List of levels for 167TM

Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 191, 1 (2023) | Cutoff date: 22-Aug-2023

hyperfine structure and isotope-shift measurements: 1986Al32, 1987Mi31, 1988Al04

Mass measurement: 1954Mi01

Theoretical structure calculations:

2021Al30: calculated rotational bandhead energies, Jπ, relative correction to energies in bands, energies and energy residuals for ground-state and higher bands using Effective field theory approach.

2020Zh17: calculated high-spin levels, Jπ, Nilsson configurations, kinematic moment of inertia versus angular frequency plots for the ground-state band, β and γ deformation parameters, proton and neutron pairing energies, total- and neutron and proton single particle Routhians, angular momentum alignments, and neutron occupation probabilities using cranked relativistic Hartree-Bogoliubov (CRHB) with Lipkin-Nogami method, the cranking covariant density functional theory (CDFT) with pairing correlations treated by a shell-model-like approach (SLAP), and the cranked shell model based on the Nilsson potential with pairing correlations from particle-number conserving (CSM-PNC) method.

2019Ta09: calculated g.s. magnetic moment, effective spin gyromagnetic factors, rotational decoupling parameter of K=1/2 states using quasiparticle phonon nuclear model (QPNM).

2017As01: calculated total Routhian surfaces (TRS), quasineutron energy levels, crossing frequency and interaction strength at the band crossing in 1/2[411] band using cranked shell model.

1994Ha22: calculated fractional changes in dynamical moments of inertia using cranking HFB theory.

1993Ha11: calculated levels, B(|l), Eγ, octupole softness using one-quasiparticle coupled to axially symmetric rotor.

1989Ja05: calculated levels, Jπ, band structures, B(|l) using quasiparticle-plus-rotor mixing.

1987Ad03: analyzed B(|l) data and B(E1) systematics.

1987Ba07: calculated ground state elctric quadrupole and magnetic dipole moments, charge radius, binding energy using Hartree-Fock theory.

1977Sc22, 1976An03: calculated and analyzed B(E1) and variations of the hexadecapole deformation parameter using Nilsson model.

1972So12: calculated levels, Jπ, K, B(E2).

1970Hj01: calculated deformation, decoupling, and rotational parameters, non-adiabatic coupling using Nilsson model.

Other theory references: 26 for structure and two for decay retrieved from the NSR database are listed in this dataset as ’document’ records.

Q-value: Q(ε)=746.1 13, S(2n)=15755.7 19, S(2p)=12223.0 14 (2021Wa16)

E(level): From a least-squares fit to γ-ray energies for levels connected with γ transitions, assuming ΔEγ=0.10 keV for Eγ, when not stated, with questionable γ rays omitted in the fitting. Seven γ rays out of a total of 344 γ rays fitted poorly, with reduced χ²=1.86, as compared to χ²=1.23 at 95% confidence level, with one γ ray deviating by 4-5 σ, six γ rays deviating by 3-4 σ, and 16 by 2-3 σ. Uncertainties for the following γ-ray energies were increased, resulting in reduced χ²=1.48, with 18 γ rays deviating by 2-3 σ: double the uncertainties for 228.67 7 from 699 level, 372.96 5 from 1160 level, 175.34 6 and 332.11 6 from 1276 level, 1332.5 2 from 1629 level; and triple the uncertainty for 639.89 4 from 1381 level. For levels not populated in γ-ray studies, values are from particle transfer reactions, with exceptions noted.

J^π(level): Ascending Jπ assumed from yrast pattern of levels populated in (α,2nγ) and (⁷Li,4nγ), and also from rotational band structures with cascades of coincident and interlocking stretched (ΔJ=2) quadrupole and stretched (ΔJ=1) dipole (or dipole+quadrupole) γ transitions determined based on measured γ(θ) in (α,2nγ) where available. Where no arguments are given specifically for levels from (α,2nγ) and/or (⁷Li,4nγ), assignments are from band assignments.

M(γ): From ce data in (p,nγ), unless otherwise noted. For Mult=(M1⁺E2) or (E1⁺M2) quoted from (α,2nγ), D+Q is from γ(θ) and electric/magnetic nature is from level scheme

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
10.417	3/2+	0.95 ns 5	10.419 25	M1+E2	0.043 +4-3	648	B(E2)(W.u.)=2.5E2 +5-4, B(M1)(W.u.)=0.0315 +26-23, α=648 38
116.594	5/2+	66 ps 7	106.18 2	M1+E2	0.116 +27-20	2.61	B(E2)(W.u.)=24 +7-6, B(M1)(W.u.)=0.070 +8-7, α=2.61 4
116.594	5/2+	66 ps 7	116.68 6	E2		1.721	B(E2)(W.u.)=231 +31-24, α=1.721 24
142.441	7/2+	343 ps 15	25.83 2	M1+E2	0.035	28.5	B(E2)(W.u.)=21 +11-9, B(M1)(W.u.)=0.024 6, α=28.5 4
142.441	7/2+	343 ps 15	132.05 4	E2		1.096	B(E2)(W.u.)=290 +23-20, α=1.096 15
171.76	(1/2)-		161.32 8	(E1)		0.0942	α=0.0942 13
171.76	(1/2)-		171.77 5	E1		0.0799	α=0.0799 11
179.501	7/2+	1.16 µs 6 % IT = 100	37.05 2	M1+E2	0.326 5	31.3	B(E2)(W.u.)=0.034 12, B(M1)(W.u.)=9.4E-7 32, α=31.3 8
	7/2+	1.16 µs 6 % IT = 100	62.91 1	M1+E2	0.065 5	11.78	B(E2)(W.u.)=0.00271 +48-43, B(M1)(W.u.)=5.39E-6 +36-33, α=11.78 17
	7/2+	1.16 µs 6 % IT = 100	169.04 3	E2		0.460	B(E2)(W.u.)=1.47E-4 +24-20, α=0.460 6
187.660	5/2-		177.26 2	E1		0.0735	α=0.0735 10
285.90	9/2-		98.25 2	E2		3.28	α=3.28 5
285.90	9/2-		143.46 1	E1		0.1284	α=0.1284 18
290.94	(3/2-)		174.26 7	(E1)		0.0769	α=0.0769 11
290.94	(3/2-)		290.92 8	(E1)		0.02073	α=0.02073 29
292.844	7/2-	0.9 µs 1	105.19 2	M1		2.68	B(M1)(W.u.)=1.40×10^-7 +24-20, α=2.68 4
	7/2-	0.9 µs 1	113.34 1	E1		0.2396	B(E1)(W.u.)=1.06E-7 +14-11, α=0.2396 34
	7/2-	0.9 µs 1	150.40 3	E1		0.1133	B(E1)(W.u.)=3.0E-11 +10-9, α=0.1133 16
	7/2-	0.9 µs 1	176.26 2	E1		0.0746	B(E1)(W.u.)=8.5E-9 +11-9, α=0.0746 10
296.21	9/2+		116.69 2	M1		1.993	α=1.993 28
326.50	9/2+		184.13 8	(M1+E2)	-0.12 +11-18	0.548	α=0.548 16
326.50	9/2+		209.93 3	E2		0.2214	α=0.2214 31
371.05	11/2+		85.16 6	(E1)		0.509	α=0.509 7
371.05	11/2+		228.61 1	(E2)		0.1675	α=0.1675 23
383.70	9/2-		90.86 3	M1		4.08	α=4.08 6
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
436.07	11/2+		139.83 2	M1+E2	+0.46 3	1.140	α=1.140 17
436.07	11/2+		256.57 1	E2		0.1158	α=0.1158 16
459.92	7/2-		169.20 10	[E2]		0.458	α=0.458 6
459.92	7/2-		174.0 2	(M1)		0.645	α=0.645 9
470.26	13/2-		99.21 1	E1		0.341	α=0.341 5
470.26	13/2-		184.42 9	E2		0.341	α=0.341 5
470.89	3/2+		460.48 14	(M1)		0.0468	α=0.0468 7
470.89	3/2+		470.62 9	(M1)		0.0442	α=0.0442 6
496.64	11/2-		112.89 4	M1+E2	+0.16 1	2.185	α=2.185 31
496.64	11/2-		203.76 5	E2		0.2443	α=0.2443 34
522.25	5/2+		379.69 20	M1		0.0774	α=0.0774 11
522.25	5/2+		405.57 8	(M1)		0.0651	α=0.0651 9
557.93	5/2+		415.50 20	(M1+E2)		0.045	α=0.045 17
	5/2+		441.2 1	(M1)		0.0523	α=0.0523 7
	5/2+		547.5 1	M1		0.0300	α=0.0300 4
597.48	13/2+		161.40 1	M1+E2	+0.40 +1-3	0.760	α=0.760 12
597.48	13/2+		301.26 1	E2		0.0705	α=0.0705 10
622.09	13/2+		251.07 8	M1+E2	-0.13 3	0.2326	α=0.2326 34
622.09	13/2+		295.59 1	E2		0.0747	α=0.0747 10
631.82	13/2-		135.20 2	M1+E2	+0.13 2	1.306	α=1.306 18
631.82	13/2-		248.12 1	E2		0.1288	α=0.1288 18
657.84	(7/2+)		331.21 22	(M1+E2)		0.082	α=0.082 29
657.84	(7/2+)		541.28 25	(M1)		0.0308	α=0.0308 4
689.19	15/2+		218.90 2	(E1)		0.0425	α=0.0425 6
689.19	15/2+		318.14 1	E2		0.0599	α=0.0599 8
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
699.17	(11/2-)		372.70 10	(E1)		0.01139	α=0.01139 16
699.17	(11/2-)		413.41 12	(M1+E2)		0.045	α=0.045 17
741.37	17/2-		271.12 2	E2		0.0975	α=0.0975 14
779.01	15/2+		181.50 2	M1+E2	+0.45 11	0.537	α=0.537 17
779.01	15/2+		342.95 1	(E2)		0.0480	α=0.0480 7
780.48	(9/2+)		222.50 19	[E2]		0.1829	α=0.1829 26
780.48	(9/2+)		453.97 4	(M1)		0.0485	α=0.0485 7
787.81	15/2-		156.04 3	M1+E2	+0.11 2	0.872	α=0.872 12
787.81	15/2-		291.150 10	(E2)		0.0783	α=0.0783 11
840.18	(11/2+)		469.25 6	(M1)		0.0445	α=0.0445 6
852.79	(3/2-)		665.13 3	(E2)		0.00856	α=0.00856 12
882.12	(5/2-)		694.46 17	(M1+E2)		0.012	α=0.012 4
927.87	(11/2+)		556.74 5	(M1)		0.0287	α=0.0287 4
929.74	(9/2-)		636.5 5	(M1)		0.02042	α=0.02042 29
935.24	(7/2-)		475.25 6	(M1)		0.0431	α=0.0431 6
935.24	(7/2-)		649.38 4	(M1)		0.01942	α=0.01942 27
944.89	(11/2+)		765.42 3	(E2)		0.00623	α=0.00623 9
965.77	17/2-		177.95 2	M1+E2	+0.12 1	0.602	α=0.602 8
965.77	17/2-		333.96 1	E2		0.0519	α=0.0519 7
978.55	17/2+		199.56 4	M1+E2	+0.46 +7-9	0.409	α=0.409 11
978.55	17/2+		380.81 21	E2		0.0356	α=0.0356 5
993.60	(17/2+)		304.41 1	(M1+E2)	-0.23 +16-17	0.136	α=0.136 7
993.60	(17/2+)		371.52 1	(E2)		0.0382	α=0.0382 5
1001.23	(13/2+)		630.14 3	(M1)		0.02095	α=0.02095 29
1007.62	(15/2-)		308.46 2	(E2)		0.0657	α=0.0657 9
	(15/2-)		385.50 2	(E1)		0.01052	α=0.01052 15
	(15/2-)		537.39 3	(M1)		0.0314	α=0.0314 4
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1008.50	(9/2-)		722.60 3	(E2)		0.00708	α=0.00708 10
1044.06	11/2-		547.42 3	(M1)		0.0300	α=0.0300 4
	11/2-		660.36 5	(M1)		0.01861	α=0.01861 26
	11/2-		751.21 10	(E2)		0.00649	α=0.00649 9, α(K)=0.00533 7, α(L)=0.000903 13, α(M)=0.0002038 29, α(N)=4.74×10^-5 7, α(O)=6.57E-6 9, α(P)=3.00E-7 4
1086.57	19/2+		345.20 2	(E1)		0.01367	α=0.01367 19
1086.57	19/2+		397.38 2	E2		0.0316	α=0.0316 4
1096.22	21/2-		354.85 1	E2		0.0435	α=0.0435 6
1160.96	19/2-		195.20 1	(M1+E2)	0.15 AP	0.464	α0.464 AP
1160.96	19/2-		372.96 5	E2		0.0377	α=0.0377 5
1194.82	19/2+		216.29 4	(M1+E2)	0.46 AP	0.326	α0.326 AP
1194.82	19/2+		415.79 2	E2		0.0279	α=0.0279 4
1216.56	7/2+		920.32 8	M1		0.00815	α=0.00815 11
1216.56	7/2+		1037.07 7	M1		0.00608	α=0.00608 9
1372.75	(17/2+)		371.52 1	(E2)		0.0382	α=0.0382 5
1378.19	21/2-		217.27 2	(M1+E2)	0.17 AP	0.344	α0.344 AP
1378.19	21/2-		412.39 2	E2		0.0285	α=0.0285 4
1380.98	(19/2-)		387.26 5	(E1)		0.01041	α=0.01041 15
1424.67	21/2+		229.85 4	(M1+E2)	0.30 AP	0.287	α0.287 AP
1424.67	21/2+		446.11 5	E2		0.02307	α=0.02307 32
1429.52	21/2(+)		435.94 2	(E2)		0.02454	α=0.02454 34
1528.69	25/2-		432.47 2	E2		0.02507	α=0.02507 35
1550.03	23/2(+)		463.44 3	(E2)		0.02086	α=0.02086 29
1808.66	(23/2-)		427.66 3	(E2)		0.0258	α=0.0258 4
1922.39	(25/2+)		497.71 4	(E2)		0.01733	α=0.01733 24
2030.77	29/2(-)		502.09 4	(E2)		0.01695	α=0.01695 24
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data

Q(β-)=-1953 keV 4	S(n)= 8728 keV 12	S(p)= 4907.9 keV 12
Reference: 2021WA16

References:
A	¹⁶⁷Yb ε decay (17.5 M)	B	¹⁶⁴Dy(⁷Li,4nγ)
C	¹⁶⁵Ho(α,2nγ)	D	¹⁶⁶Er(³He,d)
E	¹⁶⁶Er(α,t)	F	¹⁶⁷Er(p,nγ)
G	¹⁶⁹Tm(p,t)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F G	1/2+	9.25 d 2 % ε = 100
10.417 21	A B C D E F G	3/2+	0.95 ns 5	10.419 25	100	M1+E2	0.0	1/2+
116.594 24	A B C D E F G	5/2+	66 ps 7	106.18 2 116.68 6	100 5 12.55 27	M1+E2 E2	10.417 0.0	3/2+ 1/2+
142.441 25	A B C D E F G	7/2+	343 ps 15	25.83 2 132.05 4	1.7 5 100.0 30	M1+E2 E2	116.594 10.417	5/2+ 3/2+
171.76 4	A B C F	(1/2)-		161.32 8 171.77 5	94 28 100 9	(E1) E1	10.417 0.0	3/2+ 1/2+
179.501 24	A B C D E F	7/2+	1.16 µs 6 % IT = 100	37.05 2 62.91 1 169.04 3	3.9 14 100 11 3.21 29	M1+E2 M1+E2 E2	142.441 116.594 10.417	7/2+ 5/2+ 3/2+
187.660 24	A B C D E F	5/2-		177.26 2	100	E1	10.417	3/2+
282.24 5	A	(3/2)		94.53 5 110.49 5 272.1 2 282.4 2	32 10 100 20		187.660 171.76 10.417 0.0	5/2- (1/2)- 3/2+ 1/2+
285.90 3	A B C D E F	9/2-		98.25 2 143.46 1	3.4 3 100.0 29	E2 E1	187.660 142.441	5/2- 7/2+
290.94 4	A B C D E F	(3/2-)		103.32 5 174.26 7 280.55 20 290.92 8	30 13 22 9 10.6 25 100 11	(E1) (E1)	187.660 116.594 10.417 0.0	5/2- 5/2+ 3/2+ 1/2+
292.844 24	A B C D E F	7/2-	0.9 µs 1	6.93S 105.19 2 113.34 1 150.40 3 176.26 2	1.07 11 100 4 0.067 19 30.2 11	M1 E1 E1 E1	285.90 187.660 179.501 142.441 116.594	9/2- 5/2- 7/2+ 7/2+ 5/2+
296.21 3	A B C F	9/2+		116.69 2 179.55 5	96 14 100 41	M1	179.501 116.594	7/2+ 5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
326.50 3	A B C D E F G	9/2+		184.13 8 209.93 3	100 5 44.8 12	(M1+E2) E2	142.441 116.594	7/2+ 5/2+
371.05 3	B C F G	11/2+		44.4? 85.16 6 228.61 1	12.6 12 100 15	(E1) (E2)	326.50 285.90 142.441	9/2+ 9/2- 7/2+
383.70 4	A B C F	9/2-		90.86 3	100	M1	292.844	7/2-
436.07 3	B C F	11/2+		139.83 2 256.57 1	100 5 77.5 15	M1+E2 E2	296.21 179.501	9/2+ 7/2+
459.92 4	B C D E F	7/2-		169.20 10 ? 174.0 2 ? 272.30 10 343.37	72 12 100 40	[E2] (M1)	290.94 285.90 187.660 116.594	(3/2-) 9/2- 5/2- 5/2+
470.26 3	B C F	13/2-		99.21 1 184.42 9	40.3 35 100.0 30	E1 E2	371.05 285.90	11/2+ 9/2-
470.89 5	A C D E F G	3/2+		354.57 460.48 14 470.62 9	100 13 85 11	(M1) (M1)	116.594 10.417 0.0	5/2+ 3/2+ 1/2+
496.64 4	A B C D E F	11/2-		112.89 4 203.76 5	100 7 11.3 8	M1+E2 E2	383.70 292.844	9/2- 7/2-
522.25 5	A C D E F	5/2+		379.69 20 405.57 8 511.70 20	30 10 100 14	M1 (M1)	142.441 116.594 10.417	7/2+ 5/2+ 3/2+
557.93 5	A C D E F	5/2+		35.69 3 415.50 20 441.2 1 547.5 1	33 8 90 18 100 17	(M1+E2) (M1) M1	522.25 142.441 116.594 10.417	5/2+ 7/2+ 5/2+ 3/2+
597.48 3	B C F	13/2+		161.40 1 301.26 1	62.2 25 100.0 18	M1+E2 E2	436.07 296.21	11/2+ 9/2+
601.99 4	C D E G	(7/2+)		79.56 9 131.06 4 275.57 459.63 19 485.39 12	17 4 <252 <65 100 18		522.25 470.89 326.50 142.441 116.594	5/2+ 3/2+ 9/2+ 7/2+ 5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
622.09 3	B C F G	13/2+		251.07 8 295.59 1	61 6 100.0 17	M1+E2 E2	371.05 326.50	11/2+ 9/2+
631.82 4	B C F	13/2-		135.20 2 248.12 1	100 6 33 8	M1+E2 E2	496.64 383.70	11/2- 9/2-
657.84 5 ?	C F G	(7/2+)		331.21 22 515.42 4 541.28 25		(M1+E2) (M1)	326.50 142.441 116.594	9/2+ 7/2+ 5/2+
682	G
689.19 3	B C F	15/2+		67.02 5 218.90 2 318.14 1	6.1 31 25.0 6 100 4	(E1) E2	622.09 470.26 371.05	13/2+ 13/2- 11/2+
699.17 4	B C D E F G	(11/2-)		228.67 7 239.26 2 372.70 10 413.41 12	<1350 86 5 100 11	(E1) (M1+E2)	470.26 459.92 326.50 285.90	13/2- 7/2- 9/2+ 9/2-
709.12 4	C G	(9/2+)		107.13 4 186.68 11 338.01 22 382.41 30 566.83 11	100 50 70 25 35 10 30 15 30 5		601.99 522.25 371.05 326.50 142.441	(7/2+) 5/2+ 11/2+ 9/2+ 7/2+
717 2	D E
741.37 3	B C F	17/2-		271.12 2	100	E2	470.26	13/2-
771 2	D E
779.01 3	B C F	15/2+		181.50 2 342.95 1	34.2 14 100 6	M1+E2 (E2)	597.48 436.07	13/2+ 11/2+
780.48 5 ?	C	(9/2+)		222.50 19 ? 453.97 4	<17 100 5	[E2] (M1)	557.93 326.50	5/2+ 9/2+
787.81 4	B C F	15/2-		156.04 3 291.150 10	100 4 47 3	M1+E2 (E2)	631.82 496.64	13/2- 11/2-
840.18 4	C F	(11/2+)		131.06 4 218.07 17 238.13 4 469.25 6 513.66 5	<242 <96 50 4 100 25 75 8	(M1)	709.12 622.09 601.99 371.05 326.50	(9/2+) 13/2+ (7/2+) 11/2+ 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
852.79 4	C F	(3/2-)		665.13 3 680.86 16	<276 100 25	(E2)	187.660 171.76	5/2- (1/2)-
867.77 14 ?	A	(5/2+,7/2,9/2-)		571.3 2 680.3 5 688.5 2	56 12 37 12 100 28		296.21 187.660 179.501	9/2+ 5/2- 7/2+
882.12 18	C F	(5/2-)		694.46 17	100	(M1+E2)	187.660	5/2-
927.87 4	C F	(11/2+)		270.14 305.91 27 556.74 5 601.48 5	24 6 <189 100 12	(M1)	657.84 622.09 371.05 326.50	(7/2+) 13/2+ 11/2+ 9/2+
929.74 7 ?	C F	(9/2-)		636.5 5	100	(M1)	292.844	7/2-
935.24 4	C F	(7/2-)		475.25 6 649.38 4 747.50 9	<209 100 32 18 5	(M1) (M1)	459.92 285.90 187.660	7/2- 9/2- 5/2-
944.89 4	C F	(11/2+)		508.81 14 648.43 11 765.42 3	48 9 48 9 100 9	(E2)	436.07 296.21 179.501	11/2+ 9/2+ 7/2+
965.77 4	B C F	17/2-		177.95 2 333.96 1	100.0 34 67 7	M1+E2 E2	787.81 631.82	15/2- 13/2-
978.55 4	B C F	17/2+		199.56 4 356.40 14 380.81 21	24.3 13 5.1 9 100.0 21	M1+E2 E2	779.01 622.09 597.48	15/2+ 13/2+ 13/2+
993.60 3	B C F G	(17/2+)		304.41 1 371.52 1	100 6 113.7 33	(M1+E2) (E2)	689.19 622.09	15/2+ 13/2+
1001.23 3	C F	(13/2+)		161.45 6 ? 292.07 312.11 11 379.15 2 630.14 3	26.7 33 <173 100 7	(M1)	840.18 709.12 689.19 622.09 371.05	(11/2+) (9/2+) 15/2+ 13/2+ 11/2+
1007.62 3	B C F	(15/2-)		266.40 11 308.46 2 385.50 2 537.39 3	18.5 19 56 4 100 6 72 6	(E2) (E1) (M1)	741.37 699.17 622.09 470.26	17/2- (11/2-) 13/2+ 13/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1008.50 4	C F G	(9/2-)		722.60 3	100	(E2)	285.90	9/2-
1044.06 5	C D E F	11/2-		114.32 5 547.42 3 660.36 5 751.21 10	100 42 <97 65 7 <84	(M1) (M1) (E2)	929.74 496.64 383.70 292.844	(9/2-) 11/2- 9/2- 7/2-
1086.57 3	B C F	19/2+		345.20 2 397.38 2	74.2 25 100.0 19	(E1) E2	741.37 689.19	17/2- 15/2+
1092	G
1096.22 3	B C F	21/2-		354.85 1	100	E2	741.37	17/2-
1096.47 4	C	(13/2+)		168.66 4 315.79 17 407.27? 474.38 725.34 4	100 8 17 4 75 13		927.87 780.48 689.19 622.09 371.05	(11/2+) (9/2+) 15/2+ 13/2+ 11/2+
1101.24 4	C	(13/2+)		156.33 503.84 13 665.13 3 805.07 4	28 8 <88 100 8		944.89 597.48 436.07 296.21	(11/2+) 13/2+ 11/2+ 9/2+
1105.33 4	C G	(11/2-)		635.07 3 819.41			470.26 285.90	13/2- 9/2-
1125 2	D E	1/2+
1154	G
1160.96 4	B C F	19/2-		195.20 1 372.96 5	67.5 21 100.0 25	(M1+E2) E2	965.77 787.81	17/2- 15/2-
1163.96 5	C	(15/2+)		162.82 9 323.34 19 474.77 541.87 7	100 5 29 5 57 14		1001.23 840.18 689.19 622.09	(13/2+) (11/2+) 15/2+ 13/2+
1168 2	D
1192	G
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1194.82 3	B C F	19/2+		216.29 4 415.79 2	66.5 31 100.0 20	(M1+E2) E2	978.55 779.01	17/2+ 15/2+
1216.56 6	A G	7/2+		832.9 3 920.32 8 923.7 4 1037.07 7	1.70 19.0 29 1.0 4 100 12	M1 M1	383.70 296.21 292.844 179.501	9/2- 9/2+ 7/2- 7/2+
1223.11 4	C	(13/2-)		523.93 752.85 3			699.17 470.26	(11/2-) 13/2-
1229.85 10	A	(7/2-)		672.1 2 707.7 4 733.2 3 ? 846.1 2 903.3 2 933.8 3 936.7 3 1050.3 2	21 5 8 5 18 5 34 6 17 5 14 5 18 6 100 24		557.93 522.25 496.64 383.70 326.50 296.21 292.844 179.501	5/2+ 5/2+ 11/2- 9/2- 9/2+ 9/2+ 7/2- 7/2+
1235 2	D
1276.78 4	C	(15/2+)		175.34 6 332.11 6 497.71 4 679.43 7 840.70 6	100 7 54 7 <161 71 7 68 7		1101.24 944.89 779.01 597.48 436.07	(13/2+) (11/2+) 15/2+ 13/2+ 11/2+
1281.46 6	C	(15/2+)		185.11 17 ? 287.70 11 353.42 15 592.27 659.18 24	127 46 27 8 100 35 19 4		1096.47 993.60 927.87 689.19 622.09	(13/2+) (17/2+) (11/2+) 15/2+ 13/2+
1283	G
1320	G
1358.75 4	C	(15/2-)		253.43 4 617.33 4 888.37 12	<58 100 10 38 5		1105.33 741.37 470.26	(11/2-) 17/2- 13/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1372.75 3	C	(17/2+)		208.86 7 286.25 17 371.52 1 379.15 2 683.54 4	<21 7.7 23 100 12 <40.0 16.2 16	(E2)	1163.96 1086.57 1001.23 993.60 689.19	(15/2+) 19/2+ (13/2+) (17/2+) 15/2+
1374 2	D G
1378.19 4	B C	21/2-		217.27 2 412.39 2	29.8 15 100.0 23	(M1+E2) E2	1160.96 965.77	19/2- 17/2-
1380.98 4	B C	(19/2-)		284.73 16 373.42 12 387.26 5 639.89 4	12.9 32 71 23 51.6 32 100 5	(E1)	1096.22 1007.62 993.60 741.37	21/2- (15/2-) (17/2+) 17/2-
1403 2	D E G	1/2+
1424.67 4	B C	21/2+		229.85 4 431.11 4 446.11 5	10.8 6 <21 100.0 30	(M1+E2) E2	1194.82 993.60 978.55	19/2+ (17/2+) 17/2+
1429.52 3	B C	21/2(+)		334 1 342.95 1 435.94 2 450.81 21	61 4 100.0 31 3.1 8	(E2)	1096.22 1086.57 993.60 978.55	21/2- 19/2+ (17/2+) 17/2+
1432.33 10 ?	A G	(5/2-,7/2)		1048.5 3 1139.5 1	31 16 100 14		383.70 292.844	9/2- 7/2-
1457	G
1470.16 5	C	(17/2+)		193.45 7 368.99 12 491.70 691.20 872.62 8	100 5 75 10 80 10		1276.78 1101.24 978.55 779.01 597.48	(15/2+) (13/2+) 17/2+ 15/2+ 13/2+
1486	G
1487.36 8	C	(17/2+)		206.18 10 ? 390.61 12 400.56 15 798.46 10	144 22 100 22 67 22 78 11		1281.46 1096.47 1086.57 689.19	(15/2+) (13/2+) 19/2+ 15/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1524.93 4	C	(17/2-)		301.84 517.34 783.57 3			1223.11 1007.62 741.37	(13/2-) (15/2-) 17/2-
1527.45 7	A D E G	(5/2-)		1234.63 7 1340.1 4 1384.8 2 1410.7 4 1517.0 2	100 12 2.6 9 5.3 12 2.0 7 5.5 10		292.844 187.660 142.441 116.594 10.417	7/2- 5/2- 7/2+ 5/2+ 3/2+
1528.69 4	B C	25/2-		432.47 2	100	E2	1096.22	21/2-
1543.80 16	A	(5/2+,7/2+)		1217.1 2 1427.8 3 1533.1 4	100 30 46 15 24 9		326.50 116.594 10.417	9/2+ 5/2+ 3/2+
1549 2	D E
1550.03 4	B C	23/2(+)		453.77 463.44 3	62.56 31 100.0 31	(E2)	1096.22 1086.57	21/2- 19/2+
1562.93 4	C	(19/2+)		190.14 9 398.65 13 476.35 9 569.35 6	41 9 55 14 100 18 <82		1372.75 1163.96 1086.57 993.60	(17/2+) (15/2+) 19/2+ (17/2+)
1580.97 6	A D E G	(5/2+,7/2+)		1022.9 2 1110.3 1 1254.5 4 1288.1 1 1298.2 6 1393.1 2 1401.9 3 1438.3 1 1464.8 2 1570.4 2	32 6 31 6 7.7 30 100 14 6.6 30 18 4 8.3 30 64 10 17 4 83 13		557.93 470.89 326.50 292.844 282.24 187.660 179.501 142.441 116.594 10.417	5/2+ 3/2+ 9/2+ 7/2- (3/2) 5/2- 7/2+ 7/2+ 5/2+ 3/2+
1597.58 7	A D E G	(5/2-,7/2+)		1213.3 2 1304.9 1 1455.1 1 1481.1 3 1587.1 2	19 6 100 15 69 10 7.5 31 85 11		383.70 292.844 142.441 116.594 10.417	9/2- 7/2- 7/2+ 5/2+ 3/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1606.80 4	B C	(23/2-)		228.61 1 445.82 4	100 5 28.7 14		1378.19 1160.96	21/2- 19/2-
1629.65 13	A D E G	(5/2+,7/2+)		1332.5 2 1337.2 5 1487.4 2 1511.9 2 ? 1619.2 2	48 13 25 13 77 18 100 14		296.21 292.844 142.441 116.594 10.417	9/2+ 7/2- 7/2+ 5/2+ 3/2+
1644 2	D
1654.33 9	A G	(5/2+,7/2+)		1358.3 4 1361.5 1 1511.9 2 1537.5 4 1643.8 2	6.0 100 19 71 11 17 8 80 10		296.21 292.844 142.441 116.594 10.417	9/2+ 7/2- 7/2+ 5/2+ 3/2+
1668.93 4	B C	(23/2+)		244.27 3 474.09 3	86 5 100.0 25		1424.67 1194.82	21/2+ 19/2+
1672 2	D
1678.90 5	C	(19/2+)		208.86 7 402.07 5 484.08 11 700.36 7	124 35 71 12 59 18 100 12		1470.16 1276.78 1194.82 978.55	(17/2+) (15/2+) 19/2+ 17/2+
1691.24 4	C	(19/2-)		332.36 6 595.05 3 950.11 21	61 6 100 6 44.4 28		1358.75 1096.22 741.37	(15/2-) 21/2- 17/2-
1701 2	D
1705.57 6	C	(19/2+)		218.07 17 ? 276.22 11 424.05 5 619.04 7 1016.62 29	<180 <82 82 9 100 18 55 9		1487.36 1429.52 1281.46 1086.57 689.19	(17/2+) 21/2(+) (15/2+) 19/2+ 15/2+
1718 2	D
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1808.66 4	B C	(23/2-)		279.96 379.15 2 427.66 3 712.41 3	<114 65.2 22 100 4	(E2)	1528.69 1429.52 1380.98 1096.22	25/2- 21/2(+) (19/2-) 21/2-
1813.96 4	C	(21/2+)		251.03 1 384.44? 441.22 3 727.63 11	<3220 <415 100 29	(D)	1562.93 1429.52 1372.75 1086.57	(19/2+) 21/2(+) (17/2+) 19/2+
1858.66 5	B C	(25/2-)		251.84 2 480.50 17	20.6 18 100 6		1606.80 1378.19	(23/2-) 21/2-
1901.27 6	C	(21/2+)		222.50 19 431.11 4 706.35 15	<88 <263 100 25		1678.90 1470.16 1194.82	(19/2+) (17/2+) 19/2+
1915.39 5	B C	(25/2+)		365.35 3 386.67 485.98 13 491.02 26	25.6 20 100 8 35 5		1550.03 1528.69 1429.52 1424.67	23/2(+) 25/2- 21/2(+) 21/2+
1916.61 6	C	(21/2-)		391.72 5 535.61 820.44			1524.93 1380.98 1096.22	(17/2-) (19/2-) 21/2-
1922.39 4	B C	(25/2+)		253.43 4 492.89 6 497.71 4	11.1 12 ≈36 100 4	(D) (E2)	1668.93 1429.52 1424.67	(23/2+) 21/2(+) 21/2+
2022.25 9	C	(23/2+)		459.63 19 472.17 8	<88 100 24		1562.93 1550.03	(19/2+) 23/2(+)
2030.77 5	B C	29/2(-)		502.09 4	100	(E2)	1528.69	25/2-
2065.45 5	B C	(27/2+)		515.42 4 536.72	56.6 24 100.0 34		1550.03 1528.69	23/2(+) 25/2-
2098.06 5	C	(23/2-)		406.84 4 569.35 6 1001.70 23	100 8 <45 15.0 25		1691.24 1528.69 1096.22	(19/2-) 25/2- 21/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2113.89 6	B C	(27/2-)		255.12 6 507.14 4	100 10 113 6		1858.66 1606.80	(25/2-) (23/2-)
2135.94 7	C	(23/2+)		234.68 7 457.05 6 711.34?	24 6 100 12		1901.27 1678.90 1424.67	(21/2+) (19/2+) 21/2+
2186.45 5	B C	(27/2+)		264.02 8 517.53 3	20.2 24 100.0 33		1922.39 1668.93	(25/2+) (23/2+)
2279.75 7	B C	(27/2-)		471.01 7 751.21 10	100 24 <124		1808.66 1528.69	(23/2-) 25/2-
2321.08 6 ?	C	(25/2+)		405.69 4 507.14 4 ?	47 13 100 6		1915.39 1813.96	(25/2+) (21/2+)
2381.92 13 ?	C	(25/2+)		246.10 16 480.50 17	100 33 <1430		2135.94 1901.27	(23/2+) (21/2+)
2394.45 6	B C	(29/2-)		280.56 535.79 3	23.7 23 100 6		2113.89 1858.66	(27/2-) (25/2-)
2396.42 7	C	(25/2-)		479.88 6 587.45 15 867.36 26	100 12 10.0 20 8.0 20		1916.61 1808.66 1528.69	(21/2-) (23/2-) 25/2-
2440.46 7	B C	(29/2+)		375.02 518.17? 525.07 5	100 8		2065.45 1922.39 1915.39	(27/2+) (25/2+) (25/2+)
2455.62 9	B C	(29/2+)		269.17 11 533.18 12	8.2 8 100 5		2186.45 1922.39	(27/2+) (25/2+)
2573.30 7	C	(27/2-)		475.25 6 542.51 15 1044.60	<380 100 25		2098.06 2030.77 1528.69	(23/2-) 29/2(-) 25/2-
2593.46 12	B C	(33/2-)		562.68 10	100		2030.77	29/2(-)
2620.14 8	B C	(31/2+)		554.66 7 589.47 12	63.7 27 100 5		2065.45 2030.77	(27/2+) 29/2(-)
2670.64 7	B C	(31/2-)		276.22 11 556.74 5	100 16 88 5		2394.45 2113.89	(29/2-) (27/2-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2735.83 9	B C	(31/2+)		280.21 2 549.50 19	32 4 100 4		2455.62 2186.45	(29/2+) (27/2+)
2799.06 11	B C	(31/2-)		519.31 768.28 22	100 20		2279.75 2030.77	(27/2-) 29/2(-)
2972.4 10	B	(33/2-)		578 1	100		2394.45	(29/2-)
2993.5 10	B	(33/2+)		553 1	100		2440.46	(29/2+)
3013.5 7	B	(33/2+)		277 1 559 1	8.2 14 100 7		2735.83 2455.62	(31/2+) (29/2+)
3208.8 8	B	(35/2+)		589 1 615 1	100 5		2620.14 2593.46	(31/2+) (33/2-)
3210.5 10	B	(37/2-)		617 1	100		2593.46	(33/2-)
3261.6 10	B	(35/2-)		591 1	100		2670.64	(31/2-)
3311.2 8	B	(35/2+)		298 1 575 1	18.1 36 100 6		3013.5 2735.83	(33/2+) (31/2+)
3575.5 15	B	(37/2+)		582 1	100		2993.5	(33/2+)
3579.4 15	B	(37/2-)		607 1	100		2972.4	(33/2-)
3600.5 12	B	(37/2+)		587 1	100		3013.5	(33/2+)
3832.8 13	B	(39/2+)		624 1	100		3208.8	(35/2+)
3877.5 15	B	(41/2-)		667 1	100		3210.5	(37/2-)
3878.6 15	B	(39/2-)		617 1	100		3261.6	(35/2-)
3916.2 13	B	(39/2+)		605 1	100		3311.2	(35/2+)
4196.5 18	B	(41/2+)		621 1	100		3575.5	(37/2+)
4196.5 16 ?	B	(41/2+)		596 1 ?			3600.5	(37/2+)
4494.8 16	B	(43/2+)		662 1	100		3832.8	(39/2+)
4565.2 17	B	(43/2+)		649 1	100		3916.2	(39/2+)
4596.5 18	B	(45/2-)		719 1	100		3877.5	(41/2-)
4868.5 20 ?	B	(45/2+)		672 1 ?			4196.5	(41/2+)
5204.8 19	B	(47/2+)		710 1	100		4494.8	(43/2+)
5365.5 20	B	(49/2-)		769 1	100		4596.5	(45/2-)
5970.8 22	B	(51/2+)		766 1	100		5204.8	(47/2+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6185.5 23	B	(53/2-)		820 1	100		5365.5	(49/2-)
7055.5 25	B	(57/2-)		870 1	100		6185.5	(53/2-)
7979.5 27	B	(61/2-)		924 1	100		7055.5	(57/2-)
8952.5 29	B	(65/2-)		973			7979.5	(61/2-)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - π1/2[411],α=+1/2.
0.0	1/2+	9.25 d 2 % ε = 100
116.594 24	5/2+	66 ps 7	106.18 2 116.68 6	100 5 12.55 27	M1+E2 E2	10.417 0.0	3/2+ 1/2+
326.50 3	9/2+		184.13 8 209.93 3	100 5 44.8 12	(M1+E2) E2	142.441 116.594	7/2+ 5/2+
622.09 3	13/2+		251.07 8 295.59 1	61 6 100.0 17	M1+E2 E2	371.05 326.50	11/2+ 9/2+
993.60 3	(17/2+)		304.41 1 371.52 1	100 6 113.7 33	(M1+E2) (E2)	689.19 622.09	15/2+ 13/2+
1429.52 3	21/2(+)		334 1 342.95 1 435.94 2 450.81 21	61 4 100.0 31 3.1 8	(E2)	1096.22 1086.57 993.60 978.55	21/2- 19/2+ (17/2+) 17/2+
1915.39 5	(25/2+)		365.35 3 386.67 485.98 13 491.02 26	25.6 20 100 8 35 5		1550.03 1528.69 1429.52 1424.67	23/2(+) 25/2- 21/2(+) 21/2+
2440.46 7	(29/2+)		375.02 518.17? 525.07 5	100 8		2065.45 1922.39 1915.39	(27/2+) (25/2+) (25/2+)
2993.5 10	(33/2+)		553 1	100		2440.46	(29/2+)
3575.5 15	(37/2+)		582 1	100		2993.5	(33/2+)
4196.5 18	(41/2+)		621 1	100		3575.5	(37/2+)
4868.5 20	(45/2+)		672 1 ?			4196.5	(41/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - π1/2[411],α=-1/2.
10.417 21	3/2+	0.95 ns 5
142.441 25	7/2+	343 ps 15	25.83 2 132.05 4	1.7 5 100.0 30	M1+E2 E2	116.594 10.417	5/2+ 3/2+
371.05 3	11/2+		44.4? 85.16 6 228.61 1	12.6 12 100 15	(E1) (E2)	326.50 285.90 142.441	9/2+ 9/2- 7/2+
689.19 3	15/2+		67.02 5 218.90 2 318.14 1	6.1 31 25.0 6 100 4	(E1) E2	622.09 470.26 371.05	13/2+ 13/2- 11/2+
1086.57 3	19/2+		345.20 2 397.38 2	74.2 25 100.0 19	(E1) E2	741.37 689.19	17/2- 15/2+
1550.03 4	23/2(+)		453.77 463.44 3	62.56 31 100.0 31	(E2)	1096.22 1086.57	21/2- 19/2+
2065.45 5	(27/2+)		515.42 4 536.72	56.6 24 100.0 34		1550.03 1528.69	23/2(+) 25/2-
2620.14 8	(31/2+)		554.66 7 589.47 12	63.7 27 100 5		2065.45 2030.77	(27/2+) 29/2(-)
3208.8 8	(35/2+)		589 1 615 1	100 5		2620.14 2593.46	(31/2+) (33/2-)
3832.8 13	(39/2+)		624 1	100		3208.8	(35/2+)
4494.8 16	(43/2+)		662 1	100		3832.8	(39/2+)
5204.8 19	(47/2+)		710 1	100		4494.8	(43/2+)
5970.8 22	(51/2+)		766 1	100		5204.8	(47/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - π1/2[541],α=+1/2.
171.76 4	(1/2)-
187.660 24	5/2-		177.26 2	100	E1	10.417	3/2+
285.90 3	9/2-		98.25 2 143.46 1	3.4 3 100.0 29	E2 E1	187.660 142.441	5/2- 7/2+
470.26 3	13/2-		99.21 1 184.42 9	40.3 35 100.0 30	E1 E2	371.05 285.90	11/2+ 9/2-
741.37 3	17/2-		271.12 2	100	E2	470.26	13/2-
1096.22 3	21/2-		354.85 1	100	E2	741.37	17/2-
1528.69 4	25/2-		432.47 2	100	E2	1096.22	21/2-
2030.77 5	29/2(-)		502.09 4	100	(E2)	1528.69	25/2-
2593.46 12	(33/2-)		562.68 10	100		2030.77	29/2(-)
3210.5 10	(37/2-)		617 1	100		2593.46	(33/2-)
3877.5 15	(41/2-)		667 1	100		3210.5	(37/2-)
4596.5 18	(45/2-)		719 1	100		3877.5	(41/2-)
5365.5 20	(49/2-)		769 1	100		4596.5	(45/2-)
6185.5 23	(53/2-)		820 1	100		5365.5	(49/2-)
7055.5 25	(57/2-)		870 1	100		6185.5	(53/2-)
7979.5 27	(61/2-)		924 1	100		7055.5	(57/2-)
8952.5 29	(65/2-)		973			7979.5	(61/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - π1/2[541],α=-1/2.
290.94 4	(3/2-)
459.92 4	7/2-		169.20 10 ? 174.0 2 ? 272.30 10 343.37	72 12 100 40	[E2] (M1)	290.94 285.90 187.660 116.594	(3/2-) 9/2- 5/2- 5/2+
699.17 4	(11/2-)		228.67 7 239.26 2 372.70 10 413.41 12	<1350 86 5 100 11	(E1) (M1+E2)	470.26 459.92 326.50 285.90	13/2- 7/2- 9/2+ 9/2-
1007.62 3	(15/2-)		266.40 11 308.46 2 385.50 2 537.39 3	18.5 19 56 4 100 6 72 6	(E2) (E1) (M1)	741.37 699.17 622.09 470.26	17/2- (11/2-) 13/2+ 13/2-
1380.98 4	(19/2-)		284.73 16 373.42 12 387.26 5 639.89 4	12.9 32 71 23 51.6 32 100 5	(E1)	1096.22 1007.62 993.60 741.37	21/2- (15/2-) (17/2+) 17/2-
1808.66 4	(23/2-)		279.96 379.15 2 427.66 3 712.41 3	<114 65.2 22 100 4	(E2)	1528.69 1429.52 1380.98 1096.22	25/2- 21/2(+) (19/2-) 21/2-
2279.75 7	(27/2-)		471.01 7 751.21 10	100 24 <124		1808.66 1528.69	(23/2-) 25/2-
2799.06 11	(31/2-)		519.31 768.28 22	100 20		2279.75 2030.77	(27/2-) 29/2(-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - π7/2[404],α=+1/2.
296.21 3	9/2+
597.48 3	13/2+		161.40 1 301.26 1	62.2 25 100.0 18	M1+E2 E2	436.07 296.21	11/2+ 9/2+
978.55 4	17/2+		199.56 4 356.40 14 380.81 21	24.3 13 5.1 9 100.0 21	M1+E2 E2	779.01 622.09 597.48	15/2+ 13/2+ 13/2+
1424.67 4	21/2+		229.85 4 431.11 4 446.11 5	10.8 6 <21 100.0 30	(M1+E2) E2	1194.82 993.60 978.55	19/2+ (17/2+) 17/2+
1922.39 4	(25/2+)		253.43 4 492.89 6 497.71 4	11.1 12 ≈36 100 4	(D) (E2)	1668.93 1429.52 1424.67	(23/2+) 21/2(+) 21/2+
2455.62 9	(29/2+)		269.17 11 533.18 12	8.2 8 100 5		2186.45 1922.39	(27/2+) (25/2+)
3013.5 7	(33/2+)		277 1 559 1	8.2 14 100 7		2735.83 2455.62	(31/2+) (29/2+)
3600.5 12	(37/2+)		587 1	100		3013.5	(33/2+)
4196.5 16	(41/2+)		596 1 ?			3600.5	(37/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - π7/2[404],α=-1/2.
179.501 24	7/2+	1.16 µs 6 % IT = 100
436.07 3	11/2+		139.83 2 256.57 1	100 5 77.5 15	M1+E2 E2	296.21 179.501	9/2+ 7/2+
779.01 3	15/2+		181.50 2 342.95 1	34.2 14 100 6	M1+E2 (E2)	597.48 436.07	13/2+ 11/2+
1194.82 3	19/2+		216.29 4 415.79 2	66.5 31 100.0 20	(M1+E2) E2	978.55 779.01	17/2+ 15/2+
1668.93 4	(23/2+)		244.27 3 474.09 3	86 5 100.0 25		1424.67 1194.82	21/2+ 19/2+
2186.45 5	(27/2+)		264.02 8 517.53 3	20.2 24 100.0 33		1922.39 1668.93	(25/2+) (23/2+)
2735.83 9	(31/2+)		280.21 2 549.50 19	32 4 100 4		2455.62 2186.45	(29/2+) (27/2+)
3311.2 8	(35/2+)		298 1 575 1	18.1 36 100 6		3013.5 2735.83	(33/2+) (31/2+)
3916.2 13	(39/2+)		605 1	100		3311.2	(35/2+)
4565.2 17	(43/2+)		649 1	100		3916.2	(39/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - π7/2[523],α=+1/2.
383.70 4	9/2-
631.82 4	13/2-		135.20 2 248.12 1	100 6 33 8	M1+E2 E2	496.64 383.70	11/2- 9/2-
965.77 4	17/2-		177.95 2 333.96 1	100.0 34 67 7	M1+E2 E2	787.81 631.82	15/2- 13/2-
1378.19 4	21/2-		217.27 2 412.39 2	29.8 15 100.0 23	(M1+E2) E2	1160.96 965.77	19/2- 17/2-
1858.66 5	(25/2-)		251.84 2 480.50 17	20.6 18 100 6		1606.80 1378.19	(23/2-) 21/2-
2394.45 6	(29/2-)		280.56 535.79 3	23.7 23 100 6		2113.89 1858.66	(27/2-) (25/2-)
2972.4 10	(33/2-)		578 1	100		2394.45	(29/2-)
3579.4 15	(37/2-)		607 1	100		2972.4	(33/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - π7/2[523],α=-1/2.
292.844 24	7/2-	0.9 µs 1
496.64 4	11/2-		112.89 4 203.76 5	100 7 11.3 8	M1+E2 E2	383.70 292.844	9/2- 7/2-
787.81 4	15/2-		156.04 3 291.150 10	100 4 47 3	M1+E2 (E2)	631.82 496.64	13/2- 11/2-
1160.96 4	19/2-		195.20 1 372.96 5	67.5 21 100.0 25	(M1+E2) E2	965.77 787.81	17/2- 15/2-
1606.80 4	(23/2-)		228.61 1 445.82 4	100 5 28.7 14		1378.19 1160.96	21/2- 19/2-
2113.89 6	(27/2-)		255.12 6 507.14 4	100 10 113 6		1858.66 1606.80	(25/2-) (23/2-)
2670.64 7	(31/2-)		276.22 11 556.74 5	100 16 88 5		2394.45 2113.89	(29/2-) (27/2-)
3261.6 10	(35/2-)		591 1	100		2670.64	(31/2-)
3878.6 15	(39/2-)		617 1	100		3261.6	(35/2-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 9 - π3/2[411] band.
470.89 5	3/2+
557.93 5	5/2+		35.69 3 415.50 20 441.2 1 547.5 1	33 8 90 18 100 17	(M1+E2) (M1) M1	522.25 142.441 116.594 10.417	5/2+ 7/2+ 5/2+ 3/2+
601.99 4	(7/2+)		79.56 9 131.06 4 275.57 459.63 19 485.39 12	17 4 <252 <65 100 18		522.25 470.89 326.50 142.441 116.594	5/2+ 3/2+ 9/2+ 7/2+ 5/2+
709.12 4	(9/2+)		107.13 4 186.68 11 338.01 22 382.41 30 566.83 11	100 50 70 25 35 10 30 15 30 5		601.99 522.25 371.05 326.50 142.441	(7/2+) 5/2+ 11/2+ 9/2+ 7/2+
840.18 4	(11/2+)		131.06 4 218.07 17 238.13 4 469.25 6 513.66 5	<242 <96 50 4 100 25 75 8	(M1)	709.12 622.09 601.99 371.05 326.50	(9/2+) 13/2+ (7/2+) 11/2+ 9/2+
1001.23 3	(13/2+)		161.45 6 ? 292.07 312.11 11 379.15 2 630.14 3	26.7 33 <173 100 7	(M1)	840.18 709.12 689.19 622.09 371.05	(11/2+) (9/2+) 15/2+ 13/2+ 11/2+
1163.96 5	(15/2+)		162.82 9 323.34 19 474.77 541.87 7	100 5 29 5 57 14		1001.23 840.18 689.19 622.09	(13/2+) (11/2+) 15/2+ 13/2+
1372.75 3	(17/2+)		208.86 7 286.25 17 371.52 1 379.15 2 683.54 4	<21 7.7 23 100 12 <40.0 16.2 16	(E2)	1163.96 1086.57 1001.23 993.60 689.19	(15/2+) 19/2+ (13/2+) (17/2+) 15/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
1562.93 4	(19/2+)		190.14 9 398.65 13 476.35 9 569.35 6	41 9 55 14 100 18 <82		1372.75 1163.96 1086.57 993.60	(17/2+) (15/2+) 19/2+ (17/2+)
1813.96 4	(21/2+)		251.03 1 384.44? 441.22 3 727.63 11	<3220 <415 100 29	(D)	1562.93 1429.52 1372.75 1086.57	(19/2+) 21/2(+) (17/2+) 19/2+
2022.25 9	(23/2+)		459.63 19 472.17 8	<88 100 24		1562.93 1550.03	(19/2+) 23/2(+)
2321.08 6	(25/2+)		405.69 4 507.14 4 ?	47 13 100 6		1915.39 1813.96	(25/2+) (21/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 10 - π5/2[402] band.
522.25 5	5/2+
657.84 5	(7/2+)		331.21 22 515.42 4 541.28 25		(M1+E2) (M1)	326.50 142.441 116.594	9/2+ 7/2+ 5/2+
780.48 5	(9/2+)		222.50 19 ? 453.97 4	<17 100 5	[E2] (M1)	557.93 326.50	5/2+ 9/2+
927.87 4	(11/2+)		270.14 305.91 27 556.74 5 601.48 5	24 6 <189 100 12	(M1)	657.84 622.09 371.05 326.50	(7/2+) 13/2+ 11/2+ 9/2+
1096.47 4	(13/2+)		168.66 4 315.79 17 407.27? 474.38 725.34 4	100 8 17 4 75 13		927.87 780.48 689.19 622.09 371.05	(11/2+) (9/2+) 15/2+ 13/2+ 11/2+
1281.46 6	(15/2+)		185.11 17 ? 287.70 11 353.42 15 592.27 659.18 24	127 46 27 8 100 35 19 4		1096.47 993.60 927.87 689.19 622.09	(13/2+) (17/2+) (11/2+) 15/2+ 13/2+
1487.36 8	(17/2+)		206.18 10 ? 390.61 12 400.56 15 798.46 10	144 22 100 22 67 22 78 11		1281.46 1096.47 1086.57 689.19	(15/2+) (13/2+) 19/2+ 15/2+
1705.57 6	(19/2+)		218.07 17 ? 276.22 11 424.05 5 619.04 7 1016.62 29	<180 <82 82 9 100 18 55 9		1487.36 1429.52 1281.46 1086.57 689.19	(17/2+) 21/2(+) (15/2+) 19/2+ 15/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 11 - π3/2[532]+(π1/2[541]), K-2 band.
852.79 4	(3/2-)
882.12 18	(5/2-)		694.46 17	100	(M1+E2)	187.660	5/2-
935.24 4	(7/2-)		475.25 6 649.38 4 747.50 9	<209 100 32 18 5	(M1) (M1)	459.92 285.90 187.660	7/2- 9/2- 5/2-
1008.50 4	(9/2-)		722.60 3	100	(E2)	285.90	9/2-
1105.33 4	(11/2-)		635.07 3 819.41			470.26 285.90	13/2- 9/2-
1223.11 4	(13/2-)		523.93 752.85 3			699.17 470.26	(11/2-) 13/2-
1358.75 4	(15/2-)		253.43 4 617.33 4 888.37 12	<58 100 10 38 5		1105.33 741.37 470.26	(11/2-) 17/2- 13/2-
1524.93 4	(17/2-)		301.84 517.34 783.57 3			1223.11 1007.62 741.37	(13/2-) (15/2-) 17/2-
1691.24 4	(19/2-)		332.36 6 595.05 3 950.11 21	61 6 100 6 44.4 28		1358.75 1096.22 741.37	(15/2-) 21/2- 17/2-
1916.61 6	(21/2-)		391.72 5 535.61 820.44			1524.93 1380.98 1096.22	(17/2-) (19/2-) 21/2-
2098.06 5	(23/2-)		406.84 4 569.35 6 1001.70 23	100 8 <45 15.0 25		1691.24 1528.69 1096.22	(19/2-) 25/2- 21/2-
2396.42 7	(25/2-)		479.88 6 587.45 15 867.36 26	100 12 10.0 20 8.0 20		1916.61 1808.66 1528.69	(21/2-) (23/2-) 25/2-
2573.30 7	(27/2-)		475.25 6 542.51 15 1044.60	<380 100 25		2098.06 2030.77 1528.69	(23/2-) 29/2(-) 25/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 12 - π9/2[514] band.
929.74 7	(9/2-)
1044.06 5	11/2-		114.32 5 547.42 3 660.36 5 751.21 10	100 42 <97 65 7 <84	(M1) (M1) (E2)	929.74 496.64 383.70 292.844	(9/2-) 11/2- 9/2- 7/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 13 - π7/2[404], K+2 band.
944.89 4	(11/2+)
1101.24 4	(13/2+)		156.33 503.84 13 665.13 3 805.07 4	28 8 <88 100 8		944.89 597.48 436.07 296.21	(11/2+) 13/2+ 11/2+ 9/2+
1276.78 4	(15/2+)		175.34 6 332.11 6 497.71 4 679.43 7 840.70 6	100 7 54 7 <161 71 7 68 7		1101.24 944.89 779.01 597.48 436.07	(13/2+) (11/2+) 15/2+ 13/2+ 11/2+
1470.16 5	(17/2+)		193.45 7 368.99 12 491.70 691.20 872.62 8	100 5 75 10 80 10		1276.78 1101.24 978.55 779.01 597.48	(15/2+) (13/2+) 17/2+ 15/2+ 13/2+
1678.90 5	(19/2+)		208.86 7 402.07 5 484.08 11 700.36 7	124 35 71 12 59 18 100 12		1470.16 1276.78 1194.82 978.55	(17/2+) (15/2+) 19/2+ 17/2+
1901.27 6	(21/2+)		222.50 19 431.11 4 706.35 15	<88 <263 100 25		1678.90 1470.16 1194.82	(19/2+) (17/2+) 19/2+
2135.94 7	(23/2+)		234.68 7 457.05 6 711.34?	24 6 100 12		1901.27 1678.90 1424.67	(21/2+) (19/2+) 21/2+
2381.92 13	(25/2+)		246.10 16 480.50 17	100 33 <1430		2135.94 1901.27	(23/2+) (21/2+)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2+	9.25 d 2 % ε = 100	μ=-0.197 2 (1973Ek01,1988Al04,2019StZV) Evaluated rms charge radius=5.2129 fm 36 (2013An02). E(level): Evaluated rms charge radius=5.2129 fm 36 (2013An02). π1/2[411],α=+1/2.
10.417	3/2+	0.95 ns 5	E(level): π1/2[411],α=-1/2.
116.594	5/2+	66 ps 7	1974Ch44 noted that their deduced experimental nuclear structure factors in (³He,d) and (α,t) transfer reactions were two to three times larger than the predicted value for the 5/2⁺, π1/2[411] state, as also was the case for this configuration in ¹⁶⁵Tm, ¹⁶⁹Tm and ¹⁷¹Tm. Authors further stated that their Coriolis mixing calculations could not explain this strength in terms of admixtures of other Nilsson states. E(level): 1974Ch44 noted that their deduced experimental nuclear structure factors in (³He,d) and (α,t) transfer reactions were two to three times larger than the predicted value for the 5/2⁺, π1/2[411] state, as also was the case for this configuration in ¹⁶⁵Tm, ¹⁶⁹Tm and ¹⁷¹Tm. Authors further stated that their Coriolis mixing calculations could not explain this strength in terms of admixtures of other Nilsson states. π1/2[411],α=+1/2.
142.441	7/2+	343 ps 15	E(level): π1/2[411],α=-1/2.
171.76	(1/2)-		E(level): π1/2[541],α=+1/2.
179.501	7/2+	1.16 µs 6 % IT = 100	E(level): π7/2[404],α=-1/2.
187.660	5/2-		E(level): π1/2[541],α=+1/2.
285.90	9/2-		E(level): π1/2[541],α=+1/2.
290.94	(3/2-)		E(level): π1/2[541],α=-1/2.
292.844	7/2-	0.9 µs 1	E(level): π7/2[523],α=-1/2.
296.21	9/2+		E(level): π7/2[404],α=+1/2.
326.50	9/2+		E(level): π1/2[411],α=+1/2.
371.05	11/2+		E(level): π1/2[411],α=-1/2.
383.70	9/2-		E(level): π7/2[523],α=+1/2.
436.07	11/2+		E(level): π7/2[404],α=-1/2.
459.92	7/2-		E(level): π1/2[541],α=-1/2. J^π(level): From angular-distribution and cross-section data in (³He,d) and (α,t).
470.26	13/2-		E(level): π1/2[541],α=+1/2.
470.89	3/2+		E(level): π3/2[411] band. J^π(level): From angular-distribution and cross-section data in (³He,d) and (α,t).
496.64	11/2-		E(level): π7/2[523],α=-1/2. J^π(level): From angular-distribution and cross-section data in (³He,d) and (α,t).
522.25	5/2+		E(level): π5/2[402] band. J^π(level): From angular-distribution and cross-section data in (³He,d) and (α,t).
557.93	5/2+		E(level): π3/2[411] band. J^π(level): From angular-distribution and cross-section data in (³He,d) and (α,t).
597.48	13/2+		E(level): π7/2[404],α=+1/2.
601.99	(7/2+)		E(level): π3/2[411] band.
622.09	13/2+		E(level): π1/2[411],α=+1/2.
631.82	13/2-		E(level): π7/2[523],α=+1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
657.84	(7/2+)		XREF: γ(663). E(level): π5/2[402] band.
689.19	15/2+		E(level): π1/2[411],α=-1/2.
699.17	(11/2-)		E(level): π1/2[541],α=-1/2.
709.12	(9/2+)		E(level): π3/2[411] band.
741.37	17/2-		E(level): π1/2[541],α=+1/2.
779.01	15/2+		E(level): π7/2[404],α=-1/2.
780.48	(9/2+)		E(level): π5/2[402] band.
787.81	15/2-		E(level): π7/2[523],α=-1/2.
840.18	(11/2+)		E(level): π3/2[411] band.
852.79	(3/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
882.12	(5/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
927.87	(11/2+)		E(level): π5/2[402] band.
929.74	(9/2-)		E(level): π9/2[514] band.
935.24	(7/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
944.89	(11/2+)		E(level): π7/2[404], K+2 band.
965.77	17/2-		E(level): π7/2[523],α=+1/2.
978.55	17/2+		E(level): π7/2[404],α=+1/2.
993.60	(17/2+)		E(level): π1/2[411],α=+1/2.
1001.23	(13/2+)		E(level): π3/2[411] band.
1007.62	(15/2-)		E(level): π1/2[541],α=-1/2.
1008.50	(9/2-)		XREF: γ(1010). E(level): π3/2[532]+(π1/2[541]), K-2 band.
1044.06	11/2-		E(level): π9/2[514] band. J^π(level): From angular-distribution and cross-section data in (³He,d) and (α,t).
1086.57	19/2+		E(level): π1/2[411],α=-1/2.
1096.22	21/2-		E(level): π1/2[541],α=+1/2.
1096.47	(13/2+)		E(level): π5/2[402] band.
E(level)	J^π(level)	T_1/2(level)	Comments
1101.24	(13/2+)		E(level): π7/2[404], K+2 band.
1105.33	(11/2-)		XREF: γ(1092). E(level): π3/2[532]+(π1/2[541]), K-2 band.
1160.96	19/2-		E(level): π7/2[523],α=-1/2.
1163.96	(15/2+)		E(level): π3/2[411] band.
1194.82	19/2+		E(level): π7/2[404],α=-1/2.
1216.56	7/2+		XREF: γ(1210).
1223.11	(13/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
1276.78	(15/2+)		E(level): π7/2[404], K+2 band.
1281.46	(15/2+)		E(level): π5/2[402] band.
1358.75	(15/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
1372.75	(17/2+)		E(level): π3/2[411] band.
1374			XREF: γ(1380).
1378.19	21/2-		E(level): π7/2[523],α=+1/2.
1380.98	(19/2-)		E(level): π1/2[541],α=-1/2.
1424.67	21/2+		E(level): π7/2[404],α=+1/2.
1429.52	21/2(+)		E(level): π1/2[411],α=+1/2.
1470.16	(17/2+)		E(level): π7/2[404], K+2 band.
1487.36	(17/2+)		E(level): π5/2[402] band.
1524.93	(17/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
1528.69	25/2-		E(level): π1/2[541],α=+1/2.
1543.80	(5/2+,7/2+)		1533.1γ to 3/2⁺, 1217.1γ to 9/2⁺.
1550.03	23/2(+)		E(level): π1/2[411],α=-1/2.
1562.93	(19/2+)		E(level): π3/2[411] band.
1580.97	(5/2+,7/2+)		XREF: γ(1574).
1606.80	(23/2-)		E(level): π7/2[523],α=-1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
1629.65	(5/2+,7/2+)		XREF: γ(1625).
1668.93	(23/2+)		E(level): π7/2[404],α=-1/2.
1678.90	(19/2+)		E(level): π7/2[404], K+2 band.
1691.24	(19/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
1705.57	(19/2+)		E(level): π5/2[402] band.
1808.66	(23/2-)		E(level): π1/2[541],α=-1/2.
1813.96	(21/2+)		E(level): π3/2[411] band.
1858.66	(25/2-)		E(level): π7/2[523],α=+1/2.
1901.27	(21/2+)		E(level): π7/2[404], K+2 band.
1915.39	(25/2+)		E(level): π1/2[411],α=+1/2.
1916.61	(21/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
1922.39	(25/2+)		E(level): π7/2[404],α=+1/2.
2022.25	(23/2+)		E(level): π3/2[411] band.
2030.77	29/2(-)		E(level): π1/2[541],α=+1/2.
2065.45	(27/2+)		E(level): π1/2[411],α=-1/2.
2098.06	(23/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
2113.89	(27/2-)		E(level): π7/2[523],α=-1/2.
2135.94	(23/2+)		E(level): π7/2[404], K+2 band.
2186.45	(27/2+)		E(level): π7/2[404],α=-1/2.
2279.75	(27/2-)		E(level): π1/2[541],α=-1/2.
2321.08	(25/2+)		E(level): π3/2[411] band.
2381.92	(25/2+)		E(level): π7/2[404], K+2 band.
2394.45	(29/2-)		E(level): π7/2[523],α=+1/2.
2396.42	(25/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
2440.46	(29/2+)		E(level): π1/2[411],α=+1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
2455.62	(29/2+)		E(level): π7/2[404],α=+1/2.
2573.30	(27/2-)		E(level): π3/2[532]+(π1/2[541]), K-2 band.
2593.46	(33/2-)		E(level): π1/2[541],α=+1/2.
2620.14	(31/2+)		E(level): π1/2[411],α=-1/2.
2670.64	(31/2-)		E(level): π7/2[523],α=-1/2.
2735.83	(31/2+)		E(level): π7/2[404],α=-1/2.
2799.06	(31/2-)		E(level): π1/2[541],α=-1/2.
2972.4	(33/2-)		E(level): π7/2[523],α=+1/2.
2993.5	(33/2+)		E(level): π1/2[411],α=+1/2.
3013.5	(33/2+)		E(level): π7/2[404],α=+1/2.
3208.8	(35/2+)		E(level): π1/2[411],α=-1/2.
3210.5	(37/2-)		E(level): π1/2[541],α=+1/2.
3261.6	(35/2-)		E(level): π7/2[523],α=-1/2.
3311.2	(35/2+)		E(level): π7/2[404],α=-1/2.
3575.5	(37/2+)		E(level): π1/2[411],α=+1/2.
3579.4	(37/2-)		E(level): π7/2[523],α=+1/2.
3600.5	(37/2+)		E(level): π7/2[404],α=+1/2.
3832.8	(39/2+)		E(level): π1/2[411],α=-1/2.
3877.5	(41/2-)		E(level): π1/2[541],α=+1/2.
3878.6	(39/2-)		E(level): π7/2[523],α=-1/2.
3916.2	(39/2+)		E(level): π7/2[404],α=-1/2.
4196.5	(41/2+)		E(level): π1/2[411],α=+1/2.
4196.5	(41/2+)		E(level): π7/2[404],α=+1/2.
4494.8	(43/2+)		E(level): π1/2[411],α=-1/2.
4565.2	(43/2+)		E(level): π7/2[404],α=-1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
4596.5	(45/2-)		E(level): π1/2[541],α=+1/2.
4868.5	(45/2+)		E(level): π1/2[411],α=+1/2.
5204.8	(47/2+)		E(level): π1/2[411],α=-1/2.
5365.5	(49/2-)		E(level): π1/2[541],α=+1/2.
5970.8	(51/2+)		E(level): π1/2[411],α=-1/2.
6185.5	(53/2-)		E(level): π1/2[541],α=+1/2.
7055.5	(57/2-)		E(level): π1/2[541],α=+1/2.
7979.5	(61/2-)		E(level): π1/2[541],α=+1/2.
8952.5	(65/2-)		E(level): π1/2[541],α=+1/2.

E(level)	E(gamma)	Comments
10.417	10.419	E(γ): From ¹⁶⁷Yb ε decay. M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
116.594	106.18	E(γ): weighted average of 106.16 2 from ¹⁶⁷Yb ε decay, 106.18 1 from (α,2nγ), and 106.25 4 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay. Others: 100 9 from (α,2nγ) and 100 7 from (p,nγ) M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
116.594	116.68	E(γ): unweighted average of 116.57 2 from ¹⁶⁷Yb ε decay, 116.69 1 from (α,2nγ), and 116.77 5 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay. Others: 12.6 13 from (α,2nγ); 39.2 26 from (p,nγ) for a doublet M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
142.441	25.83	E(γ): from ¹⁶⁷Yb ε decay. Other: 25.80 20 from (p,nγ) I(γ): weighted average of 1.6 5 from ¹⁶⁷Yb ε decay and 2.0 10 from (p,nγ).
142.441	132.05	E(γ): unweighted average of 131.99 2 from ¹⁶⁷Yb ε decay, 132.05 2 from (α,2nγ), and 132.12 5 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay. Others: 100 5 from (α,2nγ) and 100 7 from (p,nγ) M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
171.76	161.32	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay. M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
171.76	171.77	E(γ): weighted average of 171.75 8 from ¹⁶⁷Yb ε decay, 171.76 5 from (α,2nγ), and 171.80 6 from (p,nγ) I(γ): from (p,nγ). Others: 100 28 from ¹⁶⁷Yb ε decay and 100 18 from (α,2nγ)
179.501	37.05	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay. M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
	62.91	M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
	169.04	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay. M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
187.660	177.26	E(γ): weighted average of 177.22 3 from ¹⁶⁷Yb ε decay, 177.27 2 from (α,2nγ), and 177.33 6 from (p,nγ) M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
282.24	94.53	E(γ): From ¹⁶⁷Yb ε decay.
	110.49	E(γ): From ¹⁶⁷Yb ε decay.
	272.1	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay.
	282.4	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay.
285.90	98.25	E(γ): others: 98.24 3 from ¹⁶⁷Yb ε decay and 98.30 10 from (p,nγ) I(γ): weighted average of 3.9 4 from ¹⁶⁷Yb ε decay and 3.20 29 from (α,2nγ). Other: 9.1 31 from (p,nγ) is discrepant M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
285.90	143.46	E(γ): others: 143.46 2 from ¹⁶⁷Yb ε decay and 143.53 5 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay. Others: 100 4 from (α,2nγ) and 100 7 from (p,nγ)
290.94	103.32	E(γ): γ masked by neighboring intense γ rays in ¹⁶⁷Yb ε decay I(γ): from Iγ(280.55γ) and adopted I(103.32γ)/I(280.5γ)=2.9 10 in (α,2nγ)
	174.26	E(γ): weighted average of 174.25 7 from (α,2nγ) and 174.27 7 from (p,nγ). γ masked by neighboring intense γ rays in ¹⁶⁷Yb ε decay I(γ): from Iγ(280.55γ) and adopted I(174.26γ)/I(280.5γ)=2.04 63, taken from average of values in (α,2nγ) and (p,nγ)
	280.55	E(γ): weighted average of 280.5 2 from ¹⁶⁷Yb ε decay and 280.60 20 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay, 35 11 from (α,2nγ), and 13 4 from (p,nγ)
	290.92	E(γ): weighted average of 290.86 7 from ¹⁶⁷Yb ε decay and 291.02 9 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay. No intensity is reported in (α,2nγ). Most intense γ in (p,nγ) for an unresolved doublet.
292.844	6.93	E(γ): from level energy difference.
	105.19	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay. M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
	113.34	E(γ): from (α,2nγ). Others: 113.32 2 from ¹⁶⁷Yb ε decay and 113.41 5 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay. Others: 100 9 from (α,2nγ) and 100 7 from (p,nγ) M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
	150.40	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay. M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
	176.26	E(γ): from (α,2nγ). Others: 176.23 3 from ¹⁶⁷Yb ε decay and 176.34 6 from (p,nγ) I(γ): weighted average of 30.7 11 from (α,2nγ) and 28.2 22 from (p,nγ) M(γ): From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
E(level)	E(gamma)	Comments
296.21	116.69	E(γ): weighted average of 116.66 3 from ¹⁶⁷Yb ε decay, 116.69 1 from (α,2nγ), and 116.77 5 from (p,nγ) I(γ): from ¹⁶⁷Yb ε decay
296.21	179.55	E(γ): From ¹⁶⁷Yb ε decay. I(γ): From ¹⁶⁷Yb ε decay.
326.50	184.13	E(γ): weighted average of 184.1 2 from ¹⁶⁷Yb ε decay, 184.01 15 from (α,2nγ), and 184.17 8 from (p,nγ) I(γ): others: 100 57 from ¹⁶⁷Yb ε decay and 100 5 from (p,nγ)
326.50	209.93	E(γ): weighted average of 209.92 2 from (α,2nγ) and 210.01 7 from (p,nγ) I(γ): weighted average of 44.6 12 from (α,2nγ) and 47 4 from (p,nγ). Other: 43 29 from ¹⁶⁷Yb ε decay M(γ): E2 or (E2) from ce data in (p,nγ); γ(θ) in (α,2nγ) consistent with ΔJ=2. Where a firm E2 is adopted while (E2) from (p,nγ), it is because M2 is ruled out by RUL since it would require an isomeric lifetime of ≈ or > 100 ns
371.05	44.4	E(γ): from level energy difference.
	85.16	E(γ): unweighted average of 85.10 1 from (α,2nγ) and 85.21 4 from (p,nγ) M(γ): d from γ(θ) in (α,2nγ); (E1) from level scheme
	228.61	E(γ): other: 228.67 7 from (p,nγ). Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided M(γ): for a doublet in (α,2nγ). E2 or (E2) from ce data in (p,nγ); γ(θ) in (α,2nγ) consistent with ΔJ=2. Where a firm E2 is adopted while (E2) from (p,nγ), it is because M2 is ruled out by RUL since it would require an isomeric lifetime of ≈ or > 100 ns
383.70	90.86	E(γ): unweighted average of 90.83 6 from ¹⁶⁷Yb ε decay, 90.84 1 from (α,2nγ), and 90.91 2 from (p,nγ) M(γ): also supported by γ(θ) from (α,2nγ). From ce data in ¹⁶⁷Yb ε decay. δ is deduced by evaluators using the BrIccMixing code
436.07	139.83	E(γ): weighted average of 139.83 1 from (α,2nγ) and 139.91 5 from (p,nγ) I(γ): from (α,2nγ). Other: 100 8 from (p,nγ)
436.07	256.57	E(γ): other: 256.67 8 from (p,nγ) I(γ): weighted average of 77.3 15 from (α,2nγ) and 86 9 from (p,nγ) M(γ): E2 or (E2) from ce data in (p,nγ); γ(θ) in (α,2nγ) consistent with ΔJ=2. Where a firm E2 is adopted while (E2) from (p,nγ), it is because M2 is ruled out by RUL since it would require an isomeric lifetime of ≈ or > 100 ns
459.92	174.0	E(γ): from (p,nγ)
459.92	343.37	E(γ): weak γ from (α,2nγ). In (p,nγ) a 343.28 15 γ is an unresolved doublet, placed from 460 and 779 levels. See comment for 342.95γ from 779 level.