List of levels for 71GE

Authors: Balraj Singh and Jun Chen | Citation: Nucl. Data Sheets 188, 1 (2023) | Cutoff date: 17-Jan-2023

1941Se03: ⁷¹Ge produced and identified in ⁷¹Ga(d,2n) reaction at E=8 MeV and in ⁷⁰Ge(d,p) reaction at 16 MeV, measured half-life

1948Mc32: ⁷¹Ge produced in decay of ⁷¹As.

Later references for production and identification of ⁷¹Ge: 1950Ho26, 1952Br90, 1955Bi96, 1956Ru45, 1959Gl56, 1959Mo98.

Mass measurements: 2016Al30, 2013Fr13: ⁷¹Ga - ⁷¹Ge mass difference

Other measurements:

⁷¹Ga(³He,t): 1984Ko10

2022Ba21 (also 2022Ba17): ⁷¹Ge(ν,e),E(ν)<1 MeV from ⁵¹Cr decay. Measured Eβ, Iβ; deduced yield of ⁷¹Ge yields, deficit of electron neutrinos observed in gallium-based radiochemical measurements with high-intensity neutrino sources to address the "gallium anomaly "; Baksan Experiment on Sterile Transitions (BEST).

⁷¹Ga(ν,e): 2009Ab16, solar neutrino capture rate measurements, SAGE (Soviet-American Gallium) experiment

Theoretical calculations:

2022No04: calculated single-particle energies, occupation probabilities, levels, Jπ, B(E2), B(M1), (β,γ)-deformation energy surfaces, magnetic dipole moment using constrained self-consistent mean-field (SCMF) method based on the universal relativistic functional DD-PC1.

2015Ka46: calculated level energies of low-lying, low spin states and B(E2) values in odd-A isotopes, neutron g_9/2 and proton p_3/2 occupancies for low lying states, magnetic moments and electric quadrupole moments, low- and high-spin levels, Jπ, B(E2) using shell-model with a pairing-plus-multipole Hamiltonian and monopole-based universal force interaction (PMMU model) for the pf_5/2g_9/2 shell.

2012Mu09: calculated neutron pairing gaps, ground state energy shell model Monte Carlo method.

2012Lu10: calculated β-decay strength functions, resonance structures.

2009Ho14: calculated two-body matrix elements, monopole matrix elements, single-particle proton and neutron energies, binding energies, magnetic dipole and electric quadrupole moments, levels, Jπ, B(E2) using shell-model with JUN45 effective interaction.

2004Br44: calculated levels, Jπ, magnetic dipole and electric quadrupole moments, B(M1), B(E2), transition branching ratios using proton-neutron interacting boson-fermion model.

2003Ho02: calculated levels, Jπ log ft for Gamow-Teller transitions. Discussed implications for solar neutrino detection.

1997Ka73: calculated Gamow-Teller strengths, Ga solar neutrino detector ν capture rates.

1979Pa04: calculated levels, Jπ using quasiparticle-vibration coupling, unified nuclear model.

1976Pa08: calculated levels, B(|l), neutron hole clusters coupled to quadrupole vibration using Alaga, Bohr-Mottelson microscopic models.

Q-value: Q(ε)=232.47 9, S(2n)=18948.6 15, S(2p)=16066.7 11 (2021Wa16)

E(level): From a least-squares fit to Eγ data for levels connected with γ transitions and others are from transfer reactions, unless otherwise noted. Fit to the listed Eγ data for 284 γ rays gave an unacceptable normalized χ²=3.4 with 17 γ rays outside three standard deviations, as compared to χ²=1.26 at 95% confidence level. The evaluators have increased the uncertainties, as indicated under comments, resulting in χ²=1.45 with these adjustments. Uncertainty of 0.5 keV for γ-ray energy is assumed when not stated.

T_1/2(level): From ΔS(a) in (p,nγ) (1999Iv08), unless otherwise stated. There are values available for 747, 808, 831, 1096, 1379, 1406, 1414, 1422, 1558 and 1566 levels from ΔS(a) measurements of 2002Ka51 from (p,nγ). These values are not included here due to problems associated with assignment of γ-ray lines to ⁷¹Ge, since a natural Ga target was used in the experiment. See (p,nγ) dataset for details.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
174.954	5/2-	81 ns 3	174.956 9	E2		0.0915	B(E2)(W.u.)=2.24 8, α=0.0915 13, α(K)=0.0808 11, α(L)=0.00923 13, α(M)=0.001369 19, α(N)=7.91E-5 11
198.371	9/2+	20.22 ms 12 % IT = 100	23.438 15	M2		207.5	B(M2)(W.u.)=0.0607 10, α=207.5 30, α(K)=169.5 24, α(L)=32.7 5, α(M)=5.03 7, α(N)=0.265 4
499.915	3/2-		499.94 3	M1+E2	-2.3 1	2.20×10^-3	α=2.20×10^-3 3
525.114	5/2+		326.798 19	E2		0.00955	α=0.00955 13
525.114	5/2+		350.164 7	E1+M2	-0.19 3	0.00216	α=0.00216 13
589.775	7/2+		64.7 1	[M1+E2]		2.0	α=2.0 18, α(K)=1.7 15, α(L)=0.26 24, α(M)=0.038 35, α(N)=0.0017 15
	7/2+		391.396 24	M1+E2	-0.21 +4-3	0.00257	α=0.00257 5
	7/2+		414.55 16	[E1]		1.13×10^-3	α=1.13×10^-3 2
708.196	3/2-	> 10.7 ps	533.2 1	[M1,E2]		0.0016	α=0.0016 4
747.248	5/2-		247.352 5	M1+E2	-0.18 7	0.0080	α=0.0080 5
747.248	5/2-		572.259 15	M1+E2		0.00129	α=0.00129 27
808.196	1/2-		308.25 4	(M1+E2)		0.008	α=0.008 4
831.301	3/2-		241.77 13	[M2]		0.0409	α=0.0409 6, α(K)=0.0362 5, α(L)=0.00408 6, α(M)=0.000612 9, α(N)=3.90×10^-5 6
	3/2-		306.210 25	(E1+M2)		0.00274	α=0.00274 17
	3/2-		331.42 5	E2(+M1)	1.4 GT	0.0082	α=0.0082 9
	3/2-		831.293 10	(M1+E2)	-0.6 +4-7
1026.561	5/2-	> 1.2 ps	195.22 15	[M1,E2]		0.037	α=0.037 24, α(K)=0.033 21, α(L)=0.0037 24, α(M)=5.E-4 4, α(N)=3.3E-5 20
	5/2-	> 1.2 ps	279.379 7	(M1+E2)		0.011	α=0.011 6
	5/2-	> 1.2 ps	526.642 4	(M1+E2)	-0.16 3	1.26×10^-3	B(E2)(W.u.)<13, B(M1)(W.u.)<0.07, α=1.26E-3 2
	5/2-	> 1.2 ps	828.0 1	[M2]		1.15×10^-3	α=1.15×10^-3 2
	5/2-	> 1.2 ps	851.63 7	(M1+E2)	+0.8 7		B(E2)(W.u.)<5.7, B(M1)(W.u.)<0.004
	5/2-	> 1.2 ps	1026.510 17	(E2)			B(E2)(W.u.)<4.9
1037.83	9/2+		448.1 1	M1+E2	+0.47 +5-6	0.00207	α=0.00207 6
1037.83	9/2+		839.4 1	(M1(+E2))	+0.10 18	4.47×10^-4	α=4.47×10^-4 9
1095.511	3/2-	0.62 ps 14	264.21 15	[M1,E2]		0.013	α=0.013 7
	3/2-	0.62 ps 14	287.32 4	[M1,E2]		0.010	α=0.010 5
	3/2-	0.62 ps 14	348.27 4	[M1,E2]		0.0055	α=0.0055 22
	3/2-	0.62 ps 14	387.31 4	[M1,E2]		0.0039	α=0.0039 14
	3/2-	0.62 ps 14	570.42 21	[E1]			B(E1)(W.u.)=1.62E-5 +49-31
	3/2-	0.62 ps 14	595.6 1	[M1,E2]		0.00116	α=0.00116 23
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1096.07	7/2-		596.1 5	(E2)		1.38×10^-3	α=1.38×10^-3 2
1139.441	3/2-	4.0 ps 14	392.16 5	(M1+E2)		0.0038	α=0.0038 13
	3/2-	4.0 ps 14	614.26 5	[E1]			B(E1)(W.u.)=5.6E-6 +31-17
	3/2-	4.0 ps 14	964.479 9	(M1+E2)	-0.8 +9-49		B(E2)(W.u.)<1.4, B(M1)(W.u.)<9.0E-4
1192.23	11/2+	< 0.108 ps	993.9 1	M1+E2	+1.25 21		B(E2)(W.u.)>161, B(M1)(W.u.)>0.066
1205.146	5/2+	1.11 ps 28	373.837 12	(E1)		1.49×10^-3	B(E1)(W.u.)=0.00081 +29-16, α=1.49E-3 2
	5/2+	1.11 ps 28	457.72 12	[E1]			B(E1)(W.u.)=1.7E-5 +8-5
	5/2+	1.11 ps 28	615.365 10	(M1+E2)		0.00107	α=0.00107 20
	5/2+	1.11 ps 28	705.1 3	[E1]			B(E1)(W.u.)=3.7E-6 +29-19
	5/2+	1.11 ps 28	1030.20 8	[E1]			B(E1)(W.u.)=4.8E-6 +17-10
1212.511	5/2-	> 1.2 ps	465.228 10	(M1+E2)		0.0023	α=0.0023 7
	5/2-	> 1.2 ps	504.27 5	(M1+E2)		0.0018	α=0.0018 5
	5/2-	> 1.2 ps	622.71 4	[E1]			B(E1)(W.u.)<1.9E-5
	5/2-	> 1.2 ps	1212.500 23	(E2)			B(E2)(W.u.)<2.9
1298.75	3/2-	0.42 ps 9	551.5 1	[M1,E2]		0.00143	α=0.00143 31
1298.75	3/2-	0.42 ps 9	590.5 1	[M1,E2]		0.00119	α=0.00119 23
1349.10	1/2+	0.46 ps 11	517.78 6	[E1]			B(E1)(W.u.)=0.0041 +13-8
	1/2+	0.46 ps 11	824.14 19	[E2]			B(E2)(W.u.)=31 +12-9
	1/2+	0.46 ps 11	1349.0 4	[E1]			B(E1)(W.u.)=5.8E-5 +23-16
1422.04	9/2-	< 1.2 ps	326.1 6	(M1)			B(M1)(W.u.)>0.014
	9/2-	< 1.2 ps	675.0 2	E2			B(E2)(W.u.)>25
	9/2-	< 1.2 ps	1247.0 1	E2			B(E2)(W.u.)>7.1
1477.03	11/2+	< 0.64 ps	887.4 1	E2			B(E2)(W.u.)>39
1477.03	11/2+	< 0.64 ps	1278.5 1	M1+E2	+4.8 10		B(E2)(W.u.)>6.9, B(M1)(W.u.)>2.4E-4
1506.388	7/2-	0.51 ps 16	674.33 8	[E2]		0.000975	B(E2)(W.u.)=15 +7-4, α=0.000975 14, α(K)=0.000870 12, α(L)=9.03E-5 13, α(M)=1.347E-5 19, α(N)=8.69E-7 12
	7/2-	0.51 ps 16	798.55 23	[E2]			B(E2)(W.u.)=26 +12-6
	7/2-	0.51 ps 16	1006.466 17	[E2]			B(E2)(W.u.)=15 +7-4
	7/2-	0.51 ps 16	1307.98 3	[E1]			B(E1)(W.u.)=1.9E-5 +9-5
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1558.757	5/2+		1033.55 3	(M1+E2)	+1.6 +14-19
1598.534	3/2-	0.55 ps 15	1073.4 2	[E1]			B(E1)(W.u.)=4.6E-6 +21-13
1743.385	3/2-	0.42 ps 15	445.07 17	[M1,E2]		0.0026	α=0.0026 8
1743.385	3/2-	0.42 ps 15	1218.16 7	[E1]			B(E1)(W.u.)=1.7E-5 +10-5
1959.59	13/2+		767.4 1	D+Q	+2.0 +5-10

Q(β-)=-2013 keV 4	S(n)= 7415.94 keV 11	S(p)= 8285.5 keV 14	Q(α)= -4451.2 keV 10
Reference: 2021WA16

References:
A	⁷¹Ge IT decay (20.22 MS)	B	⁷¹As ε decay (65.30 H)
C	⁶⁸Zn(α,nγ)	D	⁷⁰Ge(n,γ) E=TH
E	⁷⁰Ge(n,n),(n,γ):Resonances	F	⁷⁰Ge(d,p),(pol d,p)
G	⁷¹Ga(p,n)	H	⁷¹Ga(p,nγ)
I	⁷¹Ga(³He,t),(³He,tγ)	J	⁷¹Ga(⁶Li,⁶He)
K	⁷²Ge(p,d)	L	⁷³Ge(p,t)
M	⁷⁴Ge(α,α3nγ)	N	⁷⁶Se(μ^-,4NPG)

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - Band based on 198, 9/2⁺,α=+1/2
198.371 12	9/2+	20.22 ms 12 % IT = 100
1172.54 10	13/2+	< 0.104 ps	974.15 10	100	E2	198.371	9/2+
2298.96 17	17/2+		1126.45 15	100	E2	1172.54	13/2+
3593.07 20	21/2+		1294.1 1	100	E2	2298.96	17/2+
5009.4 4	25/2+		1416.3 3	100	Q	3593.07	21/2+
6639.7 7	29/2+		1630.3 6	100	Q	5009.4	25/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - Band based on 11/2⁺,α=-1/2
1192.23 9	11/2+	< 0.108 ps
2313.97 19	15/2+		1121.7 2 1141.2 6	100 12 9.0 15	E2 D+Q	1192.23 1172.54	11/2+ 13/2+
3599.6 4	19/2+		1285.6 3	100	Q	2313.97	15/2+
4914.8 7	23/2+		1315.2 6	100	Q	3599.6	19/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - Band based on 3/2-,α=-1/2.
499.915 8	3/2-
1096.07 10	7/2-		349.0 6 596.1 5 921.1 1	6.1 10 21 4 100 6	D (E2) M1	747.248 499.915 174.954	5/2- 3/2- 5/2-
1949.29 13	11/2-		527.2 6 853.2 1	9.7 17 100 14	D E2	1422.04 1096.07	9/2- 7/2-
2890.3 3	15/2-		541.1 6 941.0 3	12.5 21 100 12	D E2	2348.96 1949.29	13/2- 11/2-
3757.3 6	(19/2-)		867.0			2890.3	15/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - Band based on 5/2-,α=+1/2.
747.248 8	5/2-
1422.04 9	9/2-	< 1.2 ps	326.1 6 675.0 2 1247.0 1	3.9 6 18.6 28 100 4	(M1) E2 E2	1096.07 747.248 174.954	7/2- 5/2- 5/2-
2348.96 12	13/2-		399.4 6 926.9 1	3.8 8 100 13	D E2	1949.29 1422.04	11/2- 9/2-
3325.2 4	17/2-		976.2 3	100	E2	2348.96	13/2-
4363.1 6	(21/2-)		1037.9?			3325.2	17/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - Band based on 7/2⁺,α=-1/2
589.775 12	7/2+
1477.03 7	11/2+	< 0.64 ps	887.4 1 1278.5 1	87 6 100 9	E2 M1+E2	589.775 198.371	7/2+ 9/2+
2699.0 6	(15/2+)		1222.0 6	100	(Q)	1477.03	11/2+
4014.0 8	(19/2+)		1314.9?			2699.0	(15/2+)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 6 - Band based on 1038, 9/2⁺,α=+1/2
1037.83 7	9/2+
1959.59 12	13/2+		482.6 6 767.4 1 786.8 3 921.8 6 1760.9 6	74 10 100 17 71 10 26 5 36 7	D D+Q D+Q Q Q	1477.03 1192.23 1172.54 1037.83 198.371	11/2+ 11/2+ 13/2+ 9/2+ 9/2+
3097.49 17	17/2+		783.4 3 798.8 6 1138.1 3 1924.5 6	100 12 11.4 23 100 11 3.0 8	M1 D E2	2313.97 2298.96 1959.59 1172.54	15/2+ 17/2+ 13/2+ 13/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 7 - Octupole band based on 15/2-,α=-1/2
2837.20 20	15/2-
3411.59 18	19/2-		139.1 6 314.1 1 521.1 6 574.4 3 1113.1 6	6.0 12 100 16 19 4 56 8 18.0 30	(D) E1 (Q) E2 D	3272.39 3097.49 2890.3 2837.20 2298.96	17/2- 17/2+ 15/2- 15/2- 17/2+
4472.8 5	23/2-		373.9 6 1061.3 6	100 15 38 10	D Q	4098.71 3411.59	21/2- 19/2-
5727.2 6	27/2-		453.0 6 1254.4 6	54 11 100 28	D Q	5274.3 4472.8	25/2- 23/2-
7114.0 9	31/2-		1386.8 6	100	Q	5727.2	27/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 8 - Octupole band based on 17/2-,α=+1/2
3272.39 15	17/2-
4098.71 25	21/2-		687.2 3 826.2 3	62 5 100 11	M1 E2	3411.59 3272.39	19/2- 17/2-
5274.3 6	25/2-		1175.6 6	100	Q	4098.71	21/2-

E(level)	J^π(level)	T_1/2(level)	Comments
174.954	5/2-	81 ns 3	μ=+1.018 10 (1968Mo12,2020StZV), Q=0.18 4 (1973HaVW,2016St14,2021StZZ) Q(175 level)/Q(⁶⁹Ge,398)=0.22 3 (1973HaVW).
198.371	9/2+	20.22 ms 12 % IT = 100	μ=-1.039 2 (1970Be29,2020StZV), Q=0.34 5 (1975Ri03,2016St14,2021StZZ) E(level): Band based on 198, 9/2⁺,α=+1/2.
499.915	3/2-		E(level): Band based on 3/2-,α=-1/2.
589.775	7/2+		E(level): Poor fit; uncertainty increased in the fitting procedure. Band based on 7/2⁺,α=-1/2.
747.248	5/2-		E(level): Band based on 5/2-,α=+1/2.
1037.83	9/2+		E(level): Band based on 1038, 9/2⁺,α=+1/2.
1096.07	7/2-		E(level): Band based on 3/2-,α=-1/2.
1171	5/2+		XREF: K(1166).
1172.54	13/2+	< 0.104 ps	E(level): Band based on 198, 9/2⁺,α=+1/2. T_1/2(level): From (α,nγ) with DSAM; should be considered an upper limit since no feeding corrections have been made.
1192.23	11/2+	< 0.108 ps	XREF: B(?). E(level): Band based on 11/2⁺,α=-1/2. T_1/2(level): From (α,nγ) with DSAM; should be considered an upper limit since no feeding corrections have been made.
1212.511	5/2-	> 1.2 ps	XREF: K(1207).
1378.53	(1/2-)		XREF: B(?).
1378.71	5/2-		XREF: H(?).
1406.640	7/2-		XREF: F(1401).
1422.04	9/2-	< 1.2 ps	E(level): Band based on 5/2-,α=+1/2. T_1/2(level): From (α,nγ) with DSAM; should be considered an upper limit since no feeding corrections have been made.
1475.9	(5/2-)		XREF: d(?).
1477.03	11/2+	< 0.64 ps	E(level): Poor fit; uncertainty increased in the fitting procedure. Band based on 7/2⁺,α=-1/2. T_1/2(level): From (α,nγ) with DSAM; should be considered an upper limit since no feeding corrections have been made.
1743.385	3/2-	0.42 ps 15	XREF: F(1751).
1949.29	11/2-		E(level): Band based on 3/2-,α=-1/2.
1959.59	13/2+		E(level): Band based on 1038, 9/2⁺,α=+1/2.
2075.7	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
2141.2	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
2146.15	(3/2-)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available.
2257.00	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
2298.96	17/2+		E(level): Band based on 198, 9/2⁺,α=+1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
2313.97	15/2+		E(level): Band based on 11/2⁺,α=-1/2.
2348.96	13/2-		E(level): Band based on 5/2-,α=+1/2.
2351.60	1/2-,3/2-		XREF: K(2348).
2426.8	1/2,3/2,5/2+		J^π(level): Primary γ from 1/2⁺ in (n,γ) E=th.
2462.35	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
2486	1/2+		XREF: K(2487).
2515.3	1/2,3/2,5/2+		J^π(level): Primary γ from 1/2⁺ in (n,γ) E=th.
2518.5	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
2533.97	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
2642	5/2+		XREF: F(2644).
2675.8	1/2-,3/2-		XREF: F(2669).
2699.0	(15/2+)		E(level): Poor fit; uncertainty increased in the fitting procedure. Band based on 7/2⁺,α=-1/2.
2806	(5/2-)		XREF: F(2802).
2837.20	15/2-		E(level): Octupole band based on 15/2-,α=-1/2.
2890.3	15/2-		E(level): Band based on 3/2-,α=-1/2.
2924	(5/2-)		XREF: F(2922).
2952.0	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3024.9	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3097.49	17/2+		E(level): Band based on 1038, 9/2⁺,α=+1/2.
3102			XREF: K(3100).
3157.6	(1/2,3/2)		XREF: F(3161). J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3208.5	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3214.1	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3223.9	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3272.39	17/2-		E(level): Octupole band based on 17/2-,α=+1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
3286	(1/2-)		XREF: K(3287).
3325.2	17/2-		E(level): Band based on 5/2-,α=+1/2.
3339.5	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3375			See comment for 3365 level.
3404.6	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3407.5	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3411.59	19/2-		E(level): Octupole band based on 15/2-,α=-1/2.
3462.9	(1/2,3/2)		E(level): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available. J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3593.07	21/2+		E(level): Band based on 198, 9/2⁺,α=+1/2.
3599.6	19/2+		E(level): Band based on 11/2⁺,α=-1/2.
3757.3	(19/2-)		E(level): Band based on 3/2-,α=-1/2.
3866.0	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
3960	1/2+		XREF: K(1961).
4014.0	(19/2+)		E(level): Poor fit; uncertainty increased in the fitting procedure. Band based on 7/2⁺,α=-1/2.
4098.71	21/2-		E(level): Octupole band based on 17/2-,α=+1/2.
4226.5	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
4306.8	(1/2,3/2)		J^π(level): Possible γ to 1/2-, possible primary γ from 1/2⁺.
4363.1	(21/2-)		E(level): Band based on 5/2-,α=+1/2.
4472.8	23/2-		E(level): Octupole band based on 15/2-,α=-1/2.
4914.8	23/2+		E(level): Band based on 11/2⁺,α=-1/2.
5009.4	25/2+		E(level): Band based on 198, 9/2⁺,α=+1/2.
5274.3	25/2-		E(level): Octupole band based on 17/2-,α=+1/2.
5727.2	27/2-		E(level): Octupole band based on 15/2-,α=-1/2.
6639.7	29/2+		E(level): Band based on 198, 9/2⁺,α=+1/2.
7114.0	31/2-		E(level): Octupole band based on 15/2-,α=-1/2.
E(level)	J^π(level)	T_1/2(level)	Comments
7417.03	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7417.39	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7417.85	(1/2-,3/2-)		J^π(level): From assignment of p-wave (L=(1)) resonance in (n,n),(n,γ):resonances.
7419.05	(1/2-,3/2-)		J^π(level): From assignment of p-wave (L=(1)) resonance in (n,n),(n,γ):resonances.
7420.11	(1/2-,3/2-)		J^π(level): From assignment of p-wave (L=(1)) resonance in (n,n),(n,γ):resonances.
7420.28	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7421.46	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7422.64	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7424.52	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7425.76	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7426.16	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7426.83	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7427.63	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7429.04	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7434.28	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7439.67	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7441.60	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7443.44	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
7444.66	1/2+		J^π(level): From assignment of s-wave (L=0) resonance in (n,n),(n,γ):resonances.
8913	3/2-	% n ≈ 100	53% 9 decay proceeds through neutron decay to 1.22 MeV state in ⁷⁰Ge with subsequent observation of 1040γ in ⁷⁰Ge. E(level): 53% 9 decay proceeds through neutron decay to 1.22 MeV state in ⁷⁰Ge with subsequent observation of 1040γ in ⁷⁰Ge.
11.75E3			Gamow-Teller giant resonance (GTGR), wide structure from 10-16 MeV, peaking at ≈11.75 MeV (2015Fr02,2011Fr15).
18.0E3			Interpreted as T_> component of the GTGR (2015Fr02,2011Fr15).

E(level)	E(gamma)	Comments
174.954	174.956	E(γ): weighted average of 174.954 5 from ⁷¹As ε decay, 174.9 1 from (α,nγ), 175.05 3 from (n,γ) E=th, and 174.9 1 from (p,nγ) and (α,α3nγ)
499.915	499.94	E(γ): unweighted average of 499.876 10 from ⁷¹As ε decay, 500.0 1 from (α,nγ), 499.966 22 from (n,γ) E=th, and 499.9 1 from (p,nγ), 499.9 3 in (α,α3nγ)
525.114	326.798	E(γ): weighted average of 326.785 15 from ⁷¹As ε decay, 326.8 1 from (α,nγ), 326.86 3 from (n,γ) E=th, and 326.7 1 from (p,nγ)
525.114	350.164	E(γ): weighted average of 350.163 6 from ⁷¹As ε decay, 350.0 2 from (α,nγ), 350.26 5 from (n,γ) E=th, and 350.2 1 from (p,nγ) I(γ): weighted average of 12.41 30 from ⁷¹As ε decay, 13.4 6 from (α,nγ), 12.4 11 from (n,γ) E=th, and 11.8 7 from (p,nγ)
589.775	391.396	E(γ): weighted average of 391.383 18 from ⁷¹As ε decay, 391.4 1 from (α,nγ), 391.45 3 from (n,γ) E=th, 391.2 1 from (p,nγ), 391.3 1 in (α,α3nγ)
589.775	414.55	E(γ): unweighted average of 414.39 10 from ⁷¹As ε decay and 414.7 1 from (p,nγ) I(γ): other: 4.9 5 from (p,nγ) is in disagreement; this γ not reported in (n,γ) and (α,nγ)
708.196	533.2	E(γ): from (p,nγ). Others: 533.2 2 from ⁷¹As ε decay and 533.18 20 from (n,γ) E=th I(γ): unweighted average of 7.0 7 from ⁷¹As ε decay, 4.7 8 from (α,nγ), 4.0 7 from (n,γ) E=th, and 2.90 20 from (p,nγ)
708.196	708.193	E(γ): weighted average of 708.195 5 from ⁷¹As ε decay, 708.0 1 from (α,nγ), 708.14 3 from (n,γ) E=th, and 708.1 1 from (p,nγ) I(γ): from (p,nγ). Others: 100.0 31 from ⁷¹As ε decay, 100.0 8 from (α,nγ), and 100 7 from (n,γ) E=th
747.248	247.352	E(γ): poor fit, energy uncertainty increased three times to 0.015 keV in the fitting procedure. weighted average of 247.351 5 from ⁷¹As ε decay, 247.5 3 from (α,nγ), 247.40 4 from (n,γ) E=th, 247.3 1 from (p,nγ), and 247.3 6 in (α,α3nγ). Poor fit; uncertainty increased in the fitting procedure I(γ): weighted average of 73.8 19 from ⁷¹As ε decay, 75.0 30 from (α,nγ), 84 7 from (n,γ) E=th, and 85 5 from (p,nγ). Other: 117 20 in (α,α3nγ)
	572.259	E(γ): weighted average of 572.255 15 from ⁷¹As ε decay, 572.29 5 from (n,γ) E=th, and 572.3 1 from (p,nγ). Other: 572.3 3 from (α,nγ), 572.1 6 in (α,α3nγ) I(γ): others: 100 4 from (α,nγ), 100 9 from (n,γ) E=th, 100 4 from (p,nγ), and 100 17 in (α,α3nγ)
	747.272	E(γ): unweighted average of 747.28 1 from ⁷¹As ε decay, 747.3 3 from (α,nγ), 747.09 5 from (n,γ) E=th, and 747.2 1 from (p,nγ). Other: 747.3 6 in (α,α3nγ) I(γ): unweighted average of 61.7 19 from ⁷¹As ε decay, 49 5 from (α,nγ), 58 5 from (n,γ) E=th, and 53.0 20 from (p,nγ). Other: 60 12 in (α,α3nγ) M(γ): δ(O/Q)=-0.14 +14-22 or -1.9 +7-9 (p,nγ); ΔJ=2, Q from (α,α,3nγ); E2 from level scheme
808.196	308.25	E(γ): weighted average of 308.24 4 from ⁷¹As ε decay, 308.29 5 from (n,γ) E=th, and 308.2 1 from (p,nγ). Other: 307.9 5 from (α,nγ). Multiply placed with intensity suitably divided I(γ): unweighted average of 39 6 from ⁷¹As ε decay, 75 3 from (α,nγ), 34 3 from (n,γ) E=th, and 82 4 from (p,nγ). Multiply placed with intensity suitably divided
	633.2	E(γ): from (p,nγ). Eγ=633.440 25 from ⁷¹As decay is not used since its intensity of 161 20 is in severe disagreement from those in (p,nγ) and (α,nγ). This γ not reported in (n,γ) I(γ): weighted average of 54.0 30 from (α,nγ) and 48.0 20 from (p,nγ). Other: 161 20 from ⁷¹As ε decay is in severe disagreement
	808.21	E(γ): weighted average of 808.27 3 from ⁷¹As ε decay, 807.8 4 from (α,nγ), 808.13 4 from (n,γ) E=th, and 808.1 1 from (p,nγ) I(γ): from (p,nγ). Others: 100 8 from ⁷¹As ε decay, 100 4 from (α,nγ), and 100 9 from (n,γ) E=th
831.301	241.77	E(γ): weighted average of 241.75 13 from (n,γ) E=th and 241.8 2 from (p,nγ) I(γ): weighted average of 2.3 3 from (α,nγ), 4.8 9 from (n,γ) E=th, and 2.5 3 from (p,nγ)
	306.210	E(γ): weighted average of 306.217 25 from ⁷¹As ε decay, 306.21 4 from (n,γ) E=th, and 306.1 1 from (p,nγ). Other: 306.2 5 from (α,nγ) I(γ): weighted average of 29 4 from ⁷¹As ε decay, 28.5 18 from (α,nγ), 29.4 24 from (n,γ) E=th, and 28.5 19 from (p,nγ)
	331.42	E(γ): weighted average of 331.4 2 from ⁷¹As ε decay, 331.4 3 from (α,nγ), 331.45 4 from (n,γ) E=th, and 331.2 1 from (p,nγ) I(γ): weighted average of 20.1 15 from (α,nγ), 23.9 21 from (n,γ) E=th, and 25.0 22 from (p,nγ). Other: 19 10 from ⁷¹As ε decay
	831.293	E(γ): weighted average of 831.294 10 from ⁷¹As ε decay, 831.3 3 from (α,nγ), 831.29 3 from (n,γ) E=th, and 831.2 1 from (p,nγ) I(γ): from (α,nγ). Others: 100 3 from ⁷¹As ε decay, 100 8 from (n,γ) E=th, and 100.0 22 from (p,nγ)
1026.561	279.379	E(γ): poor fit, energy uncertainty increased four times to 0.028 keV in the fitting procedure. others: 279.61 22 from (n,γ) E=th and 279.2 2 from (p,nγ). Poor fit; uncertainty increased in the fitting procedure I(γ): weighted average of 21.6 8 from ⁷¹As ε decay, 12 5 from (n,γ) E=th, and 22.5 14 from (p,nγ)
	501.5	E(γ): from (n,γ) E=th only; treated as questionable by the evaluators due to no intensity reported and γ not seen in other studies
	526.642	E(γ): poor fit, energy uncertainty increased two times to 0.008 keV in the fitting procedure. weighted average of 526.642 3 from ⁷¹As ε decay, 526.4 3 from (α,nγ), 526.77 6 from (n,γ) E=th, and 526.7 1 from (p,nγ). Poor fit; uncertainty increased in the fitting procedure I(γ): others: 100 4 from (α,nγ), 100 7 from (n,γ) E=th, and 100.0 22 from (p,nγ)
	828.0	E(γ): γ treated as questionable by the evaluators
	851.63	E(γ): weighted average of 851.63 7 from ⁷¹As ε decay and 851.6 2 from (p,nγ). Other: 850.98 10 is discrepant I(γ): weighted average of 21.0 20 from ⁷¹As ε decay, 27 4 from (α,nγ), and 23.4 11 from (p,nγ). Other: 87 11 from (n,γ) E=th is discrepant
	1026.510	E(γ): poor fit, energy uncertainty increased four times to 0.034 keV in the fitting procedure. others: 1026.6 3 from (α,nγ), 1026.73 23 from (n,γ) E=th, and 1026.5 2 from (p,nγ). Poor fit; uncertainty increased in the fitting procedure I(γ): weighted average of 36.2 12 from ⁷¹As ε decay, 34 4 from (α,nγ), and 35.3 14 from (p,nγ). Other: 29 9 from (n,γ) E=th M(γ): from γ(θ,t) in ε decay and RUL
1037.83	448.1	E(γ): weighted average of 448.1 1 from (α,nγ), 448.0 2 from (p,nγ), and 447.9 3 in (α,α3nγ). Other: 448.52 10 in ε decay not used in averaging due to Iγ=286 143 in severe disagreement with others I(γ): unweighted average of 45 3 from (α,nγ), 34.8 19 from (p,nγ), and 51 8 in (α,α3nγ). Other: 286 143 from ⁷¹As ε decay is in severe disagreement M(γ): D+Q from γ(θ) in (p,nγ) and (α,nγ); M1⁺E2 from γ(lin pol) in (α,α,3nγ)
1037.83	839.4	E(γ): weighted average of 839.3 3 from ⁷¹As ε decay, 839.5 1 from (α,nγ), 839.2 2 from (p,nγ), and 839.0 3 in (α,α3nγ) I(γ): from (p,nγ). Other: 100 3 from (α,nγ), 100 43 from ⁷¹As ε decay, 100 19 in (α,α3nγ)
E(level)	E(gamma)	Comments
1095.511	348.27	I(γ): 0.96 is also possible since 1990Me01 list two different values of relative intensity differing by ≈20%
	920.553	E(γ): other: 920.49 14 from (n,γ) E=th I(γ): unweighted average of 7.4 3 from ⁷¹As ε decay and 12.1 16 from (n,γ) E=th
	1095.486	E(γ): weighted average of 1095.490 10 from ⁷¹As ε decay, 1096.1 5 from (α,nγ), 1095.42 4 from (n,γ) E=th, and 1095.5 2 from (p,nγ) I(γ): others: 100 13 from (α,nγ) and 100 8 from (n,γ) E=th
1096.07	596.1	E(γ): weighted average of 596.1 5 from (p,nγ), and 596.2 6 in (α,α3nγ). 596.2 3 in (α,nγ) not used. I(γ): weighted average of 20.8 36 from (α,α3nγ), and 20 6 in (p,nγ). Other: 104 9 in (α,nγ) in severe disagreement M(γ): ΔJ=2, Q from γγ(θ)(ADO) in (α,α3nγ). Others: γ(θ) in (p,nγ) with δ(O/Q)=+0.05 +26-24 or -4.7 to +3.5; E2 from level scheme
1096.07	921.1	E(γ): weighted average of 921.1 2 from ⁷¹As ε decay, 921.4 3 from (α,nγ), 921.1 2 from (p,nγ), and 921.2 1 in (α,α3nγ) I(γ): from (p,nγ). Others: 100 13 in (α,α3nγ); 100 8 in (α,nγ) M(γ): from γγ(θ)(ADO) and γ(lin pol) in (α,α3nγ). Others: D+Q, δ=-2.0 4 from γ(θ) in (α,nγ); δ(Q/d)=-0.10 7 or -3.0 4; -0.23 +7-8 or -2.0 +3-4 from γ(θ) in (p,nγ)
1139.441	308.24	E(γ): Multiply placed with intensity suitably divided I(γ): Multiply placed with intensity suitably divided
	331.48	E(γ): poor fit, energy uncertainty increased four times to 0.16 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
	431.279	E(γ): other: 431.0 3 from (p,nγ) I(γ): weighted average of 2.56 11 from ⁷¹As ε decay and 2.40 20 from (p,nγ)
	639.477	E(γ): poor fit, energy uncertainty increased two times to 0.028 keV in the fitting procedure. others: 639.4 2 from (n,γ) E=th and 639.5 2 from (p,nγ). Poor fit; uncertainty increased in the fitting procedure I(γ): weighted average of 6.1 3 from ⁷¹As ε decay, 8.6 24 from (α,nγ), and 6.3 7 from (p,nγ). Other: 13.9 17 from (n,γ) E=th is discrepant
	964.479	E(γ): other: 964.3 2 from (p,nγ) I(γ): unweighted average of 8.5 3 from ⁷¹As ε decay, 12 3 from (α,nγ), and 12.5 7 from (p,nγ)
	1139.41	E(γ): unweighted average of 1139.461 19 from ⁷¹As ε decay, 1139.4 5 from (α,nγ), 1139.19 4 from (n,γ) E=th, and 1139.3 2 from (p,nγ) I(γ): from (p,nγ). Others: 100.0 21 from ⁷¹As ε decay, 100 4 from (α,nγ), and 100 8 from (n,γ) E=th
1172.54	974.15	E(γ): average of 974.1 1 in (α,α3nγ) and 974.2 1 in (α,nγ) M(γ): γγ(θ)(ADO) and γ(lin pol) in (α,α,3ng); δ(M3/E2)=-0.01 2, ΔJ=2 from γ(lin pol) in (α,nγ)
1192.23	993.9	E(γ): from (α,nγ) M(γ): from γγ(θ)(ADO) and γ(pol) in (α,α3nγ); γ(θ,pol) in (α,nγ)
1205.146	373.837	E(γ): others: 373.8 3 from (α,nγ), 373.91 16 from (n,γ) E=th, and 373.7 3 from (p,nγ) I(γ): weighted average of 16.2 6 from ⁷¹As ε decay, 20 4 from (α,nγ), 19 5 from (n,γ) E=th, and 24 8 from (p,nγ)
	615.365	E(γ): others: 615.5 2 from (α,nγ), 615.33 7 from (n,γ) E=th, and 615.4 2 from (p,nγ) I(γ): others: 100 6 from (α,nγ), 100 9 from (n,γ) E=th, and 100 6 from (p,nγ)
	680.035	E(γ): other: 680.0 2 from (p,nγ) I(γ): weighted average of 18.4 9 from ⁷¹As ε decay, 13 4 from (α,nγ), and 14.4 17 from (p,nγ)
1212.511	465.228	E(γ): poor fit, energy uncertainty increased two times to 0.020 keV in the fitting procedure. other: 465.2 2 from (p,nγ). Poor fit; uncertainty increased in the fitting procedure I(γ): weighted average of 28.8 8 from ⁷¹As ε decay, 25 8 from (α,nγ), and 26.3 19 from (p,nγ)
	504.27	E(γ): weighted average of 504.28 5 from ⁷¹As ε decay and 504.1 2 from (p,nγ) I(γ): weighted average of 53 15 from ⁷¹As ε decay, 42 17 from (α,nγ), and 47 14 from (p,nγ)
	712.598	E(γ): others: 712.2 5 from (α,nγ) and 712.7 2 from (p,nγ) I(γ): others: 100 14 (α,nγ) and 100 8 from (p,nγ)
	1037.530	E(γ): others: 1037.0 10 from (α,nγ) and 1037.7 3 from (p,nγ) I(γ): weighted average of 62.1 15 from ⁷¹As ε decay, 64 14 from (α,nγ), and 70 7 from (p,nγ)
	1212.500	E(γ): others: 1212.3 5 from (α,nγ) and 1212.5 2 from (p,nγ) I(γ): weighted average of 85.6 23 from ⁷¹As ε decay and 82 3 from (p,nγ). Other: 137 15 from (α,nγ) is discrepant M(γ): ΔJ=2, quadrupole from γ(θ,t) in ε decay; δ(O/Q)=-0.12 +19-24 or -1.9 +7-12 from γ(θ) in (p,nγ); E2 from level scheme
1288.55	580.16	E(γ): weighted average of 580.10 8 from (n,γ) E=th and 580.5 2 from (p,nγ) I(γ): from (p,nγ). Other: 53 7 from (n,γ) E=th is discrepant, considering I(580γ)/I(789γ)=0.15 2 from another work (2002Ka51) in (p,nγ)
1288.55	788.66	E(γ): from (n,γ) E=th. Others: 788.5 3 from (α,nγ) and 788.7 2 from (p,nγ) I(γ): from (p,nγ). Other: 100 10 from (n,γ) E=th
1298.75	798.4	E(γ): weighted average of 797.6 4 from (α,nγ), 798.3 2 from (n,γ) E=th, and 798.9 3 from (p,nγ). γ not reported in ⁷¹As decay. I(γ): unweighted average of 14.1 20 from (n,γ)E=th and 9.4 9 from (p,nγ). Other: 36 11 from (α,nγ) is in severe disagreement
1298.75	1298.50	E(γ): unweighted average of 1298.729 15 from ⁷¹As ε decay, 1298.0 3 from (α,nγ), 1298.56 5 from (n,γ) E=th, and 1298.7 2 from (p,nγ) I(γ): from (p,nγ). Others: 100 3 from ⁷¹As ε decay, 100 16 from (α,nγ), and 100 7 from (n,γ) E=th
E(level)	E(gamma)	Comments
1378.53	1203.7	E(γ): unweighted average of 1202.5 5 from (α,nγ), 1204.5 2 from (n,γ) E=th, and 1204.2 10 from (p,nγ). Other: tentative 1202.26 5 from ⁷¹As ε decay I(γ): from (α,nγ). Others: Iγ(1378)/Iγ(1204)=100 9/23 5 in (n,γ); 61 28/100 50 in ⁷¹As decay
1378.53	1378.65	E(γ): weighted average of 1379.0 5 from ⁷¹As ε decay, 1377.3 6 from (α,nγ), 1378.66 7 from (n,γ) E=th, and 1378.7 10 from (p,nγ) I(γ): from (α,nγ). Others: Iγ(1378)/Iγ(1204)=100 9/23 5 in (n,γ); 61 28/100 50 in ⁷¹As decay
1378.71	281.8	E(γ): from (p,nγ) only, Iγ(282)/Iγ(632)=100/84
1378.71	631.52	E(γ): other: 630.8 1 from (p,nγ)
1406.640	1406.5	E(γ): could be a sum line.
1416.22	1415.9	E(γ): weighted average of 1416.00 21 from (n,γ) E=th and 1414.5 10 from (p,nγ) I(γ): from (n,γ) E=th.
1422.04	326.1	M(γ): ΔJ=1, dipole from (α,α3nγ), (M1) from level scheme
	675.0	E(γ): weighted average of 675.0 2 in (p,nγ), 675.1 3 from (α,nγ), and 674.9 3 in (α,α3nγ) I(γ): weighted average of 23 3 from (α,nγ), 26 5 from (p,nγ), 15.7 19 in (α,α3nγ)
	1247.0	E(γ): weighted average of 1247.1 1 in (p,nγ), 1247.3 3 in (α,nγ), and 1247.0 1 in (α,α3nγ), 1247.0 1 in ε decay I(γ): from (p,nγ). Others: 100 6 in (α,nγ), 100 12 in (α,α3nγ) M(γ): γγ(θ)(ADO) and γ(pol) in (α,α3nγ); γ(θ,pol) in (α,nγ).
1454.3	646.1	E(γ): from (p,nγ) only
1475.9	886.0	E(γ): weighted average of 885.97 17 from (n,γ) E=th and 887.6 10 from (p,nγ). It is possible that this γ is the same as 887.4 from 1479, 11/2⁺ level.
1477.03	887.4	E(γ): weighted average of 887.4 1 in (α,nγ), 887.0 3 in (α,α3nγ) I(γ): weighted average of 86 6 in (α,nγ), 98 18 in (α,α3nγ) M(γ): ΔJ=2, Q+O with δ=0.07 5 from γ(θ) in (α,nγ); γγ(θ)(ADO) and γ(pol) in (α,α3nγ)
1477.03	1278.5	E(γ): weighted average of 1278.5 1 in (α,nγ), 1278.1 3 in (α,α3nγ) I(γ): from (α,nγ). Other: 100 17 in (α,α3nγ) M(γ): D+Q with δ=+4.8 10 from γ(θ) in (α,nγ); ΔJ=1, dipole from γγ(θ)(ADO) in (α,α3nγ); M1⁺E2 from RUL
1506.388	674.33	E(γ): poor fit, energy uncertainty increased five times to 0.40 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
1506.388	1331.526	E(γ): poor fit, energy uncertainty increased two times to 0.046 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
1542.48	1542.3	E(γ): weighted average of 1542.2 8 from (n,γ) E=th and 1542.9 20 from (p,nγ) I(γ): from (p,nγ)
1558.757	727.531	E(γ): poor fit, energy uncertainty increased two times to 0.044 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
	1033.55	E(γ): poor fit, energy uncertainty increased two times to 0.06 keV in the fitting procedure. weighted average of 1033.542 17 from ⁷¹As ε decay, 1034.2 2 from (α,nγ), 1033.7 3 from (n,γ) E=th, and 1033.7 10 from (p,nγ). Poor fit; uncertainty increased in the fitting procedure
	1058.817	E(γ): other: 1058.8 20 with Iγ=10 from (p,nγ)
1566.2	976.4	E(γ): weighted average of 976.3 6 from (α,nγ) and 976.5 10 from (p,nγ)
1566.2	1041.0	E(γ): reported in (α,nγ) only
1598.534	1098.58	E(γ): weighted average of 1098.64 7 from ⁷¹As ε decay and 1098.54 6 from (n,γ) E=th. Other: 1098.5 5 from (α,nγ) I(γ): other: 100 9 from (n,γ) E=th
	1423.579	E(γ): others: 1423.59 21 from (n,γ) E=th and 1424.1 20 from (p,nγ) I(γ): other: 21 5 from (n,γ) E=th
	1598.50	E(γ): weighted average of 1598.505 25 from ⁷¹As ε decay, 1598.22 18 from (n,γ) E=th, and 1599.0 20 from (p,nγ) I(γ): weighted average of 28.9 15 from ⁷¹As ε decay and 27 4 from (n,γ) E=th
1629.179	881.893	E(γ): other: 882.1 20 from (p,nγ)
	1104.162	E(γ): poor fit, energy uncertainty increased two times to 0.052 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
	1629.154	E(γ): other: 1629.6 10 from (p,nγ)
E(level)	E(gamma)	Comments
1698.3	867.4	E(γ): tentative γ from (p,nγ) only
1698.3	1108.5	E(γ): from (α,nγ)
1743.385	935.178	E(γ): weighted average of 935.175 14 from ⁷¹As ε decay, 935.38 11 from (n,γ) E=th, and 935.2 10 from (p,nγ) I(γ): other: 156 20 from (n,γ) E=th is discrepant
	996.06	I(γ): weighted average of 32 3 from ⁷¹As ε decay and 36 7 from (p,nγ)
	1743.40	E(γ): others: 1743.2 6 from (n,γ) E=th and 1743.7 10 from (p,nγ) I(γ): other: 100 34 from (n,γ) E=th M(γ): D+Q from γ(θ) in (p,nγ); M1⁺E2 from level scheme
1792.096	444.8	E(γ): reported as tentative in (n,γ) only with an intensity six times that of a 1618γ (presumably the same as 1617.1γ given here). α line with this intensity should have been seen in ε decay. It is possible that 444.8γ defines another level near 1792 keV
	765.89	E(γ): poor fit, energy uncertainty increased three times to 0.21 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
	983.67	E(γ): poor fit, energy uncertainty increased three times to 0.15 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
	1617.12	E(γ): weighted average of 1617.12 3 from ⁷¹As ε decay, 1618.0 5 from (n,γ) E=th, and 1617.4 20 from (p,nγ)
1835.81	457.28	E(γ): from (n,γ) E=th
1937.45	1347.7	I(γ): 36 22 is also possible since in ε decay, values listed in table I and level-scheme figure 1 of 1990Me01 differ by a factor of 10.
1949.29	853.2	E(γ): from (α,α3nγ). Other: 853.1 3 from (α,nγ) M(γ): γγ(θ)(ADO) and γ(pol) in (α,α3nγ)
1959.59	767.4	E(γ): weighted average of 767.4 1 in (α,nγ), 767.1 3 in (α,α3nγ) I(γ): from (α,α3nγ). Other: 100 13 in (α,nγ) M(γ): from γ(θ) in (α,nγ), and γγ(θ)(ADO) in (α,α3nγ)
1959.59	786.8	E(γ): weighted average of 786.8 3 in (α,nγ), 786.9 6 in (α,α3nγ) I(γ): from (α,α3nγ). Other: 139 26 in (α,nγ) for an uncertain γ M(γ): γγ(θ)(ADO) in (α,α3nγ)
1965.03	1965.04	E(γ): others: 1965.01 11 from (n,γ) E=th and 1965.4 20 from (p,nγ)
2031.89	2032.74	E(γ): from (n,γ) E=th.. poor fit, energy uncertainty increased two times to 0.44 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure
2075.7	2075.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2141.2	2141.3	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2146.15	2146.25	E(γ): from (n,γ) E=th
2224.50	2223.7	E(γ): from (n,γ) E=th
2257.00	2257.3	E(γ): from (n,γ) E=th
2298.96	1126.45	E(γ): average of 1126.6 1 in (α,nγ), 1126.3 1 in (α,α3nγ) M(γ): γγ(θ)(ADO) and γ(lin pol) in (α,α3nγ); γ(θ) in (α,nγ) with δ(O/Q)=0.00 7
2313.97	1121.7	E(γ): weighted average of 1122.0 2 in (α,nγ) and 1121.6 1 in (α,α3nγ) I(γ): from (α,α3nγ). Other: 100 14 in (α,nγ) M(γ): γγ(θ)(ADO) and γ(pol) in (α,α3nγ); γ(θ) with δ(O/Q)=-0.06 5 in (α,nγ)
2313.97	1141.2	E(γ): weighted average of 1141.0 10 in (α,nγ) and 1141.3 6 in (α,α3nγ) I(γ): from (α,α3nγ). Other: 70 30 in (α,nγ) M(γ): γγ(θ)(ADO) in (α,α3nγ)
2348.96	926.9	E(γ): weighted average of 926.8 3 in (α,nγ) and 926.9 1 in (α,α3nγ) I(γ): from (α,α3nγ) M(γ): γγ(θ)(ADO) and γ(pol) in (α,α3nγ); γ(θ) in (α,nγ) with δ(O/Q)=0.00 5
E(level)	E(gamma)	Comments
2351.60	2351.41	E(γ): from (n,γ) E=th
2364.1	2364.2	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2462.35	2462.25	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2518.5	2518.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2533.97	2534.3	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2675.8	2675.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2868.3	2867.6	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
2952.0	2953.4	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3024.9	3025.6	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3075.2	3078.2	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3157.6	3157.7	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3183.5	3183.6	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3208.5	3208.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3214.1	3214.1	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3223.9	3223.9	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3339.5	3338.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3382.1	3381.0	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3404.6	3404.6	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3407.5	3407.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3462.9	3462.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3481.7	3481.7	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3556.1	3555.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3569.9	3569.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3866.0	3865.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
3893.5	3893.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
E(level)	E(gamma)	Comments
4226.5	4226.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
4306.8	4306.7	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
7415.957	3189.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	3522.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	3934.3	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4008.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4011.4	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4192.1	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4201.9	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4207.5	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4232.4	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4258.3	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	4740.1	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	5051.8	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	5274.7	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	5340.2	E(γ): From γγ cascade study of 2004Ho25 in (n,γ) E=th. This γ should be treated as tentative since no intensity data are available. From 2004Ho25 based on γγ-coin cascade data. This level should be treated as tentative since intensities of γ rays associated with the population and decay of this level are not available
	6319.99	E(γ): poor fit, energy uncertainty increased two times to 0.08 keV in the fitting procedure. Poor fit; uncertainty increased in the fitting procedure

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 F G H I J K L M N	1/2-	11.43 d 3 % ε = 100
174.954 6	A B C D F G H I K M	5/2-	81 ns 3	174.956 9	100	E2	0.0	1/2-
198.371 12	A B C D F H K L M N	9/2+	20.22 ms 12 % IT = 100	23.438 15	100	M2	174.954	5/2-
499.915 8	B C D F G H I K L M	3/2-		324.92 6 499.94 3	0.48 11 100.0 20	M1+E2	174.954 0.0	5/2- 1/2-
525.114 8	B C D F G H K L	5/2+		326.798 19 350.164 7	100.0 22 12.50 30	E2 E1+M2	198.371 174.954	9/2+ 5/2-
589.775 12	B C D F G H L M	7/2+		64.7 1 391.396 24 414.55 16	4.7 3 100.0 8 0.54 14	[M1+E2] M1+E2 [E1]	525.114 198.371 174.954	5/2+ 9/2+ 5/2-
620 10	F
708.196 7	B C D F G H I K	3/2-	> 10.7 ps	533.2 1 708.193 8	4.7 9 100.0 21	[M1,E2] M1+E2	174.954 0.0	5/2- 1/2-
747.248 8	B C D F G H K M	5/2-		247.352 5 572.259 15 747.272 21	75.6 21 100.0 21 55.4 28	M1+E2 M1+E2 (E2)	499.915 174.954 0.0	3/2- 5/2- 1/2-
801 3	F K
808.196 19	B C D G H I K	1/2-		308.25 4 633.2 1 808.21 4	58 12 50 3 100 3	(M1+E2)	499.915 174.954 0.0	3/2- 5/2- 1/2-
817 3	F
831.301 8	B C D G H K	3/2-		241.77 13 306.210 25 331.42 5 831.293 10	2.5 4 28.7 18 22.2 16 100.0 19	[M2] (E1+M2) E2(+M1) (M1+E2)	589.775 525.114 499.915 0.0	7/2+ 5/2+ 3/2- 1/2-
886.94 10	B F	(3/2-)		711.6 3 886.98 10	100 25 63 13		174.954 0.0	5/2- 1/2-
970 10	F
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1026.561 10	B C D F G H K	5/2-	> 1.2 ps	195.22 15 279.379 7 501.5 6 ? 526.642 4 828.0 1 ? 851.63 7 1026.510 17	1.0 5 21.6 10 100.0 22 0.4 2 23.1 11 35.7 12	[M1,E2] (M1+E2) (M1+E2) [M2] (M1+E2) (E2)	831.301 747.248 525.114 499.915 198.371 174.954 0.0	3/2- 5/2- 5/2+ 3/2- 9/2+ 5/2- 1/2-
1037.83 7	B C F H L M	9/2+		448.1 1 839.4 1	44 5 100.0 19	M1+E2 (M1(+E2))	589.775 198.371	7/2+ 9/2+
1095.511 7	B C D F G H I K	3/2-	0.62 ps 14	264.21 15 287.32 4 348.27 4 387.31 4 570.42 21 595.6 1 920.553 7 1095.486 12	0.20 10 0.52 6 1.17 18 0.30 4 0.54 4 2.01 20 9.8 24 100.0 24	[M1,E2] [M1,E2] [M1,E2] [M1,E2] [E1] [M1,E2] (M1+E2) (M1+E2)	831.301 808.196 747.248 708.196 525.114 499.915 174.954 0.0	3/2- 1/2- 5/2- 3/2- 5/2+ 3/2- 5/2- 1/2-
1096.07 10	B C G H M	7/2-		349.0 6 596.1 5 921.1 1	6.1 10 21 4 100 6	D (E2) M1	747.248 499.915 174.954	5/2- 3/2- 5/2-
1139.441 9	B C D F G H	3/2-	4.0 ps 14	308.24 4 331.48 4 392.16 5 431.279 23 614.26 5 639.477 14 964.479 9 1139.41 6	1.03 21 2.6 4 4.3 3 2.52 11 1.7 3 6.2 3 11.0 13 100.0 5	(M1+E2) [M1,E2] (M1+E2) [M1,E2] [E1] [M1,E2] (M1+E2) M1+E2	831.301 808.196 747.248 708.196 525.114 499.915 174.954 0.0	3/2- 1/2- 5/2- 3/2- 5/2+ 3/2- 5/2- 1/2-
1154 3	F
1171 3	F K L	5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1172.54 10	C L M	13/2+	< 0.104 ps	974.15 10	100	E2	198.371	9/2+
1192.23 9	B C H L M	11/2+	< 0.108 ps	993.9 1	100	M1+E2	198.371	9/2+
1205.146 9	B C D F G H L	5/2+	1.11 ps 28	373.837 12 457.72 12 615.365 10 680.035 9 705.1 3 1030.20 8	16.4 5 0.62 16 100.0 22 17.4 13 0.5 3 2.03 16	(E1) [E1] (M1+E2) (M1+E2) [E1] [E1]	831.301 747.248 589.775 525.114 499.915 174.954	3/2- 5/2- 7/2+ 5/2+ 3/2- 5/2-
1212.511 8	B C G H K	5/2-	> 1.2 ps	465.228 10 504.27 5 622.71 4 712.598 5 1037.530 15 1212.500 23	28.4 8 47 14 4.04 25 100 3 62.5 15 84.3 23	(M1+E2) (M1+E2) [E1] (M1+E2) (M1+E2) (E2)	747.248 708.196 589.775 499.915 174.954 0.0	5/2- 3/2- 7/2+ 3/2- 5/2- 1/2-
1237 5	F
1288.55 6	C D F G H K	1/2-		580.16 14 788.66 6	11 3 100 3		708.196 499.915	3/2- 3/2-
1298.75 4	B C D G H I	3/2-	0.42 ps 9	551.5 1 590.5 1 798.4 3 1123.74 8 1298.50 17	2.2 9 13 4 11.8 24 1.6 3 100.0 9	[M1,E2] [M1,E2] [M1,E2] [M1,E2] (M1+E2)	747.248 708.196 499.915 174.954 0.0	5/2- 3/2- 3/2- 5/2- 1/2-
1349.10 6	C D F G H K	1/2+	0.46 ps 11	517.78 6 824.14 19 1349.0 4	100 10 25 6 25 6	[E1] [E2] [E1]	831.301 525.114 0.0	3/2- 5/2+ 1/2-
1378.53 5	B C D G H K	(1/2-)		1203.7 6 1378.65 9	100 17 60 11		174.954 0.0	5/2- 1/2-
1378.71 5	B F G H I K	5/2-		281.8 1 ? 631.52 15 788.92 5	120 100 17 4.6 8		1096.07 747.248 589.775	7/2- 5/2- 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1406.640 10	B C F G H K	7/2-		311.15 15 380.08 6 659.428 19 698.44 2 906.696 11 1231.692 15 1406.5 1 ?	6.0 24 11.9 24 99 5 28.6 13 64.3 24 100 4 3.1 7	(M1+E2) [M3]	1095.511 1026.561 747.248 708.196 499.915 174.954 0.0	3/2- 5/2- 5/2- 3/2- 3/2- 5/2- 1/2-
1416.22 13	D F G H	(1/2-,3/2,5/2-)		916.40 14 1239.7 10 1415.9 3	100 14 74 13		499.915 174.954 0.0	3/2- 5/2- 1/2-
1422.04 9	B C H M	9/2-	< 1.2 ps	326.1 6 675.0 2 1247.0 1	3.9 6 18.6 28 100 4	(M1) E2 E2	1096.07 747.248 174.954	7/2- 5/2- 5/2-
1449.8 3 ?	B G			702.5 3 ?	100		747.248	5/2-
1454.3 10	F G H	(1/2+)		646.1 10 ?	100		808.196	1/2-
1475.9 3	D F G H L	(5/2-)		886.0 3 952.4 10	100 36		589.775 525.114	7/2+ 5/2+
1477.03 7	C L M	11/2+	< 0.64 ps	887.4 1 1278.5 1	87 6 100 9	E2 M1+E2	589.775 198.371	7/2+ 9/2+
1485 3	F G	(3/2+,5/2+)
1506.388 15	B G H K	7/2-	0.51 ps 16	674.33 8 759.11 3 798.55 23 1006.466 17 1307.98 3 1331.526 23	7.3 11 18.8 21 29.2 22 55.2 24 12.0 7 100 4	[E2] [M1,E2] [E2] [E2] [E1] [M1,E2]	831.301 747.248 708.196 499.915 198.371 174.954	3/2- 5/2- 3/2- 3/2- 9/2+ 5/2-
1542.48 8	C D F G H	(1/2+,3/2-)		447.6 10 1017.35 8 1542.3 8	29 100 12 24		1095.511 525.114 0.0	3/2- 5/2+ 1/2-
1558.757 15	B C D F G H K	5/2+		727.531 22 1033.55 3 1058.817 16 1360.44 13 1383.86 4	9.2 5 100 3 12.6 5 4.37 21 1.77 17	(M1+E2)	831.301 525.114 499.915 198.371 174.954	3/2- 5/2+ 3/2- 9/2+ 5/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1566.2 6	C G H	(5/2-,7/2+)		976.4 6 1041.0 10			589.775 525.114	7/2+ 5/2+
1598.534 17	B C D F G H I K	3/2-	0.55 ps 15	851.3 2 890.0 2 1073.4 2 1098.58 6 1423.579 25 1598.50 3	34 14 2.0 7 1.5 3 100 3 22.8 8 28.7 15	[M1,E2] [M1,E2] [E1] [M1,E2] [M1,E2] [M1,E2]	747.248 708.196 525.114 499.915 174.954 0.0	5/2- 3/2- 5/2+ 3/2- 5/2- 1/2-
1629.179 12	B G H	(3/2+,5/2-)		533.6 2 798.0 2 881.893 25 1039.34 6 1104.162 26 1129.37 5 1454.26 15 1629.154 15	11 6 54 27 100 8 30 3 38 3 19 3 2.4 8 81 3		1095.511 831.301 747.248 589.775 525.114 499.915 174.954 0.0	3/2- 3/2- 5/2- 7/2+ 5/2+ 3/2- 5/2- 1/2-
1631.2 4	D H	(1/2-,3/2,5/2-)		883.5 4 1632.0 5	58 4 100 6		747.248 0.0	5/2- 1/2-
1698.3 7	C F G H	(9/2)+		867.4 20 ? 1108.5 7		[E3]	831.301 589.775	3/2- 7/2+
1743.385 20	B D F G H I K	3/2-	0.42 ps 15	445.07 17 935.178 18 996.06 6 1218.16 7 1243.56 8 1568.4 2 1743.40 4	5.4 27 92 11 33 3 8.1 16 5.7 11 5.4 27 100 3	[M1,E2] [M1,E2] [M1,E2] [E1] [M1,E2] [M1,E2] (M1+E2)	1298.75 808.196 747.248 525.114 499.915 174.954 0.0	3/2- 1/2- 5/2- 5/2+ 3/2- 5/2- 1/2-
1780.762 19	B K	5/2-,7/2-		754.4 3 1191.18 9 1255.76 5 1280.91 6 1582.33 7 1605.749 21	11 5 35 12 29 3 12 5 21.2 18 100 7		1026.561 589.775 525.114 499.915 198.371 174.954	5/2- 7/2+ 5/2+ 3/2- 9/2+ 5/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1792.096 10	B D F G H	(3/2+,5/2-)		444.8 1 ? 696.575 12 765.89 7 983.67 5 1044.845 19 1083.86 3 1202.26 5 1267.008 20 1292.13 15 1617.12 4 1792.0 4	39 7 25 4 21 7 82 8 50 4 42 3 100 4 5.7 18 88.2 21 1.8 11		1349.10 1095.511 1026.561 808.196 747.248 708.196 589.775 525.114 499.915 174.954 0.0	1/2+ 3/2- 5/2- 1/2- 5/2- 3/2- 7/2+ 5/2+ 3/2- 5/2- 1/2-
1801.13 7	B	(5/2+,7/2)		1211.35 8 1276.0 4 1602.74 14	100 7 30 10 10.3 13		589.775 525.114 198.371	7/2+ 5/2+ 9/2+
1814 3	F
1835.81 9 ?	D			457.28 7 ?	100		1378.53	(1/2-)
1841 3	F
1868 5	F
1891 3	F
1909 5	F
1937.45 4	B H	(3/2+,5/2-)	0.69 ps 28	1347.7 5 1762.49 6 1937.41 4	3.7 22 69.3 22 100.0 22		589.775 174.954 0.0	7/2+ 5/2- 1/2-
1940.30 8	D	(1/2,3/2,5/2-)		561.86 5 1941.0 8 ?	100 10 62 10		1378.53 0.0	(1/2-) 1/2-
1941 3	F	(9/2)+
1949.29 13	C M	11/2-		527.2 6 853.2 1	9.7 17 100 14	D E2	1422.04 1096.07	9/2- 7/2-
1959.59 12	C L M	13/2+		482.6 6 767.4 1 786.8 3 921.8 6 1760.9 6	74 10 100 17 71 10 26 5 36 7	D D+Q D+Q Q Q	1477.03 1192.23 1172.54 1037.83 198.371	11/2+ 11/2+ 13/2+ 9/2+ 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1961 5	F	1/2+
1965.03 5	B D H I K L	3/2-		1965.04 7	100		0.0	1/2-
1979 3	F K
2031.89 9	D F K	(1/2,3/2)		2032.74 22	100		0.0	1/2-
2041 1	F I K	1/2-,3/2-
2075.7 4	D F	(1/2,3/2)		2075.8			0.0	1/2-
2082 5	F
2094 3	F
2139 5	F	(5/2-,7/2-)
2141.2 4	D	(1/2,3/2)		2141.3			0.0	1/2-
2146.15 5	D I	(3/2-)		2146.25			0.0	1/2-
2180 5	F
2210 5	F	(1/2+,5/2-,7/2-)
2224.50 11	D F K	1/2+		2223.7 4	100		0.0	1/2-
2240 3	F K
2257.00 11	D K	(1/2,3/2)		2257.3 3	100		0.0	1/2-
2276 1	I K	1/2-,3/2-
2277 5	F	5/2+
2297 5	F
2298.96 17	C M	17/2+		1126.45 15	100	E2	1172.54	13/2+
2313.97 19	C M	15/2+		1121.7 2 1141.2 6	100 12 9.0 15	E2 D+Q	1192.23 1172.54	11/2+ 13/2+
2330 5	F
2345 3	F	5/2+
2348.96 12	C M	13/2-		399.4 6 926.9 1	3.8 8 100 13	D E2	1949.29 1422.04	11/2- 9/2-
2351.60 22	D I K	1/2-,3/2-		2351.41 24	100		0.0	1/2-
2364.1 4	D F	(1/2+)		2364.2			0.0	1/2-
2386 3	F K	5/2-,7/2-
2426.8 5	D	1/2,3/2,5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2435 1	I	(3/2-,5/2-)
2435.2 5	D F	1/2+
2455 3	F
2462.35 15	D	(1/2,3/2)		2462.25 15			0.0	1/2-
2479 4	K
2486 3	F K	1/2+
2515.3 3	D	1/2,3/2,5/2+
2518.5 5	D	(1/2,3/2)		2518.5			0.0	1/2-
2523 3	F	5/2+
2533.97 7	D	(1/2,3/2)		2534.3			0.0	1/2-
2543 3	F
2572 5	F
2590 3	F
2616 3	F
2642 1	F I	5/2+
2675.8 4	D F K	1/2-,3/2-		2675.8			0.0	1/2-
2696 4	F K
2699.0 6	M	(15/2+)		1222.0 6	100	(Q)	1477.03	11/2+
2709 4	K	7/2+,9/2+
2725 5	F
2742 5	F	(1/2-,3/2-)
2756 3	F	3/2+,5/2+
2773 3	F	1/2+
2778 1	I K	1/2-,3/2-
2789 3	F
2806 1	F I	(5/2-)
2830 3	F
2837.20 20	M	15/2-		877.8 6 887.6 6 1664.7 3	24 5 17.3 32 100 13	D Q E1	1959.59 1949.29 1172.54	13/2+ 11/2- 13/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2857 3	F	3/2+,5/2+
2868.3 4	D K	1/2+		2867.6			0.0	1/2-
2881 3	F	3/2+
2889 2	F I K	1/2-,3/2-
2890.3 3	M	15/2-		541.1 6 941.0 3	12.5 21 100 12	D E2	2348.96 1949.29	13/2- 11/2-
2912 3	F K	3/2+,5/2+
2924 1	F I	(5/2-)
2940 3	F
2952.0 4	D K	(1/2,3/2)		2953.4			0.0	1/2-
2960 3	F	1/2+
3003 3	F	5/2+
3024.9 4	D	(1/2,3/2)		3025.6			0.0	1/2-
3035 3	F	5/2+
3065 3	F	3/2+,5/2+
3075.2 5	D			3078.2?			0.0	1/2-
3087 3	F	1/2+
3097.49 17	M	17/2+		783.4 3 798.8 6 1138.1 3 1924.5 6	100 12 11.4 23 100 11 3.0 8	M1 D E2	2313.97 2298.96 1959.59 1172.54	15/2+ 17/2+ 13/2+ 13/2+
3102 3	F K
3114 3	F
3129 3	F
3154 3	F
3157.6 4	D F	(1/2,3/2)		3157.7			0.0	1/2-
3183.5 4	D F	1/2+		3183.6			0.0	1/2-
3200 5	F K	3/2+,5/2+
3208.5 4	D	(1/2,3/2)		3208.5			0.0	1/2-
3214.1 4	D K	(1/2,3/2)		3214.1			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3223.9 4	D	(1/2,3/2)		3223.9			0.0	1/2-
3232 3	F K	(1/2+)
325E1 25	I
3260.7 5	D
3268 5	F K
3272.39 15	M	17/2-		435.3 6 923.4 1	6.0 9 100 12	D E2	2837.20 2348.96	15/2- 13/2-
3286 3	F K	(1/2-)
3293 5	F
3311 5	F	(1/2-)
3325.2 4	M	17/2-		976.2 3	100	E2	2348.96	13/2-
3334 3	F	(3/2+,5/2+)
3339.5 4	D	(1/2,3/2)		3338.8			0.0	1/2-
3361 5	F K
3375 3	F K
3382.1 4	D F	(1/2+)		3381.0			0.0	1/2-
3404.6 4	D F	(1/2,3/2)		3404.6			0.0	1/2-
3407.5 4	D	(1/2,3/2)		3407.5			0.0	1/2-
3411.59 18	M	19/2-		139.1 6 314.1 1 521.1 6 574.4 3 1113.1 6	6.0 12 100 16 19 4 56 8 18.0 30	(D) E1 (Q) E2 D	3272.39 3097.49 2890.3 2837.20 2298.96	17/2- 17/2+ 15/2- 15/2- 17/2+
3422 5	F	3/2+,5/2+
3444 5	F
3462.9 4	D F	(1/2,3/2)		3462.8			0.0	1/2-
3473 5	F	3/2+,5/2+
3481.7 4	D F	(3/2)+		3481.7			0.0	1/2-
3496 5	F
3514 5	F K	1/2-,3/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3533 5	K
3556.1 4	D F K	(3/2)+		3555.8			0.0	1/2-
3569.9 4	D F K	1/2-,3/2-		3569.8			0.0	1/2-
3593.07 20	M	21/2+		1294.1 1	100	E2	2298.96	17/2+
3597 3	F	3/2-
3599.6 4	M	19/2+		1285.6 3	100	Q	2313.97	15/2+
3615 5	F	(1/2+)
3633 3	F
3647 5	F
3661 3	F K
3681 3	F K	(1/2-,3/2,5/2+)
3721 3	F	1/2+
3744 3	F
375E1 25	I
3757.3 6	M	(19/2-)		867.0			2890.3	15/2-
3767 3	F	(5/2+)
3774 5	F K	5/2-,7/2-
3792 5	F K	1/2-,3/2-
3824 5	F
3843 3	F
3855 3	F
3866.0 4	D F	(1/2,3/2)		3865.8			0.0	1/2-
3884 5	F
3893.5 4	D K	1/2-,3/2-		3893.5			0.0	1/2-
3899 3	F	(3/2)+
3910 3	F	(5/2+)
3924 3	F K
3944 3	F K	1/2-,3/2-
3960 3	F K	1/2+
3976 5	F K
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3996 5	F K
4014.0 8 ?	M	(19/2+)		1314.9?			2699.0	(15/2+)
4050 10	F K
4080 10	F K
4090 10	F
4098.71 25	M	21/2-		687.2 3 826.2 3	62 5 100 11	M1 E2	3411.59 3272.39	19/2- 17/2-
4140 10	F
4226.5 4	D F K	(1/2,3/2)		4226.5			0.0	1/2-
425E1 25	I
4306.8 5	D F	(1/2,3/2)		4306.7			0.0	1/2-
4363.1 6 ?	M	(21/2-)		1037.9?			3325.2	17/2-
4388 7	K
4410 10	F	(1/2+)
4472.8 5	M	23/2-		373.9 6 1061.3 6	100 15 38 10	D Q	4098.71 3411.59	21/2- 19/2-
4.5E3 29	I
4520 10	F
4914.8 7	M	23/2+		1315.2 6	100	Q	3599.6	19/2+
5E3 3	J
5009.4 4	M	25/2+		1416.3 3	100	Q	3593.07	21/2+
525E1 25	I
5274.3 6	M	25/2-		1175.6 6	100	Q	4098.71	21/2-
5727.2 6	M	27/2-		453.0 6 1254.4 6	54 11 100 28	D Q	5274.3 4472.8	25/2- 23/2-
575E1 25	I
6E3 2	G
625E1 25	I
6639.7 7	M	29/2+		1630.3 6	100	Q	5009.4	25/2+
675E1 25	I
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7114.0 9	M	31/2-		1386.8 6	100	Q	5727.2	27/2-
721E1 21	I
7415.957 16 S	D	1/2+		3189.5 3522.5 3549.7 3845.9 3859.5 3934.3 3953.0 4008.5 4011.4 4032.8 4075.7 4155.1 4192.1 4201.9 4207.5 4232.4 4258.3 4340.6 4391.7 4465.2 4546.9 4740.1 4881.81 6 4900.5 3 4951 4980.6 4989 5051.8 5063.5 5158.80 11 5191.20 11 5269.60 4 5274.7 5340.2 5383.88 9 5450.71 7 5672.3 3 5817.15 4 5873.16 23 6037.21 6 6116.86 4 6276.25 5 6319.99 4 6584.32 4 6607.45 14 6707.45 4 6915.68 4 7415.58 4	17.3 18.2 23.6 17.3 23.6 13.5 12.7 16.7 27.3 8.2 4.5 38.0 24 5.8 5 7.5 15 11.1 4.2 6 18.9 15.8 13 12.9 9 17.8 9 29.5 13 64 3 8.2 9 63 3 6.5 4 100 5 96 4 48 3 33.8 14 20.0 9 3.6 2 87 4 70 3 35.5 16		4226.5 3893.5 3866.0 3569.9 3556.1 3481.7 3462.9 3407.5 3404.6 3382.1 3339.5 3260.7 3223.9 3214.1 3208.5 3183.5 3157.6 3075.2 3024.9 2952.0 2868.3 2675.8 2533.97 2515.3 2462.35 2435.2 2426.8 2364.1 2351.60 2257.00 2224.50 2146.15 2141.2 2075.7 2031.89 1965.03 1743.385 1598.534 1542.48 1378.53 1298.75 1139.441 1095.511 831.301 808.196 708.196 499.915 0.0	(1/2,3/2) 1/2-,3/2- (1/2,3/2) 1/2-,3/2- (3/2)+ (3/2)+ (1/2,3/2) (1/2,3/2) (1/2,3/2) (1/2+) (1/2,3/2) (1/2,3/2) (1/2,3/2) (1/2,3/2) 1/2+ (1/2,3/2) (1/2,3/2) (1/2,3/2) 1/2+ 1/2-,3/2- (1/2,3/2) 1/2,3/2,5/2+ (1/2,3/2) 1/2+ 1/2,3/2,5/2+ (1/2+) 1/2-,3/2- (1/2,3/2) 1/2+ (3/2-) (1/2,3/2) (1/2,3/2) (1/2,3/2) 3/2- 3/2- 3/2- (1/2+,3/2-) (1/2-) 3/2- 3/2- 3/2- 3/2- 1/2- 3/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7417.03 11	E	1/2+
7417.39 11	E	1/2+
7417.85 11	E	(1/2-,3/2-)
7419.05 11	E	(1/2-,3/2-)
7420.11 11	E	(1/2-,3/2-)
7420.28 11	E	1/2+
7421.46 11	E	1/2+
7422.64 11	E	1/2+
7424.52 11	E	1/2+
7425.76 12	E	1/2+
7426.16 12	E	1/2+
7426.83 12	E	1/2+
7427.63 12	E	1/2+
7429.04 12	E	1/2+
7434.28 12	E	1/2+
7439.67 13	E	1/2+
7441.60 13	E	1/2+
7443.44 14	E	1/2+
7444.66 14	E	1/2+
7451.99 16	E
7455.70 16	E
7.94E3 52	I
8913 5	G I	3/2-	% n ≈ 100
11.75E3	I
18.0E3	I