ADOPTED LEVELS, GAMMAS for 100Nb
Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 172, 1 (2021) | Cutoff date: 31-Jan-2021
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=6396 keV 8 | S(n)= 5533 keV 14 | S(p)= 9466 keV 13 | Q(α)= -3886 keV 10 | ||
Reference: 2017WA10 |
References: | |||
A | 100Zr β- decay (7.1 S) | B | 100Nb IT decay (12.4 μs) |
C | 252Cf SF decay | D | 100Mo(t,3He) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | A C | 1+ | 1.4 s 2 % β- = 100 | |||||
67.4 8 | C | (2+) | 67.4 | 100 | 0.0 | 1+ | ||
159.1 8 | C | (3+) | 91.6 159.1 | 100 10.8 | 67.4 0.0 | (2+) 1+ | ||
261.3 10 | C | (4+) | 102.1 194.0 | 100 5.3 | 159.1 67.4 | (3+) (2+) | ||
314 23 | B D | (5)+ | 2.99 s 11 % β- = 100 | |||||
348 23 | B | (4-,5-,6-) | 0.41 µs 6 % IT = 100 | 34.3 | 100 | (E1) | 314 | (5)+ |
368.2 11 | C | (5+) | 106.9 209.1 | 100 12.9 | 261.3 159.1 | (4+) (3+) | ||
400.52 6 | A | 1+ | 90 ps 30 | 400.50 6 | 100 | [M1] | 0.0 | 1+ |
471.39 7 | A | (1+) | 471.48 9 | 100 | 0.0 | 1+ | ||
492.6 15 | C | 124.4 | 100 | 368.2 | (5+) | |||
498.08 25 | A | (0:3+) | 498.08 25 | 100 | 0.0 | 1+ | ||
504.30 5 | A | 1+ | 33.01 10 103.73 10 504.29 5 | 0.88 16 2.6 4 100 13 | (M1) [M1] | 471.39 400.52 0.0 | (1+) 1+ 1+ | |
521 23 | B | (5-,6-,7-) | 207 ps 14 | 173.3 2 | 100 | M1 | 348 | (4-,5-,6-) |
542.4 12 | C | (6+) | 174.1 281.2 | 100 18.2 | 368.2 261.3 | (5+) (4+) | ||
653.92 12 | A | (0:3+) | 253.4 1 | 100 | 400.52 | 1+ | ||
703.72 11 | A | (0:3+) | 303.2 1 703.7 4 | 55 8 100 19 | 400.52 0.0 | 1+ 1+ | ||
706 23 | B | (6-) | 185.4 2 358.6 2 392.3 2 | 100 88 60 | M1 | 521 348 314 | (5-,6-,7-) (4-,5-,6-) (5)+ | |
734 23 | B | (8-) | 12.4 µs 3 % IT = 100 | 28 | 100 | (E2) | 706 | (6-) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
771.9 13 | C | (7+) | 229.7 403.6 | 100 26 | 542.4 368.2 | (6+) (5+) | ||
835.7 18 | C | 343.1 | 100 | 492.6 | ||||
1058.8 14 | C | (8+) | 286.9 516.4 | 100 27 | 771.9 542.4 | (7+) (6+) | ||
1235.3 18 | C | 742.6 | 100 | 492.6 | ||||
1525.9 21 | C | 290.6 | 100 | 1235.3 | ||||
0+X | D | |||||||
25+X 10 | D | |||||||
131+X 10 | D | |||||||
210+X 15 ? | D | |||||||
348+X 15 | D | |||||||
410+X 15 | D | |||||||
450+X 20 | D | |||||||
520+X 20 | D | |||||||
565+X 10 | D | |||||||
595+X 20 ? | D | |||||||
680+X 20 | D | |||||||
720+X 20 ? | D | |||||||
784+X 20 | D | |||||||
820+X 20 | D | |||||||
865+X 20 | D | |||||||
893+X 20 | D | |||||||
945+X 20 | D | |||||||
1040+X 20 | D | |||||||
1075+X 20 | D | |||||||
1136+X 20 | D | |||||||
1180+X 25 | D | |||||||
1260+X 30 | D | |||||||
1300+X 30 | D |
E(level): From least-squares fit to Eγ data for levels with γ-ray emission. Others are from (t,3He)
M(γ): From ce data in 100Nb IT decay, unless otherwise noted
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - Kπ=1+, πg9/2~#νg7/2,α=0. | |||||||
67.4 8 | (2+) | ||||||
261.3 10 | (4+) | 102.1 194.0 | 100 5.3 | 159.1 67.4 | (3+) (2+) | ||
542.4 12 | (6+) | 174.1 281.2 | 100 18.2 | 368.2 261.3 | (5+) (4+) | ||
1058.8 14 | (8+) | 286.9 516.4 | 100 27 | 771.9 542.4 | (7+) (6+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - Kπ=1+ πg9/2~#νg7/2,α=1. | |||||||
159.1 8 | (3+) | ||||||
368.2 11 | (5+) | 106.9 209.1 | 100 12.9 | 261.3 159.1 | (4+) (3+) | ||
771.9 13 | (7+) | 229.7 403.6 | 100 26 | 542.4 368.2 | (6+) (5+) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Conversion Coefficient | Additional Data |
348 | (4-,5-,6-) | 0.41 µs 6 % IT = 100 | 34.3 | (E1) | 2.55 | B(E1)(W.u.)=5.3E-6 +12-9, α=2.55 |
400.52 | 1+ | 90 ps 30 | 400.50 6 | [M1] | B(M1)(W.u.)=0.0038 +19-10 | |
504.30 | 1+ | 33.01 10 | (M1) | 5.46 | α=5.46 | |
1+ | 103.73 10 | [M1] | 0.204 | α=0.204 | ||
521 | (5-,6-,7-) | 207 ps 14 | 173.3 2 | M1 | 0.0505 | B(M1)(W.u.)=0.0195 13, α=0.0505 |
706 | (6-) | 185.4 2 | M1 | 0.0422 | α=0.0422 | |
734 | (8-) | 12.4 µs 3 % IT = 100 | 28 | (E2) | 110 | B(E2)(W.u.)=0.87 16, α=110 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 1+ | 1.4 s 2 % β- = 100 | Probable configuration=πg9/2νg7/2. |
67.4 | (2+) | E(level): Kπ=1+, πg9/2~#νg7/2,α=0. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
159.1 | (3+) | E(level): Kπ=1+ πg9/2~#νg7/2,α=1. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
261.3 | (4+) | E(level): Kπ=1+, πg9/2~#νg7/2,α=0. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
314 | (5)+ | 2.99 s 11 % β- = 100 | XREF: d(?). |
368.2 | (5+) | E(level): Kπ=1+ πg9/2~#νg7/2,α=1. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
498.08 | (0:3+) | Jπ(level): 2+,3+ less likely from log ft=6.0-6.8 from 0+, but β feeding is quite weak which could be affected by weak unobserved γ-ray feeding from higher levels. | |
542.4 | (6+) | E(level): Kπ=1+, πg9/2~#νg7/2,α=0. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
653.92 | (0:3+) | Jπ(level): 2+,3+ less likely from log ft=6.0-6.8 from 0+, but β feeding is quite weak which could be affected by weak unobserved γ-ray feeding from higher levels. | |
703.72 | (0:3+) | Jπ(level): 2+,3+ less likely from log ft=6.0-6.8 from 0+, but β feeding is quite weak which could be affected by weak unobserved γ-ray feeding from higher levels. | |
771.9 | (7+) | E(level): Kπ=1+ πg9/2~#νg7/2,α=1. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
1058.8 | (8+) | E(level): Kπ=1+, πg9/2~#νg7/2,α=0. Jπ(level): Proposed in 252Cf SF decay based on band structure. | |
450+X | E(level): Unresolved structure. | ||
520+X | E(level): Unresolved structure. | ||
595+X | E(level): Unresolved structure. | ||
865+X | E(level): Unresolved structure. | ||
945+X | E(level): Unresolved structure. | ||
1040+X | E(level): Unresolved structure. | ||
1075+X | E(level): Unresolved structure. |
E(level) | E(gamma) | Comments |
348 | 34.3 | M(γ): proposed by 1999Ge01 from ce spectrum and also based on the 28γ(E2)-185γ(M1)-173γ(M1) cascade from 735,(8-) level. But M1 from α(K)exp=4.7 5 in 1986LhZX |
504.30 | 33.01 | M(γ): from α(K)exp=3.1 8 (2007Ri01) in 100Zr β- decay |
Mass measurement by Penning-trap method: Mass excess (g.s.)=-79802 20; mass excess (2.99S isomer)= -79488 10 (2007Ri01,2007Ha32,2006Jo14)
In (t,3He) (1979Aj03), many states are suggested by the observation of 23 groups, several of which are unresolved structures. Measured Q value=-6690 30 for the energy group labeled as ’0’, and assigned to the g.s. by 1979Aj03. Based on mass values in 2017Wa10, this Q value agrees better with the first level populated in (t,3He) identified with the 2.99S, (5+) isomer, whose energy is measured as 314 23 (2007Ri01,2007Ha32).
α 0.3-μs isomer is indicated by x(t) measurements (1970Gr38,1972ClZN) of fission fragments from 235U(n,F) (1970Gr38) and 252Cf(SF) (1972ClZN), but the mass assignment is not certain. 1970Gr38 assign this isomer to α=100, whereas 1972ClZN assign it to α=102
α 3-min activity reported by 1960Or02 and 1971Ca18 from 235U fission and by 1966Gu05 from 100Mo(n,p) reaction most likely corresponds to 99Nb β- decay (T1/2=2.6-min) and not to 100Nb. No such activity has been seen in any of the later studies on the decay of 100Nb
α 12-min activity assigned to 100Nb by 1961Ta08 from 100Mo(n,p) reaction has not been confirmed in any other 100Nb study. This activity probably corresponds to the decay of 101Mo (T1/2=14.6 min) formed by neutron capture in 100Mo
The following transitions were tentatively assigned to 100Nb from a study of prompt conversion electrons from 235U(n,F) by 1973Kh05: 84.0, 119.1, 126.4, 159.0, 172.0 and 212.0. None of these were assigned to levels in 100Nb
Theory references: consult the NSR database (www.nndc.bnl.gov/nsr/) for six primary references dealing with decay half-lives, β shape factors, and other beta-decay characteristics.
2000Lh01: theoretical calculation of level energies and spin-parities of 100Nb using the Interacting Boson-Fermion-Fermion model
Q-value: S(2n)=12415 9, S(2p)=22081 11 (2017Wa10)