1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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- Σίλας Ζερβός
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1 1 Decay Scheme Pa is a member of the natural U235 decay chain. Pa disintegrates by alpha emission to various excited levels and the ground state of Ac227. Le protactinium se désintègre par émissions alpha vers des niveaux excités et le niveau fondamental de l actinium Nuclear Data T 1/2 ( Pa ) : (260) a T 1/2 ( 227 Ac ) : 21,772 (3) a Q α ( Pa ) : 5149,9 (8) 2.1 α Transitions Probability F 100 α 0, ,5 (9) 0,0021 (5) 43 α 0, ,1 (8) 0,0036 (3) 126 α 0, ,9 (8) 0,00076 (20) 930 α 0, ,6 (9) 0,008 (4) 160 α 0, ,6 (8) 0,015 (7) 146 α 0, ,9 (8) 0,078 (21) 47 α 0, ,7 (8) 0,0504 (11) 75,8 α 0, ,3 (8) 0,080 (6) 56 α 0, ,6 (8) 1,8 (3) 4,6 α 0, ,4 (8) 1,20 (22) 11,7 α 0, ,8 (8) 8,4 (4) 2,46 α 0, ,1 (8) 0,0032 (9) 9600 α 0, ,6 (8) 0,040 (15) 1300 α 0, ,1 (8) 1,40 (15) 94 α 0,8 4989,9 (22) 0,002 (1) α 0,7 5023,0 (8) 2,9 (3) 160 NPL /A. Arinc 1 19/10/ /2/2011
2 Probability F 100 α 0,6 5039,9 (8) 22,5 (5) 26,5 α 0,5 5065,3 (8) 0,4 (1) 2160 α 0,4 5075,7 (8) 1,6 (2) 629 α 0,3 5103,5 (8) 25,3 (5) 59,5 α 0,2 5119,9 (8) 20 (2) 95 α 0,1 5122,5 (8) 2,8 (3) 707 α 0,0 5149,9 (8) 11,7 (5) Gamma Transitions and Internal Conversion Coefficients P γce Multipolarity α K α L α M α T 100 γ 3,2(Ac) 16,370 (14) 2,12 (9) E1 5,06 (7) 2,68 (4) 8,58 (12) γ 3,1(Ac) 18,980 (14) 42 (4) M1 2,35 (4) 82,7 (12) 113,2 (16) γ 11,9(Ac) 23,46 (6) 1,16 (15) M1 182 (3) 44,1 (7) 241 (4) γ 16,15(Ac) 24,46 (4) 1,05 (21) M1 161,3 (24) 39,0 (6) 214 (4) γ 6,5(Ac) 25,390 (22) 18,3 (14) M1 144,6 (21) 34,9 (5) 191 (3) γ 1,0(Ac) 27,37 (1) 59 (7) E1 3,3 (4) 0,87 (13) 4,5 (6) γ 2,0(Ac) 29,98 (1) 26 (3) M1E2 202 (21) 52 (6) 270 (30) γ 6,4(Ac) 35,800 (22) 0,045 (3) E1 1,313 (19) 0,327 (5) 1,746 (25) γ 5,3(Ac) 38,200 (14) 13 (3) M1E2 66 (14) 17 (4) 89 (19) γ 4,2(Ac) 44,160 (14) 2,11 (16) M1 28,3 (4) 6,79 (10) 37,4 (6) γ 3,0(Ac) 46,35 (1) 0,357 (19) E1 0,663 (10) 0,1634 (23) 0,879 (13) γ 20,17(Ac) 50,73 (5) 0,057 (21) M1 18,8 (3) 4,52 (7) 24,9 (4) γ 7,4(Ac) 52,720 (22) 1,77 (10) M1 16,81 (24) 4,03 (6) 22,2 (4) γ 5,2(Ac) 54,570 (14) 0,110 (6) E1 0,430 (6) 0,1053 (15) 0,569 (8) γ 15,13(Ac) 56,90 (3) 0,18 (4) M1E2 28 (5) 7,1 (12) 37 (6) γ 5,1(Ac) 57,180 (14) 4,6 (5) E2 108,6 (16) 29,6 (5) 148,1 (21) γ 17,15(Ac) 57,190 (22) 0,7 (3) E2 108,5 (16) 29,6 (5) 148,0 (21) γ 9,7(Ac) 60,46 (4) 0,0076 (10) E1 0,327 (5) 0,0800 (12) 0,433 (7) γ 6,3(Ac) 63,590 (22) 3,99 (16) E2 65,1 (10) 17,8 (3) 88,8 (13) γ ( 1,1) (Ac) 70,49 (5) 0,0051 (8) γ 10,7(Ac) 71,85 (5) 0,019 (7) M1 6,79 (10) 1,630 (23) 8,98 (13) γ 12,10(Ac) 72,58 (7) 0,029 (7) M1 6,59 (10) 1,582 (23) 8,71 (13) γ 4,0(Ac) 74,14 (1) 0,97 (4) E2 31,2 (5) 8,53 (12) 42,6 (6) γ 9,6(Ac) 77,38 (4) 0,50 (4) M1 5,47 (8) 1,313 (19) 7,23 (11) γ 7,2(Ac) 96,880 (22) 1,10 (4) E2 8,81 (13) 2,41 (4) 12,02 (17) γ 11,6(Ac) 100,84 (5) 0,248 (10) E2 7,30 (11) 2,00 (3) 9,97 (15) γ 9,5(Ac) 102,77 (3) 0,20 (4) E2 6,69 (10) 1,83 (3) 9,12 (13) γ 10,4(Ac) 124,57 (4) 0,0217 (20) E2 0,285 (4) 2,75 (4) 0,752 (11) 4,04 (6) γ 12,7(Ac) 144,43 (6) 0,037 (3) E2 0,263 (4) 1,407 (20) 0,384 (6) 2,18 (3) γ 13,4(Ac) 199,00 (3) 0,0030 (12) γ 14,4(Ac) 230,59 (5) 0,0017 (8) γ ( 1,2) (Ac) 242,18 (8) 0,0099 (10) γ 13,2(Ac) 243,16 (3) 0,065 (11) M1E2 0,56 (16) 0,176 (10) 0,0445 (16) 0,80 (17) γ 15,5(Ac) 245,490 (14) 0,042 (3) M2 3,70 (6) 1,143 (16) 0,293 (5) 5,24 (8) γ 13,1(Ac) 245,77 (3) 0,013 (4) E1 0,0455 (7) 0,00867 (13) 0,00208 (3) 0,0570 (8) γ 15,4(Ac) 255,900 (14) 0,134 (3) E2 0,0992 (14) 0,1216 (17) 0,0327 (5) 0,264 (4) γ 14,3(Ac) 258,38 (5) 0,0015 (4) NPL /A. Arinc 2 19/10/ /2/2011
3 P γce Multipolarity α K α L α M α T 100 γ 17,7(Ac) 260,37 (3) 0,282 (21) M1E2 0,37 (10) 0,133 (7) 0,0340 (13) 0,55 (11) γ 13,0(Ac) 273,14 (3) 0,101 (7) M1E2 0,57 (10) 0,131 (8) 0,0323 (15) 0,74 (11) γ 17,6(Ac) 277,29 (3) 0,10 (6) E1M2 0,4 (7) 0,11 (19) 0,03 (5) 0,5 (9) γ 15,3(Ac) 283,690 (14) 1,72 (3) E1 0,0329 (5) 0,00614 (9) 0, (21) 0,0410 (6) γ ( 1,3) (Ac) 286,58 (10) 0,0104 (5) γ 15,2(Ac) 300,060 (14) 4,25 (10) M1E2 0,613 (15) 0,1146 (20) 0,0275 (5) 0,764 (17) γ 15,1(Ac) 302,670 (14) 2,4 (3) E1 0,0285 (4) 0,00527 (8) 0, (18) 0,0355 (5) γ 17,5(Ac) 302,680 (22) 0,22 (10) E1 0,0285 (4) 0,00527 (8) 0, (18) 0,0355 (5) γ ( 1,4) (Ac) 310,0 (1) 0,00092 (20) γ 17,4(Ac) 313,090 (22) 0,129 (9) M1E2 0,22 (8) 0,070 (8) 0,0177 (16) 0,31 (9) γ 16,1(Ac) 327,13 (4) 0,0372 (11) E1 0,0240 (4) 0,00440 (7) 0, (15) 0,0298 (5) γ 15,0(Ac) 330,04 (1) 2,09 (5) M1E2 0,430 (16) 0,0836 (20) 0,0202 (5) 0,541 (19) γ 17,3(Ac) 340,880 (22) 0,196 (7) E1M2 0,081 (22) 0,020 (6) 0,0050 (15) 0,11 (3) γ 18,4(Ac) 351,45 (3) 0,0029 (12) E1 0,0206 (3) 0,00373 (6) 0, (13) 0,0255 (4) γ 16,0(Ac) 354,50 (4) 0,1094 (23) M1E2 0,0855 (12) 0,0386 (6) 0,01003 (14) 0,1375 (20) γ 17,2(Ac) 357,250 (22) 0,240 (18) M1E2 0,34 (9) 0,066 (10) 0,0159 (21) 0,43 (10) γ 17,1(Ac) 359,860 (22) 0,0085 (3) γ 20,4(Ac) 363,82 (4) 0,0080 (3) γ ( 1,5) (Ac) 374,95 (10) 0,0045 (3) γ 18,3(Ac) 379,24 (3) 0,066 (6) M1E2 0,25 (10) 0,052 (11) 0,0125 (24) 0,32 (11) γ 21,5(Ac) 384,69 (6) 0,00365 (22) γ 17,0(Ac) 387,23 (2) 0,00032 (11) E2 0,0430 (6) 0,0254 (4) 0,00667 (10) 0,0773 (11) γ 20,3(Ac) 391,61 (4) 0,00687 (22) E1 0,01636 (23) 0,00293 (5) 0, (10) 0,0202 (3) γ 18,2(Ac) 395,61 (3) 0,00230 (22) E1 0,01601 (23) 0,00286 (4) 0, (10) 0,0198 (3) γ 18,1(Ac) 398,22 (3) 0,0095 (3) γ 19,1(Ac) 407,820 (22) 0,0475 (11) M1 0,269 (4) 0,0496 (7) 0,01187 (17) 0,334 (5) γ 20,1(Ac) 410,59 (4) 0,00183 (22) E1 0,01482 (21) 0,00264 (4) 0, (9) 0,0183 (3) γ 22,4(Ac) 427,14 (7) 0,0007 (4) γ 19,0(Ac) 435,19 (2) 0,00294 (17) γ 20,0(Ac) 437,96 (4) 0,0045 (3) γ ( 1,6) (Ac) 438,72 (10) 0,0013 (4) γ 24,4(Ac) 488,66 (10) 0,00165 (17) γ 23,3(Ac) 490,65 (10) 0,0004 (1) γ 22,0(Ac) 501,28 (7) 0,00076 (18) γ 23,1(Ac) 509,63 (10) 0,00036 (17) γ 24,3(Ac) 516,45 (10) 0,00137 (15) γ 24,1(Ac) 535,43 (10) 0,00061 (12) γ 25,6(Ac) 546,5 (3) 0,00083 (13) γ 25,5(Ac) 571,9 (3) 0,00048 (20) γ 25,4(Ac) 582,3 (3) 0,00031 (17) γ 25,3(Ac) 610,1 (3) 0,0005 (4) NPL /A. Arinc 3 19/10/ /2/2011
4 3 Atomic Data 3.1 Ac ω K : 0,969 (4) ω L : 0,464 (18) n KL : 0,799 (5) X Radiations Relative probability K Kα 2 87,768 61,52 Kα 1 90, Kβ 3 102,101 } Kβ 1 102,841 } Kβ 5 103,462 } 35,26 Kβ 2 105,679 } Kβ 4 106,098 } 11,74 KO 2,3 106,563 } L Ll 10,8701 Lα 12, ,6505 Lη 14,0807 Lβ 14, ,9311 Lγ 17,813 18, Auger Electrons Relative probability Auger K KLL 66,769 74, KLX 81,775 90,882 58,2 KXY 96,76 106,75 8,47 Auger L 5,87 19,69 NPL /A. Arinc 4 19/10/ /2/2011
5 4 α Emissions Probability 100 α 0, ,6 (9) 0,0021 (5) α 0, ,6 (8) 0,0036 (3) α 0, ,0 (8) 0,00076 (20) α 0, ,1 (9) 0,008 (4) α 0, ,6 (8) 0,015 (7) α 0, ,3 (8) 0,078 (21) α 0, ,0 (8) 0,0504 (11) α 0, ,5 (8) 0,080 (6) α 0, ,1 (8) 1,8 (3) α 0, ,3 (8) 1,20 (22) α 0, ,3 (8) 8,4 (4) α 0, ,2 (8) 0,0032 (9) α 0, ,1 (8) 0,040 (15) α 0, ,5 (8) 1,40 (15) α 0,8 4903,4 (22) 0,002 (1) α 0,7 4936,0 (8) 2,9 (3) α 0,6 4952,6 (8) 22,5 (5) α 0,5 4977,6 (8) 0,4 (1) α 0,4 4987,8 (8) 1,6 (2) α 0,3 5015,1 (8) 25,3 (5) α 0,2 5031,2 (8) 20 (2) α 0,1 5033,8 (8) 2,8 (3) α 0,0 5060,7 (8) 11,7 (5) 5 Electron Emissions Electrons per 100 disint. e AL (Ac) 5,87 19,69 52,6 (15) e AK (Ac) 0,078 (11) KLL 66,769 74,715 } KLX 81,775 90,882 } KXY 96,76 106,75 } NPL /A. Arinc 5 19/10/ /2/2011
6 6 Photon Emissions 6.1 XRay Emissions Photons per 100 disint. XL (Ac) 10, , ,3 (13) XKα 2 (Ac) 87,768 0,715 (23) } Kα XKα 1 (Ac) 90,885 1,16 (4) } XKβ 3 (Ac) 102,101 } XKβ 1 (Ac) 102,841 } 0,410 (15) K β 1 XKβ 5 (Ac) 103,462 } XKβ 2 (Ac) 105,679 } XKβ 4 (Ac) 106,098 } 0,136 (6) K β 2 XKO 2,3 (Ac) 106,563 } 6.2 Gamma Emissions Photons per 100 disint. γ 3,2 (Ac) 16,370 (14) 0,221 (9) γ 3,1 (Ac) 18,980 (14) 0,37 (3) γ 11,9 (Ac) 23,46 (6) 0,0048 (6) γ 16,15 (Ac) 24,46 (4) 0,0049 (10) γ 6,5 (Ac) 25,390 (22) 0,095 (7) γ 1,0 (Ac) 27,37 (1) 10,8 (4) γ 2,0 (Ac) 29,98 (1) 0,097 (4) γ 6,4 (Ac) 35,800 (22) 0,0163 (10) γ 5,3 (Ac) 38,200 (14) 0,144 (6) γ 4,2 (Ac) 44,160 (14) 0,055 (4) γ 3,0 (Ac) 46,35 (1) 0,19 (1) γ 20,17 (Ac) 50,73 (5) 0,0022 (8) γ 7,4 (Ac) 52,720 (22) 0,076 (4) γ 5,2 (Ac) 54,570 (14) 0,070 (4) γ 15,13 (Ac) 56,90 (3) 0,0047 (7) γ 5,1 (Ac) 57,180 (14) 0,031 (3) γ 17,15 (Ac) 57,190 (22) 0,0046 (21) γ 9,7 (Ac) 60,46 (4) 0,0053 (7) γ 6,3 (Ac) 63,590 (22) 0,0446 (17) γ ( 1,1) (Ac) 70,49 (5) 0,0051 (8) γ 10,7 (Ac) 71,85 (5) 0,0019 (7) NPL /A. Arinc 6 19/10/ /2/2011
7 Photons per 100 disint. γ 12,10 (Ac) 72,58 (7) 0,0030 (7) γ 4,0 (Ac) 74,14 (1) 0,0223 (9) γ 9,6 (Ac) 77,38 (4) 0,061 (4) γ 7,2 (Ac) 96,880 (22) 0,084 (3) γ 11,6 (Ac) 100,84 (5) 0,0226 (9) γ 9,5 (Ac) 102,77 (3) 0,019 (4) γ 10,4 (Ac) 124,57 (4) 0,0043 (4) γ 12,7 (Ac) 144,43 (6) 0,0115 (9) γ 13,4 (Ac) 199,00 (3) 0,0030 (12) γ 14,4 (Ac) 230,59 (5) 0,0017 (8) γ ( 1,2) (Ac) 242,18 (8) 0,0099 (10) γ 13,2 (Ac) 243,16 (3) 0,036 (5) γ 15,5 (Ac) 245,490 (14) 0,0067 (5) γ 13,1 (Ac) 245,77 (3) 0,012 (4) γ 15,4 (Ac) 255,900 (14) 0,1059 (22) γ 14,3 (Ac) 258,38 (5) 0,0015 (4) γ 17,7 (Ac) 260,37 (3) 0,182 (4) γ 13,0 (Ac) 273,14 (3) 0,0579 (12) γ 17,6 (Ac) 277,29 (3) 0,0680 (15) γ 15,3 (Ac) 283,690 (14) 1,65 (3) γ ( 1,3) (Ac) 286,58 (10) 0,0104 (5) γ 15,2 (Ac) 300,060 (14) 2,41 (5) γ 15,1 (Ac) 302,670 (14) 2,3 (3) γ 17,5 (Ac) 302,680 (22) 0,21 (10) γ ( 1,4) (Ac) 310,0 (1) 0,00092 (20) γ 17,4 (Ac) 313,090 (22) 0,0987 (20) γ 16,1 (Ac) 327,13 (4) 0,0361 (11) γ 15,0 (Ac) 330,04 (1) 1,36 (3) γ 17,3 (Ac) 340,880 (22) 0,177 (4) γ 18,4 (Ac) 351,45 (3) 0,0028 (12) γ 16,0 (Ac) 354,50 (4) 0,0962 (20) γ 17,2 (Ac) 357,250 (22) 0,168 (4) γ 17,1 (Ac) 359,860 (22) 0,0085 (3) γ 20,4 (Ac) 363,82 (4) 0,0080 (3) γ ( 1,5) (Ac) 374,95 (10) 0,0045 (3) γ 18,3 (Ac) 379,24 (3) 0,0498 (11) γ 21,5 (Ac) 384,69 (6) 0,00365 (22) γ 17,0 (Ac) 387,23 (2) 0,0003 (1) γ 20,3 (Ac) 391,61 (4) 0,00673 (22) γ 18,2 (Ac) 395,61 (3) 0,00226 (22) γ 18,1 (Ac) 398,22 (3) 0,0095 (3) γ 19,1 (Ac) 407,820 (22) 0,0356 (8) γ 20,1 (Ac) 410,59 (4) 0,00180 (22) γ 22,4 (Ac) 427,14 (7) 0,0007 (4) γ 19,0 (Ac) 435,19 (2) 0,00294 (17) γ 20,0 (Ac) 437,96 (4) 0,0045 (3) γ ( 1,6) (Ac) 438,72 (10) 0,0013 (4) NPL /A. Arinc 7 19/10/ /2/2011
8 Photons per 100 disint. γ 24,4 (Ac) 488,66 (10) 0,00165 (17) γ 23,3 (Ac) 490,65 (10) 0,0004 (1) γ 22,0 (Ac) 501,28 (7) 0,00076 (18) γ 23,1 (Ac) 509,63 (10) 0,00036 (17) γ 24,3 (Ac) 516,45 (10) 0,00137 (15) γ 24,1 (Ac) 535,43 (10) 0,00061 (12) γ 25,6 (Ac) 546,5 (3) 0,00083 (13) γ 25,5 (Ac) 571,9 (3) 0,00048 (20) γ 25,4 (Ac) 582,3 (3) 0,00031 (17) γ 25,3 (Ac) 610,1 (3) 0,0005 (4) 7 Main Production Modes Th 232(n, 2n)Th Th (β )Pa U 235 decay chain 8 References A.V.GROSSE. Naturwissensch. 20 (1932) 505 (Halflife) Q.VAN WINKLE, R.G.LARSON, L.I.KATZIN. J. Am. Chem. Soc. 71 (1949) 2585 (Halflife) P. FALKVAIRANT, M.RIOU. J. Phys. Radium 14,2 (1953) 65 (Gammaray emission probabilities and energies) J.P.HUMMEL. Thesis, Uni. Calif. (1956) (Alphaparticle emission probabilities) F.ASARO, F.S.STEPHENS,J.M.HOLLANDER,I.PERLMAN. Phys. Rev. 117, 2 (1960) 492 (L and Mshell conversion coefficients) R.FOUCHER. Comp. Rend. Acad. Sci. (Paris) 250 (1960) 1249 (Gammaray emission probabilities) F.BRAGANCA GIL, G.Y.PETIT. J. Phys. Radium 22 (1961) 680 (Spin and parity, mixing ratio, halflife excited level) H.W.KIRBY. J. Inorg. Nucl. Chem. 18 (1961) 8 (Halflife) S.BARANOV, V.M.KULAKOV,P.S.SAMOILOV,A.G.ZELENKOV,Y.F.RODIONOV,S.V.PIROZHKOV. Sov. Phys. JETP 14, 5 (1961) 1053 (Alphaparticle emission energies and probabilities, experimental conversions) V.B.SUBRAHMANYAM. Thesis, Uni. Calif. (1963) (Alphaparticle emission probabilities) H.ABOULEILA, R.FOUCHER, A.G.DE PINHO, N.PERRIN, M.VALADARES. J. Phys. (Paris) 24 (1963) 857 (Spin and parity, multipolarities) G.BASTIN, C.F.LEANG, R.J.WALES. Comp. Rend. Acad. Sci. (Paris) T.262 (1966) 89 (Alphaparticle emission energies) D.BROWN, S.N.DIXON, K.M.GLOVER, F.J.G.ROGERS. J. Inorg. Nucl. Chem. 30 (1968) 19 (Halflife) NPL /A. Arinc 8 19/10/ /2/2011
9 S.BARANOV, V.M.KULAKOV,V.M.SHATINSKII. Sov. J. Nucl. Phys. 7,4 (1968) 442 (Alphaparticle emission energies) G.R.HAGEE, R.C.LANGE,A.G.BARNETT, A.R.CAMPBELL, C.R. COTHERN, D.F. GRIFFING, H.J. HENNECKE. Nucl. Phys. A115 (1968) 157 (Spin and parity, conversion electron emission probabilities) A.G.BARNETT, A.R.CAMPBELL, G.R.HAGEE. J. Inorg. Nucl. Chem. 31 (1969) 1553 (Multipolarities, conversion electron emission probabilities, mixing ratio) R.C.LANGE, G.R.HAGEE. Nucl. Phys. A124 (1969) 412 (Gammaray emission energies and probabilities) J.ROBERT, C.F.MIRANDA, R.MUXART. Radiochim. Acta 11 (1969) 104 (Halflife) A.G.DE PINHO, E.F.DA SILVEIRA, N.L.DA COSTA. Phys. Rev.C 2,2 (1970) 572 (Gammaray emission energies and probabilities, ICC) C.F.LEANG. J. Phys. (Paris) 31 (1970) 269 (Gammaray emission energies and probabilities) C.F.LEANG. J. Phys. (Paris) 32,23 (1971) 95 (Spin and parity) R.K.GARG, S.D.CHAUHAN, S.SANYAL, S.C. PANCHOLI, S.L.GUPTA, N.K.SAHA. Z. Physik 257 (1972) 124 (Halflife of excited level) A.G.DE PINHO, L.T.AULER, A.G.DA SILVA. Phys. Rev.C 9,5 (1974) 2056 (Xray emission probabilities, gammaray emission probabilities, ICC) S.A.BARANOV. Sov.J.At.Energ. 41 (1976) 342 (Alphaparticle emission energies and probabilities) S.A.BARANOV, A.G.ZELENKOV, V.M.KULAKOV. Proc. Advisory Group Meeting on Transactinium Nucl. Data, Karlsruhe. IAEA186 Vol III (1976) 249 (Alphaparticle emission energies and probabilities) W.TEOH, R.D.CONNOR, R.H.BETTS. Nucl. Phys. A319 (1979) 122 (Gammaray emission energies and probabilities, Multipolarities, ICC) H.G.BORNER, G.BARREAU, W.F.DAVIDSON, P.JEUCH, T.VON EGIDY, J.ALMEIDA, D.H.WHITE. Nucl. Instrum. Methods 166 (1979) 251 (Gammaray emission energies) I.ANICIN, I.BIKIT, C.GIRIT, H.GUVEN, W.D.HAMILTON, A.A.YOUSIF. Nucl. Phys. 8 (1982) 369 (Gammaray emission probabilities) M.F.BANHAM, R.JONES. Int. J. Appl. Radiat. Isotop. 34, 8 (1983) 1225 (Gammaray emission probabilities) T.ISHII, I.AHMAD, J.E.GINDLER,A.M.FRIEDMAN, R.R.CHASMAN, S.B.KAUFMAN. Nucl. Phys. A444 (1985) 237 (halflife first excited state) IAEA Technical Reports Series, N 261 (1986) (Gammaray emission energies and probabilities, alphaparticle emission energies and probabilities.) N.E.HOLDEN. Pure & Appl. Chem. 62,5 (1990) 941 (Halflife) A.RYTZ. At. Data Nucl. Data Tables 47 (1991) 205 (Evaluated alphaparticle emission energies and probabilities) Y.A.AKOVALI. Nucl. Data Sheets 84 (1998) 1 (R0, radius parameter) E.BROWNE. Nucl. Data Sheets 93 (2001) 763 (Spin, parity, energy levels, multipolarities) G.AUDI, A.H.WAPSTRA, C.THIBAULT. Nucl. Phys. A729 (2003) 337 (Q value) T.KIBEDI, T.W.BURROWS, M.B.TRZHASKOVSKAYA, P.M.DAVISON, C.W.NESTOR JR.. Nucl. Instrum. Methods Phys. Res. A589 (2008) 202 (Theoretical ICC) NPL /A. Arinc 9 19/10/ /2/2011
10 LNELNHB/CEA Table de Radionucléides γ Emission intensities per 100 disintegrations 0 α Pa /2 ; 0 Pa (260) a ,000 0,000 0,000 0,000 (7/2) ; 656,4 0, ,00 0,00 0,00 4 0,000 0, ,00 0,00 0, ,00 0,00 0,00 0,00 0,00 6 0,035 0, ,002 0,049 0,002 0,009 (3/2,5/2) ; 562,8 (3/2) ; 537 (3/2,5/2) ; 501,28 (9/2) ; 469,24 (5/2) ; 437,96 (1/2) ; 435,19 5/2 ; 425,59 7/2 ; 387,23 0,0036 0, ,008 0,015 0,078 0,0504 0,08 1, ,3 ns 1 21,772 (3) a Ac α Q = 5149,9 % α = 100 (9/2) ; 109,94 (7/2) ; 84,55 (7/2) ; 74,14 5/2 ; 46,35 5/2 ; 29,98 3/2 ; 27,37 3/2 ; 0 NPL / A. Arinc Scheme page : 1/3 19/10/ /03/ ,5 0,4 1,6 25,3 20 2,8 11,7
11 LNELNHB/CEA Table de Radionucléides γ Emission intensities per 100 disintegrations 0 α Pa /2 ; 0 Pa (260) a ,004 0,182 0,068 0,21 0,098 0,177 0,168 0,008 0,000 7/2 ; 387,23 1, ,004 0,036 0, ,00 0,00 0,10 1,65 2,41 2,3 1,36 1/2 ; 354,5 3/2 ; 330,04 1,2 8, ,00 0,00 (5/2) ; 304,73 0, ,00 0,03 0,01 0,05 (5/2) ; 273,14 2,9 7 6 (9/2) ; 126,86 (9/2) ; 109,94 22,5 0,4 5 4 (7/2) ; 84,55 (7/2) ; 74,14 1,6 25,3 38,3 ns /2 ; 46,35 5/2 ; 29,98 3/2 ; 27, ,8 21,772 (3) a Ac α Q = 5149,9 % α = 100 3/2 ; 0 NPL / A. Arinc Scheme page : 2/3 19/10/ /03/ ,7
12 LNELNHB/CEA Table de Radionucléides γ Emission intensities per 100 disintegrations 0 α Pa /2 ; 0 Pa (260) a 5 0,003 0, (13/2) ; 271,29 0, ,00 0, (13/2) ; 210,78 1, ,001 0, ,00 0,06 0,01 (11/2) ; 198,71 (11/2) ; 187, ,07 0, ,09 0,01 0,04 (9/2) ; 126,86 (9/2) ; 109,94 2,9 22, ,14 0,07 0, ,05 0,02 (7/2) ; 84,55 (7/2) ; 74,14 0,4 1, ,22 0,37 0,19 5/2 ; 46,35 25,3 38,3 ns ,09 1 0,8 5/2 ; 29,98 3/2 ; 27, ,8 21,772 (3) a Ac α Q = 5149,9 % α = 100 3/2 ; 0 NPL / A. Arinc Scheme page : 3/3 19/10/ /03/ ,7
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
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:
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β Transitions
1 Decay Scheme Le césium se désintègre essentiellement par émission bêta moins vers des niveaux excités du baryum. Cs- desintegrates mainly by beta minus emissions to excited levels in Ba-. 2 Nuclear Data
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
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
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Bi- disintegrates 97.91(3) % by beta minus emission to the levels in Po- and 2.09(3) % through alpha decay to Tl-209. Le bismuth se désintègre principalement par émissions bêta vers le polonium
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Rh- disintegrates by beta minus emission to the ground state and excited levels of Pd-. Le rhodium se désintègre par émission bêta principalement vers le niveau fondamental et les niveaux
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Np decays 87,8 (6) % by electron capture to U, 12,0 (6) % by beta minus emission to Pu, a possible alpha emission of 0,16 (6)% to Pa232 has not been observed. Le neptunium se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Pb ground state (J π = 9/2 + ) decays by 100 % beta minus to Bi. The strongest branch (91.28 (12) %) decays directly to the ground state (J π = 9/2 ). Le plomb se désintègre par émissions
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Pb disintegrates by beta minus emission to excited levels and to the ground state level of Bi. Le plomb se désintègre par émission bêta moins vers des niveaux excités et le niveau fondamental
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
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
1 Decay Scheme. 2 Nuclear Data. 2.1 β + Transitions. 2.2 Electron Capture Transitions
1 Decay Scheme Ni disintegrates by electron capture (56.6 %) and positron emission (43.4 %) to excited levels in Co. The transition to the ground state has not been observed. Le nickel se désintègre par
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Bi- undergoes beta decay to Po- (64.07(7)%), and alpha decay to Tl-208 (35.93(7)%). 0.014(1)% of the beta branch undergoes prompt long-range alpha decay to Pb-208. Le bismuth se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme U- disintegrates by alpha emission mainly to the ground and 49- states in Th-232, and by 9,3 10 8 % spontaneous fission. L uranium se désintègre par émission alpha et par fission spontanée
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Sn- decays by electron capture mainly to the In-m isomer which has a half-life of 99 minutes. After a sufficient time, the ratio of the In-m (99 min) and Sn- activities remains constant
1 Decay Scheme. 2 Nuclear Data. 236m. 2.1 Electron Capture Transitions. 2.2 β Transitions
1 Decay Scheme Np- (isomer state of Np-236, J=1, E1 =60 ) decays 53(1) % by electron capture to U-236 and 47(1) % by beta minus emission to Pu-236. Le neptunium 236 isomère se désintègre par capture électronique
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pu- decays approximately 100 % by beta minus emission to the ground state of Am- and 0,00244 % by alpha emission to levels of U-237. The spontaneous fission decay branching is less than
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Eu- disintegrates 100 % via beta minus disintegration to excited levels and to the ground state in Gd-. L europium se désintègre par émission bêta moins vers des niveaux excités et le niveau
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme In- disintegrates by > 99.99% electron capture via the excited level of 416.6 in Cd- and by < 0.01% electron capture via the isomer level in Cd- (T 1/2 = 48.5 min) at 396.2. Transitions
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Uranium decays primarily by alpha decay to excited states in Th-228. A small branching of exotic decay via Ne-24 emission and a smaller branching of spontaneous fission have been reported.
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Cm decays 1% by alpha transitions to Pu38 and by spontaneous fission with branching fraction of 6.36 (14) E6 %. Le curium se désintègre à 1% par transition alpha vers le plutonium 38 et
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Am decays by emission of alpha particles to Np239, with a minute branch of 3.8 (7) 10 9 % by spontaneous fission. L américium se désintègre par émission alpha vers le neptunium 239. Un faible
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Co decays 100% by electron capture to the excited levels of 706.42 kev (0.183%) and 136.47 kev (99.80%) in Fe. Le cobalt se désintègre par capture électronique vers des niveaux excités du
1 Decay Scheme. 2 Nuclear Data. 2.1 β Transitions
1 Decay Scheme Nd- disintegrates by beta minus emission to excited levels of Pm-. If a transition to the ground state level exists, it is less than 0.15 %. Le néodyme se désintègre par émission bêta moins
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Pb- disintegrates by electron capture to Tl- via excited levels. Le plomb se désintègre par capture électronique vers des niveaux excités du thallium. 2 Nuclear Data T 1/2 ( Pb ) : 51,929
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 Gamma Transitions and Internal Conversion Coefficients
1 Decay Scheme Co disintegrates by 100% electron capture to the excited levels of 706.42 (0.18%), and 136.47 (99.82%) in Fe. Le cobalt se désintègre à 100 % par capture électronique principalement vers
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Cm- decays 100% by alpha transitions to Pu-240 and by spontaneous fission with branching fraction of 1.36 (1) E-4 %. Le curium se désintègre par émission alpha et par fission spontanée dans
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme - disintegrates 19.58 (11) % by beta plus emission and 8.2 (11) % by electron capture to Fe-. - emits gamma rays with energies up to 612 and the energies and emission probabilities for many
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions. 2.2 β + Transitions
1 Decay Scheme Zr- (half-life of 78.42 h) undergoes 100% EC/positron decay (Q EC of 2832.8(28) kev) to various nuclear levels, including the metastable and ground states of Y-. Le zirconium se désintègre
1 Decay Scheme. 2 Nuclear Data. 2.1 α Transitions
1 Decay Scheme Pu- decays 100% by alpha transitions to U-234. Most of the alpha decay populates the U-234 ground state (71.04 %) and the U-234 first excited level with energy of 43.50 (28.85 %). Branching
1 Decay Scheme. 2 Nuclear Data. 2.1 Electron Capture Transitions
1 Decay Scheme Ba disintegrates by electron capture mainly to two Cs excited levels of 437 kev (85.4%) and of 383 kev (14.5%) with three very minor branches to the 160 kev, 81 kev excited levels and the
Th, Ra, Rn, Po, Pb, Bi, & Tl K x-rays. Rn Kα1. Rn Kα2. 93( 227 Th)/Rn Kβ3. Ra Kα2. Po Kα2 /Bi K α1 79( 227 Th)/Po Kα1. Ra Kα1 /Bi K β1.
Page -1-10 8 10 7 10 6 10 5 10 4 334 ( Th) Counts/Channel 10 3 10 2 10 1 49 ( Th)/ 50 ( Th)/ 50 ( Fr) 0 100 200 300 400 500 600 700 800 900 1000 1000 1100 1200 1300 1400 1500 1600 1700 1800 1900 2000 Channel
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