ADOPTED LEVELS, GAMMAS for 199Tl
Author: Balraj Singh | Citation: Nucl. Data Sheets 108, 79 (2007) | Cutoff date: 15-Oct-2006
Full ENSDF file | Adopted Levels (PDF version)
| Q(β-)=-2.83×103 keV 3 | S(n)= 8.64×103 keV 9 | S(p)= 4.39×103 keV 3 | Q(α)= 2.09×103 keV 3 | ||
| Reference: 2012WA38 |
| References: | |||
| A | 199Tl IT decay (28.4 MS) | B | 199Pb ε decay (90 M) |
| C | 199Pb ε decay (12.2 M) | D | 197Au(α,2nγ) |
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 0.0 | ABCD | 1/2+ | 7.42 h 8 % ε = 100 | |||||
| 366.89 4 | ABCD | 3/2+ | < 1.5 ns | 366.90 6 | 100 | M1+E2 | 0.0 | 1/2+ |
| 720.35 4 | AB D | (5/2)+ | 353.39 6 720.24 6 | 100 5 69 3 | M1+E2 (Q) | 366.89 0.0 | 3/2+ 1/2+ | |
| 748.87 6 | A CD | 9/2- | 28.4 ms 2 % IT = 100 | 29 2 381.98 5 | 100 | [M2] E3 | 720.35 366.89 | (5/2)+ 3/2+ |
| 1118.29 17 | CD | 11/2- | 369.3 | 100 | (M1+E2) | 748.87 | 9/2- | |
| 1120.90 5 | B | 1/2,3/2,5/2(+) | 400.54 8 753.92 8 1121.00 7 | 81 7 100 5 94 5 | 720.35 366.89 0.0 | (5/2)+ 3/2+ 1/2+ | ||
| 1205.20 21 | B D | (7/2+) | 838.3 | 100 | Q | 366.89 | 3/2+ | |
| 1241.64 6 | B | 1/2,3/2,5/2 | 120.54 15 ? 521.28 7 874.77 9 | 3.4 10 26 5 100 5 | 1120.90 720.35 366.89 | 1/2,3/2,5/2(+) (5/2)+ 3/2+ | ||
| 1394.57 21 ? | CD | (11/2-) | 645.7 | 100 | E2+M1 | 748.87 | 9/2- | |
| 1450.46 17 | CD | 13/2- | 332.1 701.7 | 100 97 | M1+E2 E2 | 1118.29 748.87 | 11/2- 9/2- | |
| 1482.39 7 | B | 1/2,3/2,5/2 | 240.8 2 361.4 6 761.98 7 1115.1 4 1481.2 6 | 7.0 5 15 5 100 5 28 3 6.0 10 | 1241.64 1120.90 720.35 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2(+) (5/2)+ 3/2+ 1/2+ | ||
| 1502.01 5 | B | 1/2(+) TO 5/2(+) | 781.48 7 1135.04 8 1502.04 8 | 23.7 14 100 5 27.4 11 | (M1) | 720.35 366.89 0.0 | (5/2)+ 3/2+ 1/2+ | |
| 1528.24 9 | B | 1/2,3/2,5/2 | 1161.27 9 | 100 | 366.89 | 3/2+ | ||
| 1554.11 8 | B | 1/2,3/2,5/2 | 312.3 7 ? 433.2 3 833.83 10 1187.23 10 1553.3 3 | 6 2 36 10 40 6 100 10 18 4 | 1241.64 1120.90 720.35 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2(+) (5/2)+ 3/2+ 1/2+ | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 1632.11 12 | B | 1/2,3/2,5/2 | 390.3 4 510.90 10 ? 911.80 15 1265.4 3 1631.8 3 | 45 8 100 15 48 5 24 5 | 1241.64 1120.90 720.35 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2(+) (5/2)+ 3/2+ 1/2+ | ||
| 1658.35 6 | B | 1/2,3/2,5/2(+) | 937.89 8 1291.50 10 1658.43 9 | 37.7 20 5.5 5 100 | 720.35 366.89 0.0 | (5/2)+ 3/2+ 1/2+ | ||
| 1695.2 3 | B | 1/2,3/2,5/2(+) | 1328.3 3 1695.28 10 ? | 55 8 100 8 | 366.89 0.0 | 3/2+ 1/2+ | ||
| 1716.98 23 | CD | (13/2-) | 598.8 | 100 | M1+E2 | 1118.29 | 11/2- | |
| 1725.27 7 | B | 1/2,3/2,5/2 | 222.83 10 1005.13 8 1358.6 3 1725.3 5 | 5.0 21 100 5 26 3 5.0 17 | 1502.01 720.35 366.89 0.0 | 1/2(+) TO 5/2(+) (5/2)+ 3/2+ 1/2+ | ||
| 1749.65 6 | B | 1/2,3/2,5/2(+) | 267.6 2 1029.21 9 1382.71 9 1749.70 10 | 14 8 57 3 100 4 81 4 | 1482.39 720.35 366.89 0.0 | 1/2,3/2,5/2 (5/2)+ 3/2+ 1/2+ | ||
| 1768.60 7 | B | 1/2,3/2,5/2 | 1048.09 9 1401.94 10 1768.48 15 | 29 4 100 6 22 6 | 720.35 366.89 0.0 | (5/2)+ 3/2+ 1/2+ | ||
| 1866.94 20 | CD | (15/2-) | 416.6 748.5 | 100 100 | M1+E2 E2 | 1450.46 1118.29 | 13/2- 11/2- | |
| 1891.06 8 | B | 1/2,3/2,5/2(+) | 1170.70 9 1524.10 15 1891.3 3 | 76 7 40 10 100 7 | 720.35 366.89 0.0 | (5/2)+ 3/2+ 1/2+ | ||
| 1898.13 9 | B | 1/2,3/2,5/2 | 344.0 7 777.20 15 1531.23 10 1898.7 6 | 7 3 59 5 100 7 16 5 | 1554.11 1120.90 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2(+) 3/2+ 1/2+ | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 1930.11 10 | B | 1/2,3/2,5/2(+) | 1209.60 10 1930.69 20 | 100 7 43 11 | 720.35 0.0 | (5/2)+ 1/2+ | ||
| 1943.8 3 | D | (9/2-,11/2-,13/2-) | 825.5 | 100 | (M1+E2) | 1118.29 | 11/2- | |
| 1959.50 7 | B | 1/2,3/2,5/2 | 430.9 3 476.9 3 838.68 10 1239.12 10 1592.58 15 1959.50 20 | 9.3 21 8.5 21 42 8 100 4 12.4 13 3.2 5 | 1528.24 1482.39 1120.90 720.35 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2 1/2,3/2,5/2(+) (5/2)+ 3/2+ 1/2+ | ||
| 1977.48 8 | B | 1/2,3/2,5/2 | 319.2 4 494.89 10 1610.67 10 1978.5 3 | 16 5 65 10 100 7 12 2 | 1658.35 1482.39 366.89 0.0 | 1/2,3/2,5/2(+) 1/2,3/2,5/2 3/2+ 1/2+ | ||
| 1985.23 22 | D | (17/2-) | 118.2 534.8 | 23 100 | Q | 1866.94 1450.46 | (15/2-) 13/2- | |
| 2031.58 10 | B | 1/2,3/2,5/2(+) | 503.15 20 1311.28 10 2031.4 5 | 27 9 100 14 60 11 | 1528.24 720.35 0.0 | 1/2,3/2,5/2 (5/2)+ 1/2+ | ||
| 2080.07 23 | CD | (15/2+) | 363.2 629.5 | 25 100 | (E1) E1(+M2) | 1716.98 1450.46 | (13/2-) 13/2- | |
| 2159.57 17 | B | 1/2,3/2,5/2 | 605.8 6 ? 1793.10 20 2158.6 3 | <18 100 18 20 5 | 1554.11 366.89 0.0 | 1/2,3/2,5/2 3/2+ 1/2+ | ||
| 2206.5 3 | B | 1/2,3/2,5/2(+) | 574.98 15 ? 724.5 4 ? 1840.0 4 ? 2206.5 3 | 120 20 133 27 93 13 100 20 | 1632.11 1482.39 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2 3/2+ 1/2+ | ||
| 2226.48 19 | B | 1/2,3/2,5/2 | 1506.2 4 1859.3 3 2226.7 3 | 100 11 61 13 13 8 | 720.35 366.89 0.0 | (5/2)+ 3/2+ 1/2+ | ||
| E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
| 2237.39 7 | B | 1/2,3/2,5/2(+) | 605.8 6 ? 735.4 3 995.6 4 ? 1517.12 10 2237.29 10 | <6 <18 19 4 75 5 100 6 | 1632.11 1502.01 1241.64 720.35 0.0 | 1/2,3/2,5/2 1/2(+) TO 5/2(+) 1/2,3/2,5/2 (5/2)+ 1/2+ | ||
| 2367.38 14 | B | 1/2,3/2,5/2(+) | 641.3 4 735.4 3 ? 1647.2 6 2000.61 15 2367.0 5 | 33 6 <61 61 12 100 9 45 9 | 1725.27 1632.11 720.35 366.89 0.0 | 1/2,3/2,5/2 1/2,3/2,5/2 (5/2)+ 3/2+ 1/2+ | ||
| 2433.63 17 | B | 1/2,3/2,5/2(+) | 2066.95 20 2433.1 3 | 44 4 100 7 | 366.89 0.0 | 3/2+ 1/2+ | ||
| 2471.69 25 | D | (19/2-) | 486.4 604.8 | | D(+Q) | 1985.23 1866.94 | (17/2-) (15/2-) | |
| 2547.6 4 | B | 1/2,3/2,5/2(+) | 2180.2 4 ? 2547.6 4 | 154 40 100 40 | 366.89 0.0 | 3/2+ 1/2+ | ||
| 2643.2 4 | B | 1/2,3/2,5/2(+) | 984.4 5 ? 2643.2 4 | 167 67 100 33 | 1658.35 0.0 | 1/2,3/2,5/2(+) 1/2+ | ||
E(level): From least squares adjustment to adopted Eγ’s, assuming Δ(Eγ)=0.2 keV if not stated
Jπ(level): The assignments for the high spin levels are from (α,2nγ) reaction; based on γ(θ), α(K)exp, excitation function; see 1970Ne06 for detailed discussion.
E(γ): From 199Pb ε decay (90 min) and from (α,2nγ) for gammas from high spin levels above the 749.7-keV isomeric state.
I(γ): 199Pb ε (90 min) and (α,2nγ)
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
| Band 1 - 9/2[505] (oblate) band | |||||||
| 748.87 6 | 9/2- | 28.4 ms 2 % IT = 100 | |||||
| 1118.29 17 | 11/2- | 369.3 | 100 | (M1+E2) | 748.87 | 9/2- | |
| 1450.46 17 | 13/2- | 332.1 701.7 | 100 97 | M1+E2 E2 | 1118.29 748.87 | 11/2- 9/2- | |
| 1866.94 20 | (15/2-) | 416.6 748.5 | 100 100 | M1+E2 E2 | 1450.46 1118.29 | 13/2- 11/2- | |
| 1985.23 22 | (17/2-) | 118.2 534.8 | 23 100 | Q | 1866.94 1450.46 | (15/2-) 13/2- | |
| 2471.69 25 | (19/2-) | 486.4 604.8 | | D(+Q) | 1985.23 1866.94 | (17/2-) (15/2-) | |
| E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
| 366.89 | 3/2+ | < 1.5 ns | 366.90 6 | M1+E2 | +1.6 2 | 0.112 | B(E2)(W.u.)>0.49, B(M1)(W.u.)>6.1E-5, α=0.112 10, α(K)=0.083 9, α(L)=0.0214 9, α(M)=0.00522 19, α(N+)=0.00168 6 |
| 720.35 | (5/2)+ | 353.39 6 | M1+E2 | 0.6 2 | 0.211 | α=0.211 25, α(K)=0.169 22, α(L)=0.0318 22, α(M)=0.0075 5, α(N+)=0.00240 14 | |
| 748.87 | 9/2- | 28.4 ms 2 % IT = 100 | 29 2 | [M2] | 6.7×103 | B(M2)(W.u.)≈1.7×10-5, α=6.7×103 3, α(L)=4.94E+3 22, α(M)=1.35E+3 6 | |
| 9/2- | 28.4 ms 2 % IT = 100 | 381.98 5 | E3 | 0.229 | B(E3)(W.u.)≈0.0114, α=0.229, α(K)=0.0966, α(L)=0.101, α(M)=0.0266, α(N+)=0.00872 | ||
| 1118.29 | 11/2- | 369.3 | (M1+E2) | -0.25 +10-30 | 0.22 | α=0.22 3, α(K)=0.18 3, α(L)=0.031 3, α(M)=0.0073 6, α(N+)=0.0023 2 | |
| 1394.57 | (11/2-) | 645.7 | E2+M1 | -0.9 +5-8 | 0.036 | α=0.036 12 | |
| 1450.46 | 13/2- | 332.1 | M1+E2 | -0.34 9 | 0.286 | α=0.286 12, α(K)=0.232 11, α(L)=0.0409 10, α(M)=0.00957 20, α(N+)=0.00306 7 | |
| 13/2- | 701.7 | E2 | 0.0132 | α=0.0132, α(K)=0.0101, α(L)=0.00233 | |||
| 1502.01 | 1/2(+) TO 5/2(+) | 1135.04 8 | (M1) | 0.0126 | α=0.0126, α(K)=0.0103, α(L)=0.00168 | ||
| 1716.98 | (13/2-) | 598.8 | M1+E2 | -2.4 +6-7 | 0.025 | α=0.025 4, α(K)=0.020 4, α(L)=0.0044 5 | |
| 1866.94 | (15/2-) | 416.6 | M1+E2 | -0.40 +12-18 | 0.151 | α=0.151 14, α(K)=0.123 13, α(L)=0.0215 14, α(M)=0.0050 3, α(N+)=0.00161 10 | |
| (15/2-) | 748.5 | E2 | 0.0115 | α=0.0115, α(K)=0.00888, α(L)=0.00197 | |||
| 1943.8 | (9/2-,11/2-,13/2-) | 825.5 | (M1+E2) | -1.9 3 | 0.0135 | α=0.0135 12, α(K)=0.0108 11, α(L)=0.00203 15 | |
| 2080.07 | (15/2+) | 363.2 | (E1) | 0.0185 | α=0.0185, α(K)=0.0153, α(L)=0.00251, α(M)=0.000581, α(N+)=0.000185 | ||
| (15/2+) | 629.5 | E1(+M2) | -0.07 +7-5 | 0.00580 | α=0.00580, α(K)=0.00480, α(L)=0.00075 | ||
| 2471.69 | (19/2-) | 486.4 | D(+Q) | +0.1 3 |
Additional Level Data and Comments:
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 0.0 | 1/2+ | 7.42 h 8 % ε = 100 | μ=+1.60 2 (1989Ra17,1961Hu04) <r2>1/2=5.447 fm 4 (2004An14, evaluation). |
| 748.87 | 9/2- | 28.4 ms 2 % IT = 100 | E(level): 9/2[505] (oblate) band. |
| 1118.29 | 11/2- | XREF: C(?). E(level): 9/2[505] (oblate) band. | |
| 1120.90 | 1/2,3/2,5/2(+) | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1205.20 | (7/2+) | XREF: B(?). | |
| 1241.64 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1450.46 | 13/2- | XREF: C(?). E(level): 9/2[505] (oblate) band. | |
| 1482.39 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1502.01 | 1/2(+) TO 5/2(+) | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1528.24 | 1/2,3/2,5/2 | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1554.11 | 1/2,3/2,5/2 | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1632.11 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1658.35 | 1/2,3/2,5/2(+) | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1695.2 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. | |
| 1716.98 | (13/2-) | XREF: C(?). | |
| 1725.27 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1749.65 | 1/2,3/2,5/2(+) | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1768.60 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1866.94 | (15/2-) | XREF: C(?). E(level): 9/2[505] (oblate) band. | |
| 1891.06 | 1/2,3/2,5/2(+) | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1898.13 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1930.11 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1959.50 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1977.48 | 1/2,3/2,5/2 | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 1985.23 | (17/2-) | E(level): 9/2[505] (oblate) band. | |
| E(level) | Jπ(level) | T1/2(level) | Comments |
| 2031.58 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 2080.07 | (15/2+) | XREF: C(?). | |
| 2159.57 | 1/2,3/2,5/2 | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 2206.5 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. | |
| 2237.39 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 2367.38 | 1/2,3/2,5/2(+) | Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 2433.63 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. Jπ(level): log ft from 3/2- (in 199Pb ε decay (90 min)) is allowed or first-forbidden. If transition to 1/2+ g.s. is prominent, then parity for 5/2 choice is likely to Be positive. | |
| 2471.69 | (19/2-) | E(level): 9/2[505] (oblate) band. | |
| 2547.6 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. | |
| 2643.2 | 1/2,3/2,5/2(+) | E(level): Population of this level in 199Pb ε decay (90 min) is less certain than others in that decay. |
| E(level) | E(gamma) | Comments |
| 366.89 | 366.90 | M(γ): From 199Pb ε decay (90 min) |
| 720.35 | 353.39 | M(γ): From 199Pb ε decay (90 min) |
| 748.87 | 29 | E(γ): from 199Tl IT decay | 381.98 | E(γ): from 199Tl ε decay (12.2 min) |
| 1502.01 | 1135.04 | M(γ): From 199Pb ε decay (90 min) |
| 1977.48 | 1978.5 | E(γ): level-energy difference=1977.5 |
| 2159.57 | 605.8 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 2158.6 | E(γ): level-energy difference=2159.6 |
| 2237.39 | 605.8 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 735.4 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
| 2367.38 | 735.4 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
Nuclear structure calculations (levels, band structures): 1989Be34, 1980Kr20, 1977Go09, 1977Ta01, 1976De50, 1976Di14, 1975Me11, 1974Ne16, 1971Na04, 1967Co06
Levels: Except for the lowest levels, the shell model is inadequate to describe observed levels. The core-coupling model extends the description. α rotational band based upon the 9/2[505] state has been observed
Q-value: Note: Current evaluation has used the following Q record -2830 40 8640 80 4394 28 2086 28 2003Au03