1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
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1 1 Decay Scheme I- disintegrates by electron capture mainly via the 159 level of Te- (97%). L iode se désintègre par capture électronique principalement vers le niveau excité de 159 du tellure, avec une probabilité de 97%. 2 Nuclear Data T 1/2 ( I ) : 13,2234 (37) h T 1/2 ( Te ) : a Q ( I ) : 4 (3) 2.1 Electron Capture Transitions Probability Nature lg ft P K P L P M 100 ɛ 0,13 165,8 (30) 0,0079 (4) Allowed 7,59 0,8082 (21) 0,1503 (15) 0,0336 (7) ɛ 0,12 197,4 (30) 0,0025 (9) Allowed 8,27 0,8182 (18) 0,1427 (13) 0,0316 (6) ɛ 0,11 237,9 (30) 0,0035 (3) 1st Forbidden 8,31 0,8266 (16) 0,1363 (12) 0,0300 (6) ɛ 0,10 339,3 (30) 0,0744 (13) Allowed 7,32 0,8377 (15) 0,1283 (11) 0,0278 (5) ɛ 0,9 450,4 (30) 0,1461 (20) Allowed 7,29 0,8436 (14) 0,7 (10) 0,0267 (5) ɛ 0,8 464,7 (30) 0,0037 (6) Allowed 8,92 0,8441 (14) 0,3 (10) 0,0266 (5) ɛ 0,7 536,5 (30) 0,419 (13) Allowed 6,98 0,8464 (14) 0,1216 (10) 0,0262 (5) ɛ 0,6 546 (3) 1,40 (12) Allowed 6,49 0,8466 (14) 0,1214 (10) 0,0261 (5) ɛ 0,4 728,7 (30) 0,349 (42) Allowed 7,35 0,8501 (14) 0,1187 (10) 0,0254 (5) ɛ 0,3 744,3 (30) 0,0025 (10) Allowed 9,52 0,8503 (14) 0,1186 (10) 0,0254 (5) ɛ 0,2 794 (3) 0,419 (5) Allowed 7,35 0,8510 (14) 0,1181 (10) 0,0253 (5) ɛ 0, (3) 97,18 (32) Allowed 5,26 0,8533 (14) 0,1163 (10) 0,0248 (5) LNHB /V. Chisté, M.M. Bé 1 02/03/01 5/8/2004
2 2.2 Gamma Transitions and Internal Conversion Coefficients P γce Multipolarity α K α L α T 100 γ 1,0(Te) 158,99 (5) 99,22 (30) M1 1,22%E2 0,1648 (16) 0,02160 (22) 0,1918 (19) γ 13,10(Te) 174,2 (3) 0,00099 (30) M1 50% E2 0,159 (32) 0,029 (12) 0,195 (47) γ 6,4(Te) 182,61 (8) 0,021 (6) M1 50% E2 0,138 (24) 0,024 (10) 0,168 (38) γ 7,4(Te) 192,18 (9) 0,0227 (10) M1 50% E2 0,118 (20) 0,020 (8) 0,143 (30) γ 10,7(Te) 197,22 (11) 0,00037 (19) M1 50% E2 0,109 (18) 0,018 (7) 0,132 (26) γ 6,3(Te) 198,25 (12) 0,0040 (8) M1 50% E2 0,107 (17) 0,018 (7) 0,130 (26) γ 10,6(Te) 206,79 (10) 0,0037 (9) M1 50% E2 0,094 (14) 0,016 (5) 0,114 (21) γ 7,3(Te) 207,82 (13) 0,00125 (36) M1 50% E2 0,093 (14) 0,015 (5) 0,119 (20) γ 6,2(Te) 247,96 (8) 0,0743 (25) M1 50% E2 0,054 (5) 0,0084 (21) 0,065 (8) γ 7,2(Te) 257,52 (9) 0,0017 (2) E2 0,0526 (16) 0,00917 (27) 0,0640 (19) γ 9,4(Te) 278,26 (8) 0,0024 (4) M1 50% E2 0,0387 (22) 0,0058 (11) 0,0459 (36) γ 2,1(Te) 281,03 (7) 0,0822 (10) M1 13,2% E2 0,0362 (20) 0,0048 (11) 0,0422 (33) γ 10,5(Te) 295,17 (21) 0, (4) γ 8,2(Te) 329,38 (18) 0,0026 (6) γ 3,1(Te) 330,71 (11) 0,01197 (34) E2 0,0237 (7) 0,00376 (11) 0,0284 (9) γ 9,2(Te) 343,73 (8) 0,0044 (3) γ 4,1(Te) 346,35 (7) 0,1287 (9) M1 0,49% E2 0,02080 (14) 0,00262 (29) 0,02407 (23) γ 10,3(Te) 405,04 (14) 0,00298 (23) γ 12,5(Te) 437,5 (3) 0,0007 (7) γ 2,0(Te) 440,02 (5) 0,4280 (44) M1 81,5% E2 0,0103 (7) 0, (18) 0,0121 (7) γ 10,2(Te) 454,76 (15) 0,00412 (22) γ 4,0(Te) 505,34 (6) 0,268 (42) M1 1% E2 0,0081 (7) 0, (27) 0,0093 (7) γ 6,1(Te) 528,96 (7) 1,28 (12) γ 7,1(Te) 538,54 (8) 0,393 (13) E2 50% M3 0,032 (26) 0,0049 (41) 0,038 (31) γ 11,2(Te) 556,06 (16) 0,0029 (3) γ 13,4(Te) 562,84 (12) 0,00115 (7) γ 13,3(Te) 578,48 (20) 0,00126 (8) γ 5,0(Te) 599,69 (16) 0,00266 (17) γ 8,1(Te) 610,27 (23) 0,0011 (3) γ 9,1(Te) 624,61 (7) 0,0802 (20) M1 62,8% E2 0,0042 (5) 0, (40) 0,0049 (6) γ 13,2(Te) 628,26 (22) 0,00164 (14) γ 6,0(Te) 687,95 (10) 0,0269 (6) γ 10,1(Te) 735,78 (9) 0,0616 (8) γ 9,0(Te) 783,62 (6) 0,0591 (11) γ 11,1(Te) 837,1 (2) 0, (8) γ 12,1(Te) 877,65 (17) 0,00083 (7) γ 10,0(Te) 894,8 (2) 0,00101 (7) γ 13,1(Te) 909,19 (12) 0,00141 (8) γ 12,0(Te) 1036,64 (17) 0,00097 (7) γ 13,0(Te) 1068,18 (15) 0,00142 (7) 3 Atomic Data 3.1 Te ω K : 0,875 (4) ω L : 0,0862 (35) n KL : 0,917 (4) LNHB /V. Chisté, M.M. Bé 2 02/03/01 5/8/2004
3 3.1.1 X Radiations Relative probability K Kα 2 27,202 53,7 Kα 1 27, Kβ 3 30,9446 } Kβ 1 30,996 } Kβ 5 31,236 } 28,6 Kβ 5 31,241 } Kβ 2 31,7008 } Kβ 4 31,774 } 6,2 KO 2,3 31,812 } L Ll 3,336 Lα 3,76 3,77 Lη 3,606 Lβ 4,02 4,37 Lγ 4,44 4, Auger Electrons Relative probability Auger K KLL 21,804 22, KLX 25,814 27,470 45,3 KXY 29,80 31,81 5,13 Auger L 2,3 4,8 LNHB /V. Chisté, M.M. Bé 3 02/03/01 5/8/2004
4 4 Electron Emissions Electrons per 100 disint. e AL (Te) 2,3-4,8 95,3 (6) e AK (Te) 12,4 (4) KLL 21,804-22,989 } KLX 25,814-27,470 } KXY 29,80-31,81 } ec 1,0 K (Te) 127,176 (5) 13,72 (14) ec 1,0 L (Te) 154, ,649 1,798 (19) 5 Photon Emissions 5.1 X-Ray Emissions Photons per 100 disint. XL (Te) 3,336 4,82 9,0 (4) XKα 2 (Te) 27,202 24,69 (20) } Kα XKα 1 (Te) 27, ,98 (29) } XKβ 3 (Te) 30,9446 } XKβ 1 (Te) 30,996 } 13,16 (17) K β 1 XKβ 5 (Te) 31,236 } XKβ 5 (Te) 31,241 } XKβ 2 (Te) 31,7008 } XKβ 4 (Te) 31,774 } 2,86 (8) K β 2 XKO 2,3 (Te) 31,812 } 5.2 Gamma Emissions Photons per 100 disint. γ 1,0 (Te) 158,97 (5) 83,25 (21) γ 13,10 (Te) 174,2 (3) 0,00083 (25) LNHB /V. Chisté, M.M. Bé 4 02/03/01 5/8/2004
5 Photons per 100 disint. γ 6,4 (Te) 182,61 (6) 0,018 (5) γ 7,4 (Te) 192,17 (7) 0,0199 (7) γ 10,7 (Te) 197,22 0,00033 (17) γ 6,3 (Te) 198,23 0,0035 (7) γ 10,6 (Te) 206,79 0,0033 (8) γ 7,3 (Te) 207,8 0,00112 (32) γ 6,2 (Te) 247,96 (5) 0,0698 (23) γ 7,2 (Te) 257,51 (15) 0,0016 (2) γ 9,4 (Te) 278,36 (12) 0,0023 (4) γ 2,1 (Te) 281,03 (5) 0,0789 (9) γ 10,5 (Te) 295,17 0, (4) γ 8,2 (Te) 329,38 (17) 0,0026 (6) γ 3,1 (Te) 330,70 (8) 0,01164 (33) γ 9,2 (Te) 343,73 (14) 0,0044 (3) γ 4,1 (Te) 346,35 (5) 0,1257 (9) γ 10,3 (Te) 405,02 (13) 0,00298 (23) γ 12,5 (Te) 437,5 (3) 0,0007 (7) γ 2,0 (Te) 440,02 (5) 0,4229 (43) γ 10,2 (Te) 454,76 (15) 0,00412 (22) γ 4,0 (Te) 505,33 (5) 0,266 (42) γ 6,1 (Te) 528,96 (5) 1,28 (12) γ 7,1 (Te) 538,54 (5) 0,3788 (43) γ 11,2 (Te) 556,05 (13) 0,0029 (3) γ 13,4 (Te) 562,79 (12) 0,00115 (7) γ 13,3 (Te) 578,26 (20) 0,00126 (8) γ 5,0 (Te) 599,69 (16) 0,00266 (17) γ 8,1 (Te) 610,05 (23) 0,0011 (3) γ 9,1 (Te) 624,57 (5) 0,0798 (20) γ 13,2 (Te) 628,26 (22) 0,00164 (14) γ 6,0 (Te) 687,95 (10) 0,0269 (6) γ 10,1 (Te) 735,78 (7) 0,0616 (8) γ 9,0 (Te) 783,59 (6) 0,0591 (11) γ 11,1 (Te) 837,1 (2) 0, (8) γ 12,1 (Te) 877,52 (17) 0,00083 (7) γ 10,0 (Te) 894,8 (2) 0,00101 (7) γ 13,1 (Te) 909,12 (12) 0,00141 (8) γ 12,0 (Te) 1036,63 (17) 0,00097 (7) γ 13,0 (Te) 1068,12 (15) 0,00142 (7) LNHB /V. Chisté, M.M. Bé 5 02/03/01 5/8/2004
6 6 Main Production Modes Sb 121(α,2n)I Possible impurities : I 121, I 124, I 125, I 126 I 127(p,5n)Xe Te 124(p,2n)I Possible impurities : I 124, I 126, I 125 Te (p,n)i Possible impurities : I 124, I 126, I 130, I 125 Te 122(α,3n)Xe Possible impurities : I 125 Te (He 3,3n)Xe Possible impurities : I 125 Te 124(He 3,4n)Xe Possible impurities : I 125 Te 122(d,n)I Possible impurities : I 124, I 126, I 131, I References - R. K. Gupta. Nucl. Phys. 14 (1960) 606 (Gamma-ray Emission, emission probabilities) - G. Anderson, G. Rudstam, G. Sorensen. Ark. Fys. 28 (1964) 3 - Y. Y. Chu, O. C. Kistner, A. C. Li, S. Monaro, M. L. Perlman. Phys. Rev. 133 (1964) B1316 (E2/M1 ratios) - Y. Y. Chu, M. L. Perlman. Phys. Rev. 135 (1964) B319 (internal conversion coefficients) - E. N. Hatch, G. W. Eakins, G. C. Nelson, R. E. Mcadams. Proc. Inter. Conf. : Internal Conversion Process (1965) (Internal Conversion Coefficient) - H. Sergole, G. Albouy, J. Bouloume, J. M. Lagrange, L. Marcus, M.Pautrat. J. Phys. (Paris) 28 (1967) 383 (Gamma-ray Emissions) - G. G. Jonsson, B. Forkman. Nucl. Phys. A 107 (1968) 52 - H. B. Hupf, J. S. Eldridge, J. E. Breaver. Int. J. Appl. Radiat. Isotop. 19 (1968) 345 (Half-Life) - R. C. Ragaini, W. B. Walters, G. E. Gordon, P. A. Baedecker. Nucl. Phys. A 115 (1968) 611 (Gamma-ray Emissions) - B. V. Narasimha Rao, Swani Jnanananda. Phys. Rev. 165 (1968) 1296 (E2 transitions) - H. Sergole, G. Albouy, M. Jourdain, J. M. Lagrange, N. Poffe, M.Pautrat. J. Phys. (Paris) C1 (1968) 187 (Gamma-ray Emissions) - H. Sergole, J. Vanhorenbeeck. Nucl. Phys. A 139 (1969) 554 (Gamma-ray emissions, angular correlactions) - E. H. Spejewski, P. K. Hopke, F. W. Loeser Jr. Nucl. Phys. A 146 (1970) 182 (Gamma ray energy and intensity) - H. Schrader, R. Stippler, F. Munich. Nucl. Phys. A 151 (1970) 331 (Gamma-ray emission, emission probabilities) LNHB /V. Chisté, M.M. Bé 6 02/03/01 5/8/2004
7 - A. Hogleend, S. G. Malmstog, F. Munich, H. Schrader. Nucl. Phys. A 165 (1971) 513 (M1 and E2 transitions) - R. Stippler, D. Code, H. Schrader, F. Munich. Z. Phys. 242 (1971) 121 (Gamma-ray emission, K-shell conversion coefficient) - H. C. Cheung, S. K. Mark. Nucl. Phys. A 176 (1971) S. Raman. Nucl. Instrum. Methods 103 (1972) 407 (Internal Conversion Coefficient) - H. M. A. Karim. Radiochim. Acta 19 (1973) 1 - V. J. Sodd, J. W. Blue, K. L. Scholz, M. C. Oselka. Int. J. Appl. Radiat. Isotop. 24 (1973) 171 (Gamma ray energy and intensity) - W. N. Roney, D. W. Gebbie, R. R. Borchers. Nucl. Phys. A236 (1974) 165 (Mixing of different multipolarities) - W. B. Walters, R. A. Meyer. Phys. Rev. C14 (1976) 1925 (Gamma-ray energy and intensity) - D. B. Fossan, et al. Phys. Rev. C15 (1977) 1732 (Gamma-ray transitions, spin and parity) - U. Hagemann, H.-J. Keller, H.-F. Brinckman. Nucl. Phys. A289 (1977) 292 (Gamma-ray energy and intensity) - K. S. Krane. At. Data. Nucl. Data Tables 19 (1977) 363 (E2, M1 multipole mixing ratios) - E. Schoeters, J. Geenen, C. Nuytten, L. Vanneste. Nucl. Phys. A323 (1979) 1 (J, mixing of different multipolarities) - R. E. Shroy, et al. Phys. Rev. C26 (1982) 1089 (Gamma-ray emission probabilities) - F. Lagoutine, J. Legrand. Int. J. Appl. Radiat. Isotop. 33 (1982) R. Jacquemin. Int. J. Appl. Radiat. Isotop. 38 (1987) M. P. Unterweger, D. D. Hoppes, F. J. Schima. Nucl. Instrum. Methods A312 (1992) S. Ohya, T. Tamura. Nucl. Data Sheets 70 (1993) 531 (Spin, Parity) - R. Goswani, B. Sethi, P. Barnerjee, P. K. Chattopadhyay. Phys. Rev. C47 (1993) 1013 (Gamma-ray energy) - E. Schönfeld, H. Janssen. Nucl. Instrum. Methods A369 (1996) 527 (Atomic data) - M. A. L. da Silva, M. C. M. de Almeida, C. J. da Silva, J. U. Delgado. Appl. Rad. Isotopes 60 (2004) H. Schrader. Appl. Rad. Isotopes 60 (2004) 317 LNHB /V. Chisté, M.M. Bé 7 02/03/01 5/8/2004
8 BNM - LNHB/CEA - Table de Radionucléides I γ Emission probabilities per 100 disintegrations 0 ε I /2 ; 0 13,2234 (37) h 43 fs ,00 0,00 0,00 0,00 0,00 0, ,00 0,00 0, ,00 0,00 3/2,5/2 ; 1068,18 3/2,5/2 ; 1036,64 - (5/2) ; 996,06 0,0079 0,0025 0, fs ,00 0,00 0,00 0,00 0,00 0,06 0,00 3/2,5/2 ; 894,74 0, fs ,00 0,00 0,07 0, ,00 0,00 3/2,5/2 ; 783,6 769,26 7/2 ; 697,52 3/2 ; 687,95 0,1461 0,0037 0,419 1,4 5 1/2 ; 599,57 13,5 ps 30,7 ns 22 ps (5/2) ; 505,34 (7/2) ; 489,7 3/2 ; 440 0,349 0,0025 0,419 97, ps 1 3/2 ; 158,99 12 (0) x10^12 a 0 Te Q = 4 % ε = 100 1/2 ; 0 BNM-LNHB/CEA \ V. Chisté, M.M. Bé Page number : 1/2 02/03/ /07/2003
9 BNM - LNHB/CEA - Table de Radionucléides γ Emission probabilities per 100 disintegrations 0 ε I /2 ; 0 13,2234 (37) h I ,01 0,00 0,00 0,37 0,01 0,00 0,06 1,28 0,02 7/2 ; 697,52 3/2 ; 687,95 0,419 1,4 5 0, /2 ; 599,57 13,5 ps 30,7 ns ,12 0, ,01 (5/2) ; 505,34 (7/2) ; 489,7 0,349 0, ps ,07 0,42 3/2 ; 440 0, ps ,2 3/2 ; 158,99 97,18 12 (0) x10^12 a 0 Te Q = 4 1/2 ; 0 % ε = 100 BNM-LNHB/CEA \ V. Chisté, M.M. Bé Page number : 2/2 02/03/ /07/2003
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