1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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- Πορφύριος Ποσειδώνιος Αλεξίου
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1 1 Decay Scheme Se disintegrates 100% by electron capture to excited levels and to the ground state of As. Le Se se désintègre à 100% par capture électronique vers des niveaux excités et le niveau fondamental de As. 2 Nuclear Data T 1/2 ( Se ) : 119,781 (24) d Q ( Se ) : 863,6 (8) 2.1 Electron Capture Transitions Probability Nature lg ft P K P L P M 100 ɛ 0,9 42,0 (8) 0,00734 (18) 1st Forbidden 7,9 0,8038 (32) 0,1633 (26) 0,0300 (8) ɛ 0,8 245,9 (8) 0,0126 (6) 1st Forbidden 8,8 0,8724 (16) 0,1071 (13) 0,0186 (4) ɛ 0,7 291,4 (8) 0,03484 (35) 1st Forbidden 9,1 0,8740 (16) 0,1058 (13) 0,0184 (4) ɛ 0,6 395,0 (8) 0,00036 (5) 1st Forbidden 11,1 0,8762 (16) 0,1041 (13) 0,0180 (4) ɛ 0,5 462,9 (8) 94,5 (21) Allowed 6,1 0,8770 (16) 0,1033 (13) 0,0179 (4) ɛ 0,3 584,1 (8) 2,1 (14) 1st Forbidden 8 0,8781 (15) 0,1025 (13) 0,0177 (4) ɛ 0,2 598,9 (8) 1,4 (2) 1st Forbidden 8,2 0,8782 (15) 0,1024 (13) 0,0177 (4) ɛ 0,0 863,6 (8) 1,42 (22) 1st Forbidden 8,5 0,8794 (15) 0,1014 (12) 0,01 (4) 2.2 Gamma Transitions and Internal Conversion Coefficients P γce Multipolarity α K α L α M α T 100 γ 3,2(As) 14,8847 (13) 0,0206 (6) M1 (E2) γ 4,3(As) 24,3815 (14) 5,5 (13) M2 165,4 (240) 32,6 (5) 5,13 (10) 204 (3) γ 2,1(As) 66,0518 (8) 1,44 (6) M1 1,44% E2 0,29 (3) 0,034 (5) 0,0052 (7) 0,33 (3) CEA/LNE LNHB /V. Chisté, M. M. Bé 1 08/07/ /8/2013
2 P γce Multipolarity α K α L α M α T 100 γ 3,1(As) 80,9365 (15) 0,0259 (15) [E2] 1,486 (21) 0,216 (3) 0,0326 (5) 1,736 (25) γ 5,4(As) 96,7340 (9) 6,35 (14) E2 0,772 (11) 0,1044 (15) 0,01576 (22) 0,893 (13) γ 5,3(As) 121,1155 (11) 17,56 (37) E1 0,0372 (6) 0,00388 (6) 0, (9) 0,0417 (6) γ 5,2(As) 136,0001 (6) 59,2 (21) E1 0,0263 (4) 0,00274 (4) 0, (6) 0,0295 (5) γ 1,0(As) 198,6060 (12) 1,48 (6) M1 9,03% E2 0,0167 (9) 0,00182 (11) 0, (16) 0,0189 (11) γ 9,7(As) 249,3 (3) 0,00400 (13) [M1,E2] 0,015 (9) 0,0017 (10) 0,00026 (15) 0,017 (10) γ 2,0(As) 264,6576 (9) 59,17 (19) M1E2 0,00646 (25) 0,00068 (3) 0, (5) 0,0072 (3) γ 3,0(As) 279,5422 (10) 25,11 (9) M1 25,04 % E2 0,0081 (4) 0,00087 (4) 0, (6) 0,0091 (4) γ 4,0(As) 303,9236 (10) 1,378 (5) E3 0,0469 (7) 0,00592 (9) 0, (13) 0,0538 (8) γ 7,1(As) 373,61 (24) 0,00258 (11) [E2] 0,00580 (9) 0, (9) 0, (14) 0,00653 (10) γ 5,0(As) 400,6572 (8) 11,403 (43) E1 0, (17) 0, (18) 0, (3) 0, (19) γ 8,1(As) 419,1 (4) 0,0121 (6) [M1,E2] 0,003 (1) 0,00032 (11) 0, (16) 0,0034 (11) γ 6,0(As) 468,6 (4) 0,00036 (5) [M1,E2] 0,0022 (6) 0,00023 (7) 0, (10) 0,0025 (7) γ 9,3(As) 542,02 (18) 0, (6) [M1,E2] 0,0015 (3) 0,00015 (4) 0, (6) 0,0016 (4) γ 9,2(As) 556,90 (18) 0,00277 (12) [E2] 0, (25) 0, (3) 0, (4) 0,00183 (3) γ 7,0(As) 572,22 (24) 0,03626 (31) M1 3,48 % E2 0, (15) 0, (16) 0, (24) 0, (17) γ 8,0(As) 617,8 (4) 0,00453 (5) [M1,E2] 0,00103 (18) 0, (20) 0, (3) 0,00116 (20) γ 9,0(As) 821,56 (18) 0, (8) [E2] 0, (8) 0, (9) 0, (13) 0, (9) 3 Atomic Data 3.1 As ω K : 0,5 (4) ω L : 0,0155 (5) n KL : 1,232 (4) X Radiations Relative probability K Kα 2 10, ,53 Kα 1 10, Kβ 3 11,7204 } Kβ 1 11,7263 } Kβ 5 11,821 } 22,87 Kβ 2 11,8643 } Kβ 4 } 0,86 L Ll 1,1195 Lα 1,2816 1,2824 Lη 1,1552 Lβ 1,3152 1,4892 Lγ 1,3508 1,5312 CEA/LNE LNHB /V. Chisté, M. M. Bé 2 08/07/ /8/2013
3 3.1.2 Auger Electrons Relative probability Auger K KLL 8, 9, KLX 10,12 10,54 31 KXY 11,44 11,80 2,4 Auger L 1,1 1,3 4 Electron Emissions Electrons per 100 disint. e AL (As) 1,1 1,3 119,6 (15) e AK (As) 41,4 (14) KLL 8, 9,10 } KLX 10,12 10,54 } KXY 11,44 11,80 } ec 4,3 K (As) 12,5148 (14) 4,5 (12) ec 4,3 L (As) 22, ,0584 0,88 (20) ec 4,3 M (As) 24, ,3403 0,139 (31) ec 2,1 K (As) 54,1851 (8) 0,305 (32) ec 2,1 L (As) 64, ,7287 0,036 (5) ec 3,1 K (As) 69,0698 (15) 0,0141 (8) ec 5,4 K (As) 84,8673 (9) 2,59 (7) ec 5,4 L (As) 95,208 95,411 0,350 (9) ec 5,4 M (As) 96,530 96,693 0,0528 (13) ec 5,3 K (As) 109,2488 (11) 0,627 (17) ec 5,3 L (As) 119, ,7924 0,0654 (17) ec 5,2 K (As) 124,1334 (6) 1,51 (6) ec 5,2 L (As) 134, ,6770 0,158 (6) ec 5,2 M (As) 135, ,9589 0,0239 (9) ec 1,0 K (As) 186,7393 (12) 0,0244 (17) ec 2,0 K (As) 252,7909 (9) 0,378 (15) ec 2,0 L (As) 263, ,3345 0,0400 (18) ec 3,0 K (As) 267,676 (1) 0,202 (10) ec 3,0 L (As) 278, ,2191 0,0217 (10) ec 4,0 K (As) 292,057 (1) 0,0614 (9) ec 5,0 K (As) 388,7905 (8) 0,01369 (20) CEA/LNE LNHB /V. Chisté, M. M. Bé 3 08/07/ /8/2013
4 5 Photon Emissions 5.1 XRay Emissions Photons per 100 disint. XL (As) 1,1195 1,5312 1,93 (5) XKα 2 (As) 10, ,5 (6) } Kα XKα 1 (As) 10, ,9 (11) } XKβ 3 (As) 11,7204 } XKβ 1 (As) 11,7263 } 7,30 (25) K β 1 XKβ 5 (As) 11,821 } XKβ 2 (As) 11,8643 } XKβ 4 (As) } 0,276 (13) K β Gamma Emissions Photons per 100 disint. γ 3,2 (As) 14,8847 (13) 0,0206 (6) γ 4,3 (As) 24,3815 (14) 0,027 (6) γ 2,1 (As) 66,0518 (8) 1,085 (35) γ 3,1 (As) 80,9365 (15) 0,0095 (5) γ 5,4 (As) 96,7340 (9) 3,35 (7) γ 5,3 (As) 121,1155 (11) 16,86 (36) γ 5,2 (As) 136,0001 (6) 57,7 (20) γ 1,0 (As) 198,6060 (12) 1,46 (6) γ 9,7 (As) 249,3 (3) 0,00394 (12) γ 2,0 (As) 264,6576 (9) 58, (19) γ 3,0 (As) 279,5422 (10) 24,89 (9) γ 4,0 (As) 303,9236 (10) 1,308 (5) γ 7,1 (As) 373,61 (24) 0,00256 (11) γ 5,0 (As) 400,6572 (8) 11,388 (42) γ 8,1 (As) 419,1 (4) 0,0121 (6) γ 6,0 (As) 468,6 (4) 0,00036 (5) γ 9,3 (As) 542,02 (18) 0, (6) γ 9,2 (As) 557,8 (9) 0,00276 (12) γ 7,0 (As) 572,22 (24) 0,03622 (31) γ 8,0 (As) 617,8 (4) 0,00453 (5) γ 9,0 (As) 821,56 (18) 0, (8) CEA/LNE LNHB /V. Chisté, M. M. Bé 4 08/07/ /8/2013
5 6 Main Production Modes Se 74(n,γ)Se As (d,2n)se As (p,n)se 7 References H.N.Friedlander, L.Seren, S.H.Turkel. Phys. Rev. 72 (1947) 23 W.S.Cowart, M.L.Pool, D.A.McCown, L.L.Woodward. Phys. Rev. 73 (1948) 1454 J.M.Cork, W.C.Rutledge, C.E.Branyan, A.E.Stoddard, J.M.Le Blanc. Phys. Rev. 79 (1950) 889 A.W.Schardt, J.P.Welker. Phys. Rev. 99 (1955) 810 (Gammaray energies and emission intensities.) H.W.Wright, E.I.Wyatt, S.A.Reynolds, W.S.Lyon, T.H.Handley. Nucl. Sci. Eng. 2 (1957) 427 F.R.Metzger, W.B.Todd. Nucl. Phys. 10 (1959) 220 H.T.Easterday, R.L.Smith. Nucl. Phys. 20 (1960) 155 E.P.Grigorev, A.V.Zolotavin. Nucl. Phys. 14 (1960) 443 (Gammaray emission intensities, ICC.) M.De Croës, G.Bäckström. Ark. Fysik 16 (1960) 567 W.F.Edwards, C.J.Gallagher. Nucl. Phys. 26 (1961) 649 D.R.Brundrit, S.K.Sen. Nucl. Phys. 68 (1965) 287 P.V.Rao, D.K.McDaniels, B.Crasemann. Nucl. Phys. 81 (1966) 296 T.Paradellis, S.Hontzeas. Nucl. Phys. A131 (1969) 378 T.Paradellis, S.Hontzeas. Nucl. Phys. A131 (1969) 378 W.W.Pratt. Nucl. Phys. A170 (1971) 223 V.Sutela. Ann. Acad. Sci. Fen. AVI 407 (1973) R.N.Thomas, R.V.Thomas. J. Phys. (London) A6 (1973) 1037 J.L.Campbell. J. Phys. (London) A7 (1974) 1451 F.Lagoutine, J.Legrand, C.Bac. Int. J. Appl. Radiat. Isotop. 26 (19) 131 M.J.Martin. Report ORNL 5114 (1976) R.J.Gherke. Nucl. Instrum. Methods 91 (1977) 349 (Gammaray emission intensities) R.J.Gehrke, R.G.Helmer, R.C.Greenwood. Nucl. Instrum. Methods 147 (1977) 405 R.Prasad. Can. J. Phys. 55 (1977) 2036 (Gammaray emission intensities and energies.) K.S.Krane. At. Data. Nucl. Data Tables 19 (1977) 363 (Mixing Ratio.) H.Houtermans, O.Milosevic, F.Reichel. Int. J. Appl. Radiat. Isotop. 31 (1980) 153 CEA/LNE LNHB /V. Chisté, M. M. Bé 5 08/07/ /8/2013
6 U.Schötzig, K.Debertin, K.F.Walz. Nucl. Instrum. Methods 169 (1980) 43 (Halflife, gammaray emission intensities.) D.D.Hoppes, J.M.R.Hutchinson, F.J.Schima, M.P.Unterweger. NBS 626 (1982) 85 Y.Yoshizawa, Y.Iwata, T.Katoh, J.Z.Ruan, Y.Kawada. Nucl. Instrum. Methods 212 (1983) 249 K.Singh, R.Mittal, M.L.Hasiza, H.S.Sahota. Indian J. Phys. 57A (1983) 127 (Xray intensities.) K.Singh, H.S.Sahota. J. Phys. (London) G10 (1984) 241 R.Jedlovszki, T.Barta, M.Csikos, Gy.Horvath, L.Szücs, A.Zsinka. Report OHMGS/32 Budapest (1987) A.Andai, T.Barta, L.Szücs. Nucl. Instrum. Meth. Phys. Res. A286 (1990) 457 R.Jedlovszky, L.Szücs, A.Szörényi. Nucl. Instrum. Meth. Phys. Res. A286 (1990) 462 X.L.Wang, Y.Wang. Nucl. Instrum. Meth. Phys. Res. A286 (1990) 460 R.A.Meyer. Fizika 22 (1990) 153 W.Bambynek, T.Barta, R.Jedlovszky, P.Christmas, N.Coursol, K.Debertin, R.G.Helmer, A.L.Nichols, F.J.Schima, Y.Yoshizawa. Report IAEATECDOC 619 (1991) (Gammaray emission intensities, halflife.) U.Schötzig. Nucl. Instrum. Meth. Phys. Res. A312 (1992) 141 A.Iwahara, I.P.A.Salati, R.Poledna, C.J.Da Silva, L.Tauhata. Nucl. Instrum. Meth. Phys. Res A339 (1994) 381 H.Miyahara, H.Matumoto, C.Mori, N.Takeuchi, T.Genka. Nucl. Instrum. Meth. Phys. Res. A339 (1994) 203 T.E.Sazonova, A.V.Zanevsky, S.V.Sepman. Nucl. Instrum. Meth. Phys. Res. A369 (1996) 421 (Xray intensities) E.Schönfeld, H.Janssen. Nucl. Instrum. Methods A369 (1996) 527 (Atomic data.) L.C.Longoria, J.S.Benitez. Appl. Rad. Isotopes 48 (1997) 1069 A.R.Farhan, B.Singh. Nucl. Data Sheets 86 (1999) 831 (Level energies, spin, parity.) Q.S.Zhang, L.YinMing, Y.Chang, C.Yan, W.Li. At. Energ. Sci. Tech. (Chine) 34 (2000) 422 (Xray intensities) M.P.Unterweger. Appl. Rad. Isotopes 56 (2002) 125 M.He, S.Jiang, L.Diao, S.Wu, C.Li. Nucl. Instrum. Meth. Phys. Res. B194 (2002) 393 G.Audi, A.H.Wapstra, C.Thibault. Nucl. Phys. A729 (2003) 129 (Q.) D.R.Rao, K.V.Sai, M.Sainath, K.Venkataramaniah. Eur. Phys. J. A26 (2005) 41 T.Kibédi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor Jr.. Nucl. Instrum. Meth. Phys. Res A589 (2008) 202 (Theoretical ICC.) CEA/LNE LNHB /V. Chisté, M. M. Bé 6 08/07/ /8/2013
7 LNELNHB/CEA Table de Radionucléides Se Emission intensities per 100 disintegrations 0 5/2 ; 0 Se ,781 (24) d 3,0 ps ,003 0,000 0,002 0,000 7/2 ; 821,6 0, ,9 ps ,012 0, ,00 0,03 1/2,3/2 ; 617,7 5/2 ; 572,22 0,0126 0, ,67 ns ,00 8 3,35 1 6,86 5 7,7 1 1,38 1/2,3/2 ; 468,6 5/2 ; 400,6585 0, ,5 17,62 ms 0,273 ns 0,0112 ns ,02 1, ,02 0,00 2 4,8 1,08 5 8,7 9/2 ; 303,9243 5/2 ; 279,5428 3/2 ; 264,6581 2,1 1,4 0,885 ns 1 1,46 1/2 ; 198,6063 Stable 0 As Q = 863,6 % = 100 3/2 ; 0 1,42 CEA/LNE LNHB / V. Chisté, M. M. Bé Scheme page : 1/1 08/07/ /08/2013
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β Transitions
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1 Decay Scheme Cf- disintegrates by alpha emissions mainly to the Cm-248 ground state level, and by spontaneous fission for 3,086(8) %. The average number of neutrons emitted by spontaneous fission is:
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1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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