List of levels for 93NB

Author: Coral M. Baglin | Citation: Nucl. Data Sheets 112, 1163 (2011) | Cutoff date: 15-Dec-2010

Other Reactions:

¹⁷³Yb(²⁴Mg,Fγ), E=134.5 MeV (2010Fo10): observed 950γ following fission of ¹⁹⁷Pb compound nucleus.

⁸⁹Y(α,α) (2009Ki16): Eα=16.21 and 19.47 MeV; measured σ(θ) in 1|’ to 2|’ steps from θ(lab)=20|’ to 170|’; deduced local optical model parameters; predicted (89Y~#α) α cluster states in ⁹³Nb and calculated E2 reduced transition strengths within a Kπ=1/2- band based on the 31 level.

⁹³Nb(t,t) (2007Ch20):

E(t)=12 MeV; measured σ(θ); deduced optical-model parameters.

⁹³Nb(n,n’) (1996De01, 1994De41):

E(n)=14.1 MeV. Analyzed σ(E,θ) data of Takahashi et al. (OKTAVIAN report A-92-01); calculated contributions from multistep direct, compound nucleus, multistep compound nucleus mechanisms, and collective excitations.

⁹³Nb(α,α’) (1960Cr05):

Eα≈30 MeV, θ(c.m.)≈45|’-85|’; observed g.s. and E(level)=2400 300 (possibly complex); measured σ(θ).

Q-value: Note: Current evaluation has used the following Q record -406 4 8831.0 20 6042.9 16-1931.0 22 2003Au03,2009AuZZ

Q-value: Q(β^-), S(n), S(p), Q(α): from 2009AuZZ (cf. 405 4, 8831.3 20, 6043.4 16, -1931.4 23, respectively, from 2003Au03).

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
30.77	1/2-	16.12 y 12 % IT = 100	30.77 2	M4		1.693×10⁵	B(M4)(W.u.)=11.49 20, α=1.693×10⁵
686.79	3/2-	0.28 ps +48-14	655.9 2	(M1+E2)	-0.13 +9-14	0.00187	B(E2)(W.u.)=11 +16-11, B(M1)(W.u.)=0.27 +14-27, α=0.00187
743.95	7/2+	0.51 ps 4	744.06 12	M1+E2	+0.236 18	1.41×10^-3	B(E2)(W.u.)=10.2 17, B(M1)(W.u.)=0.099 8, α=1.41E-3
808.82	5/2+	6.16 ps 20	64.88 18	(M1)		0.767	B(M1)(W.u.)=0.160 12, α=0.767 13
808.82	5/2+	6.16 ps 20	808.53 12	E2		1.20×10^-3	B(E2)(W.u.)=10.4 4, α=1.20E-3
810.32	5/2-	> 1.0 ps	779.53 22	(E2)		1.31×10^-3	B(E2)(W.u.)<78, α=1.31E-3
949.80	13/2+	4.36 ps 15	949.81 3	E2		8.12×10^-4	B(E2)(W.u.)=6.70 23, α=8.12E-4
978.91	11/2+	258 fs 18	978.94 14	M1+E2	-0.255 8	7.69×10^-4	B(E2)(W.u.)=5.96 20, B(M1)(W.u.)=0.085 6, α=7.69E-4
1082.68	9/2+	> 2.8 ps	338.73 7	(E2+M1)	-0.09 2	0.00911	B(E2)(W.u.)<14, B(M1)(W.u.)<0.14, α=0.00911 16
1082.68	9/2+	> 2.8 ps	1082.53 15	M1+E2	1.8 GT	6.08×10^-4	B(E2)(W.u.)=1.03 9, B(M1)(W.u.)<0.00035, α=6.08E-4
1127.09	3/2,5/2,7/2		318.3 2	D+Q	-0.20 6	0.01053	α=0.01053
1284.26	(5/2)-	0.17 ps +6-4	597.3 2	M1+E2	+0.14 4		B(E2)(W.u.)=6 +4-5, B(M1)(W.u.)=0.11 +4-5
1297.22	9/2+	0.21 ps 3	318.3 1	(M1)		0.01053	B(M1)(W.u.)=0.73 18, α=0.01053
	9/2+	0.21 ps 3	553.10 9	(M1(+E2))	+0.02 3	0.00282	B(E2)(W.u.)=0.2 +7-2, B(M1)(W.u.)=0.16 3, α=0.00282 24
	9/2+	0.21 ps 3	1297.38 9	M1+E2	+0.355 25	4.45×10^-4	B(E2)(W.u.)=1.52 10, B(M1)(W.u.)=0.022 4, α=4.45E-4
1315.50	5/2+	0.37 ps +31-12	506.7 2	M1+E2	-1.4 8		B(E2)(W.u.)=2.3×10² +12-22, B(M1)(W.u.)=0.029 +25-29
1315.50	5/2+	0.37 ps +31-12	571.5 2	M1+E2	+0.14 4		B(E2)(W.u.)=16 +11-16, B(M1)(W.u.)=0.25 +9-22
1335.04	17/2+	< 14 ns	385.224 23	E2		0.01002	B(E2)(W.u.)>0.19, α=0.01002
1369.86	5/2-	> 0.55 ps	559.4 2	D+Q	-0.32 7
1369.86	5/2-	> 0.55 ps	683.2 2	D+Q	-0.34 5
1395.42	(7/2-)	> 0.55 ps	584.97 22	D+Q	-0.10 2
1395.42	(7/2-)	> 0.55 ps	708.6 2	[E2]			B(E2)(W.u.)<19
1483.58	7/2(+)	45.7 fs 24	674.8 1	(M1+E2)	-0.11 8		B(E2)(W.u.)=8 +12-8, B(M1)(W.u.)=0.285 25
1483.58	7/2(+)	45.7 fs 24	1483.46 16	(M1+E2)	-0.13 7		B(E2)(W.u.)=0.9 +10-9, B(M1)(W.u.)=0.109 7
1490.99	15/2+	< 14 ns	155.94 3	[M1,E2]		0.15	α=0.15 9
1490.99	15/2+	< 14 ns	541.29 7	M1+E2	-0.104 17		B(E2)(W.u.)>0.00020, B(M1)(W.u.)>7.8E-6
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1499.94	(9/2-)	0.84 ps 22	520.9 1	[E1]			B(E1)(W.u.)=4.E-5 +5-4
	(9/2-)	0.84 ps 22	689.6 1	[E2]			B(E2)(W.u.)=24 8
	(9/2-)	0.84 ps 22	756.1 1	[E1]			B(E1)(W.u.)=4.9E-5 15
	(9/2-)	0.84 ps 22	1499.9 1	(E1(+M2))	-0.02 16		B(E1)(W.u.)=9.2E-5 25, B(M2)(W.u.)=0.07 +120-7
1571.82	3/2-	0.19 ps +15-7	761.4 2	M1+E2	-0.28 3		B(E2)(W.u.)=22 +10-18, B(M1)(W.u.)=0.16 +6-13
1571.82	3/2-	0.19 ps +15-7	885.1 2	M1+E2	-1.60 14		B(E2)(W.u.)=37 +15-30, B(M1)(W.u.)=0.011 +5-9
1588.06	3/2(-),5/2(-)	> 0.87 ps	777.8 2	(M1+E2)	-4.0 +13-35		B(E2)(W.u.)<14, B(M1)(W.u.)<0.00078
1588.06	3/2(-),5/2(-)	> 0.87 ps	901.2 2	(M1+E2)	-0.53 6		B(E2)(W.u.)<9.6, B(M1)(W.u.)<0.024
1603.44	11/2+	0.32 ps +17-9	520.9 2	(M1(+E2))	-0.07 9		B(E2)(W.u.)=0.6 +16-6, B(M1)(W.u.)=0.032 +12-19
	11/2+	0.32 ps +17-9	624.4 2	(M1+E2)	+0.11 6		B(E2)(W.u.)=1.5 +17-15, B(M1)(W.u.)=0.047 +14-26
	11/2+	0.32 ps +17-9	653.6 2	M1+E2	+0.17 3		B(E2)(W.u.)=9 +4-6, B(M1)(W.u.)=0.13 +4-7
	11/2+	0.32 ps +17-9	859.5 2	[E2]			B(E2)(W.u.)=20 +7-12
1665.66	5/2+	0.24 ps +7-5	921.6 2	M1+E2	+1.4 2		B(E2)(W.u.)=92 +22-29, B(M1)(W.u.)=0.039 +11-14
1679.50	5/2(+),7/2	0.22 ps +6-4	364.1 2	D+Q	-0.17 9
1679.50	5/2(+),7/2	0.22 ps +6-4	935.7 2	D(+Q)	+0.09 9
1683.36	9/2+	104 fs +17-14	704.2 2	M1+E2	+0.21 4		B(E2)(W.u.)=10 5, B(M1)(W.u.)=0.113 +19-22
	9/2+	104 fs +17-14	939.3 2	M1+E2	-0.20 4		B(E2)(W.u.)=5.3 +22-23, B(M1)(W.u.)=0.114 +17-20
	9/2+	104 fs +17-14	1683.2 2	(M1+E2)	-0.34 25		B(E2)(W.u.)=0.4 +6-4, B(M1)(W.u.)=0.0106 +22-24
1686.34	13/2+	0.17 ps +4-3	707.4 2	M1+E2	-0.09 3		B(E2)(W.u.)=1.9 14, B(M1)(W.u.)=0.115 +22-28
	13/2+	0.17 ps +4-3	736.5 2	D+Q	-0.27 13
	13/2+	0.17 ps +4-3	1686.3 2	[E2]			B(E2)(W.u.)=3.5 +7-9
1703.51	3/2+,5/2+	0.15 ps +19-6	387.9 2	(M1(+E2))	-0.02 6		B(E2)(W.u.)=4 +22-4, B(M1)(W.u.)=1.3 +6-13
1703.51	3/2+,5/2+	0.15 ps +19-6	894.8 2	(M1+E2)	-0.3 1		B(E2)(W.u.)=10 +8-10, B(M1)(W.u.)=0.09 +4-9
1779.27	(5/2-)	73 fs +30-19	969.0 2	(M1(+E2))	+0.04 6		B(E2)(W.u.)=0.5 +17-5, B(M1)(W.u.)=0.31 +9-13
1779.27	(5/2-)	73 fs +30-19	1092.4 2	(M1(+E2))	+0.05 9		B(E2)(W.u.)=0.04 +14-4, B(M1)(W.u.)=0.017 +12-13
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1910.68	7/2+,9/2+,11/2+	162 fs 13	613.4 1	(M1+E2)	-0.20 12		B(E2)(W.u.)=5 +7-5, B(M1)(W.u.)=0.048 16
	7/2+,9/2+,11/2+	162 fs 13	828.1 1	M1+E2	-0.61 17		B(E2)(W.u.)=6 4, B(M1)(W.u.)=0.010 5
	7/2+,9/2+,11/2+	162 fs 13	1910.6 1	M1+E2	+3.9 36	4.52×10^-4	B(E2)(W.u.)=4.4 7, B(M1)(W.u.)=0.0010 +18-10, α=4.52E-4 23
1915.92	7/2	62 fs 7	600.4 2	D+Q	+0.06 4
1915.92	7/2	62 fs 7	833.4 2	D(+Q)	-0.01 2
1947.73	3/2,5/2,7/2	0.16 ps +9-5	1137.4 2	D(+Q)	+0.05 4
1949.72	(7/2+)	0.5 ps +11-2	971.1 2	[E2]			B(E2)(W.u.)=0.18 +19-18
1949.72	(7/2+)	0.5 ps +11-2	1140.8 2	(M1+E2)	+0.21 5		B(E2)(W.u.)=0.33 +21-33, B(M1)(W.u.)=0.010 +4-10
1968.87	11/2+	111 fs 19	282.5 1	[M1,E2]		0.021	α=0.021 7
	11/2+	111 fs 19	285.4 1	[M1,E2]		0.021	α=0.021 7
	11/2+	111 fs 19	990.0 1	M1+E2	-0.83 16		B(E2)(W.u.)=21 7, B(M1)(W.u.)=0.030 8
	11/2+	111 fs 19	1019.0 1	M1+E2	-0.28 7		B(E2)(W.u.)=1.6 9, B(M1)(W.u.)=0.021 5
	11/2+	111 fs 19	1225.0 1	[E2]			B(E2)(W.u.)=3.4 16
1997.12	3/2-,5/2-	64 fs +15-12	1186.9 2	M1+E2	-0.31 11		B(E2)(W.u.)=12 +8-9, B(M1)(W.u.)=0.17 +4-5
1997.12	3/2-,5/2-	64 fs +15-12	1310.2 2	(M1+E2)	-0.29 12		B(E2)(W.u.)=0.8 7, B(M1)(W.u.)=0.015 +7-8
2002.52	(11/2+)	> 0.55 ps	502.4 2	[E1]			B(E1)(W.u.)<0.00040
	(11/2+)	> 0.55 ps	1023.7 2	[E2]			B(E2)(W.u.)<2.6
	(11/2+)	> 0.55 ps	1052.8 2	(M1+E2)	-0.63 7	6.50×10^-4	B(E2)(W.u.)<7.3, B(M1)(W.u.)<0.018, α=6.50E-4 13
2012.41	(LE5/2)-	21 fs +20-8	1325.8 2	M1+E2	+4.5 +15-9		B(E2)(W.u.)=2.4×10² +10-23, B(M1)(W.u.)=0.020 +15-20
2023.91	(LE5/2)-	54 fs +28-17	1337.1 2	M1+E2	-4.7 +8-13		B(E2)(W.u.)=9.×10¹ +3-5, B(M1)(W.u.)=0.007 +4-5
2099.23	(3/2-,5/2,7/2)	92 fs +43-25	1288.9 2	D(+Q)	-0.05 5
2122.67	9/2+	97 fs 16	1143.7 1	M1+E2	+3.8 +19-10		B(E2)(W.u.)=34 7, B(M1)(W.u.)=0.003 3
2122.67	9/2+	97 fs 16	1378.9 1	M1+E2	-0.19 8		B(E2)(W.u.)=0.20 17, B(M1)(W.u.)=0.0103 21
6464.3	11/2(+)		5516 3	(M1)		1.62×10^-3	α=1.62×10^-3

Q(β-)=-406.7 keV 20	S(n)= 8830.6 keV 21	S(p)= 6042.3 keV 16	Q(α)= -1928.8 keV 23
Reference: 2012WA38

References:
A	⁹³Mo ε decay (6.85 H)	B	⁹²Zr(α,t)
C	⁹³Nb(p,p’)	D	Coulomb Excitation
E	⁹³Nb(n,n’γ)	F	⁹³Nb(γ,γ’) E=6465 KEV
G	⁹²Zr(³He,d)	H	⁹⁴Mo(d,³He)
I	⁹¹Zr(α,d)	J	⁹⁰Zr(α,pγ)
K	⁹²Zr(p,p’), (pol p,p) IAR	L	⁹⁶Mo(p,α)
M	⁸⁰Se(¹⁶O,p2nγ)	N	⁹³Nb(d,d’), (pol d,d)
O	⁹³Nb(γ,XN)	P	⁹³Zr β^- decay
Q	⁹³Nb(E,E’)	R	⁹³Mo ε decay (4.0×10³ Y)
S	⁹³Nb IT decay (16.12 Y)	T	⁹²Zr(p,α) IAR
U	⁸⁹Y(α,nγ)	V	⁹²Zr(¹⁶O,¹⁵N)
W	⁹³Nb(γ,γ’): E<2.75 MeV	X	⁹⁴Zr(p,2nγ)
Y	⁸²Se(¹⁶O,p4nγ)

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 H I J L M N P Q R S W X Y	9/2+	STABLE
30.77 2	E G H J L P R S X	1/2-	16.12 y 12 % IT = 100	30.77 2	100	M4	0.0	9/2+
686.79 10	B E G H J L X	3/2-	0.28 ps +48-14	655.9 2	100	(M1+E2)	30.77	1/2-
743.95 5	C D E J N W X	7/2+	0.51 ps 4	744.06 12	100	M1+E2	0.0	9/2+
808.82 7	B C D E G I J L X	5/2+	6.16 ps 20	64.88 18 808.53 12	1.25 8 100.00 8	(M1) E2	743.95 0.0	7/2+ 9/2+
810.32 9	B C E I J L X	5/2-	> 1.0 ps	123.3 2 779.53 22	<1 100	(E2)	686.79 30.77	3/2- 1/2-
949.80 3	A B C D E F I J L M N W X Y	13/2+	4.36 ps 15	949.81 3	100	E2	0.0	9/2+
970 10 ?	G	1/2-,3/2-
978.91 5	B C D E F I J N W X	11/2+	258 fs 18	978.94 14	100	M1+E2	0.0	9/2+
1082.68 5	B C D E F G J L N X	9/2+	> 2.8 ps	103.80 11 338.73 7 1082.53 15	9 3 100.0 17 35 3	(E2+M1) M1+E2	978.91 743.95 0.0	11/2+ 7/2+ 9/2+
1127.09 12	E J X	3/2,5/2,7/2		318.3 2	100	D+Q	808.82	5/2+
1284.26 13	E X	(5/2)-	0.17 ps +6-4	473.9 2 597.3 2 1253.5 2	5 4 25 4 100 4	M1+E2	810.32 686.79 30.77	5/2- 3/2- 1/2-
1290 12	B C G H I L	1/2-,3/2-
1297.22 6	B C D E F I W X	9/2+	0.21 ps 3	318.3 1 553.10 9 1297.38 9	44 8 52.2 20 100.0 25	(M1) (M1(+E2)) M1+E2	978.91 743.95 0.0	11/2+ 7/2+ 9/2+
1315.50 11	C E G I N X	5/2+	0.37 ps +31-12	506.7 2 571.5 2	23.5 12 100.0 25	M1+E2 M1+E2	808.82 743.95	5/2+ 7/2+
1335.04 4	A E M X Y	17/2+	< 14 ns	385.224 23	100	E2	949.80	13/2+
1369.86 17	B E H L X	5/2-	> 0.55 ps	559.4 2 683.2 2 1338.9	100 4 30 4 14	D+Q D+Q	810.32 686.79 30.77	5/2- 3/2- 1/2-
1395.42 13	E X	(7/2-)	> 0.55 ps	584.97 22 708.6 2	100 4 9 4	D+Q [E2]	810.32 686.79	5/2- 3/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1455.0 8	E I	(1/2+,3/2+)		646.2 8	100		808.82	5/2+
1483.58 7	E F I L W X	7/2(+)	45.7 fs 24	400.8 1 674.8 1 1483.46 16	8.2 18 24.4 15 100.0 16	(M1+E2) (M1+E2)	1082.68 808.82 0.0	9/2+ 5/2+ 9/2+
1490.99 5	A E F I L X Y	15/2+	< 14 ns	155.94 3 541.29 7	22 5 100.0 16	[M1,E2] M1+E2	1335.04 949.80	17/2+ 13/2+
1499.94 6	E I N W X	(9/2-)	0.84 ps 22	520.9 1 689.6 1 756.1 1 1499.9 1	2 2 18 3 6.9 10 100 2	[E1] [E2] [E1] (E1(+M2))	978.91 810.32 743.95 0.0	11/2+ 5/2- 7/2+ 9/2+
1571.82 14	B E G L X	3/2-	0.19 ps +15-7	287.4 2 761.4 2 885.1 2	20 5 100 5 37 5	M1+E2 M1+E2	1284.26 810.32 686.79	(5/2)- 5/2- 3/2-
1588.06 17	E X	3/2(-),5/2(-)	> 0.87 ps	777.8 2 901.2 2	18 8 100 8	(M1+E2) (M1+E2)	810.32 686.79	5/2- 3/2-
1603.24 16 ?	E	(9/2-)		520.5 4 ? 624.5 3 ? 859.1 3 ?	37 5 100 5 63		1082.68 978.91 743.95	9/2+ 11/2+ 7/2+
1603.44 9	E X	11/2+	0.32 ps +17-9	520.9 2 624.4 2 653.6 2 859.5 2 1603.5 2	13 3 33.0 15 100 3 26 4 23 3	(M1(+E2)) (M1+E2) M1+E2 [E2]	1082.68 978.91 949.80 743.95 0.0	9/2+ 11/2+ 13/2+ 7/2+ 9/2+
1665.66 12	B E G I L N X	5/2+	0.24 ps +7-5	856.9 2 921.6 2 1665.7 2	<1 100 2 2 2	M1+E2	808.82 743.95 0.0	5/2+ 7/2+ 9/2+
1679.50 10	B E F I L N X	5/2(+),7/2	0.22 ps +6-4	364.1 2 382.4 2 870.1 2 935.7 2 1679.58 24	60 3 16 3 7 3 100 3 37.4 17	D+Q D(+Q)	1315.50 1297.22 808.82 743.95 0.0	5/2+ 9/2+ 5/2+ 7/2+ 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1683.36 8	B E F I L N X	9/2+	104 fs +17-14	600.7 2 704.2 2 939.3 2 1683.2 2	17 4 42 4 100 3 57.4 19	M1+E2 M1+E2 (M1+E2)	1082.68 978.91 743.95 0.0	9/2+ 11/2+ 7/2+ 9/2+
1686.34 9	B E F I X	13/2+	0.17 ps +4-3	707.4 2 736.5 2 1686.3 2	88 4 90 4 100 4	M1+E2 D+Q [E2]	978.91 949.80 0.0	11/2+ 13/2+ 9/2+
1694.0?	E N			950?	100		743.95	7/2+
1703.51 16	E G X	3/2+,5/2+	0.15 ps +19-6	387.9 2 894.8 2	100 4 87 4	(M1(+E2)) (M1+E2)	1315.50 808.82	5/2+ 5/2+
1772.96 17	E L X	(LE7/2)	87 fs +14-10	318.27 17 ? 646.0 2 964.0 2	25 86 4 100 4		1455.0 1127.09 808.82	(1/2+,3/2+) 3/2,5/2,7/2 5/2+
1779.27 17	E L X	(5/2-)	73 fs +30-19	969.0 2 1092.4 2	100 5 8 5	(M1(+E2)) (M1(+E2))	810.32 686.79	5/2- 3/2-
1784.40 25	E L	(5/2+)		701.71 24	100		1082.68	9/2+
1812.34 21	E X	(19/2)	104 fs +35-24	477.3 2	100		1335.04	17/2+
1840.07 17	E X	3/2-,5/2-	71 fs +24-17	1029.6 2 1153.4 2	20 4 100 4	(M1+E2) M1+E2	810.32 686.79	5/2- 3/2-
1908.1 11	C E	(5/2)		1908.1 11	100		0.0	9/2+
1910.68 7	C E W X	7/2+,9/2+,11/2+	162 fs 13	613.4 1 828.1 1 1910.6 1	10 3 7 3 100 3	(M1+E2) M1+E2 M1+E2	1297.22 1082.68 0.0	9/2+ 9/2+ 9/2+
1915.92 10	E X	7/2	62 fs 7	600.4 2 833.4 2 1107.2 2 1172.1 2 1915.5 2	36 4 100 4 4 4 12 4 5 4	D+Q D(+Q)	1315.50 1082.68 808.82 743.95 0.0	5/2+ 9/2+ 5/2+ 7/2+ 9/2+
1947.73 22	C E N X	3/2,5/2,7/2	0.16 ps +9-5	1137.4 2	100	D(+Q)	810.32	5/2-
1949.72 10	C E N X	(7/2+)	0.5 ps +11-2	270.1 2 866.8 2 971.1 2 1140.8 2 1205.9 2	100 5 9 5 <2 100 5 89 4	[E2] (M1+E2)	1679.50 1082.68 978.91 808.82 743.95	5/2(+),7/2 9/2+ 11/2+ 5/2+ 7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1949.81 13	E F N X	(11/2)	0.6 ps +26-3	266.4 2 346.4 2 1949.8 2	32 5 50 5 100 5		1683.36 1603.44 0.0	9/2+ 11/2+ 9/2+
1968.27 17	E W X	(13/2-)		365.0 2 477.3 2	45 3 100 3		1603.24 1490.99	(9/2-) 15/2+
1968.87 5	E N W X	11/2+	111 fs 19	282.5 1 285.4 1 990.0 1 1019.0 1 1225.0 1 1968.9 1	23 5 29 6 64 5 31 4 12 5 100 3	[M1,E2] [M1,E2] M1+E2 M1+E2 [E2]	1686.34 1683.36 978.91 949.80 743.95 0.0	13/2+ 9/2+ 11/2+ 13/2+ 7/2+ 9/2+
1997.12 17	E X	3/2-,5/2-	64 fs +15-12	1186.9 2 1310.2 2	100 5 12 5	M1+E2 (M1+E2)	810.32 686.79	5/2- 3/2-
2002.52 10	B E X	(11/2+)	> 0.55 ps	399.1 2 502.4 2 511.5 2 1023.7 2 1052.8 2	20 2 12 2 <2 10 2 100 2	[E1] [E2] (M1+E2)	1603.44 1499.94 1490.99 978.91 949.80	11/2+ (9/2-) 15/2+ 11/2+ 13/2+
2012.41 18	X	(LE5/2)-	21 fs +20-8	440.4 2 1325.8 2	6 5 100 5	M1+E2	1571.82 686.79	3/2- 3/2-
2019.7 4	E	(7/2-,9/2-)		1209.4 4	100		810.32	5/2-
2023.91 18	X	(LE5/2)-	54 fs +28-17	452.1 2 1337.1 2	3 3 100 3	M1+E2	1571.82 686.79	3/2- 3/2-
2037.2 3	E	(9/2+,11/2+)		537.2 3 1087.4 6	100 28		1499.94 949.80	(9/2-) 13/2+
2099.23 17	E L X	(3/2-,5/2,7/2)	92 fs +43-25	703.8 2 1288.9 2	100 7 46 7	D(+Q)	1395.42 810.32	(7/2-) 5/2-
2122.67 6	E W X	9/2+	97 fs 16	639.0 1 1143.7 1 1378.9 1 2122.6 1	36 3 71 3 29 3 100 3	M1+E2 M1+E2	1483.58 978.91 743.95 0.0	7/2(+) 11/2+ 7/2+ 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2126.89 12	E X	(5/2-,7/2,9/2-)	0.16 ps +12-8	626.9 2 731.3 2 1316.61 20 1383.1 2	100 4 18 4 10 4 13 4		1499.94 1395.42 810.32 743.95	(9/2-) (7/2-) 5/2- 7/2+
2132.6 5	B E L	(GE7/2)		1153.7 5	100		978.91	11/2+
2153.60 20	B E X	(1/2,3/2,5/2-)	80 fs +19-14	2122.8 2	100		30.77	1/2-
2162.64 12	B E N X	(11/2+,13/2,15/2+)	0.28 ps +21-9	671.7 2 1183.7 2 1212.8 2	24 3 100 4 61 4		1490.99 978.91 949.80	15/2+ 11/2+ 13/2+
2170.65 10	B E X	9/2+	0.24 ps +11-6	1087.6 2 1192.5 2 1221.6 2 1361.1 2 1426.1 2 2171.4 5	10 3 100 3 60 3 31 3 27 3 14 2		1082.68 978.91 949.80 808.82 743.95 0.0	9/2+ 11/2+ 13/2+ 5/2+ 7/2+ 9/2+
2180 10	G N	3/2+,5/2+
2180.04 5	A Y	(17/2)-		689.053 19 844.96 6	100.0 25 37.5 25	E1	1490.99 1335.04	15/2+ 17/2+
2184.14 21	E X		76 ps +31-21	849.1 2	100		1335.04	17/2+
2203.5 3	E	(9/2+)		600.4 3 ? 808.3 4 2203.2 4	24 100 33		1603.24 1395.42 0.0	(9/2-) (7/2-) 9/2+
2250	C
2280.7 7	C E	(7/2-)		1536.7 7	100		743.95	7/2+
2310.9 9	Y			976	100		1335.04	17/2+
2320 10	B G	3/2+,5/2+
2330.0 5	B E			1351.1 5	100		978.91	11/2+
2367.5 10	B C E F	9/2,13/2(+)		2367.3 10	100		0.0	9/2+
2506.88 8	W X		66 fs +21-14	1527.9 1 2506.9 1			978.91 0.0	11/2+ 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2520 10	B C G N	(1/2+)
2584.2 7	B C E G	3/2+,5/2+		1775.4 7	100		808.82	5/2+
2752.84 5	A	(19/2)+		572.796 19 1261.91 14 1417.75 10	100 4 59 4 55 4		2180.04 1490.99 1335.04	(17/2)- 15/2+ 17/2+
2832.8 9	M Y	21/2+		522 1497.6	4.9 7 100 7	E2	2310.9 1335.04	17/2+
2838 4	B C F N	11/2
2980 20	B C
3086.0 10	Y	(21/2)		906	100	Q	2180.04	(17/2)-
3150 20	B C
3512 17	B I
3667.8 13	Y			835	100		2832.8	21/2+
3674.0 15	Y	(25/2)		588	100		3086.0	(21/2)
3684.8 12	Y			852	100		2832.8	21/2+
3720 30	B
3840 17	B I
3930 30	I
4060 30	I
4104.7 12	M Y	25/2(+)		420 1271.9	9.7 7 100 5	D+Q Q	3684.8 2832.8	21/2+
4224 17	B I
4340 20	B
4403.0 18	Y	(29/2)		729	100		3674.0	(25/2)
4460 20	B
4548 17	B I
4650 20 ?	B
4700 30	B
4810 30	B
4864.6 16	M Y	29/2(+)		759.9	100	E2	4104.7	25/2(+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5000 30	B
5155.1 18	Y			1481	100		3674.0	(25/2)
5340 40	B
5490 40	B
5904.3 19	M Y	33/2(+)		1039.7	100	E2	4864.6	29/2(+)
6464.3 10	F	11/2(+)		3626 3 4095 3 4514 3 4783 3 4971 3 4979 3 5168 3 5384 3 5486 3 5516 3 6465 3	29 9 29 9 11.4 11 11.1 4 9.3 4 4.3 11 10.7 7 16.8 7 0.7 7 100.0 18 35.7 7	D D D D D (M1) (M1)	2838 2367.5 1949.81 1490.99 1483.58 1297.22 1082.68 978.91 949.80 0.0	11/2 9/2,13/2(+) (11/2) 15/2+ 7/2(+) 9/2+ 9/2+ 11/2+ 13/2+ 9/2+
7372.3 21	Y	(35/2-)		1468	100	D+Q	5904.3	33/2(+)
7435.3 21	Y	37/2(-)		1531	100	Q	5904.3	33/2(+)
7828.3 23	Y	39/2(-)		393	100	M1	7435.3	37/2(-)
8325.4 25	Y	41/2(-)		497	100	D	7828.3	39/2(-)
8377.4 21	Y	(37/2)		942 1005	100 10 59 6	D+Q D	7435.3 7372.3	37/2(-) (35/2-)
8940 3	Y	(43/2-)		615	100	M1	8325.4	41/2(-)
9134.4 22	Y	(41/2-)		1699	100	(E2)	7435.3	37/2(-)
9425 3	Y	(45/2+)		485	100	E1	8940	(43/2-)
9699.4 22	Y	(39/2-,41/2-)		2264	100		7435.3	37/2(-)
9782.4 23 ?	Y			1405?	100		8377.4	(37/2)
9922.4 23	Y	(43/2-)		223 788	70 10 100 13	M1	9699.4 9134.4	(39/2-,41/2-) (41/2-)
10955.4 25	Y			1033	100		9922.4	(43/2-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7435.3+X	Y		1.5 µs 5
11059	G K	5/2+	13 keV 5
11981 5	K T U	1/2+	90 keV 9
≈12171	U		24 keV
12503	G K	3/2+	38 keV 3
12570 40	G	7/2+,9/2+
12993	K	1/2+	42 keV 3
13090 40	G	9/2-,11/2-
13542	K		68 keV 5
13581	K	3/2+	45 keV 5
13839	K	3/2+	63 keV 3
14091	K		30 keV 3
14363	K	5/2+	51 keV 5
14477	K	7/2-	43 keV 7
16400 50	O	-	5.05 MeV

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 1 - π=- MIXED SYMMETRY STATES.
1779.27 17	(5/2-)	73 fs +30-19
1840.07 17	3/2-,5/2-	71 fs +24-17	1029.6 2 1153.4 2	20 4 100 4	(M1+E2) M1+E2	810.32 686.79	5/2- 3/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 2 - K=37/2 OBLATE M1 BAND?
7435.3 21	37/2(-)
7828.3 23	39/2(-)		393	100	M1	7435.3	37/2(-)
8325.4 25	41/2(-)		497	100	D	7828.3	39/2(-)
8940 3	(43/2-)		615	100	M1	8325.4	41/2(-)
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 3 - π=- 2-PHONON IS STATES.
1284.26 13	(5/2)-	0.17 ps +6-4
1395.42 13	(7/2-)	> 0.55 ps	584.97 22 708.6 2	100 4 9 4	D+Q [E2]	810.32 686.79	5/2- 3/2-
1499.94 6	(9/2-)	0.84 ps 22	520.9 1 689.6 1 756.1 1 1499.9 1	2 2 18 3 6.9 10 100 2	[E1] [E2] [E1] (E1(+M2))	978.91 810.32 743.95 0.0	11/2+ 5/2- 7/2+ 9/2+
1571.82 14	3/2-	0.19 ps +15-7	287.4 2 761.4 2 885.1 2	20 5 100 5 37 5	M1+E2 M1+E2	1284.26 810.32 686.79	(5/2)- 5/2- 3/2-
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 4 - π=+ 1-PHONON IV STATES.
1297.22 6	9/2+	0.21 ps 3
1315.50 11	5/2+	0.37 ps +31-12	506.7 2 571.5 2	23.5 12 100.0 25	M1+E2 M1+E2	808.82 743.95	5/2+ 7/2+
1483.58 7	7/2(+)	45.7 fs 24	400.8 1 674.8 1 1483.46 16	8.2 18 24.4 15 100.0 16	(M1+E2) (M1+E2)	1082.68 808.82 0.0	9/2+ 5/2+ 9/2+
1603.44 9	11/2+	0.32 ps +17-9	520.9 2 624.4 2 653.6 2 859.5 2 1603.5 2	13 3 33.0 15 100 3 26 4 23 3	(M1(+E2)) (M1+E2) M1+E2 [E2]	1082.68 978.91 949.80 743.95 0.0	9/2+ 11/2+ 13/2+ 7/2+ 9/2+
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ)	I(γ)	M(γ)	Final Levels
Band 5 - π 1g_9/2~#(2⁺,⁹²Zr).
743.95 5	7/2+	0.51 ps 4
808.82 7	5/2+	6.16 ps 20	64.88 18 808.53 12	1.25 8 100.00 8	(M1) E2	743.95 0.0	7/2+ 9/2+
949.80 3	13/2+	4.36 ps 15	949.81 3	100	E2	0.0	9/2+
978.91 5	11/2+	258 fs 18	978.94 14	100	M1+E2	0.0	9/2+
1082.68 5	9/2+	> 2.8 ps	103.80 11 338.73 7 1082.53 15	9 3 100.0 17 35 3	(E2+M1) M1+E2	978.91 743.95 0.0	11/2+ 7/2+ 9/2+

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	9/2+	STABLE	Q=-0.32 2, μ=+6.1705 3 Δ<r²>(^91gIβ normalization,⁹³Nb)=+0.312 2 (2009Ch25) from LASER spectroscopy (optical pumping in ion beam cooler buncher); authors also report isotope shift and hfs coefficients. E(level): Δ<r²>(^91gIβ normalization,⁹³Nb)=+0.312 2 (2009Ch25) from LASER spectroscopy (optical pumping in ion beam cooler buncher); authors also report isotope shift and hfs coefficients.
686.79	3/2-	0.28 ps +48-14	E(level): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p_1/2^-1)#(first 2⁺ state in ⁹⁴Mo) (2006Or09).
743.95	7/2+	0.51 ps 4	E(level): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. π 1g_9/2~#(2⁺,⁹²Zr).
808.82	5/2+	6.16 ps 20	Other T_1/2: >2.8 ps from (α,pγ). E(level): Other T_1/2: >2.8 ps from (α,pγ). From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. π 1g_9/2~#(2⁺,⁹²Zr).
810.32	5/2-	> 1.0 ps	E(level): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p_1/2^-1)#(first 2⁺ state in ⁹⁴Mo) (2006Or09).
949.80	13/2+	4.36 ps 15	E(level): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. π 1g_9/2~#(2⁺,⁹²Zr).
978.91	11/2+	258 fs 18	E(level): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. π 1g_9/2~#(2⁺,⁹²Zr).
1082.68	9/2+	> 2.8 ps	E(level): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. π 1g_9/2~#(2⁺,⁹²Zr).
1127.09	3/2,5/2,7/2		E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
1284.26	(5/2)-	0.17 ps +6-4	E(level): π=- 2-PHONON IS STATES. T_1/2(level): From DSAM in (n,n’γ).
1290	1/2-,3/2-		XREF: H(1320)L(1279).
1297.22	9/2+	0.21 ps 3	E(level): π=+ 1-PHONON IV STATES.
1315.50	5/2+	0.37 ps +31-12	XREF: γ(1330). E(level): π=+ 1-PHONON IV STATES. T_1/2(level): From DSAM in (n,n’γ).
1335.04	17/2+	< 14 ns	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
1369.86	5/2-	> 0.55 ps	T_1/2(level): From DSAM in (n,n’γ).
1395.42	(7/2-)	> 0.55 ps	E(level): π=- 2-PHONON IS STATES. T_1/2(level): From DSAM in (n,n’γ).
1455.0	(1/2+,3/2+)		E(level): From (p,2nγ). J^π(level): From statistical analysis in (n,n’γ).
1483.58	7/2(+)	45.7 fs 24	E(level): π=+ 1-PHONON IV STATES.
1490.99	15/2+	< 14 ns	Other T_1/2: >0.52 ps from (n,n’γ). E(level): Other T_1/2: >0.52 ps from (n,n’γ). Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
1499.94	(9/2-)	0.84 ps 22	E(level): π=- 2-PHONON IS STATES.
1571.82	3/2-	0.19 ps +15-7	E(level): π=- 2-PHONON IS STATES. T_1/2(level): From DSAM in (n,n’γ).
1588.06	3/2(-),5/2(-)	> 0.87 ps	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
1603.24	(9/2-)		Possibly the same level as that adopted at 1603.8 keV even though Jπ from (n,n’γ) differs. E(level): Possibly the same level as that adopted at 1603.8 keV even though Jπ from (n,n’γ) differs.
1603.44	11/2+	0.32 ps +17-9	E(level): π=+ 1-PHONON IV STATES.
1665.66	5/2+	0.24 ps +7-5	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
E(level)	J^π(level)	T_1/2(level)	Comments
1679.50	5/2(+),7/2	0.22 ps +6-4	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
1683.36	9/2+	104 fs +17-14	T_1/2(level): From DSAM in (n,n’γ).
1686.34	13/2+	0.17 ps +4-3	T_1/2(level): From DSAM in (n,n’γ).
1703.51	3/2+,5/2+	0.15 ps +19-6	XREF: γ(1710). E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
1772.96	(LE7/2)	87 fs +14-10	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
1779.27	(5/2-)	73 fs +30-19	E(level): From ⁸⁰Se(¹⁶O,p2nγ). Uncertainty in Eγ unstated by authors. π=- MIXED SYMMETRY STATES.
1784.40	(5/2+)		E(level): From (p,2nγ). J^π(level): From statistical analysis in (n,n’γ).
1812.34	(19/2)	104 fs +35-24	T_1/2(level): From DSAM in (n,n’γ).
1840.07	3/2-,5/2-	71 fs +24-17	E(level): From ⁸⁰Se(¹⁶O,p2nγ). Uncertainty in Eγ unstated by authors. π=- MIXED SYMMETRY STATES.
1910.68	7/2+,9/2+,11/2+	162 fs 13	E(level): Isovector excitation is proposed by 2010Or01 for this state in (p,2nγ).
1915.92	7/2	62 fs 7	E(level): Isovector excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
1947.73	3/2,5/2,7/2	0.16 ps +9-5	T_1/2(level): From DSAM in (n,n’γ).
1949.72	(7/2+)	0.5 ps +11-2	E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level. Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
1949.81	(11/2)	0.6 ps +26-3	E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level. T_1/2(level): From DSAM in (n,n’γ).
1968.27	(13/2-)		E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level.
1968.87	11/2+	111 fs 19	E(level): Two levels at essentially the same energy are proposed in (n,n’γ) near 1950 keV and 1968 keV because, in each case, the authors were unable to fit experimental data for all the attributed γ rays (based on γγ coin) by means of a statistical theory excitation function for a single level. Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
1997.12	3/2-,5/2-	64 fs +15-12	T_1/2(level): From DSAM in (n,n’γ).
2002.52	(11/2+)	> 0.55 ps	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
2019.7	(7/2-,9/2-)		E(level): From (p,2nγ). J^π(level): From statistical analysis in (n,n’γ).
2023.91	(LE5/2)-	54 fs +28-17	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
2099.23	(3/2-,5/2,7/2)	92 fs +43-25	T_1/2(level): From DSAM in (n,n’γ).
2122.67	9/2+	97 fs 16	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ).
2126.89	(5/2-,7/2,9/2-)	0.16 ps +12-8	T_1/2(level): From DSAM in (n,n’γ).
2153.60	(1/2,3/2,5/2-)	80 fs +19-14	E(level): From (p,2nγ). J^π(level): From statistical analysis in (n,n’γ). T_1/2(level): From DSAM in (n,n’γ).
2162.64	(11/2+,13/2,15/2+)	0.28 ps +21-9	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
E(level)	J^π(level)	T_1/2(level)	Comments
2170.65	9/2+	0.24 ps +11-6	E(level): Isoscalar excitation is proposed by 2010Or01 for this state in (p,2nγ). T_1/2(level): From DSAM in (n,n’γ).
2184.14		76 ps +31-21	T_1/2(level): From DSAM in (n,n’γ).
2280.7	(7/2-)		E(level): From (p,2nγ). J^π(level): From statistical analysis in (n,n’γ).
2838	11/2		XREF: B(2810).
3086.0	(21/2)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
3150			XREF: C(3050).
3674.0	(25/2)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
4403.0	(29/2)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
6464.3	11/2(+)		Γ_γ=0.038 17 Γ_γ: from (γ,γ’) E=6465 keV. E(level): Γ_γ: from (γ,γ’) E=6465 keV.
7372.3	(35/2-)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
7435.3	37/2(-)		E(level): K=37/2 OBLATE M1 BAND?. J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
7828.3	39/2(-)		E(level): K=37/2 OBLATE M1 BAND?. J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
8325.4	41/2(-)		E(level): K=37/2 OBLATE M1 BAND?. J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
8377.4	(37/2)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
8940	(43/2-)		E(level): K=37/2 OBLATE M1 BAND?. J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
9134.4	(41/2-)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
9425	(45/2+)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
9922.4	(43/2-)		J^π(level): Based on value suggested in (¹⁶O,p4nγ) but, in some cases, the evaluator shows the resulting Jπ values in parentheses here.
11059	5/2+	13 keV 5	Γ_p0=4 keV 2. E(level): From (p,2nγ). T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
11981	1/2+	90 keV 9	E(level): From (p,2nγ). T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
12171		24 keV	Analog of possible ⁹³Zr(1169 level) (1972Ri04). E(level): Analog of possible ⁹³Zr(1169 level) (1972Ri04).
12503	3/2+	38 keV 3	Γ_p0=8.0 keV 8. E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45). J^π(level): From partial wave analysis of analyzing power in ⁹²Zr(pol p,p) IAR. T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
12993	1/2+	42 keV 3	Γ_p0=10 keV 1. E(level): From (p,2nγ). T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
13542		68 keV 5	E(level): From (p,2nγ). T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
13581	3/2+	45 keV 5	E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45). J^π(level): From partial wave analysis of analyzing power in ⁹²Zr(pol p,p) IAR. T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
E(level)	J^π(level)	T_1/2(level)	Comments
13839	3/2+	63 keV 3	Γ_p0=14.0 keV 14. E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45). J^π(level): From partial wave analysis of analyzing power in ⁹²Zr(pol p,p) IAR. T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
14091		30 keV 3	E(level): From (p,2nγ). T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
14363	5/2+	51 keV 5	Γ_p0\|<2.0 keV. E(level): From (p,2nγ). γ emitted within 1.3 ps of formation of parent state (2007Wa45). J^π(level): From partial wave analysis of analyzing power in ⁹²Zr(pol p,p) IAR. T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
14477	7/2-	43 keV 7	Γ_p0=2.0 keV 3. E(level): From (p,2nγ). T_1/2(level): From Zr(p,p’), (pol p,p) IAR.
16400	-	5.05 MeV	GDR. Γ from (γ,xn). E(level): GDR. Γ from (γ,xn).

E(level)	E(gamma)	Comments
30.77	30.77	E(γ): from IT decay M(γ): from α(K)exp and subshell ratios in IT decay.
686.79	655.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (α,pγ); Δπ=no from level scheme.
743.95	744.06	E(γ): weighted average of 743.82 17 from (n,n’γ), 743.92 16 from from Coulomb excitation and 744.2 1 from (p,2nγ). M(γ): from γ(θ) in Coulomb excitation and RUL.
808.82	64.88	E(γ): weighted average of 65.0 2 from (p,2nγ) and 64.6 3 from Coulomb excitation. I(γ): from Coulomb excitation. Other: <1.0 from (p,2nγ). M(γ): d from RUL; Δπ=no from level scheme.
808.82	808.53	E(γ): weighted average of 808.42 22 from (n,n’γ) and 808.58 15 from Coulomb excitation. I(γ): from Coulomb excitation. M(γ): Q from (¹⁶O,p2nγ); not M2 from RUL.
810.32	123.3	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
949.80	949.81	E(γ): from ε decay (6.85 h). M(γ): Q from (¹⁶O,p2nγ); not M2 from RUL.
978.91	978.94	E(γ): weighted average of 978.83 22 from (n,n’γ) and 979.01 18 from Coulomb excitation. Other Eγ: 979.3 1 from (p,2nγ). M(γ): D+Q from γ(θ) in Coulomb excitation; not E1⁺M2 from RUL.
1082.68	103.80	E(γ): weighted average of 103.7 2 from (p,2nγ), 103.94 15 from (n,n’γ) and 103.5 3 from Coulomb excitation. I(γ): unweighted average of 10.9 9 from Coulomb excitation, 3 2 from (p,2nγ) and 14.4 24 from (n,n’γ). The weighted average from (n,n’γ) and Coulomb excitation is 10.1 22.
	338.73	E(γ): weighted average of 338.67 17 from (n,n’γ), 338.77 9 from Coulomb excitation and 338.6 2 from (p,2nγ). I(γ): weighted average from (p,2nγ) and Coulomb excitation. M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
	1082.53	E(γ): weighted average of 1082.3 3 from (n,n’γ), 1082.6 3 from Coulomb excitation and 1082.6 2 from (p,2nγ). I(γ): unweighted average of 29 4, 30.9 15 and 40.0 23 from Coulomb excitation, 38 2 from (p,2nγ). Others: 51.5 15, 37, 33, and 18 6 from (n,n’γ). The weighted average of all data is 39 4. M(γ): d(+Q) from (n,n’γ); not E1⁺M2 from RUL.
1127.09	318.3	E(γ): from (p,2nγ). 318.27 17 from (n,n’γ) for triplet, 318.16 20 from Coulomb excitation for doublet.
1284.26	473.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	597.3	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=no from RUL.
	1253.5	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): not M2 from RUL.
1297.22	318.3	E(γ): from (p,2nγ). 318.27 17 from (n,n’γ) for triplet, 318.16 20 from Coulomb excitation for doublet. I(γ): unweighted average of 32.1 19 and 61 3 from Coulomb excitation, 53 2 from (n,n’γ), 31 5 from (p,2nγ). The weighted average is 44 7. M(γ): d(+Q) from (n,n’γ) and Coulomb excitation; adopted Δπ=no.
	553.10	E(γ): weighted average of 553.07 25 from (n,n’γ), 553.3 4 from Coulomb excitation and 553.1 1 from (p,2nγ). I(γ): weighted average of 49 4 and 57 6 from Coulomb excitation, 51 2 from (n,n’γ), 61 5 from (p,2nγ). M(γ): d(+Q) from (n,n’γ); adopted Δπ=no.
	1297.38	E(γ): weighted average of 1297.2 4 from (n,n’γ), 1297.3 3 from Coulomb excitation and 1297.4 1 from (p,2nγ). I(γ): weighted average of 100 6 and 100 6 from Coulomb excitation, 100 4 from (n,n’γ), 100 5 from (p,2nγ). M(γ): D+Q from (p,2nγ); not E1⁺M2 from RUL.
1315.50	506.7	M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=no from RUL.
1315.50	571.5	M(γ): D+Q from (p,2nγ); Δπ=(no) from level scheme.
1335.04	385.224	E(γ): weighted average of 385.22 2, 385.38 9 from ε decay (6.85 h), 385.07 17 from (n,n’γ) and 385.1 2 from (p,2nγ). M(γ): Q from (¹⁶O,p2nγ); not M2 from RUL.
1369.86	559.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
1369.86	683.2	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
1395.42	584.97	I(γ): from (p,2nγ). M(γ): D+Q from γ(θ) in (n,n’γ) and γγ(θ) in (p,2nγ).
1395.42	708.6	E(γ): From (p,2nγ). I(γ): from (p,2nγ). However, values of 54 and 43 are reported in (n,n’γ).. From (p,2nγ).
E(level)	E(gamma)	Comments
1483.58	400.8	E(γ): From (p,2nγ). I(γ): weighted average of 7 2 from (p,2nγ) and 11 3 from (n,n’γ).. From (p,2nγ).
	674.8	E(γ): from (p,2nγ). I(γ): weighted average of 23.5 12 from (n,n’γ) and 27 2 from (p,2nγ).
	1483.46	E(γ): weighted average of 1482.8 4 from (n,n’γ) and 1483.5 1 from (p,2nγ). Other: 1483.8 2 from 2010Or01 in (p,2nγ). I(γ): weighted average from (n,n’γ) and (p,2nγ).
1490.99	155.94	E(γ): from ε decay (6.85 h). I(γ): average of 22.3 20 from ε decay (6.85 h), 30.2 21 from ⁸²Se(¹⁶O,p4nγ) and 14 2 from (p,2nγ).
1490.99	541.29	M(γ): D+Q from (p,2nγ); M1 from ⁸²Se(¹⁶O,p4nγ).
1499.94	520.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	689.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): not M2 from RUL.
	756.1	E(γ): from (p,2nγ). I(γ): weighted average of 8 2 from (p,nγ) and 6.5 12 from (n,n’γ).
	1499.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): d(+Q) from γ(θ) in (n,n’γ); Δπ=yes from level scheme.
1571.82	287.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	761.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ); not E1⁺M2 from RUL.
	885.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ); not E1⁺M2 from RUL.
1588.06	777.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); large δ favors Δπ=no.
1588.06	901.2	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
1603.44	520.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): d(+Q) from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
	624.4	I(γ): weighted average of 33.3 18 from (n,n’γ) and 32 3 from (p,2nγ). M(γ): from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
	653.6	M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	859.5	E(γ): from (p,2nγ). I(γ): unweighted average of 29.8 18 from (n,n’γ) and 22 3 from (p,2nγ). M(γ): not M2 from RUL.
	1603.5	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
1665.66	856.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	921.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ) and (n,n’γ); Δπ=no from RUL.
	1665.7	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
1679.50	364.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): from (p,2nγ).
	382.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	870.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	935.7	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): from (p,2nγ).
	1679.58	E(γ): weighted average of 1679.7 2 from (p,2nγ) and 1679.1 4 from (n,n’γ). I(γ): weighted average of 38 2 from 1973Va09 in (n,n’γ) and 36 3 from (p,nγ).
E(level)	E(gamma)	Comments
1683.36	600.7	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	704.2	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	939.3	I(γ): weighted average from (n,n’γ) and (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	1683.2	I(γ): weighted average of 58.3 21 (1973Va09) in (n,n’γ) and 54 4 from (p,2nγ). M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
1686.34	707.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	736.5	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1686.3	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): not M2 from RUL.
1694.0	950	E(γ): order of 744γ and 950γ not known from (n,n’γ).
1703.51	387.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): d(+Q) from (p,2nγ); Δπ=no from level scheme.
1703.51	894.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
1772.96	646.0	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): M2 and higher-order multipolarity excluded by RUL.
1772.96	964.0	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): M2 and higher-order multipolarity excluded by RUL.
1779.27	969.0	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): d(+Q) from (p,2nγ); Δπ=(no) from level scheme.
1779.27	1092.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): d(+Q) from (p,2nγ); Δπ=(no) from level scheme.
1812.34	477.3	E(γ): for doubly-placed γ.. From (p,2nγ). I(γ): From (p,2nγ).
1840.07	1029.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ); Δπ=(no) from level scheme.
1840.07	1153.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL for either possible value of δ.
1910.68	613.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); Δπ=(no) from level scheme.
	828.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	1910.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γ(θ) in (n,n’γ); not E1⁺M2 from RUL.
1915.92	600.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	833.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1107.2	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1172.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1915.5	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
E(level)	E(gamma)	Comments
1947.73	1137.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): from (p,2nγ).
1949.72	270.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	866.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	971.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1140.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ); Δπ=(no) from level scheme.
	1205.9	E(γ): from (p,2nγ). I(γ): weighted average of 85 6 from (n,n’γ) and 92 5 from (p,2nγ).
1949.81	266.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	346.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1949.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
1968.27	365.0	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
1968.27	477.3	E(γ): for doubly-placed γ.. From (p,2nγ). I(γ): From (p,2nγ).
1968.87	282.5	E(γ): from (p,2nγ). I(γ): weighted average of 18 5 from (n,n’γ) and 27 5 from (p,2nγ).
	285.4	E(γ): from (p,2nγ). I(γ): weighted average of 21 6 from (n,n’γ) and 34 5 from (p,2nγ).
	990.0	E(γ): From (p,2nγ). I(γ): note that branching from (n,n’γ) varies widely (34 6 (1973Va09), 127 (1992De08), 48 (1983Av05)).. From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	1019.0	I(γ): weighted average of 28 3 from (n,n’γ) and 38 5 from (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	1225.0	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): M2 and higher-order multipolarity excluded by RUL.
	1968.9	E(γ): from (p,2nγ). I(γ): weighted average of 100 6 from (n,n’γ) and 100 5 from (p,2nγ).
1997.12	1186.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
1997.12	1310.2	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (n,n’γ); Δπ=no from level scheme.
2002.52	399.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	502.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	511.5	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1023.7	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1052.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γ(θ) in (n,n’γ); large δ favors Δπ=no.
2012.41	440.4	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2012.41	1325.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
E(level)	E(gamma)	Comments
2023.91	452.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2023.91	1337.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
2099.23	703.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2099.23	1288.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2122.67	639.0	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1143.7	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	1378.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from γγ(θ) in (p,2nγ); not E1⁺M2 from RUL.
	2122.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): D+Q from (p,2nγ); Δπ=no from level scheme.
2126.89	626.9	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	731.3	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1316.61	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1383.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2153.60	2122.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2162.64	671.7	E(γ): from (p,2nγ). I(γ): weighted average of 25 4 from (p,2nγ) and 22 6 from (n,n’γ).
	1183.7	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1212.8	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2170.65	1087.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1192.5	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
	1221.6	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): M2 and higher-order multipolarity excluded by RUL.
	1361.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ). M(γ): M2 and higher-order multipolarity excluded by RUL.
	1426.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2180.04	689.053	M(γ): from (¹⁶O,p4nγ).. From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
2184.14	849.1	E(γ): From (p,2nγ). I(γ): From (p,2nγ).
2203.5	808.3	E(γ): for doublet in (n,n’γ).
2310.9	976	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
E(level)	E(gamma)	Comments
2506.88	1527.9	E(γ): from (p,2nγ).
2506.88	2506.9	E(γ): from (p,2nγ).
2832.8	522	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
2832.8	1497.6	E(γ): from (¹⁶O,p2nγ). I(γ): from (¹⁶O,p4nγ). M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
3086.0	906	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
3667.8	835	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
3674.0	588	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
3684.8	852	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
4104.7	420	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
4104.7	1271.9	E(γ): from (¹⁶O,p2nγ). I(γ): from (¹⁶O,p4nγ). M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
4403.0	729	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
4864.6	759.9	E(γ): From ⁸⁰Se(¹⁶O,p2nγ). Uncertainty in Eγ unstated by authors. I(γ): From ⁸⁰Se(¹⁶O,p2nγ). Uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
5155.1	1481	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
5904.3	1039.7	E(γ): From ⁸⁰Se(¹⁶O,p2nγ). Uncertainty in Eγ unstated by authors. I(γ): From ⁸⁰Se(¹⁶O,p2nγ). Uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
6464.3	5516	E(γ): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p_1/2^-1)#(first 2⁺ state in ⁹⁴Mo) (2006Or09). M(γ): Mult=d (probably M1), from (γ,γ’) E=6465 keV.
6464.3	6465	E(γ): Interpreted in (p,2nγ) as symmetric one-phonon state with configuration of (π p_1/2^-1)#(first 2⁺ state in ⁹⁴Mo) (2006Or09). M(γ): Mult=d (probably M1), from (γ,γ’) E=6465 keV.
7372.3	1468	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
7435.3	1531	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
7828.3	393	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.. γ emitted within 1.3 ps of formation of parent state (2007Wa45). I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
8325.4	497	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.. γ emitted within 1.3 ps of formation of parent state (2007Wa45). I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
8377.4	942	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
8377.4	1005	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
8940	615	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.. γ emitted within 1.3 ps of formation of parent state (2007Wa45). I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
9134.4	1699	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
9425	485	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
E(level)	E(gamma)	Comments
9699.4	2264	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
9782.4	1405	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
9922.4	223	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.
9922.4	788	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. M(γ): From γ(θ), DCO ratio and/or linear polarization in ⁸²Se(¹⁶O,p4nγ).
10955.4	1033	E(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors. I(γ): From ⁸²Se(¹⁶O,p4nγ); uncertainty in Eγ unstated by authors.