List of levels for 130LA

ADOPTED LEVELS, GAMMAS for ¹³⁰La

Author: Balraj Singh | Citation: Nucl. Data Sheets 93, 33 (2001) | Cutoff date: 11-May-2001

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-2.20×10³ keV 4	S(n)= 8.37×10³ keV 4	S(p)= 3.85×10³ keV 3	Q(α)= 3.0×10² keV 3
Reference: 2012WA38

References:
A	¹³⁰Ce ε decay (22.9 M)	B	⁵¹V(⁸²Se,3nγ)
C	⁹⁸Mo(³⁶S,3npγ),¹¹⁵In(¹⁸O,3nγ)	D	¹¹⁶Cd(¹⁹F,5nγ),¹²⁴Te(¹⁰B,4nγ)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A	3(+)	8.7 m 1 % ε = 100
110.44 9	A	(1+,2,3+)	17 ns 5	110.4 2	100	[D,E2]	0.0	3(+)
131.01 8	A	1+	77 ns 10	131.1 2	100	[E2]	0.0	3(+)
219.73 9	A	(1+)		88.9 2 109.3 3 219.8 2	15.2 8 37 4 100 10	[M1,E2] [D,E2] [E2]	131.01 110.44 0.0	1+ (1+,2,3+) 3(+)
267.31 9	A	(1+)		47.5 3 136.4 2 267.3 2	0.7 4 100.0 22 94.2 22	[M1,E2] [M1,E2] [E2]	219.73 131.01 0.0	(1+) 1+ 3(+)
304.10 12	A	(1)		193.6 2 304.1 2	15 4 100 5	[D,E2] [D,E2]	110.44 0.0	(1+,2,3+) 3(+)
307.48 9	A	(1)		87.9 3 196.9 2 307.5 2	2.4 7 17.1 11 100.0 7	[D,E2] [D,E2] [D,E2]	219.73 110.44 0.0	(1+) (1+,2,3+) 3(+)
340.61 9	A	(1+)		73.5 3 209.6 2 230.5 2 340.6 2	1.1 5 100.0 17 6.9 17 36.1 8	[M1,E2] [M1,E2] [D,E2] [D,E2]	267.31 131.01 110.44 0.0	(1+) 1+ (1+,2,3+) 3(+)
350.71 10	A	(1)		46.7 3 83.4 2 131.0 3 240.1 2 350.8 2	4.1 18 16 4 51 3 42 6 100 9	[D,E2] [D,E2] [D,E2] [D,E2]	304.10 267.31 219.73 110.44 0.0	(1) (1+) (1+) (1+,2,3+) 3(+)
384.78 9	A	(1)		77.6 2 80.5 3 253.7 2 274.2 2 384.8 2	1.2 8 1.5 10 100 8 62 3 48 10	[D,E2] [D,E2] [D,E2] [D,E2]	307.48 304.10 131.01 110.44 0.0	(1) (1) 1+ (1+,2,3+) 3(+)
430.18 17	A	(1)		163.0 3 430.2 3	100 24 90 29	[D,E2]	267.31 0.0	(1+) 3(+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
431.51 15	A	(1)		127.5 3 300.5 2 431.5 3	2.8 18 100 6 32 18	[D,E2] [D,E2]	304.10 131.01 0.0	(1) 1+ 3(+)
443.22 13	A	(1)		139.0 3 175.8 3 443.2 3	3.5 24 31 15 100 29	[D,E2] [D,E2]	304.10 267.31 0.0	(1) (1+) 3(+)
444.39 9	A	(1+)		59.6 2 103.9 2 136.6 3 176.9 2 313.3 2 333.9 2 444.2 3	11.7 20 18 4 27 9 100 4 19 4 18 4 37 11	[D,E2] [M1,E2] [D,E2] [D,E2]	384.78 340.61 307.48 267.31 131.01 110.44 0.0	(1) (1+) (1) (1+) 1+ (1+,2,3+) 3(+)
477.15 18	A	(1)		209.9 2 477.0 3	85 8 100 30	[D,E2]	267.31 0.0	(1+) 3(+)
477.96 13	A	(1+)		93.3 2 170.5 3 346.8 2 478.0 3	30 6 23 3 100 10 33 10	[D,E2] [D,E2]	384.78 307.48 131.01 0.0	(1) (1) 1+ 3(+)
481.89 16	A	(1)		141.3 2 214.7 3 481.7 3	91 60 55 11 100 15	[D,E2] [D,E2]	340.61 267.31 0.0	(1+) (1+) 3(+)
523.88 11	A	(1+)		173.1 2 183.2 2 256.5 2 393.0 2 524.0 3	13 3 53 3 100 3 21 4 24 5	[D,E2] [M1,E2] [M1,E2]	350.71 340.61 267.31 131.01 0.0	(1) (1+) (1+) 1+ 3(+)
589.06 16	A	(1)		248.4 2 321.7 3 589.2 3	52 18 36 10 100 14		340.61 267.31 0.0	(1+) (1+) 3(+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
594.28 18	A	(1)		463.3 2 594.2 3	100 10 11 5		131.01 0.0	1+ 3(+)
606.75 18	A	(1)		387.0 2 606.8 3	41 3 100 33		219.73 0.0	(1+) 3(+)
645.49 14	A	(1)		294.8 2 535.1 2 645.3 3	84 25 100 50 76 19		350.71 110.44 0.0	(1) (1+,2,3+) 3(+)
672.93 23	A	(0,1)		541.7 3 562.7 3	100 5 10 6		131.01 110.44	1+ (1+,2,3+)
697.01 14	A	(1)		266.9 2 389.2 3 566.2 2 696.7 3	63 8 25 13 100 23 13 8		430.18 307.48 131.01 0.0	(1) (1) 1+ 3(+)
810.47 22	A	(1)		590.7 3 810.5 3	84 16 100 50		219.73 0.0	(1+) 3(+)
827.5 4	A	(0,1)		520.0 3	100		307.48	(1)
913.62 13	A	(1+)		470.5 2 528.8 2 605.8 3 694.2 3 782.5 3	37 9 82 16 100 33 25 13 30 4		443.22 384.78 307.48 219.73 131.01	(1) (1) (1) (1+) 1+
985.91 22	A	(0,1)		718.6 2	100		267.31	(1+)
1032.45 12	A	(1+)		724.9 2 765.2 3 901.3 2 922.0 3 1032.8 3	66 11 45 9 100 11 28 9 39 12		307.48 267.31 131.01 110.44 0.0	(1) (1+) 1+ (1+,2,3+) 3(+)
1168.72 13	A	(1+)		737.3 3 818.0 2 828.3 3 861.2 2 1037.5 3	36 7 43 5 24 5 100 6 66 7		431.51 350.71 340.61 307.48 131.01	(1) (1) (1+) (1) 1+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1196.79 10	A	1+		752.2 2 812.0 3 856.3 2 889.4 2 977.2 2 1065.8 3 1196.6 2	30.1 24 16 4 36.5 19 31.2 19 100 8 19.1 19 49.2 25		444.39 384.78 340.61 307.48 219.73 131.01 0.0	(1+) (1) (1+) (1) (1+) 1+ 3(+)
1289.04 12	A	1+		845.6 2 948.8 3 1069.3 3 1158.0 3 1289.1 2	19 3 29 5 14 3 49 4 100 5		443.22 340.61 219.73 131.01 0.0	(1) (1+) (1+) 1+ 3(+)
1431.19 13	A	(1+)		986.6 2 1123.8 3 1164.0 3 1300.3 3 1431.3 3	100 57 53 7 80 24 81 23 81 23		444.39 307.48 267.31 131.01 0.0	(1+) (1) (1+) 1+ 3(+)
0+X	B C D
5.1+X 5	B
45.1+X 10	B
88.4+X 7	B C D	(6-)
113.9+X 4	B C D			113.9 5	100		0+X
150.3+X 8	B			105.2 5	100		45.1+X
160.3+X 5	B
160.4+X 5	B C D	(7-)		46.4 5 72.0 5	<16 100 3		113.9+X 88.4+X	(6-)
279.0+X 5	B C D	(8-)		118.7 3 190.7 7	100.0 6 2.6 9	M1+E2	160.4+X 88.4+X	(7-) (6-)
385.4+X 4	B C D	(9+)		106.4 5 225.1 3 235.1 7 271.5 3 380.3 3 385.4 5	7.2 6 27.3 13 >55 100 4 40.1 18 13.1 9	Q Q	279.0+X 160.3+X 150.3+X 113.9+X 5.1+X 0+X	(8-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
456.3+X 5	B C D	(9-)		177.2 3 295.9 3	100.0 16 13.8 16	D+Q	279.0+X 160.4+X	(8-) (7-)
522.9+X 5	B C D	(10+)		137.5 3	100	D+Q	385.4+X	(9+)
677.5+X 6	B C D	(10-)		221.2 3 398.4 3	100.0 23 46.6 23	M1+E2	456.3+X 279.0+X	(9-) (8-)
802.2+X 5	B C D	(11+)		279.4 3 416.9 5	100.0 21 3.6 21	M1+E2	522.9+X 385.4+X	(10+) (9+)
947.0+X 6	B C D	(11-)		269.5 7 490.7 3	87.6 21 100.0 21	D+Q (Q)	677.5+X 456.3+X	(10-) (9-)
1048.5+X 5	B C D	(12+)		246.3 3 525.7 3	100.0 20 44.5 20	M1+E2	802.2+X 522.9+X	(11+) (10+)
1077.9+X 10	D	(11+)		555			522.9+X	(10+)
1250.2+X 6	B C D	(12-)		303.2 3 572.7 3	54.3 20 100.0 20	D+Q (Q)	947.0+X 677.5+X	(11-) (10-)
1422.8+X 6	B D	(13+)		374.3 7 620.6 3	100.0 26 39.4 26		1048.5+X 802.2+X	(12+) (11+)
1434.5+X 10	D	(12+)		357 632			1077.9+X 802.2+X	(11+) (11+)
1597.3+X 6	B C D	(13-)		347.1 7 650.3 3	39.3 21 100.0 21	(Q)	1250.2+X 947.0+X	(12-) (11-)
1748.5+X 6	B D	(14+)		325.7 3 700.0 3	68.1 19 100.0 19		1422.8+X 1048.5+X	(13+) (12+)
1778.2+X 10	D	(13+)		700 730			1077.9+X 1048.5+X	(11+) (12+)
1970.1+X 7	B C D	(14-)		372.8 7 719.9 3	39.5 22 100.0 22	Q	1597.3+X 1250.2+X	(13-) (12-)
2163.0+X 10	D	(14+)		385 728? 740			1778.2+X 1434.5+X 1422.8+X	(13+) (12+) (13+)
2194.1+X 6	B D	(15+)		445.6 7 771.3 3	100 5 72 5		1748.5+X 1422.8+X	(14+) (13+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2384.4+X 7	B C D	(15-)		414.3 5 787.1 3	16.8 21 100.0 21	(Q)	1970.1+X 1597.3+X	(14-) (13-)
2586.7+X 6	B D	(16+)		392.6 3 838.2 3	31 5 100 5		2194.1+X 1748.5+X	(15+) (14+)
2590.3+X 10	D	(15+)		426? 812 842			2163.0+X 1778.2+X 1748.5+X	(14+) (13+) (14+)
2818.2+X 7	B C D	(16-)		433.8 5 848.1 3	22.1 26 100.0 26		2384.4+X 1970.1+X	(15-) (14-)
2961.0+X 10	D	(16+)		372? 767? 798			2590.3+X 2194.1+X 2163.0+X	(15+) (15+) (14+)
3096.1+X 7	B D	(17+)		509.5 7 902.1 7	82 6 100 6		2586.7+X 2194.1+X	(16+) (15+)
3289.5+X 7	B C D	(17-)		471.3 5 905.1 7	17 3 100 3		2818.2+X 2384.4+X	(16-) (15-)
3541.5+X 7	B D	(18+)		445.4 7 954.9 7	24 4 100 4		3096.1+X 2586.7+X	(17+) (16+)
3771.4+X 8	B C D	(18-)		481.8 5 953.1 7			3289.5+X 2818.2+X	(17-) (16-)
4105.0+X 7	B	(19+)		563.5 5 1008.9 3	33 5 100 5		3541.5+X 3096.1+X	(18+) (17+)
4271.6+X 8	B C	(19-)		500.2 7 982.0 3	28 7 100 7		3771.4+X 3289.5+X	(18-) (17-)
4589.6+X 7	B D	(20+)		484.6 7 1048.1 3	19 5 100 5		4105.0+X 3541.5+X	(19+) (18+)
4720.2+X 8	B	(20-)		448.6 5 948.8 7	69 9 100 9		4271.6+X 3771.4+X	(19-) (18-)
5185.0+X 8	B	(21-)		464.8 5 913.4 5	100 6 92 6		4720.2+X 4271.6+X	(20-) (19-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5185.2+X 8	B	(21+)		595.6 5 1080.2 5	32 7 100 7		4589.6+X 4105.0+X	(20+) (19+)
5644.5+X 8	B	(22-)		459.4 5 924.2 5	69 4 100 4		5185.0+X 4720.2+X	(21-) (20-)
5696.8+X 10	B	(22+)		511.7 7 1107 1	30 9 100 9		5185.2+X 4589.6+X	(21+) (20+)
6156.8+X 8	B	(23-)		512.4 5 971.8 5	55 6 100 6		5644.5+X 5185.0+X	(22-) (21-)
6658.1+X 8	B	(24-)		501.5 7 1013.4 5	30 5 100 5		6156.8+X 5644.5+X	(23-) (22-)
6818.8+X 17	B	(24+)		1122.0 14	100		5696.8+X	(22+)
7203.2+X 10	B	(25-)		545.0 7 1046.5 5			6658.1+X 6156.8+X	(24-) (23-)
7759.0+X 10	B	(26-)		555.8 7 1100.8 14	11 6 100 6		7203.2+X 6658.1+X	(25-) (24-)
7949.8+X 22	B	(26+)		1131.0 14	100		6818.8+X	(24+)
8282.7+X 11	B	(27-)		523.7 5 1079.5 14	11 6 100 6		7759.0+X 7203.2+X	(26-) (25-)
0.0+Y	B	(7)
86.9+Y 9	B	(9)
358.8+Y 5	B	(9)		358.8 5	100	Q	0.0+Y	(7)
489.7+Y 7	B	(10)		130.9 5 402.8 5	100 7 57 5	D	358.8+Y 86.9+Y	(9) (9)
732.6+Y 8	B	(11)		242.9 3	100		489.7+Y	(10)
1046.6+Y 9	B	(12)		314.0 3	100		732.6+Y	(11)
1418.2+Y 9	B	(13)		371.6 3	100		1046.6+Y	(12)
1841.2+Y 10	B	(14)		423.0 3	100		1418.2+Y	(13)
2305.6+Y 10	B	(15)		464.4 3	100		1841.2+Y	(14)
2807.9+Y 10	B	(16)		502.3 5 966.7 5	100 9 18 2		2305.6+Y 1841.2+Y	(15) (14)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3340.0+Y 11	B	(17)		532.1 5 1034.4 14	100 10 31 5		2807.9+Y 2305.6+Y	(16) (15)
3889.5+Y 12	B	(18)		549.5 5 1081.6 14	100 11 44 11		3340.0+Y 2807.9+Y	(17) (16)
4462.0+Y 13	B	(19)		572.5 5 1122.0 14	100 13 33 5		3889.5+Y 3340.0+Y	(18) (17)
5054.8+Y 13	B	(20)		592.8 5 1165.3 14	100 15 92 15		4462.0+Y 3889.5+Y	(19) (18)
5638.0+Y 14	B	(21)		583.2 5	100		5054.8+Y	(20)
Z	B	J AP (16)
762.4+Z	B	J+2		762.4	0.35		Z	J AP (16)
1613.9+Z	B	J+4		851.5	0.80		762.4+Z	J+2
2534.4+Z	B	J+6		920.5	1.00		1613.9+Z	J+4
3532.1+Z	B	J+8		997.7	1.00		2534.4+Z	J+6
4604.7+Z	B	J+10		1072.6	1.00		3532.1+Z	J+8
5753.0+Z	B	J+12		1148.3	0.75		4604.7+Z	J+10
6982.4+Z	B	J+14		1229.4	0.65		5753.0+Z	J+12
8301.0+Z	B	J+16		1318.6	0.50		6982.4+Z	J+14
9713.4+Z	B	J+18		1412.4	0.40		8301.0+Z	J+16

M(γ): From γ(θ) in ¹¹⁶Cd(¹⁹F,5nγ), unless otherwise stated. Mult=d or D+Q is from ΔJ=1 and mult=Q for ΔJ=2, stretched (most likely E2) transition indicated by γ(θ)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - πh_11/2νg_7/2, α=1
160.4+X 5	(7-)
456.3+X 5	(9-)		177.2 3 295.9 3	100.0 16 13.8 16	D+Q	279.0+X 160.4+X	(8-) (7-)
947.0+X 6	(11-)		269.5 7 490.7 3	87.6 21 100.0 21	D+Q (Q)	677.5+X 456.3+X	(10-) (9-)
1597.3+X 6	(13-)		347.1 7 650.3 3	39.3 21 100.0 21	(Q)	1250.2+X 947.0+X	(12-) (11-)
2384.4+X 7	(15-)		414.3 5 787.1 3	16.8 21 100.0 21	(Q)	1970.1+X 1597.3+X	(14-) (13-)
3289.5+X 7	(17-)		471.3 5 905.1 7	17 3 100 3		2818.2+X 2384.4+X	(16-) (15-)
4271.6+X 8	(19-)		500.2 7 982.0 3	28 7 100 7		3771.4+X 3289.5+X	(18-) (17-)
5185.0+X 8	(21-)		464.8 5 913.4 5	100 6 92 6		4720.2+X 4271.6+X	(20-) (19-)
6156.8+X 8	(23-)		512.4 5 971.8 5	55 6 100 6		5644.5+X 5185.0+X	(22-) (21-)
7203.2+X 10	(25-)		545.0 7 1046.5 5			6658.1+X 6156.8+X	(24-) (23-)
8282.7+X 11	(27-)		523.7 5 1079.5 14	11 6 100 6		7759.0+X 7203.2+X	(26-) (25-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - πh_11/2νg_7/2, α=0
88.4+X 7	(6-)
279.0+X 5	(8-)		118.7 3 190.7 7	100.0 6 2.6 9	M1+E2	160.4+X 88.4+X	(7-) (6-)
677.5+X 6	(10-)		221.2 3 398.4 3	100.0 23 46.6 23	M1+E2	456.3+X 279.0+X	(9-) (8-)
1250.2+X 6	(12-)		303.2 3 572.7 3	54.3 20 100.0 20	D+Q (Q)	947.0+X 677.5+X	(11-) (10-)
1970.1+X 7	(14-)		372.8 7 719.9 3	39.5 22 100.0 22	Q	1597.3+X 1250.2+X	(13-) (12-)
2818.2+X 7	(16-)		433.8 5 848.1 3	22.1 26 100.0 26		2384.4+X 1970.1+X	(15-) (14-)
3771.4+X 8	(18-)		481.8 5 953.1 7			3289.5+X 2818.2+X	(17-) (16-)
4720.2+X 8	(20-)		448.6 5 948.8 7	69 9 100 9		4271.6+X 3771.4+X	(19-) (18-)
5644.5+X 8	(22-)		459.4 5 924.2 5	69 4 100 4		5185.0+X 4720.2+X	(21-) (20-)
6658.1+X 8	(24-)		501.5 7 1013.4 5	30 5 100 5		6156.8+X 5644.5+X	(23-) (22-)
7759.0+X 10	(26-)		555.8 7 1100.8 14	11 6 100 6		7203.2+X 6658.1+X	(25-) (24-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - πh_11/2νh_11/2, α=1
385.4+X 4	(9+)
802.2+X 5	(11+)		279.4 3 416.9 5	100.0 21 3.6 21	M1+E2	522.9+X 385.4+X	(10+) (9+)
1422.8+X 6	(13+)		374.3 7 620.6 3	100.0 26 39.4 26		1048.5+X 802.2+X	(12+) (11+)
2194.1+X 6	(15+)		445.6 7 771.3 3	100 5 72 5		1748.5+X 1422.8+X	(14+) (13+)
3096.1+X 7	(17+)		509.5 7 902.1 7	82 6 100 6		2586.7+X 2194.1+X	(16+) (15+)
4105.0+X 7	(19+)		563.5 5 1008.9 3	33 5 100 5		3541.5+X 3096.1+X	(18+) (17+)
5185.2+X 8	(21+)		595.6 5 1080.2 5	32 7 100 7		4589.6+X 4105.0+X	(20+) (19+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - πh_11/2νh_11/2, α=0
522.9+X 5	(10+)
1048.5+X 5	(12+)		246.3 3 525.7 3	100.0 20 44.5 20	M1+E2	802.2+X 522.9+X	(11+) (10+)
1748.5+X 6	(14+)		325.7 3 700.0 3	68.1 19 100.0 19		1422.8+X 1048.5+X	(13+) (12+)
2586.7+X 6	(16+)		392.6 3 838.2 3	31 5 100 5		2194.1+X 1748.5+X	(15+) (14+)
3541.5+X 7	(18+)		445.4 7 954.9 7	24 4 100 4		3096.1+X 2586.7+X	(17+) (16+)
4589.6+X 7	(20+)		484.6 7 1048.1 3	19 5 100 5		4105.0+X 3541.5+X	(19+) (18+)
5696.8+X 10	(22+)		511.7 7 1107 1	30 9 100 9		5185.2+X 4589.6+X	(21+) (20+)
6818.8+X 17	(24+)		1122.0 14	100		5696.8+X	(22+)
7949.8+X 22	(26+)		1131.0 14	100		6818.8+X	(24+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=1
1077.9+X 10	(11+)
1778.2+X 10	(13+)		700 730			1077.9+X 1048.5+X	(11+) (12+)
2590.3+X 10	(15+)		426? 812 842			2163.0+X 1778.2+X 1748.5+X	(14+) (13+) (14+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=0
1434.5+X 10	(12+)
2163.0+X 10	(14+)		385 728? 740			1778.2+X 1434.5+X 1422.8+X	(13+) (12+) (13+)
2961.0+X 10	(16+)		372? 767? 798			2590.3+X 2194.1+X 2163.0+X	(15+) (15+) (14+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - Collective oblate band, α=1
358.8+Y 5	(9)
732.6+Y 8	(11)		242.9 3	100		489.7+Y	(10)
1418.2+Y 9	(13)		371.6 3	100		1046.6+Y	(12)
2305.6+Y 10	(15)		464.4 3	100		1841.2+Y	(14)
3340.0+Y 11	(17)		532.1 5 1034.4 14	100 10 31 5		2807.9+Y 2305.6+Y	(16) (15)
4462.0+Y 13	(19)		572.5 5 1122.0 14	100 13 33 5		3889.5+Y 3340.0+Y	(18) (17)
5638.0+Y 14	(21)		583.2 5	100		5054.8+Y	(20)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - Collective oblate band, α=0
489.7+Y 7	(10)
1046.6+Y 9	(12)		314.0 3	100		732.6+Y	(11)
1841.2+Y 10	(14)		423.0 3	100		1418.2+Y	(13)
2807.9+Y 10	(16)		502.3 5 966.7 5	100 9 18 2		2305.6+Y 1841.2+Y	(15) (14)
3889.5+Y 12	(18)		549.5 5 1081.6 14	100 11 44 11		3340.0+Y 2807.9+Y	(17) (16)
5054.8+Y 13	(20)		592.8 5 1165.3 14	100 15 92 15		4462.0+Y 3889.5+Y	(19) (18)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 9 - SD band (1989Go13).
Z	J AP (16)
762.4+Z	J+2		762.4	0.35		Z	J AP (16)
1613.9+Z	J+4		851.5	0.80		762.4+Z	J+2
2534.4+Z	J+6		920.5	1.00		1613.9+Z	J+4
3532.1+Z	J+8		997.7	1.00		2534.4+Z	J+6
4604.7+Z	J+10		1072.6	1.00		3532.1+Z	J+8
5753.0+Z	J+12		1148.3	0.75		4604.7+Z	J+10
6982.4+Z	J+14		1229.4	0.65		5753.0+Z	J+12
8301.0+Z	J+16		1318.6	0.50		6982.4+Z	J+14
9713.4+Z	J+18		1412.4	0.40		8301.0+Z	J+16

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Conversion Coefficient	Additional Data
110.44	(1+,2,3+)	17 ns 5	110.4 2	[D,E2]	0.8	α=0.8 6
131.01	1+	77 ns 10	131.1 2	[E2]	0.77	α=0.77
219.73	(1+)		88.9 2	[M1,E2]	0.23	α=0.23 8
	(1+)		109.3 3	[D,E2]	0.8	α=0.8 6
	(1+)		219.8 2	[E2]	0.13	α=0.13
267.31	(1+)		47.5 3	[M1,E2]	21	α=21 11
	(1+)		136.4 2	[M1,E2]	0.56	α=0.56 11
	(1+)		267.3 2	[E2]	0.07	α=0.07
304.10	(1)		193.6 2	[D,E2]	0.12	α=0.12 8
304.10	(1)		304.1 2	[D,E2]	0.03	α=0.03 2
307.48	(1)		87.9 3	[D,E2]	1.8	α=1.8 14
	(1)		196.9 2	[D,E2]	0.11	α=0.11 7
	(1)		307.5 2	[D,E2]	0.03	α=0.03 2
340.61	(1+)		73.5 3	[M1,E2]	4.4	α=4.4 17
	(1+)		209.6 2	[M1,E2]	0.15	α=0.15
	(1+)		230.5 2	[D,E2]	0.07	α=0.07 5
	(1+)		340.6 2	[D,E2]	0.03	α=0.03 2
350.71	(1)		46.7 3	[D,E2]	18	α=18 16
	(1)		83.4 2	[D,E2]	2.2	α=2.2 18
	(1)		131.0 3	[D,E2]	0.44	α=0.44 33
	(1)		240.1 2	[D,E2]	0.06	α=0.06 4
384.78	(1)		77.6 2	[D,E2]	2.8	α=2.8 23
	(1)		80.5 3	[D,E2]	2.4	α=2.4 20
	(1)		253.7 2	[D,E2]	0.05	α=0.05 3
	(1)		274.2 2	[D,E2]	0.04	α=0.04 3
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Conversion Coefficient	Additional Data
430.18	(1)		163.0 3	[D,E2]	0.21	α=0.21 15
431.51	(1)		127.5 3	[D,E2]	0.5	α=0.5 4
431.51	(1)		300.5 2	[D,E2]	0.03	α=0.03 2
443.22	(1)		139.0 3	[D,E2]	0.36	α=0.36 27
443.22	(1)		175.8 3	[D,E2]	0.17	α=0.17 14
444.39	(1+)		59.6 2	[D,E2]	7.5	α=7.5 65
	(1+)		103.9 2	[M1,E2]	1.4	α=1.4 4
	(1+)		136.6 3	[D,E2]	0.38	α=0.38 28
	(1+)		176.9 2	[D,E2]	0.16	α=0.16 11
477.15	(1)		209.9 2	[D,E2]	0.09	α=0.09 6
477.96	(1+)		93.3 2	[D,E2]	1.4	α=1.4 11
477.96	(1+)		170.5 3	[D,E2]	0.18	α=0.18 13
481.89	(1)		141.3 2	[D,E2]	0.34	α=0.34 25
481.89	(1)		214.7 3	[D,E2]	0.09	α=0.09 5
523.88	(1+)		173.1 2	[D,E2]	0.17	α=0.17 12
	(1+)		183.2 2	[M1,E2]	0.22	α=0.22 2
	(1+)		256.5 2	[M1,E2]	0.08	α=0.08

E(level)	J^π(level)	T_1/2(level)	Comments
5.1+X			J^π(level): (4) for 5.1⁺x and 160.3⁺x; (5) for 113.9⁺x and 150.3⁺x, proposed (1989Go04,1989Go06) in (⁸²Se,3nγ) seem lower by 3 units of spin in view of feeding transition from higher levels whose Jπ’s have been revised by 2001Ko30 and 1996Li13.
88.4+X	(6-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
113.9+X			J^π(level): (4) for 5.1⁺x and 160.3⁺x; (5) for 113.9⁺x and 150.3⁺x, proposed (1989Go04,1989Go06) in (⁸²Se,3nγ) seem lower by 3 units of spin in view of feeding transition from higher levels whose Jπ’s have been revised by 2001Ko30 and 1996Li13.
150.3+X			J^π(level): (4) for 5.1⁺x and 160.3⁺x; (5) for 113.9⁺x and 150.3⁺x, proposed (1989Go04,1989Go06) in (⁸²Se,3nγ) seem lower by 3 units of spin in view of feeding transition from higher levels whose Jπ’s have been revised by 2001Ko30 and 1996Li13.
160.3+X			J^π(level): (4) for 5.1⁺x and 160.3⁺x; (5) for 113.9⁺x and 150.3⁺x, proposed (1989Go04,1989Go06) in (⁸²Se,3nγ) seem lower by 3 units of spin in view of feeding transition from higher levels whose Jπ’s have been revised by 2001Ko30 and 1996Li13.
160.4+X	(7-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
279.0+X	(8-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
385.4+X	(9+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
456.3+X	(9-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
522.9+X	(10+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
677.5+X	(10-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
802.2+X	(11+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
947.0+X	(11-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1048.5+X	(12+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1077.9+X	(11+)		E(level): DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1250.2+X	(12-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1422.8+X	(13+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1434.5+X	(12+)		E(level): DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1597.3+X	(13-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1748.5+X	(14+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1778.2+X	(13+)		E(level): DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
1970.1+X	(14-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
2163.0+X	(14+)		E(level): DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
2194.1+X	(15+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
2384.4+X	(15-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
E(level)	J^π(level)	T_1/2(level)	Comments
2586.7+X	(16+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
2590.3+X	(15+)		E(level): DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
2818.2+X	(16-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
2961.0+X	(16+)		E(level): DOUBLET (Chiral) PARTNER OF πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
3096.1+X	(17+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
3289.5+X	(17-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
3541.5+X	(18+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
3771.4+X	(18-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
4105.0+X	(19+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
4271.6+X	(19-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
4589.6+X	(20+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
4720.2+X	(20-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
5185.0+X	(21-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
5185.2+X	(21+)		E(level): πh_11/2νh_11/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
5644.5+X	(22-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
5696.8+X	(22+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
6156.8+X	(23-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
6658.1+X	(24-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
6818.8+X	(24+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
7203.2+X	(25-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
7759.0+X	(26-)		E(level): πh_11/2νg_7/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
7949.8+X	(26+)		E(level): πh_11/2νh_11/2, α=0. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
8282.7+X	(27-)		E(level): πh_11/2νg_7/2, α=1. J^π(level): Based on the assignments from 1987Pa27, 2001Ko30 and 1996Li13. The assignment of Jπ=(9⁺) to the bandhead of πh_11/2νh_11/2 configuration is based on detailed systematics analysis (1996Li13) of odd-odd nuclides in α=130 region. It should Be noted that Jπ assignments given by 1989Go04 and 1989Go06 are lower by 3 units of spin for πh_11/2νh_11/2 and πh_11/2νg_7/2 bands.
0.0+Y	(7)		E(level): Decays to 456⁺x, (9-) through unidentified transitions. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
86.9+Y	(9)		E(level): Decays to 802⁺x, (11⁺) through unidentified transitions. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
E(level)	J^π(level)	T_1/2(level)	Comments
358.8+Y	(9)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
489.7+Y	(10)		E(level): Collective oblate band, α=0. Decays to 677⁺x, (10-) also through unidentified transitions. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
732.6+Y	(11)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
1046.6+Y	(12)		E(level): Collective oblate band, α=0. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
1418.2+Y	(13)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
1841.2+Y	(14)		E(level): Collective oblate band, α=0. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
2305.6+Y	(15)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
2807.9+Y	(16)		E(level): Collective oblate band, α=0. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
3340.0+Y	(17)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
3889.5+Y	(18)		E(level): Collective oblate band, α=0. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
4462.0+Y	(19)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
5054.8+Y	(20)		E(level): Collective oblate band, α=0. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
5638.0+Y	(21)		E(level): Collective oblate band, α=1. J^π(level): From 1989Go06, but it is likely to Be higher by 3 units of spin, based on Jπ assignments of πh_11/2νg_7/2 and πh_11/2νh_11/2 bands from 2001Ko30, 1996Li13 and 1987Pa23.
Z	J AP (16)		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13). J^π(level): From 1989Go13.
762.4+Z	J+2		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
1613.9+Z	J+4		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
2534.4+Z	J+6		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
3532.1+Z	J+8		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
4604.7+Z	J+10		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
5753.0+Z	J+12		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
6982.4+Z	J+14		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
8301.0+Z	J+16		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).
9713.4+Z	J+18		E(level): The γ-ray peak is a part of an unresolved doublet. SD band (1989Go13).