ADOPTED LEVELS, GAMMAS for 135Ce
Authors: Balraj Singh, Alexander A. Rodionov and Yuri L. Khazov | Citation: Nucl. Data Sheets 109, 517 (2008) | Cutoff date: 22-Jan-2008
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-3680 keV 16 | S(n)= 7855 keV 23 | S(p)= 6687 keV 23 | Q(α)= -357 keV 11 | ||
Reference: 2012WA38 |
References: | |||
A | 135Ce IT decay (20 S) | B | 135Pr ε decay (24 M) |
C | 122Sn(16O,3nγ) | D | 122Sn(18O,5nγ) |
E | 124Sn(16O,5nγ) |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
0.0 | ABCDE | 1/2(+) | 17.7 h 3 % ε = 100 | |||||
82.67 5 | ABCDE | 3/2(+) | 0.53 ns 6 | 82.64 7 | 100 | M1(+E2) | 0.0 | 1/2(+) |
296.11 5 | ABCDE | (5/2+) | 213.45 6 296.12 5 | 100 4 25 3 | M1 E2 | 82.67 0.0 | 3/2(+) 1/2(+) | |
296.12 5 | B | 1/2(+),3/2(+) | 213.45 6 ? 296.12 5 | 100 | M1(+E2) | 82.67 0.0 | 3/2(+) 1/2(+) | |
445.81 21 | A CDE | (11/2-) | 20 s 1 % IT = 100 | 149.7 2 | 100 | E3 | 296.11 | (5/2+) |
620.95 11 | B | 3/2(+),5/2(+) | 324.9 2 324.9 2 538.2 2 620.9 2 | ≈4.8 ≈4.8 100 11 19 3 | M1,E2 M1,E2 M1(+E2) E2(+M1) | 296.11 296.12 82.67 0.0 | (5/2+) 1/2(+),3/2(+) 3/2(+) 1/2(+) | |
696.47 21 | B | (1/2+,3/2+,5/2+) | 400.7 5 ? 400.7 5 ? 613.8 2 697.5 2 ? | <22 <22 100 15 <77 | [M1,E2] [M1,E2] M1(+E2) M1,E2 | 296.11 296.12 82.67 0.0 | (5/2+) 1/2(+),3/2(+) 3/2(+) 1/2(+) | |
780.29 15 | B | (1/2+,3/2+,5/2+) | 484.3 3 484.3 3 697.5 2 780.6 10 | ≈133 ≈267 <350 100 24 | M1,E2 M1,E2 M1,E2 M1,E2 | 296.11 296.12 82.67 0.0 | (5/2+) 1/2(+),3/2(+) 3/2(+) 1/2(+) | |
806.90 19 | B | (1/2,3/2,5/2+) | 724.4 6 806.9 2 | 33 17 100 17 | 82.67 0.0 | 3/2(+) 1/2(+) | ||
1016.84 15 | B | (1/2+,3/2+,5/2+) | 720.6 8 934.1 2 1016.9 2 | 58 25 100 17 85 12 | M1(+E2) M1,E2 | 296.11 82.67 0.0 | (5/2+) 3/2(+) 1/2(+) | |
1035.7 4 | CDE | (13/2-) | 589.7 4 | 100 | D+Q | 445.81 | (11/2-) | |
1145.2 4 | CDE | (15/2-) | 109.5 2 699.6 4 | 1.6 4 100 11 | (Q) | 1035.7 445.81 | (13/2-) (11/2-) | |
1367.4 5 ? | B | (1/2,3/2,5/2+) | 747 1 1284.6 8 1367.3 6 | 63 40 63 19 100 19 | 620.95 82.67 0.0 | 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 | |
1670.0 5 | CDE | (15/2-) | 525 1 634.9 4 | <8 100 8 | D D(+Q) | 1145.2 1035.7 | (15/2-) (13/2-) | |
1728.7 5 ? | B | (1/2,3/2,5/2) | 1107 1 ? 1432.9 6 ? 1646.0 8 ? | 32 14 100 18 64 14 | 620.95 296.11 82.67 | 3/2(+),5/2(+) (5/2+) 3/2(+) | ||
1834.9 3 | B | (1/2,3/2,5/2) | 1538.9 4 1538.9 4 1751.9 6 | ≈105 ≈105 100 17 | 296.11 296.12 82.67 | (5/2+) 1/2(+),3/2(+) 3/2(+) | ||
1869.4 5 | CDE | (17/2-) | 724.3 4 833.1 4 | 54 6 100 11 | D+Q (Q) | 1145.2 1035.7 | (15/2-) (13/2-) | |
1950.6 9 | B | (1/2,3/2,5/2+) | 1143 2 1867 2 1951 1 | 21 14 93 40 100 30 | 806.90 82.67 0.0 | (1/2,3/2,5/2+) 3/2(+) 1/2(+) | ||
2020.6 6 | B | (1/2,3/2,5/2+) | 1214.2 8 1937 2 2020 1 | 100 30 60 20 70 20 | 806.90 82.67 0.0 | (1/2,3/2,5/2+) 3/2(+) 1/2(+) | ||
2051.5 5 | CDE | (19/2-) | 181.9 4 906.2 4 | 3.8 10 100 9 | Q | 1869.4 1145.2 | (17/2-) (15/2-) | |
2125.3 5 | CDE | (19/2+) | 8.2 ns 4 | 256.0 3 | 100 | (E1) | 1869.4 | (17/2-) |
2249.0 5 | CDE | (19/2-) | 379.2 4 579.5 4 | 38 6 100 13 | D Q | 1869.4 1670.0 | (17/2-) (15/2-) | |
2551.0 6 | CDE | (23/2+) | 425.6 4 | 100 | (Q) | 2125.3 | (19/2+) | |
2682.2 6 | CDE | (21/2-) | 433.5 4 | 100 | D+Q | 2249.0 | (19/2-) | |
2887.4 7 | CDE | (21/2-) | 836 1 1019 1 | 100 20 100 20 | D | 2051.5 1869.4 | (19/2-) (17/2-) | |
2946.2 6 | D | (19/2+) | 1076.6 4 | 100 | 1869.4 | (17/2-) | ||
2948.0 6 | CDE | (23/2-) | 265.7 4 896 1 | 100 13 88 13 | D | 2682.2 2051.5 | (21/2-) (19/2-) | |
3054.1 6 | CD | (21/2+) | 108.0 4 503.1 4 928.7 4 | <25 100 25 100 25 | D D+Q | 2946.2 2551.0 2125.3 | (19/2+) (23/2+) (19/2+) | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
3076.2 6 | D | (21/2+) | 129.8 4 525.2 4 951.1 4 | <43 100 33 <67 | D | 2946.2 2551.0 2125.3 | (19/2+) (23/2+) (19/2+) | |
3104.0 6 | CDE | (23/2-) | 216 1 1052.1 4 | <6 100 13 | (Q) | 2887.4 2051.5 | (21/2-) (19/2-) | |
3229.0 6 | CD | (23/2+) | 152.7 4 175.1 4 678 1 | <19 100 13 38 13 | D D(+Q) | 3076.2 3054.1 2551.0 | (21/2+) (21/2+) (23/2+) | |
3431.1 7 | CD | (25/2+) | 202.1 4 | 100 | D(+Q) | 3229.0 | (23/2+) | |
3505.4 6 | CDE | (25/2-) | 557.3 4 823.5 4 | 100 33 100 33 | D Q | 2948.0 2682.2 | (23/2-) (21/2-) | |
3514.6 7 | CD | (27/2+) | 963.6 4 | 100 | Q | 2551.0 | (23/2+) | |
3699.1 8 | CD | (27/2+) | 268.0 4 | 100 | D+Q | 3431.1 | (25/2+) | |
3701.8 7 | CDE | (27/2-) | 753.8 4 | 100 | Q | 2948.0 | (23/2-) | |
3771.7 6 ? | DE | (27/2+) | 257 1 ? 1220.6 4 | <40 100 20 | Q | 3514.6 2551.0 | (27/2+) (23/2+) | |
4032.3 7 | DE | (25/2-) | 928 1 ? | 100 | 3104.0 | (23/2-) | ||
4065.4 6 | CDE | (25/2-) | 962 1 1178.3 4 | 100 50 100 50 | D (Q) | 3104.0 2887.4 | (23/2-) (21/2-) | |
4127.5 9 | CD | (29/2+) | 428.3 4 696 1 | 100 9 <18 | D+Q | 3699.1 3431.1 | (27/2+) (25/2+) | |
4183.0 6 | DE | (27/2-) | 117.9 4 150.7 4 1078.6 4 | 43 14 100 14 57 14 | D D | 4065.4 4032.3 3104.0 | (25/2-) (25/2-) (23/2-) | |
4259.5 7 | CD | (31/2+) | 745.0 4 | 100 | Q | 3514.6 | (27/2+) | |
4400.1 8 | D | (31/2-) | 698.3 4 | 100 | Q | 3701.8 | (27/2-) | |
4460.4 6 | DE | (29/2-) | 277.1 4 | 100 | D(+Q) | 4183.0 | (27/2-) | |
4485.8 9 | CD | (31/2+) | 358.2 4 786.8 4 | 100 10 20 10 | D(+Q) | 4127.5 3699.1 | (29/2+) (27/2+) | |
4495.9 7 | DE | (27/2-) | 313 991 1 | 100 | 4183.0 3505.4 | (27/2-) (25/2-) | ||
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
4634.9 6 | DE | (29/2-) | 139.1 4 452 863.2 4 933 1 1130 1 | <28 100 20 <40 60 20 | D (D) (D) (Q) | 4495.9 4183.0 3771.7 3701.8 3505.4 | (27/2-) (27/2-) (27/2+) (27/2-) (25/2-) | |
4813.3 6 | DE | (31/2-) | 178.5 4 318 352.4 4 631 | 100 11 22 11 | D(+Q) D | 4634.9 4495.9 4460.4 4183.0 | (29/2-) (27/2-) (29/2-) (27/2-) | |
4830.3 7 | DE | (31/2-) | 195? 370.0 4 | 100 | D+Q | 4634.9 4460.4 | (29/2-) (29/2-) | |
4978.6 9 | D | (33/2+) | 492.9 4 851 1 | 100 14 <29 | D | 4485.8 4127.5 | (31/2+) (29/2+) | |
5062.2 7 | DE | (33/2-) | 232 249.0 4 427 603 803 1 ? | 100 11 <22 | D(+Q) | 4830.3 4813.3 4634.9 4460.4 4259.5 | (31/2-) (31/2-) (29/2-) (29/2-) (31/2+) | |
5206.0 7 | DE | (33/2-) | 375.6 4 392? 571? 746 1 | 100 25 <50 | D | 4830.3 4813.3 4634.9 4460.4 | (31/2-) (31/2-) (29/2-) (29/2-) | |
5324.4 8 | D | (35/2+) | 1064.9 4 | 100 | (Q) | 4259.5 | (31/2+) | |
5342.1 13 | D | (35/2-) | 942 1 | 100 | Q | 4400.1 | (31/2-) | |
5359.3 7 | DE | (35/2-) | 0.64 ps 11 | 153 297.5 4 529 545 | | D | 5206.0 5062.2 4830.3 4813.3 | (33/2-) (33/2-) (31/2-) (31/2-) |
5427.8 10 | D | (35/2+) | 449.2 4 942 1 | 100 20 <40 | D | 4978.6 4485.8 | (33/2+) (31/2+) | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
5651.1 7 | DE | (35/2-) | 445.1 4 589? 821 1 837? | 100 8 <15 | D+Q Q | 5206.0 5062.2 4830.3 4813.3 | (33/2-) (33/2-) (31/2-) (31/2-) | |
5751.5 7 | DE | (37/2-) | 0.451 ps 21 | 100 392.2 4 545 689 | | D(+Q) | 5651.1 5359.3 5206.0 5062.2 | (35/2-) (35/2-) (33/2-) (33/2-) |
5941.7 12 | D | (37/2+) | 514 1 963 1 | | 5427.8 4978.6 | (35/2+) (33/2+) | ||
6086.0 7 | DE | (37/2-) | 434.9 4 727 880 1 1024 | 100 9 <18 | D+Q | 5651.1 5359.3 5206.0 5062.2 | (35/2-) (35/2-) (33/2-) (33/2-) | |
6256.3 7 | DE | (39/2-) | 0.299 ps 25 | 170 504.6 4 605 897 | | D | 6086.0 5751.5 5651.1 5359.3 | (37/2-) (37/2-) (35/2-) (35/2-) |
6299.4 13 | D | (39/2+) | 975 1 | 100 | 5324.4 | (35/2+) | ||
6443.8 13 | D | (39/2+) | 502 1 1016 1 ? | | 5941.7 5427.8 | (37/2+) (35/2+) | ||
6477.1 17 | D | (39/2-) | 1135 1 | 100 | 5342.1 | (35/2-) | ||
6525.9 8 | DE | (39/2-) | 440.0 4 775 875 1 1167 | 100 17 <33 | D+Q | 6086.0 5751.5 5651.1 5359.3 | (37/2-) (37/2-) (35/2-) (35/2-) | |
6840.2 8 | DE | (41/2-) | 0.163 ps +8-10 | 314 583.6 4 754 1089 | | 6525.9 6256.3 6086.0 5751.5 | (39/2-) (39/2-) (37/2-) (37/2-) | |
E(level) (keV) | XREF | Jπ(level) | T1/2(level) | E(γ) (keV) | I(γ) | M(γ) | Final Levels | |
6993.7 8 | DE | (41/2-) | 468.0 4 737 908 1 1242 | 100 33 <67 | D | 6525.9 6256.3 6086.0 5751.5 | (39/2-) (39/2-) (37/2-) (37/2-) | |
7470.4 9 | DE | (43/2-) | 477 630 1 944? 1214 | | 6993.7 6840.2 6525.9 6256.3 | (41/2-) (41/2-) (39/2-) (39/2-) | ||
7493.1 9 | DE | (43/2-) | 500 1 652 968 1 1238 | | D | 6993.7 6840.2 6525.9 6256.3 | (41/2-) (41/2-) (39/2-) (39/2-) | |
8008.9 10 | DE | (45/2-) | 517 1 538 1168 | | 7493.1 7470.4 6840.2 | (43/2-) (43/2-) (41/2-) | ||
8034.6 9 ? | DE | (45/2-) | 542? 564 1 ? 1041? 1194? | | 7493.1 7470.4 6993.7 6840.2 | (43/2-) (43/2-) (41/2-) (41/2-) |
Jπ(level): For high-spin states (J>11/2) the assignments are from γγ(θ) (DCO) and/or γ(θ) data and associated band structures. In Jπ arguments, ΔJ=2 statement refers to stretched quadrupole (most likely E2) transition and ΔJ=1 to stretched dipole (with possible quadrupole admixture) transition
M(γ): From ce data in 135Pr decay when multipolarity is explicitly defined such as M1, E2, etc. The assignments d or Q (most likely E2) are from angular correlation/distribution data in high-spin reactions.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 1 - νh11/2~#π[(h11/2)(g7/2)]. | |||||||
2946.2 6 | (19/2+) | ||||||
3076.2 6 | (21/2+) | 129.8 4 525.2 4 951.1 4 | <43 100 33 <67 | D | 2946.2 2551.0 2125.3 | (19/2+) (23/2+) (19/2+) | |
3229.0 6 | (23/2+) | 152.7 4 175.1 4 678 1 | <19 100 13 38 13 | D D(+Q) | 3076.2 3054.1 2551.0 | (21/2+) (21/2+) (23/2+) | |
3431.1 7 | (25/2+) | 202.1 4 | 100 | D(+Q) | 3229.0 | (23/2+) | |
3699.1 8 | (27/2+) | 268.0 4 | 100 | D+Q | 3431.1 | (25/2+) | |
4127.5 9 | (29/2+) | 428.3 4 696 1 | 100 9 <18 | D+Q | 3699.1 3431.1 | (27/2+) (25/2+) | |
4485.8 9 | (31/2+) | 358.2 4 786.8 4 | 100 10 20 10 | D(+Q) | 4127.5 3699.1 | (29/2+) (27/2+) | |
4978.6 9 | (33/2+) | 492.9 4 851 1 | 100 14 <29 | D | 4485.8 4127.5 | (31/2+) (29/2+) | |
5427.8 10 | (35/2+) | 449.2 4 942 1 | 100 20 <40 | D | 4978.6 4485.8 | (33/2+) (31/2+) | |
5941.7 12 | (37/2+) | 514 1 963 1 | | 5427.8 4978.6 | (35/2+) (33/2+) | ||
6443.8 13 | (39/2+) | 502 1 1016 1 ? | | 5941.7 5427.8 | (37/2+) (35/2+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 2 - νs1/2~#νh11/22. | |||||||
2125.3 5 | (19/2+) | 8.2 ns 4 | |||||
2551.0 6 | (23/2+) | 425.6 4 | 100 | (Q) | 2125.3 | (19/2+) | |
3514.6 7 | (27/2+) | 963.6 4 | 100 | Q | 2551.0 | (23/2+) | |
4259.5 7 | (31/2+) | 745.0 4 | 100 | Q | 3514.6 | (27/2+) | |
5324.4 8 | (35/2+) | 1064.9 4 | 100 | (Q) | 4259.5 | (31/2+) | |
6299.4 13 | (39/2+) | 975 1 | 100 | 5324.4 | (35/2+) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 3 - νh11/2~#πh11/22. | |||||||
4065.4 6 | (25/2-) | ||||||
4183.0 6 | (27/2-) | 117.9 4 150.7 4 1078.6 4 | 43 14 100 14 57 14 | D D | 4065.4 4032.3 3104.0 | (25/2-) (25/2-) (23/2-) | |
4460.4 6 | (29/2-) | 277.1 4 | 100 | D(+Q) | 4183.0 | (27/2-) | |
4830.3 7 | (31/2-) | 195? 370.0 4 | 100 | D+Q | 4634.9 4460.4 | (29/2-) (29/2-) | |
5206.0 7 | (33/2-) | 375.6 4 392? 571? 746 1 | 100 25 <50 | D | 4830.3 4813.3 4634.9 4460.4 | (31/2-) (31/2-) (29/2-) (29/2-) | |
5651.1 7 | (35/2-) | 445.1 4 589? 821 1 837? | 100 8 <15 | D+Q Q | 5206.0 5062.2 4830.3 4813.3 | (33/2-) (33/2-) (31/2-) (31/2-) | |
6086.0 7 | (37/2-) | 434.9 4 727 880 1 1024 | 100 9 <18 | D+Q | 5651.1 5359.3 5206.0 5062.2 | (35/2-) (35/2-) (33/2-) (33/2-) | |
6525.9 8 | (39/2-) | 440.0 4 775 875 1 1167 | 100 17 <33 | D+Q | 6086.0 5751.5 5651.1 5359.3 | (37/2-) (37/2-) (35/2-) (35/2-) | |
6993.7 8 | (41/2-) | 468.0 4 737 908 1 1242 | 100 33 <67 | D | 6525.9 6256.3 6086.0 5751.5 | (39/2-) (39/2-) (37/2-) (37/2-) | |
7493.1 9 | (43/2-) | 500 1 652 968 1 1238 | | D | 6993.7 6840.2 6525.9 6256.3 | (41/2-) (41/2-) (39/2-) (39/2-) | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
8008.9 10 | (45/2-) | 517 1 538 1168 | | 7493.1 7470.4 6840.2 | (43/2-) (43/2-) (41/2-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 4 - TRIAXIAL band. | |||||||
445.81 21 | (11/2-) | 20 s 1 % IT = 100 | |||||
1035.7 4 | (13/2-) | 589.7 4 | 100 | D+Q | 445.81 | (11/2-) | |
1145.2 4 | (15/2-) | 109.5 2 699.6 4 | 1.6 4 100 11 | (Q) | 1035.7 445.81 | (13/2-) (11/2-) | |
1869.4 5 | (17/2-) | 724.3 4 833.1 4 | 54 6 100 11 | D+Q (Q) | 1145.2 1035.7 | (15/2-) (13/2-) | |
2051.5 5 | (19/2-) | 181.9 4 906.2 4 | 3.8 10 100 9 | Q | 1869.4 1145.2 | (17/2-) (15/2-) | |
2887.4 7 | (21/2-) | 836 1 1019 1 | 100 20 100 20 | D | 2051.5 1869.4 | (19/2-) (17/2-) | |
3104.0 6 | (23/2-) | 216 1 1052.1 4 | <6 100 13 | (Q) | 2887.4 2051.5 | (21/2-) (19/2-) | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 5 - Four-quasiparticle band. | |||||||
4495.9 7 | (27/2-) | ||||||
4634.9 6 | (29/2-) | 139.1 4 452 863.2 4 933 1 1130 1 | <28 100 20 <40 60 20 | D (D) (D) (Q) | 4495.9 4183.0 3771.7 3701.8 3505.4 | (27/2-) (27/2-) (27/2+) (27/2-) (25/2-) | |
4813.3 6 | (31/2-) | 178.5 4 318 352.4 4 631 | 100 11 22 11 | D(+Q) D | 4634.9 4495.9 4460.4 4183.0 | (29/2-) (27/2-) (29/2-) (27/2-) | |
5062.2 7 | (33/2-) | 232 249.0 4 427 603 803 1 ? | 100 11 <22 | D(+Q) | 4830.3 4813.3 4634.9 4460.4 4259.5 | (31/2-) (31/2-) (29/2-) (29/2-) (31/2+) | |
5359.3 7 | (35/2-) | 0.64 ps 11 | 153 297.5 4 529 545 | | D | 5206.0 5062.2 4830.3 4813.3 | (33/2-) (33/2-) (31/2-) (31/2-) |
5751.5 7 | (37/2-) | 0.451 ps 21 | 100 392.2 4 545 689 | | D(+Q) | 5651.1 5359.3 5206.0 5062.2 | (35/2-) (35/2-) (33/2-) (33/2-) |
6256.3 7 | (39/2-) | 0.299 ps 25 | 170 504.6 4 605 897 | | D | 6086.0 5751.5 5651.1 5359.3 | (37/2-) (37/2-) (35/2-) (35/2-) |
6840.2 8 | (41/2-) | 0.163 ps +8-10 | 314 583.6 4 754 1089 | | 6525.9 6256.3 6086.0 5751.5 | (39/2-) (39/2-) (37/2-) (37/2-) | |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
7470.4 9 | (43/2-) | 477 630 1 944? 1214 | | 6993.7 6840.2 6525.9 6256.3 | (41/2-) (41/2-) (39/2-) (39/2-) | ||
8034.6 9 | (45/2-) | 542? 564 1 ? 1041? 1194? | | 7493.1 7470.4 6993.7 6840.2 | (43/2-) (43/2-) (41/2-) (41/2-) | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) | I(γ) | M(γ) | Final Levels | |
Band 6 - νh11/2~#νh11/22. | |||||||
3701.8 7 | (27/2-) | ||||||
4400.1 8 | (31/2-) | 698.3 4 | 100 | Q | 3701.8 | (27/2-) | |
5342.1 13 | (35/2-) | 942 1 | 100 | Q | 4400.1 | (31/2-) | |
6477.1 17 | (39/2-) | 1135 1 | 100 | 5342.1 | (35/2-) |
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
82.67 | 3/2(+) | 0.53 ns 6 | 82.64 7 | M1(+E2) | 0.4 LT | 2.19 | B(M1)(W.u.)=0.022 3, α=2.19 15, α(K)=1.77 4, α(L)=0.33 9, α(M)=0.071 21, α(N)=0.015 5, α(O)=0.0024 6, α(P)=0.000133 3, α(N+)=0.018 5 |
296.11 | (5/2+) | 213.45 6 | M1 | 0.1429 | α=0.1429, α(K)=0.1221 18, α(L)=0.01645 23, α(M)=0.00344 5, α(N)=0.000763 11, α(O)=0.0001238 18, α(P)=9.40×10-6 14, α(N+)=0.000897 13 | ||
(5/2+) | 296.12 5 | E2 | 0.0508 | α=0.0508, α(K)=0.0407 6, α(L)=0.00792 12, α(M)=0.001704 24, α(N)=0.000371 6, α(O)=5.64×10-5 8, α(P)=2.68E-6 4, α(N+)=0.000431 6 | |||
296.12 | 1/2(+),3/2(+) | 296.12 5 | M1(+E2) | 0.9 LT | 0.0576 | α=0.0576 22, α(K)=0.0487 24, α(L)=0.0071 3, α(M)=0.00148 7, α(N)=0.000328 14, α(O)=5.24×10-5 14, α(P)=3.6E-6 3, α(N+)=0.000384 15 | |
445.81 | (11/2-) | 20 s 1 % IT = 100 | 149.7 2 | E3 | 3.73 | B(E3)(W.u.)=7.2E-3 4, α=3.73, α(K)=1.515 23, α(L)=1.72 3, α(M)=0.396 7, α(N)=0.0851 14, α(O)=0.01182 19, α(P)=8.39E-5 13, α(N+)=0.0970 16 | |
620.95 | 3/2(+),5/2(+) | 324.9 2 | M1,E2 | 0.042 | α=0.042 5, α(K)=0.035 5, α(L)=0.00551 21, α(M)=0.00117 6, α(N)=0.000257 11, α(O)=4.04×10-5 7, α(P)=2.6E-6 5, α(N+)=0.000300 11 | ||
3/2(+),5/2(+) | 324.9 2 | M1,E2 | 0.042 | α=0.042 5, α(K)=0.035 5, α(L)=0.00551 21, α(M)=0.00117 6, α(N)=0.000257 11, α(O)=4.04×10-5 7, α(P)=2.6E-6 5, α(N+)=0.000300 11 | |||
3/2(+),5/2(+) | 538.2 2 | M1(+E2) | 0.7 LT | 0.0123 | α=0.0123 7, α(K)=0.0105 7, α(L)=0.00140 6, α(M)=0.000292 11, α(N)=6.5×10-5 3, α(O)=1.05E-5 5, α(P)=7.9E-7 6, α(N+)=7.6E-5 3 | ||
3/2(+),5/2(+) | 620.9 2 | E2(+M1) | 1.2 GT | 0.0067 | α=0.0067 7, α(K)=0.0057 6, α(L)=0.00081 6, α(M)=0.000170 11, α(N)=3.76×10-5 25, α(O)=6.0E-6 5, α(P)=4.1E-7 5, α(N+)=4.4E-5 3 | ||
696.47 | (1/2+,3/2+,5/2+) | 400.7 5 | [M1,E2] | 0.024 | α=0.024 4, α(K)=0.020 4, α(L)=0.00295 14, α(M)=0.000621 23, α(N)=0.000137 6, α(O)=2.18×10-5 15, α(P)=1.5E-6 4, α(N+)=0.000160 8 | ||
(1/2+,3/2+,5/2+) | 400.7 5 | [M1,E2] | 0.024 | α=0.024 4, α(K)=0.020 4, α(L)=0.00295 14, α(M)=0.000621 23, α(N)=0.000137 6, α(O)=2.18×10-5 15, α(P)=1.5E-6 4, α(N+)=0.000160 8 | |||
(1/2+,3/2+,5/2+) | 613.8 2 | M1(+E2) | 0.7 LT | 0.0088 | α=0.0088 6, α(K)=0.0076 5, α(L)=0.00100 5, α(M)=0.000209 10, α(N)=4.64×10-5 21, α(O)=7.5E-6 4, α(P)=5.7E-7 4, α(N+)=5.44E-5 25 | ||
(1/2+,3/2+,5/2+) | 697.5 2 | M1,E2 | 0.0057 | α=0.0057 12, α(K)=0.0049 10, α(L)=0.00066 11, α(M)=0.000138 21, α(N)=3.1×10-5 5, α(O)=4.9E-6 9, α(P)=3.6E-7 9, α(N+)=3.6E-5 6 | |||
780.29 | (1/2+,3/2+,5/2+) | 484.3 3 | M1,E2 | 0.014 | α=0.014 3, α(K)=0.0121 24, α(L)=0.00172 18, α(M)=0.00036 4, α(N)=8.0×10-5 8, α(O)=1.28E-5 15, α(P)=8.9E-7 21, α(N+)=9.4E-5 10 | ||
(1/2+,3/2+,5/2+) | 484.3 3 | M1,E2 | 0.014 | α=0.014 3, α(K)=0.0121 24, α(L)=0.00172 18, α(M)=0.00036 4, α(N)=8.0×10-5 8, α(O)=1.28E-5 15, α(P)=8.9E-7 21, α(N+)=9.4E-5 10 | |||
(1/2+,3/2+,5/2+) | 697.5 2 | M1,E2 | 0.0057 | α=0.0057 12, α(K)=0.0049 10, α(L)=0.00066 11, α(M)=0.000138 21, α(N)=3.1×10-5 5, α(O)=4.9E-6 9, α(P)=3.6E-7 9, α(N+)=3.6E-5 6 | |||
(1/2+,3/2+,5/2+) | 780.6 10 | M1,E2 | 0.0044 | α=0.0044 9, α(K)=0.0037 8, α(L)=0.00050 9, α(M)=0.000104 17, α(N)=2.3×10-5 4, α(O)=3.7E-6 7, α(P)=2.8E-7 7, α(N+)=2.7E-5 5 | |||
1016.84 | (1/2+,3/2+,5/2+) | 720.6 8 | M1(+E2) | 1 LT | 0.0058 | α=0.0058 6, α(K)=0.0050 5, α(L)=0.00066 5, α(M)=0.000137 10, α(N)=3.03×10-5 23, α(O)=4.9E-6 4, α(P)=3.7E-7 4, α(N+)=3.6E-5 3 | |
(1/2+,3/2+,5/2+) | 934.1 2 | M1,E2 | 0.0029 | α=0.0029 6, α(K)=0.0025 5, α(L)=0.00032 6, α(M)=6.8×10-5 11, α(N)=1.50E-5 25, α(O)=2.4E-6 5, α(P)=1.8E-7 4, α(N+)=1.8E-5 3 | |||
1035.7 | (13/2-) | 589.7 4 | D+Q | -0.42 +6-10 | |||
1670.0 | (15/2-) | 634.9 4 | D(+Q) | -0.02 5 | |||
1869.4 | (17/2-) | 724.3 4 | D+Q | -0.25 9 | |||
2125.3 | (19/2+) | 8.2 ns 4 | 256.0 3 | (E1) | 0.0188 | B(E1)(W.u.)=1.8E-6 1, α=0.0188, α(K)=0.01613 24, α(L)=0.00212 3, α(M)=0.000441 7, α(N)=9.71E-5 14, α(O)=1.547E-5 23, α(P)=1.080E-6 16, α(N+)=0.0001136 17 | |
2682.2 | (21/2-) | 433.5 4 | D+Q | -0.16 4 | |||
3054.1 | (21/2+) | 928.7 4 | D+Q | -0.16 8 | |||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
3229.0 | (23/2+) | 175.1 4 | D(+Q) | +0.05 8 | |||
3431.1 | (25/2+) | 202.1 4 | D(+Q) | +0.07 7 | |||
3699.1 | (27/2+) | 268.0 4 | D+Q | -0.07 2 | |||
4127.5 | (29/2+) | 428.3 4 | D+Q | -0.11 3 | |||
4460.4 | (29/2-) | 277.1 4 | D(+Q) | -0.03 5 | |||
4485.8 | (31/2+) | 358.2 4 | D(+Q) | -0.06 7 | |||
4813.3 | (31/2-) | 178.5 4 | D(+Q) | +0.06 7 | |||
4830.3 | (31/2-) | 370.0 4 | D+Q | -0.10 6 | |||
5062.2 | (33/2-) | 249.0 4 | D(+Q) | -0.02 +4-6 | |||
5651.1 | (35/2-) | 445.1 4 | D+Q | -0.23 3 | |||
5751.5 | (37/2-) | 0.451 ps 21 | 392.2 4 | D(+Q) | -0.04 6 | ||
6086.0 | (37/2-) | 434.9 4 | D+Q | -0.18 5 | |||
6525.9 | (39/2-) | 440.0 4 | D+Q | -0.19 +8-11 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
445.81 | (11/2-) | 20 s 1 % IT = 100 | E(level): TRIAXIAL band. |
1035.7 | (13/2-) | E(level): TRIAXIAL band. | |
1145.2 | (15/2-) | E(level): TRIAXIAL band. | |
1869.4 | (17/2-) | E(level): TRIAXIAL band. | |
2051.5 | (19/2-) | E(level): TRIAXIAL band. | |
2125.3 | (19/2+) | 8.2 ns 4 | μ=-0.66 10 (1989Ra17,1982Ze01) E(level): νs1/2~#νh11/22. |
2551.0 | (23/2+) | E(level): νs1/2~#νh11/22. | |
2887.4 | (21/2-) | E(level): TRIAXIAL band. | |
2946.2 | (19/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
3076.2 | (21/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
3104.0 | (23/2-) | E(level): TRIAXIAL band. | |
3229.0 | (23/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
3431.1 | (25/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
3514.6 | (27/2+) | E(level): νs1/2~#νh11/22. | |
3699.1 | (27/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
3701.8 | (27/2-) | E(level): νh11/2~#νh11/22. | |
4065.4 | (25/2-) | E(level): νh11/2~#πh11/22. | |
4127.5 | (29/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
4183.0 | (27/2-) | E(level): νh11/2~#πh11/22. | |
4259.5 | (31/2+) | E(level): νs1/2~#νh11/22. | |
4400.1 | (31/2-) | E(level): νh11/2~#νh11/22. | |
4460.4 | (29/2-) | E(level): νh11/2~#πh11/22. | |
4485.8 | (31/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
4495.9 | (27/2-) | E(level): Four-quasiparticle band. | |
4634.9 | (29/2-) | E(level): Four-quasiparticle band. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
4813.3 | (31/2-) | E(level): Four-quasiparticle band. | |
4830.3 | (31/2-) | E(level): νh11/2~#πh11/22. | |
4978.6 | (33/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
5062.2 | (33/2-) | E(level): Four-quasiparticle band. | |
5206.0 | (33/2-) | E(level): νh11/2~#πh11/22. | |
5324.4 | (35/2+) | E(level): νs1/2~#νh11/22. | |
5342.1 | (35/2-) | E(level): νh11/2~#νh11/22. | |
5359.3 | (35/2-) | 0.64 ps 11 | E(level): Four-quasiparticle band. T1/2(level): From ΔS(a) method (2005JaZZ). |
5427.8 | (35/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
5651.1 | (35/2-) | E(level): νh11/2~#πh11/22. | |
5751.5 | (37/2-) | 0.451 ps 21 | E(level): Four-quasiparticle band. T1/2(level): From ΔS(a) method (2005JaZZ). |
5941.7 | (37/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
6086.0 | (37/2-) | E(level): νh11/2~#πh11/22. | |
6256.3 | (39/2-) | 0.299 ps 25 | E(level): Four-quasiparticle band. T1/2(level): From ΔS(a) method (2005JaZZ). |
6299.4 | (39/2+) | E(level): νs1/2~#νh11/22. | |
6443.8 | (39/2+) | E(level): νh11/2~#π[(h11/2)(g7/2)]. | |
6477.1 | (39/2-) | E(level): νh11/2~#νh11/22. | |
6525.9 | (39/2-) | E(level): νh11/2~#πh11/22. | |
6840.2 | (41/2-) | 0.163 ps +8-10 | E(level): Four-quasiparticle band. T1/2(level): From ΔS(a) method (2005JaZZ). |
6993.7 | (41/2-) | E(level): νh11/2~#πh11/22. | |
7470.4 | (43/2-) | E(level): Four-quasiparticle band. | |
7493.1 | (43/2-) | E(level): νh11/2~#πh11/22. | |
8008.9 | (45/2-) | E(level): νh11/2~#πh11/22. | |
8034.6 | (45/2-) | E(level): Four-quasiparticle band. |
E(level) | E(gamma) | Comments |
82.67 | 82.64 | E(γ): from 135Pr ε decay M(γ): from α(K)exp and K/L ratio in 135Pr ε decay and α(exp) deduced from intensity balance in 135Ce IT decay. In a ce spectrum shown by 1970Dr04 (in 135Ce IT decay), K/L ratio seems much smaller than K/L(theory for M1)=7.3, suggesting some E2 admixture |
296.11 | 213.45 | E(γ): from 135Pr ε decay. Eγ=212.9 2 in IT decay. Multiply placed | 296.12 | E(γ): from 135Pr ε decay. Eγ=295.8 5 in IT decay. Multiply placed I(γ): from IT decay M(γ): α(K)exp in IT decay gives E2(+M1) with δ>1.2, ΔJπ requires E2 |
296.12 | 213.45 | E(γ): Multiply placed I(γ): probable weak component | 296.12 | E(γ): Multiply placed |
445.81 | 149.7 | E(γ): from (16O,3nγ) |
620.95 | 324.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 324.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
696.47 | 400.7 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 400.7 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity | 697.5 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
780.29 | 484.3 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 484.3 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 697.5 | E(γ): Multiply placed with undivided intensity I(γ): Multiply placed with undivided intensity |
1035.7 | 589.7 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
1145.2 | 699.6 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
1670.0 | 525 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 634.9 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
1834.9 | 1538.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided | 1538.9 | E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided |
1869.4 | 724.3 | I(γ): other: 227 23 in (16O,3nγ) M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 833.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
2051.5 | 906.2 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
2125.3 | 256.0 | M(γ): ΔJ=1, dipole from γγ(θ) and assigned Jπ’s |
2249.0 | 379.2 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 579.5 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
E(level) | E(gamma) | Comments |
2551.0 | 425.6 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
2682.2 | 433.5 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
2887.4 | 836 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
2948.0 | 265.7 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
3054.1 | 108.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 928.7 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
3076.2 | 525.2 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
3104.0 | 1052.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
3229.0 | 152.7 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 175.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
3431.1 | 202.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
3505.4 | 557.3 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 823.5 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
3514.6 | 963.6 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
3699.1 | 268.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
3701.8 | 753.8 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
3771.7 | 1220.6 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
4065.4 | 962 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 1178.3 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
4127.5 | 428.3 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
4183.0 | 117.9 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 150.7 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
4259.5 | 745.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
4400.1 | 698.3 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
4460.4 | 277.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
E(level) | E(gamma) | Comments |
4485.8 | 358.2 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
4634.9 | 139.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 863.2 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 933 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
4813.3 | 178.5 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 352.4 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
4830.3 | 370.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
4978.6 | 492.9 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
5062.2 | 249.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
5206.0 | 375.6 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
5324.4 | 1064.9 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
5342.1 | 942 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
5359.3 | 297.5 | E(γ): Possibly the most intense branch M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
5427.8 | 449.2 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
5651.1 | 445.1 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions | 821 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=2, quadrupole (E2) |
5751.5 | 392.2 | E(γ): Possibly the most intense branch M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
6086.0 | 434.9 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
6256.3 | 504.6 | E(γ): Possibly the most intense branch M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
6525.9 | 440.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
6840.2 | 583.6 | E(γ): Possibly the most intense branch |
6993.7 | 468.0 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
7470.4 | 630 | E(γ): Possibly the most intense branch |
7493.1 | 500 | M(γ): γγ(θ) (DCO) and/or γ(θ) in high-spin reactions indicate ΔJ=1, dipole with possible quadrupole admixture for Δπ=no transitions |
8008.9 | 517 | E(γ): Possibly the most intense branch |
E(level) | E(gamma) | Comments |
Nuclear structure calculations: 2004Yo04 (levels, transition rates), 1996Gr03 (analyzed band structures), 1992Zh10 (identical bands), 1985Jo03 (levels, transition rates IBA model), 1983Ch46 (yrast and near-yrast routhians, cranking model), 1982Ch30 (M1-γ spectra, core+ quasiparticle model).
Q-value: Note: Current evaluation has used the following Q record -3689 16 7860 23 6695 23 -366 11 2003Au03