ADOPTED LEVELS, GAMMAS for 140Ce
Author: N. Nica | Citation: Nucl. Data Sheets 154, 1 (2018) | Cutoff date: 20-Nov-2018
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-3388 keV 6 | S(n)= 9200 keV 7 | S(p)= 8138.8 keV 17 | Q(α)= -1614.1 keV 16 | ||
Reference: 2017WA10 |
References: | |||
A | 140La β- decay | B | 140Pr ε decay |
C | 144Nd α decay | D | 138Ba(3He,n) |
E | 138Ba(α,2nγ) | F | 138Ce(t,p) |
G | 139La(3He,d) | H | 140Ce(γ,γ’) |
I | 140Ce(E,E’) | J | 140Ce(n,n’γ) |
K | 140Ce(p,p’) | L | 140Ce(α,α’) |
M | 140Ce(α,α’γ) | N | 140Ce(17O,17O’γ) |
O | 141Pr(d,3He) | P | 142Ce(p,t) |
Q | 142Nd(14C,16O) | R | 143Nd(n,α),(n,αγ) |
S | 144Nd(d,6Li) | T | 238U(12C,Fγ) |
U | Coulomb Excitation |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDEFGHIJKLMNOPQRSTU | 0+ | STABLE | |||||
1596.233 23 | AB DEFGHIJKL NOPQRSTU | 2+ | 0.0910 ps +48-44 | 1596.210 35 | 100 | E2 | 0.0 | 0+ |
1903.31 6 | AB EF JK NOP R | 0+ | 0.40 ns 3 | 306.9 2 1903.5 | 100 | E2 E0 | 1596.233 0.0 | 2+ 0+ |
2083.259 24 | A E G IJKL OPQR T | 4+ | 3.45 ns 3 | 487.021 12 2083.2 5 | 100.0 13 0.03 2 | E2 E4 | 1596.233 0.0 | 2+ 0+ |
2107.854 24 | A E IJ OP T | 6+ | 7.3 µs 15 | 24.595 4 | 100 | E2 | 2083.259 | 4+ |
2347.881 24 | AB E IJ L O R | 2+ | ≤ 0.2 ns | 445.5 5 751.637 18 2347.88 5 | 0.07 2 100 1 19.6 7 | [E2] M1+E2 E2 | 1903.31 1596.233 0.0 | 0+ 2+ 0+ |
2349.805 25 | A E IJ L O R | 5+ | ≤ 12 ps | 241.933 30 266.543 12 | 88.9 17 100.0 16 | M1+E2 M1+E2 | 2107.854 2083.259 | 6+ 4+ |
2412.013 24 | A E G J O R | 3+ | 1.3 ps 4 | 64.135 10 328.762 8 815.772 19 | 0.06 1 87.3 17 100.0 9 | M1 M1+E2 M1(+E2) | 2347.881 2083.259 1596.233 | 2+ 4+ 2+ |
2464.08 3 | A EFG IJKL N PQR U | 3- | 0.15 ps 3 | 867.846 20 2464.1 5 | 100 1 0.21 3 | E1 [E3] | 1596.233 0.0 | 2+ 0+ |
2480.925 24 | A E J | 4+ | 22 ps 7 | 68.916 6 131.117 8 397.52 5 | 16.1 5 100 2 15.7 10 | M1 M1+E2 (E2) | 2412.013 2349.805 2083.259 | 3+ 5+ 4+ |
2515.76 3 | A E G J OP R | 4+ | ≤ 2.5 ps | 432.493 12 919.550 23 | 100 1 92 1 | M1+E2 E2 | 2083.259 1596.233 | 4+ 2+ |
2521.428 24 | AB DE G J OP | 2+ | ≤ 2.4 ps | 109.422 11 173.543 9 438.5 5 618.12 5 925.189 21 2521.40 5 | 3.18 6 1.84 6 0.57 14 0.54 6 100 1 50.2 6 | M1+E2 M1 E2+M1 E2 | 2412.013 2347.881 2083.259 1903.31 1596.233 0.0 | 3+ 2+ 4+ 0+ 2+ 0+ |
2547.23 4 | AB J R | 1+ | 0.19 ps +11-5 | 950.987 26 2547.34 11 | 100 1 19.5 6 | M1(+E2) M1 | 1596.233 0.0 | 2+ 0+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
2628.81 4 | E G J | 6+ | 278.84 13 520.964 25 | 12.7 16 100 5 | M1,E2 E2+M1 | 2349.805 2107.854 | 5+ 6+ | |
2658.3 10 ? | E J | 575? | 100 | 2083.259 | 4+ | |||
2899.59 4 | AB GHIJKL OP | 2+ | 49 fs 9 | 996.2 3 1303.38 5 2899.55 4 | 3.2 8 53 3 100 5 | M1+E2 E2 | 1903.31 1596.233 0.0 | 0+ 2+ 0+ |
3001.12 14 | A J O | 2+ | 0.16 ps +10-5 | 1097.20 23 1405.20 17 | 39 8 100 12 | (M1+E2) | 1903.31 1596.233 | 0+ 2+ |
3016.9 5 | B F J P | 0+ | ≥ 0.14 ps | 1420.7 5 3016.3 12 | 100 15 | E2 E0 | 1596.233 0.0 | 2+ 0+ |
3039.0 4 | J L | 3- | ||||||
3118.55 16 | AB FGHIJKL NOP | 2+ | 27.5 fs 85 | 3118.51 16 | 100 | (E2) | 0.0 | 0+ |
3120.34 20 ? | J | 2+ | 3120.3 2 ? | 100 | E2 | 0.0 | 0+ | |
3122.11 5 | J | 4+ | 657.5 4 772.50 13 1525.85 4 | 2.9 10 23 2 100 5 | E2 | 2464.08 2349.805 1596.233 | 3- 5+ 2+ | |
3168.3 10 ? | E | 1085? | 100 | 2083.259 | 4+ | |||
3219.95 11 | J | (0+) | 1623.71 10 | 100 | 1596.233 | 2+ | ||
3226 2 | F P | 0+ | ||||||
3255.70 5 | E G JKL | 5- | 739.94 4 774.8 3 | 100 6 22 4 | (E1) | 2515.76 2480.925 | 4+ 4+ | |
3319.65 6 | AB HIJ | 2+ | 58 fs +19-12 | 772.50 13 ? 1235.8 6 ? 1724.7? 3319.61 6 | 39 3 11 4 52 3 100 6 | E2 | 2547.23 2083.259 1596.233 0.0 | 1+ 4+ 2+ 0+ |
3335.47 11 | FG J L P | 4+ | 855.1 4 985.63 22 1227.71 16 ? 1252.12 13 1739.4 3 | 18 4 9 3 43 5 100 8 23 4 | 2480.925 2349.805 2107.854 2083.259 1596.233 | 4+ 5+ 6+ 4+ 2+ | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3360.24 18 | J | 1010.45 19 1276.9 4 | 100 10 27 8 | 2349.805 2083.259 | 5+ 4+ | |||
3391.09 8 | E J | 1307.73 10 1794.93 10 | 100 8 79 5 | 2083.259 1596.233 | 4+ 2+ | |||
3394.92 7 | A G JK | (4-) | 0.042 ps +49-21 | 982.89? 1045.11 7 1287.03 19 1311.56 19 ? | 100 6 74 5 22 3 22 3 | 2412.013 2349.805 2107.854 2083.259 | 3+ 5+ 6+ 4+ | |
3395.1 10 ? | E | (4+) | 983.1? | 100 | M1,E2 | 2412.013 | 3+ | |
3408.02 15 | J | (2+) | ≥ 0.062 ps | 886.42 22 944.0 3 996.2 3 1811.0 3 ? 3408.1 4 | 100 11 41 7 27 7 49 7 57 7 | 2521.428 2464.08 2412.013 1596.233 0.0 | 2+ 3- 3+ 2+ 0+ | |
3424.6 3 | E G IJ P T | 7- | 1316.8 3 | 100 | E1 | 2107.854 | 6+ | |
3432.8 10 | E | 7+ | 1083.0 | 100 | E2 | 2349.805 | 5+ | |
3436.54 7 | J | (2+,1) | 1088.65 6 1533.2 4 ? 3436.8 8 | 100 5 6.2 11 5.4 12 | 2347.881 1903.31 0.0 | 2+ 0+ 0+ | ||
3471.21 11 | J | (2+) | 0.097 ps +76-35 | 1568.1 5 3471.15 11 | 16 4 100 6 | (E2) | 1903.31 0.0 | 0+ 0+ |
3473.75 4 | A G JK | 3- | 0.066 ps +21-13 | 992.9 5 1125.64 22 1877.51 3 | 33 12 22 3 100 10 | 2480.925 2347.881 1596.233 | 4+ 2+ 2+ | |
3476.3 3 | E T | 8- | 51.7 1 848.2 | 100 | 3424.6 2628.81 | 7- 6+ | ||
3484.2 10 | E | 6+ | 1134.4 | 100 | E2 | 2349.805 | 5+ | |
3491.2 3 ? | J | 944.0 3 3491.2 7 | 100 18 79 18 | 2547.23 0.0 | 1+ 0+ | |||
3492.23 25 | E T | 9- | 1.7 ns 2 | 15.7 69.5 1384.2 3 | | 3476.3 3424.6 2107.854 | 8- 7- 6+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3512.3 3 | E T | 8+ | 1404.4 3 | 100 | E2 | 2107.854 | 6+ | |
3520.87 14 | A | (4+) | 1924.62 13 | 100 | 1596.233 | 2+ | ||
3522.2 10 | E G | (5) | 1041.3 | | 2480.925 | 4+ | ||
3534.6 10 | E L | (3,4) | 1184.8 | 100 | 2349.805 | 5+ | ||
3539.1 3 | J | 2+ | ≥ 0.21 ps | 3539.1 3 | 100 | E2 | 0.0 | 0+ |
3551 3 | F K P | 2+,3- | ||||||
3567.5 3 | J | (2+) | 1484.3 3 3567.0 10 | 100 13 55 16 | 2083.259 0.0 | 4+ 0+ | ||
3602 | I | |||||||
3620.7 6 | E | 8+ | 992.2 1512.9 | | 2628.81 2107.854 | 6+ 6+ | ||
3642.8 3 | H J MN | 1- | 1.45 fs 19 | 1739.4 3 ? 3642.7 3 | 22 4 100 7 | E1 | 1903.31 0.0 | 0+ 0+ |
3646.7 6 | J | (1,2+) | ≥ 0.062 ps | 1743.31 22 ? 3646.6 6 | 75 11 100 18 | 1903.31 0.0 | 0+ 0+ | |
3648.23 14 | J | (2+,3,4+) | 1564.92 16 2052.07 22 | 100 8 69 7 | 2083.259 1596.233 | 4+ 2+ | ||
3653 3 | F K P | 2+,3- | ||||||
3657.64 18 ? | J | (4+,5,6+) | 1307.73 10 ? 1549.76 19 1574.5 5 | 100 3 45 5 12 4 | 2349.805 2107.854 2083.259 | 5+ 6+ 4+ | ||
3661.5 10 | E | (7,8) | 1032.7 | | 2628.81 | 6+ | ||
3684.2 6 | J | (1-,2+) | 1220.5 3 ? 3684.1 6 | 100 14 76 12 | 2464.08 0.0 | 3- 0+ | ||
3708.60 13 | J | (2+) | 1227.71 16 2112.30 19 3708.1 11 | 81 10 100 8 33 8 | 2480.925 1596.233 0.0 | 4+ 2+ 0+ | ||
3710 4 | FG K P | 5- | ||||||
3714.3 3 | E T | 10+ | 23.1 ns 4 | 202.0 3 222.0 3 | 54 12 100 15 | E2 E1 | 3512.3 3492.23 | 8+ 9- |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3723.54 17 | J | (2+) | ≥ 0.097 ps | 1311.56 19 3723.4 3 | 45 7 100 7 | (E2) | 2412.013 0.0 | 3+ 0+ |
3729 2 | F P | 2+ | ||||||
3735.3 4 | J | (1,2+) | 3735.2 4 | 100 | 0.0 | 0+ | ||
3746 2 | F P | |||||||
3767.97 10 | J | (2+,3+,4+) | 1220.5 3 1252.12 13 ? 1287.03 19 1684.4 3 2171.82 13 | 34 5 98 8 36 5 23 3 100 6 | 2547.23 2515.76 2480.925 2083.259 1596.233 | 1+ 4+ 4+ 4+ 2+ | ||
3780 | FG | (3+,4+) | ||||||
3792.72 15 | JK P | 3- | 893.7 3 1276.9 4 1311.56 19 2196.6 6 | 100 13 48 14 94 14 93 10 | 2899.59 2515.76 2480.925 1596.233 | 2+ 4+ 4+ 2+ | ||
3836.1 5 ? | J | (2+,3,4+) | 1753.1 4 ? 2239.8 5 | 32 10 100 17 | 2083.259 1596.233 | 4+ 2+ | ||
3847.10 14 | J | (4+,5,6+) | 808.1 3 1497.31 22 1739.4 3 1763.6 3 | 49 7 100 10 38 6 47 6 | 3039.0 2349.805 2107.854 2083.259 | 3- 5+ 6+ 4+ | ||
3853.2 5 | J | (1,2+) | 2256.8 7 3853.3 6 | 30 8 100 11 | 1596.233 0.0 | 2+ 0+ | ||
3879.3 8 | J | (1,2+) | 3879.2 8 | 100 | 0.0 | 0+ | ||
3894.5 6 | E | 9+ | 180.0 274.2 382.3 | | 3714.3 3620.7 3512.3 | 10+ 8+ 8+ | ||
3910.93 23 | J | 2314.68 22 | 100 | 1596.233 | 2+ | |||
3911 10 | FG P | 5- | ||||||
3912 4 | K | 2- | ||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3956 4 | K | |||||||
3957.93 18 | J | 1493.6 3 2361.80 22 | 69 9 100 9 | 2464.08 1596.233 | 3- 2+ | |||
3970.8 10 ? | E | 1621.0? | | 2349.805 | 5+ | |||
3980 | L P | 3- | ||||||
3984.20 16 | J | (2+,3,4+) | 1901.4 5 2387.90 16 | 87 19 100 15 | 2083.259 1596.233 | 4+ 2+ | ||
4000 4 | K | 4- | ||||||
4017 10 | G P | |||||||
4053 | H | (1) | 4053 | 100 | (D) | 0.0 | 0+ | |
4061 | I | |||||||
4125 10 | D FG P | 2+ | ||||||
4158 4 | D K | 2- | ||||||
4164.0 3 | J | (1,2+) | 2567.8 3 4163.5 9 | 100 16 53 18 | 1596.233 0.0 | 2+ 0+ | ||
4171.1 7 | FG J | (2+,1) | 2576.1 6 ? 4171.0 7 | 31 10 100 14 | 1596.233 0.0 | 2+ 0+ | ||
4173.6 8 | H MN | 1(-) | 3.6 fs 7 | 4173.5 8 | 100 | [E1] | 0.0 | 0+ |
4182 4 | K | 1- | ||||||
4183 10 | P | 2+,(3-,4+) | ||||||
4208 6 | K | |||||||
4242 10 | FG P | 2+ | ||||||
4262.5 7 | E | 10+ | 368.1 548.3 | | 3894.5 3714.3 | 9+ 10+ | ||
4279.9 4 | J | (2+,3,4+) | 2196.6 4 2683.6 7 | 74 8 100 12 | 2083.259 1596.233 | 4+ 2+ | ||
4296 6 | I K P | 3-,4+ | ||||||
4331 | H | (1) | 4331 | 100 | (D) | 0.0 | 0+ | |
4340 10 | K P | (1-) | ||||||
4354.9 7 | H N | 1 | 3.7 fs 8 | 4354.8 7 | 100 | D | 0.0 | 0+ |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4360 10 | G P | + | ||||||
4364 4 | K | 1- | ||||||
4371 | H | (1) | 4371 | 100 | (D) | 0.0 | 0+ | |
4388 | H | (1) | 4388 | 100 | (D) | 0.0 | 0+ | |
4424 4 | K P | 2+,3- | ||||||
4437 | H | (1) | 4437 | 100 | (D) | 0.0 | 0+ | |
4448.5 11 | E | (9,11) | 734.2 | 100 | 3714.3 | 10+ | ||
4450 10 | K | |||||||
4485 10 | K | |||||||
4514.9 9 | H MN | 1(-) | 2.7 fs 5 | 4514.8 9 | 100 | [E1] | 0.0 | 0+ |
4538 4 | K P | 3- | ||||||
4571.3 13 ? | E | (8+,10+) | 1058.4? | | 3512.3 | 8+ | ||
4580 4 | K | 2- | ||||||
4640 10 | K | |||||||
4655 | H | (1) | 4655 | 100 | (D) | 0.0 | 0+ | |
4660 15 | K | |||||||
4700 10 | I K | |||||||
4720 15 | K | |||||||
4748 4 | K P | 2- | ||||||
4760 15 | K | |||||||
4770 10 | K | 1- | ||||||
4787.8 9 | H MN | 1(-) | 2.3 fs 4 | 4787.7 9 | 100 | [E1] | 0.0 | 0+ |
4790 15 | K | |||||||
4827 10 | P | 2+,3- | ||||||
4851.1 4 | E T | 12+ | 588.8 1136.8 3 | 100 | E2 | 4262.5 3714.3 | 10+ 10+ | |
4860 10 | K | |||||||
4875 | H | (1) | 4875 | 100 | (D) | 0.0 | 0+ | |
4880 15 | K | |||||||
4883 | H | (1) | 4883 | 100 | (D) | 0.0 | 0+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4904.6 5 | E T | 11- | 1190.3 4 | 100 | E1 | 3714.3 | 10+ | |
4910 15 | K | |||||||
4951 | H | (1) | 4951 | 100 | (D) | 0.0 | 0+ | |
4958.0 8 | E | (11+) | 1465.9 | 100 | 3492.23 | 9- | ||
4979 10 | N P | 2+,3- | ||||||
5000 15 | K | |||||||
5026 6 | I K | 2-,3- | ||||||
5050 15 | K | |||||||
5069.5 11 | E | (9,11) | 1355.2 | 100 | D | 3714.3 | 10+ | |
5093.4 7 | E T | (12-) | 135.3 188.9 5 | 100 | 4958.0 4904.6 | (11+) 11- | ||
5101 10 | K P | GE 5 | ||||||
5102.1 5 | E T | 13- | 250.9 3 | 100 | E1 | 4851.1 | 12+ | |
5140 15 | K | |||||||
5157.3 12 | H M P | 1(-) | 2.6 fs 5 | 5157.2 12 | 100 | [E1] | 0.0 | 0+ |
5160 15 | K N P | |||||||
5190.2 10 | H MN | 1(-) | 2.1 fs 4 | 5190.1 10 | 100 | [E1] | 0.0 | 0+ |
5196 6 | K | 2-,3- | ||||||
5211.6 14 | H MN | 1(-) | 3.6 fs 9 | 5211.5 14 | 100 | [E1] | 0.0 | 0+ |
5230 15 | K P | |||||||
5245 | H | (1) | 5245 | 100 | (D) | 0.0 | 0+ | |
5295 10 | P | 5-,6+ | ||||||
5330 | H | (1) | 5330 | 100 | (D) | 0.0 | 0+ | |
5335.0 9 | E | (12-) | 232.6 377.4 | | 5102.1 4958.0 | 13- (11+) | ||
5337.3 9 | H MN | 1(-) | 1.8 fs 4 | 5337.2 9 | 100 | [E1] | 0.0 | 0+ |
5377 10 | I P | 4+,5- | ||||||
5419.0 4 | T | (14-) | 318.0 4 | 100 | 5101 | GE 5 | ||
5424 6 | K | 2-,3- | ||||||
5449 10 | P | |||||||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5466 6 | K | 2-,3- | ||||||
5470 | H | (1) | 5470 | 100 | (D) | 0.0 | 0+ | |
5494 | H | (1) | 5494 | 100 | (D) | 0.0 | 0+ | |
5548.4 7 | H MN | 1(-) | 0.97 fs 17 | 5548.3 7 | 100 | [E1] | 0.0 | 0+ |
5573.8 14 | H MN | 1(-) | 1.7 fs 4 | 5573.7 14 | 100 | [E1] | 0.0 | 0+ |
5574 15 | P | (0+) | ||||||
5624 | H | (1) | 5624 | | (D) | 0.0 | 0+ | |
5650 15 | P | 2+,3- | ||||||
5659.9 6 | H MN | 1- | 0.0121 eV 29 | 5659.8 6 | 100 | E1 | 0.0 | 0+ |
5693.3 5 | T | 592.3 5 | 100 | 5101 | GE 5 | |||
5703 15 | P | 1-,2+ | ||||||
5721 | H | (1) | 5721 | 100 | (D) | 0.0 | 0+ | |
5759 | H | (1) | 5759 | 100 | (D) | 0.0 | 0+ | |
5789 15 | P | |||||||
5809 | H | (1) | 5809 | 100 | (D) | 0.0 | 0+ | |
5823 | H | (1) | 5823 | 100 | (D) | 0.0 | 0+ | |
5896 15 | P | 1-,2+ | ||||||
5928.6 10 | H M | 1(-) | 1.16 fs 24 | 5928.5 10 | 100 | [E1] | 0.0 | 0+ |
5940 | H | (1) | 5940 | 100 | (D) | 0.0 | 0+ | |
5989 15 | P | (3-,4+) | ||||||
6029 | H | (1) | 6029 | 100 | (D) | 0.0 | 0+ | |
6078 15 | P | 2+,3- | ||||||
6119.1 15 | H | 1- | 0.69 fs 12 | 6119.0 15 | 100 | E1 | 0.0 | 0+ |
6130.6 12 | H | 1 | 1.5 fs 3 | 6130.5 12 | 100 | D | 0.0 | 0+ |
6161.7 14 | H MN | 1(-) | 1.08 fs 20 | 6161.6 14 | 100 | [E1] | 0.0 | 0+ |
6187 15 | P | 2+,3- | ||||||
6226 | H | (1) | 6226 | 100 | (D) | 0.0 | 0+ | |
6233 | I | |||||||
6245 | H | (1) | 6245 | 100 | (D) | 0.0 | 0+ | |
6255 | H | (1) | 6255 | 100 | (D) | 0.0 | 0+ | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6268 15 | P | |||||||
6273.6 10 | H | 1 | 1.05 fs 20 | 6273.4 10 | 100 | D | 0.0 | 0+ |
6295.3 8 | H | 1- | 0.46 fs 8 | 6295.1 8 | 100 | E1 | 0.0 | 0+ |
6303.6 3 | T | (15-) | 1202.6 3 | 100 | 5101 | GE 5 | ||
6327.8 12 | H | 1 | 1.3 fs 5 | 6327.6 12 | 100 | D | 0.0 | 0+ |
6343.3 11 | H | 1 | 0.78 fs 15 | 6343.1 11 | 100 | D | 0.0 | 0+ |
6352.7 10 | H | 1 | 0.69 fs 13 | 6352.5 10 | 100 | D | 0.0 | 0+ |
6364 15 | P | 3-,4+ | ||||||
6397.2 8 | H | 1- | 0.28 fs 5 | 6397.0 8 | 100 | E1 | 0.0 | 0+ |
6439.9 14 | H | 1(-) | 0.53 fs 9 | 6439.7 14 | 100 | (E1) | 0.0 | 0+ |
6449.9 15 | H | 1(-) | 0.90 fs 18 | 6449.7 15 | 100 | (E1) | 0.0 | 0+ |
6458.5 15 | H | 1(-) | 1.00 fs 20 | 6458.3 15 | 100 | (E1) | 0.0 | 0+ |
6484.8 10 | H | 1 | 1.00 fs 20 | 6484.6 10 | 100 | D | 0.0 | 0+ |
6497.0 7 | H | 1- | 0.33 fs 6 | 6496.8 7 | 100 | E1 | 0.0 | 0+ |
6535.8 6 | H | 1- | 0.22 fs 3 | 6535.6 6 | 100 | E1 | 0.0 | 0+ |
6549.1 11 | H | 1 | 1.3 fs 3 | 6548.9 11 | 100 | D | 0.0 | 0+ |
6574.9 15 | H | 1 | 1.16 fs 23 | 6574.7 15 | 100 | D | 0.0 | 0+ |
6605.5 10 | H | 1(-) | 0.69 fs 12 | 6605.3 10 | 100 | (E1) | 0.0 | 0+ |
6616.2 10 | H | 1(-) | 0.74 fs 13 | 6616.0 10 | 100 | (E1) | 0.0 | 0+ |
6678 | I | |||||||
6771.7 14 | H | (2+) | 6771.5 14 | 100 | (E2) | 0.0 | 0+ | |
6781.9 15 | H | 1 | 0.85 fs 19 | 6781.7 15 | 100 | D | 0.0 | 0+ |
6796.6 5 | T | (16-) | 493.0 4 | 100 | 6303.6 | (15-) | ||
6841.8 12 | H | 1 | 0.79 fs 22 | 6841.6 12 | 100 | D | 0.0 | 0+ |
6862.4 7 | H | 1- | 0.24 fs 4 | 6862.2 7 | 100 | E1 | 0.0 | 0+ |
6889.2 8 | T | (15,16) | 1470.2 7 | 100 | 5419.0 | (14-) | ||
6905.9 15 | H | 1 | 0.45 fs 10 | 6905.7 15 | 100 | D | 0.0 | 0+ |
6932.6 14 | H | 1 | 0.52 fs 11 | 6932.4 14 | 100 | D | 0.0 | 0+ |
6960.4 12 | H | 1 | 0.47 fs 10 | 6960.2 12 | 100 | D | 0.0 | 0+ |
7038.2 6 | T | (17-) | 734.6 5 | 100 | 6303.6 | (15-) | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
7050 | I | |||||||
7206.0 14 | H | 1 | 0.31 fs 5 | 7205.8 14 | 100 | D | 0.0 | 0+ |
7214.8 15 | H | 1 | 0.34 fs 6 | 7214.6 15 | 100 | D | 0.0 | 0+ |
7341.5 14 | H | 1 | 0.9 fs 2 | 7341.3 14 | 100 | D | 0.0 | 0+ |
7370 | D | 0+ | ||||||
7673.4 12 | H | 1 | 0.76 fs 18 | 7673.2 12 | 100 | D | 0.0 | 0+ |
E(level): From least-squares fit to γ energies
M(γ): From α(K)exp, γ(θ), γγ(θ), linear pol in β- and ε decay and in different nuclear reactions
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - γ.S. band | |||||||
0.0 | 0+ | STABLE | |||||
1596.233 23 | 2+ | 0.0910 ps +48-44 | 1596.210 35 | 100 | E2 | 0.0 | 0+ |
2083.259 24 | 4+ | 3.45 ns 3 | 487.021 12 2083.2 5 | 100.0 13 0.03 2 | E2 E4 | 1596.233 0.0 | 2+ 0+ |
2107.854 24 | 6+ | 7.3 µs 15 | 24.595 4 | 100 | E2 | 2083.259 | 4+ |
3512.3 3 | 8+ | 1404.4 3 | 100 | E2 | 2107.854 | 6+ | |
3714.3 3 | 10+ | 23.1 ns 4 | 202.0 3 222.0 3 | 54 12 100 15 | E2 E1 | 3512.3 3492.23 | 8+ 9- |
4851.1 4 | 12+ | 588.8 1136.8 3 | 100 | E2 | 4262.5 3714.3 | 10+ 10+ |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
1596.233 | 2+ | 0.0910 ps +48-44 | 1596.210 35 | E2 | 8.98×10-4 | B(E2)(W.u.)=13.9 7, α=8.98E-4, α(K)=0.000676 10, α(L)=8.63E-5 12, α(M)=1.79E-5 3, α(N)=3.97E-6 6, α(O)=6.45E-7 9, α(P)=4.92E-8 7 | |
1903.31 | 0+ | 0.40 ns 3 | 306.9 2 | E2 | 0.0454 | B(E2)(W.u.)=7.4 10, α=0.0454, α(K)=0.0365 6, α(L)=0.00697 10, α(M)=0.001498 22, α(N)=0.000327 5, α(O)=4.98E-5 7, α(P)=2.42E-6 4 | |
2083.259 | 4+ | 3.45 ns 3 | 487.021 12 | E2 | 0.01159 | B(E2)(W.u.)=0.1370 12, α=0.01159, α(K)=0.00966 14, α(L)=0.001527 22, α(M)=0.000324 5, α(N)=7.11E-5 10, α(O)=1.113E-5 16, α(P)=6.77E-7 10 | |
4+ | 3.45 ns 3 | 2083.2 5 | E4 | 1.36×10-3 | B(E4)(W.u.)=14 10, α=1.36E-3, α(K)=0.001162 17, α(L)=0.0001598 23, α(M)=3.35E-5 5, α(N)=7.43E-6 11, α(O)=1.198E-6 17, α(P)=8.83E-8 13 | ||
2107.854 | 6+ | 7.3 µs 15 | 24.595 4 | E2 | 697 | B(E2)(W.u.)=0.29 +8-5, α=697, α(L)=545 8, α(M)=122.0 18, α(N)=25.9 4, α(O)=3.52 5, α(P)=0.000945 14 | |
2347.881 | 2+ | ≤ 0.2 ns | 445.5 5 | [E2] | 0.01486 | α=0.01486, α(K)=0.01232 18, α(L)=0.00201 3, α(M)=0.000427 7, α(N)=9.36×10-5 14, α(O)=1.458E-5 21, α(P)=8.56E-7 13 | |
2+ | ≤ 0.2 ns | 751.637 18 | M1+E2 | +0.38 4 | 0.00548 | α=0.00548 9, α(K)=0.00471 8, α(L)=0.000613 10, α(M)=0.0001277 20, α(N)=2.83×10-5 5, α(O)=4.60E-6 8, α(P)=3.54E-7 6 | |
2+ | ≤ 0.2 ns | 2347.88 5 | E2 | 8.45×10-4 | α=8.45×10-4, α(K)=0.000333 5, α(L)=4.15E-5 6, α(M)=8.60E-6 12, α(N)=1.91E-6 3, α(O)=3.11E-7 5, α(P)=2.42E-8 4 | ||
2349.805 | 5+ | ≤ 12 ps | 241.933 30 | M1+E2 | -0.04 +3-6 | 0.1020 | α=0.1020, α(K)=0.0872 13, α(L)=0.01171 17, α(M)=0.00245 4, α(N)=0.000543 8, α(O)=8.81×10-5 13, α(P)=6.70E-6 10 |
5+ | ≤ 12 ps | 266.543 12 | M1+E2 | -0.04 4 | 0.0787 | α=0.0787, α(K)=0.0673 10, α(L)=0.00902 13, α(M)=0.00188 3, α(N)=0.000418 6, α(O)=6.78×10-5 10, α(P)=5.17E-6 8 | |
2412.013 | 3+ | 1.3 ps 4 | 64.135 10 | M1 | 4.26 | B(M1)(W.u.)=0.020 +14-8, α=4.26, α(K)=3.63 5, α(L)=0.499 7, α(M)=0.1046 15, α(N)=0.0232 4, α(O)=0.00375 6, α(P)=0.000281 4 | |
3+ | 1.3 ps 4 | 328.762 8 | M1+E2 | -0.049 6 | 0.0453 | B(E2)(W.u.)=2.9 +24-12, B(M1)(W.u.)=0.22 +10-5, α=0.0453, α(K)=0.0388 6, α(L)=0.00516 8, α(M)=0.001078 15, α(N)=0.000239 4, α(O)=3.88E-5 6, α(P)=2.97E-6 5 | |
3+ | 1.3 ps 4 | 815.772 19 | M1(+E2) | -0.03 1 | 0.00470 | B(E2)(W.u.)=0.013 +21-9, B(M1)(W.u.)=0.016 +8-4, α=0.00470, α(K)=0.00404 6, α(L)=0.000521 8, α(M)=0.0001085 16, α(N)=2.41E-5 4, α(O)=3.92E-6 6, α(P)=3.05E-7 5 | |
2464.08 | 3- | 0.15 ps 3 | 867.846 20 | E1 | 1.11×10-3 | B(E1)(W.u.)=0.0026 +6-4, α=1.11E-3, α(K)=0.000959 14, α(L)=0.0001200 17, α(M)=2.49E-5 4, α(N)=5.51E-6 8, α(O)=8.92E-7 13, α(P)=6.80E-8 10 | |
3- | 0.15 ps 3 | 2464.1 5 | [E3] | 9.28×10-4 | B(E3)(W.u.)=26 +12-8, α=9.28E-4, α(K)=0.000514 8, α(L)=6.61E-5 10, α(M)=1.375E-5 20, α(N)=3.05E-6 5, α(O)=4.95E-7 7, α(P)=3.81E-8 6 | ||
2480.925 | 4+ | 22 ps 7 | 68.916 6 | M1 | 3.46 | B(M1)(W.u.)=0.20 +11-6, α=3.46, α(K)=2.95 5, α(L)=0.405 6, α(M)=0.0848 12, α(N)=0.0188 3, α(O)=0.00304 5, α(P)=0.000228 4 | |
4+ | 22 ps 7 | 131.117 8 | M1+E2 | -0.13 +2-5 | 0.553 | B(E2)(W.u.)=1.1×102 +20-5, B(M1)(W.u.)=0.18 +9-5, α=0.553 9, α(K)=0.470 7, α(L)=0.0661 22, α(M)=0.0139 5, α(N)=0.00307 11, α(O)=0.000495 15, α(P)=3.61E-5 6 | |
4+ | 22 ps 7 | 397.52 5 | (E2) | 0.0206 | B(E2)(W.u.)=3.9 +23-12, α=0.0206, α(K)=0.01699 24, α(L)=0.00289 4, α(M)=0.000616 9, α(N)=0.0001349 19, α(O)=2.09E-5 3, α(P)=1.166E-6 17 | ||
2515.76 | 4+ | ≤ 2.5 ps | 432.493 12 | M1+E2 | -0.04 2 | 0.0224 | α=0.0224, α(K)=0.0192 3, α(L)=0.00253 4, α(M)=0.000527 8, α(N)=0.0001170 17, α(O)=1.90×10-5 3, α(P)=1.461E-6 21 |
4+ | ≤ 2.5 ps | 919.550 23 | E2 | 0.00242 | α=0.00242, α(K)=0.00207 3, α(L)=0.000281 4, α(M)=5.87×10-5 9, α(N)=1.298E-5 19, α(O)=2.08E-6 3, α(P)=1.496E-7 21 | ||
2521.428 | 2+ | ≤ 2.4 ps | 109.422 11 | M1+E2 | +0.26 5 | 0.952 | α=0.952 20, α(K)=0.790 12, α(L)=0.128 9, α(M)=0.0271 19, α(N)=0.0060 4, α(O)=0.00094 6, α(P)=5.98×10-5 9 |
2+ | ≤ 2.4 ps | 173.543 9 | M1 | 0.252 | α=0.252, α(K)=0.215 3, α(L)=0.0291 4, α(M)=0.00609 9, α(N)=0.001351 19, α(O)=0.000219 3, α(P)=1.658×10-5 24 | ||
2+ | ≤ 2.4 ps | 925.189 21 | E2+M1 | -0.22 4 | 0.00344 | α=0.00344 6, α(K)=0.00296 5, α(L)=0.000381 6, α(M)=7.92×10-5 12, α(N)=1.76E-5 3, α(O)=2.86E-6 5, α(P)=2.22E-7 4 | |
2+ | ≤ 2.4 ps | 2521.40 5 | E2 | 8.81×10-4 | α=8.81×10-4, α(K)=0.000293 5, α(L)=3.65E-5 6, α(M)=7.55E-6 11, α(N)=1.676E-6 24, α(O)=2.73E-7 4, α(P)=2.13E-8 3 | ||
2547.23 | 1+ | 0.19 ps +11-5 | 950.987 26 | M1(+E2) | +0.01 7 | 0.00327 | B(M1)(W.u.)=0.112 42, α=0.00327, α(K)=0.00282 4, α(L)=0.000361 5, α(M)=7.52×10-5 11, α(N)=1.669E-5 24, α(O)=2.72E-6 4, α(P)=2.12E-7 3 |
1+ | 0.19 ps +11-5 | 2547.34 11 | M1 | 9.62×10-4 | B(M1)(W.u.)=0.00114 +46-44, α=9.62×10-4, α(K)=0.000318 5, α(L)=3.97E-5 6, α(M)=8.24E-6 12, α(N)=1.83E-6 3, α(O)=2.99E-7 5, α(P)=2.36E-8 4 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
2628.81 | 6+ | 278.84 13 | M1,E2 | 0.066 | α=0.066 5, α(K)=0.054 6, α(L)=0.0089 10, α(M)=0.00190 23, α(N)=0.00042 5, α(O)=6.5×10-5 5, α(P)=3.9E-6 7 | ||
6+ | 520.964 25 | E2+M1 | -0.19 6 | 0.01387 | α=0.01387 22, α(K)=0.01189 20, α(L)=0.001563 24, α(M)=0.000326 5, α(N)=7.23×10-5 11, α(O)=1.175E-5 18, α(P)=9.01E-7 15 | ||
2899.59 | 2+ | 49 fs 9 | 1303.38 5 | M1+E2 | -1.5 +10-4 | 0.00132 | B(E2)(W.u.)=17 +8-13, B(M1)(W.u.)=0.021 +51-10, α=0.00132 21, α(K)=0.00111 18, α(L)=0.000143 22, α(M)=3.0E-5 5, α(N)=6.6E-6 10, α(O)=1.07E-6 17, α(P)=8.2E-8 15 |
2+ | 49 fs 9 | 2899.55 4 | E2 | 9.79×10-4 | B(E2)(W.u.)=0.83 +23-16, α=9.79E-4, α(K)=0.000230 4, α(L)=2.84E-5 4, α(M)=5.88E-6 9, α(N)=1.306E-6 19, α(O)=2.13E-7 3, α(P)=1.669E-8 24 | ||
3001.12 | 2+ | 0.16 ps +10-5 | 1405.20 17 | (M1+E2) | +0.7 3 | 0.00127 | B(E2)(W.u.)=3.5 +50-27, B(M1)(W.u.)=0.024 +25-14, α=0.00127 7, α(K)=0.00106 6, α(L)=0.000135 7, α(M)=2.80E-5 15, α(N)=6.2E-6 4, α(O)=1.01E-6 6, α(P)=7.8E-8 5 |
3016.9 | 0+ | ≥ 0.14 ps | 1420.7 5 | E2 | 1.03×10-3 | α=1.03×10-3, α(K)=0.000846 12, α(L)=0.0001089 16, α(M)=2.27E-5 4, α(N)=5.02E-6 7, α(O)=8.13E-7 12, α(P)=6.15E-8 9 | |
3118.55 | 2+ | 27.5 fs 85 | 3118.51 16 | (E2) | 1.04×10-3 | B(E2)(W.u.)=1.6 +7-4, α=1.04E-3, α(K)=0.000203 3, α(L)=2.50E-5 4, α(M)=5.18E-6 8, α(N)=1.149E-6 16, α(O)=1.87E-7 3, α(P)=1.472E-8 21 | |
3120.34 | 2+ | 3120.3 2 | E2 | 1.04×10-3 | α=1.04×10-3, α(K)=0.000203 3, α(L)=2.50E-5 4, α(M)=5.17E-6 8, α(N)=1.148E-6 16, α(O)=1.87E-7 3, α(P)=1.470E-8 21 | ||
3122.11 | 4+ | 1525.85 4 | E2 | 9.43×10-4 | α=9.43×10-4, α(K)=0.000737 11, α(L)=9.44E-5 14, α(M)=1.96E-5 3, α(N)=4.35E-6 6, α(O)=7.05E-7 10, α(P)=5.36E-8 8 | ||
3255.70 | 5- | 739.94 4 | (E1) | 1.53×10-3 | α=1.53×10-3, α(K)=0.001319 19, α(L)=0.0001662 24, α(M)=3.45E-5 5, α(N)=7.63E-6 11, α(O)=1.234E-6 18, α(P)=9.33E-8 13 | ||
3319.65 | 2+ | 58 fs +19-12 | 3319.61 6 | E2 | 1.10×10-3 | B(E2)(W.u.)=0.29 9, α=1.10E-3, α(K)=0.000182 3, α(L)=2.24E-5 4, α(M)=4.64E-6 7, α(N)=1.031E-6 15, α(O)=1.680E-7 24, α(P)=1.322E-8 19 | |
3395.1 | (4+) | 983.1 | M1,E2 | 0.0026 | α=0.0026 5, α(K)=0.0022 5, α(L)=0.00029 5, α(M)=6.0×10-5 10, α(N)=1.33E-5 22, α(O)=2.1E-6 4, α(P)=1.6E-7 4 | ||
3424.6 | 7- | 1316.8 3 | E1 | 6.01×10-4 | α=6.01×10-4, α(K)=0.000444 7, α(L)=5.48E-5 8, α(M)=1.134E-5 16, α(N)=2.51E-6 4, α(O)=4.08E-7 6, α(P)=3.16E-8 5 | ||
3432.8 | 7+ | 1083.0 | E2 | 1.70×10-3 | α=1.70×10-3, α(K)=0.001459 21, α(L)=0.000194 3, α(M)=4.04E-5 6, α(N)=8.94E-6 13, α(O)=1.440E-6 21, α(P)=1.059E-7 15 | ||
3471.21 | (2+) | 0.097 ps +76-35 | 3471.15 11 | (E2) | 1.15×10-3 | B(E2)(W.u.)=0.23 +15-11, α=1.15E-3, α(K)=0.0001690 24, α(L)=2.08E-5 3, α(M)=4.30E-6 6, α(N)=9.54E-7 14, α(O)=1.556E-7 22, α(P)=1.226E-8 18 | |
3484.2 | 6+ | 1134.4 | E2 | 1.55×10-3 | α=1.55×10-3, α(K)=0.001325 19, α(L)=0.0001749 25, α(M)=3.65E-5 6, α(N)=8.07E-6 12, α(O)=1.302E-6 19, α(P)=9.63E-8 14 | ||
3512.3 | 8+ | 1404.4 3 | E2 | 1.05×10-3 | α=1.05×10-3, α(K)=0.000865 13, α(L)=0.0001115 16, α(M)=2.32E-5 4, α(N)=5.14E-6 8, α(O)=8.32E-7 12, α(P)=6.29E-8 9 | ||
3539.1 | 2+ | ≥ 0.21 ps | 3539.1 3 | E2 | 1.17×10-3 | α=1.17×10-3, α(K)=0.0001636 23, α(L)=2.01E-5 3, α(M)=4.16E-6 6, α(N)=9.23E-7 13, α(O)=1.505E-7 21, α(P)=1.186E-8 17 | |
3642.8 | 1- | 1.45 fs 19 | 3642.7 3 | E1 | 1.61×10-3 | B(E1)(W.u.)=0.0030 5, α=1.61E-3, α(K)=9.12E-5 13, α(L)=1.102E-5 16, α(M)=2.28E-6 4, α(N)=5.05E-7 7, α(O)=8.24E-8 12, α(P)=6.50E-9 10 | |
3714.3 | 10+ | 23.1 ns 4 | 202.0 3 | E2 | 0.178 | B(E2)(W.u.)=0.55 14, α=0.178, α(K)=0.1351 20, α(L)=0.0335 5, α(M)=0.00731 12, α(N)=0.001583 24, α(O)=0.000234 4, α(P)=8.31E-6 13 | |
10+ | 23.1 ns 4 | 222.0 3 | E1 | 0.0274 | B(E1)(W.u.)=6.0E-7 10, α=0.0274, α(K)=0.0235 4, α(L)=0.00311 5, α(M)=0.000646 10, α(N)=0.0001423 21, α(O)=2.26E-5 4, α(P)=1.555E-6 23 | ||
3723.54 | (2+) | ≥ 0.097 ps | 3723.4 3 | (E2) | 1.23×10-3 | α=1.23×10-3, α(K)=0.0001502 21, α(L)=1.84E-5 3, α(M)=3.81E-6 6, α(N)=8.46E-7 12, α(O)=1.381E-7 20, α(P)=1.089E-8 16 | |
4173.6 | 1(-) | 3.6 fs 7 | 4173.5 8 | [E1] | 0.00180 | B(E1)(W.u.)=9.6E-4 +23-16, α=0.00180, α(K)=7.56E-5 11, α(L)=9.12E-6 13, α(M)=1.88E-6 3, α(N)=4.18E-7 6, α(O)=6.81E-8 10, α(P)=5.39E-9 8 | |
4514.9 | 1(-) | 2.7 fs 5 | 4514.8 9 | [E1] | 0.00192 | B(E1)(W.u.)=0.00101 +23-16, α=0.00192, α(K)=6.80E-5 10, α(L)=8.19E-6 12, α(M)=1.691E-6 24, α(N)=3.75E-7 6, α(O)=6.12E-8 9, α(P)=4.84E-9 7 | |
4787.8 | 1(-) | 2.3 fs 4 | 4787.7 9 | [E1] | 0.00201 | B(E1)(W.u.)=9.9E-4 +21-15, α=0.00201, α(K)=6.28E-5 9, α(L)=7.57E-6 11, α(M)=1.562E-6 22, α(N)=3.47E-7 5, α(O)=5.65E-8 8, α(P)=4.47E-9 7 | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
4851.1 | 12+ | 1136.8 3 | E2 | 1.54×10-3 | α=1.54×10-3, α(K)=0.001320 19, α(L)=0.0001741 25, α(M)=3.63E-5 5, α(N)=8.03E-6 12, α(O)=1.296E-6 19, α(P)=9.59E-8 14 | ||
4904.6 | 11- | 1190.3 4 | E1 | 6.38×10-4 | α=6.38×10-4, α(K)=0.000530 8, α(L)=6.57E-5 10, α(M)=1.360E-5 19, α(N)=3.01E-6 5, α(O)=4.90E-7 7, α(P)=3.78E-8 6 | ||
5102.1 | 13- | 250.9 3 | E1 | 0.0198 | α=0.0198, α(K)=0.01700 25, α(L)=0.00224 4, α(M)=0.000465 7, α(N)=0.0001024 15, α(O)=1.632×10-5 24, α(P)=1.137E-6 17 | ||
5157.3 | 1(-) | 2.6 fs 5 | 5157.2 12 | [E1] | 0.00211 | B(E1)(W.u.)=7.0E-4 +17-11, α=0.00211, α(K)=5.70E-5 8, α(L)=6.85E-6 10, α(M)=1.414E-6 20, α(N)=3.14E-7 5, α(O)=5.12E-8 8, α(P)=4.05E-9 6 | |
5190.2 | 1(-) | 2.1 fs 4 | 5190.1 10 | [E1] | 0.00212 | B(E1)(W.u.)=8.5E-4 +20-14, α=0.00212, α(K)=5.65E-5 8, α(L)=6.80E-6 10, α(M)=1.402E-6 20, α(N)=3.11E-7 5, α(O)=5.08E-8 8, α(P)=4.02E-9 6 | |
5211.6 | 1(-) | 3.6 fs 9 | 5211.5 14 | [E1] | 0.00213 | B(E1)(W.u.)=4.9E-4 +17-10, α=0.00213, α(K)=5.62E-5 8, α(L)=6.76E-6 10, α(M)=1.395E-6 20, α(N)=3.09E-7 5, α(O)=5.05E-8 7, α(P)=4.00E-9 6 | |
5337.3 | 1(-) | 1.8 fs 4 | 5337.2 9 | [E1] | 0.00217 | B(E1)(W.u.)=9.1E-4 +26-17, α=0.00217, α(K)=5.45E-5 8, α(L)=6.55E-6 10, α(M)=1.351E-6 19, α(N)=3.00E-7 5, α(O)=4.89E-8 7, α(P)=3.87E-9 6 | |
5548.4 | 1(-) | 0.97 fs 17 | 5548.3 7 | [E1] | 0.00223 | B(E1)(W.u.)=0.00151 +32-23, α=0.00223, α(K)=5.18E-5 8, α(L)=6.22E-6 9, α(M)=1.284E-6 18, α(N)=2.85E-7 4, α(O)=4.65E-8 7, α(P)=3.68E-9 6 | |
5573.8 | 1(-) | 1.7 fs 4 | 5573.7 14 | [E1] | 0.00223 | B(E1)(W.u.)=8.5E-4 +26-16, α=0.00223, α(K)=5.15E-5 8, α(L)=6.19E-6 9, α(M)=1.276E-6 18, α(N)=2.83E-7 4, α(O)=4.62E-8 7, α(P)=3.66E-9 6 | |
5659.9 | 1- | 0.0121 eV 29 | 5659.8 6 | E1 | 0.00226 | B(E1)(W.u.)=3.7E-5 9, α=0.00226, α(K)=5.05E-5 7, α(L)=6.06E-6 9, α(M)=1.251E-6 18, α(N)=2.78E-7 4, α(O)=4.53E-8 7, α(P)=3.59E-9 5 | |
5928.6 | 1(-) | 1.16 fs 24 | 5928.5 10 | [E1] | 0.00233 | B(E1)(W.u.)=0.00104 +27-18, α=0.00233, α(K)=4.75E-5 7, α(L)=5.71E-6 8, α(M)=1.178E-6 17, α(N)=2.61E-7 4, α(O)=4.27E-8 6, α(P)=3.38E-9 5 | |
6119.1 | 1- | 0.69 fs 12 | 6119.0 15 | E1 | B(E1)(W.u.)=0.00159 +34-24 | ||
6161.7 | 1(-) | 1.08 fs 20 | 6161.6 14 | [E1] | B(E1)(W.u.)=9.9E-4 +23-16 | ||
6295.3 | 1- | 0.46 fs 8 | 6295.1 8 | E1 | B(E1)(W.u.)=0.00219 +46-33 | ||
6397.2 | 1- | 0.28 fs 5 | 6397.0 8 | E1 | B(E1)(W.u.)=0.0034 +8-5 | ||
6439.9 | 1(-) | 0.53 fs 9 | 6439.7 14 | (E1) | B(E1)(W.u.)=0.00177 +37-26 | ||
6449.9 | 1(-) | 0.90 fs 18 | 6449.7 15 | (E1) | B(E1)(W.u.)=0.00104 +26-17 | ||
6458.5 | 1(-) | 1.00 fs 20 | 6458.3 15 | (E1) | B(E1)(W.u.)=9.3E-4 +23-16 | ||
6497.0 | 1- | 0.33 fs 6 | 6496.8 7 | E1 | B(E1)(W.u.)=0.0028 +6-4 | ||
6535.8 | 1- | 0.22 fs 3 | 6535.6 6 | E1 | B(E1)(W.u.)=0.0041 +7-5 | ||
6605.5 | 1(-) | 0.69 fs 12 | 6605.3 10 | (E1) | B(E1)(W.u.)=0.00126 +27-19 | ||
6616.2 | 1(-) | 0.74 fs 13 | 6616.0 10 | (E1) | B(E1)(W.u.)=0.00117 +25-18 | ||
6862.4 | 1- | 0.24 fs 4 | 6862.2 7 | E1 | B(E1)(W.u.)=0.0032 +7-5 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
0.0 | 0+ | STABLE | E(level): From 140Pr ε Decay. γ.S. band. |
1596.233 | 2+ | 0.0910 ps +48-44 | μ=+1.9 2 (2014StZZ) RMS charge radius <r2>1/2=4.8771 fm 18 (2013An02). E(level): From 140Pr ε Decay. γ.S. band. |
2083.259 | 4+ | 3.45 ns 3 | μ=+4.20 15, Q=0.35 7 (2013StZZ,2014StZZ) E(level): From 140Pr ε Decay. γ.S. band. |
2107.854 | 6+ | 7.3 µs 15 | E(level): From 140Pr ε Decay. γ.S. band. |
3120.34 | 2+ | Extra 2+ level found only by 1985Di11 about 2 keV higher in energy than the previous 2+, 3118.5 level found only by 1993Go23, both levels being mainly determined by a γ transition to g.s., which suggests that this can be a same level. | |
3226 | 0+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
3255.70 | 5- | Jπ(level): From L in (p,p’) (1977Sh06). | |
3394.92 | (4-) | 0.042 ps +49-21 | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). |
3395.1 | (4+) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3473.75 | 3- | 0.066 ps +21-13 | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). |
3476.3 | 8- | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3484.2 | 6+ | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3492.23 | 9- | 1.7 ns 2 | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). |
3512.3 | 8+ | E(level): From 140Pr ε Decay. γ.S. band. Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3534.6 | (3,4) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3551 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
3620.7 | 8+ | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3653 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
3710 | 5- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
3714.3 | 10+ | 23.1 ns 4 | μ=+10.3 4 (2014StZZ,1988Ka04) E(level): From 140Pr ε Decay. γ.S. band. Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). |
3792.72 | 3- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
3894.5 | 9+ | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
3912 | 2- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4000 | 4- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4053 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
4125 | 2+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
4158 | 2- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4173.6 | 1(-) | 3.6 fs 7 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
4182 | 1- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4262.5 | 10+ | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
4296 | 3-,4+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
4331 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4340 | (1-) | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4354.9 | 1 | 3.7 fs 8 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
4364 | 1- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4371 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4388 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4424 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
4437 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4448.5 | (9,11) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
4514.9 | 1(-) | 2.7 fs 5 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
4538 | 3- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4580 | 2- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4655 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4748 | 2- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4770 | 1- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
4787.8 | 1(-) | 2.3 fs 4 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
4827 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
4851.1 | 12+ | E(level): From 140Pr ε Decay. γ.S. band. Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
4875 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
4883 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4904.6 | 11- | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
4951 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
4958.0 | (11+) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
4979 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5026 | 2-,3- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
5069.5 | (9,11) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
5093.4 | (12-) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
5101 | GE 5 | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5102.1 | 13- | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
5157.3 | 1(-) | 2.6 fs 5 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5190.2 | 1(-) | 2.1 fs 4 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5196 | 2-,3- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
5211.6 | 1(-) | 3.6 fs 9 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5245 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5295 | 5-,6+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5330 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5335.0 | (12-) | Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN). | |
5337.3 | 1(-) | 1.8 fs 4 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5377 | 4+,5- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5419.0 | (14-) | Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities. | |
5424 | 2-,3- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
5466 | 2-,3- | E(level): From (α,α’γ) and (γ,γ’) datasets. Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05). | |
5470 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5494 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
5548.4 | 1(-) | 0.97 fs 17 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5573.8 | 1(-) | 1.7 fs 4 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5574 | (0+) | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5624 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5650 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5703 | 1-,2+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5721 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5759 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5809 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5823 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5896 | 1-,2+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
5928.6 | 1(-) | 1.16 fs 24 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
5940 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
5989 | (3-,4+) | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
6029 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
6078 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
6119.1 | 1- | 0.69 fs 12 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6130.6 | 1 | 1.5 fs 3 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6161.7 | 1(-) | 1.08 fs 20 | Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6187 | 2+,3- | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
6226 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
6245 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
6255 | (1) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
6273.6 | 1 | 1.05 fs 20 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6295.3 | 1- | 0.46 fs 8 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
E(level) | Jπ(level) | T1/2(level) | Comments |
6303.6 | (15-) | Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities. | |
6327.8 | 1 | 1.3 fs 5 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6343.3 | 1 | 0.78 fs 15 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6352.7 | 1 | 0.69 fs 13 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6364 | 3-,4+ | E(level): From 140Ce(γ,γ’) dataset. Jπ(level): From L in (p,t) (1977Sh06). | |
6397.2 | 1- | 0.28 fs 5 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6439.9 | 1(-) | 0.53 fs 9 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6449.9 | 1(-) | 0.90 fs 18 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6458.5 | 1(-) | 1.00 fs 20 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6484.8 | 1 | 1.00 fs 20 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6497.0 | 1- | 0.33 fs 6 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6535.8 | 1- | 0.22 fs 3 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6549.1 | 1 | 1.3 fs 3 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6574.9 | 1 | 1.16 fs 23 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6605.5 | 1(-) | 0.69 fs 12 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6616.2 | 1(-) | 0.74 fs 13 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6771.7 | (2+) | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. | |
6781.9 | 1 | 0.85 fs 19 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6796.6 | (16-) | Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities. | |
6841.8 | 1 | 0.79 fs 22 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6862.4 | 1- | 0.24 fs 4 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6889.2 | (15,16) | Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities. | |
6905.9 | 1 | 0.45 fs 10 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6932.6 | 1 | 0.52 fs 11 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
6960.4 | 1 | 0.47 fs 10 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
E(level) | Jπ(level) | T1/2(level) | Comments |
7038.2 | (17-) | Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities. | |
7206.0 | 1 | 0.31 fs 5 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
7214.8 | 1 | 0.34 fs 6 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
7341.5 | 1 | 0.9 fs 2 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
7673.4 | 1 | 0.76 fs 18 | Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset. T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation. |
E(level) | E(gamma) | Comments |
2628.81 | 278.84 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 520.964 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
2899.59 | 996.2 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1303.38 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2899.55 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3016.9 | 1420.7 | E(γ): From 140Pr ε Decay I(γ): From 140Pr ε Decay | 3016.3 | E(γ): From 140Pr ε Decay I(γ): From 140Pr ε Decay |
3120.34 | 3120.3 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3122.11 | 657.5 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 772.50 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1525.85 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3168.3 | 1085 | E(γ): γ peak confounded with first Ge escape of intense 1596γ (1993Go23, (n,n’γ)) |
3219.95 | 1623.71 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3255.70 | 739.94 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 774.8 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3319.65 | 772.50 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1235.8 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1724.7 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3319.61 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3335.47 | 855.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 985.63 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1227.71 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1252.12 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1739.4 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3360.24 | 1010.45 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1276.9 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
E(level) | E(gamma) | Comments |
3391.09 | 1307.73 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1794.93 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3394.92 | 982.89 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1045.11 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1287.03 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1311.56 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3424.6 | 1316.8 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
3436.54 | 1088.65 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1533.2 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3436.8 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3471.21 | 1568.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3471.15 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3473.75 | 1125.64 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3476.3 | 51.7 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
3491.2 | 944.0 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3491.2 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3492.23 | 1384.2 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
3512.3 | 1404.4 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
3567.5 | 1484.3 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3567.0 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3642.8 | 1739.4 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3642.7 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) M(γ): from γ(θ) and linear pol in (γ,γ’) |
3646.7 | 1743.31 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3646.6 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3648.23 | 1564.92 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2052.07 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
E(level) | E(gamma) | Comments |
3657.64 | 1307.73 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1549.76 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1574.5 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3684.2 | 1220.5 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3684.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3708.60 | 1227.71 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2112.30 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3708.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3714.3 | 202.0 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) | 222.0 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
3723.54 | 1311.56 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3723.4 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3735.3 | 3735.2 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3767.97 | 1220.5 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1252.12 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1287.03 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1684.4 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2171.82 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3792.72 | 893.7 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1276.9 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1311.56 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2196.6 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3836.1 | 1753.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2239.8 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3847.10 | 808.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1497.31 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1739.4 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 1763.6 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
E(level) | E(gamma) | Comments |
3853.2 | 2256.8 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 3853.3 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3879.3 | 3879.2 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3910.93 | 2314.68 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3957.93 | 1493.6 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2361.80 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
3984.20 | 1901.4 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2387.90 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
4053 | 4053 | E(γ): From 140Ce(γ,γ’) dataset |
4164.0 | 2567.8 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 4163.5 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
4171.1 | 2576.1 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 4171.0 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
4173.6 | 4173.5 | E(γ): from (α,α’γ) and (γ,γ’) |
4279.9 | 2196.6 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) | 2683.6 | E(γ): From 140Ce(n,n’γ) I(γ): From 140Ce(n,n’γ) |
4331 | 4331 | E(γ): From 140Ce(γ,γ’) dataset |
4354.9 | 4354.8 | E(γ): From 140Ce(γ,γ’) dataset |
4371 | 4371 | E(γ): From 140Ce(γ,γ’) dataset |
4388 | 4388 | E(γ): From 140Ce(γ,γ’) dataset |
4437 | 4437 | E(γ): From 140Ce(γ,γ’) dataset |
4514.9 | 4514.8 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
4655 | 4655 | E(γ): From 140Ce(γ,γ’) dataset |
4787.8 | 4787.7 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
4851.1 | 1136.8 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
E(level) | E(gamma) | Comments |
4875 | 4875 | E(γ): From 140Ce(γ,γ’) dataset |
4883 | 4883 | E(γ): From 140Ce(γ,γ’) dataset |
4904.6 | 1190.3 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
4951 | 4951 | E(γ): From 140Ce(γ,γ’) dataset |
5093.4 | 188.9 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
5102.1 | 250.9 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
5157.3 | 5157.2 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
5190.2 | 5190.1 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
5211.6 | 5211.5 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
5245 | 5245 | E(γ): From 140Ce(γ,γ’) dataset |
5330 | 5330 | E(γ): From 140Ce(γ,γ’) dataset |
5337.3 | 5337.2 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
5419.0 | 318.0 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
5470 | 5470 | E(γ): From 140Ce(γ,γ’) dataset |
5494 | 5494 | E(γ): From 140Ce(γ,γ’) dataset |
5548.4 | 5548.3 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
5573.8 | 5573.7 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
5624 | 5624 | E(γ): From 140Ce(γ,γ’) dataset |
5659.9 | 5659.8 | E(γ): From (α,α’γ) and (γ,γ’) datasets M(γ): from γ(θ) and linear pol in (γ,γ’) |
5693.3 | 592.3 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
5721 | 5721 | E(γ): From 140Ce(γ,γ’) dataset |
5759 | 5759 | E(γ): From 140Ce(γ,γ’) dataset |
5809 | 5809 | E(γ): From 140Ce(γ,γ’) dataset |
5823 | 5823 | E(γ): From 140Ce(γ,γ’) dataset |
5928.6 | 5928.5 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
E(level) | E(gamma) | Comments |
5940 | 5940 | E(γ): From 140Ce(γ,γ’) dataset |
6029 | 6029 | E(γ): From 140Ce(γ,γ’) dataset |
6119.1 | 6119.0 | E(γ): From 140Ce(γ,γ’) dataset |
6130.6 | 6130.5 | E(γ): From 140Ce(γ,γ’) dataset |
6161.7 | 6161.6 | E(γ): From (α,α’γ) and (γ,γ’) datasets |
6226 | 6226 | E(γ): From 140Ce(γ,γ’) dataset |
6245 | 6245 | E(γ): From 140Ce(γ,γ’) dataset |
6255 | 6255 | E(γ): From 140Ce(γ,γ’) dataset |
6273.6 | 6273.4 | E(γ): From 140Ce(γ,γ’) dataset |
6295.3 | 6295.1 | E(γ): From 140Ce(γ,γ’) dataset |
6303.6 | 1202.6 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
6327.8 | 6327.6 | E(γ): From 140Ce(γ,γ’) dataset |
6343.3 | 6343.1 | E(γ): From 140Ce(γ,γ’) dataset |
6352.7 | 6352.5 | E(γ): From 140Ce(γ,γ’) dataset |
6397.2 | 6397.0 | E(γ): From 140Ce(γ,γ’) dataset |
6439.9 | 6439.7 | E(γ): From 140Ce(γ,γ’) dataset |
6449.9 | 6449.7 | E(γ): From 140Ce(γ,γ’) dataset |
6458.5 | 6458.3 | E(γ): From 140Ce(γ,γ’) dataset |
6484.8 | 6484.6 | E(γ): From 140Ce(γ,γ’) dataset |
6497.0 | 6496.8 | E(γ): From 140Ce(γ,γ’) dataset |
6535.8 | 6535.6 | E(γ): From 140Ce(γ,γ’) dataset |
6549.1 | 6548.9 | E(γ): From 140Ce(γ,γ’) dataset |
6574.9 | 6574.7 | E(γ): From 140Ce(γ,γ’) dataset |
6605.5 | 6605.3 | E(γ): From 140Ce(γ,γ’) dataset |
6616.2 | 6616.0 | E(γ): From 140Ce(γ,γ’) dataset |
E(level) | E(gamma) | Comments |
6771.7 | 6771.5 | E(γ): From 140Ce(γ,γ’) dataset |
6781.9 | 6781.7 | E(γ): From 140Ce(γ,γ’) dataset |
6796.6 | 493.0 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
6841.8 | 6841.6 | E(γ): From 140Ce(γ,γ’) dataset |
6862.4 | 6862.2 | E(γ): From 140Ce(γ,γ’) dataset |
6889.2 | 1470.2 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
6905.9 | 6905.7 | E(γ): From 140Ce(γ,γ’) dataset |
6932.6 | 6932.4 | E(γ): From 140Ce(γ,γ’) dataset |
6960.4 | 6960.2 | E(γ): From 140Ce(γ,γ’) dataset |
7038.2 | 734.6 | E(γ): From 238U(12C,Fγ)) I(γ): From 238U(12C,Fγ)) |
7206.0 | 7205.8 | E(γ): From 140Ce(γ,γ’) dataset |
7214.8 | 7214.6 | E(γ): From 140Ce(γ,γ’) dataset |
7341.5 | 7341.3 | E(γ): From 140Ce(γ,γ’) dataset |
7673.4 | 7673.2 | E(γ): From 140Ce(γ,γ’) dataset |
Measured nuclear charge radii and isotopes shifts: 2000Ga58, 1999GaZU, 1999Is02, 1997Is06, 1997IsZY.