGW15 WRDM79. HGW75 HOW75 NFS82 383.8 WRDM79, Wagn75, GaWi77 GaWi77 GaWiTI GaWiTI GaWiTI GaWi77 GaWi77 QaWin K1Re(\ KlR~ KJSnt\ KlWa. K""" KlRhC16 ~MOlCII Na,PdC4 Co(NHl>.sllO. P(NH,),CI, Pl(NHl)cCb Pt(NH)~C1l Rh(NH)ACll C"Sb,CI, c.sbC1o 00, CdS< CdS 381' 381.4 381.1 381.0 378.8 3812 Cdb CdF, CdO c<3d '"'" <>A" "'I'd, CoSo """"', "'0, 00, C<H, 883.8 883.9 883.5 884.3 884.3 883.6 881.8 881' 88M • &0.82 WBCgo ll'BCiO Il'BC8O I.FBCSO WRDM79 NODS75. SaRalll S<o.82 KlrCl,NO '0 UCla. KOo, KOO. uoo. NaCIO. Ni(NHJ>.(CI01h Nielo. . 6Ht<) RbCIo. "'-NO "'NO I'I4NO N14a """"""'" Panachlaobenzene ORh(phJPh (El)PlJPtHCI (I'tIJPnPLHCl trans (B,P),""" CI2p KCI = KO N.a Liel RbCl Cue!! NO, PdCl, RbCJ, RhCll' """, z,a, 12H~ "'' ' ' KlM0C!6 Kl0sC~ "'PdCh kPlCk "'PlCIo 198.5 196.l 198.2 198.' 198.5 197.9 2000 199.4 198.' 199.3 199.2 199.7 1985 198.6 [98.4 198.6 198.8 198.8 198.8 • MVS73 MVS73,NSLS77, YYS78 MVS73,NSLSn, SGS07Q MVS73,CSFG79 MVS73 VWHSSI KJHe83, TRLI<73, YYS 78 NKBP73 01"'" CMllL77 Ben 75 KIHo8l NSBN71. LeBrn, CoHe72 CoHen CoUe72. LeBr72 NKBP73 CMHL77, SNMK78 CoIle72.ltBr72, SNMK78 (El)P'hPtCh (Ph)i'hNiCh (f'hlPhNiCh ",PBCJ, Ph,PO"'" (NbjO'a)(.\(EtJi)J (Nb6all)CI'~E4Nh CdC" OCJ, HA loCl InCi) T'," UCb ua. 00, UDCI UDO, "o, (N14''''''' OPO, 19.. 199J 198.4 199.0 198.7 198.' 198.8 199J 198.' 198.8 197.8 197.8 198.1 198.0 199.2 198.9 200.1 208.2 206.5 208.8 209.0 208.5 208.2 2Ol6 208., 196.2 196.4 1%.1 191.9 200.1 200.0 198.0 198.0 191.1 199.2 198.1 199.0 198.3 199.4 198.' 199.4 197.5 199.0 199.2 198.7 19M 199.0 198.2 198.1 191.7 191.7 198.5 198.3 199.7 198.2 201.7 If'\, 21R \lI CoHen LeBr72 CoHen LeBrn NS81m SNMK78 HUGH79 SeTs76 Tnc74 CMHL77, Nefe78 SNMKn SNMK78 Nefe78 BCH75. Tnc74 Tric74 NSBN77 Sher76 MVS73 MVS73 MVS73 MVS73 MVS73 NZB18 NZB78 MVS73 EMGK74 EMGK74 HVV79 EMGK74 CKAM75 CKAM75 Nefe78, Olm9, MMRC72 Rigg72 CBA13 LeBr12, Ncfe78, RiU72 Riggn BNSA70, STIIU76 NZB78 HVV19 HVV19 BeW,79 BeWa79 SAID73 YYS78 SATD13 FH177 HIm MRV83 TBVL82 TBYL82 TBVL82 TBYL82 TBVL82 SA1D73 K_ FlWe75 Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Koo, Koo. HOPl(RllPh HOPl(FJ:fh ChPl(PhlPh P!ljPCuCh PhIPCuCi) C,lhO c.ll~CCb C(NHllJCJ ~CH,""HCI) Co2p ll)6j """ 197.9 198.0 198.0 198.9 199.0 201.0 201.0 198.0 100.0 NZKn NZKn ALn ALn AL77 FSJL83 FSJL83 CKMll LeRaTI CrlN Crl< CrBl n., Co Co nB3 ns.1 LANM81 WROM19 ThSh" Co;l nS.4 778.0 781.9 783.0 782.6 782.4 180,2 780.4 MElX13 MElX13 LimoSl CSC72 Co~ ·4HJO COFl COO COO eo,o. eo,o. 780.2 Co,(>, 779.9 780.0 781.0 780.8 781.9 780.2 CoOOH Co(OH), CoAIA CoAIA CoO"' . COfei)1 n9.5 Cl)Sl $ $ NBMO?) csen WRDM'79 Kim75. NGDS75, NFS82, CBR76 NGDS15.0kHi76 GPIlG19 Mc:Co75 McCo75 McCo7S otHi76 781.2 z.co,o. 784.0 780.• OkHi76 C5JCo~ 180.' 180.8 181.0 180.' 781.8 Cs~oBr. c.""", K,Co(CAn K,Co(_ Co<CO),NO K,Co(CN' K,Co(CN' Co{NHJlJC:h Co(Nlh))OJ Co(NHJl.C1J Co(Nlh16Cb Co(C}li5h Co(C}Hili 780.7 181.2 7811 181.4 781.9 ?8U 781.8 779,1 7S1.3 Perkin-Elmer Corporation Physical Electronics Division S76.l 578.3 580.3 C<O, Cri', C<o, Cr(DHh C<OCH Cr(COl6 Cr(COl. "',00. ",,c,,o, C..oo, C","", K~lOI LoOO, <';,00. NazC!O. Na£rlOl NaJCrO. Na£rO. N.oo, ZoO"" B.ao, c.c.o. (Nl-4hCrl~. BCGH1' Ollii76 Vann76 NBM073 YNAB17 csen NBMO?3 BCDH73 CIAd71 574.3 576.7 c.o, NBM013 NBM013 576.9 514,3 514.3 576.1 575.3 5743 576.8 NBMon HBMon = 574.4 Cl)()l Na£~ CoSO. "'"'"" 5161 LiCJ(h CoMoO. CoMoO. CoRhzQ. n9.7 780.0 780.9 782.8 "'" Cn, Cril>, COO, PCLH76 OkHi76 OkHi76 OkHi76 GPOO79 PCLH76 NFS82 Lim081 CoMni>. Cr2p PRCV77, WRDM79 780.' CoO COS COr'1 CbCo(lbioureah CKM71 CoO m, Br.<:o(EJ.Nh c~n C, Cr?OJ C, C, Co eo,os.. Appendix B. Chemical States Tabl~ D{NH,;a, K,D{CN' <,of, Cr{acacb Cliacacb C!JCr(ureal. Cr{CsHsn Cr(CSHlh CnCSHIXC1H1) C<{OJ" C<{CJ<.' CI(COhPHJ m.' 579.8 S77J 517.0 576.3 517.0 579.8 519.5 516.4 577.1 579.9 515.& 519.8 517.0 519.8 580,5 579.4 518.5 577.9 517.1 517.2 579.1 578.9 519.5 "Ill 516.3 583.0 517.7 576.1 579.9 574.8 576.3 574.4 574,J 575.4 575.3 EMGK14 EMGK74 NBM073 • <,< LANM8! WRDM79 RoRo16 STAB76 MElX13 = = = = BOFP8I, CDFM82, <:sen, WRDM79. NGDS75 IIKK76 ACHTI) CSC72 COFMS2 CDFM82 IlKK76 BeGHn, BCHMn PfD13 A11' A11' ACHT73 CDFM82 NSSPOI HoThlll AClffi3 AClm3 ACHT73 LaKe76 ACHT73 LaKe76 LaKe76 LaKc76. ACHT73 BDFP81 ArJb76 ACHT73 A'M. AITh1<i Vaon16. ZeHa7l AITu'16 AITh1<i leHa?l AITh76 BCOIl73, CDH 74. GSMJ74 ClAd?1 COll74, GSMJ74 CDH74 PF07l BCGHn "" Appendix 8. Chemical States Tables C:l(CO)sNH) D(co},c.Il. C,CObc.H. Cl(COJs(MeJI)j CI~r(CsHs) IC,c.H.l CrLl\lM C, Cs JdSll C. C. 515j 515.1 576.3 575.2 576.1 516.4 BCGH72, B01M72 CDH74 PfD73 BCGH72, BCI-lM72 GSMJ74 CDH74 527.2 WROM'19 OCro. 726.4 726.0 723.9 724.0 723.1 724.0 m6 723.9 723.9 723.8 724.2 c.,c,," n45 DOH m, 724.5 c.r CsBr ocr ill DN, c.~o. Cs;PO, C>.p,o, c.,e"o, Hand~ok ""0 a.et 9313 VWIlS81 9325 CA.wm. Wtgn75 CuF) "',0 934.4 935.2 934.8 935.6 93" 931.0 936.8 932.5 • Gawm WRDM79 VWllS81 YYS18 "'W077 WRDM19 VWHS81 CDFM82, GaWi77, Wagn75. HMUZ18, MSSS81, Scho73b M 933.7 MVS73 MVS73 MVS73 MVS73 SGRS72 Wag.17 MVS73 MVS73 MVS73 ACKT7l ACHl73 WRDM79 "'tOH}, Cu(NOJh CoCN COC, CuCh OCt, COC, "'" "''' KDR77 c.qCNb 935.1 935.5 933.1 9312 c.co, 93" c.so. •• ColO"'}, Cll(OAch Cu(acach Cll(8-HydlOzyquiooJ.) C. Salicylakllnime 934.' 935.5 934.9 931.6 934.1 934.6 932.3 933.8 932.6 934.1 934.4 931.8 935.0 934.5 935.0 934.0 LANM8I """'IE>JIb '325 ""0. CuSiO) ClIlMOJOII c>",o,o, <>coo. a.ao, CuFeIO~ CsMNN c.~ DOH Cu2p C, M c> a. C, C, C, a. c> c..."" CutsSns a.,P """ c.s, """ CuAgSe Culn$ez Co~ c.s c.s C"' COS CoB, 220 568.4 '8'-' 932.7 9316 9316 9316 9316 932.6 932.7 932.7 9316 932.6 932.5 932.2 932.2 931.9 932.0 931.9 931.9 932.5 9312 9331 931.9 935.0 932.1 of X-ray Photoelectron Spectroscopy Waf'17 WRDM79 AtMP82 BiSw80 BiSw80 BiSw80 PEl82 KPMl.73, WRDM79, Wagn75 V,,;yn llegd82 NSDU75 !iSDU7' RRD78 RRD18 RRD78 KJI081 WllgII75 RRD18 Asam76,~Wm, LimoSl BSRR81 NSSPSO BrFr74 CuFe0l CuMo04 """"'" CUJO(I'hNCONHCONHlbl 935.8 HMU'l18, Qawm. WRDM79, MSSSSI MSSS&1 NZK77 Wagn75 NZKn WRDM79 CmoSI NZK77 WRDM79 HMUZ18 HMl1l78 CDI'M82 AClm3 LDDB80 LDDB80 HMUZ18 NFS82 BrFr74 YY~ BrFr74 BrFr74 BuBu74 EMGK74 YYS7lI Cu Ll\1M a. c> a. a. Co c..z.. """ Cl& CuAgSe C,~ c.s CuBrl c.cr a.et ocr, CuF I Co', 918.6 918.1 918.6 9117 918.6 918.6 917.6 918.4 917.7 917.4 917.9 916.9 915.0 915.6 915.3 916.0 914.8 m BiSw80 BiSwSO BiSwSO PEl82 KPMl.13, WRDM79, Wagn75, Asam16,GaWin _n RROJ. RROJ, RRD78 Wagn75 RRD78 VWHS81 Wap75 GaWi77 WRDM79, VWHS81, GaWi77 GaWi77 WRDM79 Perkin-Elmer Corporation \ j / Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy C,F, c,,o c"o c"o c"o 00 Cu(OHh c.(NQ,), OCN c.qCNh c.co, c.so. "";0, CU1MOJO. CuJMOJO, e,e"o. ""''''' 914,4 916,2 916.2 916.6 917.2 918.1 916.2 9153 914j 914j 916.3 915.6 9152 916.5 91 .. 91 .. 916.6 Dy4d Dy ""'" ""'" 152.4 167.7 Dy JdYl Dy 1295j 1298.9 E,4d "" ""', 167.3 169.4 168.7 VWHS81 CDFM82. HMUZ78 CDFM82. GaWi71. Wagn75, HMUZ78. MSSS8 [. SclJ:l73b MSSSBI, Wagn75 GaWin GaWi77, MSSS81. Scbo73b MSSSSI Cd~ Cd~ NZKn CdI', Wagn75 c,~ NZKn WRI>M79 NZKn c,~ WRDM79 HMl1l78 HMl1l78 CDFM82 HMl1l18 . . s..... SaRaSO . WRDM79 WRDM79 Eu 3dYl '" 1125.6 E, 128.2 135.9 KF KF LiF LiF N,F N,F N,F 'bF RbF ,,~ 'oF, c.F, D~ S,~ AiF ,,~ 684.9 685.9 683.9 6$4.4 685.1 685.0 684.5 684.5 683.7 683.6 682' 683.7 6843 684. 684. Perkin-Elmer Corporation Physical Electronics Division . WRDM79 NBK74. MVS73 PMDS77 WRD~179 MVS73, NBK74 WRDM19 NBK74. NSLS71 MVS73 MVS73 NBK74 WRDM79 NBK74 WRDM79 NBK74. NSLS71 Wagn80 NBK74 WRDM79 NBK74 GaWi77 NBK74, NKBP73 GaWin, WRDM79 NBK74, SATD73 NSI.S77 Ga Win. WRDM79 VWIIS8I H8~ 686:. SAID73 684.8 685.0 '684.7 6816 684.6 685.1 WRDM1'J GaWi77, WRDM79 NSI.S77 WRDM79 GaWin, Wagn77 NBK74 NBK74, NKBP73 NBK74, NKBrn Mol'" WRDM79 NBK74. NKBP73 WRDM79 WRDM79 WRDM79 WRDM79 WRDM79 TOVL81 TBVL82, PMDS77 TOVL82 WRDM79 WRDM79 NKBP73 NKBP73 NKBP73 WRDM79 RNS73 WRDM79 Wagnn NSLS77 NBK74 WRDM79 NBK74 Wagnn WRDM79 Pb~ z.~ z.~ AIF) ·3Hz{) ""'·lH,o 00, 1,1\ lnf)' 3Hz{) 1.01\ N<IF, """ SmF, YF, UF, UF, UF, ThF, . HfF4 NaBeF) NNBF68 NNBF68 685' 685.7 685.0 684' 6817 685' 684.' 684.8 684.2 684. 685.9 M"', NiF:! NiFz ·4Hz{) NalBeF~ FIs UF CoF MgF, MiF, S<f, uF, Eu 4d Eu10j Appendix B. Chemical States Tables NaBr~ NF~BF. NaJAIF, NaJ5iFj NaJSiFj KJSi~ KlliF, K1liF, NalTiF, KJFeF, K1NiF, """F. N""'~ K,Z<F, N"",. KZfFs' Hz{) K,z,~ N""I\ ~FI'HP OO>F, 686J 68>1 684.8 68>1 68'3 684' 6848 684> 684.6 685.3 685.3 684.' 684.' 684.9 685.4 685.1 685.7 685.2 687.0 694.2 685.5 686.0 686,4 68.. 685.0 684.9 685.3 684.' 687.6 685.2 685.9 684.6 685.0 684.8 6843 6853 685.1 683.6 TRLK73 NBK74 WRDM19 NBK74, NKBP73 WRDM79 NKBP73 NKBP73 WRDM79 NBK74 BeH75 22\ Appendix B. Chemical Slates Tables K2SbFl KSbF. KSblFJ NazSbF; NaSbF. K)RhF, KlNbFl K2NbFl K2TaF1 K2TaF1 NaTaI'. Na2TaF7 NaJTaFI K2UF6 EuOF "OF NdDF PrOF YOF Cs2Mo(hF. Cs2WOIF. U01F2 p-(CF1=CFV NiOOCCF) CHlCNBF) NHlBF) Clli;NBFJ EtNH2BF) E!4NSbF. Phy>BFl Ph,POBFJ Handbook of X-ray Photoelectron Spectroscopy 683.9 686.6 684.3 683.4 685.l 685.7 685.4 685.2 685.2 685.1 685.2 685.6 685.5 684.7 685.3 685.2 685.1 685.0 685.5 684.7 684.7 685.6 689.0 688.4 687.0 686.6 685.6 686.6 684.7 685.7 685.8 Trie74 Wagn77 Trie74 Trie74 BCH75 Ncfe78 WRDM79 NBK74 WRDM79 NBK74 NKBI'73 NKBP73 NKBP73 PMDS77 RGBH80 RGBH80 RGBli80 RGBli80 RGBli80 NKBP73 NKBP73 TBVL82 Wagn77 WRDM79 BCGm3 BCGH73 BCGli73 BCGlm BCH 75 HVV79 HVV79 653.8 654.7 655.0 656.2 655.4 6S4.4 656.3 659.3 656.0 657.0 656.2 656.2 655.5 658.5 655.6 656.4 658.0 657.0 657.2 657.0 655.8 657.0 655.3 WRDM79 WRDM79 Wagn77 WRDM79 WRDM79 Wagn77 WRDM79 GaWi77 GaWi77, WRDM79 GaWi77 WRDM79 WRDM79 GaWi77, WRDM79 WRDM79 GnWi77, WRDM79 WRDM79 WRDM79 WRDM79 WRDM79 WRDM79 WRDM79 WRDM79 WRDM79 FKLL C,F LiF N,F B,~ C.~ MgFI SrFl AgF OJF, C"~ C"~ C"~ NiF) Pb~ ,,~ InF) "F, NdF) PrFJ SinFl YF, ThF. HIF, 222 NaBF. Nay'llF, NazSiF. Kl1iF. NaJ1iF. K)FcFb NailcF, Na2ZrF, NaSnF) KSbF. KINbFJ K1TaF1 p-(CF1=Ch) NiOOCCFJ Fc2p F, FeID) F, F, F, FeJAI FClSi Ft1B F'B FeJC FoS FoS Fesl (markasite, pyr) KFe.'h FeBrl FcRr) FeCh FeCI, FeFI FcF) F<O FeJO. Fe)O. Fe20) Fe20), alpha Fe20), gamma FCOOH, alpha FeOOH, gamma CeFtjO. Fe(C:(hlJ 61bO FeSO. K)FeF6 NiFeil. Kj Fe(CNl6 K.Fe(CN),; K.Fc(CNl6 Na2Fe(CN))(NO) Na)re(CN)~N20) Na.Fe(CNHNOJl Na)Fc(CN)14HJ 652.8 654.1 653.0 655.7 655.1 656.0 654.0 655.1 655.3 656.6 655.2 655.0 652.4 652.9 WRDM79 WRDM79 Wagn77 WRDM79 Wagn77 WRDM79 WRD.\179 WRDM79 WRDM79 Wagn77 WRDM79 WRDM79 Wagn77 WRDM79 707.0 710.9 706.7 706.8 707.0 707.6 707.5 706.9 707.1 708.1 710.3 712.2 706.7 708.7 710.3 710.1 710.6 711.3 711.3 714.2 709.4 708.2 710.4 710.8 7l0,9 710.9 711.8 711.3 710.5 713.6 712.1 714.4 710.5 709.6 7fJ7.1 708.5 709.7 707.4 706.8 707.6 $ " LANM81 Asam76 WRDM79, MeZe77 ShTr75 ShTr75 MECC73 MECC73 ShTr75 cscn Bind73, LimeSI Sind73 Bind73 CSC72 CSC72 CSC72 CSC72 CSC72 CSC72 MeZe77 MeZe77 OkHi76 WRDM79, NGDS75 MeZen MeZe77 MeZe77 KoNa80 MeZe77 Kilk73 Lime8l CSC72 MeZe77 Vann76 Vann76 YNNA77 YNNA77 YNNA77 YNNA77 YNNA77 Perkin-Elmer Corporation (J) Physical Electronics Division Handbook of X-relY Photoelectron Spectroscopy Na~CN~11i4 F«COl> F«COh(NOh KFee(NOh~h .2HzO Fe(SMe)(COh R<W1sn lJPe(CI~ls)l Fc(CsHACOOHh Fc(phlhaloeyanine) FeLMM F< Ga 2pYl 0. G. G.' Gop, G.,o, 1m} 109.6 '095 BCGH12 BCGlm 709.9 708.4 109.1 Neft78 BBFRn FWUM79, BCDH73, CDH74, Nefe18 CDH74 FWUM79 MSV79 '0&, '707.1 0&' '02' 1116.7 1116.5 1116.8 1116.9 1117.8 YNNAn WRDM19 • Scho73a NSDU75 BDFPSI ScooBa GaLMM G. GoA, GoA, G.' G., GoN o.,so, o.,so, 0.,0, MO, Gop, G,Jd G. 1068.2 I,,"] 1067.1 1065.6 106l>ll 111645 1ll6i2 106i' 1061.6 1062.4 1062.9 18.6 GaSb GaAs 20.2 GoA, G.' G.' o.P o.P 19.2 o.N AIOW o..so, Ga~) GaPI GaP) GaJO) GaJO) las las 19j I" I" 195 19.0 19.1 19.9 19.6 20.2 20.5 21.0 Gd 4d Gd 140.4 Perkin-Elmer Corporation Physical Electronics Division WRDM79. MINN18, Scho73a MINN78 MINN78 M1NN78, MIN81 MINai "'11182 11182 MINN18 11182 Sehona MINN78, LBHK73, Scho13a. WRDM19 LBHK73 lPMK14 IMNN79, MlNN78, Tayl82, MINHI NIMN18, IMNN79 LBHK13, MlN81 LPMK74 Appendix B. Chemical States Tables Gd,(), Gd 3d Gd Gd,O, Ge 2pyz Go G< G<S, G<S, """ ad, G<F, G<Q, ">G<Q, "'''''~ K!ieF, ""'" GeLMM G< G< G< G<To Go& GoS G<Q, N"""" G<Jd G< G< G< G< GoA" GeTejAsl GcSlTeAsl GoS,A, G<T~ G<T, G<T, Go&, Go& He~U80 G<S, Toy'" GoS GoS 11182 11182 GGVL19 lBHK73, Schema 11182 MINN18 • 1418 G<Q, ""'" PbJC;el PhIGeBr Ph.JGeCI 1187.0 1189.0 1217.2 1217.4 121~.8 1219.8 1218.8 121&.2 .1220.1 1220.. 121&.9 1221.3 1220.7 1218.9 1146.2 1145.4 1145.1 1144.8 11418 11417 1137.7 I13i1 29.4 29.3 29.0 29.1 29.7 29.9 30.2 J<l.' 30.1 30.0 29.7 3\.0 Jo.9 30.. J<lj 29.5 J15 31.2 31.8 31.8 31.8 1If4f Hf 14.3 ,,"'" • SaRaSO McWe76 TI.R78, MoYa13, Wagn75 MoYa73 MoYa73 n.R78 MoYa13 MoYa13 MoYa1), Wqn75 MoYa7) Wagn75 MoYan MoYa1) McWe16 SFS77 Wagn15, WRDM79 SFSn SFSn SFSn Wap75 W>p71 • McWe16 SFSn HKMP74, UeOd82, WRDM79 HKMP74 IlKMP74 HKMP74 HKMP74 HKMP74 SFSn HKMP7-4 lJoOd82 SFSn HKMP74 SFSn HKMP74 HKMP74 HWVV74 HWVV74 HWVV74 HWVV74 • Appendix B. Chemical States Tahles Handbook of X.ray Photoelectron Spectroscopy '. IIf 1I1D, 14.4 16.7 Uf4d 1I1D, 213.2 WRDM19 bN",Ph,p), SaRa80 hPt(EtJP)1 41njPr.N) SaRallO, NGDS75 llPl(MeJPh cis hP(MeJ'h trall 4(MoJ''> Hg4f HgS (cillllabar) II, Hr,..CduTe 1Ol.0 99.' II,S '00.2 100.8 II~, 100.7 HgBr! IIgCI, 101.0 1IgF, Hg(lhiodibenzoylll¥h 101.2 100.8 101.3 101.3 101.3 (l'bJ'hllg{SCN' 101.4 llgO EIINCJ4HgOAc CIzHg(H~HroNHV! 101.4 • &Men, SATD73, 5MBM76, WRDM79 SBSSO NSSPSO SATD73 SATD73 SAID13 SAT073 NSSPSO NSSP80 YYS78 TBHH77 R>U82 Li' A" Cdi X, """ '"N_ K1 Li' I.iI A~ Cd! Cdi C., II~, ,,' ~" Nih Nih·6H{) lob Zob NalO! Nal0~ 1110, H"'" ',0, '0 ·le!) es,shrJg """", Na(NilO6) . H10 224 619.3 619.9 618.2 618.2 618.8 618.6 619.7 61&.9 619.4 619.2 619.4 619,0 619.4 619.0 619.1 619.0 619.7 619.8 619.7 623.5 624.0 623.1 6210 ,23.3 621.5 622.5 618.5 ,"'. 624.4 • ""''' MVS73 501.3 506.0 In Jdsn '0 '0 4418 Ill9sSnl 443.6 [nSb 444.1 444.6 "".5 ~,s, ~" '0' "".8 4460 443.9 InCh 445.1 446.0 446.9 MVS13 r.WiI1 ~C1 'I«" Shcr76 SIler76 S1«16 ...... ....., ~C1, GaWi77 NZB18 GaWin SATD1J 443.9 ~'" WRDM79 FIm1 FIm1 Gawm GaWi77 Nih !nBf) InSr SAT073 Ga\\'i77 SATD73 501.0 lob MVS73 MVS73 MVS73, Sher76 Gawm ''' InJOJ lnJOJ In~l In(OHh (Nl-4.hinF. CulnSez In(acach BfllnEwN OllnE4N Br.lnPr.N 4lnPr.N C4InPr.N .....0 ...... ...... 444.3 444.6 444.9 445.0 445.6 "".7 445.4 445.7 445.2 445.9 445.4 445.8 G>WiI1 G>WiI1 • Bert81.liegd82, WRDM79, PVVA19, LAKn ""'" IMNN79 Bert8!. CFRS80 WRDM19 WRllM19 WJgo n, MSC 73 Wagnn. MSC 73 Am1 .....n MSC13 FIm1 Wagn77 MSC73 MSC13 ~75,MSC73 Wagn77, NGDS75. Bert81 CFRS80 LAK77. MSC73 WRDM19 ....on KJID81 MSC13 Arm FIm1 FIm1 Arm FHm InMNN Sher76 BCH75 Tric74 '0' 410.4 410.5 401.6 408.0 411.0 NZB18 linTel 408.' ""''' SI«" BcWa79 BeWa79 WRDM79 G>WiI1 SOH ,""" l3dsn CAB?I CAB11 517.0 50,," C,' In)Tt] 159.6 NZB" Riggn FHT71 IMNN '0' Ho4d 110 l'.(M06I!) 6193 619.2 619.6 621.1 621.9 620.' 619.3 "In,sSn, lnSh ~, m W WRDM79 PVVA19. KISCSO, LAKn lMNN79 Den8l K1SCSO WRDM79 Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Pbotoelectron Spectroscopy ''""""", Inh InBl) ''''' "'~ 1,,0, In(OHJ] (N1~)llnP. 408.3 WROM79 4073 w""n "",n w""n "",n ....., .... 405.' .737 ""'71 "",n ." .. ...., 405.0 WRDM79 Wago77 Appendix B. Chemical States Tables K!I'ICIi K,""" K1RtO. K""" K2Wa. 29),] K31~ 293.0 "''''''''' 2912 i.cllm NSBN77 HUGH79 KSbfF, 293.7 KUFFJ' Hi> "'-7 "".n KIUF, K2Zrl<, K,Zrri K,Co(CN\; K,Cr<CN16 63.0 WRDM79. BUliK7D, EPC75 Folk?3 Nerc78KllrBr~ 1.8Nefe78 CoHe72, LeBr72 63.6 62.5 KSPB76, NSBN71 NSBN77 KJMn(CN>. K.Ft(CN16 EPCl5 EPCl5 KJrCI~O KIrCisNO 63.1 63.0 63.4 65.0 "'CO,a. '27 &Q,(Bd'h 63.0 63.6 KSPB16 KSPB76 LeBrn lrONaPhMl: 60.7 ""'73 "liH,)<CH,cH,N!hh I<O,(H,NOl,QI,NH", &Q,(H,NCH,cH,NH", 63.1 NcBan NeBa12 Nefe78 IrCl, K2[rBr6 K,lrClr, KllrCli; KJlrC" (N~hlrC\ (NH.o)JItC!6 l>(COhCl Kllrt<CO}.(\ 60.9 60.8 62.7 62.6 KSPB76 NSBN77 631 63.2 K KO K Ki KB, KCl KF KF KF KCN KN, KNo, Kao, Kao. KJPO. ""A K,oo. K,o,o, K,o,o, K,MoO. KR>O, KAb(A1Si,oIOMOHh KllrC\j K,MoClo K,a.a. Kl Ft(CNl6 !<..V(CNl6 K1Pl(CN).·3Hi) K1Pl(CN).0:!· 3H~ K.JC(SCH:oCHNH1COO») K U\1M KB' KF KSbF. K'3d Kr in graplite K2p 294.. 2929 $ $ 294.6 292.8 SMKM17, PeKa77 MVS73 MYS73, WRDM79 MVS73, NSLS77 2910 292,8 292.5 Wagn75 292.8 2911 PMDS77 MV$73 Vann76 294.7 292.5 292.9 293.2 SGRS72 293.4 NSLSn MVS73 MVS73 293j "'-2 MVS1J MVS1J "'-I ACHTJJ Aom3 "'-, "'-8 NSSPOO NfS82 NfS82 WPHK82 NSBN77. LeBr72,CoHen illle12 "'"'-5-, 293.0 292.8 2927 293.0 J)erkin-Elmcr Corporation Physical Electronics Division CoHen, LeBr72 (J) 1.<Bm CoHen $ U I, 293.7 CoHen. LeBrn ",,",n "'-, KtNiF, Ir 4£ "'-, "'-, La 3d La La Lalh LaIO) La,o, Lll4d La La,O, LaOO, 294.2 293.1 292.6 292.8 293.7 ~92.2 NKBP73 TRLK13 PMDS77 NKBP73 NKBP73 Vann76 ZcHa71 Vann76 291.9 291.9 291.9 293.7 293.1 293.3 292.9 292.. SSEW79 "".7 "".1 249.3 "",n w..,n Vann76 Vann76 Vann76 NSBN71 001.<73 001.<73 WRDM79 87.0 835.8 835.9 838.8 835.1 8317 SCSC82 ScSc82 WRDM79 SaRaSO 103.9 IOU NISTI, KEML74 SaRaBO, NGDS?S, HoThllO 1OJ.1 ~loThro $ Lib LiF Li LiN, UBr CO CF Li~ LiOIl Li~l LhPO. 55.6 ".7 55.2 56.8 56.0 55.7 55.' ".9 55.2 55.4 $ KLMm, CSffi79 SGRsn MVS1J CSFG79, MVS13 MVS73. WRDM19 CSFG79 CSFG79 CSFG79 MVS73 Appendix B. Chemical Stales Tables LiJ'>o, 55.6 u,oo. 571 57.1 l.iao. u~ LiNbOJ 55.6 54.' Lu 4f '" Lu4d 7J L" 196.2 196.0 Lu~) Mg2p ''"" ". 49.6 Handbook of X-ray Photoelectron Spectroscopy MVS73 MVS73 MnF) ACHT13 ACHT73 5111079 • HAS1S. LMKn5, HfV 71, FuggT1, WRDM79 49.8 fWFA15 M&lBh "tf, 50.6 FWFA75 WagnfK) "to 50.8 Mg(OHh "tAlA Tak, M&JSilOIO(OHh "j 50.4 505 MnzO~alpha 641.7 MnOJ:. bela "',j "'641.1 Mn02 MnOOH 6423 641.7 """ CoMnzO.. CuMnA • IIYaSl HNUW7i> HNUW7Sb WPtlK82 """"" MnSo. KMnOl Mnz(CO}lo B"'~CO' (BrMn(COJ.ih BrMn(COMPh}i'j BrMn(COb(P(OMebh Mn~COMPhJPh K)Mn(CN16 N~Mn(CN16 Mg Is ",,00 1303.1 13010 Mz,BiJ, MgF1 Mg(Ollh MgAhO. 1304.0 13OS.0 1302.7 1304.0 '" HAS7S. LMK175, FuUT1 FWFA1S FWFA1S Wagn80 HNUW78a HNUW78b Mn(C,H,h "~COh(e,"" MIl(CO)iCs~ '" 1185.5 IMKJ7S,SRHH'1S. WRDM79, Fuggn.HFVTI M&2Cu Mg,Bil 1185.7 11&4.6 1178.2 11803 ~WFA1S Mn2p ".MnOJ ". "'21 Mo 638.8 639.0 "oN "'" "'13 MnS. beu MnS. alpha "'., "oS "oa, "'21 641.9 "'20 "'20 MnF1 642.6 MnB~ 226 "',j "". ...., 640.6 647.0 641.6 641.9 641.7 ""j "". 6<07 639.7 6383 638..5 .." 6<0. FWFA1S WagnSO WPHK~ 639.0 6<03 641.9 •• LANM81 WRDM79 <:sen <:sen Aoki76 Aoki76 LimoSl Aoki76. Aoki76, cscn Aoki76. Aoki76, cscn cscn cscn eSC12 OHm otHi76 Aoki16, CSC72 011175 CSC72 otHi76 otHi16 00115 WRDM79 OHm Aoki76, cscn, NODS7S OH175 otHi76 OtHi76 otHi76 Limolll UmRe78 VWVBn VWVBTI VWVBn VWVBTI VWVBn vwvnn Vann76 Vann76 BCDH73, COH?4 ffiH74 ""<!II MnLMM ". ", ", ", MoB! MOlBs "o,C ·MnIJ .. 641.4 617.6 VayrSl m.O • MoJd MgKLL MgFI Talc, M&lSi.OrO(OHh 6<07 Mn~) MuzO). alpha "oA KEML74, LPWF1S SaRa~O, NODS7S "',. MQj 641.4 641.2 641.6 MnzOJogamma M~Cu 51.0 ",o ",o ",o m., 228.0 227.9 2273 227.8 MoSil 227.7 "oS<, 22<3 MoS1 229.0 229.6 "oCh 230.0 230.. "oCh "oe, 231.0 229.3 "00, 2316 "oS, MoCk ",o, {NH)QMoO. AIJ(MoO.b Ah{MoOilJ 232' 2321 232.5 233.3 NyMa80 CiDe75, WRDM79. CGR 78, GrMa75, KBAW74, WaTaSO "ECC73 "'BrWh78 Wh" WPHK82 GrMa75 PCLH76, GrMn75 SSOTSI.SIEd7S GrMa7S OrMa7S GrMa75,SwHe71 SaRaSO, CGR18, CiDe75, KBAW74 G1'0079, KBAW74. SaRaSO. ODe7S, CGR78, GrMa7S WRDM79 SwHe71 PCLH76 NFS82 Perkin-Elmer Corporation Physical E1cclronics Division Handbook of X-ray Photoelectron Spectroscopy CaMo<>. CoMo04 CrMo04 CUMo04 K1MoO. NajMoUt NalMoUt ·2Hi) (NH.)lMOlOJ (NIl4hMo~' 4Hi) CUjMoJOlo CuJM0109 RhlMoO o ChMo(NOh !<4M{}JClg r..(MQ61s) Br4(Moollr!l CI4Mo(PhlPh C~Moi&,pj4 ChMo(PhPMew mer C~MOJ(PhPMC1l4 (COhMo(PhlPj (CO).J.1o(PhJPh (CO)sMO(PhlPll ChMo(COh{PhJPh ChMo(COlJ{PhJPh CllMo(NOh(PhlPh ChMo(NO)j(MeCNh ChMo(pyridylh C4MOl(pyridyl14 Ci4Mo(pyridylh Br4(MOr,Brs)(pyridylh ChJM06(Pyridyl) C4Molbipyridyl) ChMoO(bipyridylj ChMoOz(bipyridyl) (CO)4Mo(bipyridyl) Cll1M06(PhlPh C4(MOr,Brl)(E4N)l Br6lMCl6Brl}(E4Nh (B UlNhMo(COl4 (BI4N}.>MOiIIi (BI4NjJMOlCI, (CIH.llMo(COh MoOiacach 232.8 232.4 232.2 232.7 232.1 232.1 232.5 232.5 232.7 232.4 232.8 231.8 230.4 229,2 228.8 229.3 231.9 228.7 229,4 228.7 228.3 227.8 227.4 229.3 228,8 230.3 23l.5 22905 228,9 230.8 229.7 229,6 232.0 231.9 232.3 226.3 229.6 229.2 229.3 227.4 229.0 229.5 227,4 232,0 N Is BN NH, NH, Cr1N C," G.N GcJN~ SoN TiN 398.1 399,6 398.7 3974 396,7 397.0 397.4 396.2 396.9 Perkin-Elmer Corporation Physical Electronics Division NFS82 GPDG79, CiDc75, AMA...74 TVG76 HMUZ78 NFS82 CiDe75, NFS82, SwHe71, NSLS77 GrMa75 AMA...74 GrMa75 HMUZ78 HMUZ78 NFS82 Nefe78 HUGH79 BeWa79 BcWa79 HuBa74 Walt77 LeBrn Walt77 HVV79 HuBa74 HuBa74 Nefc78 HuBa74 HuBa14 Nefe78 CEt.C76 Walt77 SwHe71 BeWa79 HaWa74 CELC76 CELC76 CELC76 GrMa75 HaWa74 BeWa79 BeWa79 GrMa75 BeWa79 Walm GrMa75 GrMa75 • HHJ69 LaLu79, RNS73 RoRo76 STAB76 HcMa80 TLR18 STAB?6 STAB76 Appendix B. Chemical States Tables VN ON SiJN~ SlN 1 SP{NHlh S~N3CI (NPCh)J CS(N*NN*) Cs(NN*N) K(N*NN*) K(NN*N) Li(N*NN*) Li(NN*Nj Na(N*NN*) Na(N*NN*) Na(NN'Nj Na(NN'N) Rb(N*NN'j Rb(NN*N) K3Co(CNl6 K3Cr(CNl6 KJFe(CNl6 KlMn(CNl6 !<4Fe(CNl6 !<4Fe(CNl6 !<4Y{CNl6 N34Mn(CNl6 NaJf"c(CN)j(N*Oj NaJf"e(CN*h(NO) 397.4 398.1 397.4 398.9 398.8 400.4 400.3 397.9 402.2 398,S 402,8 398.7 403.1 39805 400.1 402.9 404.5 398.1 402.4 3!>9.6 397.6 398.1 398.3 398.0 397.8 39805 JIn.6 402.7 m,4 N34Fe(CN~*Ol 404.3 N34Fc(CN*hNOl 396.6 399.8 398.3 400.6 400.2 400.3 40lJ 401.9 402.3 403.1 403.3 401.7 402.9 401.4 402.6 402.1 3993 399.1 397.9 417.1 404.9 403.9 4075 408.0 407.2 407.3 KCN KCN KCN NaCN (NH.)lPlC4 (NH.hSOl N*H~NO) N*H~Ol N*H~Ol N1H~O. N1H~o. NHlOI1Cl, ionic NHlOHC1, ionic NHlSO J NaN1Ch KSCN KOCN KOCN NF4BF4 NaNOJ, NaNOJ, Ba(NOlh Ca(NOlh KNO, NH.N'Ol STAB76 WRDM79, HJGN70 TLR78 SOI077 F1We75 HHJ69 HHJ69 SGRS72 SGRS72 SGRS72 SGRS72 SGRS72 SGRS72 SGRSn HHJ69 SGRS72 HHJ69 SGRS72 SGRS72 Vann76 Vann76, ZtHa71 Yann76 Yann76 Yann76 YNNA77 Yann76 Yann76 YNNA77 YNNA77 YNNA77 YNNA77 HHJOO YNNA74 Yann76 Yann76 KaEI79 SwAI74 SwA174, BCM78 BTE7) HHJ69 HHJ69 Folk73 HHJ69 Folk73 HHJ69 HHJ69 HHJ69 HHJ69 Folk?3 RNS73 HHJ69, uHc75 BTE77 CLSW83 CLSW83 NSLS77 BTE77 ','.7 Appendix B. Chemical States Tables Ni'LN"OJ NHIN*OJ NaNOl NaNOl Ni(NOln Ni(NOJh'6H~ I'b(NChh Sr(NOln KII~(NOJ. K2Pl(NOzlt, K,co(NO,Jo K,Rh(NO,Jo K,RhlNQ,), MoC!J(NOh K1Os(NO}Cls K1Ru(NOlh K~u(NO)Br} IU1](NO)J.'h Co(COhNO Fc(COh(NOh Co(NHI)!Ol Ni(NH~l"1: Ni(NH~c:IO.n Pt(NtHJh(NOth Pt(NHln(NtChh Pt(NHlhCh Rh(NtU~J M~Br ",.Na "oNa EIiNCI ElJNHCI Et!NHHSOt B,,,. BlNHJH50. Bl4NHS~ EINHl EiNH)BF) NH.O N140 NHJllF.l C,H,N CjHsN CvisNHO CsHsNBF.l Hwmelhy\epdelJal'llll PhCN C(NHlhO PhNHl ",,NO OI'(NM"" P\NM<,), Cysteine HCI Hyoolte Cyslcine lhN(CHuJCOOIl ionic HN(CH~h ioric 1.111: <nao 405.8 408,1 407.' 401.0 .". 407.1 <nal 404.7 404.7 404.2 404.1 407.3 401.4 4<)'8 4<)2.5 403.30 4OI.SO ""10 401.80 ""'0 399.60 399.90 ""4<) 404.4<) 400,20 400.10 401.40 4<)150 ""30 401.40 401.20 401.80 3..90 401.00 401.10 39&.90 401.40 400.80 4<)150 401.90 398.80 399.30 401.00 401.40 399,40 399.20 400.10 399.40 403.00 399.10 3..30 401.20 400,00 400.80 "'70 Handbook or X.ray Pholoeledron Spectroscopy HIU69 BCM78 HHJ69, uHe7S BTE77 TRU73 ""'78 11.R18 a.5\Y33 SNMK78 SNMK78 NBM073 SNMK7S SHMK78 Nefe78 Nefe7S Nefe78 Nefe78 Hefe7S BCmln BCOIl72 YNAB77 ""'18 "'" 18 Hefe78, CMHLT1 Nefe78, CMHLT1 Nefe7&, CMHL77 Hefe7S SGCT7' EM.GJC74 Wle7S EMGK74 LiHe7S EyRe81 LiHe7S EyRe81 EvRe81 BCGH73 BCGH73 SwAf14 EMGK74,mn Ooon73 LiHe75 BCGH73 HHJ 69 BCGII73 LiHe7S lille7S teRa77 ulle75 LiHe75 AWe75 GBMP79 SSEW79 UMa79 YoSa74 YoSa7. NtO"COOHh H2NCHlCOOH HJNClitCOQ ionic EtCHNH 2COOH HIN(Oh)JCOOH CUJCHNthCOQH IhNCo.~1l1 H1NCSNHt H1NCSNHl CthCONlh PhCONHI PhN::NPh PhN==NPh PhCH==NPh 1,1··azonaphthalcne NCN=C(NtHili AmONO PhC==NOHC==NOHPII MeC=NOHC::NOHMe Ni(di methylglyoximeh Cu Salicylaldoxime Cu(8·hydroxyquinolh 8-QuinolillOl Cl(CObNfh N(EtO)JSiCl N(EtO)JSill Morphine MClIphine H2SOc Na Is N. NaCI "' N. N.1 NoB, NaBr NaCI NoCl NoCI NoCI NoCl N.f N.f N.,co, N.,co, Na;-IPO~ NalHPO~ NI2S,oJ ",,so, N.so. N.,sd), NalTeO~ NalPO~ NllPi'J ""p,o, "'10 398.70 400.(/) 400,60 398.80 401.00 39950 399.80 399.20 399.60 39950 399.(/) 400.10 399.10 400.00 399.20 4045 4006 399.8 400.4 400.3 3995 398.9 3995 400.5 399.& 398.5 4<)11 1071.8 1072.1 1071.8 1071.4 1071.7 107L7 1071.4 1071.6 lon, 1071.5 1071.8 lon3 1071.2 1071.0 1071.5 1071.7 1071.6 1071.5 1071.6 1071.3 10711 1070.8 1071.1 1071.1 1070.8 1071.6 YoSa74 YoSa74 Yo$a74 YNAIl77 YoSa74 YNAB77, KNPP74 LcRaT1 SrWaT1, NBMOn LcRa77 SNMK7S LBNN78, Hill 69 BiFe76 Lille7S S"lNsn Yosh80 LcRa77 Wle7S YOIh7S YOIh78 NZB7S BuBu74 YoSa74 V",.., OCGHn GrHe77 GrHe77 SCKK7S SCKK75 •• BaSl15 KLMP73 WRoM'79 Wagn7S MVS73 Wagn7S SOS070 KOK83 NSLS17 HHoDSI Wagn7S MVS73, NSLS77 WRDM79 HHODSI WRDM'79 Swif82 Wagn75 Wagn75 ""''' Wagn7S Wagn75 MVS73, Swif"82, GMD79 MVS73 GMD79 Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Noaa. NaHzl'OJ NaH:PQ. NaHOh N>N, N>NO, N>NO, NaPO) NaPO, N"o,o, N,,oo. NaJCrO~ NallrC\t, NalMoO. NalMoO. NalPdCl. NalSnOJ·3Hll Na lW(1 N...o, NaBi~ NaC~ NIjBeF~ N"od'. NllSiI) NllSiF. NIjTaI; NIlTIf. N.,z,F. NaJA-IF, NairaF, NaBF~ NaBeF) NaTaF. N,,o NoOOCH NaJCll. NaA1SijO,. albile HydroxysodalilC Nalrolile Mol Sieve A Mol Sieve X Mol Sieve Y NaOAc NoOA< NaOOCCHlSH NoO,S", PiNaOCOCMe:=CHtl 1011.8 1071.1 IIl1l0 10713 1070.8 1071.6 1071.4 1011.7 1011.7 1011.6 1071.4 1071.0 1071.9 1070.9 1071.8 1011.8 1071.1 10720 1070.9 1071.3 11l1l' 1071.8 1071.7 1071.7 11l1l1 1071.9 1071.6 1071.5 1071.8 1071.8 IIl1l7 1071.9 1071.7 10725 107l.! 1070.8 1072.2 1070.5 1072.4 1011.8 10723 10726 1071.1 1071.7 1011.2 1071.3 IIl1l2 MVS13 Swif82 Swif82 WRDM79 SGRS72 Wagn15 Wagn75 Wagn75 Swif82, GMD 79 WRDM79 Wagn75 Aam3 Wagn75 Wagn75 NSLS77 Wagn7S WRDM79 Wagn7S Wagn7S WRDM79 Aam3 NKBP73 Wagn7S Wagn7S NSLSn NKBm War,17S WIl17S Wail7S NKBP73 Wagn75 NKBf'73 NKBP73 Ba$t75 WROM79 WROM79 WPHK82 WPHK82 WPHK82 WPlIK82 WPHK82 WPHK82 Wap75 IIH0081 WRDM79 WRDM79 HHOOSI NaKLL N. N. No N.I NaBr N>Cl NaCI Appendix B. Chemical States Tahles NoCl N,F N,,co, NalHpo' NalHPO. N""'" N,,so, N,"'" N.""" BaSt75 9943 994j 'LMm 9911 990.' 9903 990.0 Perkin-Elmer Corporation Phv.. ir~1 Ji',1f'rlroni,... nivkinn SRHII78 WRDM79 Wat,n75 Wagn75 SGS070 988.0 987.1 989.8 989.8 990,5 988.8 988.4 987.8 989.9 990.4 989.7 KOK83 Wagn7S WRDM79 WRllM19 Swif82 Waga1S Waga75 Waga7S Wagn7S Wagn75 Swif82 Swif82 Swif82 WRDM79 Wagn7S Wagn7S Wagn7S Swif82 WRDM79 Wagn75 Wagn75 Wap75 Wagn75 WROM79 Wagn75 Waga75 WRDM79 Waga7S WagD75 WagD75 Wagn75 Wagn75 Wagn75 BaSt75 WROM79 WROM79 WPHK82 WPHK82 WPHK82 Wags75 WROM79 WROM79 202.. 202.J • NllTeO~ 99O.S N.,po. 990.1 989.8 989.1 .989.8 989.8 989.6 989.3 989.4 990.. 9911 9891 991.0 990.2 9903 989.' 990.7 990., 998.1 987.7 NIHlP02 NaHlPO. NaHCO) NaNClj NaND) N.ro, N.ro, NaJOA N,,oo. N,,.,,. NalMl:JOi N.PdC4 NIlSIlOJ . 3HJC) N.wo, Nv..o, NaBiO.l N"od'. NllSiF, NIjTIf, NIjZrf, NaJA-1F, NaBF. No,Q NaOOCH Na2CtO. Mol Sieve A Mol Sieve X Mol Sieve Y NoOA< NaOOCCHlSH NaOJSPh '''' 988.7 Nb3d Nb Nb Nb Nb Nb)Te. 99" 990.1 998.. 989.8 989.' 989.7 990.1 990.. 989.8 991.0 NbT~ Nb"'NbS<, NbS, .'N NbBr) NbCI, 202.2 201.8 202.8 2018 2010 203.4 207.7 203.8 207.1 "".0 NyMaSO MSC73, NSCP74, WRDM79 ""' ""'0.,' Bah175 ""'., Bah175 MSC73 Ball175 MSC73 MSC73 Appendix B, Chemical States Tables Handbook of X-ray Photoelectron Spectroscopy NOO NbO NbO 202.8 203.7 '04.7 SPB76 Bahl75 Nb,O, ""j N~NOJ)j.6H~ LiNbO, KNbOJ 207.1 SPB76, MSC73, fCFGn. NFS82, NGDS75 SlHo79 MSC73 ""'"' NiOa.·6H~ ,.., 2()6j CoNbA DlNbA CazNbih RhNb(h C~NbtChiH~).· 4tiJO CW''''''.xE4Nh Br~Nb60I1XBt4Nh Ch{N~J IIXP1)P)., CIiN~IlX~)' "".0 206.7 2065 '01.7 204.7 204.7 204.6 204.' R:FG71 Bah05 Bah175 NFS82 NbO, Ni(OHh Ni(NOJ)j NiAIA NiAIA Ni~~ BeWa79 BeWa79 NiFeA NiRhJ0. NiSO. NiSiO:I NiWa. NaNil06·BlO K1NiF. &W.79 N,CO, &W.79 &W.79 BrlNi(NHlli Nd3d Nd Ndi}) 980.8 9820 • SaRaSO N~NHUi(CIC4n N~acach N~OAeh· N,C",,) Nd,(), 120.8 Nels Ne in zraphile Ne in Ag Ne in Au NeinCu Ne in Fe 8611 862.4 861.6 8622 863.4 SaRa80 • CiHa74 CiHa74 CiHa74 Wap75 ChNi(Ph)!'h ChNi(PhV'h CIv"fi(PhP>h N~dirrabylglYOlimh ChNi(bipyridyl) Ni(SPbh ChNi(NlizCON~ICONHili N(2-amillObenzolleh 1f(P(llElh). NeKLL Ne in Fe 818.0 857.7 856.4 861.0 854.8 855.9 ,56.5 ChNi(EtlPh Brl Ni(E4Nh 85" 854.2 "" 855.0 854.4 857.0 855.0 855.7 854.6 856.7 855.9 853.8 854.7 855.2 KiWi74 DPsn, U:WS79, McCo75 TRLK73 NZB78 SDR 80, LrwS79 NgHe76 U-'WS79 H'"lB78 McCo75 NFS82 ShRe79 SRD79 NgHe76 NZB78 TRLK73 BCGHn NZB78 NZB78 NZB78, TRLK73 NZB78 BCOH73 QAd7I, TRl.K73 BNSA70 N'lB78 STHU76 N'lB78,YoYaBl NSWU77, NZB7a BBFR71 YYS78 YoYaSl TRLK73 FaBa79 EMGK74 NiLMM Ni2p N; NiO N; N; N; N; Ni~Yb NhSi NiSi NiS NiS If' Nil ·6Hi) l N'"rCh NiF1 '4H1O N<) N;o N<) NiJO) 710 Wagn75 ,56., 855.9 4H1O N~CsHs) Nd4d 855.8 855.6 857.1 856.9 855.8 851.4 856.1 857.2 855.4 855.9 856.8 852.7 853.8 85" 85" 8518 852.7 8517 853.0 8535 852.8 853.2 855.1 855.3 856.7 857.5 853.5 854.3 854.3 857.3 •• LANM81 illlP82 PfJ82 WRDM79, ShRe79 WWC78 GGM82 GO." ShRe79 DPS77 NgUe76 NZB78 TRLK73, KIHe83, YVm NSLS77 WRDM79 DPS77, KJHe83, LFWS79, NFS32. NZ878. SRD79 KiWi74. McCo75 NgHe76 '" N; N; 846.1 846.2 846.1 o Is AlzOJ, sapphire A.,o AsO AI,Q, AIIO. sapphire AhQ" alpha AlA g:unrna "'A,,o,' ' 0,0, "'" Il<O Biz{)) C.O 531.0 529.2 528.6 531.3 531.0 531.8 530.9 531.7 531.6 533.0 ,2>, 531.7 530.0 529.4 PfJ82 WRDM79 KiWi74, KGW76 • Scho73 Sl::ho73, SRD80 Nefe82, SORBO, BGD75, ZS0S79 Tay182, WPHK82 WPHK82 BanSJ, wPHK82 Tay182, MlNN78 WZRSO NGDS75 laYaSl NGDS75. NFS75, HJGN70 NGDS75, DSBG82 JnYaSl Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ra)' Photoelectron Spectroscopy C,O CdO CdOl <>,0, CoO, C""', COlO. ColO. CoP. 00 CrlO) CrlO) 00, 531.3 529.2 530.3 530.3 529.2 529.9 530.2 529.6 529.7 . 530.1 531.0 Cu!> CoO 531.5 529.3 530.2 527.5 530.5 530.3 529.6 F~O) 530.2 Fel0) Fe:JO), alpha feJO), gamma FelO. FoO Ga!» 529.6 529.6 529.8 530.0 529.8 530.8 Goo, MgO MgO M,O M"O Mn)O. MnJOl M"o, MnO:!, bela MoO, MoO, MoO, MoO) MoO, M"", 520.0 533.2 530.4 529.9 529.8 530.3 530.5 528.6 531.3 529.5 530.0 531.2 532.1 529.1 529.6 529.6 530.0 529.6 531.l 530.7 529.9 530.9 531.6 530.4 NajO Nb,Q, 529.7 529.6 00, C,o, 0,,0, H,o HID, hO~ ln lOj lnj0:2 InlO) ",,0, LiJO w2D) Perkin-Elmer Corporation Phvsical Electronics Division WZRSO NFS75, NGDS75, SBBSO HGW75 PKHLSO NGDS75 McC075 NGDS75, WZRSO BGD75 CBR76, 01'0079. I1SU76 BGD75, NFS82, NODS75 HoThSO, OPS76, WZR80, BOrPSI NGDS75 JIKK76 OPS76 YaBaSO YaBaSO HMUZ78, MSSS81, RB072, Seh073b MSSS81, Mct::075, HMUZ78, RBOn, Scho73b NGDS75, WZR80, Kilk73, Limo81 HSU76, NSLS77 Meum MeZe77 MeZe77 McZc77 NGDS75, Scho73a, WZR80, ZSOS79 NGDS75, WZR80 NGDS15, WZR80 NGDS75 Shcr76 NGDS75 CFRS80 LAK77 NGDS75 CSFG79 NGDS75 NFS82, NGDS75 lnYa81 WZR80 OH[75 OHl75 OHI75 NGDS75, WZR80 OHI75 PCLH76 CGR78, KBA\V74 SaRa80 NGDS75, NFS82 PCLH76 SaRa80. KBAW74. I1MUZ78, CGR78 BaSt75 OBPSI Appendix n. Chemical States Tables Nb,O, Nb,O, NbO, NdlOl NilO) NiO 530.6 531.3 530.7 530.6 531.8 529.6 P{l~ ti32.2 532.6 533.6 534.3 528.9 531.6 529.4 530,9 521.5 528.9 527.4 529.0 529.3 529.3 528.6 531.4 530.1 531.9 530.4 529.4 529.4 530.7 530.0 530.0 533.0 534.3 5325 5328 5329 5325 5327 533.2 530.1 530.6 (bridging 0) (bridging 0) P{ls (nonbridging 0) I'{ls (nonbridging 0) PbO PbO PbO.rhombic PbO,rhombic PbO, telrngonal PbO, telrngonal P{l~ PbD, PbD, PdO PrjO) PR), ~O, RoO, RoO, RIljO) RUOI R"o, RuO) SbIO) Sel0l Si0:2 Si0:2 Si0:2 Si0:2, gel SiDl, Yyoor SiOl, alpha cristobal Si0:2, alpha quartz Si0:2, alpha quartz 5"0 5"0, 5<0 Th,O, ThO, TeOl 11\01 TiO l Uo, UO, Y1Dl V,o, Y10 l V,o, WO, 530.5 528.8 528.8 530.2 530.0 529.9 530.4 529.9 530.5 530.0 529.9 530.5 530.4 NGDS75, NFSS2 SaRa80 SaRa80 SaRu80 KiWi74, NgHc76 DPS77, LFWS79, NFSS2, NGDS75, SRD79, WZR80 NGDS15 OMD79 NGDS75 GMD79 NFS82 WZR80 KOW73 ZiHe78 KOW73 ZiHe78 KOW73 TLR78 KGW74 SaRaSO SaRa80 CMHL77 BHU81 BHUSI CMHL77, NFS82 MWLF78 KiWi74, McGi82, SaRaW KiWi74 WZR80 NGOS75, WZR80 BarrS3, KMH78, NGDS75 Kilk73 NSLS77, SRD79 WPHK82 WPHK82 WPHK82 WPHK82 TLR78 ADPS77 AD1'S77, LAK77, MWl.FJ8, NGDS75, TLR78 VaVe80 SaRa80 SaRa80 GBPSI. SBB80 NGDS7S MWLF78, WZR80, NGDS75 MSSS81 MSSS81 CGR78 KKL83 BCM78, KKL83 NSLS77, NODS75, NFS82 CoRa76 Appendix B. Chemical Stales Tables wo, "., ZOO 530.4 W, 530.2 5JO,' 531.4 531.5 531.5 531.2 531.2 z.o, A__Oflh, bayoite A1(OI/h, :ibbsile AIOOH, boehmite Co(OHh O(OHh CI(OHh R(OHh FeO'OH FeOO*H In(OUh KOH UlH Mg(OHh NaOH Ni(OHh AII'O< c.""" c..P,o, KjPO. I4P2OJ LhPO. u.p,o, "'' ' ' Na.P~ (bridling 0) Na.PzOJ (nonbridgin8 0) NaPOJ (bridging 0) NaPOJ (noabridging 0) "NO,), D(NO,J, <No, Pb(NOJ), BaW. """" c.so. O><Sl1b ,<so, K;SO. NiSo. I'bSl1 z.so. N.;;o, NalS20, I'bSOj PbS,o, ..,co, a.co, 'DCo, CdCO j CuCO) Li,CO, 232 5311 531.3 530.1 531.2 531.8 BI.8 531.2 530,9 532.8 531.3 532.8 5JO,I 5JO,2 53<1.4 530.1 531.5 531.7 5JO,4 531.! 532.9 531.5 533.4 5310 m.6 532.7 532.7 531.8 532.5 5310 5311 5)2,4 531.2 5311 5315 5315 531.2 531.8 530.8 531.1 5JO,6 531.) 531.4 531.4 531.5 531.5 Han~book or X-ray Photoelectron Spectroscop)' CoRa76, KMH7&, NFS82, NGDS75, NSLSn NFS82, NGDS75. NSLS77, StOO73, WZR80, ZSOS79 NGDS75 Cseto, WZRIlO LiC1o, 5314 WPHK82 WPIlKSO Tayl82 HSU76 DPS76 MSSS81 HSU16 McZe77 MeZe77 N.c](), 5310 AhSiOs. sillimanilc AIJ5iOs. silhmanile Ca,(HSiOth COlSi(h Na!SiO'" SHt)· WZR80 NllSiOl · 5HP' Kilk73 CSFG79, WZR80 Ni»iO. NiSiOJ MgSiO*)' 2Hjl} 5323 532.0 532.8 531.0 532.0 529j 5JO,6 529.9 532.2 533.5 531.4 532.5 532.7 532.6 532.2 SRD79 ORi16 CIRi16 PCLH76 NgHe16 ACHTIJ HNUW18 BaSt7S LFWS79 CFRSSO MVS13 MVS73 MVS13 MVS73 MVS13 MVS73 MVS71GMIm GM079 GMD19 GMD79 GMD19 a..sW8J a..sW8J NSLS71 TLR78 CLSW83 WZR80 a..sW83. WZRSO OPS16 N.,co, PbCO, 531.6 531.2 5317 532.2 Ket04 KetOl 532.3 RbClGc 5318 AI~iOl, kyanitc 531.3 AI~i(h. mullile 531.6 MgSiOl'21[zO~ Ah(MoO.h AIt(WO.h e.c"" c.MoO. COWO, p.Benzoquinone Hydroquinone PlCOO", p(MeJSi(O» Methylsificone Resin Phenylsilicone Resin PhCONlh 531.3 OsCh 00, 00, Oo(HSQ,), K""'- WPHK82 532.5 ORi76 WZR80 CIRi76 CIRi76 531.9 lJ'WS79 530.6 ".7 "6 50.2 511 '" 5V WZRSO ZiHc78 ZiHe78 Os(NHl)~2h 0s(NHllli'llBr2 HGW75 52' O:l:(NH~iliBf2 51.6 522 WZR80 Os(NI!JhN,cb KPsl;NO)Brj K10s(NO)Ch HOs(Ph]P)CI(CO) CSFG79 o.a.("J'h No'' ' WZRIlO a..sW", CLSW83. WZRSO HGW75 KzOsBr6 K,o.a. K,o.a. K,o.a. K,o.a. Ki>sOl.(OH). AnSw74 AnSw74 531.2 531.6 521 51.9 52.9 510 531 515 519 55.2 50.9 LimoSl WZR80 NSLS77. Nefe82 Zil1e78 \\7JtIlO MVS73 MVS73 MVS73 MVS73 MVS13 MVS13 AnSw14 531.9 Os" '"'" '" HHDOSI, WlRlIl 513 53.4 51.l 52.6 m. ':II NFS82 NFS82 OYK14 OYK74 LBNN7& WPHK82 WPHK82 WPHK82 LBNN78 • Folk13, BNMN79 RHHK70 Nefe78 SaRaSO FoIt13 Ncfe78 Nere78 NcfdS FoIk73 Collen leBrn Ncfe78 Ncfe78 Folk73 FoIk73 FoIk73 FoIk13 Nde78 Nefe78 Hcfe7S leBr72 Perkin-Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy OsOilllPMe2n lrm OsCh(PhPMeJ)J Iller OsOillll'MeUi lrans ,, 53.0 51.1 SI)'1 LeBr72 LeBr72 LeBr72 """"" GaP, anodiany oxid. GaP, thomally oxid. '" 'In'', " In', .,po. ",,po. K,HPO. K)PO. LhP04 NaflP<h NaY'O. NaHlP<h NaPOJ RbJ!'O. NaHjPfh """,0, ",',0, LilP~ Na.PA RbJl207 P.01o OPeh 129.9 130.0 130.0 129.6 129.7 128.8 128.5 129J 128.3 129.~ 128J 129.8 132' 132.1 132.8 133.2 133.6 133.1 132' 134,2 134.2 132.5 132.6 132.6 132.6 134J 133.2 Ill! 135.3 Ph,p 135.7 13SJ 133.4 130.9 Ph,p Ph" Ph,ps 130.9 130.9 1325 Ph"" Ph,po 132.6 132.5 PIlJPBh 1322 132.1 1322 1320 1323 1323 134.3 133.1 134.7 SPell SP(Nrh)1 PhJ!'BBl) Ph,p1lCJ, Ph,FBfJ PhlPSI! ""P&II (PJ>Sh\' (PJ>ShfS (PbOh\' (PhOhPS (PhOlJI'Se (PhO)jI'O (PhOhl'O P2p P (red) Co" Aplicndix B. Chemical States Tables Perkin-Elmer Corporation Physical Electronics Division ~ I'h"POBD!) I'h"POBQ) I'h"PODF) NSD1J75 ScBrSl NSD1J75 NSD1J75 WITa8O, IMNtn9. NIMN78 MIN81 MIN81 CFRSill """ ""PH, ""'" ""PC! Mel'PhJBr NSD1J75 NSD1J75 CFRSOl 1'h2PO{OH) OI'O(OOh 0PIiN'" 0l'O,0O OP(NMe))J (PbJ'hl"·P, (PI1rhPF, MVS13 Pl(P>,P), ""'" Ph,l'=CHCOPh Ph,l'=CHCOOM< CJ,N,Ph"h MVS73 MVS73 Swif82, WRDM79, WaTaSO MVS73, GMD79, Swi182 Swif82 Swif82,GMD79 MVS13 Swif82 MVS13 MVS13 MVS13 MVS7J, GMD79, Bert81 MVS73 NIMN78, NGDS75, CFRSSO, Bert8!. GMD79 F1We75 FIWe75 F1Wc75 Da!c76. NSMS79, TRLK73, GBMP79 HVV79, LMFSO, SRH72 MSAV7I, GZF73 HVV79, STA74, RWe75, MSAV71 HVV79, MSAV71 GZF73, SfA74, AWe75, MSAV7I, HVV79, BNSA70 HVV79 HVV1') HVV19 HVV19 NSWM80 NSWMSO MSAV11 MSAV11 MSAV11 Ni(COh(PhJPn Ph4f Ph Ph Ph Ph Pb """", Pb" PbS< PbS PhI, PbBrj Ph~ PbO PbO Ph,o. PbO, I'h(OHh I'h(NO,j, 1'hSO, J'hS(h I'hS,Q, """"' I'4I'h " Ph,I'bCI Ph,J'bCl, Pb(OAch Pb(OAe). 134.7 134J 133.6 J3.U l3J.7 133.4 l3J.3 133.3 134.8 135.8 135.2 133.4 133.0 133.5 132.8 133.0 136.1 133.5 131.2 132.2 IJ2j 132.4 iliA 136.9 136..01 B6.8 136.8 136.8 136.8 137.4 137.4 137.6 138.7 138.8 139.0 138.9 138.9 138,0 137A 138.4 139.3 138.6 139.4 138.4 137.3 138.2 138.9 139.4 138.5 137.2 MSAV71 MSAV71 CFRSill AWe75 HVV19 HVV1') HVV79 MSAV71 AWe75 AWe75 AWe75 AWe75 HVV19 LMFSO, SRHn HVV19 SRH' I),lF!O I),lF!O Rizgn Dale76, srA7~ STA74 BNSA70 TRLK73 ~ LKMr73 SfS22 BeA8O, K0W73, KiWi73, TLR78, WRDM79, WaTa80 HSBSSI, OCH79 HSBS8l SfS22 SfS22 MoVan, SFS77, 'liHe78 MoVan NeFe82 MoVan KOwn, 'liHe78, WRDM79, NFS82, NSSPSO, MoVa73 MoVan, BeASO MoVan BeRSO, KOW73, TLR78, MoVa73 NSS,,", BeFl8O, TLR78, NSSPlIO Zille78 NSSPll, 'liHe78 ZiHe78 ""82 MoVa73 MoVa73 MoVa73 ""'" ""'" 233 Appendix B. Chemical States Tables Handbook nr X-ray Photoelectron Spectroscopy Pd 3d P,4d Pd Pd Pd Pd Pd Pd Pd 335.1 335.1 335.2 335.2 335.5 335.2 335.3 Agt>PdIO AgsOl'dJO Ag,OPdrO AJ,OPd,O 3J4.6 334.9 334.9 337.4 336.2 336.8 336.2 Mg:rsPd~ Pd~i Pd,5i Pd. PdBo "CI PdO PdOI NatPdo. K,1'dCIo K2Pt1Br. K2Pd(N'h). K2PdC4 BrIPd(PhlPh ChPd(RlJI'h bPd(",P), (CNhPd(",Ph ",(Ph,P), ChPd(~P)l Pd(Ph~ Pd(OAch Pd(SPhh 336.4 JJ1.l JJ1.8 336.3 337.9 338.0 338.2 JJ1J 339.0 340.2 337.8 337.8 337.5 338.2 336.6 342.9 336.0 338.6 337.7 $ NyMaSO BiSwSO BiSwBO BiSwSO JHBK73.Asam76 WRDM79, WtAnlltl, BHHK70, Scllon. GGM82, KBAM12 WcAn80 -"so W<A"", W<A"", WeAnSO GGM82 AWUQ KBAM12 KBAM72 KBAM12, NKBP73 KGW74 KGW14 SeTs76 KBAM72. NKBP73 KBAM72 KBAM12 KBAM72, Nefe78 KBAM72 KBAM12, NSMS79 KBAM72 KBAM72 NSMS79 BNSA70 NSMS79 NSMS79 BOffin I'd MNN Pd A""PdP A""P<W A&!OPdIO At.OPlhQ MglSPdn Pm 3d PmCI, Pm4d PmClJ Pr~l 1'<0, 234 "" " "PIS; 71.2 71.0 71.2 ",s; "CI 725 "C~ "0 1'<0 "0, "'" P1(OH)l K2Pll6 KlPlBr. K2P1Br, K2Pl:U K2P1CI. K2P1C4 K2P1F, Pl(NHJ).Brl Pl(l%hCIl Pl(NHJ)'Cb P1(NHlJoCI. Pt(NHJ)z(NOm Pt(NHJMNOili K2Pt(OHlri K2f'1(N0V0 K2f'1(N~Ji WcAn80, WRDM79 W<AolO 71.2 73.0 73.6 15.5 73.8 74.2 74.6 75.0 n.6 73.4 72.6 74.6 73.0 73.4 15.4 77.6 73.4 73.2 73.4 76.3 73.7 74.4 75.1 74.1 15.9 72.4 71.4 71.4 _olO WeAn80 WcAn80 OIPl(PhtPh cis Q 2PtO'blP)z cis O.Pt(EiJPh ClIPt(EhPh HCIPt(EltPh 1033j MNTB70 o,l\{Ph,P), 73.0 Pt(SPhh Ph,PPt{SPPhl) ChPt(EllPh hl'l(EllPh hPl(f\.1cJlh cis hPtCMe.tPh traItS hPttCHJCONH). Br2Pt(CtbCONH). CIIPI(CHJCONH). 718 """'" 128.3 MNT1l7Q 931.8 933.2 935.3 $ SaRa80 SaRaBO "'oM SaRaSO PI4f 327.8 328.8 329.1 329J 315.5 326.4 "'3d '" """ """ 116.1 116.2 (NH.)lPtCl. Pt(Ph)!lh "(Ph"" 71] 73.0 15.3 75.9 716 11.8 13.1 72.5 716 711 74.6 14.9 74.8 m. W' $ lHBK73 BHUK70, KW07I, Nefen, &0072, WRDM79. Wagn75 CMHL77, CaLe73, HaWi77, BACB75 GGM82 GGM82 EPCCl5 EPCC75 KWD71 EPCCl5 KWD71 EPCC15 HaWi77 SNMK18 SNMK78 SNMK78 CMHL77, EPCC75, SNMK78 Wagn75 Collen, EPCC75, LeBr72, SNMK78 SNMK78 Nefe78 CMHLn, Neft7S SNMK78 SNMK18 Nefc78 CMHLn SNMK78 SNMK78 SNMK78 KaEl19 Nefc78 Rigg72 CAB71 Riggn LeBr72 Nefe78. Rigg72 RiUn Rig:72 BBFRn Ne5a78 Rigg12 Rigg72 CAB11 CAB71 NeSa78 NeSa18 NeSa78 Perkin·Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy 0,zI't(H2NCHJCH!NHm Qzl't(cydooctadim) KIPlC\ 710 719 318.1 EPCC7S 196<>.7 21)41.1 Wago78 Wagn78 YMK78 CMHLn Pt MNN ~ " Rb3d Rb RhO RbN, Rbi RbBr RbC1 RbF R_ RboP"" Rbe'" ilLS 109.9 109.8 110.4 Ro no Ro Ro RoO, RoO, ''''<CIo a,Rdl(Ph>1'h Q,R<N(Ph,p), a.R«El,p, (\Rc(PMe:!Pbh C1 jRc(I'MeIPbh. mer OlRc(PMClPbJ.. uw C1ReNi:I'MtJ:A1)., trans •• 109.9 109.8 110.0 110.0 110.4 40.3 40.S • Re 4r 4QS 41.0 43.6 468 442 419 417 413 416 41.8 "",WOo "'bO. RbTaO. RhVo. K,'hClo SGRS72 MVS73 MVS73 MVS73 MVS73 MVS73 MVS73 MVS73 lJo.O Appendix n. Chemical SUiles Tables FJ-IRSO SSHU83, WRDM79 RHUSI BHUSI BHUSI CoHen, LeBr12 Folk13. Ncfe1S Nefe78 '-'Bm '-'Bm 4QS '-'l1<n '-'l1<n 40.3 LeBrn, FoDm KIRhF, KJRh(NOJJ. K)Rh(N01J. Rh(NHj)J:!] Rh(NOJ.O) C1Rh(Phlfl» a,R1(Ph,Ph C\Rh(Ph,Ph B<oRh(I'h,I'h NORI(1'h,P), a,Rh(I'h,P),M<CT< H(COjRl(I"',p), C1(COhRb(Ph,p) CI(CO)Rh(PluPh CbRhI(cyclooctadih RhiOAc).·2H10 Rh(NHt:H1COOh' H2O Rh Rh Rh RhI, RhO, RbCh ·3Hil RhCIJ· 12H:oO Rh,O, Rh,o, B""",,, BoRhA DRhA CoRbp. PbKh2O.c KRhOl LiRh01 307.2 301.2 307.2 30<. 310.[ 310.0 310.1 30<' 30<2 30<4 30<' 30<8 308.8 308.6 308.5 308.9 • NyMa80 OIlT19, WRDM79, FHPW73 Nefe78 0IIT79 CWn82 CMHLn NFS82, CMHLTI 0IIT79 NFSI,· NFS82 NFS82 NFS82 NFS82 NFS82 NFS82 Zo'hA 30&7 NFS82 RhjMo(% 309.2 NFS82 Perkin-Elmer Corporation Ph)'sical Electronics Division 309.' lO8.5 30<7 30<. 308.7 309.0 310.3 Ru 3d NFS82 NFS82 NFS82 NFS82 SNMK78 Nefe78 SNMK78 SNMK78 Nefe78 Nde78 CWH82. Nde78, 0ITT19 CWn82 Nefe78 Nefe78 Nefe78 OlWa79 OIIT79 Nefe78 CWIl82, OIIT19 CMHL77, CWH82 Nefe78 NPBS74 • R, R. R. 18111 18110 18111 RoCI, RoO, RoO, R.o. 281.8 18117 28ll RIl(NBJ)sNlll 2812 2805 28?S 27&6 LeBr12 164.0 164.1 • Ru(NHM~lBr1 Ru(NHM~:Ch ChRu(PhPMelh mer Rh3d 309.4 309.2 3095 309.2 3098 3122 310.5 311.1 310.5 309.8 301.4 309.7 309.7 lm.' .lO8.2 2833 S 2p S S .., CdS CdS eo,s A." CdS CdS ""F", Gajo.';' G" G<S, HgS MoS 1601 161.7 1620 1613 1624 1620 161J 16\.6 162.9 162.2 161.8 161.1 162.0 162.5 NyMaSO Folk73. BHHK1O, KiWi14, FEMY77. WRDM19 ",~73 SlRaBO. KiWi14, McGi82 KiWi74 KiWi14 ",~73 Folk13 Folm SNRS76, WRDM79, RiVeS3. LHJG70 SiWo8O BSRR81 Urro81 BSRR81 NSS"" Umo8I. NSSPSO BSRR81 Bind73. LimoSl Bind73, UrnoS! llWB12 SFS77 HKMP74 NSSPSO LimoSl '" Appendix B. Cherni",' Slales Tables MoS, 162.5 SSOTS!. StEm. PCLH76 N"s N,oS NiS '''' SWlI7I PbS 160.8 Sb,S, 161.8 161.1 161.5 ""us, US 161.8 162.2 162.6 WS, WS, W 162.1 163.0 GeS1TeAsl N»(55'O,) 161.5 161.6 161.6 162.5 161.7 167.1 ,,so, 167.5 NatS~ 165.6 166.6 167.2 168.6 GeSJASl KFeSl Nat(S·SOJ) NaiS-SO)) Na1S0J Na§(h A.,so. Al,(so.h a.so. CaSa. COSO. CoSo. 164.0 ,,8.8 168.8 169.0 169.7 169.3 "",a. ,,8.8 F<,(so.h 169.1 169.1 ,,so. mo LHlG10 ShRe79, NgHe16, DPsn SFSn BOt" SFm SNRS76 SNRS76 Nglle76 Wagn7S LimoSl HKMP74 HKMP74 Bin:l73 Wagn7S UilGlII LHJG'Xl TMR80 SWH71 WaTa82, lllJG70 TMRSO TMR80 LIUG1II SiWoSO, a.sW83 CLSW83 Limo8l WaTa8O, NSSPSO, Um08J Lidl. UUG71l LHIGIO TMRSO LimoSl TMR80 Udl, NSLS77, Nefe82, ShRe79 MnS04 Na}S04 NiSo. 168.8 169.2 PbSa. 168.' NSSP80 srSo~ z.so. 169.1 169.1 169.s No,so, 166.8 SoN> 164.6 174.4 177.2 167.4 168.1 168.1 170.0 162.3 163.7 163.5 174.4 163.7 163.7 163.3 163.1 163.2 CLSW83 Chad73 Nere82 BCM18 SOI077 WaTa82 LHJG70 WaTa82 UilG10 U(SO~h SF, SF, SO, So, soa, SOF, SP(NH)n SPCb S,a, S,a. CS, (CHJCQOHhS (CIIIPhhS PhSH PhoS 236 Handbook of X-ray Photoelectron Spectroscopy Ul1070 LlUG10 FlWe75 FlWe75 LIllG10 LIllG10 UilG1ll LHlG1II LHJG70 LHJG70 LHlG70 Ph,ps Ph,PS P11)AsS PhSSPh PbClhSSClhPII l!'l>SbP l!'l>SbPS BuSSBu MeSSMe NHJCSNH2 2·Mm:apIObenrimidn 2·Mereapobcnzimidll. BuNH3 HSO; lJu;NHS04 ElJNHHS04 1'hSCM" TetRthiouplthalc:De Cysteine Cysceine 110 hydrate Cysteine HO hydrate MClbioniJle NBMH.SO»H 1M"". M,,so (PhOhhSO PhlSO "',so, 164.3 161. 161.8 161.7 164.4 164.2 163.6 163.5 164.1 164.3 1611 162.2 162.8 167.] 168.0 168.5 162.4 164.4 163.2 163.1 163.6 162.8 161.8 164.s 166.' 165.9 166.0 169.0 OiJOS(O)OQiJ ,,8.4 """'" 169.3 168.5 166.3 167.9 ~CH~ PhS01Na p-NHl4H.SQMl4NHr p-Nth4H.tS02NHI "'~ p-NfuCJioSOJNa p-O:!NCJt,SNa COlN411~SH oWl",",," ~CJt.SMe o-OIN4H.SNH1 o-OzNc.H.SCJ p-(hNCH4S01F o-OJNCl-I.S01F PhOl»SCJhPh PbQI§tSOCJhPh PhOhSS"OCH1Ph PhOl§tS01QhPh PhCH~S·O:zCH1Ph (OhhS+I. (CHWS~OII· (HOOCCH>hS<Oi,coo. 168.. 168.' UilGlII AWe7S. MSAV71 HVV79 HYV79 RiVeS3, UUG70 RiVt83 MSAV7I MSAV11 RiVeS3 RiVeS3 LeRan, NBM073, SrWaTI YYS79 "'''''' EvRe81 EvRe81 EvRc81 PiLu72 RiVeS] L1Ma19, LHJG70 SSEWJ' LHIG70 BBFR77 HaSIl?3 UilGlII LHlGIO LHIGW LHJG71l LHlG70 UilG10 LHlG7lJ LHlG1ll LHIG7ll LHJG70 LHlO;,) LHlG;,} LHlG1ll LHlG1ll LHlG7ll UUG70 168.1 161.0 163.5 163.9 163.5 164.1 163.9 169.6 170.0 163.6 163.7 165.9 163.9 168.0 165.8 168.2 166.2 LJUG'70 LIUG1II LIUG1II LHlG70 LHJG70 LHlG70 LHlG1ll LHlG1ll LHJG70 LHJG70 LHlG70 UilG1ll LHlG1ll 2116.1 2115.9 WaTaSO W",,18 SKLL NiS NiW§ IT\. Perkin-Elmer Corporation \ j ! Physical Electronics Division Handbook of X-ray Photoelectron SpectroscOIJ)' WS2. """" ~SS*O.ll NaiS*SOiJ a.So. so, SF. 2115.6 ".,., 2107.8 2112.5 2108.0 2106.2 2100.5 Wap78 WaTa82 Wagn15 Wagn75 WaTa80 WaTaS2 WaTaS2 Appendix S<2p S< 398.6 """ 401.8 S< S<N Sc:-O, C1Sc(C l lhh Sc(C~H.\XC,HI) 51) 3d512 Sb Sb A.b Sb"So, Sb,S. Sb>'. Sbb SbCl, SbFJ Sb,O, Sb,O, Rb,.lIblBr, Rb,J$bll, Cs1Sbll, Cs1SblBl't C"SbA c.,sbA C"",," Co(NHillSbBr, Co(NH,~ KSbF, KSbF. NLIbF. C&F, KSb,F, K1SbFl Na~bF, BuNH,$bt. BuNH,5!J..lI, E4NSbF6 Pb,sb Bu.JSb PltJSbBrl Me,sbBrl Pb,sbS {C,tHnhSSb """""'" SbMNN Sb Sb~J Sb~s Sb!Ol KSbF, 528.3 528.2 52&.6 52&.0 '''5 529.2 ,,0., "<l9 531.1 530.0 BO.8 529,9 529.9 529.2 530.0 529.3 ,,0., 530.9 ')0.1 ')0.' "23 5329 5321 BO.6 53L2 BLO 531,3 529.6 529.9 B14 52&.9 52&.1 '''J ')0.3 ",.1 529.8 531.7 464.1 4611 462.2 462.1 454.4 Perkin-Elmer Corporation Physical Electronics Division • HSBSBI,MSV 13,PVVA79, SFS77,WRDM79,Wagn15 MSV73 HSBS81 MSV73,Wap15 MSV73,Wagn15 MSV73 BCH15 MSV73 MSV73.Wagn15 MSV73 Tric74 Tric74 BCH75 BCH75,Tric74 BCII75 Tric74 Tric14 Tric74 Tlic14 MSV73 Wagn7S Be"" aCH15 Tric74 Tric74 Tric74 BCH75 aCH75 BCH75 aCtf75 BCH15 Be"" BCIf75 BCH7S MSV73 MSV73 WRDM79. PVVA79, Wagn75 Wagn75 Wagn75 Wagn7S Wagn75 Se3d S< S< S< "'' '" ""' G<S< G<S<, CulnSe:z In1SeJ NbJ5tl NbS. PbS< PbS< S"S< SoS< MoS<, ""'" S<Q, S<Q, """" """" ">S<O, Na~J Na1SeO. Na~eS.o. Ph1Se (BrCJ{.hSe PI"S. ,,"""'»S<, (CI4H~h 1,&"'" 39<' 400.7 401.9 401.4 400.2 55.6 555 55.1 55.1 54.6 54' 545 54.0 54.' 54.9 517 514 54.1 517 55.0 54.6 ><' ", 59.8 59.2 59.9 61.2 59.1 61.6 ,., 55.8 '" ,., '"' S5.S '"m Cl,S<Pb, '''''''''' 57.1 a~l C"H""", '"57.1 HSd'b,I' S<PbI Pb>S<O (PhCHiliSeO (BrCJ14)zSeO (C.HsCQOflhSeO PhSeO(OHj C14HoSeO(OH) 54' 543 ,,. '" '" 58.4 58.8 59,3 n. Chemical States Tables •• SMKMn STAB76 NGDS7S,WRDM79 WcMe78 WcMe78 • Sfo'sn. BWlao, l.IcQ182, WRDM79, wsm, MllIB71 ,W"" UeOd82., WSP77 m82, l1WBn SFSn lJ<Od82 KJIOSI KIIOS1 Bnh175 Bnh175 SFsn WSP1 SFSn wsm 'WI79 'WI79 BWlSI. IT182 MTHB11. WSPT1 BWISI MlllB11 BWISI WSP17 WSP77 WSP77 BWISI MTHB1! aWISI BWISI MllIB71 BWtBl BWI8I aW1S1 M1lIB11 MlliB71 NSWMlll HVV79 aWISI MTIlB11 MTHB71 MTHB11 MTIlB11 MTIlB71 Appendix B. Chemical States Tables FCJi.'<O(OII) CJCoH&{),(OH) (MeCJ(4Il.chScOl (HOC1H..snse 59.3 60.2 60.0 Handbook or X-ray Photoelectron Spectroscnpy M'ffiB71 MTliB71 MTliB71 ,<2 wsm 1301.0 1306.1 lJOU 1l00.8 1297.9 aWI81 WarJl75 aW1S1 sWI81 SWI81 Wagn75 BWl81 BWISI BWISI BWI81 aWl81 SeL!\IM "" "'" H_ H?5eO~ Na<StOJ non ""'""""" 1304.0 1304.3 1l02.1 13Ol.' 1301.9 '''''' Q,Sd'h, I'l>,S<O Si 2p 99.3 1013 995 & S<h ~ Si, p-Iype Si, n-1ype SUIOO) !'<,Si MoS, MoS, 98.9 NhSi NiSi NiSi PdJSi PdJo'ii P1JSi P>Si 9&8 9&' 99.1 99.6 99.8 100.5 100.5 Si~ 1Ol.8 SiS2 SiD, 103.4 103.6 "" SiOl, Vycor SiDl, qUU12. SiD" oJ,.. """"" SiOJlCl NilSiO. NiSiOJ AhSiO l , kyanite A~SiOs. mullitc AIJSiO), sillimanite NaALSiA, albite BellCr1ile II Ztolon Zn.tSh(},(OHh ·2Hll 238 99.0 100.0 99.1 995 99.6 99.1 103.5 103.7 1033 1014 102.. 103.3 102.8 103.0 102.6 102.6 102.. 103.3 102.0 •• A\VlM. PADS78. WRDM79, WPHK82, 1ay181, KBHN74 HBSK72 HBBK72 11..R78 ShTr75 Wi'll"" BrWh78 GGM82 GGM82 AW180 GGM82 AW1.8O WaTaSO GGM82 GGMS2 WHMC18, WaTa8O, TayI81.1U78 MoVa1J KBHN14, NGDS15, MoYa73, Barr83 WPHK82 WPHK82, TLR 78 WPI-IK82 WFtlK82 lFWS19 SRD79 AnSw74 AnSw74 AnSw74 Wi'll"" a"", WPHK82 WPHK82 Hydrolysa;lalite JUoIillde KaoIi.ite Mica, Muscovile Natrolite PyrojXJyllite AlSiOs, sillimanite LiALSiA, spolklmellt Talc. Mg)!i40.0Hh WoIlaslOnii.CaJSi,o, Mol Sieve A Mol Sieve A Mol Sieve A. Ca fllll11 Mol Sieve X Mol Sieve X Mol Sieve X, Ca ram Mol Sieve Y Mol Sieve Y Mol Sieve Y, Ca form Klo'ii~ Na:}5iF. p.MdbyisiL (IiDw) p-MethyisiL (resin) p-Phel'Jylsil. (resin) M~Si Pb.si Pb.si Et,sill E1Jo'iiOH Et,siBr EtjSiCI Et,siF F.lJ5i01 ElSie!] (CHFCHJ,.Si MeJSiSiMe) M~iOSiMeJ Ph,5iSiPbJ PhJSiOSiPh, 101.7 102.1 10lO 10204 102.2 102.9 102.7 102.5 lOll 102.. lOlA 101.3 101.8 102.2 102.2 102.7 102.8 102.8 102.8 I(M.6 104.3 102.. 102.. 102.7 100.5 100.1 101.2 100.1 101.1 101.0 lOlA 101.8 102.1 102.. 100.1 100.5 100.9 100.7 101.3 WPHK82 """ WPHK82 WPIIK82 WPHK82 WPHK82 WPHK82 WPHK82 WP!IK82 WPHK82 WPHK82 BarrS3 "n83 WPHK82 """ "n83 WPHK82 BarrS3 BarrS3 MoVa73 NSLSn WPHK82 WPHKS2 WPHK82 GCH76 MoYa73 00176 GCII16 GCH16 GCH76 GCH76 GCH16 GCH76 GCII16 GCII16 GCH16 GCH76 GCH76 GCH76 S;(KLL) 50 MoS~ PdSi SiJN~ SiD, SiD,,_ S~,quanz SiDl, aljXJa aistobal Si~ gel NaAlSi,o" albite II Zcolon Hemimorphilc Hydroxysodalilt Kaolinite Mica, MllSCOvite 1616.6 1611.2 1617.4 16126 ,'' '-, ''''' ' ...6 1608.8 1608.3 1609.3 ,'' '-. 1610.5 1610.7 1609.0 1609.6 m WPHK82, roN 77 WPHK82 WaTa80 WaTaSO KBHN74 WffiK82 WFtlKS2 WPHK82 WPHK82 WPHK82 WPltK82 WFtlK82 WP'tlK82 WPHK82 WPllK82 Perkin-Elmer Corporation \ j I Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Natrolite Pyropbyllitc A1SiO}. sillimanite LiAISiIO.. spodumenc Talc, MSJS~Olo(OHh Wollastonii, Ca)$i,Q, Mol Sieve A Mol Sieve X Mol Sieve Y p-Methylsil. Oincar) p-MclhylsiL (resin) p-Phenylsil. (resin) 1609.6 1609.2 1609.5 1609.6 1608.9 1610.0 1610.1 1609.4 1608.6 1609.4 1608.8 1610.0 8m 3d512 Sm Sm SffijOJ 1081.1 1081.2 1083.4 8n 3d512 S" S" S" S" 485.0 484.9 485.1 485.0 Sn alpha Sn beta Ag9lSnS 485.0 484.6 485.6 485.2 484.9 485.3 485,6 485.2 486.4 485,2 485,6 485.7 485,6 486,9 486.7 481.0 481.0 486,0 486,9 486,7 A,s" AuSJ14 Cdw' 5Sn' OOs C~Snj [n9lSnj P~Snj S~SIl5 SoT> SnSe SoS SnBrl SuCh SnFl SnFl SoD SoD SnO) (NH4hSnC!I; BaSnCk Ba(SnCbh KSnFj KISnF, NaSnFl Na~nOl Na2SnOl Na~nOl Ph,S0 PI4Sn 486.1 486.8 486.8 486.1 487.6 487.4 486.2 486.7 487.2 485.1 486,3 Perkin-Elmer Corporation Phvsical Electronics Division WPHK82 WPHK82 WPHK82 WPHK82 WPHK82 WPHK82 WPflK82 WPflK82 WPHK82 WPHK82 WPHK82 WPHK82 • DKMB76 WRDM79 • NyMa80 SFSn WRDM79, PYVA79, LAK 77, Wagn75, OCH 79 Hcgd82 Hegd82, HSBS81 HSBS81, Hegd82 FHPW73 FHPW73 Hcgd82 Hegd82 Hegd82 Hcgd82 Hcgd82 SFSn SFsn SFsn GZF73 WVV79 MoYa73 MoVa73 ADPS77 WYV79, MoVa73 LAK 77, MoYa73, WRDM79, NGDS75, WYV79 GZF73 WVV79 WVV79 GZF73 MoYa73 Wagn75 MoVa73 Wagn75 ADPS77 WVV19 MoYa?3 Appendix B. Chemical States Tables 487.1 486.3 487.5 487.5 486.3 487,0 487.6 486,2 487.3 485.6 487.3 487.2 487.2 486.7 487.1 487.0 485.6 487.0 486.1 487.0 HWYV74 WYY79 HWVV74 HWVV74 WVV79 MoYa13 HWVV14 WVV19 HWVV14 WVV79 WVV79 WVV79 WVV79 WVV79 WVV79 WVV79 WVV79 WVV79 OZF73 GZF73, WVV19 S" 437.4 S"S SnOI NaSnFl 435.7 432.7 430.8 431.7 PVVA79, Wagn75, WRDM79, LAK 77 Wagn75 LAK77 Wagn75 Wagn75 ""S" Ph)$nl Ph.Jo'jnl Ph)$nBr Ph)$nCl Ph.Jo'jnCI Ph)$nCI Ph)$nF Ph)$nP Ph)$nOH CLtSn(pyridineh CbSn&(pyridineh ChSnPh(pyridineh Me)$nF MC1SnF2 Me lSnS04 Bd~nO Br6Sn(Et 4Nn CbSn(Ml'-lN) CLtSn(Me:JSOh SnMNN Na2SnO~ S,3<I S, S, S"' SrFI S,ro, SIS0. Sr{NOln SrMoO. ScRh,O. Ta4f T. T. T, T' T.S TaS, TaBrl TaCh 134.3 134.4 135.3 133.8 133.2 134.3 134.1 133.5 133.0 TaJOj 21.9 21.6 21.6 21.9 26.6 26.1 26.9 27.3 27.8 26.1 KTa04 RhTa04 KiraF J 25.9 25.8 29.4 TaF~ • VaVe80 VaVe80 WRDM79 CLSW83 CLSW83 CLSW83 NFS82 NFS82 • VHP.82 MSC73 WRDM79, WaTa80 MSC73 MSC73 MSC73 MSC7J MSC73 SaRa80, MSC 73, NFS82, NGDS75 MSC73 NFS82 MSC73 110 Appendix B. Chemical States Tables QzT..aIl(H!Olt·4HJO Br6f!'I6CI12XBll.lNh C4(Tflt,aI1XE\.iNh 25.8 26.3 26.2 Handbook of X-ray Pholoeledron Spectroscopy 8<"'19 8<"'19 BeWa79 TeMNN T'TeBl) ChTePl1., Bl)TePIQ hTeAll 49'2.2 48703 486.1 487.1 4855 485.1 486.4 485,5 48603 486.6 487.8 hTeEh 487.' Ph2TCl BrircPh bTePh !}TeMC1 p-lOIylTeOOH Br)TeBu 488,5 486.8 488.2 TcC~ TaMNN To T"" 1674.8 Tb4d Th Th,o, 1bO> 146.0 148.7 149.2 Tb3<l Th Th,o, 1bO> Te JdY): T, T, T, T, T' CdT, GeTe """""'1< 1242.0 1241.5 1241.4 513.1 573.0 513.0 5110 m.T sno3 sn.7 5no3 Nb,T~ '722 S71. NbT~ 5n.8 PbTe SnTe VIle, 572.0 sno3 N~Te Uf. "'T, T," TeBll T<O. T"" T"" 5n.9 513.0 '72.9 515.8 576.7 576.9 515.1 576.6 Te(O~ m.l (NH.hTeC16 (NH.lJTeO. 576,9 576.5 5155 576.8 576.2 576.2 575.4 ",no, NIITe<1 C1JTePh1 BrlTePhl bTePh) bTeEi1 Ph1Tez Bf)TcPIJ IjTePh IzTeMC) p'lolylTcOOll Br)TeBu 515.3 513.9 576.6 575.8 575.6 576.1 516.6 WaTaSO • ".... • SaRaSO SaRaBO SaRaSO • T"" Te(OHJr, (NH.hTtCI6 NalTeO~ 486. 486. 486' NyMa80 SFSn PVVA.79, WRDM79. BWtn,BmI75 SNRS76. SWH71 SBSSO SFS77 SBBSO SWH71 B""" Bahl75 SFS77 SFS77 SNRS76 SNRS76 SWH71 BW177 BW[77 BW177 GBPSl, SBRSO SWH71 BWI71 BW177 SWH71 SWHll Wa&n15 Th 4h12 Th Th ThO, ThF. 333.2 333.2 334.4 336.5 • WRDM79 VLDH77 WRDM79 Th 4d!ll Th ThO, Ti 2p Ti T"" TI TI TI TiB) TIN Toa. m T"" TiOJ {anatase. rutile} BaTrO) (cubic.Idn1.) CaTIO) BWm !'bTrO) BWI71 BWI77 BWI71 BWI71 SIr"" Chli(CjH.I)) CIT(CVisll TI(CjH.sXC.h) 67503 6755 454.1 458.8 453.7 453.9 453.9 454.4 m.8 FBWF7' VlDH77 •• 459.2 458.5 458.9 458.6 458.8 457.1 455.8 455.4 ALltP82 LANM81 NSCP74, WRDM79 MECC73 STAB76 MRVgJ SPB76i NSCP74, SPB16a. WRDM19, NGDS75 MWl75 MWI15 MWI7' MW175 MWI15 GSMJ14 GSMJ14 GSMJ14 419.1 WRDM19 '585 m.l 458.1 BWm BWm BWI77 BWI77 BWI17 TI LMM TI m 240 WRDM19 BW178 BWl78 BWl78 BWl78 BWl78 BWl78 Wago75 BWI78 aWI78 aWI7S aW178 aW[78 BW[78 aWl78 aWl78 aW17S BWt7S !)erkill-Elmer Corporation ' " Physical Electronics Division Handbook of X·ray Photoelectron Spectroscopy TI4I 11 11 111 11B' m l1F TJ,S TJ,S, 11,0, ChTI(pyridineh C~TIiPhPEl')J 111.7 $ 111.8 ,,8.5 MBNg). WRDM19 MSC73 MSC73 MSC13 MSC13 MSC13 MSC13 MSC13 WaltTI WallTI 1191 119.0 119.2 118.7 118.7 117.5 118.5 117.9 Appendix 8. Chemical States Tables V 2p V vI» V V V V V v"' VN v,o, yo, v,o, Tm4d 1'111 175.4 U4rm U U U,TCl Iff" US< us.. US US, U"" UII<, Ua, Ua. Ua, UF, UF, UF, UF, uo, U,o. U,o. UO, UOBr UOBr, UOCI UOCI, UO!Br U(hBr, uo,a, U<J,/\ U(SCMl UO!<NOlh ' 6HJO U(IQC). UQiAtOh·2H,Q COUO, LhUO. K,UF, 377.3 377.2 J80.1 381.3 380J 379.1 J80.1 379.4 378.4 319.9 $ VRPC74, Chad73, WRDM79 SNRS76 SNRS76 SNRS76 SNRS76 SNRS76 SNRS76 THVl82 THVl82 J783 TB~2 380.2 381.9 380.1 3m 382.7 3816 380.0 381.0 379.9 381.7 380.1 380.4 380.0 380J 380j 38LJ 381.6 3829 381.6 3820 379.7 381.0 380.7 381.4 382' THVl82 TBVL82 THVl82 TBVL82 Ch>d13 TBVL82 VRPC74, Chad73. MSSS81 Chad73, ChGr72 HoTh79 MSSS81, Chad73, ChOm TBVL82 TBVL82 TBVL82 TBVL82 TBVL82 THV,", THv,", TBVL82,Chad73 a..m a..m Ch>d13 Cbod13 a..d13 Ch>d13 PMDS17 VOCh YOSO. CsNO. RbNo. NaNo. Li,Va. Rh.No. K.V(CN~ V(acach V(Xaach aV{CsHsb V(CsH,), V(CsH.!XC:lh) <D $ $ 512.9 5133 LANM81 WROM79, NSCP74 KKLXl SMKMTI RoRo76, lFS 73, Fm,75 MECC13 RoRo76, STAB76 aJR78 KKL83 NSLSTI, NSCP74, WRDM79, NGDS75, NFSB2 LFS73 LFS73 NFS82 NFS82 NFS82 NFS82 NFS82 Vann76 LFS1J LFS1J GSM/14 GSMJ74, BCDH73 GSMJ74 472.0 ....6 468.0 WRDM79 KKJ.83 KKl.8J 516.4 515.9 516.9 516.9 5173 5175 516.9 513J 514.2 515.1 513.s VLMM v yo, VI» W4r W W W 31.4 31.4 31.4 we we WS, WB" WBr, Wa. woo. wo, 3J.S 32.2 33.2 ~3 35.9 ~9 Wo, 37.2 32' l4J 35.1 Wo, 35.1 WI{J~ Ab(WOth ~1 COWO. H1WOi H,WOI 35.0 35.3 36.2 36.0 ~wo. Perkin-Elmer Corporation Phvsical Electronics Division 1121 511.4 512.1 512.3 512.9 513.4 512.4 513.2 514.4 515.7 516.3 517.6 •VHE82 WRDM19, CoRa76, COR 7B. BiPo73, NSLS77 CoRa16 MSC13 Wagn75 MSC13 MSC13 MSC73 MSC73 CGR78, CoRa76, NgHe76 BiPon SaRaSO, CoRa76, COR 18. BiPon, KMH 78 NFS82, NGDS75 BiPon Nefe82. NFS 82 CGR78 RiPon NFS82 '" Appendi, B. Chemical Slates Tables LiJ:Wo. N~Wo. Nac.,WO) NilQ.1WO, NiWO. Rh I WC4 (NH.l6WA·4H;P K1WC16 Cl j W(EtJPh CI,snW(COn<CsHs) Pl"rW(CCh 36.0 36.3 35.8 35.6 35.4 35.6 303 34.' 34.6 HandbOOk of X-ray Pholoeleclron Spectroscopy NFS S2, MSC 73 Wagn75 BiPo13 lliPo13 NgHe76 NFS82 BiPo73 Lesrn 3>' LeBrn WWVV77 31.6 HV"" 1.o~, 1.o~ 1.01, ZnBr2 z.a, z.a, 1.o~ 1.o~ 1.00 1.00 Zn(""h (MC4N~r4 z.so. Xl' Jdy} Xe in graphite Xc in Ag Xc in Au Xc in Cu Xc in Fe Xe in graphile NoJ<"" 669.1 669.6 668.' 669.6 670.2 669.1 674.1 XeMNN Xc in Fe Xc in graphilC Na.X~ 544.8 ,.." ~ CiHa74 CiHa?4 W3gJl15 WROM79 Wagn17 .... " WRDM19 1.0 9921 Z" 992.1 99V 989.1 '88.1 C..z.. z.s ZnI, Wagn17 V 1>6.0 ~ V VA LS5.8 156.8 NyMa80 WRDM79, NGDS75 ZnF, ZnF, ZoO ZoO ~ 1.00 Zll(acac12 Zn.sil).,(OHh· 2HzO Vb4d V"", 1824 1813 182.7 [85.4 Zn ZP3i2 HHL70. KEML74 lPWF7' HHL70 • 1.0 1.0 Z. 1021.8 1021.9 102\.8 1.0 1021.8 1021.6 GaWi77, KLMP74, MaDu77, SchoBa, KPML13, K1He83 WRDM79, Wagn7S, SMKM77 VooOT/ lOll. GaWi77 c..z.. z.s 1021.4 1020.' 1023.1 1022.0 1022.1 1021.7 Gawm, SATon Wagn75, SATD73 KIHe&3 SAmn Gawm Wagn75 Scho73a, WRDM79 GaWi17 Wagn75 EMGK74 Ncfe82 WPHK82 BOFPSI NFS82 ZnLMM S41.4 Vb Vb Vb 1023.1 1022.2 1022.8 1021.8 10215 NSDU15 NSDlJ/5 aHa? V3d 242 Wi2OJ(Olih' 2HtO ZnCrIl. 1.oRh,O. 1020.6 IOW.9 10210 10214 1021.9 lANM81. LKMY13 1.0'0 ZnCb "'3 989.4 986.2 GaWi17, KlMP74, MaDlIn, S<:ho73a, KPML73, K1Hc83 WRDM79, Wagn75 Vo.on GaWi17 Gawm Wagn75 K1He83 GaWi77 "'" ,.,,, "","" 988.2 KIHc83 Wagn75 WPHK82 !l88.5 987.7 987.3 S<ho'" GaWi77 Z,3d Z, Z, Z, Z, 17&.9 178.8 178.3 118.9 K1JFj' H2O BrJl40HhCHJCHNHJC 1812 ISB 184.2 1817 184.7 181' QZJ{OHncthCHNHzC 1810 W, aF, Kluf(, K"'~ if\. W' ~ NyMa80 NSCP74 WRDM79 SaRa8O, NGDS7S, NS0'74 NKBP73 NKBP13 NKBP73 NKBP73 KNPP74 KNPP74 Perkin-Elmer Corporation Physical Electronics Division Appendix C. Chemical States Tables References N{)/t: ]ht reftrtnus in the Chemical Slalts Tab/es an madt wilh IhfU orfOlU Itltm II'hiclr rtJlTUtni Ihe aulhon' initials. Thru or four capital leQm intiicale thrte or more authors; alternating upptr· and lowtr-case letlen repreunl two Qu/hort (the letlm art! the ftrSllI«J ltllen of tach last namt): and a CQpilalltltu followed by three iOWlr ca.ft /tllers indicmis Q single author. The initials QI"l! lal/owed try IWO digits, which represenllhe Iiw two digits of/Ire year of publica/ion. This mllY be followed by Q small/cller; /0 disringuish betWtflllWa olhefWise idemical reference /lO/lIIio/1.!. AClrri3 ADPS77 AU1P82 AMFL74 AWI.8(l AT76 ALn AnSw74 ...." Aoki76 BACB7S BAlS76 nBFR71 BCDH7] BCGlIn BCGH7J 8(1175 BCII~t72 ReM78 B1H'I'81 BG075 BHIIK7Q BHUSI Allen, G.C., Curtis, M.T~ Hooper, AJ., locker. P.M. 1. Oltm. Soc. Dol/OIl TffUU., 1617 (191]). AnseI~ R.O~ Didinson., T., Povey. A..F~ Shefwood. f,M.A. J. Ekclmt Sptarosc. Rdllt. PInom. 11,301 (1977). 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Acta 24, 207 (1977). Bcmdsson, A" Nyholm, R., Mal'1ensson, N., Nilsson, R., Hedman, J. Phys. Status Solidi (b) 93, K103 (1919), Blackburn, J.R., NOfdbtTx, C.R., Slevje, F., Albridge. R.G.• Jones, M.M./II01'8' Chtnl. 9, D74 (1970). Bl)ide, V.G~ Salka1adlc:n. S.. RaslOgi, A.C., 100, C.N.R., Hegde, M.s. J. PIrys. D 14, 16(7 (1981). Bwger, K. Tschismarov. F~ EbeI, H., J. E1taron Spta.1I)J(:. IkIaL Phtnom. 10,461 (1m). Perkin-Elmer Corporation PhYSical Electronics Division Bahl, M.K. WaIson, Rl.., Irgolic, KJ~ J. C1Itm.. P#rp. 68, 32n (191~. 8W]79 RWI80 1bhI, M.K. Watson, R.L, lrgolic, KJ, PItys. Rtv.lLJt. 42, 165 (1979). Bahl, M.K. WaISOn, Rl.., lrgolic, KJ., J. CIItm. PIIys. 72, 4069 (1980). 8W181 IIWW]76 8aSl7.5 Bahl75 ll=S3 "1lSO ReWa79 ""'I BiPo73 8,i8\\'80 Rind73 BrFe76 BrFr74 BrMc72 8rWh7S 8uBu74 CAB7] CBA73 CBR76 cm'MS2 M.K. Watson, R.I.., Irgolic, KJ., cf (seJd-13) WGR, Alla/. Chem. 51, 466 (1979J, Bahl, M,K. Woodall, R.o., Walson, R.l., lrgolic, KJ., J, Chem. PhJj. 64,1210{l976). 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MIn., 517 (1971} '" Appendix C, Chemical States Tables References CLSW83 CMIIL17 CSC72 CS~'G7? CWII82 CaLt73 ChGr72 Chlla79 Chad73 Ci~75 Cilla74 Citr73 CIAd?1 CIRi7/) CITh78 Colle72 CoRa76 OKMB76 DPS7. DI'S77 DSBG!2 Oalt76 EMGK74 I!:PC75 EI'CC75 EvRtSl FBWli;4 rCfG71 FEM\'77 FlWW1) FHR80 nrrn t'KWJo'77 Ouistie, A,B~ lee, J., SutherlRl, L Walls. J.M. AppI, SIlrf. Sci. 15, 224 (1983), COllIOOf, J.P~ Moumr, G., Hoogewijs, M., LeClere, C. J. CllkJI, 48, 217 (1977). Carver, J.e., Schwcitzer, G.K.. Carlsoo, tA. J. ~m. flIp. 57, 973 (1972). Conlour, J.P., Salcssc, A.. Fromenl. M" Garreau, M" 1'hevenin, J., \Varin. D. J. Micro.l'(. SpeCirosc. Eleclroll, 4, 483 (1979). Carvalho, M., Wiescrman, LE, Hcltulcs, D.M. A/JP/. Sr'eetmsc. 36, 290(1982). Caben, D~ Lester, 1.E. ~IIL Phyt. 1.Lf/, 18, 109 (1973). OIadwict, D., Graham. J.. NaJurr (Lom/oo) PhJS. Sri., 237, 127 (1912). Oladwick, O~ Hzhc:mi, T. Surf. Sd. 89, 649 (1979). OIadwid. D. Omt Phys. un, 21, 293(1913). Cimino, A., De Angdis. 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Ii. J. Alii. T8VL82 Chmt. .sox. I~, 5266(19R2). 1luna, J.M. Albms, L WiUiarns. R.H~ Ba'btt, M. 1. Chmt. $«. l1WB72 Farodtry TIUnJ. If 68. 755 (1972~ Taylor. lA., LaIaSICf, G.M., Ibbalais, lW. J. £ltc/rat Sp«IrOSf. TLR78 Rd(l/. ,btllOf,l. 13,435 (1978~ Turner, NJi.. Murda~, 1.5.• Ramaker, D,E. Allal. Olcm. 52. 84 (1980). TMR80 TRI,K73 Tolman. CA, Riggs, w'M" Linn, w.J., King. C.M., Wcndt, R.C. //lorg. Cbem. 12. 2772{l973). TtQltI-NoeI, c.. Vemisl, J., Bogillon, Y. J. MiaolC. Sp«/ffllC. TVG76 EkrfCffl,255(1976l. Taylor, J.A.. Rabmis.. 1.W. J. the.. /'Irfi. 15, 1735 (1981). TaRaSI Taykx, lA. AppI. Surf. Sci. 1. 168 (1981). rayt81 Taylor, lA. 1. \be. Sci. Technd. 20, 151 (1982). "'~8l Thomas, JR, Shanna, S.P. J. \be. Sci. Tedllrd. 15. 1707 (1978). ThSh78 Tricker, MJ. /norg. Chelll. 13.743 (1974). 1'rie14 Ueno, T., Odajima, A.l/1l1. J. Appl. Pbys. 20, L501 (1981). UeOd81 UtQd82 Ueno, T.. Odajiml, A. Jpn. J. Appl. Pbl'S. 21.230 (1982). Umczawa, Y, Reilley, CN. AlJ(Jj. Clwrt. SO, 1294 (1978). UmRe78 VHES2 ¥aD Der Veen. l.F. Himpsd, FJ~ Easurwt, DE. Ph]S. R~. B 25. 7388 (1982). VLDJln Veal, B.W.. Lan, DJ~ DiamoDd. H.• HotbUl, H.R.1'tIys. Rn'. B IS, 2929 (19m. VRP(;74 Verbis!. J.. Rip. J~ PirelU~. JJ., Caooano. R. J. Electron SptCl/we. RellIl. Phenom, 7, 193 (1974). VVSW77 Van De Voodel, D.P., Van DeT Kelen, G.P., Schmidbaur, H" Wollebtn, A, Wagner, F.E. Phys. Scr. 16,364 (1977). VWIIS81 Van Der lIan, G~ WCSli1., Haas, C. SawalUy, GA Phys. Rel~ B 23, 4369 (1981). v",van Vaa De \bldeI, D1'.. Wuyts, LP~ Van Der KdCll, G.P., Bt~, L J. EkarotI Spte:tIUSC. Rtl4t ~11110111- 10,389 (1917). V._ YalI DoYmn, H., Verhoeven, l.A. J. £I«lron Sp«trosc. Reltll. Pbmom. 21, 265 (1980). Van Ooij, W.J. S1l1(1(;~ T«h/lolo8Y 6, 1(1977). Vanon VanntTbc:rg, N,G. Chem. Sa. 9. 122 (l976), Vann76 Vayr81 Vayrynen. l. 1. Eleelroo Spec:,IWf:. Re/lI1. Pherwm. 22, 27 (19BI). WHMC78 Willbe:rg. T.N~ Hocnigman. J.R., Moddemall, W.E., ilihcm, C.R., QlIeU, M.R. J. \OC Sci. T«/moL 15. 348 (1918). WPl1K82 Wagner. CD.. Passoja, DE, Hillery, H1'~ Kinisky, T.G.. Six. H.A~ J-.sert, W.T.• TaYD_ lA. J. Ibc-. Sci. TtehtoL 21, 933 (19S2~ 5iWoSO ' 'JJ. c.. 248 Handbook of X-ray Photoelectron WRlJM79 WSI'77 WVV1'J WagnCf, CD., Riggs, W.M.. OJV~. LE., Moulder, lE, Mullcnbcrg, G.E. 1/IIIIdbol!k of X.my I'lw/odeclron SpWI"OUO/l)'. Perkin-E1mcr COfpOf3liOll, l'bysicaJ EI('.C\ronic.~ Divisioo, Eden Prairie, MN 55344 (19791. Wcser, U~ Sokolowsti, G.. PiJz. w. J. El«lroo Sprorosc:. Nt/al. PIImt.. 10. 429 (911). Wil\emen, H., Van IX '*-del. D.F.. Viln Ocr Kdc:n. G.P. /"'/fl. C1Ii... Acta 34. WW(.iS WWVY77 WZR80 WaTaSO WaTa82 Wagn75 Wagn77 Wagn1S W""" w.lm WtAn80 WeMt78 YMK7B YNAB77 YI\'NA14 YNNAn YYS78 Y\'S79 Spectroscop~' m (1919). Wcrlhtirn. G.K.. Wernick. lH., Cltttlius. G. Pltp. R~. B 18. B78 (1978). WillcmCll. H.. WU~l~, LE, Van Dc Voodcl, D.P., Van Der Kclcn. G.I'. J. EI«/1'O/1 Sp«/IWf:. Re/lIl. PhC/J()III, 11.245 (1977). Wagner. C.D.• Zalko, D.A., Ra)'mood, R.l1. AI/Ill. CheRl. 52, 1445 (1980). Wqner, (;.D.. Taylor. J.A. J. £ltc/1TJfI Spfflrosc. Rdal. Ph~ 2lJ. 83 (1980~ Wagner. CD., Taylor. lA. J. £ltc/1TJfI Sp«11WC. Rt/ul. Phnrum. 28, 211 (19&2). Wagroer. CO. Di.'lc:llS.t Faraday Soc. 60, 291 (1975). Wagner, CO. Chapler ? in Ilmlilbook of X.m)' and UI/f(!I'iol~/ PholOcltelrlJ/l SptcIIWf:OPY. Ed. Briggs, Heyden and Sons, Loodoo (1971). WJgner, CD. J. \be.. &1'. T«Iw>I. 15.518 (l978). Wagner, CD. J. fltcJff7l Sp«1I'OJC. Rtim. Phmoa 18,345 (1980). Wahoa. ElA. J. 11IOf'g. Nud. CltlIL 39, S49 (1m). \lkightman, P.• AndleW$., P.T. J. Ptr/t. C IJ, LJ15, L821 (1980). Westerhof, A.. Meijer, HJ.D. 1. O'rQllometal. Chen!. 144,61 (1978). Yamashila, M" MalSulnoIo. N., Kida, S./1I0rg. Chim. ACia 31, LlBI (1978). Yatsimirskii, KB., Nemoshalcnko, V.V., Aleshin, V.G., Bratushko, Y.I., Moiscenko, E.P. C1ltm. P/rys. Ull. 52. 48 I (1977). YatsimUskii, K.a~ NemoshaJcnko, V.V~ Naz.arent.o. Y.P., Aleshin, V.G, Zhilinsbya. V.V., TaideJio. Y.D. DoH Abd. Nauk SSSR (Ph]f. 0-..)211.835(197-4). Yatsimirskii, K.8. NemoshaIenko, v.v~ Naz.arent.o, Y.P.• Aleshill. V.G.. Zhilinsbya, V.V.. Tomashevsky, N.A. J. EI«11TJfI Sp«froSf. Re/ol. PlreIlOIll. 10,239 (1977). Yoshida. T.• Y~masaki, K., Sawada, S. Bull, Chem. SM. JWI. 51, 1561 (1978). Yoshida, T., Yamasaki, K. Sawada, S. Bull. 0rCII. Soc. JjJfI. 52,291ll (1979). y,"", YoSt1. YoYa81 Yosh78 YoshBO ZSQS79 leHa?1 ZiHt1S Yang. SJ~ BaleS, C. w. Appl. PIrys.. Lett. 36, 675 (198O). Yoshida, T.. S3wab., S. B/Ii/. a-. Soc. Jpn. 47, SO (I914). Yoshida, T., Yamasaki, K. Bull. Oem. Soc. JfJII. 54, 935 (1981). Yoshida, T. Bull. Q(III. Soc. Jpll. 51, 3257 (1978). Yoshida, T. Bull. Chem. Soc. Jpn. 53, 498 (1980). Zhdan, P,A., Shepelin, A.P., OsiflOva, ZoG., Sokolovskii. V.D. 1. Caw/. 58.8(1979). zeller, M.Y., Hayes. R.G. CMm. Phys. Len. 10,610 {197ll. Zingg. DS., Hcl'tUles, D.M. J. Phys. a-. 82, 1992 (1978). Perkin-Elmer Corporation Physical Electronics t;>ivision Handbook of X-ray Pbotoelectron Sptctl1lSC<lpy Appendix C. Chemical States Tables Rererences Acknowledgment: Perkin-Elmer Corporation, Physical Electronics Division (PHI). acknowledges Dr. Charles Wagners conlributions 10 the Chemical States Tables. The entries in Ihe tables, used with his permission, were compiled by Dr. Wagner in collaboration with PHI. Perkin-Elmer Corporation Physical Electronics Division ?An Appendix D.Valence Band Spectra III sOllie castS, lilt chemical shifts oburvtd ill core level XPS are IlOl su!ficiCIII /(I idell/if! the surface chemisrry af a pafticular S(llIIple. /lIllie case of XPS aml/y.fi,1 oj polymers. the c1lallges in carbOlI chetnisrry may be quill sllblle ill core level XPS or the chemical shifls may /)( Dilly (/ secondary or tertiary effect. Willi Ihe mu/ille list ofmonochromators ill XPS and the high tounring rates made possible by currem s/ltcrrometer technologies. ill/lilY onolysls use valence btJnds for ide/ilificOlioli oj lIIa/uials. In mmlY CClses. Ihe )!(lie/Ice /)(mds me used lIS fingerfl'im.> for II sample or a slHface treatment, mlker limn/or identifying .specific molewlar orbitals, Theflngerprin'ts of/he role/lCt /Ill/Ills may II'CII be used 10 aid in 001" tl,e identificatioll of polymers olld the qilalllificalioll of polymer mi~l!Ift$ by 1I,ling methods such as linear leas/ squores filling. The following i£ a smoll campi/a/jar, 0/ valence band spectra ofargauic and inorganic ma/erial.! /0 iIIuslmte ti,e u/ility a/villella band dow. Poly(methy/methacrylate) /'oly(ethylelle) -5 35 35 Binding Energy (eV) Binding Energy (eV) Poly(isobutyl methacry/ate) Poly(eiher ether ketO/ie) -5 35 Binding Energy (eV) Po/y(phenylmt) sulfide Binding Energy (eV) 250 f'o/y(n-bmy/ methacry/ote) ·5 35 -5 35 Binding Energy (eV) -5 35 Binding Energy (eV) Pcrkin~Elmer Corporation Physical Electronics Division Handbook of X-ray Photoelectron Spectroscopy Appendix D. Valence Band Spectra Poiy(propyltnt) (\ COfOnO-!ftottd Pofy(propylent) 1\ t'\ f\ ~- \ 35 \ -5 35 Bildn! Eacrgy (tV) -5 Binding Energy (tV) Nael M~ \ 35 -5 Binding Energy (eV) ~\ 35 F(ZOJ (lremulitt} 35 FtJ04 (magnetite) -5 Bindin& Energy (tV) Perkin-Elmer Corporation Physical Electronics Division -5 Binding Energy (eV) 35 -5 Blndinx Enc:tu (eV) HI Appendix E. Atomic Sensitivity Factors for X-ray Sources at 90' This lobLe is based upon empirical peak area lIalues* corrected for the system s rrallSmission function. The values are only valid for and should only be applied when the electron energy analyzer used has the transmission characteristics of the spherical CalJaci/or type analyzer equipped with an Olnn; Focus III lens supplied by Perkin-Elmer. The dara are calculated for x-rays at 90° relative to the analyzer. Ag 3d 5198 Eu 4d 2.210 Element Line I, Na AI 2p 0193 F 1.000 Nb 3d 2.517 Sm 3d", 2.907 Ar 2p 1.011 Fe I' 2p 2686 Nd 4.697 Sn 3d", 4.095 A, 3d 0.570 Gn 3.341 Ne 1.340 Sr 3d 1.578 Au 4r 5.240 Gd 2PJn 4d 3d I, 2207 Ni 2p 3653 Ta 4f 2.589 B 0.159 Ge 2pJJ1 3100 0.711 Tb 4d 2.201 2.627 Hf 4f 2.221 ° I, Ba I' 4d 0, 4f 3747 Te 3d 3266 Be I' 0.074 Hg 4f 5.797 P 2p 0.412 Te 3d", 4.925 Bi 4f 7.632 .Ho 4d 2.189 Ph 4f 6.968 Th 4fm 7.498 Br 3d 0895 I 3d", 5.337 Pd 3d 4.642 11 2p 1.798 C I' 0.296 In 3d", 3m Pm 3d 3754 T1 4f 6.447 Ca 2p 1.634 Ir 4f 4.217 Pr 3d 6.356 Tm 4d 2.172 Cd 3d", 3.444 K 2p 1.300 PI 4f 4.674 U 4fm 8.476 Ce 3d 7.399 Kr 3d 1.096 Rb 3d 1.316 V 2p 1.912 CI 2p 0770 La 3d 7708 Re 4f 3.327 W 4f 2.959 Co 2p 3.255 Li 0.025 Rh 3d 4.179 5.702 2p 2201 Lu 2.156 Ru 3d 3696 Xe y 3d", Cr I' 4d 3d 1.867 Cs 3d", 6.032 Mg 2s 0.252 S 2p 0.570 Vb 4d 2.169 Cu 2p 4.798 Mn 2p 2.420 Sb 3d", 4.473 Zn 2PJn 3.354 Dy 4d 2.198 Mo 2.867 50 2p 1.678 Zr 3d 2.216 Er 4d 2.184 N 3d I, 0.477 Se 3d 0.722 ASP Element Line 'C.D Wagner," al. 252 Element Line ASP ASP Element Line ASP 1.685 Si 2p 0.283 S",! In">!a,, Anal. 3, 211 (1981).. if\. W' Perkin-Elmer Corporation Physical Electronics Division Appendix F. Atomic Sensitivity Factors for X-ray Sources at 54.7' This table is based upon empirical peak area values* correcledJor the syslem~' transmission function. The values are only valid for and should only be applied when the electron energy Qnalyzer used has the transmission charaClerLstics oj the spherical capacitor type analyzer equipped with an Glnni Focus miens supplied by Perkin-Elmer. The data afe calculated for x-rays at 54.7" relative to the analyzer. Element Line ASF Element Line Ag 3d 5.987 Eu 4d ASF 2.488 Al 2p 0.234 F Is 1.000 Ar 2p 1.155 Fe 2p 2.957 As 3d 0.677 Ga Is 1.340 Sr 3d 1.843 4f 6.250 Gd 3.720 2.484 Ne Au 2P3n 4d Ni 2p 4.044 Ta 4f 3.082 B Is 0.159 Ge 0 Is 0.711 Tb 4d 2.477 Ba 3d,n 7.469 Hf 2P312 4f 3.457 2639 Os 4f 4.461 Tc 3d 3.776 Be Is 0.074 Hg 4f 6.915 P 2p 0486 Te 3ds12 5.705 Bi 4f 9.140 Ho 4d 2.469 Pb 4f 8.329 Th 4fm 9.089 Br 3d 1.053 3ds12 6.206 Pd 3d 5.356 Ti 2p 2.00! C Is 0.296 In 3dsf2 4.359 Pm 3d 4.597 TI 4f 7.691 Ca 2p 1.833 Ir 4f 5.021 Pr 3d 7.627 Tm 4d 2.454 Cd 3ds12 3.974 K 2p 1.466 PI 4f 5.575 U 4f712 10.315 Ce 3d 8.808 Kr 3d 1.287 Rb 3d 1.542 V 2p 2.116 CI 2p 0.891 La 3d 9.122 Re 4f 3.961 W 4f 3.523 Co 2p 3.590 Li Is 0.025 Rh 3d 4.822 Xe 3ds12 6.64 Cr 2p 2.427 Lu 4d 2.441 Ru 3d 4.273 Y 3d 2.175 Cs 3ds12 7.041 Mg 2s 0.252 S 2p 0.666 Yb 4d 2.451 Cu 2p 5.321 Mn 2p 2.659 Sb 3ds12 5.176 Zn 2P312 3.726 Dy Er 4d 2.474 Mo 3d Is 3.321 Sc 2p 1.875 Zr 3d 2.576 Sc 3d 4d 2.463 N 'C.D Wagner, et ,I. Sniffnlerface Anal 3,211 (1981). Perkin-Elmer Corporation Phv..;;ir.al Rl~r.tmJli('" nivi"itll1 iF\. W 0.477 Element Line Na Is Nb 3d Nd 3d ASF 1.685 Si 2p ASF 0.339 2.921 Sm 3ds12 3.611 5.671 Sn 3d,n 4.725 0.853 Element Line Appendix G. Line Positions') by Element for AI Ka X-rays AI_ NWlbffl'lo::lt...c " " , 2plll 2M :II ~l""" JplII )p.rj 3d1'l 30IlIl ,. • ,• ,""" '" ,,,• , .,'" III " " ~ C • AU&tl' UIllI 1'1.,1" 4JM 4pl'l - lIS " .. ~ II ~ III Il P Il ~ Co To 0 • . . 1,).\Il1o\lll~,"\llI,\lllq "'", loo:%f ,. ., '" " , m ,...., ,. • '" '"'" " " • '"'" '" ,.'"," •"n nn '"'" '"'" '"rn'" nm "• '"". ,., '"m,.,, .","lOll "'m " " " ,., ,., ,m " "'"'" '" '",u '"'" '" ,SI '" '"'" '" ,,., " , III II Il ,~ ~, "• "" •• " b G. Go 'm 11m ~ ~ "" ~ . "" " ••• •• "" ,..•" •" II b \144 lJ59~ 4 10 ,.,. ,. ,.,. ..,. •"" "•••" • . 10 In . 21• ,~ 1lO 1lO .~ 1lO .. '".. .. ''''' II 1117 1211 »' 11m ...'"'" '" ~ 1,J.\lLJ>\'" ('rJ LJ.\111\101 ci'l k.\b\l.oI('Pl ~14\loo· ,. ,. " ,"'. ,.,. "" ~ a III 'SI Il , • " "" "" 21 .. m " ,m"" CI m m ,. III m Mll.\l<l>~ I- '"' n" ~ :4 '''" II 51> 119S '"'m" "'''''~ '336 7Il ~ '"'" '"'" '"'61 " ~ ,. ,t,. ,.,. ,. ....., "" .. "" . • ,. , " ," "IS a ,• " " •, n ... no ~ F Kl.tlk>ll BIG IQIl 0 10 KL,14I m .Il .....'" ... ••'" . ..,. .. ". m 1lO '" '" '" '" m m 1Il 106 ~, m .ll ,. M.s/'I:lY 'll6 '"'" 1Il ~, 'n ,. II> m m '"'IS'" ,. ". ~Iao""'" '03 I) Lines enclosed in boxes are the ones which are most useful for identifying chemical Slales. b) Includes KVV dr.$ignalion when Ln is nol a £ore level. c) [ksigoaliOll is oveaimplified. d) locludes LVV wIlerI M btls an: not in corelnd MVY wbca N Ieveb are not in core. e) No simple 4Pln 1ft aim f(l" this groupofelements. l) The -4d doublel for ltcse ~ is ~ and is Ylrilble with clcnical $We because of IIllltiplet spIittill& &I1d muhi-dectron puuses. g) The ~ is of low intellSity and is ofieD in the 5hili-up stnJdure of the 4f lines. These yahleS ae estimates of the energy. 254 Perkin-Elmer Corporation Physical Electronics Diyision . ~I(."ir N"""~r/..:lt"",,, • " . . '",.. '" lplI' ~. ~, lOS .- . PhOl""l«tron Li... 4p", 4pl'> "'" "'" .... '" ....'" '"'" '" '"'"'" .."" ",f' • . '" '"... .. "• • '" '"'" '" '"'" "". ." ""• '" "" .., ''"" .'"'" ". "'" " '" '" ..'" '" " " • '" '" .,...'" '" ,.'" '"'" " " '" ." "" ",.. '" ,. '" '" • ,. """ .. ". ,.. '" ..'"'" '"'"'" ,. ,. •",. '" " "" . '" '" 0 0 n' T, lIS SOl s• 941 IIXl9 1071 1141 1219 II) 111 • 5,. SPl'l Sd.., "". .. AU):,r l.[nlll 5.- M.l!I"lllV lIS "" '''' p 1191 50• ~ ~ so 0 m 996 1069 1292 IUS •" • "" " .... ~ ~ So •.. os •.. ••" ,.•'" '" & Th Ho ~ "nn w "" • ,"" ," •" n.. "•0 • .. •u " •" •'" •" '""'" •" a ~ T. ~ ~ M Th It "n W '50 m s. s. .,.. ,~ u on on so 50 '50 n '» m ,m ,m ,,,. ,n '" '" "" '''' '",,,. ,., '" '" , '"' ,.,m '"'",., '" '" ,,~ 2D l~ ,m 'u' '0' . '" ..,. ,,.. ,.'" 0 .~ '0 .. . ,. .. 0' lJI ,~ Perkin-Elmer Corporation Physical Electronics Division .. lO II S> 214· 2&:1 lJl1 1116 ,m ,m II W 1326 "" '''' ,'''' .~ lOS '20 . ill ~, . . ,. . .. . .. .. 50S ,~ 850 ." 5U 161" m '" • '"" OJ.'" ""'''' ..... '"~ ~ II .. . .. ., ,. 'Ii! 0' on 211 "50 '"'" ,.,. .".. .. ..•• '" lO 5l 8ll '" 5l ,~ '"" ~ 50 2l ~, .: sn 0 50 1129 110) ~ 900 ~ '00 M,...... ,~, '"'" '" "" "" n" "" .."" "n ,m /til"'''' '00' 'ms '", '"'"m ,, m '" ,. m "" ,, ,m '"' m '" '" '" '"' '"'" '"'"os ""m'" '"on ,, " " "" • , , so " "n '",,,"" '"m "" '"m , ,• • • ., , '",.s. so, ...'" '" '" " """ • "" " • • " ., '"'",. '" ,.'""' '"'"m ..""• """« ""'",,',00"" " ,,,.. "u " "' on '" ,,,. '" '"'" '"'" '"s. •• '"'" '" mm'" ,,.. •'00 ""« '",m ,m '" m os '"'" "on ,m '" '" '" '" ~ ,,,. ,m '''' '" m ... '" .n•• '" '" '"'" 1m '" .., os '" no '"'"m m '" 2. '"os 'u '" •• "' 11lll~1 lISS 1116 1211 U2 .. "" ,,.. , "n "" """ " • •. 1lS~ JQ5 "" ,., "'1m" "" tHO 0 OP M~u· M.,N.!V ,,~ 1111 50 50 0 M~~ ;) ,"" ~ m ill 4rlll ~ III m "- " "" "n "'" 1311 131• 1311 OJ" OJ. OJ. OJ" ",,"V "" ,., "" "" •" •" ", "" '" " "" '" on "n "" " "" '" ,. ,. II '00 II """V 1419 1412 --- ,,,, "" ,,~ N~:rO ,w ". '"' ~"" ,m ,m ,m NJOoAs H.O..ou '416 ,,'" "" ,os "" ,,., ,.,'''' ,m '0' ". ''''' Appendix H. Line Positions') by Element for Mg Ka X-rays , .. . ,C ,- ..• •,, ,c, , "" F ". 10 II "" ,," IS , "a ,• " "n n • , "" c, •"n ".• •• " • "'" n " "" "» •" • "• •, •• • II I! ~ 1I 10 II D JS 6b .'. '" "" f'hoIwlffil'Qll Una AIIlllW Numbrr/'FJralmI '" 2PM 3s ,." • ... JI"Ctf UIIII ,C'" Kl~"', -F• KLuLu" ~ '",. '"'" "i"iSl ..'" " ~ OJ " "" •" ~ ,t ' ,.'" ,.00:',." L"IobMll~LlMo.,Jo!Jl,j ". 'I! '" ,~ ~, ., '" ...'" '"'" " » .w ...,. '"""'" ,., •n "''" "'" '" ~, ., . 62l II,. I!~ '"•• '"'" ,.••,. "' ,,,. '" ~ " ~ c'PJ ~ll-\lol ('P) ,. ,.,. " " •,. ..,.'"'" ,.,.,. ',.," ,. • " ,. ,. '" '" '" ..'" ",. ,."' ••'" '"'" '" " 10' n • » '00 12J7 ,~ In '61 ~ Il 113 lIIl IN no 1I JI » 63 I!' '" ~, 63 ~ w 62l ~@,.. 63 II .'! , """ " J . '""' , ill ...""., 10 IlUW '" OJ !IS leMS Ian IN, lIIl 61 ~~IoI· ..'.... 1071 10• Il ID 114 4.\I:J.'ioI (." LJ)b\1ol 1103 ••" •» » "" • "" III 14 II~ , II ,~ 1IIl ..'" '"'"m '"-~ 1161 " ,. '" . ,. .." ,U ..,. ,..., '",. 2J ,on M;<J.\1t!'111 ,. •• ,.'" '" ~...,,. ..,.." ..'"••'" ..., ..'"'" ,.'" '",. '",. .."' '",. ,. on '" .,'" '" 61' 'IS n IIS7 1152 ~~OI M.s<"l»V 1I11 "'" '106 a) UIle.'i enclosed in boxes arc 1he ones whicll are mostllSeful for idenlifying chemical stales. b) IlICludes KVV designalioo wilen Ln is not a core 1evtI. c) Designation is oYmimplifled. d) hx:ludes LVV when Mbock are Il)( in core and MVV Il'hc:n N b'eIs m not in core. e) No simple 4pm1ine cxisu for !his gl\lllp or elements. I) The 4d doubkc for these elemenu is comllleJ. and is variable with chemical state because of 1lJJlliplet splitting and JTI\llti-elr:ctron processes. g) The 5s is of low intensity and is often in tlte sltake·up structure of the 4f lines. These yalues are estimates of the energy. 256 Perkin-Elmer Corporation (I) Physical Electronics Division , Alorpi( Numbr,fUtmenl " . M. S,. " ". ", '" '""" ."•• su ," ,ron, ,,,'" m m "" m ~, " To •" .Po " ."" •,.'" m "n To, '" " "R. "" "ro " "" S."" "" • """' ", • T.• •13 '" n " 13 , "'w " P, " "" ~ N Cd ~ ~ lJ lJ ~ 944 813 1009 871 1011 930 1141 996 1219 1001 ~ Nd Gd Th ~ ., n, 217 2• 201 , ~ 665 531 320 .. U Jll on ~, ,~ ... ,. 1108 ~ ILIS 1126 1213 ,,~ 3% '" m 309 S. S" s~ on 00 6" ~ "" •'" " "' •, "" " em •" a n % Th ,~ m .,,. .,'" ,~ U N, So % Ok Aug.. 1.lotS M.sNllV MU...."ll· M~~<lNlS"l Mtio~,V MsVV ~ ,., "" .,n 43") "" '"m"" "n ..'" '00' "89 "" 'on" " " .." ", "6J " 9Q2 '" '" .,m "J ill • '"'" ,. OJ '" 201 ,,,on 'OJ '00 ,.'" '" ,.'" ",m"" .g:.'" 1lSQ "' 212 .S '"m '" '" '" ,. "''" fill'm" .,'"m "",w mm '" '...'"" .,," m " "'m sn '<OS S20 m "' m '" Sl9 "' '"'"'" "' ...'""' 'n"' ",m '" '"m "' 331 " ~, '26 "3 274. 26ll 219 'HI .3 '00 1170 96S '~3 00" 1121 ,. ,.,,, ,'"'" "' 3lS 3iS 616 13' .'" m ro' m '"m '" II 8 9 Sl J~ "" .."" """ "" 22 2l "• '"'" '"'", '0 " •" "" " "" "" •" • "",.',,0' "" 6J 2l 38 115') is 9S 161 1l J2l M .<9 <1J "' ,m, '00' ,m, ,m, '003 'ms ,OJ '089 . lIOI " 00 1II9 1131 ". ,~ NINln'll '.s 1l '" '"'" '" ..'", '"s" ••m !32 N,N"N, 2l . . <0. , , •" " m' '"'"m ,,,, '" """ """ ,'" "m ,ro m ... '" " ~ '" m 00' . ,''''.. ~ Sl 600~ '" .,., 12 8 333 1% ,. ,, •"" • " " "" 309 2Cl6 ,.'" .,''S007 """ "" """ " .."" 8 8 '" '<9 29 ,..'" ill ,.,.'" .. "" m • •" "" 11 8% .J .,~ .. m ~ on """ ~l.VV ~ ~ .... '" US . ". ". 2l ,~ 9J2 ". " ". ". "" ". @ '00 1184 9Q2 "" I'holoele<:lron lint! 4dl/l 41S/l ro ,~ 1l 18 19 8, 29 1l '" 368 . 6" '"'" '" '",n '" '" ." ," '"m '" on ,."' '"6. '22'" ,'00' ,., ,. '"'" ,.'" '"mm ,", m '00 '00' "'" '""" .,'"m '" 'M' '" '" 12l "" ~ m @ 16 4plll 4j>l'l " . '" '" '" " "' ••'" \138 '201 1128 17 l8 ,. " ." '" ,. M .• ~ "''00'" 1103 1110 1121 N~'1,O 101'\ 1013 '''' """ ,," """'"'16" " •" "" "" '" ",,,, '" "" "" '"'" '" '" •" """ '" " 2l 206 N!OuV ,.,. .. ~ 2l 26 . ,."' N<N,O N,OJsO<! N,OuO,,! 1183 "."" ". 1161 11M 1113 "ro "" "" Hil 1153 32 35 Perkin-Elmer Corporation Physical Electronics Division 257 Appendix J. Line Positions in Numerical Order· For photoelectroll lilies, the spin orbi! split/ing is indicated Auger excitation is jnJicated in parentheses. 7 14 23 22 25 29 30 31 37 40 41 42 43 48 49 50 51 53 56 60 61 64 67 69 71 73 75 77 84 87 89 Lu 4f712 Hf4f,. 02s Ta 4f Sn 4d Ge 3d", F2s (2) (2) W4fm (2) (2) (I) . V 3p Rc4fm Ne2s As 3d", Cr 3p Mn3p 14d", Mg2p Os 4fm Fe 3p Li Is Se 3d", Co3p IT 4f712 Xe 4dsn Na2s NiJp Br 3d", PI 4f1l2 AI2p Cu 3p", Cs4d", Au 4fm Kr 3d", Zn 3p", (2) 89 90 98 99 101 103 104 109 Mg 2, Ba 4<1112 (3) Er (AI) Si 2p", Hg 4f,. La 4d", Ga 3p", Ce 4d", (I) (4) (3) (3) (3) Ge (Mg) 112 Rb 3d", (I) Be Is (I) . (2) (3) (I) (3) (2) (I) (3) (2) (3) (4) (I) (2) 115 Pr 4d 117 Ho 118 TI4f1l2 AI2s 121 Nd 4d 122 Ge 3p", 128 Eu 4d 129 Sm 4d 131 P2p", 134 Sf Jdsn 137 Pb 4f,. 140 Gd 4d 141 As3p", 146 Tb4d 151 Si 2s 152 Dy 4d 156 V3d", 157 Bi 4f1l2 160 Ho4d 163 Se 3p", 164 S 2p", 167 Er4d (AI) (4) (4) (1) (2) (5) ill parentheses. Auger lines are ill ;lalies, alld the phD/on source for the 175 179 181 182 186 188 189 196 199 202 208 211 226 228 (6) (1) (2) S, (AI) Vb 4d Br 3p", (7) Ga (Mg) P2s B Is Lu 4d5fl C12p", Nb 3d", Kr 3p", flf 4d", Ta 4d.sn S2s Mo 3dy'! Rb 3p", AT 2p312 IV 4d", Re 4d sn (9) . (2) (13) (14) Na (Mg) Tb (AI) 262 2" (Mg) As (AI) Sr3p", Cl2s Os 4d", (II) 240 242 243 260 (5) (2) (5) Tm 4d Zr 3d", 270 271 279 280 285 Ru Jdj,'l Tb4p", Cis 294 K 2p", 297 Dy 4p", If 4djJ2 (10) (2) (3) (8) (II) (12) (3) (14) (4) (37) (3) (40) (15) 299 301 307 309 315 320 321 330 333 Y3p", (12) Mg (AI) Rh 3d", flo 4p", PI 4d", (5) (44) (17) AT 25 Er4p", Zr 3pJll Th4f,. Tm4p:lI1 335 Pd 3d", Au4d.l/2 CII 341 Vb 4p", 342 G, 347 Ca 2p", 360 Lu 4p", 361 fig 4d", Nb 3p", 368 Ag 3d", 369 Gd 377 U4f712 380 K 2s 385 T14d", 394 Mo 3p", 398 N Is 399 Sc 2p", 404 Ell 405 Cd 3d", 408 Ni 412 Pb 4d", 419 Ga 436 N, (47) (14) (9) (51 ) (5) (18) (Mg) (48) (AI) (3) (53) (20) (15) (6) (Mg) (11) (21) (17) (5) (Mg) (7) (Mg) (22) (AI) (Mg) Corpor~lion 258 Perkin-Elmer (J) Physicnl Electronics Division Handbook of X-ray Photoelectron Spectroscopy 440 Ca 2s 449 44\ 444 454 462 480 485 493 495 497 499 512 525 526 528 531 533 551 561 564 568 573 Sm Bi 4d", In 3d", 11 2p", Ru 3p", (Mg) Co (Mg) 669 670 676 682 685 (24) (8) (6) (22) Sn Jdsn (8) No (AI) Zn Rh 3p", Sc 2, V 2p", (AI) 696 707 709 713 715 726 (24) (8) Nd (Mg) Dy Sh 3d", o Is Pd 3p", (AI) (27) F, (Mg) 736 738 745 758 767 772 778 781 (9) 11 2s Pr (Mg) Cu (AI) Ag 3p", Te3d", 574 Cr 2p", 599 F 600 C, 602 Gd 619 Cd 3p", \ 3d", 634 La 637 Eu 639 Mn 2p", 641 Ni 653 80 665 In 3p", 667 M" (31) (10) (9) 784 797 799 816 820 832 833 835 836 843 853 863 867 870 (Mg) (Mg) (AI) (34) (12) (Mg) (AI) (II) (AI) (Mg) (38) Appendix J. Line Positions in Numerical Order N, (AI) Xe 3d", Th 4d", Sm F Is (13) (37) C, (Mg) (AI) . 874 884 886 8% 900 916 918 926 932 933 942 952 959 964 971 N (Mg) Ce 3dyz 80 (\8) Ag (Mg) Mn Sc (AI) (Mg) C, (AI) 1103 Cd 1107 N 1117 Ga 2p", 1126 Eo 3d", 1129 Ag 1149 Sc 1154 8j (Mg) Pd (Mg) 1159 Pd (AI) Pr 3dyz Cu 2p", (20) (20) 1161 Pb (Mg) 1168 TI (Mg) X, (AI) . 1179 Hg (Mg) Rh (Mg) 1183 AI< (Mg) Cr (AI) 1185 Rh (AI) Co (Mg) 1186 Gd 3d", (32) U (Mg) 1197 Co (AI) (AI) (AI) (AI) (27) (30) (AI) (AI) Cr2s Fe 2plI2 (13) X, (Mg) Co (AI) Sn3p", C,3d", (42) (14) Cr (Mg) U 4d", (42) I (Mg) 0 (Mg) I (AI) 1204 U (AI) Nd (AI) (AI) (46) (Mg) (31) T, (Mg) (21) 1212 Ru 1217 Ge 2p", 1223 C (AI) Sb3p", 978 0 979 Ru 981 Nd 3d", Co 2p", Ba3d", (15) (15) 990C (Mg) 1239 Th (AI) 1005 T, (AI) K (AI) V (Mg) 1006 K (Mg) F, Th (Mg) Pr (AI) .1014 V (AI) 1241 Th 3d", 1272 Ar 1296 Dy 3d", (35) (AI) Sb (Mg) 1022 Zn 2p", (23) 1299 Mo (AI) S" Te 3p", (Mg) 1032 Sb . (AI) (51) 1039 Ar (Mg) (AI) F C, (AI) S" (AI) 13\9 Nb (AI) (Mg) Ii CI (AI) Ii (Mg) (35) La 3d", (17) I" (Mg) Ni 2p", Ne Is La (18) Cd (Mg) 1049 1068 1071 1072 1076 1077 1081 1086 1103 1303 Mg Is 1304 CI 13108 (AI) (AI) (AI) (AI) (37) (AI) I" (AI) 1324 As 2p", 1336S 1387 8i 8 Sm 3d", (Mg) 1394 Pb (AI) (27) \401 TI (AI) Nb (Mg) \4\2 Hg (AI) S (Mg) \416 Au (AI) Na Is (AI) (AI) (Mg) Perkin-Elmer Corporation Physical Electronics Division m 'lI 259 Appendix K. Periodic Table 9 Atomic number 3 0.025 Is Kll Most intense photoelcetronlransition Most intense Auger transitioo H 4 PHI sensitivity faetor* for designated p/'Kltoelectron lransit;on F Element symbol 1 1.0 685 647 Binding energy, most intense photoelectron transition Kinetic energy. most inlense Auger transition Be . " ,.'" """ Li U1l5 10 1.340 13 0.193 14 "'" IS 0.412 16 o..s7Q 170.710 18 1.011 6 0,159 7 0.417 8 0.711 9 53l 1$ u"" II He ,. "" N 0 F Ne B C " . """ ."'''"" . " " ... """ ,.. "" "" "" Si ., P , S,. CI,. ,Ar,. ......AI .... ", .... ..." ,. 5 0.074 2 In 12 "" Na Mg """ "'" "" • .. ". '" K ,Ca Sc Ti V Cr ,Mn.. Fe ,Co,. Ni Cu Zn Ga Ge As Se Br Kr .. .. ..... " ... '"'" ..." .,. "........ " •. ...... I:' :; " ., " '" .... '" ........'"'" ...... " " • Rb Sr Y,. Zr Nb Mo Tc Ru., Rh., Pd Ag Cd In Sn Sb Te Xe . . .. ... "" . ..... "" '" '",... '",. .... ,. .. "" '" "'" ... .... ..... ........ '" "''" n Hf Ta W Re Os Ir PI Au Hg TI Pb Bi Po AI Rn ...Ba,. ...La... . . ,..... . ......Cs.. ..... .... • • •• • • • • •• '" , . .. .... .... ... .. •• '" ."" ."" 19 1.30 20 37 1..316 I3l 1.634 21 1.678 38Lm 39 U6? 22 1.798 23 25 1.912 24 VIOl 2p 512 IlIl '" 2.42 26 2.1;86 273255 28 3.653 29 4.798 30 3.354 ... '02 UlII 50 UlII "' IlIl .. 1lIl,. UlII . . 31 a- 3.341 323.100 lMM lSI 330.570 34 0.722 ~ 1117 3S 0.995 ~ 40 2.216 41 2..517 42,.., 43 "" 44a__ 4S 4.119 46 4.6'3 47 5.198 48 a", 491m 50 ... 514.(73 UIM 215 36 1.096 .~ UlII ' " 52 4.925 ION 53"" 545.102 I ~ III 3d ~ ~ ~ '31 lIN SS 6.1132 56 6.361 57 7.1ll8 ~ ~ ~ ... ~ MIN 188 72 z..22\ 73"", 74 2.959 75 3.327 76 am ~ ~. 88 ~ ""N '" 51 • ... 181 HtIl 180 81 ~ 4.217 335 ~ ~ WIN 78 4.674 79 s.2<lO 587.399 ;9 "" 60 ..... 61 307S( 622.'1J7 $.197 816,1447 • ~ 9»);l !1&1 III 82 ..... 83 7.ffR. 84 ~19 ,., 50 516 . . ,<5 8; 86 "" 63 t210 64 "" 65 2.201 66 Ce Pr Nd Pm Sm Eu Gd Tb :li1 411 118 • '51 tftl" 110 89 Fr Ra Ac 80 3dw r.IItI 1034 3I:U IOB1.td 1215'- 140 «:I 2.1118 67 68 tIll 692.m 702-1E1!l 71 2.l56 Ho Er Tm Yb Lu Dy 146 4lI 2.189 152 4d 1m 4d 161 4d 115 4d II! 41 7 ~~~~~~_m_e_ti~eH~~11"~lm~. 90 Hill! 91 92 lU76 93 ..... "" . "" . 94 95 96 97 98 99 100 101 102 103 Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr 'M ., 'The values aTe for area measurements of the designated transitions and are only valid when the electron energy analyzer used has the transmission characteristics of the spherical capacitor type analyzer equipped with an Omni Focus 111 lens supplied by Perkin-Elmer and with x-rays at 90" relative to the analyzer. Where a spin-orbit splitting is 001 designated the nlue is for a measurement including both spin-Olbit componenl~ Perkin-Elmer Corporation Physical Electroni~ Di\lision 26\