241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
241 95
1
Am
Am 146
146
Decay Scheme
Am-241 decays 100% by alpha transitions to Np-237. Most of the decay (84.6 %) populate the excited level of Np-237 with energy of 59.54 keV. Branching of Am-241 decay by spontaneous fission is 3,6 (9) E-10 %. L’am´ericium 241 se d´esint`egre ` a 100 % par ´emission alpha vers le neptunium 237. Le branchement principal (84,6 %) se fait vers le niveau excit´e de 59 keV. Un faible branchement (3,6 (9) E-10 %) par fission spontan´ee a ´et´e observ´e.
2
Nuclear Data T1/2 (241 Am ) T1/2 (237 Np ) Qα (241 Am )
2.1
: : :
432,6 2,144 5637,82
(6) (7) (12)
a 106 a keV
α Transitions Energy keV α0,36 α0,34 α0,33 α0,32 α0,30 α0,29 α0,28 α0,27 α0,25 α0,24 α0,23 α0,22 α0,21 α0,20
4838,00 4882,14 4915,86 4971,62 5039,83 5045,49 5047,73 5091,70 5140,81 5151,60 5178,13 5185,27 5193,04 5203,70
(13) (13) (13) (15) (15) (14) (13) (14) (13) (15) (13) (13) (16) (13)
Probability × 100
F
0,00004 (3) 0,000086 0,0007
47 44 9,5
0,0001 0,00011 ∼ 0,0004 ∼ 0,0004
KRI /V. P. Chechev, N. K. Kuzmenko
0,0004
1000 2300 ∼ 1000 ∼ 1000 1400
1
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV α0,19 α0,18 α0,17 α0,16 α0,15 α0,14 α0,13 α0,12 α0,11 α0,9 α0,8 α0,6 α0,5 α0,4 α0,3 α0,2 α0,1 α0,0
2.2
5219,6 5242,25 5266,89 5269,21 5277,90 5305,44 5313,40 5321,0 5332,77 5370,25 5411,82 5479,32 5507,83 5534,86 5561,92 5578,28 5604,62 5637,82
(2) (13) (13) (13) (23) (13) (13) (3) (13) (13) (13) (13) (13) (12) (12) (12) (12) (12)
F
0,0007 0,0003 0,0009 0,0006
1400 4600 1600 2700
0,0013
2100
0,0022 0,0005 0,014 1,66 ∼ 0,01 13,23 < 0,04 84,45 0,23 0,38
(3) (3) (3) (10) (10) (1) (1)
1600 12000 770 16,4 ≈ 4000 4,3 > 2000 1,3 600 610
Gamma Transitions and Internal Conversion Coefficients Energy keV
γ10,9 (Np) γ2,1 (Np) γ4,3 (Np) γ27,26 (Np) γ(−1,1) (Np) γ1,0 (Np) γ17,14 (Np) γ3,1 (Np) γ4,2 (Np) γ14,10 (Np) γ5,3 (Np) γ6,4 (Np) γ13,9 (Np) γ(−1,2) (Np) γ2,0 (Np) γ7,5 (Np) γ14,9 (Np) γ8,6 (Np) γ4,1 (Np) γ3,0 (Np) γ36,33 (Np) γ11,8 (Np) γ15,9 (Np) γ5,1 (Np) γ6,2 (Np)
Probability × 100
Am 146
13,81 26,34460 27,06 31,92 32,183 33,1963 38,54 42,704 43,420 51,01 54,09 55,56 56,86 57,85 59,5409 61,56 64,83 67,50 69,76 75,90 77,86 79,05 92,35 96,79 98,97
(2) (24) (1) (8) (3) (3) (5) (3) (3) (3) (2) (3) (5) (1) (7) (2) (2) (3) (1) (4) (3) (20) (3) (2)
Pγ+ce × 100
21 (5)
0,0174 (4) 21,3 (30) ≈ 0,42 (9) 12,1 (16) 0,000046 (21)
Multipolarity
αK
M1 + 0,10 % E2 E1 anomalous
M1 + 1,66 % E2 M1 + > 30 % E2 (M1 + ≈ 1,7 % E2) M1 + 16,6 % E2 E1
1,19 (16)
M1 + 17,5 % E2
77,6 (25)
E1 anomalous
0,000196 (28) 0,013 (4) 0,0039 (5) 0,032
E1 (M1 + 17 % E2) (E1) (E2)
0,000047 (16) 0,329 (10)
E2
KRI /V. P. Chechev, N. K. Kuzmenko
αL
6 (2)
131 > 94 ≈ 56 132 0,564
(17) (5) (17) (11)
48 (4)
0,84 (6) 0,301 22 0,248 38,6
(6) (5) (5) (8)
11,07 (22)
2
αM
αT
365 (7) 1,6 (2)
494 (10) 8 (2)
33 > 345 ≈ 13,9 35 0,141
(5) (14) (5) (3)
12,6 (11)
0,226 (7) 0,0744 5,7 0,0612 10,76
(15) (13) (12) (22)
3,08 (6)
175 > 472 ≈ 75 180 0,753
(24) (7) (23) (11)
65 (6)
1,16 (7) 0,400 29 0,330 53,1
(8) (6) (7) (11)
15,2 (3)
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV γ4,0 (Np) γ(−1,3) (Np) γ20,13 (Np) γ7,3 (Np) γ21,13 (Np) γ8,4 (Np) γ6,1 (Np) γ(−1,4) (Np) γ20,11 (Np) γ23,13 (Np) γ(−1,5) (Np) γ30,23 (Np) γ29,22 (Np) γ11,6 (Np) γ8,3 (Np) γ26,15 (Np) γ(−1,6) (Np) γ29,20 (Np) γ24,13 (Np) γ9,4 (Np) γ13,6 (Np) γ18,8 (Np) γ11,5 (Np) γ(−1,7) (Np) γ25,11 (Np) γ29,18 (Np) γ(−1,8) (Np) γ18,7 (Np) γ9,2 (Np) γ13,4 (Np) γ26,10 (Np) γ9,1 (Np) γ26,9 (Np) γ13,3 (Np) γ24,8 (Np) γ22,7 (Np) γ27,10 (Np) γ13,2 (Np) γ9,0 (Np) γ(−1,9) (Np) γ(−1,10) (Np) γ20,6 (Np) γ27,9 (Np) γ13,1 (Np) γ16,3 (Np) γ15,2 (Np) γ20,5 (Np) γ16,2 (Np) γ12,0 (Np) γ28,9 (Np) γ22,5 (Np) γ(−1,11) (Np) γ(−1,12) (Np) γ14,0 (Np) γ16,1 (Np) γ17,1 (Np) γ(−1,13) (Np) γ20,3 (Np) γ16,0 (Np)
102,98 106,42 109,70 115,65 120,36 123,05 125,30 128,05 129,07 135,27 136,7 138,30 139,44 146,55 150,04 154,27 156,4 159,26 161,54 164,61 165,81 169,56 175,07 190,4 191,96 196,76 201,70 204,06 208,005 221,46 232,81 234,40 246,73 248,52 260,22 261,00 264,76 264,88 267,54 270,63 271,54 275,77 278,04 291,3 292,77 300,13 304,21 309,1 316,8 322,52 322,56 324,69 329,69 332,35 335,37 337,7 350,71 358,25 368,62
(2) (5) (7) (6) (8) (1) (2)
Pγ+ce × 100
Multipolarity
0,0218 (5) 0,000051
0,00675 (30) 0,00533 (26)
αK
αL
αM
Am 146
αT
E1
0,0895 (18)
0,0219 (4)
0,1189 (24)
[E2]
6,86 (14)
1,91 (4)
9,44 (19)
1,127 (23) 0,0132 (3)
5,75 (12) 0,299 (6)
E2 (E1)
0,184 (4) 0,228 (5)
4,05 (8) 0,0538 (11)
[E2] E2 [E1] [M1]
0,211 0,210 0,152 5,59
(4) (4) (3) (11)
2,29 1,83 0,0339 1,108
(5) (4) (7) (22)
0,638 0,51 0,00827 0,269
(13) (1) (17) (6)
3,37 2,73 0,197 7,06
(7) (6) (4) (14)
[E1] [M1] E2 [M1 + E2] E2 [E1]
0,132 4,91 0,195 2,4 0,189 0,1066
(3) (10) (4) (22) (4) (21)
0,0292 0,971 1,095 0,98 0,961 0,0230
(6) (19) (22) (8) (19) (5)
0,00711 0,236 0,304 0,26 0,267 0,00560
(14) (5) (6) (4) (6) (11)
0,171 6,20 1,70 3,7 1,51 0,137
(4) (12) (4) (22) (3) (3)
(6) (4) (9) (8) (3) (3) (20) (3) (20) (10) (2) (6) (3) (4)
0,000023 (5) 0,00172 (5) 0,000087 (6) 0,000004 0,0000016 0,000011 0,000178 0,00011 0,000427 0,000021
(6)
(4) (8) (14) (6) (23) (3) (5) (4) (10) (3) (9) (7) (7) (3) (4) (15)
0,0000415 0,00000054 0,0000008 0,00000226 0,00313 0,00011 0,0000155 0,0000080 0,00000703 0,00000155
(20)
[E2] [E1]
(7) (6) (5) (4) (8) (22) (3)
[E1] M1 + 2,38 % E2 [M1 + E2] [M1] M2 [M1] [E1]
(8) (15) (2) (6) (6) (20) (3) (2) (4) (3)
0,000011 0,00000270 0,00000318 0,0000173
(3) (3) (2) (20) (3)
(9) (5) (26) (3)
0,00000169 (8) 0,000018 (7) 0,000055 (2)
(4) (8) (8) (4)
0,000000966 (21) 0,00000210 (31)
0,000257 0,0000018 0,0000011 0,000172 0,00084 0,00000556 0,00000139 0,00000133 0,000347
(7) (3) (2) (5) (4) (10) (5) (5) (9)
KRI /V. P. Chechev, N. K. Kuzmenko
0,162 (3) 0,0816 (16) 0,0752 2,35 1,1 1,76 5,60 1,49 0,0482
(15) (5) (10) (4) (11) (3) (10)
0,561 (11) 0,0172 (4) 0,0157 0,473 0,35 0,345 1,95 0,294 0,00975
(3) (9) (5) (7) (4) (6) (20)
0,155 (3) 0,00418 (9)
0,932 (19) 0,1045 (21)
0,00382 0,1149 0,090 0,0837 0,511 0,0711 0,00236
0,0960 2,98 1,5 2,22 8,24 1,88 0,0612
(8) (23) (7) (17) (10) (14) (5)
(19) (6) (10) (5) (17) (4) (12)
[E2]
0,0979 (20)
0,156 (3)
0,0428 (9)
0,312 (6)
[M1 + E2] E1 + 19,4 % M2
0,7 (6) 0,74 (4)
0,19 (5) 0,238 (12)
0,049 (9) 0,062 (2)
0,9 (7) 1,06 (6)
[M1 + E2] [M1] [E1] [E2]
0,6 1,072 0,0341 0,0796
(5) (21) (7) (16)
0,17 0,210 0,00671 0,0991
(5) (4) (14) (20)
0,043 0,0509 0,00162 0,0270
(9) (10) (3) (6)
0,8 1,35 0,0430 0,215
(6) (3) (9) (4)
[E1] [E1]
0,0310 (6) 0,0300 (6)
0,00607 (12) 0,00585 (12)
0,00147 (3) 0,00142 (3)
(M1 + 26,5 % E2)
0,541 (8)
0,1204 (17)
0,0297 (5)
0,702 (12)
E2 M1 + 17,3 % E2 (E2)
0,0631 (13) 0,54 (7) 0,0612 (12)
0,0611 (12) 0,113 (8) 0,0575 (11)
0,0165 (4) 0,0278 (10) 0,0156 (3)
0,147 (3) 0,69 (8) 0,140 (3)
[E1] (M1)
0,0220 (4) 0,494 (10)
0,00419 (8) 0,0963 (19)
3
0,00101 (2) 0,0233 (5)
0,0391 (8) 0,0377 (8)
0,0275 (6) 0,622 (12)
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV γ17,0 (Np) γ(−1,14) (Np) γ22,3 (Np) γ23,3 (Np) γ(−1,15) (Np) γ(−1,16) (Np) γ32,9 (Np) γ29,7 (Np) γ30,7 (Np) γ(−1,17) (Np) γ22,1 (Np) γ23,1 (Np) γ(−1,18) (Np) γ(−1,19) (Np) γ(−1,20) (Np) γ35,13 (Np) γ22,0 (Np) γ26,2 (Np) γ23,0 (Np) γ29,5 (Np) γ30,5 (Np) γ(−1,21) (Np) γ28,4 (Np) γ(−1,22) (Np) γ(−1,23) (Np) γ27,1 (Np) γ26,0 (Np) γ30,3 (Np) γ(−1,24) (Np) γ38,13 (Np) γ(−1,25) (Np) γ27,0 (Np) γ(−1,26) (Np) γ(−1,27) (Np) γ33,6 (Np) γ36,8 (Np) γ(−1,28) (Np) γ31,2 (Np) γ28,0 (Np) γ34,6 (Np) γ(−1,29) (Np) γ33,4 (Np) γ38,8 (Np) γ32,1 (Np) γ(−1,30) (Np) γ36,6 (Np) γ34,4 (Np) γ33,2 (Np) γ32,0 (Np) γ36,5 (Np) γ37,5 (Np) γ34,3 (Np) γ33,1 (Np) γ(−1,31) (Np) γ34,2 (Np) γ(−1,32) (Np) γ(−1,33) (Np) γ33,0 (Np) γ37,3 (Np)
370,94 374,83 376,65 383,81 389,0 390,61 398,64 400,78 406,35 411,27 419,33 426,47 429,9 440,63 442,81 446,15 452,6 454,66 459,68 462,34 468,12 486,05 487,13 494,39 501,39 512,5 514,0 522,06 525,14 529,17 532,44 546,12 548,15 555,25 563,46 573,94 582,89 586,59 590,09 597,19 600,26 619,01 627,18 632,93 636,9 641,32 652,73 662,40 666,2 669,83 675,78 679,79 688,72 693,46 696,14 709,42 712,5 721,96 729,72
(3) (3) (3) (3) (5) (15) (10) (15) (4) (4) (1) (7) (6) (2) (8) (10) (8) (15) (4)
(3) (5) (15) (20) (6)
(2) (20) (20) (4) (2) (2) (20) (15) (4) (2) (2) (2) (2) (13) (2) (4) (2) (5) (2) (15)
Pγ+ce × 100 0,000080 0,00000313 0,000225 0,000037 0,0000005 0,00000573 0,00000018 0,00000175 0,00000018 0,000036 0,000039 0,00000109 0,00000056 0,00000331 0,00000011 0,00000251 0,0000129 0,0000043 0,0000012 0,0000032 0,00000105 0,00000080 0,00000010 0,00000014 0,00000210 0,0000039 0,00000113 0,00000016 0,00000072 0,00000008 0,00000025 0,00000005 0,00000009 0,000000460 0,00000142 0,00000101 0,00000128 0,00000283 0,0000080 0,00000022 0,000065 0,00000056 0,00000124 0,00000021 0,0000076 0,0000410 0,00045 0,00000095 0,00000051 0,00000091 0,00000334 0,0000325 0,00000354 0,0000055 0,00000641 0,00000020 0,000197 0,00000151
Multipolarity
(4) (5) (9) (7)
αK
αL
αM
Am 146
αT
M1 + 16 % E2
0,42 (6)
0,086 (8)
0,0211 (10)
0,53 (7)
(M1) [M1 + E2]
0,466 (9) 0,25 (20)
0,0908 (18) 0,06 (3)
0,0220 (5) 0,015 (6)
0,586 (12) 0,33 (23)
[M1 + E2] [M1 + E2]
0,22 (18) 0,21 (17)
0,054 (23) 0,052 (22)
0,013 (6) 0,013 (5)
0,29 (21) 0,28 (20)
[M1 + E2] [M1 + E2]
0,19 (16) 0,19 (15)
0,047 (21) 0,045 (20)
0,012 (5) 0,011 (5)
0,26 (18) 0,25 (18)
(8) (5) (28) (4) (5) (9) (5) (3) (7) (2) (7) (2) (5) (4) (6) (6) (2) (2) (41) (2) (11) (3) (5) (2) (3) (2) (2) (21) (12) (6) (5) (6) (5) (3) (5) (4) (5) (3) (5) (25) (10) (7) (7) (7) (8) (6) (7) (3) (18) (3) (5) (6)
KRI /V. P. Chechev, N. K. Kuzmenko
[E2] [M1] [M1 + E2] [M1 + E2] [M1 + E2]
0,0357 0,279 0,15 0,15 0,15
(7) (6) (12) (12) (12)
0,0205 0,0542 0,036 0,035 0,034
(4) (11) (17) (17) (16)
0,00543 0,0131 0,009 0,009 0,008
(11) (3) (4) (4) (4)
0,0635 0,351 0,20 0,20 0,19
(13) (7) (14) (14) (14)
[M1]
0,232 (6)
0,0449 (9)
0,0109 (2)
0,291 (6)
[E1] [E1] [M1 + E2]
0,0107 (2) 0,0106 (2) 0,11 (9)
0,00195 (4) 0,00194 (4) 0,025 (13)
0,00047 (1) 0,00047 (1) 0,006 (3)
0,0133 (3) 0,0132 0,14 (10)
[E2]
0,0269 (5)
0,0124 (2)
0,00324 (6)
0,0437 (9)
[E1]
0,00947 (19)
0,00171 (3)
0,00041 (1)
0,0117 (2)
[E2] [M1 + E2]
0,0241 (5) 0,09 (7)
0,0102 (2) 0,019 (10)
0,00266 (5) 0,0027 (16)
0,0378 (8) 0,11 (8)
[E2] [E1] [M1 + E2]
0,0224 (4) 0,00818 (16) 0,08 (6)
0,00903 (18) 0,00147 (3) 0,017 (9)
0,00235 (5) 0,000351 (7) 0,0042 (20)
0,0346 (7) 0,0101 (2) 0,10 (7)
[M1 + E2] [M1 + E2]
0,07 (5) 0,07 (5)
0,016 (8) 0,015 (8)
0,0037 (10) 0,0037 (10)
0,09 (7) 0,09 (6)
[M1 + E2] [M1 + E2] (E0+M1+E2)
0,06 (5) 0,06 (5) 0,18 (4)
0,014 (8) 0,013 (7) 0,045 (15)
0,0035 (10) 0,0033 (10)
0,08 (6) 0,08 (6) 0,23 (5)
[E1] [E2,M1] [E1] [E1]
0,00647 0,06 0,00630 0,00615
[M1 + E2]
[E1] [M1]
4
(13) (4) (13) (12)
0,00114 0,012 0,00111 0,00108
(2) (7) (2) (2)
0,05 (4)
0,011 (6)
0,0056 (1) 0,079 (2)
0,00099 (2) 0,0151 (4)
0,00073 0,0030 0,000265 0,000259
(1) (15) (5) (5)
0,0028 (10)
0,00024 (1) 0,0036 (1)
0,0080 0,07 0,00776 0,00758
(2) (5) (16) (16)
0,07 (5)
0,0070 (2) 0,099 (2)
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV γ(−1,34) (Np) γ(−1,35) (Np) γ35,1 (Np) γ(−1,36) (Np) γ(−1,37) (Np) γ(−1,38) (Np) γ(−1,39) (Np) γ34,0 (Np) γ(−1,40) (Np) γ(−1,41) (Np) γ36,1 (Np) γ35,0 (Np) γ37,1 (Np) γ(−1,42) (Np) γ(−1,43) (Np) γ(−1,44) (Np) γ(−1,45) (Np) γ39,3 (Np) γ(−1,46) (Np) γ(−1,47) (Np) γ(−1,48) (Np) γ39,2 (Np) γ(−1,49) (Np) γ37,0 (Np) γ(−1,50) (Np) γ(−1,51) (Np) γ(−1,52) (Np) γ39,1 (Np) γ(−1,53) (Np) γ(−1,54) (Np) γ(−1,55) (Np) γ(−1,56) (Np) γ(−1,57) (Np) γ(−1,58) (Np) γ(−1,59) (Np) γ(−1,60) (Np) γ(−1,61) (Np) γ40,2 (Np) γ39,0 (Np) γ(−1,62) (Np) γ(−1,63) (Np) γ(−1,64) (Np) γ40,1 (Np) γ(−1,65) (Np) γ(−1,66) (Np) γ(−1,67) (Np) γ(−1,68) (Np) γ(−1,69) (Np) γ(−1,70) (Np) γ40,0 (Np) γ(−1,71) (Np) γ(−1,72) (Np) γ41,0 (Np) γ(−1,73) (Np) γ(−1,74) (Np) γ42,0 (Np) γ(−1,75) (Np) γ(−1,76) (Np) γ43,0 (Np)
731,44 736,68 737,34 740,51 742,9 745,02 750,39 755,68 759,5 763,31 766,62 770,57 772,57 774,67 777,39 780,53 782,2 786,00 789,0 792,6 794,92 801,94 803,19 805,77 811,9 819,33 822,21 828,60 835,21 838,88 841,14 843,7 846,86 847,4 851,6 854,95 856,26 861,34 861,80 870,63 882 886,53 887,68 890,38 894,47 898,17 902,61 909,95 912,4 920,88 928,95 939,2 946,06 952,72 955,91 962,19 969,09 980,84 1014,33
(5) (3)
(2) (1) (4) (10) (12)
(5) (15) (3) (20) (20) (12) (3)
(12)
(5) (10)
(20) (12)
(20)
(20)
Pγ+ce × 100 0,00000046 0,00000128 0,00000794 0,00000019 0,00000035 0,00000009 0,00000006 0,00000789 0,00000181 0,00000023 0,00000504 0,00000481 0,00000303 0,00000011 0,00000015 0,00000031 0,00000015 0,00000062 0,00000042 0,00000003 0,00000094 0,00000123 0,00000016 0,00000033 0,00000063 0,00000043 0,00000024 0,00000021 0,00000003 0,00000004 0,00000010 0,00000097 0,00000016 0,0000003 0,00000041 0,00000023 0,00000010 0,00000008 0,00000061 0,00000150 0,00000004 0,00000015 0,00000033 0,00000032 0,00000003 0,00000006 0,00000033 0,00000005 0,00000028 0,00000019 0,00000009 0,00000005 0,000000010 0,00000003 0,00000060 0,00000004 0,00000003 0,00000003 0,0000010
Am 146
Multipolarity
αK
αL
αM
αT
[E1]
0,0052 (1)
0,00091 (1)
0,000217 (4)
0,0064 (1)
[E1]
0,00507 (10)
0,00088 (2)
0,000211 (4)
0,00623 (12)
[M1]
0,0675 (14)
0,0129 (3)
0,00312 (6)
0,0847 (17)
[M1,E2]
0,037 (24)
0,008 (4)
(4) (5) (8) (3) (2) (2) (11) (5) (2) (6) (5) (5) (2) (2) (2) (0) (6) (1) (7) (3) 0,0019 (10)
0,05 (3)
(6) (6) (6) (4) (1) (1) (3) (8) (3) (6) (4) (3) (6) (3) (1) (3) (6) (5) (1) (2) (3) (1) (3) (3) (2) (1) (3) (1) (5) (1) (1) (1) (2)
KRI /V. P. Chechev, N. K. Kuzmenko
5
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
3
Am 146
Atomic Data
3.1
Np ωK ω ¯L nKL
3.1.1
: : :
0,971 0,511 0,791
(4) (20) (5)
X Radiations
Energy keV
Relative probability
Kα2 Kα1
97,069 101,059
62,82 100
Kβ3 Kβ1 00 Kβ5
113,303 114,234 114,912
} } }
Kβ2 Kβ4 KO2,3
117,463 117,876 118,429
} } }
XK
36,21
12,47
XL L` Lα Lη Lβ Lγ
3.1.2
11,89 13,76 – 13,944 15,876 16,13 – 17,79 20,12 – 22,2
Auger Electrons
Energy keV
Relative probability
Auger K KLL KLX KXY
73,50 – 83,13 90,36 – 97,28 107,10 – 114,58
100 60,2 9,06
Auger L
6,04 – 13,52
55000000
KRI /V. P. Chechev, N. K. Kuzmenko
6
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
4
Am 146
α Emissions
Energy keV α0,36 α0,34 α0,33 α0,32 α0,30 α0,29 α0,28 α0,27 α0,25 α0,24 α0,23 α0,22 α0,21 α0,20 α0,19 α0,18 α0,17 α0,16 α0,15 α0,14 α0,13 α0,12 α0,11 α0,9 α0,8 α0,6 α0,5 α0,4 α0,3 α0,2 α0,1 α0,0
4757,58 4800,99 4834,15 4888,98 4956,06 4961,63 4963,83 5007,07 5055,36 5065,97 5092,06 5099,08 5106,72 5117,21 5132,8 5155,12 5179,35 5181,63 5190,17 5217,26 5225,08 5232,6 5244,13 5280,99 5321,87 5388,25 5416,28 5442,86 5469,47 5485,56 5511,46 5544,11
(13) (13) (13) (15) (15) (14) (13) (14) (13) (15) (13) (13) (16) (13) (2) (13) (13) (13) (23) (13) (13) (3) (13) (13) (13) (13) (13) (12) (12) (12) (12) (12)
Probability × 100 0,00004 (3) 0,000086 0,0007
0,0001 0,00011 ∼ 0,0004 ∼ 0,0004
KRI /V. P. Chechev, N. K. Kuzmenko
0,0004 0,0007 0,0003 0,0009 0,0006 0,0013 0,0022 0,0005 0,014 1,66 ∼ 0,01 13,23 < 0,04 84,45 0,23 0,38
(3) (3) (3) (10) (10) (1) (1)
7
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
5
Electron Emissions
Energy keV eAL
(Np)
6,04 - 13,52
eAK
(Np) KLL KLX KXY
73,50 - 83,13 90,36 - 97,28 107,10 - 114,58
(Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np) (Np)
3,92 10,769 20,28 20,606 20,99 27,46 31,70 33,13 36,97 37,114 37,68 41,92 49,82 53,802 54,06 76,54 93,23
ec2,1 ec1,0 ec3,1 ec2,1 ec4,2 ec1,0 ec1,0 ec6,4 ec3,1 ec2,0 ec4,2 ec4,2 ec6,4 ec2,0 ec6,4 ec6,2 ec6,2
6 6.1
Am 146
L L L M L M N L M L M N M M N L M
Electrons per 100 disint. 33,4 (17) 0,000114 (16)
-
} } }
8,73 15,590 25,09 22,681 25,81 29,53 32,79 37,95 39,04 41,930 39,76 43,02 51,90 55,877 55,16 81,36 95,31
14 15,9 0,31 3,7 8,8 4,0 1,08 0,87 0,076 30,2 2,3 0,65 0,228 8,12 0,062 0,225 0,0625
(5) (21) (7) (5) (12) (6) (16) (11) (17) (22) (4) (9) (30) (25) (8) (5) (16)
Photon Emissions X-Ray Emissions Energy keV XL
(Np)
11,89 — 22,2
XKα2 XKα1
(Np) (Np)
97,069 101,059
XKβ3 XKβ1 00 XKβ5
(Np) (Np) (Np)
113,303 114,234 114,912
XKβ2 XKβ4 XKO2,3
(Np) (Np) (Np)
117,463 117,876 118,429
KRI /V. P. Chechev, N. K. Kuzmenko
Photons per 100 disint. 37,66 (17) 0,001134 (30) 0,00181 (5)
} Kα }
} } }
0,000658 (21)
K β1
} } }
0,000226 (8)
K β2
8
0
0
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
6.2
Am 146
Gamma Emissions Energy keV γ2,1 (Np) γ(−1,1) (Np) γ1,0 (Np) γ3,1 (Np) γ4,2 (Np) γ14,10 (Np) γ6,4 (Np) γ(−1,2) (Np) γ2,0 (Np) γ14,9 (Np) γ8,6 (Np) γ4,1 (Np) γ3,0 (Np) γ5,1 (Np) γ6,2 (Np) γ4,0 (Np) γ(−1,3) (Np) γ20,13 (Np) γ21,13 (Np) γ8,4 (Np) γ6,1 (Np) γ29,22 (Np) γ11,6 (Np) γ8,3 (Np) γ26,15 (Np) γ29,20 (Np) γ24,13 (Np) γ9,4 (Np) γ13,6 (Np) γ18,8 (Np) γ11,5 (Np) γ(−1,7) (Np) γ25,11 (Np) γ29,18 (Np) γ(−1,8) (Np) γ18,7 (Np) γ9,2 (Np) γ13,4 (Np) γ26,10 (Np) γ9,1 (Np) γ26,9 (Np) γ13,3 (Np) γ22,7 (Np) γ13,2 (Np) γ9,0 (Np)
26,3446 32,183 33,1963 42,704 43,420 51,01 55,56 57,85 59,5409 64,83 67,50 69,76 75,90 96,79 98,97 102,98 106,42 109,70 120,36 123,05 125,30 139,44 146,55 150,04 154,27 159,26 161,54 164,61 165,81 169,56 175,07 190,4 191,96 196,76 201,70 204,06 208,005 221,46 232,81 234,40 246,73 248,52 261,00 264,88 267,54
(2) (3) (5) (3) (3) (2) (5) (1) (2) (2) (3) (1) (3) (2) (2) (5) (7) (8) (1) (2) (8) (3) (3) (20) (20) (10) (2) (6) (3) (4) (4) (8) (14) (6) (23) (3) (5) (4) (10) (3) (7) (3) (4)
KRI /V. P. Chechev, N. K. Kuzmenko
Photons per 100 disint. 2,31 0,0174 0,1215 0,0055 0,0669 0,000026 0,0181 0,0052 35,92 0,00014 0,00042 0,0029 0,0006 0,000047 0,0203 0,0195 0,000015 0,0000049 0,0000045 0,00100 0,0041 0,0000053 0,00046 0,000073 0,0000005 0,0000014 0,0000015 0,000066 0,000023 0,00017 0,000018 0,0000022 0,0000215 0,00000049 0,0000008 0,00000206 0,000786 0,0000434 0,00000482 0,00000087 0,00000244 0,00000146 0,00000129 0,00000943 0,0000268
(8) (4) (28) (11) (29) (12) (18) (15) (17) (2) (10) (4) (16) (4) (4)
(4) (2) (11) (1) (5) (5) (3) (1) (1) (3) (5) (10)
(6) (9) (8) (9) (8) (7) (3) (6) (12) (6)
9
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV γ(−1,9) (Np) γ(−1,10) (Np) γ20,6 (Np) γ27,9 (Np) γ13,1 (Np) γ16,3 (Np) γ20,5 (Np) γ16,2 (Np) γ22,5 (Np) γ(−1,11) (Np) γ(−1,12) (Np) γ14,0 (Np) γ16,1 (Np) γ17,1 (Np) γ(−1,13) (Np) γ20,3 (Np) γ16,0 (Np) γ17,0 (Np) γ(−1,14) (Np) γ22,3 (Np) γ23,3 (Np) γ(−1,15) (Np) γ(−1,16) (Np) γ29,7 (Np) γ30,7 (Np) γ(−1,17) (Np) γ22,1 (Np) γ23,1 (Np) γ(−1,18) (Np) γ(−1,19) (Np) γ(−1,20) (Np) γ35,13 (Np) γ22,0 (Np) γ26,2 (Np) γ23,0 (Np) γ29,5 (Np) γ30,5 (Np) γ(−1,21) (Np) γ28,4 (Np) γ(−1,22) (Np) γ(−1,23) (Np) γ27,1 (Np) γ26,0 (Np) γ30,3 (Np) γ(−1,24) (Np) γ38,13 (Np) γ(−1,25) (Np)
270,63 271,54 275,77 278,04 291,3 292,77 304,21 309,1 322,56 324,69 329,69 332,35 335,37 337,7 350,71 358,25 368,62 370,94 374,83 376,65 383,81 389,0 390,61 400,78 406,35 411,27 419,33 426,47 429,9 440,63 442,81 446,15 452,6 454,66 459,68 462,34 468,12 486,05 487,13 494,39 501,39 512,5 514,0 522,06 525,14 529,17 532,44
(15) (8) (15) (2) (6) (20) (3) (3)
(3) (3) (2) (20) (3) (3) (3) (3) (3) (5) (10) (15) (4) (4) (1) (7) (6) (2) (8) (10) (8) (15) (4)
(3) (5) (15) (20)
KRI /V. P. Chechev, N. K. Kuzmenko
Am 146
Photons per 100 disint. 0,0000005 0,00000144 0,00000632 0,00000115 0,00000305 0,0000142 0,00000093 0,0000020 0,000151 0,0000018 0,0000011 0,000150 0,000496 0,00000488 0,00000139 0,00000129 0,000214 0,0000520 0,00000313 0,000137 0,0000281 0,00000049 0,00000573 0,00000014 0,00000137 0,00000018 0,0000284 0,000031 0,00000109 0,00000056 0,00000331 0,00000011 0,00000236 0,00000953 0,00000355 0,000001 0,00000269 0,00000105 0,00000062 0,00000010 0,00000014 0,0000021 0,0000038 0,00000099 0,00000016 0,00000069 0,00000008
(2) (5) (10) (3) (8) (3) (2) (3) (4) (3) (2) (4) (7) (9) (5) (5) (5) (8) (6) (3) (6) (10) (3) (5) (4) (4) (6) (5) (3) (8) (2) (7) (12) (7) (6) (6) (5) (2) (2) (4) (2) (5) (3) (5) (2)
10
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV γ27,0 (Np) γ(−1,26) (Np) γ(−1,27) (Np) γ33,6 (Np) γ36,8 (Np) γ(−1,28) (Np) γ31,2 (Np) γ28,0 (Np) γ34,6 (Np) γ(−1,29) (Np) γ33,4 (Np) γ38,8 (Np) γ32,1 (Np) γ(−1,30) (Np) γ36,6 (Np) γ34,4 (Np) γ33,2 (Np) γ32,0 (Np) γ36,5 (Np) γ37,5 (Np) γ34,3 (Np) γ33,1 (Np) γ(−1,31) (Np) γ34,2 (Np) γ(−1,32) (Np) γ(−1,33) (Np) γ33,0 (Np) γ37,3 (Np) γ(−1,34) (Np) γ(−1,35) (Np) γ35,1 (Np) γ(−1,36) (Np) γ(−1,37) (Np) γ(−1,38) (Np) γ(−1,39) (Np) γ34,0 (Np) γ(−1,40) (Np) γ(−1,41) (Np) γ36,1 (Np) γ35,0 (Np) γ37,1 (Np) γ(−1,42) (Np) γ(−1,43) (Np) γ(−1,44) (Np) γ(−1,45) (Np) γ39,3 (Np) γ(−1,46) (Np)
546,12 548,15 555,25 563,46 573,94 582,89 586,59 590,09 597,19 600,26 619,01 627,18 632,93 636,9 641,32 652,73 662,40 666,2 669,83 675,78 679,79 688,72 693,46 696,14 709,42 712,5 721,96 729,72 731,44 736,68 737,34 740,51 742,9 745,02 750,39 755,68 759,5 763,31 766,62 770,57 772,57 774,67 777,39 780,53 782,2 786,00 789,0
(6)
(2) (20) (20) (4) (2) (2) (20) (15) (4) (2) (2) (2) (2) (13) (2) (4) (2) (5) (2) (15)
(5) (3)
(2) (1) (4) (10) (12)
(5) (15) (3)
KRI /V. P. Chechev, N. K. Kuzmenko
Am 146
Photons per 100 disint. 0,00000025 0,00000005 0,00000009 0,00000044 0,00000128 0,00000101 0,00000124 0,00000280 0,00000729 0,00000022 0,000060 0,00000051 0,00000124 0,00000021 0,00000704 0,0000376 0,000367 0,00000095 0,00000051 0,00000085 0,00000331 0,0000323 0,00000354 0,00000517 0,00000641 0,00000020 0,000196 0,00000137 0,00000046 0,00000128 0,00000794 0,00000019 0,00000035 0,00000009 0,00000006 0,00000784 0,00000181 0,00000023 0,00000501 0,00000481 0,00000279 0,00000011 0,00000015 0,00000031 0,00000015 0,00000062 0,00000042
(3) (2) (2) (2) (5) (6) (5) (6) (11) (3) (2) (2) (5) (3) (10) (9) (6) (7) (7) (5) (8) (6) (8) (8) (19) (3) (5) (5) (4) (5) (11) (3) (2) (2) (11) (5) (2) (6) (7) (4) (2) (2) (2)
(6)
11
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Energy keV γ(−1,47) (Np) γ(−1,48) (Np) γ39,2 (Np) γ(−1,49) (Np) γ37,0 (Np) γ(−1,50) (Np) γ(−1,51) (Np) γ(−1,52) (Np) γ39,1 (Np) γ(−1,53) (Np) γ(−1,54) (Np) γ(−1,55) (Np) γ(−1,56) (Np) γ(−1,57) (Np) γ(−1,58) (Np) γ(−1,59) (Np) γ(−1,60) (Np) γ(−1,61) (Np) γ40,2 (Np) γ39,0 (Np) γ(−1,62) (Np) γ(−1,63) (Np) γ(−1,64) (Np) γ40,1 (Np) γ(−1,65) (Np) γ(−1,66) (Np) γ(−1,67) (Np) γ(−1,68) (Np) γ(−1,69) (Np) γ(−1,70) (Np) γ40,0 (Np) γ(−1,71) (Np) γ(−1,72) (Np) γ41,0 (Np) γ(−1,73) (Np) γ(−1,74) (Np) γ42,0 (Np) γ(−1,75) (Np) γ(−1,76) (Np) γ43,0 (Np)
7
792,6 794,92 801,94 803,19 805,77 811,9 819,33 822,21 828,60 835,21 838,88 841,14 843,7 846,86 847,4 851,6 854,95 856,26 861,34 861,80 870,63 882 886,53 887,68 890,38 894,47 898,17 902,61 909,95 912,4 920,88 928,95 939,2 946,06 952,72 955,91 962,19 969,09 980,84 1014,33
(20) (20) (12) (3)
(12)
(5) (10)
(20) (12)
(20)
(20)
Am 146
Photons per 100 disint. 0,00000003 0,00000094 0,00000123 0,00000016 0,00000031 0,00000063 0,00000043 0,00000024 0,00000021 0,00000003 0,00000004 0,00000010 0,00000097 0,00000016 0,00000027 0,00000041 0,00000023 0,00000010 0,00000008 0,00000061 0,00000150 0,00000004 0,00000015 0,00000033 0,00000032 0,00000003 0,00000006 0,00000033 0,00000005 0,00000028 0,00000019 0,00000009 0,00000005 0,000000010 0,00000003 0,00000060 0,00000004 0,00000003 0,00000003 0,0000010
(1) (7) (3) (6) (6) (6) (4) (1) (1) (3) (8) (3) (3) (6) (4) (3) (3) (6) (4) (1) (3) (6) (5) (1) (2) (3) (1) (3) (3) (2) (1) (2) (1) (5) (1) (1) (1) (2)
Main Production Modes Pu − 241(β − )Am − 241
KRI /V. P. Chechev, N. K. Kuzmenko
12
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
8
Am 146
References - J. K. Beling, J. O. Newton, B. Rose. Phys. Rev. 86 (1952) 797 (gamma-ray emission probabilities.) - J. F. TURNER. Phil. Mag. 46 (1955) 687 (gamma-ray emission probabilities.) - H. Jaffe, T. O. Passell, C. I. Browne, I. Perlman. Phys. Rev. 97 (1955) 142 (gamma-ray emission probabilities.) - R. B. Day. Phys. Rev. 97 (1955) 689 (gamma-ray emission probabilities.) - J. M. HOLLANDER, W. G. Smith, J. O. Rasmussen. Phys. Rev. 102 (1956) 1372 (gamma-ray emission probabilities.) - L. L. Goldin, G. I. Novikova, E. F. Tretyakov. Conf. Acad. Sci. USSR Moscow (1956) 226 (energies of alpha-particles, alpha-particle emission probabilities.) - S. Rosenblum, M. Valadares, J. Milsted. J. Phys. Radium 18 (1957) 609 (energies of alpha-particles.) - L. B. Magnusson. Phys. Rev. 107 (1957) 161 (gamma-ray energies and emission probabilities.) - P. S. Samoilov. Columbia Tech. Transl. (Izv.Akad.Nauk SSSR, ser.fiz. 23 (1959) 1416) 23 (1960) 1401 (gamma-ray energy, gamma transition probabilities and multipolarities.) - F. Asaro, F. S. Stephens, J. M. Hollander, I. Perlman. Phys. Rev. 117 (1960) 494 (anomalous electric dipole gamma-ray transitions.) - C. F. Leang. Comp. Rend. Acad. Sci. (Paris) 255 (1962) 3155 (energies of alpha-particles.) - J. L. Wolfson, J. H. Park. Can. J. Phys. (also Erratum Can. J. Phys. 48(1970)2782) 42 (1964) 1387 (gamma-ray energies and multipolarities.) - S. A. Baranov, V. M. Kulakov, V. M. Shatinsky. Nucl. Phys. 56 (1964) 252 (alpha-particle energies and emission probabilities.) - W. Michaelis. Z. Phys. 186 (1965) 42 (alpha particle energies and emission probabilities.) - G. BERTOLINI, F. Cappellani, G. Restelli. Nucl. Instrum. Methods 32 (1965) 86 (gamma-ray emission probabilities.) - L. D. McIsaac. Report IDO-17052 (1965) 31 (gamma-ray emission probabilities.) - W. Yamazaki, J. M. Hollander. Nucl. Phys. 84 (1966) 505 (internal conversion probabilities.) - C. M. Lederer, J. K. Poggenburg, F. Asaro, J. O. Rasmussen, I. Perlman. Nucl. Phys. 84 (1966) 481 (internal conversion coefficients.) - H. -C. Pauli, K. Alder. Z. Physik 202 (1967) 255 (anomalous electric dipole gamma-ray transitions.) - C. Gunther, D. R. Parsignault. Nucl. Phys. A104 (1967) 588 (XK-ray emission probabilities.) - C. Briancon, M. Valadares, R. J. Walen. Comp. Rend. 265B (1967) 1496 (gamma-ray emission probabilities.) - F. L. Oetting, S. R. Gunn. J. Inorg. Nucl. Chem. 29 (1967) 2659 (half-life.) - L. N. Kondratev, E. F. Tretyakov. Bull. Acad. Sci. URSS, Phys. Ser. 30 (1967) 393 (internal conversion probabilities.) - R. E. Stone, E. K. Hulet. J. Inorg. Nucl. Chem. 30 (1968) 2003 (half-life.) - R. W. Jewell, W. John, R. Massey, B. G. Saunders. Nucl. Instrum. Methods 62 (1968) 68 (gamma-ray energies.) - L. C. Brown, R. C. Propst. J. Inorg. Nucl. Chem. 30 (1968) 2591 (half-life.) - S. A. Baranov, V. M. Kulakov, V. M. Shatinskii. Sov. J. Nucl. Phys. 7 (1968) 442. (energies of alpha-particles.) - R. Kamoun, R. Ballini, S. Bergstrom-Rohlin, J. -M. Kuchly, P. Siffert. Comp. Rend. Acad. Sci. (Paris) B266 (1968) 1241 (energies of alpha-particles.)
KRI /V. P. Chechev, N. K. Kuzmenko
13
10/10/2000 − 7/7/2010
241 95
LNE – LNHB/CEA – Table de Radionucl´ eides
Am 146
- A. PEGHAIRE. Nucl. Instrum. Methods 75 (1969) 66 (gamma-ray emission probabilities.) - G. C. Nelson, B. G. Saunders. Nucl. Instrum. Methods 84 (1970) 90 (gamma-ray energies.) - V. N. Grigorev, A. P. Feresin. Sov. J. Nucl. Phys. 12 (1970) 361 (anomalous electric dipole gamma-ray transitions.) - J. E. CLINE. IN-1448 Rev. (1971) (1971) (gamma-ray emission probabilities.) - R. L. Watson, T. K. Li. Nucl. Phys. A178 (1971) 201 (LX-ray emission probabilities.) - B. Grennberg, A. Rytz. M´etrologia 7 (1971) 65 (energies of alpha-particle.) - E. Karttunen, H. U. Freund, R. W. Fink. Phys. Rev. A4 (1971) 1695 (MX-ray emission probability.) - R. J. Gehrke, R. A. Lokken. Nucl. Instrum. Methods 97 (1971) 219 (XL- and gamma -ray emission probabilities.) - J. Jove, R. Robert. Radiochem. Radioanal. Letters 10 (1972) 139 (half-life.) - R. L. Heath. Report ANCR 1000 (1974) 2 (gamma - ray energies and emission probabilities.) - W. J. Gallagher, S. J. Cipolla. Nucl. Instrum. Methods 122 (1974) 405 (LX- ray emission probabilities.) - J. L. Campbell, L. A. McNelles. Nucl. Instrum. Methods 117 (1974) 519 (LX- and gamma - ray emission probabilities.) - W. W. Strohm, K. C. Jordan. Trans. Am. Nucl. Soc. 18 (1974) 185 (half-life.) - V. G. Polyukhov, G. A. Timofeev, P. A. Privalova, P. F. Baklanova. Soviet J. At. Energy 36 (1974) 402 (half-life.) - H. Ramthun, W. Muller. Int. J. Appl. Radiat. Isotop. 26 (1975) 589 (half-life.) - J. Legrand, J. P. Perolat, C. Bac, J. Gorry. Int. J. Appl. Radiat. Isotop. 26 (1975) 179 (gamma - ray emission probabilities.) - J. Plch, J. Zderadicka, L. Kokta. Czech. J. Phys. 26B (1976) 1344 (gamma-ray emission probability.) - R. Gunnink, J. E. Evans, A. L. Prindle. Report UCRL-52139 (1976) (LX-, KX- and gamma-ray emission probabilities.) - A. Genoux-Lubain, G. Ardisson. Radiochem. Radioanal. Letters 33 (1978) 59 (gamma-ray energies and emission probabilities.) - V. V. Ovechkin. Bull. Acad. Sci. URSS, Ser. Phys. 42(1) (1978) 82 (gamma-ray energies and emission probabilities.) - A. Genoux-Lubain, G. Ardisson. Comp. Rend. Acad. Sci. (Paris) B287 (1978) 13 (Gamma-ray emission energies and intensities.) - C. Ardisson, A. Genoux-Lubain, V. Barci, G. Ardisson. Radiochem. Radioanal. Letters 40 (1979) 207 (gamma-ray energies.) - D. D. Cohen. Nucl. Instrum. Methods 178 (1980) 481 (LX-ray emission probabilities.) - G. Barreau, H. G. Borner, T. von Egidy, R. W. Hoff. Z. Phys. A308 (1982) 209 (KX-ray energies.) - K. Debertin, W. Pessara. Int. J. Appl. Radiat. Isotop. 34 (1983) 515 (gamma-ray emission probabilities.) - J. M. R. Hutchinson, P. A. Mullen. Int. J. Appl. Radiat. Isotop. 34 (1983) 543 (gamma-ray emission probabilities.) - I. Ahmad, J. Hines, J. E. Gindler. Phys. Rev. C27 (1983) 2239 (LX-, KX-ray energies and KX-, gamma-ray emission probabilities.) - I. Ahmad. Nucl. Instrum. Methods 223 (1984) 319 (alpha-particle emission probabilities.) - V. V. Ovechkin, A. E. Khokhlov. Izv. Akad. Nauk SSSR, Ser. Fiz. 48 (1984) 1032 (gamma-ray energies and emission probabilities.) - G. Bortels, P. Collaers. Appl. Rad. Isotopes 38 (1987) 831 (alpha-particle emission probabilities.)
KRI /V. P. Chechev, N. K. Kuzmenko
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LNE – LNHB/CEA – Table de Radionucl´ eides
Am 146
- B. Denecke. Appl. Rad. Isotopes 38 (1987) 823 (gamma-ray emission probabilities.) - V. P. Chechev, N. K. Kuzmenko, V. O. Sergeev, K. P. Artamonova. Evaluated decay data, Energoatomizdat Ed. Moscow (1988) (gamma-ray energies.) - D. D. Cohen. Nucl. Instrum. Meth. Phys. Res. A267 (1988) 492 (LX-ray emission probabilities.) - J. H. Hubbell. Report NIST 89-4144 (1989) (M fluorescence yield.) - L. J. Martin, P.A.Burns. Nucl. Instrum. Meth. Phys. Res. A312 (1992) 146 (gamma-ray emission probabilities.) ´py. Nucl. Instrum. Meth. Phys. Res. A312 (1992) 323 - C. J. Bland, J. Morel, E. Etcheverry, M. C. Le (LX-ray emission probabilities.) ´py, K. Debertin, H. Janssen, U. Scho ¨ tzig. Report PTB- Ra-31 (1993) - M. C. Le (L X-ray emission intensities.) - I. Ahmad. Private communication, cited in 1994Bl12 (1993) (alpha-particle emission probabilities.) ´py, B. Duchemin, J. Morel. Nucl. Instrum. Meth. Phys. Res. A353 (1994) 10 - M. C. Le (LX-ray emission probabilities.) - C. J. Bland. Nucl. Instrum. Meth. Phys. Res. A339 (1994) 180 (alpha-particle emission probabilities.) - Y. A. Akovali. Nucl. Data Sheets 74 (1995) 461 (Decay scheme.) - C. C. Bueno, J. A. C.Gonc ¸ alves, M. D. S. Santos. Nucl. Instrum. Meth. Phys. Res. A371 (1996) 460 (alpha-particle emission probabilities.) - A. M. Sanchez, P. R. Montero, F. V. Tome. Nucl. Instrum. Meth. Phys. Res. A369 (1996) 593 (alpha-particle emission probabilities.) - P. N. Johnson. Nucl. Instrum. Meth. Phys. Res. A369 (1996) 107 (evaluated gamma-ray emission probabilities and internal conversion coefficients.) - A. Abdul-Hadi. J. Radional. Nucl. Chem 231 (1998) 147 (Gamma-ray emission energies and intensities.) - A. Kovalik, E. A. Yakushev, V. M. Gorozhankin, M. Novgorodov, M. Rysavy. J. Phys. (London) G24 (1998) 2247 (Conv. Elec. emission energies and intensities.) - Y. Jang, J. Ni. Nucl. Instrum. Meth. Phys. Res. A413 (1998) 239 (Alpha emission intensities.) ¨ nfeld, G. Rodloff. Report PTB 6.11-1, Braunscheig (1999) - E. Scho (XK-ray energies and emission probabilities.) - N. E. Holden, D. C. Hoffman. Pure Appl. Chem. 72 (2000) 1525 (241Am spontaneous fission half-life.) - R. G. Helmer, C. van der Leun. Nucl. Instrum. Meth. Phys. Res. A450 (2000) 35 (gamma-ray energies.) ¨ nfeld, U. Scho ¨ tzig. Appl. Rad. Isotopes 54 (2001) 785 - E. Scho (calculated absolute emission probabilities of LX-rays.) ´, R. Helmer, V. Chiste ´. J. Nucl. Sci. Tech., suppl.2 (2002) 481 - M.M. Be (Saisinuc software.) - G. Audi, A. H. Wapstra, C. Thibault. Nucl. Phys. A729 (2003) 337 (Q value.) - A. Iwahara, M. A. L. da Silva, A. E. Carvalho Filho, E. M. de Oliveira Bernardes, J. U. Delgado. Appl. Rad. Isotopes 63 (2005) 107 (absolute emission probabilities of gamma-rays.) - M. S. Basunia. Nucl. Data Sheets 107 (2006) 2323 (241Am decay scheme, 237Np level energies and gamma-ray transition multipolarities.) ´py, J.Plagnard, L.Ferreux. Appl. Rad. Isotopes 66 (2008) 715 - M. C. Le (absolute emission probabilities of LX-rays.) ´. Appl. Rad. Isotopes 66 (2008) 722 - V. M. Gorozhankin, M. -M.Be (ICC for anomalous E1 gamma-ray transitions.) - T. Kibedi, W. Burrows, M. B. Trzhaskovskaya, P. M. Davidson, C. W. Nestor Jr.. Nucl. Instrum. Methods Phys. Res. A589 (2008) 202 (Band-Raman ICC for gamma-ray transitions.)
KRI /V. P. Chechev, N. K. Kuzmenko
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LNE – LNHB/CEA – Table de Radionucl´ eides
Am 146
¨ nfeld, U. Scho ¨ tzig. Appl. Rad. Isotopes 54 (2001) 785 - E. Scho (calculated absolute emission probabilities of LX-rays.) ´, R. Helmer, V. Chiste ´. J. Nucl. Sci. Tech., suppl.2 (2002) 481 - M.M. Be (Saisinuc software.) - G. Audi, A. H. Wapstra, C. Thibault. Nucl. Phys. A729 (2003) 337 (Q value.) - A. Iwahara, M. A. L. da Silva, A. E. Carvalho Filho, E. M. de Oliveira Bernardes, J. U. Delgado. Appl. Rad. Isotopes 63 (2005) 107 (absolute emission probabilities of gamma-rays.) - M. S. Basunia. Nucl. Data Sheets 107 (2006) 2323 (241Am decay scheme, 237Np level energies and gamma-ray transition multipolarities.) ´py, J.Plagnard, L.Ferreux. Appl. Rad. Isotopes 66 (2008) 715 - M. C. Le (absolute emission probabilities of LX-rays.) ´. Appl. Rad. Isotopes 66 (2008) 722 - V. M. Gorozhankin, M. -M.Be (ICC for anomalous E1 gamma-ray transitions.) - T. Kibedi, W. Burrows, M. B. Trzhaskovskaya, P. M. Davidson, C. W. Nestor Jr.. Nucl. Instrum. Methods Phys. Res. A589 (2008) 202 (Band-Raman ICC for gamma-ray transitions.)
KRI /V. P. Chechev, N. K. Kuzmenko
16
10/10/2000 − 15/10/2009
241 95
LNE-LNHB/CEA - Table de Radionucléides 5/2 - ; 0 0
Am146
432,6 (6) a
241
α 95
Am
146
γ Emission intensities per 100 disintegrations
0
,0
0
0
0
1 0
43 0 42 41 40
39 38
37 36
,0
0
0 0
0
0
0
0
4
0
0
1014 1 0
8 3 9 0 3 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
962 946
2 3 1 1 6 2 2 6 0 1 0 0 9 1 0 0 0 0 6 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 (5/2,7/2)+ ,0 ,0 5 7 9 1 0 0 8 3 7 3 11/2 0 1 2 0 8 4 1 1 0 0 0 0 2 0 5 0 0 0 0 0 1 7 0 5 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 4 1 ,0 ,0 ,0 ,0 0 0 0 0 1 9 8 0 0 0 0 0 0 0 0 + 0 7 (7/2,9/2) 4 0 0 , , ,0 ,0 0 0 0 0 0 0 0 0 0 0 9/2 0 0 0 0 0 0 ,0 ,0 ,0 0 0 0
920,88
; 861,65 ; 853,36
; 805,77 ; 799,82
0,00004
770,57
35
0,0007 5/2 - ; 721,961
33
0,0013 (7/2) - ; 324,42 13
0,014 11/2 - ; 225,957 8
1,66 9/2 - ; 158,497 6
0,01
11/2+ ; 129,99
5 9/2+ ; 75,899 5/2 - ; 59,54092
56 ps 3 67 ns 2
7/2+ ; 33,19629
54 ps 1 2,144 (7) 10^6 a
0,04 84,45 0,23 0,38
5/2+ ; 0 0
237 93
Np
144
α
Q = 5637,82 keV % α = 100
KRI / V.P. Chechev, N.K. Kuzmenko
Scheme page : 1/6
10/10/2000 - 29/09/2009
241 95
LNE-LNHB/CEA - Table de Radionucléides 5/2 - ; 0 0
Am146
432,6 (6) a
241
α
Am
95
146
γ Emission intensities per 100 disintegrations 9 1 7 4 2 6 3 1 8 7 7 3 5 7 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 4 0 0 0 0 0 4 3 0 7 2 6 0 6 6 3 9 0 0 3 0 1 34 0 0 0 0 0 0 0 0 0 0 ,0 ,0 ,0 ,0 ,0 0 0 0 0 0 33
32
0,000086 7/2 - ; 755,685
0,0007 5/2 - ; 721,961
4 5 2 9 1 0 0 0 0 0 4 0 0 2 0 0 1 0 ,0 ,0 0 0 0 0 0 ,0 0
(5/2,7/2)+ ; 666,19
7 9 9 3 6 9 1 2 0 9 4 0 0 0 3 4 4 1 0 0 0 5 1 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 0 0 0 0
31
30 29
(9/2) - ; 646,03
11/2+ ; 597,99 13/2+ ; 592,33
7/2+ ; 459,693 9/2+ ; 452,545
23 22
0,0004 0,0004 0,0004
(11/2) - ; 434,12
20
0,0007 15/2 - ; 395,53 18
0,0005 3/2 - ; 267,556
5,2 ns 9
13/2+ ; 191,53 7
1,66 9/2 - ; 158,497
6
0,01 11/2+ ; 129,99
13,23
5
80 ps
7/2 - ; 102,959
0,04
4 9/2+ ; 75,899
56 ps 3 67 ns 2 54 ps
2,144 (7) 10^6 a
84,45
5/2 - ; 59,54092
0,23 7/2+ ; 33,19629
1
0,38 5/2+ ; 0
0
237 93
Np
144
α
Q = 5637,82 keV % α = 100
KRI / V.P. Chechev, N.K. Kuzmenko
Scheme page : 2/6
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241 95
LNE-LNHB/CEA - Table de Radionucléides 5/2 - ; 0 0
Am146
432,6 (6) a
241
α 95
Am
146
γ Emission intensities per 100 disintegrations 2 6 8 0 2 0 0 0 0 0 0 0 0 ,0 ,0 0 0 28
27
26 25
(7/2) - ; 590,09
5 5 1 1 2 1 2 0 0 0 0 0 0 0 0 0 0 0 0 0 ,0 ,0 ,0 0 0 0 2 4 3 5 8 4 5 8 0 4 2 9 3 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 5 0 0 0 0 0 1 ,0 ,0 ,0 ,0 ,0 2 0 0 0 0 0 0 5 0 1 0 0 0 ,0 0 0 0 ,0 0
0,0001 (5/2) - ; 546,12
(3/2) - ; 514,19
17/2 - ; 497,01 5 1 5 8 1 3 9 6(9/2) ; 486,21 2 3 0 2 4 3 0 0 0 1 1 7 8 2 0 0 0 0 5 3 2 0 0 0 0 0 1 1 0 0 ,0 ,0 ,0 0 0 0 0 0 0 0 0 0 0 0 0 0 7/2+ ; 459,693 0 0 , , ,0 ,0 ,0 0 0 0 0 0 9/2+ ; 452,545
24
23 22
0,00011
0,0004 0,0004
0,0006 (5/2) - ; 359,7 15
0,0013 (7/2) - ; 324,42 13
0,0022
13/2 - ; 305,05 11 1/2 - ; 281,356 10
5,2 ns
0,0005
3/2 - ; 267,556
9
0,014 11/2 - ; 225,957 8
13/2+ ; 191,53 7
0,01 11/2+ ; 129,99 5
13,23 7/2 - ; 102,959
80 ps 4
0,04 9/2+ ; 75,899
56 ps 3
84,45
5/2 - ; 59,54092
67 ns 2
0,23 7/2+ ; 33,19629
54 ps 1
0,38 2,144 (7) 10^6 a
5/2+ ; 0 0
237 93
Np
144
α
Q = 5637,82 keV % α = 100
KRI / V.P. Chechev, N.K. Kuzmenko
Scheme page : 3/6
10/10/2000 - 29/09/2009
241 95
LNE-LNHB/CEA - Table de Radionucléides 5/2 - ; 0 0
Am146
432,6 (6) a
241
α 95
Am
146
γ Emission intensities per 100 disintegrations
0 21
0
0
4
5
2 3 9 3 9 2 6 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
4 0
9
444,78
0,0004
(11/2) - ; 434,12
20 7 0 1 0 0 0 0 0 0 0 , , 0 0 18
17 16
2
0
6
0,0007 15/2 - ; 395,53
8 8 4 2 0 5 2 0 0 4 2 6 4 0 0 1 0 9 1 0 0 0 0 4 2 0 0 , , 0 0 0 0 0 0 0 0 0 0 ,0 ,0 ,0 ,0 0 0 0 0
15
3/2+ ; 370,928 5/2+ ; 368,602 (5/2) - ; 359,7 6 2 4 5 0 1 1 0 0 0 0 0 0 ,0 ,0 ,0 0 0 0
1 ns 14
1/2+ ; 332,376
0,0003 0,0009 0,0006
0,0013
(7/2) - ; 324,42
13
0,0022 13/2 - ; 305,05
11 1/2 - ; 281,356 10
0,0005
3/2 - ; 267,556
5,2 ns 9
0,014 11/2 - ; 225,957 8
13/2+ ; 191,53 7
1,66 9/2 - ; 158,497 6
0,01 11/2+ ; 129,99 5
0,04 56 ps 67 ns
9/2+ ; 75,899
84,45
3 5/2 - ; 59,54092 2
0,23 7/2+ ; 33,19629
54 ps 1
0,38 2,144 (7) 10^6 a
5/2+ ; 0 0
237 93
Np
144
α
Q = 5637,82 keV % α = 100
KRI / V.P. Chechev, N.K. Kuzmenko
Scheme page : 4/6
10/10/2000 - 29/09/2009
241 95
LNE-LNHB/CEA - Table de Radionucléides 5/2 - ; 0 0
Am146
432,6 (6) a
241
α 95
Am
146
γ Emission intensities per 100 disintegrations 6 3 5 4 4 4 0 3 3 1 9 3 2 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 13 12
0,0013 (7/2) - ; 324,42
8 6 1 4 0 0 0 0 0 ,0 ,0 0 0
316,8
0,0022 13/2 - ; 305,05
11
10
7 8 8 6 6 0 6 6 8 0 2 0 7 0 0 0 0 0 0 0 0 0 0 ,0 ,0 ,0 ,0 0 0 0 0
1/2 - ; 281,356
0,0005 3/2 - ; 267,556
5,2 ns 9
2 7 4 0 0 1 0 0 0 0 ,0 ,0 ,0 0 0 0
3
0,014 11/2 - ; 225,957
8
13/2+ ; 191,53 7
1 3 1 8 0 4 1 2 0 ,0 ,0 ,0 0 0 0
1,66 9/2 - ; 158,497
6
0
,0
0
0
4 0
7
0,01 11/2+ ; 129,99
5
13,23 80 ps
7/2 - ; 102,959 4
0,04 56 ps
9/2+ ; 75,899 3
84,45 5/2 - ; 59,54092
67 ns 2
0,23 7/2+ ; 33,19629
54 ps 1
0,38 2,144 (7) 10^6 a
5/2+ ; 0 0
237 93
Np
144
α
Q = 5637,82 keV % α = 100
KRI / V.P. Chechev, N.K. Kuzmenko
Scheme page : 5/6
10/10/2000 - 29/09/2009
241 95
LNE-LNHB/CEA - Table de Radionucléides
5/2 - ; 0 0
9 9 5 6 2 9 6 0 1 ,0 ,0 ,0 0 0 0
80 ps
Am
146
13,23
4
0,04 9/2+ ; 75,899
3
1 ,9 ,3 5 2 3
2
84,45 5/2 - ; 59,54092
67 ns 2
0
54 ps
95
7/2 - ; 102,959
5 6 5 0 0 0 ,0 ,0 0 0
56 ps
432,6 (6) a
241
α γ Emission intensities per 100 disintegrations
Am146
,1
1 2
5
0,23 7/2+ ; 33,19629
1
0,38 2,144 (7) 10^6 a
5/2+ ; 0 0
237 93
Np
144
α
Q = 5637,82 keV % α = 100
KRI / V.P. Chechev, N.K. Kuzmenko
Scheme page : 6/6
10/10/2000 - 29/09/2009