Radiation Protection Dosimetry (2016), Vol. 168, No. 1, pp. 1–70 Advance Access publication 26 October 2014 doi:10.1093/rpd/ncu316 PERSONAL DOSE-EQUIVALENT CONVERSION COEFFICIENTS FOR 1252 RADIONUCLIDES Thomas Otto* Technology Department, CERN, CH-1211 Geneve 23, Switzerland *Corresponding author: thomas.otto@cern.ch Dose conversion coefficients for radionuclides are useful for routine calculations in radiation protection in industry, medicine and research. They give a simple and often sufficient estimate of dose rates during production, handling and storage of radionuclide sources, based solely on the source’s activity. The latest compilation of such conversion coefficients dates from 20 y ago, based on nuclear decay data published 30 y ago. The present publication provides radionuclide-specific conversion coefficients to personal dose based on the most recent evaluations of nuclear decay data for 1252 radionuclides and fluence-to-dose-equivalent conversion coefficients for monoenergetic radiations. It contains previously unknown conversion coefficients for >400 nuclides and corrects those conversion coefficients that were based on erroneous decay schemes. For the first time, estimates for the protection quantity Hp(3) are included. INTRODUCTION Dose conversion coefficients for radionuclides are useful for routine calculations in radiation protection in industry, medicine and research. They give a simple and often sufficient estimate of dose rates during production, handling and storage of radionuclide sources, based solely on the source’s activity. If the dose equivalents thus estimated turn out to be too large to be handled safely, they point out the need for a more detailed risk assessment and potentially for protective measures. After the introduction of the operational radiation protection quantities in 1993(1), a collection of dose coefficients for radionuclides has been calculated and published by Petoussi et al.(2) and widely distributed as an annexe to the Swiss Radiological Protection Ordinance(3) It lists the quantities ambient dose equivalent H*(10) and directional dose equivalent H0 (0.07.08) for .800 radionuclides contained in ICRP Publication 38(4) At the time of publication, a recommended set of fluence-to-dose-equivalent conversion coefficients were not yet available, and Petoussi et al.(2) calculated their own set. This collection has proved useful in numerous applications, but it suffers from a few limitations: ICRP Publication 38 does not list short-lived radionuclides (t1/2 , 2 min), produced copiously in present day’s research facilities, for example, the on-line mass separator ISOLDE at CERN(5). The nuclear decay data contained in (4) have been in numerous cases superseded by more recent measurements and evaluations. Recently, the ICRP has recommended to limit the dose to the eye lens to 20 mSv in a year. The appropriate operational quantity is personal dose in 3-mm depth Hp(3)(6), and it would be useful to have an estimate of this operational quantity. In 2007, the ICRP has replaced ICRP Report 38(4) with ICRP report 107(7), a compilation of nuclear decay data for 1252 radionuclides. This data set has been used previously to calculate conversion coefficients to exposure rate from photons(8). Exposure rate is, however, not a recommended protection quantity. A recalculation of the phantom-based operational radiation protection quantities defined by the ICRU(1) was missing; this gap is filled with the present publication. The motivation for the choice of personal dose Hp(d ) as the target quantity of the present calculations is 2-fold: on one hand, personal dose-equivalent Hp(d ) is the operational quantity used to estimate effective dose for an individual worker, to protect him from stochastic radiation detriment from exceeding limits on Hp(10) and deterministic damage from exceeding limits on Hp(0.07) or Hp(3). On the other hand, two detailed sets of conversion coefficients have been published recently(9, 10), and missing conversion coefficients are easy to calculate. In any case, the difference between the quantities Hp(d ) and H0 (d, 0) is small and in any case negligible for the present application, where it is overshadowed by other uncertainties in dose estimation based on source activity only. The second section of this paper explains the calculation of the personal dose conversion coefficients for radionuclides. The third section reviews the availability of fluence-to-dose-equivalent conversion coefficients for different radiation types and presents new calculations for electrons and positrons in air. In Section 4, the resulting radionuclide-specific personal dose-equivalent conversion coefficients are presented and discussed. # The Author 2014. Published by Oxford University Press. All rights reserved. For Permissions, please email: journals.permissions@oup.com Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Received 13 June 2014; revised 11 August 2014; accepted 17 September 2014 T. OTTO In the following sections, the calculation of the nuclide-specific conversion coefficients for the differZ ent radiation types hA; p ðd; rÞrad at depth d and a reference distance r is explained in more detail. CALCULATION OF PERSONAL DOSE COEFFICIENTS The personal dose coefficient hA,Z p (d, r) for a radionuclide relates the activity A(A, Z) of a radionuclide source with mass number A and proton number Z to Hp(d), the personal dose equivalent at depth d at a reference distance r between the ( point-like) radioisotope source and the receptor: Hp ðdÞ ¼ hA;Z p ðd; rÞ AðA; ZÞ Photons ð1Þ In the typical exposure situation of an operator handling a radioactive source, his critical organs and the eye lens will be at a distance of 1 m, whereas the hands are much closer to the source (order of 0.1 m). This fact is taken into account by calculating Hp(10) and Hp(3), the operational quantities for whole-body dose and the eye-lens dose, at r ¼ 100 cm, whereas Hp(0.07), the quantity used to estimate dose to the extremities, is calculated at r ¼ 10 cm. Furthermore, it is assumed that source and receptor are surrounded by air. The radionuclide R(A,Z) can transform in a daughter nuclide R 0 (A 0 ,Z 0 ) in a variety of decay modes under emission of different particles (Table 1). In the present work, only emitted particles contributing to external exposure are considered. Omitted are therefore alphaparticles and fission fragments, which are a concern for internal exposure, as well as photons and electrons with energies below a threshold under which the particles are stopped in the insensitive layer of skin or the air surrounding the subject. The personal dose from a radionuclide can be represented as a sum of components, each caused by a different radiation type: Hp ðdÞg ¼ Ka hk ðdÞ Air kerma of photons with energy E can be related to photon fluence by the relation: mtr ð4Þ Ka ðEÞ ¼ fðEÞ E @ where mtr is the mass energy transfer coefficient and r the density of air. Introducing the fluence-to-doseequivalent conversion coefficient: mtr ð5Þ hp ðd; EÞg ¼ hk ðEÞ E @ and substituting for the fluence f from a point source at distance r the expression (4 pr 2)21, the personal dose equivalent for one nuclear transmission can be written as follows: Hp ðdÞ ¼ Hp ðdÞg þ Hp ðdÞe þ Hp ðdÞn Z A; Z ¼ ðhA; p ðd; rÞg þ hp ðd; rÞe þ Z hA; p ðd; ð3Þ ð2Þ Z hA; p ðd; rÞg ¼ rÞn ÞAðA, ZÞ 1 X hp ðd; EÞg Yi 4pr2 i ð6Þ Table 1. Sources of the conversion coefficients for monoenergetic radiations used in the calculation of radionuclide-specific dose-equivalent conversion coefficients. Radiation Symbol d ¼ 10 mm d ¼ 3 mm, slab phantom d ¼ 0.07 mm, slab phantom Photons hp(d, E)g In vacuum(9) (Figure 1) In vacuum(9) In air(9), r ¼ 100 cm (Figure 2) Electrons hp(d, E)e Calculated for this work in air at r ¼ 100 cm; for E . 15 MeV from (10) (Figure 3) Calculated for this work in air at r ¼ 100 cm; Figure 6 Positrons Neutrons Calculated for this work in air Calculated for this work in air at r ¼ 100 cm; for E . 10 at r ¼ 10 cm; for E . 3 MeV MeV from (10) (Figure 4) from (10) (Figure 5) hp(10, E)n In vacuum(12) — 2 Calculated for this work in air at r ¼ 10 cm; Figure 6 — Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 In decay of a radionuclide, discrete photons with energy Ei are emitted with yield Yi, the emission probability per nuclear transmutation. One can distinguish between gamma-rays, emitted by the nucleus, and X-rays, emitted by the electron shell, but for the present work, the distinction is not important. The personal dose equivalent in a photon radiation field of is calculated from air kerma determined without phantom Ka, by multiplying with a suitable conversion coefficient (7, 11): PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES The summation extends over all photons that are emitted by the parent radionuclide. In the summation, they are weighted by the yield per transmutation Yi, so that the evaluation of (6) results the conversion coefficient for the photons emitted in one transmutation. The coefficient is the energy-dependent conversion coefficient for photons from fluence to personal dose equivalent at depth d, evaluated for energy E. Here, as in the following instances of conversion coefficients, they are assumed to be a continuous function of particle energy E, although they are tabulated at only a few fixed energy values Ej, where they are either calculated from kerma-conversion coefficients as in Equation (5) or directly in Monte–Carlo radiation transport programmes. For values of E lying between Ej and Ej þ 1, the corresponding conversion coefficient hp ðd; EÞrad is evaluated by interpolation. annihilation photons to personal dose must be calculated with Equation (6). Neutrons A few heavy radionuclides undergo spontaneous fission and emit neutrons, contributing to personal dose equivalent at 10-mm depth Hp(10). In ICRP report 107(7), yield and energy of fission neutrons are given as a continuous spectrum and the dose equivalent is calculated by integration over this spectrum: E¼0 dE FE hp ð10; EÞn ð9Þ CONVERSION COEFFICIENTS FOR MONOENERGETIC RADIATIONS A nucleus emits electrons with discrete energies as conversion electrons or Auger electrons and electrons or positrons with a continuous energy spectrum in b-decay. The contribution of the discrete spectrum of electrons to personal dose equivalent is similar to the contribution of photons: 1 X hp ðd; EÞe Yi 4pr2 i ð Emax Equation (9) is formally equivalent to Equation (8) for a single b-spectrum. Electrons and positrons Z hA; p ðd; rÞe ¼ 1 4pr2 As seen in Section 2, the calculation of radionuclidespecific dose conversion coefficients precedes by a summation or integration over the fluence spectra of the particles/radiations emitted in the decay. In the summand or integrand, the fluence at energy E is multiplied with a fluence-to-dose-equivalent conversion coefficient, which must be evaluated at the same energy E. Values of the conversion coefficients for arbitrary energies E are interpolated from a table of coefficients at fixed energies Ej, calculated with the Monte –Carlo method. In previous Monte–Carlo calculations of conversion coefficients for monoenergetic radiations, e.g. tabulated in (11, 12), two assumptions were made: ð7Þ In Equation (7), the symbols have an analogous meaning as in Equation (6). For the electron/positron emission from b-decay, the dose equivalent is calculated by integration over each branch of the spectrum, and a summation weighted by the yield of the branch Yi: ð Emax;i 1 X Z Y dE FE hp ðd; EÞe hA; i p ðd; rÞe ¼ 4pr2 i E¼0 (1) Source and receptor of the radiation are placed in vacuum, (2) The kerma approximation was used for the calculation of energy deposited by photons in the receptor. This means that the energy imparted by the photon in an interaction is deposited locally. This approximation is valid when secondary electron equilibrium is installed, as is the case for dose in 10-mm depth for photons with energies of ,3 MeV for 3-mm depth for energies of ,800 keV and for 0.07-mm depth for energies of ,300 keV. ð8Þ where FE ¼ dfðEÞ=dE is the spectral fluence of electrons/positrons. ICRP report 107(7) tabulates composite b-spectra and integration and summation can be reversed in (5), simplifying the calculation to a single integration over the composite spectrum: ! ð X 1 Emax; i A; Z dE Yi FE hp ðd; EÞe hp ðd; rÞe ¼ 4pr2 E¼0 i These two assumptions would represent a limitation for the usefulness of radionuclide-specific conversion coefficients presented here: (1) The coefficients are given to estimate external dose rates in practical cases. This implies that source and receptor are surrounded by air, not vacuum. (2) A realistic estimation of the dose to the skin or the eye lens, at 0.07-mm or 3-mm depth in tissue, is sought. Conversion coefficients calculated without the kerma approximation, explicitly ð8aÞ Note that the conversion coefficients differ for b2-decay (electrons) and bþ-decay ( positrons). In the case of bþ-decay, the positron may annihilate before leaving the source, in this case the contribution of the 3 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 hpA; Z ðd; rÞn ¼ T. OTTO The conversion coefficients presented in this publication are evaluated for whole-body exposure, i.e. on the water-filled slab phantom of 30` 30` 15 cm3. This is the standard phantom for the quantity Hp(10). For Hp(3), the difference between irradiation on a cylinder phantom representing the head and the slab phantom is small for irradiation under 08. The results Hp(0.07)slab correspond to a measurement of ‘skin dose’ on the trunk, as required by many countries’ radiation protection dosimetry regulations. This quantity is, however, only an approximate substitute for the quantity Hp(0.07)rod on the cylindrical rod phantom(11) used for dosimetry of extremities. In order to avoid confusion, the quantities for eye and skin dosimetry presented in this work are indicated Hp(3)slab and Hp(0.07)slab. In order to approximately take into account typical exposure situations, the quantities Hp(10) and Hp(3) are calculated for a distance to the source of r ¼ 100 cm (exposure to the source in a typical working distance) and Hp(0.07) for a distance of 10 cm (exposure of the hand and forearm while handling a source).The respective air layers have a significant influence electron and positron fluence by absorption and scattering in air. Table 1 gives an overview of the sources of the conversion coefficients and a reference to the corresponding figure. The following sections review these choices. Neutrons For neutrons, the conversion coefficients from fluence to personal dose equivalent at a depth of 10 mm are taken from the ICRU report 57(12), confirmed as the presently best available reference in (16). In the energy range of interest for this work, E ¼ 3–10 MeV, personal dose is underestimated at most by 20 %. Electrons and positrons Veinot and Hertel have published conversion coefficients from fluence to personal dose equivalent for Photons Veinot and Hertel(9) have published a comprehensive set of conversion coefficients from fluence to personal dose for monoenergetic photons. The coefficients were calculated with the Monte –Carlo code MCNPX 2.6(13). In the simulation, a slab phantom of dimensions 30` 30` 15 cm3 made of ICRU 4-component tissue is irradiated uniformly and perpendicular to the front face with a broad beam of monoenergetic photons. The kerma approximation is dropped, i.e. secondary electrons are explicitly transported. This leads to marked differences in conversion coefficients from previous sources (Figure 1). Absorbed dose is scored in receptor volumes at a depth of 0.07, 3 and 10 mm and yields the operational quantities at these depths. Veinot and Hertel did not observe a significant difference between conversion coefficients hp ðd; EÞg for d ¼ 3, 10 mm in vacuum or in 100 cm of air. Only for hp ð0:07; EÞg; slab ; they could find a difference between the calculations in vacuum and in 100 cm of air, owing to the build-up of secondary electrons in the air layer, which contribute to the dose in 0.07-mm depth. In the present work, the air layer of hp ð0:07; EÞg; slab is supposed to have a depth of only Figure 1. Comparison between the conversion coefficient for photons from fluence to H*(10) used in (2), the coefficient recommended by the ICRU(12) and the conversion coefficient from fluence to Hp(10) by Veinot and Hertel(9) used in this work. The difference between ambient and personal dose equivalent is negligible until E ¼ 4 MeV. Above this value, the influence of secondary electron transport in the calculations leading to (9) is visible. 4 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 10 cm. The corresponding conversion coefficients were calculated for a few energies with the Monte– Carlo code FLUKA(14, 15) in an identical numerical set-up as the one used by Veinot and Hertel (see Section 3.3). These calculations showed that the thickness of the air layer (100 cm or 10 cm) was irrelevant. The reason is that secondary electrons contributing to the dose at a depth of 0.07 mm in tissue are generated only in the last few centimetres of air before the phantom, and the additional scattering and absorption in 90 cm of air do not reduce significantly the dose per emitted photon. To conclude, for the conversion of photon fluenceto-personal dose equivalent, the coefficients published in (9) for vacuum, hp ð10, EÞg and hp(3, E)g,slab and in air, hp(0.07, E)g,slab, are used. Figures 1 and 2 show a comparison between the coefficients by Veinot and Hertel(9) used in this work, the conversion coefficient used in (2) and the coefficients presently recommended by the ICRU(12). transporting secondary electrons, are available in the literature or can be calculated with Monte– Carlo radiation transport programmes. PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES scattered in air and do not contribute to dose in 0.07-mm depth. From energies of .150 keV, the contribution to dose at 0.07-mm depth from electrons passing 10 cm of air is larger than the one of electrons out of vacuum, because of the contribution of inscattered electrons from the air layer. In Figures 3 and 5, one sees that the inscattering effect is more important for the geometry of the slab phantom used in this work for Hp(d ) than for the ICRU sphere phantom used in (2) for H0 (d, 08). For positrons, no conversion coefficients from fluence to personal dose are published. For this work, they have been calculated in the distances of r ¼ 100 and 10 cm in air and in vacuum. On the contrary to electrons, positrons contribute to personal dose at all Figure 3. Conversion coefficients for electrons from fluence to H*(10) for electrons in air used in (2), from fluence to Hp(10) in vacuum from (10) and in air, calculated in this work. Figure 2. Comparison between the conversion coefficient for photons from fluence to H0 (0.07.08) used in (2), the coefficient recommended by the ICRU(12) and the conversion coefficient from fluence to Hp(0.07)slab by Veinot and Hertel(9) used in this work. The difference between directional and personal dose equivalent is negligible until E ¼ 300 keV. The inclusion of full secondary electron transport and absorption and scatter in air in (9) lowers the conversion coefficients significantly above this threshold, with a remarked influence on many radionuclide-specific conversion coefficients. Figure 4. Conversion coefficients for electrons from fluence to Hp(3)slab in vacuum from (10) and in air, calculated in this work. 5 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 electrons(10). Calculated in vacuum, these coefficients incorporate neither the absorption and scattering of electrons nor the build-up of secondary electrons and inscattering in the air layer between source and phantom. For the present work, conversion coefficients have been calculated for Hp(d ) from electrons where source and receptor are separated by an air layer of 100 cm (d ¼ 10, 3) or 10 cm (d ¼ 0.07). The Monte–Carlo code FLUKA 2011 2b.2(14, 15) was used for these calculations. A slab phantom (30` 30` 15 cm3) made of ICRU four-component tissue (76.2 % oxygen, 11.1 % carbon, 10.1 % hydrogen and 2.6 % nitrogen) and a density of 1 g cm23 is irradiated with a homogeneous broad beam of monoenergetic electrons or positrons. Source and phantom are separated by a layer of 100 cm of air [10 cm for Hp(0.07)slab]. Scoring volumes for absorbed dose are placed at depths of 0.07 mm, 3 mm or 10 mm from the front face of the phantom. The ratio between absorbed dose in the scoring volume at a given depth d and the incident fluence of particles starting from the source yields the respective conversion coefficient. More details on these calculations and full numerical results will be given in another, forthcoming publication. The comparison of conversion coefficients from different authors and for different conditions are given in Figures 3–5 for Hp(10), Hp(3)slab and Hp(0.07)slab, respectively. In Figure 5, the particular behaviour of this coefficient deserves a comment. At energies E , 100 keV, the electrons are absorbed or T. OTTO Figure 6. Fluence-to-personal dose conversion coefficients for positrons. The coefficients from fluence to Hp(10) and Hp(3)slab are calculated for a distance r of 100 cm in air, whereas those for Hp(0.07)slab are calculated for r ¼ 10 cm. The uncertainty bars show the statistical uncertainty of the Monte– Carlo calculation. most of the electron/positron component of the decay. Table 2 gives two different boundary cases of personal dose equivalent, termed for simplicity ‘shielded’ and ‘unshielded’. In this context, ‘shielded’ means that directly ionising particles are held back in the source, leading eventually to annihilation of positrons. Photons and neutrons are not affected by the ‘shielding’, which could for example consist of a light metal or plastic encasing of the radionuclide source. The two totals are defined as the sum of the following contributions to personal dose equivalent: depths also for very low energies, by positrons stopping and annihilating in the phantom or in air. Figure 6 shows the energy dependence of the calculated personal dose conversion coefficients for positrons at depths d ¼ 0.07, 3 and 10 mm. A simple argument makes the value of the conversion coefficient at low energies plausible: annihilation photons are created in air or upon first contact with the phantom. One of the two annihilation photons is emitted in the hemisphere where the phantom is placed, and the average conversion coefficient in the range below 0.1 MeV, matches closely the conversion coefficient for photons with E ¼ 511 keV in secondary electron equilibrium at 0.07-mm depth. Hp ðdÞunshielded ¼ Hp ðdÞphoton þ Hp ðdÞe ; eþ þ Hp ðdÞneutron Hp ðdÞshielded ¼ Hp ðdÞphoton þ Hp ðdÞannihilation Interpolation for arbitrary energies þ Hp ðdÞneutron In Equations (6), (7), (8) and (9), the conversion coefficients are required at a specific energy E. A cubic spline interpolation over a logarithmic energy-axis between the monoenergetic values is performed with a tested library function (function interp1d from the scipy.interpolate library of the Python programming language(17)). Hp ðdÞe ; eþ includes the contributions from b-decay, internal transition and Auger electrons. On a first glance, it seems contradictory that Hp(d)shielded exceeds Hp(d)unshielded (d ¼ 3, 10 mm) for numerous radioisotopes decaying by bþ-decay. The explanation is that, in a shielded source, the positrons are held back, but annihilation photons are generated, the contribution of which exceeds the contribution of positrons at the specified depths. Table 3 gives the detailed contributions to personal dose for photons, internal transition and Auger electrons, b-spectra, annihilation photons and neutrons for the three depths of 0.07, 3 and 10 mm. In both tables, the results are given in microsievert per hour RESULTS AND DISCUSSION Presentation of the conversion coefficients Depending on the decay scheme of the radionuclide, the total personal dose equivalent is composed of contributions from photons, electrons/positrons and neutrons. If required, it is relatively easy to shield 6 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Figure 5. Comparison between the conversion coefficient for electrons from fluence to H’(0.07, 08) in air used in (2), the coefficient for Hp(0.07)slab in vacuum calculated by Veinot and Hertel(10) and the coefficient for Hp(0.07)slab in air calculated in this work. The coefficients calculated in air vanish for low energies and exceed the coefficient calculated in vacuum in the interval between E ¼ 150 keV and 1 MeV, due to the contribution of inscattered electrons from the air layer. Table 2. Total personal dose equivalent for the ISO slab phantom, ‘shielded’ and ‘unshielded’, for the depths of 10, 3 and 0.07 mm for radionuclides listed in ICRP report 107(7). Nuclides 7 1 4 4 6 6 6 7 7 8 8 8 9 9 10 10 11 11 12 12 13 13 13 14 14 15 15 15 16 16 16 17 17 17 17 17 17 3 7 10 10 11 14 13 16 14 15 19 17 18 19 24 22 24 27 28 26 28 29 31 32 30 32 33 35 37 38 34 34 36 38 39 40 Half-live 12.32 y 53.22 d 1.51E þ 6 y 19.255 s 20.39 m 5.70E þ 3 y 9.965 m 7.13 s 70.606 s 122.24 s 26.464 s 64.49 s 109.77 m 17.22 s 3.38 m 2.6019 y 14.9590 h 9.458 m 20.915 h 7.17E þ 5 y 2.2414 m 6.56 m 157.3 m 132 y 2.498 m 14.263 d 25.34 d 87.51 d 5.05 m 170.3 m 1.5264 s 32.00 m 3.01E þ 5 y 37.24 m 55.6 m 1.35 m Decay Mode B2 EC B2 ECBþ ECBþ B2 ECBþ B2 ECBþ ECBþ B2 ECBþ ECBþ ECBþ B2 ECBþ B2 B2 B2 ECBþ B2 B2 B2 B2 ECBþ B2 B2 B2 B2 B2 ECBþ ECBþIT B2ECBþ B2 B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 0 9 0 156 11 0 14 3882 319 33 1519 34 7 49 94 188 497 140 215 249 299 196 0 0 414 1 0 0 479 230 2353 211 0 2080 256 1414 0 9 0 291 174 0 174 209 447 174 140 174 169 174 92 340 496 139 215 380 230 193 0 0 174 0 0 0 299 212 174 281 0 181 209 463 0 9 0 1428 6 0 38 7246 1248 876 6217 894 5 2229 1462 175 482 902 205 221 4245 2636 297 0 4990 736 0 0 1323 720 6835 1021 0 4598 1705 5145 0 9 0 292 174 0 174 69 328 174 128 174 169 174 92 327 316 138 205 315 170 170 0 0 174 0 0 0 126 143 174 213 0 122 189 299 0.0 0.3 1726.4 1171.0 1578.6 31.7 1443.6 851.8 1191.1 1217.9 908.8 1214.7 1675.6 1080.2 1158.5 1563.8 1323.6 1211.8 1336.5 1130.3 982.8 1074.8 1281.4 321.2 940.7 1211.3 463.9 52.3 1179.1 1401.6 857.7 744.1 1511.3 1052.2 1156.3 965.9 0.0 0.3 0.0 8.5 6.0 0.0 6.0 0.7 7.4 6.0 4.2 6.0 5.8 6.0 3.2 7.4 3.1 2.3 4.9 6.6 1.6 2.0 0.0 0.0 6.0 0.0 0.0 0.0 1.1 1.3 6.0 5.4 0.0 1.1 3.5 3.2 Daughter nuclei with highest yield 3 He Li B 10 B 11 B 14 N 13 C 16 O 14 N 15 N 19 F 17 O 18 O 19 F 24 Na 22 Ne 24 Mg 27 Al 28 Al 26 Mg 28 Si 29 Si 31 P 32 P 30 Si 32 S 33 S 35 Cl 37 Cl 38 Cl 34 S 34 Cl 36 Ar 38 Ar 39 Ar 40 Ar 7 10 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES H Be 10 Be 10 C 11 C 14 C 13 N 16 N 14 O 15 O 19 O 17 F 18 F 19 Ne 24 Ne 22 Na 24 Na 27 Mg 28 Mg 26 Al 28 Al 29 Al 31 Si 32 Si 30 P 32 P 33 P 35 S 37 S 38 S 34 Cl 34m Cl 36 Cl 38 Cl 39 Cl 40 Cl A 34 36 S S Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 3 7 Z Table 2. Continued 37 8 18 18 18 18 18 18 19 19 19 19 19 19 19 20 20 20 20 21 21 21 21 21 21 21 21 21 22 22 22 22 23 23 23 23 23 23 24 24 A 37 39 41 42 43 44 38 40 42 43 44 45 46 41 45 47 49 42 43 44 44 46 47 48 49 50 44 45 51 52 47 48 49 50 52 53 48 49 Half-live 35.04 d 269 y 109.61 m 32.9 y 5.37 m 11.87 m 7.636 m 1.251E þ 9 y 12.360 h 22.3 h 22.13 m 17.3 m 105 s 1.02E þ 5 y 162.67 d 4.536 d 8.718 m 62.0 s 3.891 h 3.97 h 58.61 h 83.79 d 3.3492 d 43.67 h 57.2 m 102.5 s 60.0 y 184.8 m 5.76 m 1.7 m 32.6 m 15.9735 d 330 d 1.50E þ 17 y 3.743 m 1.61 m 21.56 h 42.3 m Decay Mode EC B2 B2 B2 B2 B2 ECBþ B2ECBþ B2 B2 B2 B2 B2 EC B2 B2 B2 ECBþ ECBþ ECBþ ITEC B2 B2 B2 B2 B2 EC ECBþ B2 B2 ECBþ ECBþ EC ECB2 B2 B2 ECBþ ECBþ Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 0 0 184 0 1056 268 398 22 665 162 1939 450 4086 0 0 153 321 615 27 193 47 304 20 495 2 1353 31 11 65 29 40 355 0 197 211 160 75 43 0 0 184 0 211 262 436 22 38 162 305 245 336 0 0 152 318 635 168 336 47 304 20 495 0 463 31 148 63 28 169 438 0 197 201 156 78 182 0 0 222 0 4358 527 3926 192 4885 186 4025 2609 6731 0 0 413 1959 4466 44 477 48 300 19 478 1429 6267 29 7 1830 1035 1318 351 0 166 3217 2775 75 373 0 0 169 0 177 206 332 19 32 164 233 188 244 0 0 141 134 591 168 330 48 300 19 478 0 419 29 148 64 32 169 420 0 166 176 154 78 182 0.0 1560.9 1395.5 1559.6 1016.8 1363.6 986.5 1133.6 973.3 1516.9 1040.0 1101.0 881.3 0.0 491.1 1457.8 1117.5 978.2 1319.4 1237.4 298.5 1015.2 1356.2 1512.9 1133.6 922.0 3.0 1315.9 1117.8 1184.3 1114.4 894.0 0.0 80.2 1032.5 1054.0 24.8 1261.0 0.0 0.0 1.9 0.0 2.5 4.1 7.5 0.2 0.3 6.1 2.9 4.0 2.6 0.0 0.0 1.8 1.2 12.9 6.0 7.8 3.2 4.5 1.9 6.7 0.0 6.6 2.9 5.1 3.4 3.4 5.8 7.4 0.0 1.8 1.8 2.3 5.5 7.5 Daughter nuclei with highest yield 37 Cl K K 42 K 43 K 44 K 38 Ar 40 Ca 42 Ca 43 Ca 44 Ca 45 Ca 46 Ca 41 K 45 Sc 47 Sc 49 Sc 42 Ca 43 Ca 44 Ca 44 Sc 46 Ti 47 Ti 48 Ti 49 Ti 50 Ti 44 Sc 45 Sc 51 V 52 V 47 Ti 48 Ti 49 Ti 50 Ti 52 Cr 53 Cr 48 V 49 V 39 41 40 Ar 44 Ca 50 Cr T. OTTO Ar Ar 41 Ar 42 Ar 43 Ar 44 Ar 38 K 40 K 42 K 43 K 44 K 45 K 46 K 41 Ca 45 Ca 47 Ca 49 Ca 42m Sc 43 Sc 44 Sc 44m Sc 46 Sc 47 Sc 48 Sc 49 Sc 50 Sc 44 Ti 45 Ti 51 Ti 52 Ti 47 V 48 V 49 V 50 V 52 V 53 V 48 Cr 49 Cr 39 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 51 51 55 56 50 51 52 52 53 54 56 57 58 52 53 53 55 59 60 61 62 54 55 56 57 58 58 60 60 61 62 62 56 57 59 63 65 66 57 59 60 61 62 64 66 27.7025 d 3.497 m 5.94 m 1.75 m 46.2 m 5.591 d 21.1 m 3.7E þ 6 y 312.12 d 2.5789 h 85.4 s 65.2 s 8.275 h 8.51 m 2.526 m 2.737 y 44.495 d 1.5E þ 6 y 5.98 m 68 s 1.48 m 17.53 h 77.23 d 271.74 d 70.86 d 9.04 h 5.2713 y 10.467 m 1.650 h 1.50 m 13.91 m 6.075 d 35.60 h 1.01E þ 5 y 100.1 y 2.51719 h 54.6 h 0.1963 s 81.5 s 23.7 m 3.333 h 9.673 m 12.700 h 5.120 m EC B2 B2 ECBþ ECBþ ECBþ ECBþIT EC ECBþB2 B2 B2 B2 ECBþ ECBþ IT EC B2 B2 B2 B2 ECBþ ECBþ ECBþ EC ECBþ IT B2 ITB2 B2 B2 B2 ECBþ ECBþ ECBþ B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþB2 B2 6 14 29 1177 48 470 287 0 132 274 37 1699 36 118 448 0 173 0 239 88 2779 199 467 24 131 0 360 1 20 1286 457 276 211 0 0 80 0 7147 807 514 40 198 1 31 6 0 28 705 170 520 367 0 132 239 18 349 127 200 448 0 173 0 202 86 603 317 496 24 157 0 360 1 20 220 378 276 282 0 0 79 0 191 238 557 139 172 31 15 6 3240 340 5838 2123 444 3580 0 132 2424 3208 6392 34 3221 418 0 167 0 3427 1576 7231 354 434 27 131 0 338 2 67 5826 3580 271 180 0 0 1155 0 8159 5082 2367 57 4249 1 3068 6 0 30 671 170 494 341 0 132 204 22 319 127 199 417 0 165 0 187 86 576 310 411 27 156 0 337 1 19 188 336 271 252 0 0 71 0 190 234 480 138 171 31 15 0.7 1019.3 1278.6 929.6 1048.7 552.6 969.4 0.0 2.5 1197.5 1033.8 908.7 980.7 989.8 9.8 0.0 953.8 163.4 1042.0 1132.7 863.8 1065.1 259.4 24.9 276.0 0.0 805.6 3.1 1360.4 923.8 1051.3 45.4 740.8 0.0 0.0 1253.6 436.2 799.0 921.8 1024.8 909.2 942.3 876.0 1038.4 0.3 0.0 3.0 13.2 5.8 8.2 7.6 0.0 2.3 2.9 1.6 5.0 6.3 7.2 6.3 0.0 2.2 0.0 3.3 3.0 13.0 7.6 6.2 2.9 3.2 0.0 4.0 0.0 1.3 2.3 4.2 8.5 4.8 0.0 0.0 0.9 0.0 6.2 7.1 9.3 4.7 5.9 1.1 0.2 51 V Mn Mn 50 Cr 51 Cr 52 Cr 52 Mn 53 Cr 54 Cr 56 Fe 57 Fe 58 Fe 52m Mn 53 Mn 53 Fe 55 Mn 59 Co 60m Co 61 Co 62 Co 54 Fe 55 Fe 56 Fe 57 Fe 58 Fe 58 Co 60 Ni 60 Co 61 Ni 62 Ni 62 Ni 56 Co 57 Co 59 Co 63 Cu 65 Cu 66 Cu 57 Ni 59 Ni 60 Ni 61 Ni 62 Ni 64 Ni 66 Zn 55 56 52 Cr 54 Fe 60 Ni 64 Zn Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 9 24 24 24 25 25 25 25 25 25 25 25 25 26 26 26 26 26 26 26 26 27 27 27 27 27 27 27 27 27 27 27 28 28 28 28 28 28 29 29 29 29 29 29 29 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Cr Cr 56 Cr 50m Mn 51 Mn 52 Mn 52m Mn 53 Mn 54 Mn 56 Mn 57 Mn 58m Mn 52 Fe 53 Fe 53m Fe 55 Fe 59 Fe 60 Fe 61 Fe 62 Fe 54m Co 55 Co 56 Co 57 Co 58 Co 58m Co 60 Co 60m Co 61 Co 62 Co 62m Co 56 Ni 57 Ni 59 Ni 63 Ni 65 Ni 66 Ni 57 Cu 59 Cu 60 Cu 61 Cu 62 Cu 64 Cu 66 Cu 55 Table 2. Continued 67 10 29 29 30 30 30 30 30 30 30 30 30 30 31 31 31 31 31 31 31 31 31 32 32 32 32 32 32 32 32 33 33 33 33 33 33 33 33 33 A 67 69 60 61 62 63 65 69 69 71 71 72 64 65 66 67 68 70 72 73 74 66 67 68 69 71 75 77 78 68 69 70 71 72 73 74 76 77 Half-live 61.83 h 2.85 m 2.38 m 89.1 s 9.186 h 38.47 m 244.06 d 56.4 m 13.76 h 2.45 m 3.96 h 46.5 h 2.627 m 15.2 m 9.49 h 3.2612 d 67.71 m 21.14 m 14.10 h 4.86 h 8.12 m 2.26 h 18.9 m 270.95 d 39.05 h 11.43 d 82.78 m 11.30 h 88 m 151.6 s 15.23 m 52.6 m 65.28 h 26.0 h 80.30 d 17.77 d 1.0778 d 38.83 h Decay Mode B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ B2 ITB2 B2 B2 B2 ECBþ ECBþ ECBþ EC ECBþ B2EC B2 B2 B2 ECBþ ECBþ EC ECBþ EC B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ EC ECBþB2 B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 21 93 205 2022 63 71 83 0 72 81 261 29 1970 81 1089 28 42 2 399 61 640 80 282 0 109 0 6 176 49 2625 223 538 51 295 3 76 141 1 21 81 259 243 77 184 86 0 72 51 260 29 465 198 314 28 161 1 375 61 420 118 235 0 147 0 6 175 49 555 191 638 97 288 3 126 66 1 21 2124 3421 6086 63 2250 82 1 72 2994 512 33 5259 1601 3372 28 1203 570 1128 120 2897 82 3744 3 115 3 24 1161 50 6916 3977 2463 52 3137 9 126 3218 2 21 79 260 229 77 184 84 0 72 51 261 33 387 196 236 28 161 1 307 65 320 121 229 3 146 3 6 171 50 510 187 595 99 282 9 128 65 2 1194.2 1129.7 975.8 878.7 159.5 1000.6 22.2 1488.3 81.0 1052.7 1303.8 677.7 909.0 1021.3 528.5 16.9 1030.9 1227.3 1358.6 1374.8 1109.6 427.9 981.5 0.9 352.6 1.0 1410.2 1330.6 1497.1 863.1 928.3 995.3 730.8 919.8 2.1 927.6 1046.9 1473.5 2.0 1.4 8.8 6.9 2.9 6.0 1.2 0.0 3.0 1.5 9.0 4.1 8.6 7.4 5.0 2.2 5.4 0.0 4.7 4.7 5.6 6.5 8.8 0.9 3.9 1.0 0.5 7.5 3.6 11.1 6.6 12.3 5.5 7.6 2.1 4.3 1.7 0.1 Daughter nuclei with highest yield 67 Zn Zn Cu 61 Cu 62 Cu 63 Cu 65 Cu 69 Ga 69 Zn 71 Ga 71 Ga 72 Ga 64 Zn 65 Zn 66 Zn 67 Zn 68 Zn 70 Ge 72 Ge 73 Ge 74 Ge 66 Ga 67 Ga 68 Ga 69 Ga 71 Ga 75 As 77 As 78 As 68 Ge 69 Ge 70 Ge 71 Ge 72 Ge 73 Ge 74 Ge 76 Se 77 Se 69 60 69 Ga 70 Zn 74 Se T. OTTO Cu Cu 60 Zn 61 Zn 62 Zn 63 Zn 65 Zn 69 Zn 69m Zn 71 Zn 71m Zn 72 Zn 64 Ga 65 Ga 66 Ga 67 Ga 68 Ga 70 Ga 72 Ga 73 Ga 74 Ga 66 Ge 67 Ge 68 Ge 69 Ge 71 Ge 75 Ge 77 Ge 78 Ge 68 As 69 As 70 As 71 As 72 As 73 As 74 As 76 As 77 As 69 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 78 78 79 70 71 72 73 73 75 77 79 79 81 81 83 83 84 72 73 74 74 75 76 76 77 77 78 80 80 82 82 83 84 84 85 74 75 76 77 79 81 81 83 85 85 90.7 m 9.01 m 41.1 m 4.74 m 8.40 d 7.15 h 39.8 m 119.779 d 17.36 s 2.95E þ 5 y 3.92 m 18.45 m 57.28 m 22.3 m 70.1 s 3.1 m 78.6 s 3.4 m 25.4 m 46 m 96.7 m 16.2 h 1.31 s 57.036 h 4.28 m 6.46 m 17.68 m 4.4205 h 35.30 h 6.13 m 2.40 h 31.80 m 6.0 m 2.90 m 11.50 m 4.29 m 14.8 h 74.4 m 35.04 h 2.29E þ 5 y 13.10 s 1.83 h 10.756 y 4.480 h B2 B2 ECBþ ECBþ EC ECBþ ITECBþ EC IT B2 ITB2 B2 ITB2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ITECBþ ECBþ IT ECBþB2 B2ECBþ IT B2 ITB2 B2 B2 B2 B2 ECBþ ECBþ EC ECBþ ECBþ EC ITEC IT B2 B2IT 900 7 60 655 14 88 16 71 17 0 5 2 6 408 506 73 5170 473 961 1358 101 547 20 57 8 83 10 17 412 12 1 1204 416 20 76 859 83 69 37 7 26 2 0 29 193 6 130 262 14 191 45 71 17 0 5 1 6 392 143 73 458 243 570 578 206 395 20 58 8 176 13 17 412 6 1 217 414 10 185 218 83 180 48 7 26 2 0 29 3934 1861 108 4685 51 164 171 100 30 0 27 425 28 833 4079 280 7790 4544 2977 4175 660 2237 69 85 29 2880 1199 59 416 132 3 3754 2349 2934 724 5417 118 1055 64 34 34 10 0 32 176 6 171 259 51 206 52 100 30 0 27 1 28 356 130 74 436 247 421 495 214 342 59 86 29 178 15 59 404 28 1 158 386 10 197 224 118 187 75 34 34 10 0 32 1062.8 1105.5 695.9 946.3 13.6 943.4 260.5 48.2 1274.8 32.5 6.7 1255.4 7.4 1424.2 1010.1 1304.5 854.1 921.4 974.0 908.5 932.3 640.1 14.0 61.5 6.1 947.9 1095.1 11.5 1221.4 29.8 1470.1 1089.1 1104.6 1047.0 1017.9 912.4 25.5 1000.8 143.6 7.3 1061.8 1.9 1470.9 1397.2 3.4 0.2 19.7 8.8 13.6 13.2 3.6 15.1 5.1 0.0 6.5 0.1 6.6 9.1 2.4 3.3 11.0 9.7 10.9 12.5 10.9 11.4 11.3 10.7 5.9 6.6 0.9 11.5 8.2 5.9 0.0 2.1 7.3 0.2 11.4 10.8 13.5 10.0 8.8 7.2 4.3 1.9 0.0 3.2 78 Se Se As 71 As 72 As 73 As 73 Se 75 As 77 Se 79 Br 79 Se 81 Br 81 Se 83 Br 83 Br 84 Br 72 Se 73m Se 74 Se 74 Se 75 Se 76 Se 76 Br 77 Se 77 Br 78 Se 80 Kr 80 Br 82 Kr 82 Br 83m Kr 84 Kr 84 Kr 85m Kr 74 Br 75 Br 76 Br 77 Br 79 Br 81 Br 81 Kr 83 Kr 85 Rb 85 Kr 79m 79 Se 73 As 79 Br 81 Br 73 Se 76 Se 78 Kr Se 70 80 82 83 85 Kr Kr Kr 76m 77m Br Br 81 Br 85 Rb Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 11 33 33 34 34 34 34 34 34 34 34 34 34 34 34 34 34 35 35 35 35 35 35 35 35 35 35 35 35 35 35 35 35 35 35 36 36 36 36 36 36 36 36 36 36 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES As As 70 Se 71 Se 72 Se 73 Se 73m Se 75 Se 77m Se 79 Se 79m Se 81 Se 81m Se 83 Se 83m Se 84 Se 72 Br 73 Br 74 Br 74m Br 75 Br 76 Br 76m Br 77 Br 77m Br 78 Br 80 Br 80m Br 82 Br 82m Br 83 Br 84 Br 84m Br 85 Br 74 Kr 75 Kr 76 Kr 77 Kr 79 Kr 81 Kr 81m Kr 83m Kr 85 Kr 85m Kr 79 Table 2. Continued 87 12 36 36 36 37 37 37 37 37 37 37 37 37 37 37 37 37 37 37 37 37 37 37 38 38 38 38 38 38 38 38 38 38 38 38 38 38 39 39 A 87 88 89 77 78 78 79 80 81 81 82 82 83 84 84 86 86 87 88 89 90 90 79 80 81 82 83 85 85 87 89 90 91 92 93 94 81 83 Half-live 76.3 m 2.84 h 3.15 m 3.77 m 17.66 m 5.74 m 22.9 m 33.4 s 4.576 h 30.5 m 1.273 m 6.472 h 86.2 d 32.77 d 20.26 m 18.642 d 1.017 m 4.923E10 y 17.78 m 15.15 m 158 s 258 s 2.25 m 106.3 m 22.3 m 25.36 d 32.41 h 64.84 d 67.63 m 2.815 h 50.53 d 28.79 y 9.63 h 2.66 h 7.423 m 75.3 s 70.4 s 7.08 m Decay Mode B2 B2 B2 ECBþ ECBþ ECBþIT ECBþ ECBþ ECBþ ITECBþ ECBþ ECBþ EC ECBþB2 IT B2EC IT B2 B2 B2 B2 B2IT ECBþ ECBþ ECBþ EC ECBþ EC ITECBþ ITEC B2 B2 B2 B2 B2 B2 ECBþ ECBþ Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 660 267 1224 1413 1281 1565 143 2436 47 11 528 429 91 110 70 15 92 0 3097 705 3389 1523 1690 66 160 11 104 95 40 58 0 0 120 190 403 208 1991 532 108 250 256 260 514 486 248 202 92 12 188 463 91 151 70 14 92 0 83 307 201 402 210 82 236 11 146 95 40 58 0 0 109 190 338 200 209 232 4498 862 4381 5764 3924 5210 1693 6780 66 32 4914 483 119 246 80 919 93 0 6298 2505 5643 4482 6397 91 2754 37 149 122 45 63 368 0 1234 226 1812 1787 6560 4403 83 176 205 261 381 444 261 202 112 33 189 476 119 170 80 14 93 0 63 259 122 297 223 107 241 37 180 122 45 63 0 0 109 170 313 176 224 246 1023.9 1339.0 1037.2 898.9 886.6 800.2 1125.9 842.1 441.8 19.0 893.3 381.8 12.1 467.5 1126.2 1213.6 26.0 1143.3 895.0 1152.0 944.3 976.5 873.1 191.4 1052.2 6.2 405.4 18.4 87.5 304.0 1254.2 1456.8 1265.6 1385.5 1699.3 1125.0 860.2 895.4 2.2 3.7 4.2 10.5 10.3 11.7 12.9 6.8 7.9 5.0 6.4 14.9 9.5 8.0 6.4 0.2 3.0 0.0 0.7 3.5 1.6 4.2 11.2 8.4 10.5 6.2 12.0 9.2 4.3 3.7 0.0 0.0 2.0 2.0 7.4 1.9 11.8 11.2 Daughter nuclei with highest yield 87 Rb Rb Rb 77 Kr 78 Kr 78 Rb 79 Kr 80 Kr 81m Kr 81 Rb 82 Kr 82 Kr 83m Kr 84 Kr 84 Rb 86 Sr 86 Rb 87 Sr 88 Sr 89 Sr 90 Sr 90 Sr 79 Rb 80 Rb 81 Rb 82 Rb 83 Rb 85 Rb 85 Sr 87 Rb 89 Y 90 Y 91m Y 92 Y 93 Y 94 Y 81 Sr 83 Sr 88 89 78 Kr 81 Kr Kr 81 83 84 Kr Sr 86 Kr 90 Rb 81m 85 87 91 Rb Rb Sr Y 81m Kr T. OTTO Kr Kr 89 Kr 77 Rb 78 Rb 78m Rb 79 Rb 80 Rb 81 Rb 81m Rb 82 Rb 82m Rb 83 Rb 84 Rb 84m Rb 86 Rb 86m Rb 87 Rb 88 Rb 89 Rb 90 Rb 90m Rb 79 Sr 80 Sr 81 Sr 82 Sr 83 Sr 85 Sr 85m Sr 87m Sr 89 Sr 90 Sr 91 Sr 92 Sr 93 Sr 94 Sr 81 Y 83 Y 88 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 83m 83 84 85 85 86 86 87 87 88 89 90 90 91 91 92 93 94 95 85 86 87 88 89 89 93 95 97 87 88 88 89 89 90 91 91 92 92 93 94 94 95 95 96 97 2.85 m 39.5 m 2.68 h 4.86 h 14.74 h 48 m 79.8 h 13.37 h 106.65 d 15.663 s 64.10 h 3.19 h 58.51 d 49.71 m 3.54 h 10.18 h 18.7 m 10.3 m 7.86 m 16.5 h 1.68 h 83.4 d 78.41 h 4.161 m 1.53E þ 6 y 64.032 d 16.744 h 3.75 m 14.5 m 7.78 m 2.03 h 66 m 14.60 h 680 y 60.86 d 3.47E þ 7 y 10.15 d 16.13 y 2.03E þ 4 y 6.263 m 34.991 d 3.61 d 23.35 h 72.1 m ECBþIT ECBþ ECBþ ECBþ ECBþ ITECBþ ECBþ ITECBþ ECBþ IT B2 ITB2 B2 IT B2 B2 B2 B2 ECBþ ECBþ ECBþ EC ECBþ ITECBþ B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ITECBþ EC ECBþ IT B2 ITB2 B2 ITB2 B2 B2 227 906 91 137 497 39 88 55 379 140 2 112 1 89 760 107 1918 1530 552 80 58 81 156 101 0 118 142 1186 1115 1317 378 129 500 16 18 253 163 3 248 12 123 23 388 108 148 623 187 208 537 40 88 56 380 140 0 112 0 89 38 14 115 133 246 80 158 81 193 104 0 118 140 220 676 638 208 225 581 17 18 253 164 3 248 12 123 23 388 108 2674 4281 630 1457 694 42 113 61 339 140 2345 115 457 91 4959 3794 6113 4467 4571 124 2007 106 173 107 0 119 1156 5958 5349 5286 3809 1897 591 37 34 274 184 6 249 25 123 36 385 167 157 612 195 202 512 41 114 62 338 140 0 115 0 91 37 12 110 90 245 124 161 106 211 105 0 119 140 235 685 618 190 229 469 38 33 274 184 6 249 25 123 35 384 109 739.8 903.6 830.8 640.0 449.3 187.1 16.0 366.3 13.5 10.6 1086.9 218.8 1241.5 67.9 979.2 1029.0 909.8 1049.2 881.7 131.6 870.1 54.6 392.4 79.3 0.0 1030.0 1213.6 1383.0 894.0 887.9 714.9 873.1 931.9 6.6 3.9 14.6 8.4 0.8 1406.4 9.9 32.0 2140.6 1497.5 1362.1 8.0 13.5 8.0 7.8 13.4 3.6 8.6 3.7 9.5 2.3 0.0 6.6 0.0 3.1 0.6 0.4 1.8 1.1 8.6 14.0 6.0 8.6 7.8 3.3 0.0 2.4 2.9 13.1 19.6 15.0 6.3 8.5 12.6 4.9 3.8 10.0 7.3 0.8 4.7 3.0 2.3 3.9 8.0 2.7 83 Sr Sr 85m Sr 85 Sr 86 Sr 86 Y 87m Sr 87 Y 88 Sr 89 Y 90 Zr 90 Y 91 Zr 91 Y 92 Zr 93 Zr 94 Zr 95 Zr 85m Y 86 Y 87m Y 88 Y 89 Y 89 Zr 93m Nb 95 Nb 97 Nb 87 Zr 88 Zr 88 Zr 89 Zr 89m Zr 90 Zr 91 Zr 91 Nb 92 Zr 92 Zr 93 Nb 94 Mo 94 Nb 95 Mo 95 Nb 96 Mo 97 Mo 83 84 Y 85m Sr 86 Sr 87 Sr 90 Zr 85 Y 87 Y 89 Y Nb 95m Nb 93 89m Zr 91 Zr 94 Mo 95 Mo Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 13 39 39 39 39 39 39 39 39 39 39 39 39 39 39 39 39 39 39 40 40 40 40 40 40 40 40 40 41 41 41 41 41 41 41 41 41 41 41 41 41 41 41 41 41 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Y Y 85 Y 85m Y 86 Y 86m Y 87 Y 87m Y 88 Y 89m Y 90 Y 90m Y 91 Y 91m Y 92 Y 93 Y 94 Y 95 Y 85 Zr 86 Zr 87 Zr 88 Zr 89 Zr 89m Zr 93 Zr 95 Zr 97 Zr 87 Nb 88 Nb 88m Nb 89 Nb 89m Nb 90 Nb 91 Nb 91m Nb 92 Nb 92m Nb 93m Nb 94 Nb 94m Nb 95 Nb 95m Nb 96 Nb 97 Nb 84m Table 2. Continued 98m 14 41 41 41 42 42 42 42 42 42 42 42 42 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 43 44 44 44 44 44 A 98 99 99 89 90 91 91 93 93 99 101 102 91 91 92 93 93 94 94 95 95 96 96 97 97 98 99 99 101 102 102 104 105 92 94 95 97 103 Half-live 51.3 m 15.0 s 2.6 m 2.11 m 5.56 h 15.49 m 64.6 s 4.0E þ 3 y 6.85 h 65.94 h 14.61 m 11.3 m 3.14 m 3.3 m 4.25 m 2.75 h 43.5 m 293 m 52.0 m 20.0 h 61 d 4.28 d 51.5 m 2.6E þ 6 y 90.1 d 4.2E þ 6 y 2.111E þ 5 y 6.015 h 14.2 m 5.28 s 4.35 m 18.3 m 7.6 m 3.65 m 51.8 m 1.643 h 2.9 d 39.26 d Decay Mode B2 B2 B2IT ECBþ ECBþ ECBþ ECBþIT EC ITEC B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ITECBþ ECBþ ECBþ EC ECBþIT EC ITECBþ EC IT B2 B2 ITB2 B2 B2 B2IT B2 B2 ECBþ ECBþ ECBþ EC B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 438 477 924 2261 120 606 259 17 348 25 220 3 1974 2059 1954 220 128 420 230 144 129 414 16 18 14 229 0 25 59 2028 374 1560 411 330 104 187 61 85 427 43 100 202 161 167 216 17 348 25 218 3 357 238 594 238 132 438 308 144 130 414 16 18 14 229 0 25 59 13 356 313 130 371 104 210 61 85 1709 5221 4717 6502 143 5132 1780 35 329 51 957 6 5429 6354 6454 211 160 435 2206 161 146 429 23 34 25 231 0 26 128 6656 1742 5441 4129 2248 119 198 76 85 404 52 74 199 184 167 208 35 326 26 199 4 301 236 558 227 103 453 297 161 147 429 23 34 25 231 0 26 60 12 308 257 124 381 119 215 76 85 1220.8 993.2 993.6 833.4 857.9 862.7 457.8 4.4 1064.8 1376.2 1494.0 1457.3 841.6 838.5 1138.4 197.7 364.4 201.5 734.7 8.7 125.7 16.4 2.2 4.1 2.9 1294.7 906.0 67.5 1397.3 874.4 1147.6 980.7 1105.9 1019.1 20.0 234.4 115.8 280.8 7.3 5.6 1.8 6.4 12.9 5.9 5.1 4.4 7.8 1.0 4.4 0.3 7.5 7.8 16.4 6.3 4.1 11.9 8.0 6.6 8.3 11.3 2.1 4.1 2.9 5.1 0.0 2.6 3.6 0.3 6.4 6.4 5.5 21.6 7.1 8.8 7.5 3.0 Daughter nuclei with highest yield 98 Mo Mo Mo 89 Nb 90 Nb 91 Nb 91m Nb 93m Nb 93 Mo 99m Tc 101 Tc 102 Tc 91 Mo 91m Mo 92 Mo 93 Mo 93 Tc 94 Mo 94 Mo 95 Mo 95 Tc 96 Mo 96 Tc 97 Mo 97 Tc 98 Ru 99 Ru 99 Tc 101 Ru 102 Ru 102 Tc 104 Ru 105 Ru 92 Tc 94m Tc 95 Tc 97 Tc 103m Rh 99 99 99 Nb 91m Nb Mo Nb 93 Nb 99 Tc 91 93 91m 91 Mo Mo 93 Mo 95 Mo 96 Mo 99 Ru 102 Ru 95m Tc Tc 103 Rh 97m T. OTTO Nb Nb 99m Nb 89 Mo 90 Mo 91 Mo 91m Mo 93 Mo 93m Mo 99 Mo 101 Mo 102 Mo 91 Tc 91m Tc 92 Tc 93 Tc 93m Tc 94 Tc 94m Tc 95 Tc 95m Tc 96 Tc 96m Tc 97 Tc 97m Tc 98 Tc 99 Tc 99m Tc 101 Tc 102 Tc 102m Tc 104 Tc 105 Tc 92 Ru 94 Ru 95 Ru 97 Ru 103 Ru 99 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 105 105 106 107 108 94 95 95 96 96 97 97 98 99 99 100 100 101 101 102 102 103 104 104 105 106 106 107 108 109 96 97 98 99 100 101 103 107 109 109 111 112 114 99 100 4.44 h 373.59 d 3.75 m 4.55 m 70.6 s 5.02 m 1.96 m 9.90 m 1.51 m 30.7 m 46.2 m 8.7 m 16.1 d 4.7 h 20.8 h 4.6 m 3.3 y 4.34 d 207 d 3.742 y 56.114 m 42.3 s 4.34 m 35.36 h 29.80 s 131 m 21.7 m 16.8 s 80 s 122 s 3.10 m 17.7 m 21.4 m 3.63 d 8.47 h 16.991 d 6.5E þ 6 y 13.7012 h 4.69 m 23.4 m 21.03 h 2.42 m 124 s 2.24 m B2 B2 B2 B2 ECBþ ECBþ ITECBþ ECBþ ITECBþ ECBþ ECBþIT ECBþ ECBþ ECBþ ECBþ ITECBþ EC ECIT ECBþB2 ECBþIT IT B2EC ITB2 B2 B2 B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ EC ECBþ EC B2 B2 IT B2 B2 B2 ECBþ ECBþ 126 0 118 13 5787 439 206 576 461 164 295 633 114 112 396 34 72 69 70 365 2 6 29 14 496 445 55 1623 59 195 435 85 152 59 83 21 0 11 27 9 8 5 940 2473 126 0 54 13 562 385 128 620 201 241 315 296 121 124 400 35 72 69 97 365 2 2 29 14 34 445 55 54 55 247 362 93 214 59 92 21 0 11 27 8 8 5 362 436 172 0 3169 82 8005 3008 565 2398 1880 1105 681 4744 131 123 444 47 85 81 91 377 3 2555 38 14 4911 481 113 6379 2194 283 2318 97 978 76 101 31 0 17 30 1702 14 197 4499 6388 129 0 53 14 516 357 113 603 189 237 261 290 137 135 342 46 85 81 104 377 3 2 38 14 34 431 56 54 57 252 329 105 209 76 109 31 0 14 30 7 14 5 340 409 1484.6 0.0 1087.6 1476.4 813.9 729.3 192.1 755.6 337.2 674.6 414.4 848.4 104.4 155.6 57.0 10.1 142.1 175.2 540.1 27.5 0.4 1055.2 5.7 1146.0 963.8 1475.7 1419.4 899.2 1145.9 477.9 725.7 109.3 589.4 10.2 111.6 3.4 0.0 1440.7 1405.5 1122.9 501.4 1317.8 862.4 825.4 4.2 0.0 1.6 1.5 11.0 8.6 3.6 14.5 5.3 8.5 8.6 8.7 9.0 7.4 9.3 4.7 8.5 6.7 5.1 12.2 0.4 0.1 4.1 0.9 1.0 9.8 3.3 2.0 3.7 9.2 10.1 7.1 8.8 8.2 8.2 3.4 0.0 1.5 3.0 0.2 1.6 0.4 10.5 10.0 105 Rh Rh Rh 108 Rh 94 Ru 95 Ru 95 Rh 96 Ru 96 Rh 97 Ru 97 Ru 98 Ru 99 Ru 99 Ru 100 Ru 100 Rh 101 Ru 101 Rh 102 Ru 102 Rh 103 Rh 104 Pd 104 Rh 105 Pd 106 Pd 106 Pd 107 Pd 108 Pd 109 Pd 96m Rh 97 Rh 98 Rh 99m Rh 100 Rh 101m Rh 103m Rh 107 Ag 109 Ag 109 Pd 111m Ag 112 Ag 114 Ag 99 Pd 100 Pd 106 107 95 Ru 96 Ru 97 Rh 100 Ru 101 Ru Pd 102 Ru 102 104 104 Ru Pd 97m 99 Rh Rh 101 103 111 Rh Rh Ag Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 15 44 44 44 44 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 45 46 46 46 46 46 46 46 46 46 46 46 46 46 47 47 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ru Ru 107 Ru 108 Ru 94 Rh 95 Rh 95m Rh 96 Rh 96m Rh 97 Rh 97m Rh 98 Rh 99 Rh 99m Rh 100 Rh 100m Rh 101 Rh 101m Rh 102 Rh 102m Rh 103m Rh 104 Rh 104m Rh 105 Rh 106 Rh 106m Rh 107 Rh 108 Rh 109 Rh 96 Pd 97 Pd 98 Pd 99 Pd 100 Pd 101 Pd 103 Pd 107 Pd 109 Pd 109m Pd 111 Pd 112 Pd 114 Pd 99 Ag 100m Ag 106 Table 2. Continued 101 16 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 47 48 48 48 48 48 48 48 48 48 48 48 48 48 48 A 101 102 102 103 104 104 105 105 106 106 108 108 109 110 110 111 111 112 113 113 114 115 116 117 101 102 103 104 105 107 109 111 113 113 115 115 117 117 Half-live 11.1 m 12.9 m 7.7 m 65.7 m 69.2 m 33.5 m 41.29 d 7.23 m 23.96 m 8.28 d 2.37 m 418 y 39.6 s 24.6 s 249.76 d 7.45 d 64.8 s 3.130 h 5.37 h 68.7 s 4.6 s 20.0 m 2.68 m 73.6 s 1.36 m 5.5 m 7.3 m 57.7 m 55.5 m 6.50 h 461.4 d 48.50 m 7.7E þ 15 y 14.1 y 53.46 h 44.6 d 2.49 h 3.36 h Decay Mode ECBþ ECBþ ECBþIT ECBþ ECBþ ECBþIT EC ITECBþ ECBþB2 EC B2ECBþ ECIT IT B2EC B2IT B2 ITB2 B2 B2 ITB2 B2 B2 B2 B2 ECBþ ECBþ ECBþ EC ECBþ ECBþ EC IT B2 B2IT B2 B2 B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 228 536 331 111 412 239 109 0 48 458 4 285 11 73 427 5 6 837 14 38 2770 182 1924 791 649 134 300 68 163 33 30 60 0 0 34 6 162 281 261 517 272 152 437 281 109 0 127 458 4 285 11 5 427 5 6 101 12 38 39 70 289 173 382 155 309 68 202 33 30 60 0 0 34 5 162 281 2522 2687 1157 212 436 2346 120 0 839 455 505 295 14 3766 421 8 8 4424 1249 149 6879 3451 5900 3991 3388 139 1041 77 370 43 40 64 0 0 39 471 717 307 257 475 213 156 430 258 120 0 130 454 4 295 14 5 418 5 8 91 12 39 35 59 222 128 347 160 265 77 183 44 40 64 0 0 34 5 150 232 789.7 774.8 375.2 422.5 256.7 638.2 54.4 0.1 677.8 40.6 1212.0 29.4 1.5 999.0 434.0 1443.1 11.2 1013.9 1174.5 493.6 863.2 1129.6 927.6 1091.6 948.7 226.2 476.1 6.8 348.4 7.7 4.3 1104.6 752.1 1393.6 1411.2 1241.7 1237.8 1287.6 9.4 11.7 5.0 7.6 11.3 8.2 7.8 0.0 5.4 13.0 0.2 10.7 1.5 0.1 7.7 0.3 0.8 1.8 0.6 2.1 0.8 1.9 4.3 3.2 10.0 7.2 7.4 5.6 5.7 4.6 4.3 5.6 0.0 0.0 1.3 0.1 3.7 3.4 Daughter nuclei with highest yield 101 Pd Pd Ag 103 Pd 104 Pd 104 Ag 105 Pd 105 Ag 106 Pd 106 Pd 108 Cd 108 Ag 109 Ag 110 Cd 110 Ag 111 Cd 111 Ag 112 Cd 113 Cd 113 Ag 114 Cd 115 Cd 116 Cd 117 Cd 101 Ag 102m Ag 103 Ag 104m Ag 105m Ag 107 Ag 109 Ag 111 Cd 113 In 113 Cd 115m In 115 In 117m In 117 In 102 102 102 Pd 104 Pd 105 Pd Cd 106 108 108 110 110 111 Pd Pd Pd Cd Cd 113m 113 Cd Cd 115m Cd 117m Cd 102 Ag 105 Ag 113 In 115m In In 117m In 117 T. OTTO Ag Ag 102m Ag 103 Ag 104 Ag 104m Ag 105 Ag 105m Ag 106 Ag 106m Ag 108 Ag 108m Ag 109m Ag 110 Ag 110m Ag 111 Ag 111m Ag 112 Ag 113 Ag 113m Ag 114 Ag 115 Ag 116 Ag 117 Ag 101 Cd 102 Cd 103 Cd 104 Cd 105 Cd 107 Cd 109 Cd 111m Cd 113 Cd 113m Cd 115 Cd 115m Cd 117 Cd 117m Cd 102 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 118 118 119 119 103 105 106 106 107 108 108 109 109 110 110 111 111 112 112 113 114 114 115 115 116 117 117 118 118 119 119 121 121 106 108 109 110 111 113 113 117 119 121 121 123 50.3 m 2.69 m 2.20 m 60 s 5.07 m 6.2 m 5.2 m 32.4 m 58.0 m 39.6 m 4.2 h 1.34 m 4.9 h 69.1 m 2.8047 d 7.7 m 14.97 m 20.56 m 1.6579 h 71.9 s 49.51 d 4.41E þ 14 y 4.486 h 54.41 m 43.2 m 116.2 m 5.0 s 4.364 m 2.4 m 18.0 m 23.1 s 3.88 m 1.92 m 10.30 m 18.0 m 4.11 h 35.3 m 115.09 d 21.4 m 13.76 d 293.1 d 27.03 h 43.9 y 129.2 d B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ IT ECBþ ECBþ EC IT ECBþB2 IT IT B2ECBþ ITEC B2 ITB2 B2 B2 B2IT B2 B2 B2 B2IT B2 B2IT ECBþ ECBþ ECBþ EC ECBþ EC ITEC IT IT B2 ITB2 B2 0 305 324 1464 553 899 1710 195 576 546 114 100 505 181 93 82 22 20 51 2 22 0 37 354 120 21 1818 413 128 29 148 655 185 136 314 69 45 21 14 43 16 0 4 1 0 228 320 414 309 572 414 240 614 375 121 100 505 256 93 82 51 20 51 0 22 0 37 354 120 21 11 412 128 12 144 19 216 137 326 69 90 21 14 43 16 0 4 1 0 1883 1146 5371 3482 3757 5380 807 610 2351 117 102 511 1650 99 82 130 23 53 1283 25 0 39 327 121 372 6486 1208 517 2915 2703 5380 201 142 310 74 117 26 17 47 19 0 5 204 0 188 269 377 292 570 363 217 596 304 124 102 511 247 99 82 53 23 53 0 25 0 39 320 121 22 11 396 129 12 144 20 219 143 287 74 89 26 17 47 19 0 5 1 1319.5 1224.8 1221.7 965.3 771.4 803.8 805.7 509.5 412.7 558.8 252.9 79.3 22.6 659.1 424.7 173.2 915.0 1264.5 629.9 1145.6 2558.2 1280.6 1104.5 1445.1 1666.9 1302.4 883.6 1242.1 1266.5 1057.2 1067.7 942.2 377.7 139.1 128.0 93.8 390.0 5.4 1.7 1752.3 2.0 1025.3 257.9 1279.9 0.0 4.1 4.1 10.9 9.8 14.2 9.4 7.9 14.5 7.9 7.0 2.7 12.4 7.7 9.3 2.9 2.4 2.4 3.0 0.0 2.0 0.0 2.8 4.7 5.8 1.8 0.1 6.2 3.0 0.5 2.6 1.6 9.4 8.6 6.7 6.1 3.9 2.7 1.7 4.7 2.0 0.0 0.5 0.0 118 In In In 103 Cd 105 Cd 106 Cd 106 Cd 107 Cd 108 Cd 108 Cd 109 Cd 109 In 110 Cd 110 Cd 111m Cd 111 In 112 Cd 112 In 113 In 114 Sn 114 In 115 Sn 115 In 116 Sn 117m Sn 117 In 118 Sn 118 Sn 119m Sn 119 In 121 Sn 121 Sn 106m In 108m In 109 In 110m In 111 In 113m In 113 Sn 117 Sn 119 Sn 121 Sb 121 Sn 123 Sb 119m 119 119 119m In In 111 Cd 112 Sn 114 Cd Cd 114 115 Sn 117 Sn Sn 117 119 Sn Sn Sn 121 In 119 121m 109m In 111m 113 113 121 In In In Sb Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 17 48 48 48 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 49 50 50 50 50 50 50 50 50 50 50 50 50 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Cd Cd 119m Cd 103 In 105 In 106 In 106m In 107 In 108 In 108m In 109 In 109m In 110 In 110m In 111 In 111m In 112 In 112m In 113m In 114 In 114m In 115 In 115m In 116m In 117 In 117m In 118 In 118m In 119 In 119m In 121 In 121m In 106 Sn 108 Sn 109 Sn 110 Sn 111 Sn 113 Sn 113m Sn 117m Sn 119m Sn 121 Sn 121m Sn 123 Sn 119 Table 2. Continued 123m 18 50 50 50 50 50 50 50 50 50 50 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 51 A 123 125 125 126 127 127 128 129 130 130 111 113 114 115 116 116 117 118 118 119 120 120 122 122 124 124 124 125 126 126 127 128 128 129 130 130 131 133 Half-live 40.06 m 9.64 d 9.52 m 2.30E þ 5 y 2.10 h 4.13 m 59.07 m 2.23 m 3.72 m 1.7 m 75 s 6.67 m 3.49 m 32.1 m 15.8 m 60.3 m 2.80 h 3.6 m 5.00 h 38.19 h 15.89 m 5.76 d 2.7238 d 4.191 m 60.20 d 93 s 20.2 m 2.75856 y 12.35 d 19.15 m 3.85 d 9.01 h 10.4 m 4.40 h 39.5 m 6.3 m 23.03 m 2.5 m Decay Mode B2 B2 B2 B2 B2 B2 B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC ECBþ EC B2ECBþ IT B2 ITB2 IT B2 B2 B2IT B2 B2 B2IT B2 B2 B2 B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 28 52 62 20 348 120 136 452 168 696 735 145 901 112 278 469 48 81 424 24 28 396 75 32 270 73 0 85 449 256 115 501 319 222 537 489 312 385 28 50 60 20 282 94 136 157 168 145 254 220 410 162 342 495 52 140 425 24 86 396 74 32 269 73 0 85 449 255 115 501 310 222 520 424 302 379 79 2046 1502 21 1294 3431 142 4236 210 4708 4764 1984 4350 246 1399 465 53 2642 423 30 329 396 543 35 753 84 0 87 696 1145 126 883 2775 587 1953 3113 1073 1398 28 47 61 21 261 91 142 153 170 140 255 220 386 164 313 485 56 141 420 30 89 393 75 35 239 74 0 87 453 258 116 502 312 211 511 417 275 320 1565.3 1088.6 1193.7 606.6 1346.7 1035.7 1413.6 1021.7 1673.4 1014.4 919.2 708.9 750.4 444.5 581.2 282.9 225.5 728.6 191.7 3.0 501.2 421.9 1253.8 3.5 1212.7 354.0 0.0 601.2 1341.6 1052.7 1455.1 1420.9 1116.9 1320.4 1634.7 1322.1 1303.6 1247.1 2.8 0.8 3.4 2.1 5.2 2.9 8.3 3.4 7.7 4.3 9.8 8.2 8.5 6.7 6.9 12.7 5.3 5.2 12.7 3.0 4.0 11.8 2.3 3.5 4.6 2.2 0.0 4.2 11.6 7.3 3.5 12.7 8.3 3.9 13.4 8.5 4.8 4.6 Daughter nuclei with highest yield 123 Sb Sb Sb 126m Sb 127 Sb 127 Sb 128m Sb 129 Sb 130m Sb 130 Sb 111 Sn 113 Sn 114 Sn 115 Sn 116 Sn 116 Sn 117 Sn 118 Sn 118 Sn 119 Sn 120 Sn 120 Sn 122 Te 122 Sb 124 Te 124 Sb 124m Sb 125m Te 126 Te 126 Sb 127 Te 128 Te 128 Sb 129 Te 130 Te 130 Te 131 Te 133 Te 125 125 130m Sb 113m Sn T. OTTO Sn Sn 125m Sn 126 Sn 127 Sn 127m Sn 128 Sn 129 Sn 130 Sn 130m Sn 111 Sb 113 Sb 114 Sb 115 Sb 116 Sb 116m Sb 117 Sb 118 Sb 118m Sb 119 Sb 120 Sb 120m Sb 122 Sb 122m Sb 124 Sb 124m Sb 124 Sbn 125 Sb 126 Sb 126m Sb 127 Sb 128 Sb 128m Sb 129 Sb 130 Sb 130m Sb 131 Sb 133 Sb 125 Z 122 Sn 124 Te 125 Te 126 Te Te 127m 128 Te Te 129m 131m 133m Te Te Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 113 113 114 115 115 116 117 118 119 119 121 121 123 123 125 127 127 129 129 131 131 132 133 133 134 118 118 119 120 120 121 122 123 124 125 126 128 129 130 130 131 132 132 133 134 1.7 m 15.2 m 5.8 m 6.7 m 2.49 h 62 m 6.00 d 16.05 h 4.70 d 19.16 d 154 d 6.00E þ 14 y 119.25 d 57.40 d 9.35 h 109 d 69.6 m 33.6 d 25.0 m 30 h 3.204 d 12.5 m 55.4 m 41.8 m 13.7 m 8.5 m 19.1 m 81.6 m 53 m 2.12 h 3.63 m 13.27 h 4.1760 d 59.400 d 12.93 d 24.99 m 1.57E þ 7 y 12.36 h 8.84 m 8.02070 d 2.295 h 1.387 h 20.8 h 52.5 m ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC ECBþ ECBþ EC ITEC EC IT IT B2 ITB2 B2 ITB2 B2 B2IT B2 B2 B2IT B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC ECBþ EC ECBþB2 B2ECBþ B2 B2 ITB2 B2 B2 ITB2 B2 B2 1894 189 376 425 44 204 19 135 241 113 49 0 36 31 1 9 14 12 73 232 57 185 303 152 2730 753 97 1263 625 68 318 48 152 37 79 14 18 349 22 67 358 63 101 401 341 212 351 396 45 241 19 138 241 113 49 0 36 31 1 9 14 12 72 231 57 181 289 152 328 607 164 384 553 84 165 48 183 37 80 13 18 349 21 67 357 63 101 400 5772 254 2628 2330 49 449 22 137 235 117 51 0 38 35 1 11 216 189 1086 304 59 1425 576 154 6316 4119 1120 3978 3267 70 3795 51 439 42 88 1372 20 355 395 68 758 88 138 911 315 198 335 366 50 221 22 140 233 117 51 0 38 35 1 11 14 13 72 226 59 166 277 154 321 603 165 328 526 86 165 51 174 42 83 13 20 351 22 68 353 65 101 389 791.1 249.5 716.6 600.0 16.5 330.3 2.3 48.8 83.8 13.0 237.8 0.0 196.0 5.4 1442.0 35.3 1309.9 464.8 1307.1 1563.1 618.9 1236.8 1358.6 1621.4 790.6 800.6 713.4 641.3 707.2 405.5 737.4 196.4 279.5 4.3 693.7 1066.9 37.4 1440.6 176.3 1382.5 1350.0 244.7 1369.8 1320.2 7.9 7.0 8.5 8.3 4.4 5.8 2.3 5.1 7.6 5.3 4.4 0.0 3.8 3.5 0.0 1.1 0.8 0.9 3.5 5.7 5.4 4.8 6.5 6.6 9.4 16.2 8.1 8.6 14.2 6.1 5.8 5.0 5.6 4.3 3.4 0.6 2.0 9.1 1.0 3.4 7.4 2.6 3.0 7.2 113 Sb Sb Sb 115 Sb 116 Sb 117 Sb 118 Sb 119 Sb 119 Sb 121 Sb 121 Te 123 Sb 123 Te 125 Te 127 I 127 Te 129 I 129 Te 131 I 131 I 132 I 133 I 133 I 134 I 118 Te 118 Te 119 Te 120 Te 120 Te 121 Te 122 Te 123 Te 124 Te 125 Te 126 Te 128 Xe 129 Xe 130 Xe 130 I 131m Xe 132 Xe 132 I 133 Xe 134 Xe 114 115 121 Sb 127 I 129 I 131 Te 133 Te 119m Te 121m Te 123m Te 126 128 130 131 132 Xe Te Xe Xe Xe Xe 133m Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 19 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 52 53 53 53 53 53 53 53 53 53 53 53 53 53 53 53 53 53 53 53 53 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Te Te 115 Te 115m Te 116 Te 117 Te 118 Te 119 Te 119m Te 121 Te 121m Te 123 Te 123m Te 125m Te 127 Te 127m Te 129 Te 129m Te 131 Te 131m Te 132 Te 133 Te 133m Te 134 Te 118 I 118m I 119 I 120 I 120m I 121 I 122 I 123 I 124 I 125 I 126 I 128 I 129 I 130 I 130m I 131 I 132 I 132m I 133 I 134 I 114 Table 2. Continued 134m 20 53 53 54 54 54 54 54 54 54 54 54 54 54 54 54 54 54 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 55 A 134 135 120 121 122 123 125 127 127 129 131 133 133 135 135 137 138 121 121 123 124 125 126 127 128 129 130 130 131 132 134 134 135 135 136 137 138 138 Half-live 3.60 m 6.57 h 40 m 40.1 m 20.1 h 2.08 h 16.9 h 36.4 d 69.2 s 8.88 d 11.84 d 5.243 d 2.19 d 9.14 h 15.29 m 3.818 m 14.08 m 155 s 122 s 5.88 m 30.8 s 45 m 1.64 m 6.25 h 3.640 m 32.06 h 29.21 m 3.46 m 9.689 d 6.479 d 2.0648 y 2.903 h 2.3E þ 6 y 53 m 13.16 d 30.1671 y 33.41 m 2.91 m Decay Mode ITB2 B2 ECBþ ECBþ EC ECBþ ECBþ EC IT IT IT B2 IT B2 ITB2 B2 B2 ECBþ ECBþIT ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþB2 ITEC EC ECBþB2 B2EC IT B2 IT B2 B2 B2 ITB2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 66 225 93 192 27 83 67 67 40 33 14 18 17 45 75 1214 163 1717 1166 244 2629 81 785 84 147 68 36 29 17 129 251 10 0 255 333 0 518 132 66 225 94 226 27 117 68 67 40 33 14 18 17 45 75 31 155 201 205 191 195 134 197 89 155 68 93 29 17 130 251 10 0 255 333 0 328 70 125 277 98 1761 29 163 70 69 41 36 15 19 19 46 79 5979 1565 5935 4645 3053 6430 657 4635 86 2802 71 694 31 19 132 252 11 0 255 332 1 4329 974 69 201 99 198 29 114 71 69 41 36 15 19 19 45 75 30 123 201 205 191 193 133 195 91 155 71 93 31 19 133 252 11 0 255 330 0 276 66 551.2 1336.9 109.4 552.2 16.0 505.8 305.0 367.9 1542.5 2991.0 1852.8 858.0 2755.3 1661.8 267.6 918.1 1301.2 878.1 831.2 731.7 787.0 461.7 754.4 90.0 676.8 31.1 505.8 5.3 1.9 42.0 1051.8 338.7 710.3 49.5 1172.4 1370.7 1024.0 283.1 5.3 2.9 6.2 6.9 2.6 5.9 6.1 6.2 4.0 3.6 1.5 1.8 1.8 3.4 2.7 1.0 3.4 7.6 8.7 7.4 6.8 5.3 7.0 5.1 5.7 4.8 3.9 3.0 1.9 4.7 5.9 1.2 0.0 4.6 7.4 0.0 4.3 2.6 Daughter nuclei with highest yield 134 134 135 135m I Xe 120 I 121 I 122 I 123 I 125 I 127 I 127 Xe 129 Xe 131 Xe 133 Cs 133 Xe 135 Cs 135 Xe 137 Cs 138 Cs 121 Xe 121 Xe 123 Xe 124 Xe 125 Xe 126 Xe 127 Xe 128 Xe 129 Xe 130 Xe 130 Cs 131 Xe 132 Xe 134 Ba 134 Cs 135 Ba 135 Cs 136 Ba 137m Ba 138 Ba 138 Cs Xe Xe 135 Cs 121 Cs 130 Ba Xe 130 132 134 Ba Xe 137 Ba 138 Ba T. OTTO I I 120 Xe 121 Xe 122 Xe 123 Xe 125 Xe 127 Xe 127m Xe 129m Xe 131m Xe 133 Xe 133m Xe 135 Xe 135m Xe 137 Xe 138 Xe 121 Cs 121m Cs 123 Cs 124 Cs 125 Cs 126 Cs 127 Cs 128 Cs 129 Cs 130 Cs 130m Cs 131 Cs 132 Cs 134 Cs 134m Cs 135 Cs 135m Cs 136 Cs 137 Cs 138 Cs 138m Cs 135 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 139 139 140 124 126 127 128 129 129 131 131 133 133 135 137 139 140 141 142 128 129 130 131 132 132 133 134 135 136 137 138 140 141 142 143 130 131 132 133 133 134 135 137 137 139 9.27 m 63.7 s 11.0 m 100 m 12.7 m 2.43 d 2.23 h 2.16 h 11.50 d 14.6 m 10.52 y 38.9 h 28.7 h 2.552 m 83.06 m 12.752 d 18.27 m 10.6 m 5.18 m 11.6 m 8.7 m 59 m 4.8 h 24.3 m 3.912 h 6.45 m 19.5 h 9.87 m 6.0E þ 4 y 1.02E þ 11 y 1.6781 d 3.92 h 91.1 m 14.2 m 22.9 m 10.2 m 3.51 h 97 m 4.9 h 3.16 d 17.7 h 9.0 h 34.4 h 137.641 d B2 B2 ECBþ ECBþ ECBþ EC ECBþ ECBþ EC IT EC ITEC IT IT B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ITECBþ ECBþ ECBþ ECBþ ECBþ EC ECB2 B2 B2 B2 B2 ECBþ ECBþ EC ECBþ ECBþ EC ECBþ ECBþ ITEC EC 1296 2877 77 106 67 25 38 260 99 22 92 21 19 98 11 34 182 166 1167 108 852 92 411 110 28 83 19 29 16 184 329 10 670 370 91 247 61 64 276 16 150 18 18 41 40 233 107 107 129 25 66 262 99 22 92 21 19 98 9 34 148 166 457 164 359 126 308 120 39 126 19 77 16 184 329 4 300 36 98 269 61 113 283 16 150 18 18 41 5710 5862 197 107 1536 26 73 254 101 22 95 23 20 100 2013 37 2514 290 4777 1667 3888 239 1966 150 29 2351 20 441 17 171 552 2622 2123 4415 92 1863 62 593 302 17 151 20 18 42 31 178 108 107 127 26 65 255 101 22 95 23 20 100 9 35 142 163 446 164 345 126 278 120 40 126 20 78 17 167 284 3 211 31 99 260 62 113 265 17 152 20 18 42 926.5 939.5 390.0 120.3 620.2 26.2 305.1 314.0 136.5 2.3 75.2 2227.1 2295.2 121.6 1176.7 1396.4 1433.5 1528.7 872.3 640.0 718.4 365.9 457.6 236.7 120.5 621.9 2.4 410.6 1.7 277.5 1349.2 1062.7 1180.8 999.2 251.3 644.7 130.1 424.3 126.7 3.5 179.3 2.6 2571.7 261.8 0.4 3.0 5.1 5.0 5.3 2.4 3.5 8.9 6.1 2.1 6.9 2.1 1.8 2.6 0.8 1.8 5.8 4.5 13.9 7.2 10.8 6.5 8.3 5.3 2.7 4.6 1.8 3.4 1.7 2.9 4.9 0.0 3.1 0.5 5.6 9.1 5.5 6.3 8.6 1.7 7.1 1.9 1.6 4.1 139 Ba Ba Cs 126 Cs 127 Cs 128 Cs 129 Cs 129 Cs 131 Cs 131 Ba 133 Cs 133 Ba 135 Ba 137 Ba 139 La 140 La 141 La 142 La 128 Ba 129 Ba 130 Ba 131 Ba 132 Ba 132 La 133 Ba 134 Ba 135 Ba 136 Ba 137 Ba 138 Ba 140 Ce 141 Ce 142 Ce 143 Ce 130 La 131 La 132 La 133 La 133 La 134 La 135 La 137 La 137 Ce 139 La 140 124 133 Cs 129m Ba 132 Ba 138 Ce 137 La Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 21 55 55 56 56 56 56 56 56 56 56 56 56 56 56 56 56 56 56 57 57 57 57 57 57 57 57 57 57 57 57 57 57 57 57 58 58 58 58 58 58 58 58 58 58 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Cs Cs 124 Ba 126 Ba 127 Ba 128 Ba 129 Ba 129m Ba 131 Ba 131m Ba 133 Ba 133m Ba 135m Ba 137m Ba 139 Ba 140 Ba 141 Ba 142 Ba 128 La 129 La 130 La 131 La 132 La 132m La 133 La 134 La 135 La 136 La 137 La 138 La 140 La 141 La 142 La 143 La 130 Ce 131 Ce 132 Ce 133 Ce 133m Ce 134 Ce 135 Ce 137 Ce 137m Ce 139 Ce 140 Table 2. Continued 141 22 58 58 58 58 59 59 59 59 59 59 59 59 59 59 59 59 59 59 59 59 59 59 59 60 60 60 60 60 60 60 60 60 60 60 60 60 60 60 A 141 143 144 145 134 134 135 136 137 138 138 139 140 142 142 143 144 144 145 146 147 148 148 134 135 136 137 138 139 139 140 141 141 144 147 149 151 152 Half-live 32.508 d 33.039 h 284.91 d 3.01 m 11 m 17 m 24 m 13.1 m 1.28 h 1.45 m 2.12 h 4.41 h 3.39 m 19.12 h 14.6 m 13.57 d 17.28 m 7.2 m 5.984 h 24.15 m 13.4 m 2.29 m 2.01 m 8.5 m 12.4 m 50.65 m 38.5 m 5.04 h 29.7 m 5.50 h 3.37 d 2.49 h 62.0 s 2.29E þ 15 y 10.98 d 1.728 h 12.44 m 11.4 m Decay Mode B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ B2EC IT B2 B2 ITB2 B2 B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ EC ECBþ ECBþIT EC ECBþ ITECBþ A B2 B2 B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 16 57 5 145 794 1722 106 381 34 486 369 19 39 10 0 0 108 6 4 964 95 1515 1254 74 433 57 162 18 47 259 15 19 113 0 30 69 137 31 16 57 5 144 513 361 157 338 70 141 402 32 98 8 0 0 4 6 3 147 91 148 156 104 225 64 200 18 81 261 15 23 113 0 30 68 136 31 16 114 5 815 3938 5186 1547 2618 230 4104 521 19 1454 1754 0 1 3933 7 797 4161 1862 5597 5991 208 3393 58 758 19 309 260 16 19 118 0 30 187 929 36 16 58 5 145 503 332 155 316 69 141 400 32 99 6 0 0 3 6 3 130 89 134 155 104 223 64 192 19 81 256 16 23 113 0 30 69 133 33 1278.0 1460.8 600.9 1280.6 903.5 762.6 618.6 577.8 307.8 689.2 651.6 125.9 528.1 1137.5 0.0 1454.3 1001.4 1.1 1208.4 1032.4 1186.1 1018.4 1056.4 331.4 1007.9 91.5 389.4 12.4 307.6 404.0 1.6 47.3 94.9 0.0 1357.9 1682.1 1344.4 1469.8 1.6 3.6 0.5 5.1 16.3 10.1 6.9 9.3 3.0 5.0 10.8 2.0 3.9 0.1 0.0 0.0 0.0 0.6 0.1 2.7 4.3 3.8 6.2 6.3 10.1 4.2 6.8 1.8 3.3 7.2 1.6 1.8 2.3 0.0 1.9 4.4 4.5 2.5 Daughter nuclei with highest yield 141 Pr Pr Pr 145 Pr 134 Ce 134 Ce 135 Ce 136 Ce 137 Ce 138 Ce 138 Ce 139 Ce 140 Ce 142 Nd 142 Pr 143 Nd 144 Nd 144 Pr 145 Nd 146 Nd 147 Nd 148 Nd 148 Nd 134m Pr 135 Pr 136 Pr 137 Pr 138 Pr 139 Pr 139 Pr 140 Pr 141 Pr 141 Nd 140 Ce 147 Pm 149 Pm 151 Pm 152 Pm 143 144 144m Pr 142 Ce 144 Nd 139 Nd 141 Pr T. OTTO Ce Ce 144 Ce 145 Ce 134 Pr 134m Pr 135 Pr 136 Pr 137 Pr 138 Pr 138m Pr 139 Pr 140 Pr 142 Pr 142m Pr 143 Pr 144 Pr 144m Pr 145 Pr 146 Pr 147 Pr 148 Pr 148m Pr 134 Nd 135 Nd 136 Nd 137 Nd 138 Nd 139 Nd 139m Nd 140 Nd 141 Nd 141m Nd 144 Nd 147 Nd 149 Nd 151 Nd 152 Nd 143 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 136 136 137 139 140 140 141 142 143 144 145 146 147 148 148 149 150 151 152 152 153 154 154 139 140 141 141 142 143 143 145 146 147 148 151 153 155 156 157 142 142 143 144 145 146 107 s 2.4 m 4.15 m 9.2 s 5.95 m 20.90 m 40.5 s 265 d 363 d 17.7 y 5.53 y 2.6234 y 5.368 d 41.29 d 53.08 h 2.68 h 28.40 h 4.12 m 7.52 m 5.25 m 1.73 m 2.68 m 2.57 m 14.82 m 10.2 m 22.6 m 72.49 m 8.75 m 66 s 340 d 1.03E þ 8 y 1.060E11 y 7E þ 15 y 90 y 46.50 h 22.3 m 9.4 h 8.03 m 2.34 s 1.223 m 2.59 m 10.2 s 5.93 d 4.61 d ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC EC ECA ECB2 B2 B2 B2IT B2 B2 B2 B2 B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþIT ECBþ ECBþ ITECBþ EC A A A B2 B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ 3481 753 449 2950 646 86 850 61 267 15 132 0 88 327 2 279 60 422 293 19 334 337 625 72 285 299 16 44 111 29 0 0 0 0 19 21 23 76 5210 2508 1273 3183 194 370 451 308 160 178 489 124 146 61 267 15 132 0 85 327 2 220 60 45 238 18 247 271 243 100 230 315 28 94 111 29 0 0 0 0 19 21 23 71 197 551 182 180 198 377 6821 3573 3651 6419 3692 1857 4616 62 270 16 132 0 1585 329 6 1878 63 4419 1946 769 1845 2117 3810 248 2397 1121 17 1350 118 29 0 0 0 0 18 293 23 2055 7286 6076 4656 6351 189 369 453 306 158 177 487 121 144 62 270 16 132 0 79 329 2 204 60 42 227 18 201 245 238 97 220 303 28 94 112 29 0 0 0 0 18 21 23 70 192 548 173 174 181 359 835.4 1415.4 643.7 741.8 731.0 508.6 686.2 4.3 31.0 1.5 488.1 255.5 1205.9 1227.3 1428.4 1237.1 1442.3 1018.3 1497.5 1228.5 1180.5 1392.7 802.1 310.7 555.0 937.1 108.5 464.1 110.4 2.8 0.0 0.0 0.0 0.0 1433.8 1305.7 1349.8 1231.8 754.3 736.3 655.7 726.0 41.1 85.8 14.0 12.9 5.7 5.9 12.5 4.2 5.0 2.4 8.3 1.5 4.5 0.0 1.4 9.3 0.1 4.8 3.5 1.2 7.7 1.6 3.3 6.7 9.0 4.0 7.3 9.9 1.8 3.6 2.3 2.8 0.0 0.0 0.0 0.0 1.7 1.9 2.2 4.1 6.1 13.4 5.4 5.6 4.2 8.3 136 Nd Nd Nd 140 Nd 140 Nd 141 Nd 142 Nd 143 Nd 144 Nd 145 Nd 146 Sm 147 Sm 148 Sm 148 Sm 149 Sm 150 Sm 151 Sm 152 Sm 152 Sm 153 Sm 154 Sm 154 Sm 139 Pm 140 Pm 141 Pm 141 Pm 142 Pm 143 Pm 143 Sm 145 Pm 142 Nd 143 Nd 144 Nd 151 Eu 153 Eu 155 Eu 156 Eu 157 Eu 142 Sm 142 Sm 143 Sm 144 Sm 145 Sm 146 Sm 137 139 141m 141 146 Nd Pr Nd 148 Pm 141 Sm 143 Pm 143m Sm Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 23 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 61 62 62 62 62 62 62 62 62 62 62 62 62 62 62 62 62 63 63 63 63 63 63 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Pm Pm 139 Pm 140 Pm 140m Pm 141 Pm 142 Pm 143 Pm 144 Pm 145 Pm 146 Pm 147 Pm 148 Pm 148m Pm 149 Pm 150 Pm 151 Pm 152 Pm 152m Pm 153 Pm 154 Pm 154m Pm 139 Sm 140 Sm 141 Sm 141m Sm 142 Sm 143 Sm 143m Sm 145 Sm 146 Sm 147 Sm 148 Sm 151 Sm 153 Sm 155 Sm 156 Sm 157 Sm 142 Eu 142m Eu 143 Eu 144 Eu 145 Eu 146 Eu 137m Table 2. Continued 147 24 63 63 63 63 63 63 63 63 63 63 63 63 63 63 63 64 64 64 64 64 64 64 64 64 64 64 64 64 64 64 65 65 65 65 65 65 65 65 A 147 148 149 150 150 152 152 152 154 154 155 156 157 158 159 142 143 144 145 145 146 147 148 149 150 151 152 153 159 162 146 147 147 148 148 149 149 150 Half-live 24.1 d 54.5 d 93.1 d 36.9 y 12.8 h 13.537 y 9.3116 h 96 m 8.593 y 46.0 m 4.7611 y 15.19 d 15.18 h 45.9 m 18.1 m 70.2 s 110.0 s 4.47 m 23.0 m 85 s 48.27 d 38.1 h 74.6 y 9.28 d 1.79E þ 6 y 124 d 1.08E þ 14 y 240.4 d 18.479 h 8.4 m 23 s 1.64 h 1.87 m 60 m 2.20 m 4.118 h 4.16 m 3.48 h Decay Mode ECBþA ECBþA EC ECBþ B2ECBþ ECBþB2 B2ECBþ IT B2EC IT B2 B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ITECBþ EC ECBþ A ECBþ A ECA A EC B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþA ECBþA ECBþA Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 87 365 21 267 8 189 50 17 193 20 14 176 58 235 62 289 1122 133 299 175 65 236 0 101 0 22 0 32 11 73 2005 300 239 744 481 203 198 388 88 365 21 267 9 189 49 17 193 20 14 174 58 194 60 172 345 143 328 113 65 236 0 101 0 22 0 32 11 73 518 334 277 357 514 213 229 341 87 362 21 267 10 202 689 17 277 19 14 952 89 2087 1897 2502 4253 1907 1058 391 65 235 0 102 0 22 0 32 13 75 5103 829 917 2991 1083 243 484 1088 88 360 21 266 9 182 49 17 187 19 14 150 58 184 60 166 331 127 255 114 65 234 0 102 0 22 0 32 11 73 452 316 241 324 512 197 228 282 186.9 57.4 21.1 129.6 1293.4 438.4 872.7 1.7 1152.3 1.9 93.6 1038.9 1428.6 1165.0 1151.2 562.5 943.0 465.6 346.4 196.0 109.8 541.6 0.0 311.0 0.0 120.2 0.0 3.3 1443.9 1470.3 648.2 324.2 337.8 512.4 397.5 273.4 304.6 240.5 4.3 10.5 1.9 10.4 0.4 5.3 1.4 1.7 4.2 1.9 1.3 2.4 3.2 3.3 3.2 5.7 11.3 4.3 5.0 2.9 6.3 8.8 0.0 6.0 0.0 2.1 0.0 3.1 0.8 3.3 8.6 7.5 4.7 7.8 13.8 6.4 6.1 6.7 Daughter nuclei with highest yield 147 143 148 144 Sm Sm 149 Sm 150 Sm 150 Gd 152 Gd 152 Gd 152 Eu 154 Gd 154 Eu 155 Gd 156 Gd 157 Gd 158 Gd 159 Gd 142 Eu 143 Eu 144 Eu 145 Eu 145 Gd 146 Eu 147 Eu 144 Sm 149 Eu 146 Sm 147 Sm 148 Sm 153 Eu 159 Tb 162 Tb 146 Gd 147 Gd 147 Gd 148 Gd 148 Gd 149 Gd 149 Gd 150 Gd 150 152 152 Pm Pm Sm Sm Sm 154 Sm 145 Eu 151 Eu T. OTTO Eu Eu 149 Eu 150 Eu 150m Eu 152 Eu 152m Eu 152 Eun 154 Eu 154m Eu 155 Eu 156 Eu 157 Eu 158 Eu 159 Eu 142 Gd 143m Gd 144 Gd 145 Gd 145m Gd 146 Gd 147 Gd 148 Gd 149 Gd 150 Gd 151 Gd 152 Gd 153 Gd 159 Gd 162 Gd 146 Tb 147 Tb 147m Tb 148 Tb 148m Tb 149 Tb 149m Tb 150 Tb 148 Z 145 Eu Eu 146 Eu 145 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 150m 150 151 151 152 152 153 154 155 156 156 156 157 158 160 161 162 163 164 165 148 149 150 151 152 153 154 155 157 159 165 165 166 167 168 150 153 153 154 154 155 156 157 159 160 5.8 m 17.609 h 25 s 17.5 h 4.2 m 2.34 d 21.5 h 5.32 d 5.35 d 24.4 h 5.3 h 71 y 180 y 72.3 d 6.906 d 7.60 m 19.5 m 3.0 m 2.11 m 3.3 m 4.20 m 7.17 m 17.9 m 2.38 h 6.4 h 3.0E þ 6 y 9.9 h 8.14 h 144.4 d 2.334 h 1.257 m 81.6 h 6.20 m 8.7 m 76.8 s 2.01 m 9.3 m 11.76 m 3.10 m 48 m 56 m 12.6 m 33.05 m 25.6 m ECBþ ECBþA ITECBþ ECBþ ITECBþ ECBþ ECBþ EC EC IT IT EC ECB2 B2 B2 B2 B2 B2 B2 ECBþ ECBþ ECBþA ECBþA ECA ECBþA A ECBþ EC EC B2 ITB2 B2 B2 B2 ECBþ ECBþA ECBþA ECBþA ECBþA ECBþ ECBþ ECBþ ECBþ ECBþ 405 175 16 221 137 67 310 44 308 12 1 2 134 175 15 181 137 411 145 118 239 53 214 58 152 0 113 69 17 5 4 12 93 71 3256 159 191 884 392 82 449 102 80 276 425 177 16 229 139 67 313 44 308 12 1 2 134 175 15 181 137 376 121 125 250 53 218 58 154 0 115 69 17 5 4 12 92 71 312 176 185 308 413 108 328 111 80 277 470 175 16 792 140 67 305 43 298 12 1 2 134 178 16 298 153 1686 2197 119 322 53 218 58 148 0 111 69 17 55 4 12 850 100 6108 1659 2139 3837 1799 351 2128 108 80 277 428 175 17 204 139 67 243 43 294 12 1 2 133 173 16 181 137 354 110 125 228 53 208 58 149 0 112 69 17 5 4 12 93 71 312 175 185 301 412 103 303 110 80 277 269.2 367.0 10.3 323.7 1614.4 93.0 80.2 113.5 311.6 1.2 0.1 0.2 310.8 1418.1 1270.2 1430.8 1535.2 1458.2 1149.2 67.4 156.7 13.7 141.1 77.2 183.6 0.0 121.3 35.4 1.6 1352.8 37.7 1052.1 1966.4 1808.7 687.3 643.8 672.6 729.5 675.9 333.1 875.3 311.9 177.8 138.9 13.8 8.3 0.9 6.7 7.7 4.5 5.2 4.0 9.0 1.2 0.1 0.2 3.9 4.1 1.6 6.1 6.1 9.5 1.8 4.4 5.9 2.9 5.9 4.7 6.9 0.0 5.4 4.7 1.6 0.3 0.3 1.1 4.4 3.7 8.5 7.1 8.0 10.2 15.5 5.0 10.2 6.4 6.1 7.3 150 Gd Gd Tb 152 Gd 152 Tb 153 Gd 154 Gd 155 Gd 156 Gd 156 Tb 156 Tb 157 Gd 158 Gd 160 Dy 161 Dy 162 Dy 163 Dy 164 Dy 165m Dy 148 Tb 149 Tb 150 Tb 151 Tb 152 Tb 153 Tb 150 Gd 155 Tb 157 Tb 159 Tb 165 Ho 165 Dy 166 Ho 167 Ho 168 Ho 150 Dy 153 Dy 153 Dy 154 Dy 154 Dy 155 Dy 156 Dy 157 Dy 159 Dy 160 Dy 151 147 151 151 Eu Gd 152 Gd 158 Dy 165 Dy 149m Tb Gd Tb 148 Gd 149 Gd 146 151m 165 147 Gd Ho 149m Tb Tb 150 Tb 150m Tb 149 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 25 65 65 65 65 65 65 65 65 65 65 65 65 65 65 65 65 65 65 65 66 66 66 66 66 66 66 66 66 66 66 66 66 66 66 67 67 67 67 67 67 67 67 67 67 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Tb Tb 151m Tb 152 Tb 152m Tb 153 Tb 154 Tb 155 Tb 156 Tb 156m Tb 156 Tbn 157 Tb 158 Tb 160 Tb 161 Tb 162 Tb 163 Tb 164 Tb 165 Tb 148 Dy 149 Dy 150 Dy 151 Dy 152 Dy 153 Dy 154 Dy 155 Dy 157 Dy 159 Dy 165 Dy 165m Dy 166 Dy 167 Dy 168 Dy 150 Ho 153 Ho 153m Ho 154 Ho 154m Ho 155 Ho 156 Ho 157 Ho 159 Ho 160 Ho 151 Table 2. Continued 161 26 67 67 67 67 67 67 67 67 67 67 67 67 68 68 68 68 68 68 68 68 68 68 68 69 69 69 69 69 69 69 69 69 69 69 69 69 69 69 A 161 162 162 163 164 164 166 166 167 168 168 170 154 156 159 161 163 165 167 169 171 172 173 161 162 163 164 165 166 167 168 170 171 172 173 174 175 176 Half-live 2.48 h 15.0 m 67.0 m 4570 y 29 m 38.0 m 26.80 h 1.20E þ 3 y 3.1 h 2.99 m 132 s 2.76 m 3.73 m 19.5 m 36 m 3.21 h 75.0 m 10.36 h 2.269 s 9.40 d 7.516 h 49.3 h 1.434 m 30.2 m 21.70 m 1.810 h 2.0 m 30.06 h 7.70 h 9.25 d 93.1 d 128.6 d 1.92 y 63.6 h 8.24 h 5.4 m 15.2 m 1.85 m Decay Mode EC ECBþ ITECBþ EC ECB2 IT B2 B2 B2 B2 IT B2 ECBþA EC ECBþ ECBþ ECBþ EC IT B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC ECBþB2 B2EC B2 B2 B2 B2 B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 24 28 95 0 10 16 7 269 66 142 2 281 21 22 149 163 13 13 19 0 69 92 141 191 448 207 159 104 289 33 211 1 0 69 68 291 175 439 24 34 96 0 10 16 5 269 66 140 2 271 26 22 157 163 13 13 19 0 69 92 140 210 276 208 126 104 291 33 211 1 0 68 68 291 175 285 25 27 94 0 10 15 849 272 67 1503 2 1462 22 23 152 161 13 12 18 0 80 92 910 426 1849 195 1957 103 279 33 211 2 0 646 71 309 412 2424 25 33 93 0 10 15 5 270 66 138 2 269 27 23 150 160 13 12 18 0 69 92 140 186 235 193 119 103 255 33 210 1 0 61 69 291 173 250 5.2 62.3 206.5 0.0 580.4 1.5 1200.8 663.2 1485.3 1206.0 0.2 1420.4 45.9 14.0 495.7 481.1 1.4 1.2 1739.0 843.5 1488.3 844.2 1396.5 304.6 383.4 196.3 413.1 394.4 148.5 1740.4 208.0 1443.9 0.0 1130.9 1511.8 2092.9 1660.8 1703.1 2.5 1.9 3.9 0.0 0.9 1.5 0.3 9.2 4.0 3.1 0.2 7.4 2.4 2.1 5.0 4.5 1.3 1.2 1.7 0.0 4.8 4.0 6.4 7.8 5.8 6.2 4.0 5.7 6.0 3.0 7.7 0.1 0.0 1.0 3.2 11.7 4.7 7.3 Daughter nuclei with highest yield 161 Dy Dy Ho 163 Dy 164 Dy 164 Ho 166 Er 166 Er 167 Er 168 Er 168 Ho 170 Er 154 Ho 156 Ho 159 Ho 161 Ho 163 Ho 165 Ho 167 Er 169 Tm 171 Tm 172 Tm 173 Tm 161 Er 162 Er 163 Er 164 Er 165 Er 166 Er 167 Er 168 Er 170 Yb 171 Yb 172 Yb 173 Yb 174 Yb 175 Yb 176 Yb 162 162 162 Dy 164 Er 150 Dy 168 Yb Er T. OTTO Ho Ho 162m Ho 163 Ho 164 Ho 164m Ho 166 Ho 166m Ho 167 Ho 168 Ho 168m Ho 170 Ho 154 Er 156 Er 159 Er 161 Er 163 Er 165 Er 167m Er 169 Er 171 Er 172 Er 173 Er 161 Tm 162 Tm 163 Tm 164 Tm 165 Tm 166 Tm 167 Tm 168 Tm 170 Tm 171 Tm 172 Tm 173 Tm 174 Tm 175 Tm 176 Tm 162 Z 170 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 162 162 163 164 165 166 167 169 175 177 178 179 165 167 169 169 170 171 171 172 172 173 174 174 176 176 177 177 178 178 179 180 181 167 169 170 172 173 174 175 177 178 179 180 181 18.87 m 11.05 m 75.8 m 9.9 m 56.7 h 17.5 m 32.026 d 4.185 d 1.911 h 74 m 8.0 m 10.74 m 51.5 m 34.06 h 160 s 2.012 d 8.24 d 79 s 6.70 d 3.7 m 1.37 y 3.31 y 142 d 3.85E þ 10 y 3.635 h 6.647 d 160.4 d 28.4 m 23.1 m 4.59 h 5.7 m 3.5 m 2.05 m 3.24 m 16.01 h 1.87 y 23.6 h 2.0E þ 15 y 70 d 51.4 m 31 y 25.05 d 5.5 h 42.39 d ECBþ ECBþ EC ECBþ EC ECBþ EC B2 B2 B2 B2 ECBþ ECBþ ECBþ IT ECBþ ECBþ IT ECBþ IT EC ECBþ ITEC B2 B2EC B2 B2IT B2 B2 B2 B2 B2 ECBþ ECBþ EC EC ECBþ A EC IT IT IT ITB2 B2 50 92 15 54 25 60 75 7 31 7 163 161 245 202 0 341 117 0 306 0 42 24 16 87 3 7 184 20 189 5 231 100 105 97 82 31 76 0 67 412 392 168 178 94 50 119 15 65 25 61 75 7 31 7 163 182 253 203 0 341 117 0 306 0 42 24 16 87 3 7 184 19 189 5 229 98 110 115 82 31 76 0 67 412 392 168 178 94 49 706 15 75 24 59 74 7 116 7 860 968 297 192 1 280 120 1 302 0 42 23 17 88 49 7 186 1274 194 127 644 1362 1589 260 83 34 77 0 68 416 395 169 179 94 50 114 15 63 24 60 74 7 31 7 164 171 219 188 1 263 120 1 298 0 42 23 17 88 4 7 186 17 190 5 219 99 110 115 83 34 77 0 68 416 395 169 179 94 31.1 270.0 4.1 112.5 2.4 43.0 517.6 1072.9 1224.8 1325.7 1548.3 490.1 291.4 84.7 0.2 36.3 12.2 0.3 219.2 0.1 31.5 2.0 20.2 2057.7 1363.2 1098.7 1066.9 1178.2 2210.8 1350.0 1508.3 1519.2 404.8 173.6 78.5 17.2 113.9 0.0 234.7 4528.0 1472.5 960.9 706.0 1393.0 3.8 3.9 1.3 3.6 2.4 5.5 6.9 0.4 1.2 0.4 5.5 6.9 6.6 5.2 0.2 4.6 4.8 0.3 7.5 0.1 3.7 1.5 2.0 6.9 0.4 0.6 14.1 0.5 12.2 0.5 5.6 4.4 5.5 5.2 5.3 3.9 6.3 0.0 4.7 29.2 21.3 11.1 10.9 4.8 162 Tm Tm Tm 165 Tm 166 Tm 167 Tm 169 Tm 175 Lu 177 Lu 178 Lu 179 Lu 165 Yb 167 Yb 169 Yb 169 Lu 170 Yb 171 Yb 171 Lu 172 Yb 172 Lu 173 Yb 174 Yb 174 Lu 176 Hf 176 Hf 177 Hf 177 Lu 178 Hf 178 Hf 179 Hf 180 Hf 181 Hf 167 Lu 169 Lu 170 Lu 172m Lu 173 Lu 170 Yb 175 Lu 177 Hf 178 Hf 179 Hf 180 Hf 181 Ta 163 164 174 Yb 176 Yb 177 Hf 169m Lu 180m Ta Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 27 70 70 70 70 70 70 70 70 70 70 70 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 71 72 72 72 72 72 72 72 72 72 72 72 72 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Yb Yb 164 Yb 165 Yb 166 Yb 167 Yb 169 Yb 175 Yb 177 Yb 178 Yb 179 Yb 165 Lu 167 Lu 169 Lu 169m Lu 170 Lu 171 Lu 171m Lu 172 Lu 172m Lu 173 Lu 174 Lu 174m Lu 176 Lu 176m Lu 177 Lu 177m Lu 178 Lu 178m Lu 179 Lu 180 Lu 181 Lu 167 Hf 169 Hf 170 Hf 172 Hf 173 Hf 174 Hf 175 Hf 177m Hf 178m Hf 179m Hf 180m Hf 181 Hf 163 Table 2. Continued 182 28 72 72 72 72 73 73 73 73 73 73 73 73 73 73 73 73 73 73 73 73 73 74 74 74 74 74 74 74 74 74 74 75 75 75 75 75 75 75 A 182 182 183 184 170 172 173 174 175 176 177 178 178 179 180 182 182 183 184 185 186 177 178 179 179 181 185 185 187 188 190 178 179 180 181 182 182 183 Half-live 9E þ 6 y 61.5 m 1.067 h 4.12 h 6.76 m 36.8 m 3.14 h 1.14 h 10.5 h 8.09 h 56.56 h 9.31 m 2.36 h 1.82 y 8.152 h 114.43 d 15.84 m 5.1 d 8.7 h 49.4 m 10.5 m 132 m 21.6 d 37.05 m 6.40 m 121.2 d 75.1 d 1.597 m 23.72 h 69.78 d 30.0 m 13.2 m 19.5 m 2.44 m 19.9 h 64.0 h 12.7 h 70.0 d Decay Mode B2 B2IT B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC ECBþ EC EC ECB2 B2 IT B2 B2 B2 B2 ECBþ EC EC ITEC EC B2 IT B2 B2 B2 ECBþ ECBþ ECBþ ECBþ EC ECBþ EC Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 43 159 129 45 2016 311 84 150 173 313 16 22 212 7 12 196 52 58 261 30 361 158 4 17 12 10 0 5 76 0 32 388 174 180 139 289 186 34 43 159 129 45 180 266 98 156 174 312 16 24 212 7 12 196 52 58 261 29 238 158 4 17 12 10 0 5 76 0 32 242 176 193 139 289 188 34 44 161 216 51 5002 1634 205 1256 163 298 17 25 213 7 13 197 53 59 278 696 2848 160 5 18 13 11 0 7 99 0 41 1947 166 335 140 289 198 36 44 160 128 47 180 255 94 147 160 263 17 24 213 7 13 190 53 59 262 30 238 158 5 18 13 11 0 7 78 0 39 203 166 192 139 281 180 36 335.3 1318.9 1404.7 1755.0 701.7 675.3 301.6 690.3 213.9 90.0 4.8 23.6 837.8 0.9 199.7 1080.5 2551.2 2019.2 1871.6 1589.4 1318.1 188.7 0.6 2.3 2561.5 1.3 1110.7 533.4 1426.9 842.6 2340.3 588.8 204.3 134.6 680.6 803.7 57.2 236.4 3.4 8.1 3.8 4.3 6.7 8.1 4.7 6.5 6.1 5.4 1.7 1.8 14.2 0.9 1.4 4.8 5.5 5.3 10.4 2.9 9.9 7.9 0.6 2.0 1.3 1.2 0.0 1.1 3.3 0.0 6.0 7.1 7.2 5.3 6.6 12.3 5.3 3.8 Daughter nuclei with highest yield 182 Ta Ta Ta 184 Ta 170 Hf 172 Hf 173 Hf 174 Hf 175 Hf 176 Hf 177 Hf 178 Hf 178 Hf 179 Hf 180 Hf 182 W 182 Ta 183 W 184 W 185 W 186 W 177 Ta 178 Ta 179 Ta 179 W 181 Ta 185 Re 185 W 187 Re 188 Re 190 Re 178 W 179 W 180 W 181 W 182 W 182 W 183 W 182 182 Hf 180 W 179 Ta 183 179m W 182m Ta T. OTTO Hf Hf 183 Hf 184 Hf 170 Ta 172 Ta 173 Ta 174 Ta 175 Ta 176 Ta 177 Ta 178 Ta 178m Ta 179 Ta 180 Ta 182 Ta 182m Ta 183 Ta 184 Ta 185 Ta 186 Ta 177 W 178 W 179 W 179m W 181 W 185 W 185m W 187 W 188 W 190 W 178 Re 179 Re 180 Re 181 Re 182 Re 182m Re 183 Re 182m Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 184 184 184 186 186 187 188 188 189 190 190 180 181 182 183 183 185 186 189 190 191 191 193 194 196 180 182 183 184 185 186 186 187 188 189 190 190 190 191 192 192 192 193 194 194 38.0 d 169 d 3.7183 d 2.00E þ 5 y 4.12E þ 10 y 17.0040 h 18.59 m 24.3 h 3.1 m 3.2 h 21.5 m 105 m 22.10 h 13.0 h 9.9 h 93.6 d 2.0E þ 15 y 5.8 h 9.9 m 15.4 d 13.10 h 30.11 h 6.0 y 34.9 m 1.5 m 15 m 58 m 3.09 h 14.4 h 16.64 h 1.92 h 10.5 h 41.5 h 13.2 d 11.78 d 1.120 h 3.087 h 4.94 s 73.827 d 1.45 m 241 y 10.53 d 19.28 h 171 d ECBþ ITEC B2EC IT B2 B2 IT B2 B2 B2IT ECBþ ECBþ EC ECBþ ECBþIT EC A IT IT B2 IT B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþIT ECBþ ECBþ EC EC IT ECIT IT B2EC ITB2 IT IT B2 B2 146 67 4 5 0 12 16 10 224 159 29 215 79 114 155 116 0 0 271 18 2 13 2 15 1360 959 172 314 127 254 183 59 288 18 253 0 14 17 142 1 2 0 17 395 146 67 4 5 0 10 16 10 223 157 29 218 79 114 155 116 0 0 271 18 2 13 2 15 268 235 183 309 131 262 191 59 288 18 253 0 14 17 142 1 2 0 15 395 147 73 8 18 0 1332 25 13 862 621 40 221 87 124 161 123 0 3 280 30 5 22 6 25 4015 3435 304 886 129 331 311 70 246 28 263 3 21 29 145 9 19 3 1625 402 147 73 5 18 0 11 25 12 224 162 40 216 87 124 157 123 0 3 280 30 5 15 6 16 275 240 176 302 129 253 181 70 232 28 262 3 21 29 145 9 19 3 15 402 25.9 173.8 1400.4 5.3 0.0 1340.9 12.5 1555.2 1736.0 996.9 51.8 261.9 116.0 121.7 355.5 29.5 0.0 0.8 689.5 81.4 1.4 1471.5 1.5 1448.4 957.3 779.8 384.0 573.9 303.5 632.2 305.4 78.2 379.4 56.7 579.5 0.7 158.0 68.7 1637.6 2.6 2333.8 0.9 1172.8 482.3 4.3 5.7 0.7 5.3 0.0 0.9 4.8 1.3 9.3 8.3 6.0 10.6 7.7 10.4 5.4 5.7 0.0 0.8 14.0 5.4 1.4 1.6 1.5 1.3 12.2 11.7 9.5 13.6 9.7 12.4 7.0 6.4 7.8 5.1 13.7 0.7 3.6 5.3 7.9 2.4 5.1 0.9 0.7 16.2 184 W Re Os 186 Re 187 Os 188 Os 188 Re 189m Os 190 Os 190 Re 180 Re 181 Re 182m Re 183 Re 183 Re 185 Re 182 W 189 Os 190 Os 191 Ir 191 Os 193m Ir 194 Ir 196 Ir 180 Os 182 Os 183m Os 184 Os 185 Os 186 Os 186 Os 187 Os 188 Os 189m Os 190 Os 190 Ir 190m Os 191 Ir 192 Pt 192 Ir 192 Ir 193 Ir 194 Pt 194 Pt 184 184 186 186 W W 189 Os 190 Os 183 Os 193 Ir 183 Os 186 Ir 189 Os 190 Ir 192 Os Pt 192 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 29 75 75 75 75 75 75 75 75 75 75 76 76 76 76 76 76 76 76 76 76 76 76 76 76 77 77 77 77 77 77 77 77 77 77 77 77 77 77 77 77 77 77 77 77 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Re Re 186 Re 186m Re 187 Re 188 Re 188m Re 189 Re 190 Re 190m Re 180 Os 181 Os 182 Os 183 Os 183m Os 185 Os 186 Os 189m Os 190m Os 191 Os 191m Os 193 Os 194 Os 196 Os 180 Ir 182 Ir 183 Ir 184 Ir 185 Ir 186 Ir 186m Ir 187 Ir 188 Ir 189 Ir 190 Ir 190m Ir 190 Irn 191m Ir 192 Ir 192m Ir 192 Irn 193m Ir 194 Ir 194m Ir 184m Table 2. Continued 195 30 77 77 77 77 78 78 78 78 78 78 78 78 78 78 78 78 78 78 78 79 79 79 79 79 79 79 79 79 79 79 79 79 79 79 79 79 79 79 A 195 195 196 196 184 186 187 188 189 190 191 193 193 195 197 197 199 200 202 186 187 190 191 192 193 193 194 195 195 196 196 198 198 199 200 200 201 202 Half-live 2.5 h 3.8 h 52 s 1.40 h 17.3 m 2.08 h 2.35 h 10.2 d 10.87 h 6.50E þ 11 y 2.802 d 50 y 4.33 d 4.02 d 19.8915 h 95.41 m 30.80 m 12.5 h 44 h 10.7 m 8.4 m 42.8 m 3.18 h 4.94 h 17.65 h 3.9 s 38.02 h 186.098 d 30.5 s 6.183 d 9.6 h 2.69517 d 2.27 d 3.139 d 48.4 m 18.7 h 26 m 28.8 s Decay Mode B2 B2IT B2 B2 ECBþA ECA ECBþ ECA ECBþ A EC EC IT IT B2 ITB2 B2 B2 B2 ECBþ ECBþA ECBþ ECBþ ECBþ EC ITEC ECBþ EC IT ECB2 IT B2 IT B2 B2 B2IT B2 B2 Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 14 67 198 419 134 118 101 41 87 0 58 1 3 19 6 18 34 13 1 1208 153 332 106 267 35 37 156 20 38 86 51 70 101 19 43 336 6 93 14 67 38 419 135 118 109 41 87 0 58 1 3 19 6 18 34 13 0 245 161 323 106 273 35 37 159 20 38 86 51 70 101 19 42 336 6 27 24 75 3673 430 155 128 176 52 101 0 71 6 8 34 12 32 387 19 725 3490 339 781 118 371 44 47 164 33 49 94 75 72 115 22 1449 343 44 3212 22 74 38 428 156 128 122 52 101 0 71 6 8 34 12 32 35 19 0 243 155 252 118 226 44 47 150 33 49 94 75 71 115 22 40 343 7 26 1476.3 1482.7 1076.1 1518.8 720.6 185.5 484.5 301.5 175.9 0.0 145.1 1.6 734.6 419.5 1406.9 1980.3 1438.3 1380.5 1220.4 1086.5 319.1 424.2 458.8 271.5 248.5 923.7 186.4 10.5 951.4 203.8 3220.4 1513.0 1567.1 1299.2 1195.4 1954.8 1379.6 1068.5 3.7 5.5 1.3 18.0 15.1 7.3 9.7 6.8 8.9 0.0 7.9 1.6 1.6 6.2 2.0 5.2 1.7 2.8 0.0 10.9 7.4 9.5 8.9 8.5 5.7 5.6 7.2 5.7 5.8 7.2 11.1 3.2 12.8 2.8 1.0 15.3 0.4 0.6 Daughter nuclei with highest yield 195 Pt Pt Pt 196 Pt 184 Ir 186m Ir 187 Ir 188 Ir 189 Ir 186 Os 191 Ir 193 Ir 193 Pt 195 Pt 197 Au 197 Pt 199 Au 200 Au 202 Au 186 Pt 187 Pt 190 Pt 191 Pt 192 Pt 193 Pt 193 Au 194 Pt 195 Pt 195 Au 196 Pt 196 Au 198 Hg 198 Au 199 Hg 200 Hg 200 Au 201 Hg 202 Hg 195m 195 Ir 180 Os Ir 196 186 184 Os 197 Au 183 Ir 193m Pt 196 Hg 200 Hg 195 Pt 182 Os T. OTTO Ir Ir 196 Ir 196m Ir 184 Pt 186 Pt 187 Pt 188 Pt 189 Pt 190 Pt 191 Pt 193 Pt 193m Pt 195m Pt 197 Pt 197m Pt 199 Pt 200 Pt 202 Pt 186 Au 187 Au 190 Au 191 Au 192 Au 193 Au 193m Au 194 Au 195 Au 195m Au 196 Au 196m Au 198 Au 198m Au 199 Au 200 Au 200m Au 201 Au 202 Au 195m Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 190 190 191 192 193 193 194 195 195 197 197 199 203 205 206 207 190 190 194 194 195 196 197 198 198 199 200 201 202 204 206 206 207 208 209 210 194 195 196 197 197 198 199 200 201 20.0 m 50.8 m 4.85 h 3.80 h 11.8 h 440 y 10.53 h 41.6 h 64.94 h 23.8 h 42.66 m 46.612 d 5.2 m 8.15 m 2.9 m 2.6 m 3.7 m 33.0 m 32.8 m 1.16 h 1.84 h 2.84 h 5.3 h 1.87 h 7.42 h 26.1 h 72.912 h 12.23 d 3.78 y 4.200 m 3.74 m 4.77 m 3.053 m 2.161 m 1.30 m 12.0 m 15 m 37 m 8m 43 m 2.4 h 90 m 21.5 h 9.33 h ECBþ ECBþ EC ECBþ ECBþIT EC ECBþ ITECBþ EC ITEC IT B2 B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþIT ECBþ ECBþ EC EC B2EC B2 IT B2 B2 B2 B2 ECBþA ECBþ ECBþ ECBþ ECBþIT EC ECBþ EC ECBþ 42 238 55 132 162 1 38 40 18 21 36 43 1 22 393 2484 943 522 408 180 276 77 293 208 48 208 22 85 0 0 398 0 440 315 1142 172 267 91 228 197 82 158 44 130 42 242 55 133 163 1 38 40 18 21 36 43 1 22 376 218 407 157 420 182 279 78 294 210 48 208 22 85 0 0 398 0 420 314 405 173 280 91 233 200 82 162 44 130 54 275 68 140 168 7 52 57 31 32 46 46 263 58 1191 4617 2907 2071 973 191 687 87 291 228 58 222 32 92 1 269 419 149 772 1053 3679 187 628 111 319 257 102 195 69 148 54 244 68 138 164 7 51 57 31 32 46 46 1 24 327 221 412 162 432 173 252 85 261 229 58 209 32 92 0 0 409 0 275 280 370 183 310 112 227 225 102 165 69 147 124.3 1142.7 202.5 294.4 171.9 1.6 59.8 532.4 9.9 2443.0 2546.9 754.8 1303.4 1742.5 1821.8 587.0 603.2 365.5 580.8 244.1 210.8 204.5 116.6 2035.1 491.4 156.2 117.2 64.9 1336.4 1290.9 1509.5 1319.2 1491.7 1286.2 1357.5 504.5 613.3 1008.0 231.2 2460.2 704.6 216.1 896.1 388.1 7.4 12.1 8.2 7.8 6.9 1.6 5.7 7.1 5.1 4.6 5.5 3.9 0.1 1.9 7.7 8.5 14.2 7.3 16.9 7.6 8.4 5.6 8.4 13.5 5.7 8.3 4.7 6.1 0.1 0.0 17.4 0.0 5.6 8.0 10.6 11.9 19.0 11.7 10.5 15.9 11.4 9.5 11.3 11.0 190 Au Au Au 193 Au 193m Au 194 Au 195 Au 195 Hg 197 Au 197 Hg 199 Hg 203 Tl 205 Tl 206 Tl 207 Tl 190 Hg 190 Hg 194 Hg 194 Hg 195 Hg 196 Hg 197 Hg 198 Hg 198 Tl 199 Hg 200 Hg 201 Hg 202 Hg 204 Pb 206 Pb 206 Tl 207 Pb 208 Pb 209 Pb 210 Pb 194 Tl 195 Tl 196 Tl 197 Tl 197 Tl 198 Tl 199 Tl 200 Tl 201 Tl 191 192 193m 193 Au Hg 195 Au 197 Au 195m 193 Au Hg 198 Hg 204 Hg 190 Hg 197 Pb Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 31 80 80 80 80 80 80 80 80 80 80 80 80 80 80 80 81 81 81 81 81 81 81 81 81 81 81 81 81 81 81 81 81 81 81 81 82 82 82 82 82 82 82 82 82 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Hg Hg 192 Hg 193 Hg 193m Hg 194 Hg 195 Hg 195m Hg 197 Hg 197m Hg 199m Hg 203 Hg 205 Hg 206 Hg 207 Hg 190 Tl 190m Tl 194 Tl 194m Tl 195 Tl 196 Tl 197 Tl 198 Tl 198m Tl 199 Tl 200 Tl 201 Tl 202 Tl 204 Tl 206 Tl 206m Tl 207 Tl 208 Tl 209 Tl 210 Tl 194 Pb 195m Pb 196 Pb 197 Pb 197m Pb 198 Pb 199 Pb 200 Pb 201 Pb 191m Table 2. Continued 201m 32 82 82 82 82 82 82 82 82 82 82 82 83 83 83 83 83 83 83 83 83 83 83 83 83 83 83 83 83 83 83 84 84 84 84 84 84 84 84 A 201 202 202 203 204 205 209 210 211 212 214 197 200 201 202 203 204 205 206 207 208 210 210 211 212 212 213 214 215 216 203 204 205 206 207 208 209 210 Half-live 61 s 5.25E þ 4 y 3.53 h 51.873 h 67.2 m 1.53E þ 7 y 3.253 h 22.20 y 36.1 m 10.64 h 26.8 m 9.3 m 36.4 m 108 m 1.72 h 11.76 h 11.22 h 15.31 d 6.243 d 32.9 y 3.68E þ 5 y 5.013 d 3.04E þ 6 y 2.14 m 60.55 m 7.0 m 45.59 m 19.9 m 7.6 m 2.17 m 36.7 m 3.53 h 1.66 h 8.8 d 5.80 h 2.898 y 102 y 138.376 d Decay Mode IT ECA ITEC EC IT EC B2 B2A B2 B2 B2 ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ ECBþ EC B2A A A B2A B2 B2A B2A B2 B2 ECBþA ECA ECBþA ECA ECBþA A A A Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 62 1 322 61 328 1 0 4 11 28 46 261 396 256 429 348 453 247 514 243 310 0 47 8 17 0 22 253 44 429 246 200 244 202 204 0 1 0 62 1 322 61 328 1 0 4 11 28 46 265 402 259 437 348 453 247 514 243 305 0 47 8 16 0 22 210 43 126 255 200 247 202 205 0 1 0 70 11 333 78 331 11 0 15 109 35 53 941 898 289 630 341 464 253 519 306 191 13 50 9 981 259 117 1243 766 4476 413 241 269 237 221 0 1 0 70 11 331 78 331 11 0 15 11 35 53 273 422 255 444 325 457 235 514 254 170 0 50 9 19 0 23 183 46 127 264 240 255 235 219 0 1 0 570.0 3.6 355.4 573.8 224.5 3.6 1390.2 3.3 1343.2 1896.8 2144.0 284.3 629.3 138.5 539.2 237.8 371.8 107.8 637.0 131.0 7.9 1394.8 566.1 82.0 749.4 1292.5 1422.3 1288.6 1911.3 1118.0 1056.2 844.8 213.9 767.2 172.2 0.0 11.1 0.0 4.0 3.6 10.4 9.9 8.2 3.6 0.0 3.3 0.4 4.2 4.6 11.3 19.3 10.1 16.5 11.3 16.2 9.7 18.7 10.8 6.2 0.0 4.0 0.6 1.4 0.0 1.1 3.1 2.9 4.8 11.7 18.5 10.5 15.7 9.6 0.0 0.1 0.0 Daughter nuclei with highest yield 201 Pb Tl Pb 203 Tl 204 Pb 205 Tl 209 Bi 210 Bi 211 Bi 212 Bi 214 Bi 197 Pb 200 Pb 201 Pb 202 Pb 203 Pb 204m Pb 205 Pb 206 Pb 207 Pb 208 Pb 210 Po 206 Tl 207 Tl 212 Po 212m Po 213 Po 214 Po 215 Po 216 Po 203 Bi 204 Bi 205 Bi 206 Bi 207 Bi 208 Bi 205 Pb 206 Pb 202 198 202 202 206 Hg Tl Hg 197m Pb 201m Pb 204 Pb 206 Tl 211 Po Tl 208 209 210 199 Tl Tl Pb Pb 201 Pb 202 Pb 203 Pb 204 Pb 209 Bi 200 T. OTTO Pb Pb 202m Pb 203 Pb 204m Pb 205 Pb 209 Pb 210 Pb 211 Pb 212 Pb 214 Pb 197 Bi 200 Bi 201 Bi 202 Bi 203 Bi 204 Bi 205 Bi 206 Bi 207 Bi 208 Bi 210 Bi 210m Bi 211 Bi 212 Bi 212 Bin 213 Bi 214 Bi 215 Bi 216 Bi 203 Po 204 Po 205 Po 206 Po 207 Po 208 Po 209 Po 210 Po 202 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 211 211 212 212 213 214 215 216 218 204 205 206 207 208 209 210 211 215 216 217 218 219 220 207 209 210 211 212 215 216 217 218 219 220 222 223 212 219 220 221 222 223 224 227 219 0.516 s 2.99E 2 7 s 45.1 s 4.2E 2 6 s 1.643E 2 4 s 1.781E 2 3 s 0.145 s 3.10 m 9.2 m 26.2 m 30.6 m 1.80 h 1.63 h 5.41 h 8.1 h 7.214 h 1.00E 2 4 s 3.00E 2 4 s 3.23E 2 2 s 1.5 s 56 s 3.71 m 9.25 m 28.5 m 2.4 h 14.6 h 23.9 m 2.30usA 4.5E 2 5 s 5.40E 2 4 s 3.5E 2 2 s 3.96 s 55.6 s 3.8235 d 24.3 m 20.0 m 2.0E 2 2 s 27.4 s 4.9 m 14.2 m 22.00 m 3.33 m 2.47 m 10 msA A A A A A A A A ECBþA ECBþA ECBþA ECBþA ECBþA ECBþA ECBþA ECA A A A A A B2A ECBþA ECBþA A ECBþA A 327500 A A A A A A B2 ECBþA A A A B2 B2A B2 B2 298739 1 0 10 0 0 0 0 0 510 234 455 308 474 377 438 10 0 1 0 0 0 312 173 185 11 294 0 0 0 0 0 10 0 0 62 176 1 3 6 38 19 100 84 31 1 0 10 0 0 0 0 0 392 186 406 310 478 377 438 10 0 1 0 0 0 80 167 192 11 294 0 0 0 0 0 10 0 0 62 181 1 3 6 37 19 88 82 31 1 0 6 0 0 0 0 0 1654 823 1274 349 549 405 443 18 0 1 0 3 0 3925 707 332 12 309 0 0 0 0 0 11 0 0 518 331 1 8 7 730 36 1968 1208 36 1 0 6 0 0 0 0 0 408 196 415 308 483 402 425 18 0 1 0 0 0 84 179 196 12 302 0 0 0 0 0 11 0 0 76 196 1 8 7 49 31 89 94 36 0.4 0.0 0.7 0.0 0.0 0.0 0.0 0.1 507.6 443.3 522.1 915.9 1082.4 358.1 568.0 3.3 0.2 4.9 1.3 1.0 0.0 1549.8 409.2 376.8 43.9 280.5 0.0 0.0 0.0 0.0 0.0 75.9 0.0 0.0 1378.1 515.3 3.2 25.1 95.8 1284.1 1508.1 1242.0 1473.4 676.2 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 16.2 9.7 16.1 12.6 18.1 18.0 14.9 3.1 0.0 0.1 0.0 0.0 0.0 5.7 9.1 9.5 0.8 10.7 0.0 0.0 0.0 0.0 0.0 0.8 0.0 0.0 5.6 10.4 0.0 1.3 0.7 5.4 4.2 4.5 6.7 2.9 207 Pb Pb Pb 209 Pb 210 Pb 211 Pb 212 Pb 214 Pb 204 Po 205 Po 206 Po 207 Po 208 Po 209 Po 210 Po 211 Po 211 Bi 212 Bi 213 Bi 214 Bi 215 Bi 220 Rn 207 At 209 At 206 Po 211 At 208 Po 211 Po 212 Po 213 Po 214 Po 215 Po 216 Po 218 Po 223 Fr 212 Rn 215 At 216 At 217 At 222 Ra 223 Ra 224 Ra 227 Ra 215 Rn 208 208 218 At Bi 201 Bi 202 Bi 203 Bi 204 Bi 205 Bi 206 Bi 207 Bi 200 218 Rn 216 Bi Po 205 Po 210 At 207 Po 203 208 At 220 Ra 219 At Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 33 84 84 84 84 84 84 84 84 85 85 85 85 85 85 85 85 85 85 85 85 85 85 86 86 86 86 86 86 86 86 86 86 86 86 86 87 87 87 87 87 87 87 87 88 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Po Po 212m Po 213 Po 214 Po 215 Po 216 Po 218 Po 204 At 205 At 206 At 207 At 208 At 209 At 210 At 211 At 215 At 216 At 217 At 218 At 219 At 220 At 207 Rn 209 Rn 210 Rn 211 Rn 212 Rn 215 Rn 216 Rn 217 Rn 218 Rn 219 Rn 220 Rn 222 Rn 223 Rn 212 Fr 219 Fr 220 Fr 221 Fr 222 Fr 223 Fr 224 Fr 227 Fr 219 Ra 212 Table 2. Continued 220 34 88 88 88 88 88 88 88 88 88 88 89 89 89 89 89 89 89 89 89 89 90 90 90 90 90 90 90 90 90 90 90 90 90 91 91 91 91 91 A 220 221 222 223 224 225 226 227 228 230 223 224 225 226 227 228 230 231 232 233 223 224 226 227 228 229 230 231 232 233 234 235 236 227 228 229 230 231 Half-live 1.79E 2 2 s 28 s 38.0 s 11.43 d 3.66 d 14.9 d 1600 y 42.2 m 5.75 y 93 m 2.10 m 2.78 h 10.0 d 29.37 h 21.772 y 6.15 h 122 s 7.5 m 119 s 145 s 0.60 s 1.05 s 30.57 m 18.68 d 1.9116 y 7.34E þ 3 y 7.538E þ 4 y 25.52 h 1.405E10 y 22.3 m 24.10 d 7.1 m 37.5 m 38.3 m 22 h 1.50 d 17.4 d 3.276E þ 4 y Decay Mode A A A A A B2 A B2 B2 B2 A ECA A B2ECA B2A B2 B2 B2 B2 B2 A A A A A A A B2 A B2 B2 B2 B2 A ECBþA ECA ECB2A A Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 1 10 2 29 2 9 1 37 4 17 5 51 6 28 1 141 117 80 269 88 20 5 3 34 2 32 2 21 2 9 4 10 7 9 232 20 119 19 1 10 2 29 2 9 1 37 4 17 5 51 6 28 1 141 81 80 162 85 20 5 3 34 2 32 2 21 2 9 4 9 7 9 233 20 119 19 1 21 2 40 2 15 2 89 10 22 9 73 15 39 2 347 2371 399 2483 1755 35 6 6 57 6 66 5 47 5 37 8 853 15 19 269 36 142 40 1 21 2 40 2 15 2 57 10 22 9 73 15 36 2 150 77 91 141 85 35 6 6 57 6 66 5 47 5 12 8 9 10 19 262 36 142 40 0.7 320.6 7.8 608.9 29.7 731.3 58.0 1744.6 1.3 1399.6 22.8 56.6 14.4 1229.9 0.4 1420.0 1164.8 1883.1 1131.4 1154.2 154.4 205.0 4.8 316.2 3.9 202.0 1.9 524.9 1.2 1398.8 86.1 1249.1 1446.5 2.8 263.4 5.0 161.1 107.6 0.0 3.3 0.1 4.9 0.2 2.0 0.2 6.3 1.3 2.3 1.3 9.2 2.4 4.2 0.4 6.2 2.8 8.0 4.0 2.9 5.0 0.7 0.9 7.5 1.0 10.0 0.8 6.8 0.8 1.2 1.1 0.3 0.9 2.7 15.0 4.9 8.6 5.8 Daughter nuclei with highest yield 216 Rn Rn Rn 219 Rn 220 Rn 225 Ac 222 Rn 227 Ac 228 Ac 230 Ac 219 Fr 224 Ra 221 Fr 226 Th 227 Th 228 Th 230 Th 231 Th 232 Th 233 Th 219 Ra 220 Ra 222 Ra 223 Ra 224 Ra 225 Ra 226 Ra 231 Pa 228 Ra 233 Pa 234m Pa 235 Pa 236 Pa 223 Ac 228 Th 229 Th 230 Th 227 Ac 217 218 220 Fr 226 Ra Fr 223 222 Fr 227 Th Ac Ac 230 U 224 225 226 Ac T. OTTO Ra Ra 222 Ra 223 Ra 224 Ra 225 Ra 226 Ra 227 Ra 228 Ra 230 Ra 223 Ac 224 Ac 225 Ac 226 Ac 227 Ac 228 Ac 230 Ac 231 Ac 232 Ac 233 Ac 223 Th 224 Th 226 Th 227 Th 228 Th 229 Th 230 Th 231 Th 232 Th 233 Th 234 Th 235 Th 236 Th 227 Pa 228 Pa 229 Pa 230 Pa 231 Pa 221 Z Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 232 232 233 234 234 235 236 237 227 228 230 231 232 233 234 235 235 236 237 238 239 240 242 232 233 234 235 236 236 237 238 239 240 240 241 242 242 232 234 235 236 237 238 239 240 1.31 d 26.967 d 6.70 h 1.17 m 24.5 m 9.1 m 8.7 m 1.1 m 9.1 m 20.8 d 4.2 d 68.9 y 1.592E þ 5 y 2.455E þ 5 y 7.04E þ 8 y 26 m 2.342E þ 7 y 6.75 d 4.468E þ 9 y 23.45 m 14.1 h 16.8 m 14.7 m 36.2 m 4.4 d 396.1 d 1.54E þ 5 y 22.5 h 2.144E þ 6 y 2.117 d 2.3565 d 61.9 m 7.22 m 13.9 m 2.2 m 5.5 m 33.7 m 8.8 h 25.3 m 2.858 y 45.2 d 87.7 y 2.411E þ 4 y 6564 y B2EC B2 B2 B2IT B2 B2 B2 A A A ECA A A A A IT A B2 A B2 B2 B2 ECBþ ECA ECBþ ECA ECB2A ECB2 A B2 B2 B2 B2IT B2 B2 B2 ECA ECA ECA A ECA A A A 159 50 252 4 0 150 99 28 3 3 41 3 1 2 36 0 2 42 2 14 8 8 211 25 171 8 58 15 20 97 46 190 59 11 54 168 18 21 30 3 20 3 1 3 159 50 252 3 0 140 98 28 3 3 41 3 1 2 36 0 2 42 2 14 8 8 212 25 171 8 58 15 20 97 46 190 59 11 39 168 18 21 30 3 20 3 1 3 176 69 291 1651 121 1531 595 41 7 7 82 7 4 6 47 0 6 63 5 40 17 25 241 39 212 20 103 24 41 120 64 250 953 53 2331 500 29 34 48 7 35 6 3 6 175 69 280 3 0 137 99 41 7 7 82 7 4 6 47 0 6 63 5 18 17 9 239 39 172 20 103 24 41 107 64 218 67 16 37 196 29 34 48 7 35 6 3 6 756.7 1710.6 1993.1 1143.6 1330.0 1373.2 1321.0 926.2 7.9 5.1 12.8 1.7 1.3 1.1 100.7 0.0 0.9 918.2 0.7 1383.8 832.3 1416.3 388.8 37.3 53.1 3.0 1326.6 612.7 23.2 812.6 1883.0 2063.5 1243.7 1497.9 1110.6 2239.0 3.6 4.3 6.7 1.0 4.6 1.0 0.5 0.9 7.4 7.1 14.0 0.1 0.0 5.0 2.3 4.8 0.9 1.1 11.6 1.1 0.5 1.0 5.5 0.0 0.9 7.7 0.7 2.0 2.4 0.7 13.1 4.9 7.6 3.0 13.5 3.0 5.6 3.9 7.1 11.8 3.6 1.9 0.9 10.5 3.6 4.2 5.9 1.0 4.6 0.9 0.4 0.9 232 U U 234 U 234 U 235m U 236 U 237 U 223 Th 224 Th 226 Th 231 Pa 228 Th 229 Th 230 Th 231 Th 235 U 232 Th 237 Np 234 Th 239 Np 240m Np 242 Np 232 U 233 U 234 U 235 U 236 U 236 U 233 Pa 238 Pu 239 Pu 240 Pu 240 Pu 241 Pu 242 Pu 242 Pu 232 Np 234 Np 235 Np 232 U 237 Np 234 U 235m U 236 U 232 Th 234 Pa U 233 235 227 Th SF 229 Pa 235m 231 236 232 Pu 236 Pu 240 Pa Pa Np 228 U U U SF 233 U SF 235 U SF 230 231 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 35 91 91 91 91 91 91 91 92 92 92 92 92 92 92 92 92 92 92 92 92 92 92 93 93 93 93 93 93 93 93 93 93 93 93 93 93 94 94 94 94 94 94 94 94 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Pa Pa 234 Pa 234m Pa 235 Pa 236 Pa 237 Pa 227 U 228 U 230 U 231 U 232 U 233 U 234 U 235 U 235m U 236 U 237 U 238 U 239 U 240 U 242 U 232 Np 233 Np 234 Np 235 Np 236 Np 236m Np 237 Np 238 Np 239 Np 240 Np 240m Np 241 Np 242 Np 242m Np 232 Pu 234 Pu 235 Pu 236 Pu 237 Pu 238 Pu 239 Pu 240 Pu 233 Table 2. Continued 241 36 94 94 94 94 94 94 95 95 95 95 95 95 95 95 95 95 95 95 95 95 96 96 96 96 96 96 96 96 96 96 96 96 96 96 97 97 97 97 A 241 242 243 244 245 246 237 238 239 240 241 242 242 243 244 244 245 246 246 247 238 239 240 241 242 243 244 245 246 247 248 249 250 251 245 246 247 248 Half-live 14.35 y 3.75E þ 5 y 4.956 h 8.00E þ 7 y 10.5 h 10.84 d 73.0 m 98 m 11.9 h 50.8 h 432.2 y 16.02 h 141 y 7.37E þ 3 y 10.1 h 26 m 2.05 h 39 m 25.0 m 23.0 m 2.4 h 2.9 h 27 d 32.8 d 162.8 d 29.1 y 18.10 y 8.5E þ 3 y 4.76E þ 3 y 1.56E þ 7 y 3.48E þ 5 y 64.15 m 8300 y 16.8 m 4.94 d 1.80 d 1.38E þ 3 y 23.7 h Decay Mode B2A A B2 A B2 B2 ECA ECBþA ECA ECA A B2EC ITA A B2 B2 B2 B2 B2 B2 ECA ECBþ A ECA A A A A A A A B2 A B2 ECA EC A B2EC Hp(10), 100 cm Hp(3)slab, 100 cm Hp(0.07)slab, 10 cm Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 Unshielded Shielded mSv h21 GBq21 0 2 8 12 71 39 80 154 67 179 16 10 7 17 153 6 8 157 156 31 25 59 3 109 3 35 2 32 3 55 861 3 27729 20 60 156 31 16 0 2 8 5 71 39 80 155 67 179 16 10 7 17 153 6 8 157 155 31 25 59 3 109 3 35 2 32 2 55 431 3 22475 20 60 156 31 16 0 5 12 47 78 52 101 178 98 205 28 19 14 23 180 210 11 211 396 154 36 75 6 136 6 51 5 50 10 56 2554 4 29734 114 80 179 37 23 0 5 12 7 76 52 101 171 98 205 28 19 14 23 179 9 11 193 160 39 36 75 6 136 6 51 5 50 4 56 152 3 1504 22 80 178 37 22 0.0 0.8 1273.1 9.1 2148.6 456.8 457.9 45.4 1065.7 23.8 3.8 1134.1 2.6 2.8 1773.5 1315.7 1603.1 3513.7 1427.0 2115.3 4.6 81.8 1.0 511.1 0.8 904.8 0.7 371.0 2.2 132.6 564.2 1412.8 5300.6 1486.7 829.4 16.2 756.8 958.9 0.0 0.7 1.4 0.7 3.9 5.9 9.2 8.4 11.4 9.8 3.7 2.3 1.9 2.8 9.6 1.0 1.2 13.7 4.3 4.0 4.3 8.3 0.9 11.1 0.8 5.8 0.7 6.1 0.5 2.8 4.0 0.1 35.5 1.1 8.7 9.2 3.6 2.3 Daughter nuclei with highest yield 241 Am U 243 Am 240 U 245 Am 246m Am 237 Pu 238 Pu 239 Pu 240 Pu 237 Np 242 Cm 242 Am 239 Np 244 Cm 244 Cm 245 Cm 246 Cm 246 Cm 247 Cm 238 Am 239 Am 236 Pu 241 Am 238 Pu 239 Pu 240 Pu 241 Pu 242 Pu 243 Pu 244 Pu 249 Bk 246 Pu 251 Bk 245 Cm 246 Cm 243 Am 248 Cf 238 237 U SF SF 233 Np Np 235 Np 236 Np 234 242 238 Pu Np T. OTTO Pu Pu 243 Pu 244 Pu 245 Pu 246 Pu 237 Am 238 Am 239 Am 240 Am 241 Am 242 Am 242m Am 243 Am 244 Am 244m Am 245 Am 246 Am 246m Am 247 Am 238 Cm 239 Cm 240 Cm 241 Cm 242 Cm 243 Cm 244 Cm 245 Cm 246 Cm 247 Cm 248 Cm 249 Cm 250 Cm 251 Cm 245 Bk 246 Bk 247 Bk 248m Bk 242 Z 234 Pu SF 237 Pu SF 243 Am SF SF SF SF 250 Bk 241 Am 248 Cm SF Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 37 97 97 97 98 98 98 98 98 98 98 98 98 98 98 99 99 99 99 99 99 99 99 99 100 100 100 100 100 100 100 249 250 251 244 246 247 248 249 250 251 252 253 254 255 249 250 250 251 253 254 254 255 256 251 252 253 254 255 256 257 330 d 3.212 h 55.6 m 19.4 m 35.7 h 3.11 h 334 d 351 y 13.08 y 900 y 2.645 y 17.81 d 60.5 d 85 m 102.2 m 8.6 h 2.22 h 33 h 20.47 d 275.7 d 39.3 h 39.8 d 25.4 m 5.30 h 25.39 h 3.00 d 3.240 h 20.07 h 157.6 m 100.5 d B2A B2 B2 A A ECA A A A A A B2A A B2 ECBþA EC ECBþ ECA A A B2A B2A B2 ECBþA A ECA A A A A 0 141 28 3 2 40 2 63 5 35 233 6 53103 0 85 265 100 36 1 22 87 0 4 40 2 31 4 20 43584 51 For the meaning of ‘shielded’ and ‘unshielded’, refer to the main text. 0 141 28 3 2 40 2 63 3 35 106 6 47177 0 85 265 100 36 1 22 85 0 4 40 2 31 3 20 40618 43 0 205 42 5 4 64 5 69 17 48 791 10 34411 0 100 323 115 55 1 43 104 1 440 51 4 48 12 38 19258 107 0 145 41 5 4 64 4 69 4 48 55 10 1905 0 99 323 112 55 1 43 93 0 7 51 4 48 4 38 1415 58 0.2 1413.0 1826.3 0.7 0.6 68.3 0.7 142.8 5.1 1604.9 199.4 433.4 6899.2 1404.4 157.7 1115.8 24.7 157.6 1.4 8.1 1233.8 510.5 1269.0 64.0 0.6 91.3 3.8 6.4 5632.4 650.4 0.0 3.4 4.7 0.7 0.5 7.5 0.6 4.5 0.5 5.5 1.7 1.3 45.0 0.0 7.3 23.7 6.3 6.5 0.2 5.5 3.8 0.0 0.8 4.9 0.4 5.6 0.5 4.8 33.7 6.3 249 Cf Cf 251 Cf 240 Cm 242 Cm 247 Bk 244 Cm 245 Cm 246 Cm 247 Cm 248 Cm 253 Es 250 Cm 255 Es 249 Cf 250 Cf 250 Cf 251 Cf 249 Bk 250 Bk 254 Fm 255 Fm 256 Fm 251 Es 248 Cf 253 Es 250 Cf 251 Cf 252 Cf 253 Cf 245 250 Am SF 243 Cm SF SF SF SF 249 Cm SF 245 Bk 247 Bk SF 254 Fm 250 Bk 251 Bk 247 Cf SF 249 Cf SF SF SF SF SF 254 Cf SF PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Bk Bk 251 Bk 244 Cf 246 Cf 247 Cf 248 Cf 249 Cf 250 Cf 251 Cf 252 Cf 253 Cf 254 Cf 255 Cf 249 Es 250 Es 250m Es 251 Es 253 Es 254 Es 254m Es 255 Es 256 Es 251 Fm 252 Fm 253 Fm 254 Fm 255 Fm 256 Fm 257 Fm 250 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 249 Table 3. Contribution of the different decay modes to personal dose equivalent for the ISO slab phantom Hp(d) in 10, 3 and 0.07 mm. 3 10 38 Electron 0 9 0 116 0 0 0 209 273 0 140 0 0 0 92 183 496 139 215 237 230 193 0 0 0 0 0 0 299 212 0 187 0 181 209 463 0 0 0 0 0 0 0 0 0 16 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 39 11 0 14 3658 46 33 1380 34 7 49 2 5 0 1 0 12 69 3 0 0 414 1 0 0 180 18 2353 24 0 1898 47 951 0 0 0 0 0 174 174 0 174 0 174 174 0 174 169 174 0 157 0 0 0 143 0 0 0 0 174 0 0 0 0 0 174 94 0 0 0 0 0 0 Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 0 9 0 118 0 0 0 69 153 0 128 0 0 0 92 170 316 138 205 173 170 170 0 0 0 0 0 0 126 143 0 119 0 122 189 299 0 0 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 0 0 13 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1311 6 0 38 7164 1094 876 6088 894 5 2229 1369 5 166 764 0 48 4076 2465 297 0 4990 736 0 0 1197 576 6835 903 0 4476 1516 4846 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 174 174 0 174 0 174 174 0 174 169 174 0 157 0 0 0 142 0 0 0 0 174 0 0 0 0 0 174 94 0 0 0 0 0 0 0.0 0.3 0.0 2.4 0.0 0.0 0.0 0.7 1.4 0.0 4.2 0.0 0.0 0.0 3.2 2.0 3.1 2.3 4.9 1.6 1.6 2.0 0.0 0.0 0.0 0.0 0.0 0.0 1.1 1.3 0.0 2.1 0.0 1.1 3.5 3.2 0.0 0.0 Electron b 2/b þ mSv h21 GBq21 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.1 0.0 0.0 7.2 0.0 0.0 0.0 0.7 0.0 0.0 0.1 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 91.9 0.0 0.0 1.2 0.1 0.0 0.0 0.0 0.0 1726.4 1168.6 1578.6 31.7 1443.6 850.0 1189.7 1217.9 897.4 1214.7 1675.6 1080.2 1154.6 1561.8 1320.5 1209.5 1331.5 1128.6 981.2 1072.8 1281.4 321.2 940.7 1211.3 463.9 52.3 1178.0 1400.2 857.7 650.1 1511.3 1051.0 1151.6 962.6 0.0 1560.9 Annihilation 0.0 0.0 0.0 6.0 6.0 0.0 6.0 0.0 6.0 6.0 0.0 6.0 5.8 6.0 0.0 5.4 0.0 0.0 0.0 4.9 0.0 0.0 0.0 0.0 6.0 0.0 0.0 0.0 0.0 0.0 6.0 3.3 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO H Be Be 10 C 11 C 14 C 13 N 16 N 14 O 15 O 19 O 17 F 18 F 19 Ne 24 Ne 22 Na 24 Na 27 Mg 28 Mg 26 Al 28 Al 29 Al 31 Si 32 Si 30 P 32 P 33 P 35 S 37 S 38 S 34 Cl 34m Cl 36 Cl 38 Cl 39 Cl 40 Cl 37 Ar 39 Ar 7 Photon Contribution to Hp(3)slab in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Contribution to Hp(10) in 100 cm Nuclides 41 43 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 845 7 136 0 627 0 1634 205 3749 0 0 0 2 153 12 21 0 0 0 0 2 890 0 11 2 1 39 5 0 0 10 4 0 22 0 14 0 645 47 2 89 0 0 0 0 0 173 0 0 0 0 0 0 0 0 0 0 173 153 164 0 0 0 0 0 0 0 148 0 0 168 88 0 0 0 0 3 162 0 0 0 173 169 52 168 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 169 0 177 206 158 19 32 164 233 188 244 0 0 141 134 418 15 165 48 300 19 478 0 419 29 0 64 32 1 333 0 166 176 154 75 20 6 0 30 498 1 442 173 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 53 0 4181 322 3768 174 4853 22 3791 2421 6487 0 0 271 1825 4048 30 311 0 0 0 0 1429 5848 0 6 1766 1003 1317 18 0 0 3041 2621 0 353 0 3240 310 5339 2123 2 3406 0 0 0 0 0 173 0 0 0 0 0 0 0 0 0 0 173 153 164 0 0 0 0 0 0 0 148 0 0 168 88 0 0 0 0 3 162 0 0 0 173 169 52 168 0 1.9 0.0 2.5 4.1 1.5 0.2 0.3 6.1 2.9 4.0 2.6 0.0 0.0 1.8 1.2 6.9 0.7 2.2 3.2 4.5 1.9 6.7 0.0 6.6 2.9 0.0 3.4 3.4 0.0 4.4 0.0 1.8 1.8 2.3 5.4 1.9 0.3 0.0 3.0 7.2 0.0 6.4 1.8 0.0 0.1 0.0 0.2 6.5 0.0 0.0 0.0 1.4 0.1 7.9 0.0 0.0 0.0 0.1 0.0 1.7 0.2 0.1 295.4 0.2 8.8 1.4 0.0 1.0 0.1 0.0 3.4 4.7 0.0 0.2 0.0 0.1 0.1 0.2 11.0 55.5 0.4 0.0 0.0 4.4 0.0 0.6 1.2 0.0 1393.5 1559.6 1014.1 1353.0 985.0 1133.5 973.0 1509.5 1037.0 1089.1 878.7 0.0 491.1 1455.9 1116.3 969.6 1318.4 1235.1 0.0 1010.5 1345.5 1504.8 1133.6 914.5 0.0 1315.9 1110.9 1176.2 1114.4 889.4 0.0 78.3 1030.6 1051.6 8.4 1203.6 0.0 1019.3 1275.6 918.0 1048.7 545.5 966.4 0.0 0.0 0.0 0.0 0.0 6.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 6.0 5.3 5.7 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.1 0.0 0.0 5.8 3.0 0.0 0.0 0.0 0.0 0.1 5.6 0.0 0.0 0.0 6.0 5.8 1.8 5.8 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 39 184 0 211 262 263 22 38 162 305 245 336 0 0 152 318 462 15 171 47 304 20 495 0 463 31 0 63 28 1 351 0 197 201 156 75 21 6 0 28 532 1 468 198 0 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ar Ar Ar 44 Ar 38 K 40 K 42 K 43 K 44 K 45 K 46 K 41 Ca 45 Ca 47 Ca 49 Ca 42m Sc 43 Sc 44 Sc 44m Sc 46 Sc 47 Sc 48 Sc 49 Sc 50 Sc 44 Ti 45 Ti 51 Ti 52 Ti 47 V 48 V 49 V 50 V 52 V 53 V 48 Cr 49 Cr 51 Cr 55 Cr 56 Cr 50m Mn 51 Mn 52 Mn 52m Mn 53 Mn 42 Table 3. Continued 54 57 40 Photon Electron 132 239 18 349 31 31 448 0 173 0 202 86 429 184 463 24 131 0 360 1 20 220 378 276 206 0 0 79 0 17 66 396 31 1 1 15 21 81 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 35 19 1350 6 87 0 0 0 0 37 2 2349 15 4 0 1 0 0 0 0 1067 80 0 5 0 0 1 0 7130 741 118 9 197 0 16 0 12 0 0 0 0 97 169 0 0 0 0 0 0 174 132 33 0 26 0 0 0 0 0 0 0 76 0 0 0 0 174 171 161 107 171 30 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 132 204 22 319 30 30 417 0 165 0 187 86 402 178 378 27 130 0 337 1 19 188 336 271 176 0 0 71 0 16 63 320 31 1 1 15 21 79 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 0 1 0 0 0 0 0 1 0 1 0 0 0 1 0 0 1 1 0 1 0 0 0 0 0 0 1 0 0 0 0 0 0 0 2219 3186 6072 4 3191 0 0 1 0 3239 1489 6828 176 56 0 1 0 1 1 48 5638 3243 0 3 0 0 1084 0 8143 5019 2047 26 4248 0 3053 0 2045 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 97 169 0 0 0 0 0 0 174 132 33 0 26 0 0 0 0 0 0 0 76 0 0 0 0 174 171 161 107 170 30 0 0 0 2.3 2.9 1.6 5.0 2.9 1.4 6.3 0.0 2.2 0.0 3.3 3.0 7.1 3.0 5.0 2.9 2.3 0.0 4.0 0.0 1.3 2.3 4.2 8.5 2.2 0.0 0.0 0.9 0.0 0.2 1.2 3.7 1.0 0.0 0.0 0.2 2.0 1.4 Electron b 2/b þ mSv h21 GBq21 0.2 0.3 4.0 0.7 24.0 0.8 3.4 0.0 1.3 0.0 2.1 1.0 4.1 0.4 0.4 22.0 0.3 0.0 0.3 0.0 0.0 0.1 0.3 36.8 1.6 0.0 0.0 0.2 0.0 0.0 0.5 0.3 1.1 0.0 0.0 0.0 28.5 0.6 0.0 1194.3 1028.2 903.0 953.7 987.6 0.0 0.0 950.3 163.4 1036.6 1128.7 852.6 1061.7 254.0 0.0 273.4 0.0 801.3 3.0 1359.0 921.3 1046.8 0.0 737.0 0.0 0.0 1252.5 436.2 798.8 920.1 1020.8 907.0 942.3 876.0 1038.2 1163.8 1127.8 Annihilation 0.0 0.0 0.0 0.0 3.3 5.8 0.0 0.0 0.0 0.0 0.0 0.0 6.0 4.6 1.1 0.0 0.9 0.0 0.0 0.0 0.0 0.0 0.0 0.0 2.6 0.0 0.0 0.0 0.0 6.0 5.9 5.5 3.7 5.9 1.0 0.0 0.0 0.0 T. OTTO Mn Mn Mn 58m Mn 52 Fe 53 Fe 53m Fe 55 Fe 59 Fe 60 Fe 61 Fe 62 Fe 54m Co 55 Co 56 Co 57 Co 58 Co 58m Co 60 Co 60m Co 61 Co 62 Co 62m Co 56 Ni 57 Ni 59 Ni 63 Ni 65 Ni 66 Ni 57 Cu 59 Cu 60 Cu 61 Cu 62 Cu 64 Cu 66 Cu 67 Cu 69 Cu 56 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 60 62 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 115 1950 1 49 0 0 0 29 0 0 1675 39 871 0 36 1 24 0 220 2 209 0 3 0 0 1 0 2242 196 57 3 160 0 0 75 0 707 2 6 560 0 11 6 0 168 172 15 162 2 0 0 0 0 0 170 156 96 0 155 0 0 0 0 41 162 0 41 0 0 0 0 172 164 157 49 153 0 51 0 0 0 0 75 167 0 114 36 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 91 57 63 22 81 0 72 51 261 33 217 41 140 28 6 1 307 65 320 80 67 3 105 3 6 171 50 338 24 437 50 129 9 78 65 2 176 6 96 92 51 92 16 100 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 1 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 3330 6029 0 2228 0 1 0 2943 251 0 5042 1560 3233 0 1197 569 820 55 2576 2 3677 0 9 0 18 989 0 6577 3953 2025 2 3008 0 49 3153 0 3757 1855 11 4593 0 72 155 0 168 172 15 162 2 0 0 0 0 0 170 156 96 0 155 0 0 0 0 41 162 0 41 0 0 0 0 172 164 157 49 153 0 51 0 0 0 0 75 167 0 114 36 0 3.0 1.0 2.4 0.4 1.1 0.0 3.0 1.5 9.0 4.1 2.7 2.0 1.7 2.2 0.1 0.0 4.7 4.7 5.6 5.1 3.2 0.9 2.5 1.0 0.5 7.5 3.6 5.1 1.0 6.9 3.8 2.3 2.1 2.5 1.7 0.1 3.4 0.2 17.1 3.0 13.6 9.3 2.4 15.1 2.0 0.4 1.5 0.1 0.1 0.0 77.6 0.9 7.2 31.2 0.3 7.4 0.2 14.7 0.0 0.9 7.0 9.6 2.1 18.1 45.6 0.0 0.5 0.0 3.0 102.0 8.9 2.0 8.7 9.6 238.6 22.9 0.0 1.3 1.3 4.3 2.1 0.2 8.8 33.3 0.0 23.4 1.5 33.1 970.8 877.3 155.6 1000.1 21.0 1488.3 0.5 1050.4 1287.6 642.3 906.0 1011.9 526.7 0.0 1030.8 1226.4 1346.9 1360.5 1101.9 404.6 932.7 0.0 349.6 0.0 1406.8 1221.1 1484.6 856.0 918.6 978.7 488.4 894.6 0.0 923.8 1043.9 1469.1 1057.3 1105.1 670.0 909.9 0.0 910.8 256.6 0.0 5.8 5.9 0.5 5.6 0.1 0.0 0.0 0.0 0.0 0.0 5.9 5.4 3.3 0.0 5.3 0.0 0.0 0.0 0.0 1.4 5.6 0.0 1.4 0.0 0.0 0.0 0.0 5.9 5.6 5.4 1.7 5.3 0.0 1.7 0.0 0.0 0.0 0.0 2.6 5.8 0.0 3.9 1.2 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 41 90 72 62 23 83 0 72 51 260 29 295 42 218 28 6 1 375 61 420 78 72 0 106 0 6 175 49 383 27 481 48 135 3 76 66 1 193 6 54 95 14 77 10 71 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Zn Zn Zn 63 Zn 65 Zn 69 Zn 69m Zn 71 Zn 71m Zn 72 Zn 64 Ga 65 Ga 66 Ga 67 Ga 68 Ga 70 Ga 72 Ga 73 Ga 74 Ga 66 Ge 67 Ge 68 Ge 69 Ge 71 Ge 75 Ge 77 Ge 78 Ge 68 As 69 As 70 As 71 As 72 As 73 As 74 As 76 As 77 As 78 As 79 As 70 Se 71 Se 72 Se 73 Se 73m Se 75 Se 61 Table 3. Continued 77m 79m 42 Photon Electron 17 0 5 1 6 392 143 73 285 76 415 425 78 300 20 57 8 15 9 17 412 6 1 217 414 10 51 52 83 38 36 7 26 2 0 29 108 250 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 0 16 363 0 4885 397 546 933 23 247 0 0 0 69 1 0 0 6 0 987 2 10 26 808 0 32 0 0 0 0 0 0 552 17 0 0 0 0 0 0 0 0 173 167 155 153 127 96 0 1 0 161 4 0 0 0 0 0 0 0 135 167 0 142 12 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 30 0 27 1 28 356 130 74 263 80 266 342 86 247 59 85 29 17 11 59 404 28 1 158 386 10 63 58 118 45 63 34 34 10 0 32 83 176 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 1 0 0 1 0 1 1 0 1 0 0 0 0 0 0 1 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 423 0 476 3948 206 7526 4464 2711 3833 573 1990 11 0 0 2863 1188 0 12 104 1 3596 1962 2924 661 5359 0 1010 0 0 0 0 0 0 4415 685 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 0 0 0 0 173 167 155 153 127 96 0 1 0 161 4 0 0 0 0 0 0 0 135 166 0 142 12 0 0 0 0 0 0 0 5.1 0.0 6.5 0.1 6.6 9.1 2.4 3.3 5.1 4.0 5.5 7.2 6.6 8.1 11.2 10.6 5.9 1.0 0.7 11.5 8.2 5.9 0.0 2.1 7.3 0.2 6.7 5.1 13.5 5.1 8.4 7.2 4.3 1.9 0.0 3.2 2.2 3.7 Electron b 2/b þ mSv h21 GBq21 1269.7 0.0 0.0 0.3 0.1 18.7 2.4 2.4 33.3 4.4 26.8 9.9 13.1 2.4 0.0 38.9 0.1 0.2 0.2 0.0 5.2 0.0 0.0 0.6 3.4 0.1 68.7 30.7 12.0 40.8 6.8 0.1 1057.5 0.0 0.0 223.9 3.5 47.3 0.0 32.5 0.2 1255.0 0.7 1396.4 1005.3 1298.7 815.7 913.0 941.6 891.4 912.6 629.6 2.8 12.0 0.0 946.6 1094.3 0.0 1208.0 23.9 1470.0 1086.3 1094.0 1046.7 942.5 876.6 0.0 954.9 128.4 0.0 0.0 0.0 1470.8 1170.1 1018.2 1288.0 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 6.0 5.8 5.4 5.3 4.4 3.3 0.0 0.0 0.0 5.6 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 4.6 5.7 0.0 4.9 0.4 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Se Se Se 81 Se 81m Se 83 Se 83m Se 84 Se 72 Br 73 Br 74 Br 74m Br 75 Br 76 Br 76m Br 77 Br 77m Br 78 Br 80 Br 80m Br 82 Br 82m Br 83 Br 84 Br 84m Br 85 Br 74 Kr 75 Kr 76 Kr 77 Kr 79 Kr 81 Kr 81m Kr 83m Kr 85 Kr 85m Kr 87 Kr 88 Kr 79 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 89 78 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 968 1321 922 1230 40 2406 3 0 507 3 0 6 0 1 0 0 3014 398 3187 1121 1651 1 77 0 4 0 0 0 0 0 11 0 65 8 1953 460 177 443 21 29 16 0 0 0 0 168 155 151 145 172 47 2 166 38 0 47 0 0 0 0 0 0 0 0 171 17 153 0 45 0 0 0 0 0 0 0 0 0 170 160 98 159 116 101 56 1 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 205 94 226 293 116 31 65 31 22 438 119 122 80 14 93 0 63 259 122 297 52 90 88 37 135 122 45 63 0 0 109 170 313 176 54 86 59 453 79 101 457 40 113 60 1 0 1 1 0 0 0 0 0 1 0 0 0 0 0 0 0 1 0 1 0 0 0 0 0 0 0 0 0 0 0 1 1 1 0 0 0 1 0 0 1 0 0 0 4174 5671 3697 4916 1577 6749 2 1 4891 44 0 124 0 905 0 0 6235 2245 5521 4185 6344 1 2665 0 14 0 0 0 368 0 1125 55 1498 1610 6507 4317 2616 3827 550 1356 236 2 0 0 0 168 155 151 145 171 47 2 166 38 0 47 0 0 0 0 0 0 0 0 171 17 153 0 45 0 0 0 0 0 0 0 0 0 170 160 98 159 116 101 56 1 0 1 4.2 4.8 4.9 6.5 7.9 0.9 6.3 4.9 0.7 13.6 9.5 6.3 6.4 0.2 3.0 0.0 0.7 3.5 1.6 4.2 5.3 7.8 5.2 6.2 10.4 9.2 4.3 3.7 0.0 0.0 2.0 2.0 7.4 1.9 5.9 5.6 4.6 8.0 4.0 4.3 11.5 3.6 8.5 3.7 21.2 25.2 4.6 6.5 190.4 0.6 2.2 0.0 0.2 5.6 2.6 0.5 1119.8 0.0 23.0 0.0 0.1 1.0 0.5 1.2 12.2 13.6 140.2 0.0 15.3 9.2 83.1 300.3 0.0 0.0 1.4 4.1 503.3 0.2 8.1 8.3 200.6 3.2 2.4 13.4 9.2 177.9 4.0 351.9 1011.8 868.9 877.1 787.2 927.6 840.6 433.2 14.1 892.4 362.6 0.0 460.7 0.0 1213.4 0.0 1143.3 894.2 1147.4 942.1 971.1 855.6 170.0 906.8 0.0 379.7 0.0 0.0 0.0 1254.2 1456.8 1262.2 1379.4 1188.6 1122.9 846.2 881.4 534.7 892.4 824.4 622.3 428.7 5.7 3.4 10.7 0.0 5.8 5.3 5.2 5.0 5.9 1.6 0.1 5.7 1.3 0.0 1.6 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.9 0.6 5.3 0.0 1.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.9 5.5 3.4 5.5 4.0 3.5 1.9 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 43 256 92 359 335 102 30 44 11 21 426 91 103 70 14 92 0 83 307 201 402 40 65 84 11 101 95 40 58 0 0 109 190 338 200 38 72 50 464 71 107 481 39 88 55 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Kr Rb Rb 78m Rb 79 Rb 80 Rb 81 Rb 81m Rb 82 Rb 82m Rb 83 Rb 84 Rb 84m Rb 86 Rb 86m Rb 87 Rb 88 Rb 89 Rb 90 Rb 90m Rb 79 Sr 80 Sr 81 Sr 82 Sr 83 Sr 85 Sr 85m Sr 87m Sr 89 Sr 90 Sr 91 Sr 92 Sr 93 Sr 94 Sr 81 Y 83 Y 83m Y 84m Y 85 Y 85m Y 86 Y 86m Y 87 Y 87m Y 77 Table 3. Continued 88 90 44 Photon Electron 379 140 0 112 0 89 38 14 115 133 87 80 15 81 154 101 0 118 140 53 514 476 77 85 487 16 18 253 163 3 248 12 123 23 388 108 427 43 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 2 0 1 0 722 93 1803 1397 466 0 43 0 3 0 0 0 1 1133 601 842 301 44 13 0 0 0 0 0 0 0 0 0 0 0 11 435 0 0 0 0 0 0 0 0 0 0 160 0 143 0 40 3 0 0 0 168 162 163 132 140 94 0 0 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 337 140 0 115 0 91 37 12 110 90 85 124 18 106 171 102 0 119 140 67 523 455 58 89 375 37 33 274 184 6 249 25 123 35 384 109 404 52 Electron b 2/b þ mSv h21 GBq21 2 0 1 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 2 0 1 2 0 0 5 0 0 0 0 0 0 0 0 0 1 0 2 0 0 0 2344 0 457 0 4921 3781 6004 4377 4486 0 1989 0 2 5 0 0 1014 5891 4825 4829 3750 1808 211 0 0 0 0 0 0 0 0 1 0 57 1302 5169 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 0 0 0 0 0 0 160 0 143 0 40 3 0 0 0 168 162 162 132 140 94 0 0 0 0 0 0 0 0 0 0 0 0 0 9.5 2.3 0.0 6.6 0.0 3.1 0.6 0.4 1.8 1.1 3.1 14.0 1.1 8.6 6.5 3.2 0.0 2.4 2.9 7.3 14.0 9.4 1.8 3.6 9.4 4.9 3.8 10.0 7.3 0.8 4.7 3.0 2.3 3.9 8.0 2.7 7.3 5.6 Electron b 2/b þ mSv h21 GBq21 0.4 8.3 0.1 212.1 0.0 64.8 0.6 4.9 1.0 0.4 8.1 117.4 0.0 46.0 8.3 51.9 0.0 1.6 23.8 519.4 11.4 11.7 0.4 3.5 230.8 0.0 0.0 4.6 0.8 0.0 3.1 0.0 1.6 2058.7 14.8 2.4 27.4 42.3 3.6 0.0 1086.8 0.0 1241.5 0.0 978.0 1023.7 906.9 1047.7 870.4 0.2 869.0 0.0 377.6 24.2 0.0 1026.0 1186.8 856.3 868.6 866.7 712.7 865.9 691.7 1.7 0.0 0.0 0.4 0.0 1398.5 6.9 28.1 78.0 1474.6 1357.1 1186.2 945.4 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.5 0.0 4.9 0.0 1.4 0.1 0.0 0.0 0.0 5.8 5.6 5.6 4.5 4.8 3.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Y Y Y 90m Y 91 Y 91m Y 92 Y 93 Y 94 Y 95 Y 85 Zr 86 Zr 87 Zr 88 Zr 89 Zr 89m Zr 93 Zr 95 Zr 97 Zr 87 Nb 88 Nb 88m Nb 89 Nb 89m Nb 90 Nb 91 Nb 91m Nb 92 Nb 92m Nb 93m Nb 94 Nb 94m Nb 95 Nb 95m Nb 96 Nb 97 Nb 98m Nb 99 Nb 89m Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 99m 90 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 824 2228 3 603 120 0 0 0 2 0 1779 1988 1527 1 2 1 44 0 0 0 0 0 0 0 0 0 0 2015 17 1247 281 69 0 2 0 0 0 0 64 0 5396 178 93 77 0 169 45 163 76 0 0 0 0 0 162 167 166 19 5 19 122 0 1 0 0 0 0 0 0 0 0 0 0 0 0 110 0 24 0 0 0 0 0 0 172 125 15 121 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 74 31 140 4 132 35 326 26 199 4 139 69 392 208 98 434 174 161 146 429 23 34 25 231 0 26 60 12 308 257 124 271 119 191 76 85 129 0 53 14 345 233 97 482 0 0 0 0 1 0 2 0 1 0 1 0 2 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 2 1 0 1 0 1 0 0 0 0 0 0 3 1 0 1 4643 6471 3 5129 1647 0 0 25 757 2 5289 6284 6059 1 62 1 2031 0 0 0 0 0 0 0 0 0 68 6644 1431 5183 4004 1977 0 6 0 0 43 0 3116 68 7657 2774 467 1915 0 169 45 163 76 0 0 0 0 0 162 167 166 19 5 19 122 0 1 0 0 0 0 0 0 0 0 0 0 0 0 110 0 24 0 0 0 0 0 0 172 125 15 121 1.8 0.6 11.4 0.3 2.5 4.4 7.8 1.0 4.4 0.3 1.9 2.0 10.6 5.7 4.0 11.3 3.8 6.6 8.3 11.3 2.1 4.1 2.9 5.1 0.0 2.6 3.6 0.3 6.4 6.4 5.5 17.8 7.1 8.0 7.5 3.0 4.2 0.0 1.6 1.5 5.1 4.3 3.1 10.3 16.6 0.2 457.1 0.0 21.3 0.0 1057.0 31.0 179.3 10.1 1.3 2.8 290.1 0.4 327.9 4.7 1.1 2.1 109.1 5.1 0.1 0.0 0.0 4.9 0.0 64.8 38.8 0.8 10.7 28.7 87.6 328.5 12.8 22.3 108.3 7.2 93.8 0.0 31.4 117.9 8.8 5.1 105.5 8.2 975.2 832.6 389.4 862.4 434.0 0.0 0.0 1344.3 1310.3 1446.8 838.4 833.7 837.6 191.7 32.6 185.6 729.9 0.0 8.3 0.0 0.0 0.0 0.0 1284.6 906.0 0.0 1354.8 873.4 1130.5 945.6 1012.8 672.9 0.0 204.1 0.0 270.7 1386.5 0.0 1054.7 1357.0 800.0 719.9 83.5 737.1 0.0 5.8 1.5 5.6 2.6 0.0 0.0 0.0 0.0 0.0 5.6 5.8 5.7 0.7 0.2 0.6 4.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 3.8 0.0 0.8 0.0 0.0 0.0 0.0 0.0 0.0 5.9 4.3 0.5 4.2 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 45 100 34 117 3 140 17 348 25 218 3 195 71 428 219 127 419 186 144 129 414 16 18 14 229 0 25 59 13 356 313 130 261 104 185 61 85 126 0 54 13 390 260 113 499 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Nb Mo Mo 91 Mo 91m Mo 93 Mo 93m Mo 99 Mo 101 Mo 102 Mo 91 Tc 91m Tc 92 Tc 93 Tc 93m Tc 94 Tc 94m Tc 95 Tc 95m Tc 96 Tc 96m Tc 97 Tc 97m Tc 98 Tc 99 Tc 99m Tc 101 Tc 102 Tc 102m Tc 104 Tc 105 Tc 92 Ru 94 Ru 95 Ru 97 Ru 103 Ru 105 Ru 106 Ru 107 Ru 108 Ru 94 Rh 95 Rh 95m Rh 96 Rh 89 Table 3. Continued 96m 97m 46 Photon Electron 139 139 284 139 114 112 393 34 72 69 70 365 2 2 29 14 34 445 55 54 55 188 250 84 131 59 83 21 0 11 27 8 8 5 214 272 135 389 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 322 25 11 494 0 1 3 0 0 0 0 0 0 4 0 0 462 0 0 1570 4 7 185 0 21 0 1 0 0 0 0 2 0 0 726 2201 93 147 62 102 31 157 7 13 7 1 0 0 27 0 0 0 0 0 0 0 0 0 0 59 112 8 84 0 9 0 0 0 0 0 0 0 148 164 126 128 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 128 136 230 133 130 122 335 46 85 81 77 377 3 2 38 14 34 431 56 54 57 193 217 96 125 76 100 31 0 14 30 7 14 5 192 245 131 347 Electron b 2/b þ mSv h21 GBq21 1 0 1 0 0 0 1 0 0 0 0 1 0 0 0 0 0 2 0 0 0 1 1 0 1 0 0 0 0 0 0 0 0 0 1 2 1 2 1752 969 450 4611 0 1 107 1 0 0 14 0 0 2553 0 0 4877 48 57 6325 2137 90 2100 0 852 0 0 0 0 3 0 1694 0 192 4306 6142 2390 2339 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 62 102 31 157 7 13 7 1 0 0 27 0 0 0 0 0 0 0 0 0 0 59 112 8 84 0 9 0 0 0 0 0 0 0 148 164 126 128 3.2 5.0 7.5 3.3 8.8 7.0 9.1 4.6 8.5 6.7 4.1 12.2 0.4 0.1 4.1 0.9 1.0 9.8 3.3 2.0 3.7 7.1 6.2 6.8 5.9 8.2 7.9 3.4 0.0 1.5 3.0 0.2 1.6 0.4 5.4 4.4 5.0 7.3 Electron b 2/b þ mSv h21 GBq21 0.9 11.4 209.3 2.9 23.9 20.1 7.1 0.2 133.6 168.5 4.8 15.0 0.0 0.2 0.0 9.5 2.1 27.4 38.0 7.2 55.0 12.7 44.4 15.8 44.9 2.0 14.3 0.0 0.0 0.0 1402.5 0.6 0.0 10.5 59.9 3.6 46.8 7.7 333.2 658.2 197.6 842.2 71.7 128.5 40.8 5.3 0.0 0.0 531.1 0.4 0.0 1054.9 1.6 1135.7 960.8 1438.5 1378.1 890.1 1087.2 458.1 675.0 86.7 538.5 0.0 89.5 0.0 0.0 1439.2 0.0 1122.1 499.8 1306.9 797.1 817.4 737.9 759.8 Annihilation 2.1 3.5 1.1 5.4 0.2 0.4 0.2 0.0 0.0 0.0 0.9 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 2.0 3.9 0.3 2.9 0.0 0.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.1 5.7 4.3 4.4 T. OTTO Rh Rh Rh 98 Rh 99 Rh 99m Rh 100 Rh 100m Rh 101 Rh 101m Rh 102 Rh 102m Rh 103m Rh 104 Rh 104m Rh 105 Rh 106 Rh 106m Rh 107 Rh 108 Rh 109 Rh 96 Pd 97 Pd 98 Pd 99 Pd 100 Pd 101 Pd 103 Pd 107 Pd 109 Pd 109m Pd 111 Pd 112 Pd 114 Pd 99 Ag 100m Ag 101 Ag 102 Ag 97 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 102m 104 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 120 7 3 66 0 0 24 0 1 0 0 68 0 0 0 735 1 0 2731 112 1635 618 401 2 51 0 9 0 0 0 0 0 0 1 1 0 0 77 4 1203 373 464 1451 15 61 48 27 108 0 0 102 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 134 23 60 0 49 0 0 0 0 0 0 0 0 0 0 0 0 154 128 138 155 60 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 152 108 402 150 120 0 28 454 3 295 14 5 418 5 8 91 12 39 35 59 222 128 213 137 205 77 134 43 40 64 0 0 34 5 150 232 0 188 269 223 164 432 208 156 1 1 1 1 0 0 0 2 0 0 0 0 2 0 0 1 0 0 0 0 2 1 2 0 2 0 1 0 0 0 0 0 0 0 1 2 0 1 2 1 1 1 2 1 1004 104 32 2195 0 0 811 0 501 0 0 3760 2 3 0 4333 1237 110 6844 3392 5676 3862 3173 1 834 0 235 0 0 0 0 0 5 466 567 73 0 1694 874 5147 3317 3324 5170 649 61 48 27 108 0 0 102 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 134 23 60 0 49 0 0 0 0 0 0 0 0 0 0 0 0 154 128 138 155 60 2.9 5.9 10.3 4.5 7.8 0.0 1.8 13.0 0.2 10.7 1.5 0.1 7.7 0.3 0.8 1.8 0.6 2.1 0.8 1.9 4.3 3.2 5.3 6.4 5.3 5.6 4.0 4.6 4.3 5.6 0.0 0.0 1.3 0.1 3.7 3.4 0.0 4.1 4.1 5.6 5.4 9.5 4.1 5.8 2.7 55.7 13.3 5.3 46.6 0.1 1.3 27.6 0.2 18.7 0.0 0.2 8.7 4.9 1.3 2.4 10.7 23.7 1.5 62.8 7.5 60.6 184.7 19.8 72.8 1.2 5.1 0.0 0.0 1099.0 0.0 3.1 3.4 0.1 35.8 4.8 0.0 40.5 5.5 164.9 54.4 25.2 3.7 113.8 369.7 360.8 233.0 628.4 0.0 0.0 674.6 0.0 1211.7 0.0 0.0 998.7 417.6 1437.9 9.1 1009.6 1163.2 467.8 860.9 1065.0 915.7 1027.8 758.7 200.0 398.0 0.0 339.3 3.1 0.0 0.0 752.1 1390.6 1406.5 1241.5 1198.3 1279.4 1319.5 1180.2 1212.1 794.8 711.6 769.2 797.9 389.9 2.1 1.7 0.9 3.7 0.0 0.0 3.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 4.6 0.8 2.1 0.0 1.7 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.3 4.4 4.8 5.3 2.1 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 47 211 104 409 173 109 0 25 458 3 285 11 5 427 5 6 101 12 38 39 70 289 173 247 133 249 68 153 33 30 60 0 0 34 5 162 281 0 228 320 261 181 434 260 179 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ag Ag Ag 104m Ag 105 Ag 105m Ag 106 Ag 106m Ag 108 Ag 108m Ag 109m Ag 110 Ag 110m Ag 111 Ag 111m Ag 112 Ag 113 Ag 113m Ag 114 Ag 115 Ag 116 Ag 117 Ag 101 Cd 102 Cd 103 Cd 104 Cd 105 Cd 107 Cd 109 Cd 111m Cd 113 Cd 113m Cd 115 Cd 115m Cd 117 Cd 117m Cd 118 Cd 119 Cd 119m Cd 103 In 105 In 106 In 106m In 107 In 103 Table 3. Continued 108 109 48 Photon Electron 571 281 113 100 505 148 93 82 14 20 51 0 22 0 37 354 120 21 11 412 128 12 144 19 182 136 312 69 39 21 14 43 16 0 4 1 28 50 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 5 264 1 0 0 32 0 0 8 0 0 1 0 0 0 0 0 0 1807 1 0 18 4 636 3 0 2 0 6 0 0 0 0 0 0 0 0 3 43 94 8 0 0 108 0 0 37 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 34 1 14 0 51 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 553 210 116 102 511 139 99 82 16 23 53 0 25 0 39 320 121 22 11 396 129 12 144 20 186 142 274 74 38 26 17 47 19 0 5 1 28 47 Electron b 2/b þ mSv h21 GBq21 2 2 0 0 0 0 0 0 0 0 0 0 0 0 0 5 0 0 0 4 0 0 0 0 1 0 3 0 0 0 0 0 0 0 0 0 0 0 55 2139 0 0 0 1511 0 0 114 0 0 1283 0 0 0 1 0 350 6476 808 387 2903 2558 5359 15 0 33 0 79 0 0 0 0 0 0 203 51 1998 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 43 94 8 0 0 108 0 0 37 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 34 1 14 0 51 0 0 0 0 0 0 0 0 0 13.1 4.7 6.7 2.7 12.4 3.9 9.3 2.9 1.1 2.4 3.0 0.0 2.0 0.0 2.8 4.7 5.8 1.8 0.1 6.2 3.0 0.5 2.6 1.6 8.2 8.6 6.2 6.1 2.1 2.7 1.7 4.7 2.0 0.0 0.5 0.0 2.8 0.8 Electron b 2/b þ mSv h21 GBq21 68.2 4.1 164.5 76.6 9.8 3.7 415.4 170.3 0.3 1262.1 626.9 0.0 2556.3 0.0 1028.4 9.8 193.9 654.1 0.1 13.9 2.6 76.5 4.6 16.1 90.4 119.1 15.1 87.7 0.5 2.8 0.0 1747.6 0.0 0.0 0.0 0.0 202.9 1.4 331.4 550.0 81.7 0.0 0.4 651.5 0.0 0.0 913.5 0.0 0.0 1145.6 0.0 1280.6 73.3 1430.6 1467.3 646.4 883.4 1222.0 1260.9 980.2 1060.5 924.4 279.1 11.5 106.6 0.0 387.4 0.0 0.0 0.0 0.0 1025.3 257.4 1279.9 1359.6 1086.4 Annihilation 1.5 3.2 0.3 0.0 0.0 3.7 0.0 0.0 1.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.2 0.0 0.5 0.0 1.8 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO In In In 109m In 110 In 110m In 111 In 111m In 112 In 112m In 113m In 114 In 114m In 115 In 115m In 116m In 117 In 117m In 118 In 118m In 119 In 119m In 121 In 121m In 106 Sn 108 Sn 109 Sn 110 Sn 111 Sn 113 Sn 113m Sn 117m Sn 119m Sn 121 Sn 121m Sn 123 Sn 123m Sn 125 Sn 108m Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 125m 127 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 2 0 66 27 0 295 0 552 631 41 629 9 27 2 0 69 0 0 13 0 0 0 1 0 0 0 0 1 0 0 9 0 16 65 9 6 1709 4 142 129 0 10 0 0 0 0 0 0 0 0 0 0 150 116 138 59 92 29 3 128 0 0 72 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 156 27 116 100 1 47 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 61 21 261 91 142 153 170 140 105 104 248 106 221 457 52 13 420 30 17 393 75 35 239 74 0 87 453 258 116 502 312 211 511 417 275 320 159 171 219 266 49 174 22 136 0 0 2 0 0 1 0 1 0 0 4 0 3 4 0 0 4 0 0 3 0 0 2 0 0 0 0 0 0 1 0 1 1 1 2 3 1 1 3 2 0 1 0 0 1442 0 1031 3340 0 4083 39 4567 4659 1879 4098 141 1175 4 0 2629 0 0 312 0 469 0 513 11 0 0 242 887 9 380 2463 375 1441 2694 796 1075 5611 82 2407 2062 0 274 0 0 0 0 0 0 0 0 0 0 150 116 138 58 92 29 3 128 0 0 71 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 156 27 116 100 1 47 0 4 3.4 2.1 5.2 2.9 8.3 3.4 7.7 4.3 4.7 4.2 3.7 4.7 3.7 11.7 5.2 0.7 12.7 3.0 1.5 11.8 2.3 3.5 4.6 2.2 0.0 4.2 11.6 7.3 3.5 12.7 8.3 3.9 13.4 8.5 4.8 4.6 2.5 6.1 4.5 4.9 4.4 4.2 2.3 5.0 50.5 0.0 52.4 11.7 27.5 9.4 269.9 26.7 125.9 16.3 6.0 11.4 1.1 28.0 184.5 0.1 176.4 0.0 0.0 410.1 5.5 0.0 7.2 5.6 0.0 42.9 47.3 27.0 28.7 77.4 76.6 18.3 413.4 247.0 19.6 6.4 3.5 44.3 40.4 3.6 2.1 2.6 0.0 4.6 1139.7 604.5 1289.1 1021.1 1377.8 1009.0 1395.7 983.5 788.6 688.4 740.7 428.5 576.4 243.2 35.9 727.8 2.6 0.0 499.7 0.0 1246.1 0.0 1200.9 346.3 0.0 554.2 1282.7 1018.4 1423.0 1330.7 1032.0 1298.2 1207.9 1066.6 1279.2 1236.1 785.1 199.0 671.7 591.5 10.0 323.4 0.0 39.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.2 4.0 4.8 2.0 3.2 1.0 0.1 4.4 0.0 0.0 2.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.4 0.9 4.0 3.5 0.0 1.6 0.0 0.1 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 49 60 20 282 94 136 157 168 145 105 104 272 104 251 467 48 12 424 24 15 396 74 32 269 73 0 85 449 255 115 501 310 222 520 424 302 379 185 185 235 296 44 195 19 134 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Sn Sn Sn 127m Sn 128 Sn 129 Sn 130 Sn 130m Sn 111 Sb 113 Sb 114 Sb 115 Sb 116 Sb 116m Sb 117 Sb 118 Sb 118m Sb 119 Sb 120 Sb 120m Sb 122 Sb 122m Sb 124 Sb 124m Sb 124 Sbn 125 Sb 126 Sb 126m Sb 127 Sb 128 Sb 128m Sb 129 Sb 130 Sb 130m Sb 131 Sb 133 Sb 113 Te 114 Te 115 Te 115m Te 116 Te 117 Te 118 Te 119 Te 126 Table 3. Continued 119m 121m 50 Photon Electron 241 113 49 0 36 31 1 9 14 12 72 231 57 181 289 152 169 469 72 266 432 66 29 48 143 37 79 13 18 349 21 67 357 63 101 400 66 225 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 0 0 0 0 0 0 1 0 0 4 15 0 2560 284 25 998 192 1 289 0 8 0 0 1 0 0 1 0 0 0 0 1 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 158 137 92 119 121 17 136 0 40 0 2 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 232 117 51 0 38 35 1 11 14 13 72 226 59 166 277 154 163 466 73 209 405 69 29 51 134 42 81 13 20 351 22 68 353 65 101 389 69 201 Electron b 2/b þ mSv h21 GBq21 2 0 0 0 0 0 0 0 0 0 0 1 0 2 1 0 1 2 0 1 1 0 0 0 1 0 0 0 0 1 0 0 1 0 0 2 0 4 0 0 0 0 0 0 0 0 201 176 1014 77 0 1257 298 0 6152 3651 1047 3768 2862 1 3766 0 304 0 7 1359 0 4 373 0 404 24 36 520 56 71 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 158 137 92 119 120 17 136 0 40 0 2 0 0 0 0 0 0 0 0 0 0 0 7.6 5.3 4.4 0.0 3.8 3.5 0.0 1.1 0.8 0.9 3.5 5.7 5.4 4.8 6.5 6.6 3.9 11.5 4.9 4.5 10.0 5.5 1.1 5.0 4.2 4.3 3.4 0.6 2.0 9.1 1.0 3.4 7.4 2.6 3.0 7.2 5.3 2.9 Electron b 2/b þ mSv h21 GBq21 71.1 7.7 233.4 0.0 192.2 1.8 0.7 0.0 4.0 0.3 94.3 662.2 274.9 61.2 259.6 248.2 8.4 43.9 134.6 6.8 18.0 245.0 1.5 191.4 4.3 0.0 13.8 2.6 0.0 28.3 1.7 46.0 19.6 54.2 11.4 27.4 521.3 14.7 5.2 0.0 0.0 0.0 0.0 0.0 1441.3 34.2 1305.0 463.6 1209.3 895.1 338.6 1170.7 1092.5 1366.6 778.3 745.2 573.9 630.0 679.1 155.0 734.8 0.0 271.0 0.0 676.5 1063.7 35.4 1403.2 173.7 1333.1 1323.0 187.9 1355.4 1285.5 24.6 1319.4 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.5 4.7 3.2 4.1 4.2 0.6 4.7 0.0 1.4 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Te Te Te 123 Te 123m Te 125m Te 127 Te 127m Te 129 Te 129m Te 131 Te 131m Te 132 Te 133 Te 133m Te 134 Te 118 I 118m I 119 I 120 I 120m I 121 I 122 I 123 I 124 I 125 I 126 I 128 I 129 I 130 I 130m I 131 I 132 I 132m I 133 I 134 I 134m I 135 I 121 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 120 122 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 49 0 6 0 0 0 0 0 0 0 0 0 1183 7 1671 1088 176 2593 16 729 0 112 0 19 0 0 0 0 0 0 0 0 0 189 61 1256 2644 6 0 32 0 4 0 1 84 0 39 1 0 0 0 0 0 0 0 0 0 0 156 126 123 159 69 141 5 120 0 76 0 0 1 0 0 0 0 0 0 0 0 0 0 36 1 94 0 32 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 98 114 29 75 70 69 41 36 15 19 19 45 75 30 123 45 79 68 33 64 54 85 35 71 17 31 19 132 252 11 0 255 330 0 276 66 31 178 71 106 33 26 33 253 0 1 0 0 0 0 0 0 0 0 0 0 0 0 21 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 2 0 5 1 1 3 0 1 0 0 0 1 0 1646 0 88 0 0 0 0 0 0 0 1 4 5949 1421 5890 4566 2985 6396 593 4581 0 2767 0 677 0 0 0 0 0 0 0 0 1 4047 907 5678 5681 125 0 1503 0 40 0 1 84 0 39 1 0 0 0 0 0 0 0 0 0 0 156 126 123 159 69 141 5 120 0 76 0 0 1 0 0 0 0 0 0 0 0 0 0 36 1 94 0 32 2 6.2 4.1 2.6 4.5 6.0 6.2 4.0 3.6 1.5 1.8 1.8 3.4 2.7 1.0 3.4 2.3 4.4 3.1 1.3 2.9 2.2 4.9 1.6 4.8 1.2 3.0 1.9 4.6 5.9 1.2 0.0 4.6 7.4 0.0 4.3 2.6 0.4 3.0 3.8 4.9 2.0 2.4 2.4 8.8 92.2 63.8 13.4 211.2 292.5 361.7 1538.4 2987.4 1851.3 0.2 2753.5 204.3 257.5 6.0 96.4 101.8 187.7 43.8 12.3 6.4 14.8 32.7 5.6 26.3 0.5 2.3 0.0 5.3 13.2 337.4 0.0 44.9 223.0 0.0 22.9 97.4 0.7 5.1 125.8 103.4 58.4 23.8 55.0 286.7 11.0 484.4 0.0 290.1 6.4 0.0 0.0 0.0 0.0 856.0 0.0 1454.1 7.3 911.0 1201.4 774.1 639.1 684.8 773.4 452.4 737.5 52.3 669.5 0.0 504.1 0.0 0.0 32.1 1032.7 0.0 710.3 0.0 942.1 1370.7 996.8 183.0 925.4 931.5 260.3 12.0 559.8 0.0 247.7 18.5 0.0 2.9 0.0 1.4 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.4 4.4 4.2 5.5 2.4 4.9 0.2 4.1 0.0 2.6 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.3 0.0 3.3 0.0 1.1 0.1 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 51 93 143 27 78 67 67 40 33 14 18 17 45 75 31 155 46 79 68 36 65 55 83 35 68 17 29 17 129 251 10 0 255 333 0 328 70 40 233 71 106 35 25 34 260 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Xe Xe Xe 123 Xe 125 Xe 127 Xe 127m Xe 129m Xe 131m Xe 133 Xe 133m Xe 135 Xe 135m Xe 137 Xe 138 Xe 121 Cs 121m Cs 123 Cs 124 Cs 125 Cs 126 Cs 127 Cs 128 Cs 129 Cs 130 Cs 130m Cs 131 Cs 132 Cs 134 Cs 134m Cs 135 Cs 135m Cs 136 Cs 137 Cs 138 Cs 138m Cs 139 Cs 140 Cs 124 Ba 126 Ba 127 Ba 128 Ba 129 Ba 129m Ba 121 Table 3. Continued 131 133 52 Photon Electron 99 22 92 21 19 98 9 34 148 166 318 70 235 85 234 109 27 16 19 15 16 184 329 4 300 36 90 185 61 48 274 16 150 18 18 41 16 57 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 0 0 2 0 33 0 849 39 617 7 178 2 1 67 0 14 0 0 0 6 370 333 1 62 0 16 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 139 94 123 40 74 11 12 110 0 62 0 0 0 0 0 0 8 84 0 65 8 0 1 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 101 22 95 23 20 100 9 35 142 163 307 69 221 86 204 109 28 16 20 16 17 167 284 3 211 31 91 176 62 49 257 17 151 20 18 42 16 58 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 0 0 0 1 1 2 0 2 0 1 0 0 0 0 0 0 4 7 0 4 1 0 1 0 0 2 0 0 0 0 0 0 0 0 0 0 0 0 0 2005 2 2371 126 4468 1597 3665 154 1761 41 0 2336 0 424 0 0 261 2619 1908 4384 0 1686 0 544 42 0 0 0 0 0 0 56 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 0 0 0 0 0 0 139 94 123 40 74 11 12 110 0 62 0 0 0 0 0 0 8 84 0 64 8 0 1 0 0 0 0 0 6.1 2.1 6.9 2.1 1.8 2.6 0.8 1.8 5.8 4.5 9.1 4.0 6.6 5.1 5.7 4.9 2.2 0.9 1.8 1.2 1.7 2.9 4.9 0.0 3.1 0.5 5.4 6.2 5.5 4.0 8.3 1.7 7.0 1.9 1.6 4.1 1.6 3.6 Electron b 2/b þ mSv h21 GBq21 130.3 0.1 68.3 2225.0 2293.4 119.0 77.4 28.8 326.7 122.5 140.9 80.5 54.1 71.6 25.1 152.9 9.1 0.4 0.5 0.1 0.0 1.7 35.2 0.0 6.3 0.9 176.3 151.2 124.6 2.3 57.4 1.8 165.7 0.6 2570.1 257.7 65.9 81.0 0.0 0.0 0.0 0.0 0.0 0.0 1098.4 1365.8 1101.0 1401.6 722.3 555.6 657.7 289.2 426.7 78.9 109.1 620.6 0.0 409.3 0.0 272.9 1309.1 1062.7 1171.4 997.9 69.6 487.3 0.0 417.9 61.0 0.0 6.6 0.0 0.0 0.0 1210.5 1376.2 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 4.8 3.3 4.3 1.4 2.6 0.4 0.4 3.8 0.0 2.1 0.0 0.0 0.0 0.0 0.0 0.0 0.3 2.9 0.0 2.2 0.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Ba Ba Ba 133m Ba 135m Ba 137m Ba 139 Ba 140 Ba 141 Ba 142 Ba 128 La 129 La 130 La 131 La 132 La 132m La 133 La 134 La 135 La 136 La 137 La 138 La 140 La 141 La 142 La 143 La 130 Ce 131 Ce 132 Ce 133 Ce 133m Ce 134 Ce 135 Ce 137 Ce 137m Ce 139 Ce 141 Ce 143 Ce 131m Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 144 134 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 405 1502 35 142 8 476 7 1 30 2 0 0 104 0 1 817 4 1368 1099 6 324 1 16 0 9 0 0 0 0 0 0 0 1 0 3186 559 407 2927 273 50 838 0 0 0 124 141 87 100 44 131 40 14 89 0 0 0 0 0 0 0 0 0 0 36 116 7 53 0 44 2 0 5 0 0 0 0 0 0 156 114 119 155 116 88 134 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 5 145 379 192 68 216 25 10 360 18 9 6 0 0 3 6 3 130 89 134 155 68 107 57 139 19 37 254 16 19 113 0 30 69 133 33 296 192 39 22 370 33 11 62 0 0 1 2 0 2 0 2 1 0 10 0 0 0 0 0 0 2 1 2 1 0 0 0 1 0 0 1 0 0 5 0 0 0 1 0 0 0 0 0 2 1 0 0 0 670 3558 4992 1478 2400 204 4092 160 1 1435 1748 0 1 3930 0 794 4029 1772 5461 5835 140 3285 0 618 0 271 5 0 0 0 0 0 118 795 3 6524 3381 3612 6397 3320 1823 4605 0 0 0 124 141 87 100 44 131 40 14 89 0 0 0 0 0 0 0 0 0 0 36 116 7 53 0 44 2 0 5 0 0 0 0 0 0 156 114 119 155 116 88 134 0 0.5 5.1 12.0 5.2 3.9 5.8 1.5 0.5 9.4 1.5 0.8 0.1 0.0 0.0 0.0 0.6 0.1 2.7 4.3 3.8 6.2 5.1 6.1 4.0 5.0 1.8 1.8 7.2 1.6 1.6 2.3 0.0 1.9 4.4 4.5 2.5 8.6 9.0 1.6 0.6 8.5 1.1 0.4 2.4 9.7 37.8 229.0 46.3 105.6 16.6 4.0 0.4 357.7 0.6 1.1 0.0 0.0 0.0 0.1 0.0 0.2 12.5 46.1 81.9 134.8 74.1 375.6 21.4 48.7 10.6 8.7 377.5 0.0 0.4 92.6 0.0 10.6 329.9 90.5 35.6 81.3 798.3 12.3 0.3 98.5 10.8 0.1 1.9 590.8 1237.6 662.4 711.1 509.1 555.4 302.3 688.4 284.5 123.8 526.3 1137.4 0.0 1454.3 1001.3 0.5 1208.2 1017.2 1135.7 932.7 915.3 252.2 626.2 66.1 335.8 0.0 297.1 19.3 0.0 45.3 0.0 0.0 1345.3 1347.8 1249.4 1431.6 745.4 608.1 629.8 740.9 624.0 496.7 685.6 0.0 0.0 0.0 4.3 4.9 3.0 3.4 1.5 4.5 1.4 0.5 3.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.2 4.0 0.2 1.8 0.0 1.5 0.1 0.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 5.4 3.9 4.1 5.3 4.0 3.0 4.6 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 53 5 144 389 220 70 239 26 10 361 18 9 8 0 0 4 6 3 147 91 148 156 68 108 57 147 18 37 259 15 19 113 0 30 68 136 31 295 194 41 23 373 37 12 61 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ce Ce Pr 134m Pr 135 Pr 136 Pr 137 Pr 138 Pr 138m Pr 139 Pr 140 Pr 142 Pr 142m Pr 143 Pr 144 Pr 144m Pr 145 Pr 146 Pr 147 Pr 148 Pr 148m Pr 134 Nd 135 Nd 136 Nd 137 Nd 138 Nd 139 Nd 139m Nd 140 Nd 141 Nd 141m Nd 144 Nd 147 Nd 149 Nd 151 Nd 152 Nd 136 Pm 137m Pm 139 Pm 140 Pm 140m Pm 141 Pm 142 Pm 143 Pm 145 Table 3. Continued 144 146 54 Photon Electron 267 15 132 0 85 327 2 220 60 45 238 18 247 271 124 65 137 258 15 15 111 29 0 0 0 0 19 21 23 71 36 407 53 28 194 369 87 365 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 3 0 0 59 0 377 55 1 87 67 501 7 148 41 1 28 0 0 0 0 0 0 0 0 0 5 5175 2102 1221 3155 1 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 119 34 93 57 13 79 0 0 0 0 0 0 0 0 0 0 162 144 129 152 4 8 1 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 270 16 132 0 79 329 2 204 60 42 227 18 201 245 119 63 127 246 15 15 111 29 0 0 0 0 18 21 23 70 30 404 44 22 177 351 87 360 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 1 0 0 2 0 0 2 0 4 6 1 1 2 2 0 0 4 0 0 0 0 0 0 0 0 0 13 2 2 1 2 3 0 2 0 0 0 0 1506 0 4 1671 3 4376 1717 751 1640 1866 3691 185 2267 873 2 1335 2 0 0 0 0 0 0 273 0 1985 7243 5671 4611 6328 10 15 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 0 0 0 0 0 0 0 0 0 0 119 34 93 57 13 79 0 0 0 0 0 0 0 0 0 0 162 144 129 152 4 8 1 0 8.3 1.5 4.5 0.0 1.4 9.3 0.1 4.8 3.5 1.2 7.7 1.6 3.3 6.7 4.8 2.8 4.1 8.0 1.4 0.9 2.3 2.8 0.0 0.0 0.0 0.0 1.7 1.9 2.2 4.1 0.5 8.4 0.9 0.4 4.1 8.1 4.2 10.5 Electron b 2/b þ mSv h21 GBq21 22.8 0.0 17.8 0.0 3.4 67.8 8.0 66.0 74.9 20.9 335.1 13.2 23.4 267.7 169.9 74.4 34.8 578.8 0.0 0.9 107.2 0.0 0.0 0.0 0.0 0.0 0.4 19.0 54.6 106.5 2.5 23.2 0.8 0.1 8.1 16.8 175.6 45.1 0.0 0.0 465.8 255.5 1201.2 1150.2 1420.2 1166.3 1363.9 996.3 1154.7 1213.7 1153.8 1118.4 627.4 233.4 516.1 350.4 107.1 462.3 1.0 0.0 0.0 0.0 0.0 0.0 1431.6 1284.8 1293.0 1121.2 751.3 704.7 654.0 725.4 28.9 60.9 7.0 1.8 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 4.1 1.2 3.2 2.0 0.4 2.7 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 5.6 5.0 4.5 5.2 0.1 0.3 0.0 0.0 T. OTTO Pm Pm Pm 147 Pm 148 Pm 148m Pm 149 Pm 150 Pm 151 Pm 152 Pm 152m Pm 153 Pm 154 Pm 154m Pm 139 Sm 140 Sm 141 Sm 141m Sm 142 Sm 143 Sm 143m Sm 145 Sm 146 Sm 147 Sm 148 Sm 151 Sm 153 Sm 155 Sm 156 Sm 157 Sm 142 Eu 142m Eu 143 Eu 144 Eu 145 Eu 146 Eu 147 Eu 148 Eu 145 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 149 150m 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 1 0 41 2 209 898 70 27 70 0 0 0 0 0 0 0 0 0 0 1613 14 17 481 18 2 9 84 4 0 0 26 0 0 2 0 0 0 1 0 0 0 0 0 0 0 0 0 0 92 121 79 56 8 0 0 0 0 0 0 0 0 0 0 127 48 55 93 51 12 40 38 24 2 0 34 2 0 4 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 21 266 8 182 49 17 187 19 14 150 58 184 60 75 210 48 199 106 65 234 0 102 0 22 0 32 11 73 325 268 186 231 462 185 188 244 404 173 16 170 137 67 239 43 0 1 0 1 0 0 1 0 0 3 0 2 0 1 3 1 8 1 0 1 0 0 0 0 0 0 0 0 19 4 11 3 1 2 1 5 0 1 0 3 0 0 6 0 0 0 2 18 640 0 89 0 0 799 31 1902 1838 2426 4040 1858 851 284 0 0 0 0 0 0 0 0 1 2 4760 557 720 2758 620 56 295 840 65 1 0 620 3 0 61 0 0 0 1 0 0 0 0 0 0 0 0 0 0 92 121 79 56 8 0 0 0 0 0 0 0 0 0 0 127 48 55 93 51 12 40 38 24 2 0 34 2 0 4 0 1.9 10.4 0.4 5.3 1.4 1.7 4.2 1.9 1.3 2.4 3.2 3.3 3.2 2.6 7.2 1.5 3.0 2.6 6.3 8.8 0.0 6.0 0.0 2.1 0.0 3.1 0.8 3.3 4.3 5.8 2.8 4.6 12.0 6.0 4.7 5.4 12.9 8.3 0.9 5.5 7.6 4.5 5.0 4.0 19.2 118.8 5.7 81.4 10.2 0.0 82.8 0.0 0.3 7.3 22.3 16.8 22.8 58.2 310.7 25.4 6.0 155.0 103.6 531.1 0.0 304.9 0.0 118.1 0.0 0.2 3.3 18.5 12.2 19.3 1.9 8.8 72.2 177.7 36.6 12.2 84.1 340.9 7.0 114.1 1589.3 86.8 46.6 109.5 0.0 0.4 1287.3 351.7 861.1 0.0 1065.3 0.0 92.0 1029.1 1403.0 1144.9 1125.1 501.7 625.1 438.6 337.3 38.4 0.0 1.7 0.0 0.1 0.0 0.0 0.0 0.0 1439.9 1448.5 631.7 299.1 333.1 499.0 313.2 89.7 263.2 223.0 172.2 17.8 2.4 204.1 17.5 1.7 28.6 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 3.2 4.2 2.7 1.9 0.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 4.4 1.6 1.9 3.2 1.8 0.4 1.4 1.3 0.8 0.1 0.0 1.2 0.1 0.0 0.2 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 55 21 267 8 189 49 17 193 20 14 174 58 194 60 81 224 63 272 105 65 236 0 101 0 22 0 32 11 73 391 287 222 263 463 201 189 303 401 175 16 194 137 67 309 44 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Eu Eu Eu 152 Eu 152m Eu 152 Eun 154 Eu 154m Eu 155 Eu 156 Eu 157 Eu 158 Eu 159 Eu 142 Gd 143m Gd 144 Gd 145 Gd 145m Gd 146 Gd 147 Gd 148 Gd 149 Gd 150 Gd 151 Gd 152 Gd 153 Gd 159 Gd 162 Gd 146 Tb 147 Tb 147m Tb 148 Tb 148m Tb 149 Tb 149m Tb 150 Tb 150m Tb 151 Tb 151m Tb 152 Tb 152m Tb 153 Tb 154 Tb 155 Tb 150 Table 3. Continued 156 156 56 Photon Electron 308 12 1 2 134 175 15 181 137 376 121 118 236 53 213 58 152 0 113 69 17 5 4 12 92 71 170 104 101 197 340 74 253 101 80 276 24 27 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 0 0 0 0 0 34 24 1 3 0 1 0 0 0 0 0 0 0 0 0 1 0 3086 54 90 687 51 8 196 1 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 7 14 0 5 0 2 0 2 0 0 0 0 0 0 0 142 72 85 111 72 34 75 10 0 1 0 7 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 294 12 1 2 133 173 16 181 137 354 110 119 214 53 202 58 147 0 110 69 17 5 4 12 93 71 170 103 100 190 340 69 227 101 80 276 25 26 Electron b 2/b þ mSv h21 GBq21 5 0 0 0 0 1 0 0 0 5 1 0 3 0 1 0 1 0 1 0 0 0 0 0 0 0 0 1 0 2 2 0 3 0 0 0 0 1 0 0 0 0 0 5 0 117 15 1326 2085 0 105 0 15 0 0 0 0 0 0 50 0 0 757 29 5937 1555 2038 3645 1458 282 1898 7 0 0 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 0 0 0 0 0 0 0 7 14 0 5 0 2 0 2 0 0 0 0 0 0 0 142 72 85 111 72 34 75 10 0 1 0 7 9.0 1.2 0.1 0.2 3.9 4.1 1.6 6.1 6.1 9.5 1.8 4.1 5.4 2.9 5.8 4.7 6.9 0.0 5.3 4.7 1.6 0.3 0.3 1.1 4.4 3.7 3.6 4.7 5.1 6.4 13.0 3.9 7.6 6.0 6.1 7.2 2.5 1.7 Electron b 2/b þ mSv h21 GBq21 302.6 0.0 0.0 0.0 65.5 53.7 0.3 94.4 97.5 257.0 8.5 4.6 50.6 9.7 95.4 72.4 155.3 0.0 93.5 30.8 0.0 7.4 4.9 0.3 744.1 393.1 7.6 233.5 198.3 145.3 252.1 109.5 449.5 229.8 166.9 122.8 2.8 2.9 0.0 0.0 0.0 0.0 241.4 1360.3 1268.3 1330.2 1431.7 1191.7 1138.9 58.6 100.7 1.1 39.9 0.0 21.4 0.0 22.5 0.0 0.0 1345.1 32.5 1050.8 1217.9 1411.8 676.1 405.6 469.1 577.9 410.8 219.7 418.2 76.0 4.8 8.9 0.0 57.7 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.2 0.5 0.0 0.2 0.0 0.1 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 4.9 2.5 2.9 3.8 2.5 1.2 2.6 0.3 0.0 0.0 0.0 0.2 T. OTTO Tb Tb Tbn 157 Tb 158 Tb 160 Tb 161 Tb 162 Tb 163 Tb 164 Tb 165 Tb 148 Dy 149 Dy 150 Dy 151 Dy 152 Dy 153 Dy 154 Dy 155 Dy 157 Dy 159 Dy 165 Dy 165m Dy 166 Dy 167 Dy 168 Dy 150 Ho 153 Ho 153m Ho 154 Ho 154m Ho 155 Ho 156 Ho 157 Ho 159 Ho 160 Ho 161 Ho 162 Ho 156m Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 162m 164 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 2 0 10 0 0 1 0 0 0 0 0 0 0 1 7 234 0 106 0 1 0 0 0 0 1 0 0 0 153 0 14 0 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 5 0 9 0 0 0 0 0 0 0 0 25 62 1 74 0 2 0 0 0 0 0 0 0 0 0 0 41 0 12 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 93 0 10 15 5 270 66 138 2 269 22 23 141 160 13 12 18 0 69 92 140 161 173 192 45 103 252 33 210 1 0 61 69 291 173 250 49 73 15 51 24 59 74 7 1 0 0 0 0 0 0 1 0 1 0 0 1 2 0 0 0 0 0 0 0 2 5 3 3 0 8 0 0 0 0 3 0 1 1 6 0 1 0 0 0 0 0 0 0 0 1 0 844 2 0 1364 0 1192 0 0 11 0 0 0 0 0 11 0 770 263 1671 0 1909 0 19 0 0 1 0 583 3 18 237 2168 0 631 0 23 0 0 0 0 0 0 0 0 0 0 0 0 0 0 5 0 9 0 0 0 0 0 0 0 0 25 62 1 74 0 2 0 0 0 0 0 0 0 0 0 0 41 0 12 0 1 0 0 3.9 0.0 0.9 1.5 0.3 9.2 4.0 3.1 0.2 7.4 2.2 2.1 4.7 4.5 1.3 1.2 1.7 0.0 4.8 4.0 6.4 6.9 3.7 6.1 1.4 5.7 5.9 3.0 7.7 0.1 0.0 1.0 3.2 11.7 4.7 7.3 3.8 2.5 1.3 3.2 2.4 5.5 6.9 0.4 202.4 0.0 0.0 0.0 0.0 554.4 348.1 44.5 0.0 227.3 0.0 11.9 423.5 475.7 0.1 0.0 1737.3 0.0 72.2 57.3 145.3 139.5 40.4 180.8 9.4 388.7 127.4 1737.4 200.2 0.0 0.0 18.5 58.1 688.1 329.8 544.1 23.7 25.7 2.8 18.8 0.0 28.2 510.7 8.9 0.2 0.0 579.5 0.0 1200.5 99.6 1133.3 1158.4 0.0 1185.7 43.7 0.0 67.5 0.9 0.0 0.0 0.0 843.5 1411.4 782.9 1244.8 158.3 339.3 9.4 402.3 0.1 15.2 0.0 0.1 1443.8 0.0 1111.4 1450.4 1393.0 1326.3 1151.7 3.6 241.8 0.0 90.6 0.0 9.3 0.0 1063.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.2 0.0 0.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.9 2.1 0.0 2.5 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.4 0.0 0.4 0.0 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 57 95 0 10 16 5 269 66 140 2 271 21 22 148 163 13 13 19 0 69 92 140 184 214 207 53 104 289 33 211 1 0 68 68 291 175 285 50 79 15 53 25 60 75 7 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ho Ho Ho 164m Ho 166 Ho 166m Ho 167 Ho 168 Ho 168m Ho 170 Ho 154 Er 156 Er 159 Er 161 Er 163 Er 165 Er 167m Er 169 Er 171 Er 172 Er 173 Er 161 Tm 162 Tm 163 Tm 164 Tm 165 Tm 166 Tm 167 Tm 168 Tm 170 Tm 171 Tm 172 Tm 173 Tm 174 Tm 175 Tm 176 Tm 162 Yb 163 Yb 164 Yb 165 Yb 166 Yb 167 Yb 169 Yb 175 Yb 163 Table 3. Continued 177 179 58 Photon Electron 31 7 163 137 242 202 0 341 117 0 306 0 42 24 16 87 3 7 184 19 189 5 229 98 43 91 82 31 76 0 67 412 392 168 178 94 43 159 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 1 24 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 2 3 61 5 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 45 10 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 66 24 0 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 31 7 164 126 208 188 1 262 120 1 298 0 42 23 17 88 4 7 186 17 190 5 219 99 44 92 83 34 77 0 68 416 395 169 179 94 44 160 Electron b 2/b þ mSv h21 GBq21 1 0 0 2 6 4 0 10 0 0 4 0 0 0 0 0 0 0 0 1 0 0 8 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 85 0 695 841 82 0 0 7 0 0 0 0 0 0 0 0 46 0 0 1256 4 122 418 1262 1546 168 0 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 45 10 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 66 24 0 0 0 0 0 0 0 0 0 0 0 0 1.2 0.4 5.5 5.3 6.2 5.2 0.2 4.6 4.8 0.3 7.5 0.1 3.7 1.5 2.0 6.9 0.4 0.6 14.1 0.5 12.2 0.5 5.6 4.4 3.2 4.4 5.3 3.9 6.3 0.0 4.7 29.2 21.3 11.1 10.9 4.8 3.4 8.1 Electron b 2/b þ mSv h21 GBq21 46.5 20.4 285.6 219.0 217.0 77.2 0.0 28.0 7.2 0.0 211.1 0.0 27.8 0.1 18.2 687.1 0.0 19.7 1041.0 8.1 775.3 20.8 222.8 336.8 35.2 12.7 73.2 13.3 107.4 0.0 230.0 4498.8 1451.2 949.9 694.6 326.4 331.9 628.2 1177.2 1304.9 1257.2 265.7 68.2 2.3 0.0 3.8 0.1 0.0 0.6 0.0 0.0 0.4 0.0 1363.6 1362.8 1078.4 11.8 1169.6 1423.3 1328.7 1279.9 1178.0 366.4 156.4 0.0 0.0 0.2 0.0 0.0 0.0 0.0 0.0 0.6 1061.7 0.0 682.5 Annihilation 0.0 0.0 0.0 1.6 0.4 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 2.3 0.8 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Yb Yb Yb 165 Lu 167 Lu 169 Lu 169m Lu 170 Lu 171 Lu 171m Lu 172 Lu 172m Lu 173 Lu 174 Lu 174m Lu 176 Lu 176m Lu 177 Lu 177m Lu 178 Lu 178m Lu 179 Lu 180 Lu 181 Lu 167 Hf 169 Hf 170 Hf 172 Hf 173 Hf 174 Hf 175 Hf 177m Hf 178m Hf 179m Hf 180m Hf 181 Hf 182 Hf 182m Hf 178 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 183 170 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1960 105 4 44 0 0 0 0 0 0 0 0 0 0 0 1 123 0 0 0 0 0 0 0 0 0 0 208 0 5 0 0 1 0 0 0 0 0 0 1 0 0 0 0 124 60 18 51 1 2 0 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 62 2 18 0 0 3 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 128 47 56 195 76 96 159 261 17 22 213 7 13 190 53 59 262 30 238 158 5 18 13 11 0 7 78 0 39 141 164 174 139 281 177 36 147 73 5 18 0 11 25 12 1 0 0 37 1 4 4 22 0 3 0 0 0 6 0 0 1 0 1 2 0 0 0 0 0 0 0 0 0 2 2 1 1 7 6 0 0 0 0 0 0 0 0 0 87 3 4946 1402 128 1157 0 14 0 0 0 0 0 1 0 0 15 666 2609 0 0 0 0 0 0 0 20 0 1 1804 0 160 0 0 15 0 0 0 3 0 0 1320 0 1 0 0 124 60 18 51 1 2 0 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 62 2 18 0 0 3 0 0 0 0 0 0 0 0 0 3.8 4.3 2.5 6.0 4.0 4.7 6.1 5.4 1.7 1.8 14.2 0.9 1.4 4.8 5.5 5.3 10.4 2.9 9.9 7.9 0.6 2.0 1.3 1.2 0.0 1.1 3.3 0.0 6.0 4.9 7.1 4.7 6.6 12.3 5.2 3.8 4.3 5.7 0.7 5.3 0.0 0.9 4.8 1.3 41.3 325.4 99.0 338.9 176.0 400.3 201.4 73.8 3.1 1.3 823.6 0.0 0.0 85.5 2545.7 643.6 468.9 357.5 229.0 176.5 0.0 0.2 2560.1 0.2 0.0 532.3 52.6 5.7 889.8 253.5 180.0 12.3 673.9 791.4 31.4 232.6 21.6 168.2 80.8 0.0 0.0 184.5 7.8 130.0 1359.6 1425.3 600.2 330.4 121.5 285.4 6.5 10.8 0.0 20.6 0.0 0.0 198.3 990.1 0.0 1370.3 1392.2 1229.0 1079.1 4.3 0.0 0.0 0.0 0.0 1110.7 0.0 1370.9 836.9 1444.5 330.4 17.2 117.6 0.1 0.0 20.6 0.0 0.0 0.0 1318.9 0.0 0.0 1155.5 0.0 1423.8 0.0 0.0 4.3 2.1 0.6 1.8 0.0 0.1 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 2.1 0.1 0.6 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 59 129 45 56 206 80 105 173 311 16 22 212 7 12 196 52 58 261 29 238 158 4 17 12 10 0 5 76 0 32 180 174 175 139 289 186 34 146 67 4 5 0 10 16 10 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Hf Hf Ta 172 Ta 173 Ta 174 Ta 175 Ta 176 Ta 177 Ta 178 Ta 178m Ta 179 Ta 180 Ta 182 Ta 182m Ta 183 Ta 184 Ta 185 Ta 186 Ta 177 W 178 W 179 W 179m W 181 W 185 W 185m W 187 W 188 W 190 W 178 Re 179 Re 180 Re 181 Re 182 Re 182m Re 183 Re 184 Re 184m Re 186 Re 186m Re 187 Re 188 Re 188m Re 189 Re 184 Table 3. Continued 190 180 60 Photon Electron 223 157 29 214 79 114 155 116 0 0 271 18 2 13 2 15 166 143 169 279 126 252 180 59 287 18 253 0 14 17 142 1 2 0 15 395 14 67 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 1 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1194 816 4 36 0 2 4 0 0 0 0 0 0 0 0 0 0 0 2 0 0 0 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 102 92 15 30 4 10 11 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 224 162 40 212 87 123 157 123 0 3 280 30 5 15 6 16 173 148 161 272 125 243 170 70 232 28 262 3 21 29 145 9 19 3 15 402 22 74 Electron b 2/b þ mSv h21 GBq21 1 0 0 4 0 0 4 0 0 0 0 0 0 0 0 0 0 0 4 4 2 6 2 0 13 0 0 0 0 0 0 0 0 0 2 0 0 0 637 459 0 5 0 0 0 0 0 0 0 0 0 6 0 9 3842 3286 139 611 3 82 139 0 1 0 0 0 0 0 0 0 0 0 1608 0 2 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 4 0 0 0 0 0 0 0 0 0 0 0 0 102 92 15 30 4 10 11 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 9.3 8.3 6.0 10.5 7.7 10.3 5.4 5.7 0.0 0.8 14.0 5.4 1.4 1.6 1.5 1.3 8.7 8.5 9.0 12.6 9.6 12.1 6.6 6.4 7.8 5.1 13.7 0.7 3.6 5.3 7.9 2.4 5.1 0.9 0.7 16.2 3.7 5.5 Electron b 2/b þ mSv h21 GBq21 493.0 314.7 44.8 222.0 108.2 106.8 350.0 23.7 0.0 0.0 675.5 70.5 0.0 64.4 0.0 40.9 443.1 309.0 281.4 384.9 261.3 554.4 230.1 71.1 367.3 51.6 565.7 0.0 154.4 63.4 389.6 0.0 2328.7 0.0 33.1 347.5 38.8 337.8 1233.7 673.8 1.1 29.4 0.0 4.5 0.0 0.0 0.0 0.0 0.0 5.5 0.0 1405.5 0.0 1406.2 505.5 462.4 93.6 176.4 32.6 65.7 68.7 0.7 4.3 0.0 0.0 0.0 0.0 0.0 1240.1 0.2 0.0 0.0 1138.9 118.5 1433.9 1139.3 Annihilation 0.0 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 3.5 3.2 0.5 1.0 0.1 0.3 0.4 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Re Re Os 181 Os 182 Os 183 Os 183m Os 185 Os 186 Os 189m Os 190m Os 191 Os 191m Os 193 Os 194 Os 196 Os 180 Ir 182 Ir 183 Ir 184 Ir 185 Ir 186 Ir 186m Ir 187 Ir 188 Ir 189 Ir 190 Ir 190m Ir 190 Irn 191m Ir 192 Ir 192m Ir 192 Irn 193m Ir 194 Ir 194m Ir 195 Ir 195m Ir 190m Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 196 184 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 160 0 0 0 2 0 0 0 0 0 0 0 0 0 0 0 1 1052 5 32 0 3 0 0 0 0 0 0 0 0 0 0 1 0 0 66 0 1 0 0 0 0 0 0 0 0 0 0 10 0 1 0 0 0 0 0 0 0 0 0 0 90 13 23 0 9 0 0 3 0 0 0 0 0 0 0 0 0 0 0 0 5 0 1 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 38 428 155 128 112 52 100 0 71 6 8 34 12 32 35 19 0 154 142 228 118 217 44 47 147 33 49 94 75 71 115 22 40 343 7 26 54 238 68 136 163 7 51 57 51 1 0 0 1 0 1 0 0 0 0 0 0 0 0 0 0 4 3 6 0 13 0 0 13 0 0 0 0 0 0 0 4 0 0 1 0 3 0 4 5 0 0 0 3585 1 0 0 63 0 0 0 0 0 0 0 0 0 352 0 725 3332 194 547 0 141 0 0 4 0 0 0 0 1 0 0 1405 0 37 3185 0 34 0 0 0 0 0 0 0 0 0 0 10 0 1 0 0 0 0 0 0 0 0 0 0 89 13 23 0 9 0 0 3 0 0 0 0 0 0 0 0 0 0 0 0 5 0 1 1 0 0 0 1.3 18.0 15.1 7.3 9.4 6.8 8.9 0.0 7.9 1.6 1.6 6.2 2.0 5.2 1.7 2.8 0.0 7.8 6.9 8.7 8.9 8.1 5.7 5.6 7.1 5.7 5.8 7.2 11.1 3.2 12.8 2.8 1.0 15.3 0.4 0.6 7.4 12.0 8.2 7.7 6.9 1.6 5.7 7.1 43.7 268.5 702.6 178.2 403.8 294.7 161.2 0.0 137.2 0.0 733.0 413.2 27.7 1928.0 133.7 142.4 0.0 633.9 230.4 283.4 446.7 209.5 242.9 918.1 156.7 4.7 945.6 163.2 3209.3 77.9 1554.3 718.8 25.6 855.1 14.7 12.6 116.6 1093.5 194.3 274.5 157.4 0.0 52.8 525.1 1031.1 1232.3 2.8 0.0 71.4 0.0 5.8 0.0 0.0 0.0 0.0 0.0 1377.1 47.1 1302.9 1235.2 1220.4 444.8 81.8 132.0 3.2 53.9 0.0 0.0 22.6 0.0 0.0 33.4 0.0 1431.8 0.0 577.6 1168.8 1084.5 1364.4 1055.2 0.3 37.3 0.0 12.1 7.7 0.0 1.3 0.3 0.0 0.0 0.0 0.0 0.4 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 3.1 0.5 0.8 0.0 0.3 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 61 38 419 134 118 99 41 87 0 58 1 3 19 6 18 34 13 0 156 148 300 106 264 35 37 156 20 38 86 51 70 101 19 42 336 6 27 42 237 55 132 162 1 38 40 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ir Ir Pt 186 Pt 187 Pt 188 Pt 189 Pt 190 Pt 191 Pt 193 Pt 193m Pt 195m Pt 197 Pt 197m Pt 199 Pt 200 Pt 202 Pt 186 Au 187 Au 190 Au 191 Au 192 Au 193 Au 193m Au 194 Au 195 Au 195m Au 196 Au 196m Au 198 Au 198m Au 199 Au 200 Au 200m Au 201 Au 202 Au 190 Hg 191m Hg 192 Hg 193 Hg 193m Hg 194 Hg 195 Hg 195m Hg 196m Table 3. Continued 197 199m 62 Photon Electron 18 21 36 43 1 22 376 111 334 99 391 180 258 76 292 208 48 208 22 85 0 0 398 0 420 314 405 172 258 91 226 196 82 157 44 130 62 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 19 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 0 0 16 2374 610 423 17 0 18 0 0 0 0 0 0 0 0 0 0 0 0 1 736 0 9 0 2 1 0 1 0 0 0 0 0 0 0 0 0 0 0 108 73 58 29 2 22 2 1 2 0 1 0 0 0 0 0 0 0 0 0 1 21 1 7 4 0 5 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 31 32 46 46 1 24 327 113 339 104 402 170 231 83 260 227 58 209 32 92 0 0 409 0 275 280 370 182 288 111 220 221 102 161 69 147 70 11 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 0 34 2 3 0 0 14 14 3 21 0 0 13 0 0 0 2 10 0 85 20 13 5 2 0 12 2 0 9 0 2 0 0 0 0 0 0 262 34 830 4503 2566 1967 570 7 443 0 10 1 0 0 0 0 0 267 0 148 413 753 3295 1 338 0 87 34 0 24 0 0 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 0 0 0 0 0 0 0 108 73 58 29 2 22 2 1 2 0 1 0 0 0 0 0 0 0 0 0 1 21 1 7 4 0 5 0 0 0 0 5.1 4.6 5.5 3.9 0.1 1.9 7.7 4.8 11.6 5.3 15.8 7.5 7.7 5.6 8.3 13.5 5.7 8.3 4.7 6.1 0.1 0.0 17.4 0.0 5.6 8.0 10.6 11.8 18.3 11.7 10.3 15.8 11.4 9.3 11.3 11.0 4.0 3.6 Electron b 2/b þ mSv h21 GBq21 4.8 2438.3 2541.3 556.6 12.0 352.0 590.6 70.9 219.6 61.8 398.4 220.4 78.4 184.0 98.8 2008.2 485.1 142.7 112.5 58.8 0.0 0.9 1492.1 0.1 204.3 59.7 278.2 484.6 468.6 991.1 176.6 2419.4 693.2 175.2 884.8 375.8 566.0 0.0 0.0 0.0 0.0 194.2 1291.3 1388.6 1223.5 511.4 371.9 298.4 166.5 16.1 124.7 14.9 9.6 13.4 0.6 5.3 0.0 0.0 1336.3 1289.9 0.0 1319.1 1281.7 1218.5 1068.7 8.1 126.4 5.2 44.3 24.9 0.0 31.6 0.0 1.3 0.0 0.0 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 3.7 2.5 2.0 1.0 0.1 0.7 0.1 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.7 0.0 0.2 0.1 0.0 0.2 0.0 0.0 0.0 0.0 T. OTTO Hg Hg Hg 203 Hg 205 Hg 206 Hg 207 Hg 190 Tl 190m Tl 194 Tl 194m Tl 195 Tl 196 Tl 197 Tl 198 Tl 198m Tl 199 Tl 200 Tl 201 Tl 202 Tl 204 Tl 206 Tl 206m Tl 207 Tl 208 Tl 209 Tl 210 Tl 194 Pb 195m Pb 196 Pb 197 Pb 197m Pb 198 Pb 199 Pb 200 Pb 201 Pb 201m Pb 202 Pb 197m Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 202m 204m 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 5 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 28 18 1 6 0 0 0 0 0 0 0 0 0 1 0 0 43 1 304 4 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 32 24 4 13 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 12 0 4 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 331 78 331 11 0 15 11 35 53 240 398 251 431 325 457 235 514 254 170 0 50 9 19 0 23 183 46 127 252 240 251 235 218 0 1 0 1 0 6 0 0 0 0 0 2 0 0 0 0 0 0 0 0 9 1 8 3 15 8 18 5 51 21 0 0 0 1 0 0 45 1 0 5 1 6 2 2 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 98 0 0 691 499 30 197 1 0 0 0 0 0 13 0 0 960 259 94 1015 719 4348 156 0 12 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 32 24 4 13 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 12 0 4 0 1 0 0 0 0 0 0 0 0 0 0 0 10.4 9.9 8.2 3.6 0.0 3.3 0.4 4.2 4.6 10.2 18.5 9.9 16.0 11.3 16.2 9.7 18.7 10.8 6.2 0.0 4.0 0.6 1.4 0.0 1.1 3.1 2.9 4.8 11.3 18.5 10.4 15.7 9.5 0.0 0.1 0.0 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 345.0 563.9 216.3 0.0 0.0 0.0 17.9 1084.3 762.4 93.5 474.8 100.8 441.2 222.9 352.4 95.7 618.3 119.5 1.7 0.0 562.1 77.6 8.6 0.0 95.8 33.7 667.2 124.0 968.7 826.3 174.8 751.5 154.3 0.0 11.0 0.0 0.3 0.0 0.6 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1390.2 0.0 1325.0 808.2 1377.0 180.6 136.0 27.7 82.0 3.6 3.2 2.4 0.0 0.7 0.0 1394.8 0.0 3.7 739.4 1292.5 1325.3 1251.8 1241.1 989.2 76.1 0.0 28.7 0.0 8.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1.1 0.8 0.1 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.4 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 63 322 61 328 1 0 4 11 28 46 233 378 255 423 348 453 247 514 243 305 0 47 8 16 0 22 210 43 126 242 200 243 202 204 0 1 0 1 0 10 0 0 0 0 0 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Pb Pb Pb 205 Pb 209 Pb 210 Pb 211 Pb 212 Pb 214 Pb 197 Bi 200 Bi 201 Bi 202 Bi 203 Bi 204 Bi 205 Bi 206 Bi 207 Bi 208 Bi 210 Bi 210m Bi 211 Bi 212 Bi 212 Bin 213 Bi 214 Bi 215 Bi 216 Bi 203 Po 204 Po 205 Po 206 Po 207 Po 208 Po 209 Po 210 Po 211 Po 212 Po 212m Po 213 Po 214 Po 215 Po 216 Po 218 Po 203 Table 3. Continued 204 206 64 Photon Electron 349 160 374 307 473 377 438 10 0 1 0 0 0 80 144 182 11 294 0 0 0 0 0 10 0 0 62 173 1 3 6 37 19 88 82 31 1 10 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 161 74 81 1 2 0 0 0 0 0 0 0 0 232 29 3 0 0 0 0 0 0 0 0 0 0 1 3 0 0 0 1 0 12 1 0 0 0 42 26 32 3 6 0 0 0 0 0 0 0 0 0 23 10 0 0 0 0 0 0 0 0 0 0 0 8 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 365 170 383 305 478 402 425 18 0 1 0 0 0 84 156 186 12 302 0 0 0 0 0 11 0 0 76 187 1 8 7 49 31 89 94 36 1 21 Electron b 2/b þ mSv h21 GBq21 1 3 2 12 6 3 18 0 0 0 0 0 0 0 0 2 0 7 0 0 0 0 0 0 0 0 1 9 0 0 0 0 0 10 1 0 0 0 1288 649 888 32 65 0 0 0 0 0 0 3 0 3841 551 144 0 0 0 0 0 0 0 0 0 0 442 134 0 0 0 680 5 1869 1114 0 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation Photon 42 26 32 3 6 0 0 0 0 0 0 0 0 0 23 10 0 0 0 0 0 0 0 0 0 0 0 8 0 0 0 0 0 0 0 0 0 0 14.8 8.8 15.0 12.5 17.9 18.0 14.9 3.1 0.0 0.1 0.0 0.0 0.0 5.7 8.3 9.1 0.8 10.7 0.0 0.0 0.0 0.0 0.0 0.8 0.0 0.0 5.6 10.1 0.0 1.3 0.7 5.4 4.2 4.5 6.7 2.9 0.0 3.3 Electron b 2/b þ mSv h21 GBq21 269.2 292.1 335.5 883.8 1029.5 339.0 552.0 0.2 0.2 4.7 1.3 0.0 0.0 625.0 273.5 305.0 43.1 269.6 0.0 0.0 0.0 0.0 0.0 75.1 0.0 0.0 96.7 456.9 3.1 18.9 95.0 46.7 97.7 84.9 272.4 673.3 0.7 317.3 223.6 142.3 171.5 19.6 35.0 1.2 1.1 0.0 0.0 0.0 0.0 1.0 0.0 919.1 127.4 62.7 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 1275.7 48.2 0.0 4.9 0.0 1232.0 1406.1 1152.7 1194.3 0.0 0.0 0.0 Annihilation 1.5 0.9 1.1 0.1 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.8 0.4 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.3 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO At At At 207 At 208 At 209 At 210 At 211 At 215 At 216 At 217 At 218 At 219 At 220 At 207 Rn 209 Rn 210 Rn 211 Rn 212 Rn 215 Rn 216 Rn 217 Rn 218 Rn 219 Rn 220 Rn 222 Rn 223 Rn 212 Fr 219 Fr 220 Fr 221 Fr 222 Fr 223 Fr 224 Fr 227 Fr 219 Ra 220 Ra 221 Ra 205 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 222 224 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 36 0 107 3 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 2 0 10 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 2 40 2 15 2 57 10 22 9 73 15 36 2 150 77 91 141 85 35 6 6 57 6 66 5 47 5 12 8 9 10 19 262 36 142 40 175 69 280 3 0 137 99 41 0 0 0 0 0 0 0 0 0 0 0 0 0 5 10 0 28 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 7 0 0 0 0 0 9 0 0 12 0 0 0 0 0 0 0 32 0 0 0 0 0 2 0 192 2284 308 2314 1669 0 0 0 0 0 0 0 0 0 25 0 844 5 0 0 0 0 0 1 0 2 1648 121 1382 496 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0.1 4.9 0.2 2.0 0.2 6.3 1.3 2.3 1.3 9.2 2.4 4.2 0.4 6.2 2.8 8.0 4.0 2.9 5.0 0.7 0.9 7.5 1.0 10.0 0.8 6.8 0.8 1.2 1.1 0.3 0.9 2.7 15.0 4.9 8.6 5.8 7.4 7.1 14.0 0.1 0.0 5.0 2.3 4.8 7.7 604.0 29.5 0.0 57.8 353.9 0.0 173.1 21.5 47.4 12.0 42.1 0.0 106.0 28.6 588.2 9.9 16.0 149.4 204.4 3.9 308.6 2.9 192.0 1.1 6.2 0.4 26.0 0.0 34.2 41.2 0.1 247.3 0.2 50.9 101.9 57.7 1427.3 786.6 7.0 0.0 165.2 40.6 921.4 0.0 0.0 0.0 729.3 0.0 1384.4 0.0 1224.3 0.0 0.0 0.0 1183.7 0.0 1307.8 1133.4 1286.9 1117.6 1135.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 512.0 0.0 1371.7 85.0 1214.6 1404.4 0.0 1.1 0.0 101.6 0.0 691.5 276.2 1192.6 1136.5 1330.0 1202.9 1278.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 65 2 29 2 9 1 37 4 17 5 51 6 28 1 141 81 80 162 85 20 5 3 34 2 32 2 21 2 9 4 9 7 9 232 20 119 19 159 50 252 3 0 140 98 28 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Ra Ra Ra 225 Ra 226 Ra 227 Ra 228 Ra 230 Ra 223 Ac 224 Ac 225 Ac 226 Ac 227 Ac 228 Ac 230 Ac 231 Ac 232 Ac 233 Ac 223 Th 224 Th 226 Th 227 Th 228 Th 229 Th 230 Th 231 Th 232 Th 233 Th 234 Th 235 Th 236 Th 227 Pa 228 Pa 229 Pa 230 Pa 231 Pa 232 Pa 233 Pa 234 Pa 234m Pa 235 Pa 236 Pa 237 Pa 227 U 223 Table 3. Continued 228 231 66 Photon Electron 3 3 41 3 1 2 36 0 2 42 2 14 8 8 211 25 171 8 58 15 20 97 46 190 59 11 39 168 18 21 30 3 20 3 1 3 0 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 14 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 7 7 82 7 4 6 47 0 6 63 5 18 17 9 238 39 172 20 103 24 41 107 64 218 67 16 37 196 29 34 48 7 35 6 3 6 0 5 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 0 0 0 0 0 0 0 0 0 2 0 41 0 0 0 0 1 0 1 1 0 3 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 21 0 16 1 0 0 0 0 0 0 13 0 31 885 37 2291 304 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(0.07)slab in 10 cm Annihilation 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 0.9 1.1 11.6 1.1 0.5 1.0 5.5 0.0 0.9 7.7 0.7 2.0 2.4 0.7 13.1 4.9 7.6 3.0 13.5 3.0 5.6 3.9 7.1 11.8 3.6 1.9 0.9 10.5 3.6 4.2 5.9 1.0 4.6 0.9 0.4 0.9 0.0 0.7 Electron b 2/b þ mSv h21 GBq21 7.0 4.0 1.2 0.6 0.8 0.1 95.2 0.0 0.0 562.8 0.0 2.7 13.9 31.3 374.1 32.4 44.7 0.0 1302.2 2.7 17.6 9.4 934.2 632.2 17.2 122.7 2.5 938.8 0.0 0.0 0.8 0.0 0.0 0.0 0.1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 347.8 0.0 1379.1 816.1 1384.3 1.6 0.0 0.8 0.0 10.9 607.1 0.0 799.3 941.7 1419.5 1222.9 1373.3 1107.2 1289.7 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO U U U 232 U 233 U 234 U 235 U 35m U 236 U 237 U 238 U 239 U 240 U 242 U 232 Np 233 Np 234 Np 235 Np 236 Np 236m Np 237 Np 238 Np 239 Np 240 Np 240m Np 241 Np 242 Np 242m Np 232 Pu 234 Pu 235 Pu 236 Pu 237 Pu 238 Pu 239 Pu 240 Pu 241 Pu 242 Pu 230 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Nuclides 243 245 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 8 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 429 0 5254 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 251 0 20661 0 0 0 0 0 0 0 0 0 0 0 0 0 12 7 76 52 101 170 98 205 28 19 14 23 179 9 11 193 160 39 36 75 6 136 6 51 5 50 4 56 152 3 1504 22 80 178 37 22 0 145 41 5 4 64 4 69 0 0 0 0 0 7 0 1 0 0 0 0 1 1 0 0 3 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 0 0 0 2 0 0 0 0 0 0 0 41 2 0 0 0 0 0 0 0 0 0 0 200 1 18 232 114 0 0 0 0 0 0 0 0 5 0 2401 1 28229 92 0 0 0 0 0 58 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1.4 0.7 3.9 5.9 9.2 8.4 11.4 9.8 3.7 2.3 1.9 2.8 9.6 1.0 1.2 13.7 4.3 4.0 4.3 8.3 0.9 11.1 0.8 5.8 0.7 6.1 0.5 2.8 4.0 0.1 35.5 1.1 8.7 9.2 3.6 2.3 0.0 3.4 4.7 0.7 0.5 7.5 0.6 4.5 13.8 0.0 1003.0 389.2 448.6 35.1 1054.3 14.0 0.1 0.0 0.8 0.1 814.4 10.5 185.2 2114.4 88.1 775.7 0.2 72.5 0.2 500.0 0.1 899.0 0.0 364.9 0.0 129.8 0.1 11.5 0.0 135.1 820.6 7.0 753.2 1.2 0.0 13.7 390.3 0.0 0.1 60.8 0.0 138.2 1258.0 8.4 1141.7 61.6 0.0 2.0 0.0 0.0 0.0 1131.7 0.0 0.0 949.4 1304.1 1416.7 1385.6 1334.5 1335.6 0.0 0.9 0.0 0.0 0.0 0.0 0.0 0.0 1.6 0.0 560.0 1401.1 5265.0 1350.4 0.0 0.0 0.0 955.5 0.2 1395.9 1431.2 0.0 0.0 0.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 Continued Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 67 8 4 71 39 80 154 67 179 16 10 7 17 153 6 8 157 155 31 25 59 3 109 3 35 2 32 2 55 180 3 1813 20 60 156 31 16 0 141 28 3 2 40 2 63 PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES Pu Pu Pu 246 Pu 237 Am 238 Am 239 Am 240 Am 241 Am 242 Am 242m Am 243 Am 244 Am 244m Am 245 Am 246 Am 246m Am 247 Am 238 Cm 239 Cm 240 Cm 241 Cm 242 Cm 243 Cm 244 Cm 245 Cm 246 Cm 247 Cm 248 Cm 249 Cm 250 Cm 251 Cm 245 Bk 246 Bk 247 Bk 248m Bk 249 Bk 250 Bk 251 Bk 244 Cf 246 Cf 247 Cf 248 Cf 249 Cf 244 Nuclides 250 68 Photon Electron 3 35 64 6 2294 0 85 265 100 36 1 22 85 0 4 40 2 31 3 20 1698 43 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 b 2/b þ Annihilation mSv h21 GBq21 2 0 128 0 5926 0 0 0 0 0 0 0 2 0 1 0 0 0 1 0 2965 8 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 Contribution to Hp(3)slab in 100 cm Neutron Photon 0 0 42 0 44883 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 38920 0 4 48 55 10 1905 0 99 323 112 55 1 43 93 0 7 51 4 48 4 38 1415 58 Electron b 2/b þ mSv h21 GBq21 0 0 0 0 0 0 1 0 3 0 0 0 0 0 0 0 0 0 0 0 0 0 13 0 736 0 32505 0 0 0 0 0 0 0 12 1 434 0 0 0 7 0 17843 49 Contribution to Hp(0.07)slab in 10 cm Annihilation 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 Photon 0.5 5.5 1.7 1.3 45.0 0.0 7.3 23.7 6.2 6.5 0.2 5.5 3.8 0.0 0.8 4.9 0.4 5.6 0.5 4.8 33.7 6.3 Electron b 2/b þ mSv h21 GBq21 0.1 1599.4 0.0 0.0 0.0 0.0 150.3 1092.1 13.7 151.0 1.2 2.6 34.8 0.0 0.0 58.9 0.0 85.7 0.0 1.7 0.0 630.8 4.5 0.0 197.7 432.2 6854.2 1404.4 0.1 0.0 4.8 0.0 0.0 0.0 1195.2 510.5 1268.2 0.2 0.1 0.0 3.3 0.0 5598.7 13.4 Annihilation 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 T. OTTO Cf Cf 252 Cf 253 Cf 254 Cf 255 Cf 249 Es 250 Es 250m Es 251 Es 253 Es 254 Es 254m Es 255 Es 256 Es 251 Fm 252 Fm 253 Fm 254 Fm 255 Fm 256 Fm 257 Fm 251 Contribution to Hp(10) in 100 cm Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Table 3. Continued PERSONAL DOSE COEFFICIENTS FOR RADIONUCLIDES per gigabecquerels in 1-m distance for depths of 3 and 10 mm and in millisievert per hour per gigabecquerels in 10-cm distance for a depth of 0.07 mm. Photons and neutrons are only little affected by absorption and scattering in air. Their contribution to personal dose, as well as the ‘shielded’ personal dose equivalent, can be scaled to other distances r than the reference distance ro ¼ 1 m or 10 cm by multiplying with r2/ro2. For the electron/positron component, scaled results would be affected by a large uncertainty, with a tendency of underestimation for smaller distances. In this work, the conversion coefficients from activity to personal dose equivalent for .1200 radionuclides have been calculated including full secondary electron transport. Therefore, a comparison with the results of the previous compilation(2), where photon dose has been calculated in the kerma approximation, is possible only for the dose from electrons and positrons. For most radionuclides in (2), the photon component calculated in the kerma approximation is 100 times larger than the component simply because of the geometrical factor. Figure 7 shows the statistical distribution of the differences between the conversion coefficient for personal dose in 0.07-mm depth from electrons and positrons, from (2) and from the present work, evaluated for the same radionuclide. It can be seen that the present work delivers slightly higher dose estimates than the previous work. For photons in a depth of 10 mm, where the difference between kerma approximation and electron transport does not play a large role for most photon energies in radioactive decay, the results should also not differ by a large margin. Figure 8 shows a comparison between the conversion coefficients for personal dose in 10-mmdepth photons from (2) and from the present work. ‘Outliers’ in the tails of the two graphs can be traced back to improvement of knowledge of the relevant nuclear decay schemes in the quarter-century between 1983 and 2008, the years in which the respective data sets were published by the ICRP. Figure 7. Comparison of the results for hpA; Z ð0:07Þe; slab for electrons and positrons between the 820 radionuclides in the previous evaluation(2) and the present work. The bin width is 25 mSv. A small tendency of the present work to deliver higher personal dose estimates is discernible. Figure 8. Comparison of the results for hpA; Z ð10Þg for photons between the 820 radionuclides in the previous evaluation(2) and the present work. The bin width is 5 mSv. A small tendency of the present work to deliver higher personal dose estimates is discernible. SUMMARY The purpose of this publication is to enlarge and to update the available set of dose conversion coefficients for radionuclides. It is based on the ICRP’s latest publication of nuclear decay data for radiation protection purposes and on modern calculations of fluence-to-personal dose conversion coefficients for photons and electrons. With respect to previously calculated conversion coefficients, the present work - - replaces the kerma approximation for photons by full transport of charged secondary particles, resulting in more realistic estimates for Hp(0.07)slab, includes the (small) difference between electrons and positrons in the calculations and presents an approximation for ‘shielded’ and ‘unshielded’ radioactive sources. Comparison with the previously published conversion coefficients shows a globally very good agreement. The data from this publication will be useful to make rapid estimates of the external radiation hazard when handling or being involuntarily exposed to sealed or unsealed sources of radionuclides. for the first time lists conversion coefficients for .400 mostly short-lived radionuclides, 69 Downloaded from https://academic.oup.com/rpd/article/168/1/1/2380124 by guest on 22 June 2023 Comparison with previous work T. OTTO REFERENCES 1. 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