Hard X-ray Photoelectron Spectroscopy (HAXPES) Of Correlated Materials A. Chainani,1,2 Y. Takata,1* M. Oura,2 M. Taguchi,3 M. Matsunami,3 R. Eguchi,3 S. Shin,3 1 Coherent X-ray Optics Lab 2 Advanced Photon Technology Division 3 Soft X-ray Spectroscopy Lab RIKEN Harima Institute @ SPring-8 *deceased 4/8/2015 1 4/8/2015 2 Acknowledgements For the development of HAXPES @ BL29XU Coherent X-ray Optics Lab. @ RIKEN SPring8 Center M. Yabashi, K. Tamasaku, Y. Nishino, D. Miwa, T. Ishikawa JASRI/SPring-8 E. Ikenaga (BL47XU), K. Kobayashi(BL15XU, NIMS) HiSOR, Hiroshima Univ. M. Arita, K. Shimada, H. Namatame, M. Taniguchi Musashi Inst. Technology H. Nohira, T. Hattori (Tohoku Univ.) VG SCIENTA 4/8/2015 3 Acknowledgements For Collaborations Titanates Vanadates Manganites Cobaltates Cuprates Ruthenates Ce compounds Yb compounds Nitrides 4/8/2015 H. Hwang, H. Takagi H. Hwang, K Motoya, Z Hiroi M. Oshima, Y. Tokura E. Takayama-Muromachi T. Mochiku, K Hirata A. Yamamoto H. Sugawara N. Tsujii, A. Ochiai, S Nakatsuji K. Takenaka 4 Outline 1) Introduction 2) Experimental Setup, Performance & Characteristics 3) Applications : Strongly correlated electron systems 4) Future directions 5) Summary 4/8/2015 5 Main Characteristic of HAXPES Large probing depth! Inelastic Mean Free Path (IMFP) of Electron (From NIST Database) Inelastic Mean Path (A) 250 140Å (SiO2) 200 210Å (SiO2) NaCl SiO2 150 30Å (SiO2) 100 Al Ka Si GaAs Au 50 0 0 4/8/2015 2000 4000 6000 8000 Electron Kinetic Energy (eV) IMFPs 1-4nm @ 1 keV 7-20nm @ 8 keV 10000 Bulk sensitive Free from surface prep. Functional thin films Chemical depth analysis Embedded interfaces (non destructive) 6 Early HAXPES with Cu Ka@8keV S. Hagstrom, C. Nordlimg, K. Siegbahn, Phys. Lett. 9, 235 (1964) 4/8/2015 Chuck Fadley, S. Hagstrom, J. Hollander, M. Klein, D. A. Shirley, Science 157, 1571 (1967) 7 The first HAXPES with SR I. Lindau, P. Pianetta, S. Doniach & W E Spicer, Nature 250, 214 (1974) Au 4f 4/8/2015 core level: possible valence band: impossible 8 Obstacle to development of HAXPES (Mb/atom) at 1.04 KeV 1E-3 abs Small10photoionization Cross Sections 1s 1E-8 1 0.1 0.01 1E-4 1E-5 1E-6 1keV 1E-7 0 10 20 30 40 50 60 70 80 90 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p 6s 5d 4f 6p abs (Mb/atom) at 8.05 KeV Atomic Number Rapid decrease! ~ 1/100 1s 10 1 0.1 8keV 0.01 1E-3 1E-4 1E-5 1E-6 1E-7 1E-8 0 10 20 30 40 50 60 70 80 90 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p 6s 5d 4f 6p Atomic Number 4/8/2015 9 High-energy Ce-3d photoemission: Bulk properties of CeM2 (M=Fe,Co,Ni) and Ce7Ni3 L. Braicovich, N. B. Brookes, C. Dallera, M. Salvietti, and G. L. Olcese Phys. Rev. B 56, 15047 (1997) @ESRF High-energy resonant photoemission and resonant Auger spectroscopy in Ce-Rh compounds @ESRF P. Le Fèvre, H. Magnan, D. Chandesris, J. Vogel, V. Formoso, and F. Comin Phys. Rev. B 58, 1080 (1998) Hybridization and Bond-Orbital Components in Site-Specific X-Ray Photoelectron Spectra of Rutile TiO2 @NSLS J. C. Woicik, E. J. Nelson, Leeor Kronik, Manish Jain, James R. Chelikowsky, D. Heskett, L. E. Berman, and G. S. Herman, Phys. Rev. Lett. 89, 077401 (2002) Quadrupolar Transitions Evidenced by Resonant Auger Spectroscopy @HASYLAB J. Danger, P. Le Fèvre, H. Magnan, D. Chandesris, S. Bourgeois, J. Jupille, T. Eickhoff, and W. Drube, Phys. Rev. Lett. 88, 243001 (2002) Looking 100 Å deep into spatially inhomogeneous dilute systems with hard x-ray photoemission @ESRF C Dallera, L. Duò, L. Braicovich, G. Panaccione, G. Paolicelli, B. Cowie, and J. Zegenhagen Appl. Phys. Lett. 85, 4532 (2004) High resolution-high energy x-ray photoelectron spectroscopy using third-generation synchrotron radiation source, and its application to Si-high k insulator systems @SPring8 K. Kobayashi et al. Appl. Phys. Lett. 83, 1005 (2003) A probe of intrinsic valence band electronic structure: Hard x-ray photoemission @SPring8 Y. Takata et al. Appl. Phys. Lett. 84, 4310 (2004) HAXPES for Valence Bands with hn = 6 – 8 KeV. 4/8/2015 10 Experimental Setup 4/8/2015 11 Pol. How to gain in stability, resoluton, photoelectron intensity 1. High brilliance SR at SPring-8 55mm(V) 1deg. 35mm(H) 2. High performance analyzer 3. Top-up injection 4. Matching the detection angle to the polarization of SR 5. Grazing incidence of X-rays 6. Well-focused X-ray beam 7. Low emittance operation 90 3 2 120 b value magic angle attenuation length -1 10mm range -0.5 60 IMFP 150 10nm range e- 30 X-ray 1 0 0 0.5 1 1.5 2 180 0 1 deg. 330 electric vector 1 2 3 210 240 300 270 angular For linearly polarized light, intensity distribution of photoemitted electrons depends on the asymmetry parameter b b>0 at energies of several keV, for almost all subshells J.Yeh & I.Lindau At. Data.Nucl Data Tables 32, 1(1985) Their intensities have a maximum in a direction parallel to the electric polarization vector Experimental setup at BL29XU in SPring-8 Y. Takata et al., Nuclear Instrum. and Methods A547, 50 (2005). T. Ishikawa et al., Nuclear Instrum. and Methods A547, 42 (2005). He flow cryostat to reduce sample vibration ★ excitation energy: 5.95 or 7.94keV, DE (hn): 55 meV ★ photon flux: ~5x1011 photons/sec @ 55(V)x 35(H) mm2 ★ analyzer:R4000-10kV (VG Scienta) 4/8/2015 13 Optics Layout for the HAXPES experiments 4/8/2015 14 High Energy Resolution & High Throughput (at 7.94 keV) VOLPE @ESRF DE=55±5 meV (Ep=50 eV) E/DE=140000! 5 sec 15min 30 sec P. Torelli et al., Rev. Sci. Instrum. 76, 023909 (2005) 4/8/2015 15 VOLPE @ ESRF 4/8/2015 P. Torelli et al., Rev. Sci. Instrum. 76, 023909 (2005) 16 KMC-1@ BESSY-II F. Schafers et al., Rev. Sci. Instrum. 78, 123102 (2007) 4/8/2015 17 Au 4f core levels @ BESSY-II 4/8/2015 18 Surface Insensitivity SiO2/Si(100) @ 7.94keV SiO2-0.8nm/Si(100) @0.85keV (Exp.) Si 1s BE:1840eV Intensity Normalized Intensity SiO2 Si x 10 SiO2-0.8nm/Si(100) 10sec SiO2 Intensity SiO2-0.58nm/Si(100) Si Si 2p BE:100eV x 10 30sec SiO2 0 6090 @7.94keV (Exp.) 15 7830 7835 Kinetic Energy (eV) 7840 Si : SiO2=42 : 1 SiO2 contribution < 3% 10 5 Binding Energy (eV) Y. Takata et al. Appl. Phys. Lett. 84, 4310 (2004) 4/8/2015 6100 Kinetic Energy (eV) 300sec 20 6095 0 Contribution of surface SiO2 is negligible! IMFP: Si=12nm, SiO2=16nm @ 8keV Si=1.8nm, SiO2=3nm @ 0.85keV 19 Effect of Grazing Incidence of X-rays see also V Strocov, condmat/2013 4/8/2015 20 High Sensitivity (Buried Layer and Interface) H. Wadati, A. Fujimori, H. Y. Hwang et al., PRB77, 045122 (2008) LaAlO3:3ML LaVO3:3ML LaAlO3:30ML abs (Mb/atom) at 8.05 KeV SrTiO3 10 1 0.1 0.01 1E-3 1E-4 1E-5 1E-6 5x10-7 Mb 1E-7 1E-8 0 10 20 30 40 50 60 70 80 90 1s 2s 2p 3s 3p 4s 3d 4p 5s 4d 5p 6s 5d 4f 6p Photoelectron Intensity hn=7.94 keV V 1s (BE:5467eV) 2465 2470 2475 Kinetic Energy (eV) Atomic Number 4/8/2015 21 Large Probing Depth e- eLa0.85Ba0.15MnO3 (20nm) SrTiO3 Normalized Intensity Sr 2p3/2 (BE=1940eV) x65 4015 4010 Kinetic Energy (eV) 4005 H. Tanaka et al., Phys. Rev. B 73, 094403 (2006) 4/8/2015 22 Applications 4/8/2015 23 La1-xSrxMnO3 M-I transition with Colossal magnetoresistance A.Urushibara et al., Phys. Rev. B 51, 14103 (1995) H. Fujishiro et al., J. Phys. Soc. Jpn. 67, 1799 (1998) Feature absent in earlier soft-ray PES A.Chainani et al. Phys. Rev. B 47, 15397 (1993) T.Saitoh et al., Phys. Rev. B 56 8836 (1997) MO6 Cluster model calculations Ground state:linear combination of 6 configurations 3d6C2 UH D 3d5C 3d4 3d6LC 3d5L LH 3d6L2 1.Intra-atomic multiplets 2.Crystal Field D* EF U O 2p band 4.Hybridization between coherent states at EF and Ru 3d orbitals : metallicity 3.Hybridization between O 2p and Ru 3d orbital : Covalency M. Taguchi G. Van der Laan et al PRB 23, 4369(1981) J. Imer & E. Wuilloud. Z Phys. B 21 66, 153 (1987) Comparison with cluster calculations Good agreement! AFM V* = 0.28V Δ* = 3.6 eV FM V* = 0.39V Δ* = 4.0 eV FM V* = 0.425V Δ* = 4.0 eV AFI 4/8/2015 V* = 0.25V Δ* = 3.0 eV low BE feature CT from coherent states 2p53d5C K. Horiba et al. Phys. Rev. Lett 93, 236401 (2004) 29 V1.98Cr0.02O3 (experiments) Insulator Metal (hn : 5950 eV) (hn = Al Ka :1486.7 eV) M. Taguchi et al. PRB 71,155102(2005) K. Smith et al. PRB 50, 1382 (1994) V2O3 VB Photoemission (Coherent Peak) Coherent part DMFT cal. U Mo et al. PRL 90, 186403 (2003) Zhang et al. PRL 70, 1666 (1993) Incoherent part Calculation vs. Experiment |g> 2p53d2 |D-Udc| 2p53dL 3d3L D 3d3C |f > D* |D*- Udc| 2p53d3C 3d2 M. Taguchi et al. PRB 71,155102(2005) Hole- and Electron-Doped High-Tc Cuprates * M. van Veenendaal et al. PRB 49, 1407 (1994) * Ino et al., PRL 79, 2101 (1997) * Harima et al., PRB 64, 220507(R) (2001) * Steeneken et al. PRL 90, 247005 (2003) La2CuO4 Nd2CuO4 Background(doping induced chemical potential shift) Mid-gap pinning scenario formation of new states within the band gap on doping Crossing the gap scenario M. van Veenendaal et al. PRB 49, 1407 (1994) m moves to the top of the valence band by hole-doping and bottom of the conduction band on electron-doping Calculation vs. Experiment |g > 2p53d9 |D-Udc| 2p53d10L 3d10L D 3d10C 3d9 |f > D* |D*- Udc| 2p53d10C M. Taguchi et al. Phys. Rev. Lett. 95, 17702 (2005). Cu 2p XPS (Estimated Parameters) NCCO D UH B D* LSCO EF D UHB D* O 2p band O 2p band EF CT type system: Nd1.85Ce0.15CuO4 (NCCO) M. Taguchi et al., Phys. Rev. Lett. 95, 17702 (2005). Charge-Transfer type 5.9keV 1.5keV UH D D* EF O 2p band U LH See also G. Panaccione et al. PRB 77, 125133 (2008) 4/8/2015 37 Valence Transition of YbInCu4 5950eV 800eV 43eV H. Sato et al., Phys. Rev. Lett., 93, 246404 (2004) 4/8/2015 See also Suga et al., J. Phys. Soc. Jpn, 78, 074704 (2009) 38 Combining HAXPES with optical spectroscopy Evidence for purely Yb2+ bulk state, Yb3+ surface state, and energy-loss satellite due to interband transitions YbS: Ionic crystal Yb2+S2-, hence typical Yb2+ system However, the Yb valence estimated by L-edge RIXS & XAS: K. Syassen, Physica B+C 139-140 (1986) 277. E. Annese et al., Phys. Rev. B 70 (2004) 075117. e- Intensity (arb. units) Yb 3d hn = 7.94 keV hn YbS YbS T = 300 K = 80° = 0° YbCu2Si2 T = 20 K = 0° Yb 1600 4/8/2015 3+ Yb Binding Energy (eV) 1550 1540 1530 1520 Intensity (arb. units) ~2.08 ~2.35 2+ Yb 1580 1560 1540 Binding Energy (eV) M. Matsunami 3+ Yb 2+ 1520 et al., Phys. 78, 185118(2008) Yb 3d5/2 = 0° = 80° ×3 Loss Function [Im(1/)] optical reflectivity 0 10 20 Rev. Relative B, Energy (eV) 30 -10 39 Remote hole-doping at an interface M. Takizawa et al., PRL. 102, 236401(2009) V3+(bulk) For LaAlO3/SrTiO3, see M. Sing et al. PRL 102, 176805 (2009) 4/8/2015 40 • Electronic structure of the room temperature ferromagnet Co:TiO2 anatase Science, 291, 854 (2001) 4/8/2015 41 Nature Materials 4,173(2005) Carriers : hydrogenic type 4/8/2015 42 Core level spectra 4/8/2015 T. Ohtsuki et al PRL 106, 047602(2011) Al Ka XPS J W Quilty et al PRL 96, 027202(2006) 43 Valence band spectra CoO/Co metal J W Quilty et al PRL 96, 027202(2006) 4/8/2015 44 J. Woicik et al Phys. Rev. Lett. 89, 077401(2002) 4/8/2015 45 Co 2p-3d XAS 4/8/2015 46 Co 2p-3d Resonant PES 4/8/2015 47 Ti 2p-3d Resonant PES Coherent + Incoherent feature T. Ohtsuki et al PRL 106, 047602(2011) 4/8/2015 48 4/8/2015 49 charge neutrality condition : Co2+ + VO 2− + 2Ti 4+ Co 2+ + 2Ti 3+ (VO is oxygen vacancy) Surface Science, 601, 5034(2007) 4/8/2015 50 correspondence between the well-screened feature and coherent states S. Biermann et al, PRL, 94, 026404, 2005 ; J. M. Tomczak & S. Biermann, J. Phys.: Cond. Matter, 19, 365206, 2007. J. M. 4/8/2015 Tomczak, F. Aryasetiawan & Silke Biermann, PRB, 78,115103, 2008. See also T. Koethe et al PRL 97, 166402(2006) ; S. Suga et al, New J. Physics 11, 103015 (2009). 51 Hg2Ru2O7 and Tl2Ru2O7 exhibit first order metal-insulator transitions(MIT) • • • • • • • • Hg2Ru2O7 Tc = 108 K meff ~3.7mB Ru 5+ Tl2Ru2O7 Tc = 125 K meff ~ 2.8mB Ru 4+ A Yamamoto et al JPSJ(Letters) 4, 043703 (2007) W. Klein et al J. Mat. Chemistry 17, 1356 (2007) S. Lee et al Nature Materials 5, 471 (20 2 Clear temperature dependence across the MIT Covalency and metallicity of TMCs and some standard bonding energies . Compound Tl2Ru(IV)2O7 Hg2Ru(V)2O7 Ti4O7 VO2 V2O3 CrN La0.8Sr0.2MnO3 La0.85Ba0.15MnO3 La1.85Sr0.15CuO4 Nd1.85Ce0.15CuO4 Standard bond C-H bond C-C bond C-N bond Hydrogen bonding Van der Waals Metallic bonding energy (kcal/mol) 12.60 21.68 20.06 11.07 17.29 17.53 9.80 9.22 28.83 41.51 energies in water bonding Covalent bonding energy (kcal/mol) 50.73 46.12 66.88 55.34 66.88 62.26 67.80 67.80 86.48 80.71 99 83 73 ~5 ~1 Reference No. present work present work 44 45 22 46 30 47 24 24 1 1 1 1 1 A. Chainani et al. PRB 87, 045108 (2013) HAXPES results from our group : Zhang-Rice doublet state in NiO PRL 100 206401(2008) Changes across successive first-order transitions in the Magneli compound Ti4O7 PRL 104,106401(2010) Paramagentic insulator to Anti-ferromagnetic metal transition in CrN PRL 104,236404(2010) Mixed Valency in a quantum critical f-electron system YbAlB4 PRL 104,247401(2010) Recoil effects of core and valence photoelectron in solids Y. Takata, et al., PRL101, 137601(2008) Recoil effects in PES: C 1s core level spectra of graphite Y. Takata et al., PRB 75, 233404 (2007) Pnotoelectron Intensity KE dependence at normal emission hn=870eV (DE=100meV) hn=5950eV (DE=120meV) hn=7940eV (DE=120meV) 285.5 285.0 284.5 Binding Energy (eV) 284.0 ★ not observed in Au ★ not due to semimetallic character ★ not due to bulk vs surface but due to recoil effect ! Recoil effects in core level spectra of other light elements, such as (Be, B, Al) Recoil effects in valence band (Fermi-edge) of Al @ 7.94keV Y. Takata, Y. Kayanuma et al.,Phys. Rev. Lett.101, 137601(2008) Intensity (arb. units) M(Au): 197 (m/M)xE: 22meV 1.0 M(Al): 27.0 (m/M)xE: 160meV dE=119meV 2p:115meV hn = 7.94 keV DE = 120 meV T = 20 K Al Au 0.5 0.0 -0.5 Binding Energy (eV) -1.0 Gaussian width Au:124meV Al: 160meV Theory by Y. Kayanuma, S. Tanaka and S. Oshima Y. Takata, Y. Kayanuma et al.,Phys. Rev. Lett.101, 137601(2008) isotropic Debye model 4/8/2015 61 4/8/2015 62 Bulk electronic structure of Ga1-xMnxAs 4/8/2015 A X Gray et al, Nature Materials, 11, 957(2012) 63 Bulk electronic structure of Ga1-xMnxAs 4/8/2015 A X Gray et al, Nature Materials, 11, 957(2012) 64 Future Prospects ★ Improvement of energy resolution to ~10 meV ★ Angle resolved measurements VB mapping Gray et al Photoelectron diffraction ★ Polarization dependence Ueda et al ★ Atoms and molecules Simon et al Castro et al non-dipole effects ★ Dynamics using time resolved HAXPES ★Application to high vapor pressure systems Liquids/Wet samples/Gels 4/8/2015 65 Y Takashima et al Nature Commun. Dec 2012 DOI:10.1038/ncomms2280 4/8/2015 66 Irene Chen et al., Advanced Functional Materials 22, 2535(2012) 4/8/2015 67 HAXPES has become a valuable tool ! SPring-8 (6 beamlines, not dedicated) ESRF BNL BESSY II SOLEIL PETRA III ERL ? ….. 4/8/2015 68 International WS to Conferences on HAXPES 1st in 2003 @ ESRF by Zegenhagen 2nd in 2006@ SPring-8 by Kobayashi and Suga 3rd in 2009 @ NSLS by Woicik and Fadley 4th in 2011 @ HASYLAB by Drube 5th in 2013 @ Uppsala by Svensson and Martensson 4/8/2015 69 Thank you very much for your attention 4/8/2015 70 Science 287, 1019 (2000) Mn:GaAs 4/8/2015 71 4/8/2015 72 Ti 2p HX-PES 4/8/2015 M. Taguchi et al, 73 PRL 104, 106401 (2010) HT phase 2p53d0 3d1L |D-Udc| 2p53d1L D 3d1C D* 3d0 | g› |D*-Udc| 2p53d1C | f› CT 4/8/2015 74 LT phase Ti 3+ Ti4+ cluster (V* =0) Ti4+ Ti3+ 4/8/2015 75 4/8/2015 76 IT phase Ti 3+ Ti4+ cluster (V* =0.3 eV) Remnant of Coherent states 4/8/2015 77 SUMMARY Ruthenates with and without orbital order exhibit Mott-Hubbard type band-width controlled metal-insulator transitions The Magneli phase compound Ti4O7 has an anomalous intermediate phase sandwiched between a Fermi liquid and charge ordered insulator Equivalence of screening due to coherent states and non-local screening Accurate Valence determination in d and f electron systems 4/8/2015 78 Semiconductors : HfO2:SiO2 (K. Kobayashi et al) SiO2/Si(100) (Y. Takata et al), GaAs (C. Dallera et al), Cr : GaN( J.J. Kim et al), Si (F. Offi et al), In2O3 (A. Walsh et al), etc. Elements : Co, Cu, Ag, Ni, etc. (M.Sacchi et al, G. Panaccione et al, O. Karis et al) f-electron systems : Ce systems (L. Braicovich et al, P. Fevre et al, M. Matsunami et al) Yb Mixed valence (H. Sato et al, A. Yamasaki et al), Yb Kondo (L. Moreschini et al) Titanates : XSW partial DOS ( J Woicik et al) ; Resonant Auger (J. Danger et al ) Vanadates : Mott-Hubbard transition (N. Kamakura et al, M. Taguchi et al, G. Panaccione et al, J. Woicik et al ) Cobaltates : charge order (A. Chainani et al) Manganites : doping dependence(K. Horiba et al), bilayer (F. Offi et al , S. de Jong et al) T-dependence (H. Tanaka et al, F. Offi et al, S. Ueda et al,) Cuprates : hole and electron doping (M. Taguchi et al, G. Panaccione et al, K. Maiti et al) Iron Pnictides : LaFePO(Y Kamihara et al) ; BaFe2As2 (S. de Jong et al) Nickelates : NiO (J. Woicik et al, M. Taguchi et al) Importance of s-states in a metallic oxide : PbO2 (D. J. Payne et al) Intermetallics : Huesler alloys ( C. Felser et al) Ruthenate complexes : role of intermolecular interactions ( S Svensson et al) Multilayers Oxide Multilayers 4/8/2015 : Ni/Cu (Holmstrom et al) : LaAlO3/SrTiO3 (M. Sing et al) ; LaVO3/LaAlO3 (M. Takizawa et al) 79 HAXPES has become a standard tool ! SPring-8 (6 beamlines, not dedicated) ESRF NSLS BESSY II SOLEIL APS PETRA III ALS? MAX-IV? ….. 4/8/2015 80 International WS on HAXPES 1st in 2003 @ ESRF by Zegenhagen 2nd in 2006@ SPring-8 by Kobayashi and Suga 3rd in 2009 @ NSLS by Woicik and Fadley 4th in 2011 @ HASYLAB by Drube 5th in 2013 @ Uppsala by Svensson and Martensson 4/8/2015 81 Future Prospects ★ Improvement of energy resolution to ~20 meV ★ Angle resolved measurements VB mapping Fadley, Papp et al Photoelectron diffraction ★ Polarization dependence Ueda et al ★ Application to high vapor pressure systems Liquids/Wet samples ★ Atoms and molecules non-dipole effects Simon et al Castro et al Recoil & Dynamics 4/8/2015 82 Thank You very much 4/8/2015 83 Comparison with Nb:STO(SrTiO3) Y. Ishida et al PRL 100, 056401 (2008) 4/8/2015 84 Y. Ishida et al PRL 100, 056401 (2008) 4/8/2015 85 4/8/2015 86 4/8/2015 87 Y Aiura et al. Surface Science 515, 61 (2002) 4/8/2015 88 n-type SrTiO3-d J. Chang et al PRB 81,235109(2010) 4/8/2015 89 Nature 469, 189 (2011) 4/8/2015 90 O K-edge XAS 4/8/2015 91 O K-edge Resonant PES 4/8/2015 92 Constant initial state spectra across the O K-edge 4/8/2015 93 Partial density of states near EF Y. Ishida et al PRL 100, 056401 (2008) 4/8/2015 94 Ti 2p-3d Resonant PES Coherent + Incoherent feature T. Ohtsuki et al PRL 106, 047602(2011) 4/8/2015 95 Cu 2p XPS (experiments) M. A. van Veenendaal and G. A. Sawatzky, Phys. Rev. B 49, 3473 (1994) K. Okada and A. Kotani, J. Electron Spectrosc. Relat. Phenom. 86, 119 (1997). K. Karlsson, O. Gunnarsson and O. Jepsen, Phys. Rev. Lett. 82, 3528 (1999) ; A. Koitzsch et al., Phys. Rev. B 66, 024519 (2002). O 1s XPS (Experiment) Peak shift LCO NCCO 0.25 eV LCO LSCO 0.2 eV Peak shift is rather small as compared with optical gap( 1.0 eV) O 1s XAS O 1s level LSCO UHB NCCO UHB C. T. Chen et al. Phys. Rev. Lett 66, 104(1991) ; M. Romberg et al. Phys. Rev. B 43, 333(1991) T. Fukumura et al New Journal of Physics 10, 055018 (2008) 4/8/2015 99 Recoil effects in valence band (Fermi-edge) of Al @ 880eV Intensity (arb. units) M(Au): 197 (m/M)xE: 2meV 150 1.0 hn = 880 eV DE = 120 meV T = 50 K Au Au Al Al 1000.5 50 0.0 0 -50-0.5-100 -150 -1.0 Binding BindingEnergy Energy(meV) (eV) M(Al): 27.0 (m/M)xE: 18meV dE=12meV Gaussian width Au:118meV Al: 140meV Our Experiments : Epitaxial films grown by pulsed laser deposition Characterization : Structure and ferromagnetism X-ray Absorption Spectroscopy(XAS) Resonant photoemission(PES) @ BL17 DE ~230 meV at Ti L-edge Hard X-ray PES @ BL 29 DE ~250 meV at hn = 8 KeV 4/8/2015 101 XRD RHEED Samples : PLD grown films characterized by x-ray diffraction RHEED oscillation RHEED pattern 4/8/2015 102 New Journal of Physics 10, 055018 (2008) 4/8/2015 103 0.8 mB/Co T. Fukumura et al New Journal of Physics 10, 055018 (2008) 4/8/2015 104 Recoil effects in photoelectron emission Theory by Y. Kayanuma & S. Tanaka (PRB 75, 233404 (2007) ) For an atom in free space dE=(m/M)E dE:recoil energy M: atomic mass m: electron mass E: kinetic energy For C atom at 8 keV m/M=1/22000 dE=0.36 eV In graphite dE is absorbed by the phonon bath. Excitation of phonons Mössbauer effect in g-ray emission Theoretical calculation: Debye model Normal emission: hwD=75meV Emission Angle Dependence e- Normal emission: hwD=75meV Grazing emission: hwD=150meV 285.5 Recoil effects in PES reflect phonon dynamics! Binding Energy (eV) 285.0 284.5 284.0 Graphite C 1s hn=7940eV (a) Experiment grazing (30deg) normal (85deg) (b) Theory in-plane (stretching) out-of-plane (bending) 1.0 0.5 0.0 Recoil Energy (eV) -0.5 Comparison of recoil effects in graphite M. Vos, et al., PRB 78, 024301(2008) electron scattering photoelectron emission neutron scattering Comparison between Diamond & Graphite Normakized Intensity C 1s R.T. B-doped Diamond HOPG 287 286 285 5.95keV 7.94keV 284 283 Binding Energy (eV) 282 LDA & (LDA + DMFT) of Hg2Ru2O7 Importance of multi-orbital correlations negligible influence of spin-orbit coupling L. Craco et al, PRB 79, 075125 (2009) 24 S. Baidya et al, PRB 86, 125117 (2012) (3~4 A. Chainani et al. PRB 87, 045108 (2013) Large Probing Depth e- e- Estimation of IMFP value La0.85Ba0.15MnO3 (20nm) SrTiO3 N(z)=N0exp(-z/l) l(4keV)=5nm in LBMO Sr 2p3/2 (BE=1940eV) Normalized Intensity surface layer contribution layer distance 0.4nm l=1nm: 33% l=5nm: 8% l=10nm: 4% higher KE larger l x65 4015 4010 Kinetic Energy (eV) 4005 H. Tanaka et al., Phys. Rev. B 73, 094403 (2006) 4/8/2015 113 Photoelectron Intensity Be 1s core level of polycrystalline Be Be Be 1s @ 20K DE=110meV (SX) 125meV(HX) hn=7940eV hn=5950eV hn=5950eV 114 hn=880eV Surface Surface feature 113 112 Binding Energy (eV) 111 Atomic weight: 9.0 dE(5950eV)=330meV (m/M)xE: 355meV dE(7940eV)=440meV (m/M)xE: 475meV B 1s core level of MgB2 Photoelectron Intensity a bundle of needle crystals supplied by H. Kitoh @NIMS MgB 2 B 1s @20K DE=110meV (SX) 125meV(HX) hn=880eV hn=7940eV hn=5950eV 189 188 187 Binding Energy (eV) 186 Atomic weight: 10.8 dE(5950eV)=240meV (m/M)xE: 290meV dE(7940eV)=340meV (m/M)xE: 390meV Photoelectron Intensity Al 2p core level of Al thin film Al Al 2p @ 20K DE=110meV (SX) 125meV(HX) hn=880eV hn=7940eV hn=5950eV 74.5 74.0 73.5 73.0 72.5 Binding Energy (eV) 72.0 Atomic weight: 27.0 dE(5950eV)=90meV (m/M)xE: 120meV dE(7940eV)=115meV (m/M)xE: 160meV 4/8/2015 117 XMCD synthesis and annealing in oxygen K. Mamiya, T. Koide, A. Fujimori et al, APL 89, 062506 (2006) 4/8/2015 118 Early spectroscopy : Controversy PRL 90, 017401(2003) 4/8/2015 119 Ferromagnetism is due to Co clusters postannealing in Vacuum J. Y. Kim et al PRL 90, 017401(2003) 4/8/2015 120 What is different ? Reducing atmosphere : Co clusters versus Oxidizing atmosphere : Co2+ Intrinsic ferromagnetism 4/8/2015 121 EXAFS of Co:TiO2 4/8/2015 122 Ti 2p and O 1s core levels 4/8/2015 123 (3~4 A. Chainani et al. PRB 87, 045108 (2013) V 1s core level PES of V2O3 • PM (V ∗ = 0.75) • T = 250 K • AFI (V ∗ = 0) phases. • T = 90 K N. Kamakura et al. Europhysics Letters 68, 557(2004) charge neutrality condition : Co2+ + VO 2− + 2Ti 4+ Co 2+ + 2Ti 3+ (VO is oxygen vacancy) Surface Science, 601, 5034 (2007) New.J.Phys. 10, 055018 (2008) 4/8/2015 127 Need to account for X-ray photoelectron diffraction intensity and density of states effects 4/8/2015 A X Gray et al, Nature Materials, 10, 759(2011) 128