List of levels for 31P

Authors: Jun Chen and Balraj Singh | Citation: Nucl. Data Sheets 184, 29 (2022) | Cutoff date: 24-Jun-2022

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1266.08	3/2+	510 fs 24	1266.1 1	M1+E2	+0.26 3	3.32×10^-5	B(E2)(W.u.)=3.7 +9-8, B(M1)(W.u.)=0.0199 10, α=3.32E-5 5, α(K)=1.681E-5 24, α(L)=1.252E-6 18, α(M)=9.51E-8 14
2233.63	5/2+	256 fs 17	2233.6 1	E2		0.000436	B(E2)(W.u.)=6.69 +48-44, α=0.000436 6, α(K)=6.92E-6 10, α(L)=5.15E-7 7, α(M)=3.91E-8 5
3134.3	1/2+	7.1 fs 4	1868.1	[M1,E2]		0.000231	α=0.000231 30, α(K)=9.0×10^-6 6, α(L)=6.7E-7 4, α(M)=5.09E-8 32
3134.3	1/2+	7.1 fs 4	3134.1	(M1)		0.000717	B(M1)(W.u.)=0.098 +6-5, α=0.000717 10, α(K)=3.78×10^-6 5, α(L)=2.81E-7 4, α(M)=2.134E-8 30
3294.90	5/2+	85 fs 17	1061.5 2	M1+E2	+0.40 6		B(E2)(W.u.)=25 +10-7, B(M1)(W.u.)=0.039 +10-7
	5/2+	85 fs 17	2028.8 2	M1+E2	+0.42 2	0.000276	B(E2)(W.u.)=3.9 +10-7, B(M1)(W.u.)=0.021 +5-4, α=0.000276 4, α(K)=7.51E-6 11, α(L)=5.59E-7 8, α(M)=4.25E-8 6
	5/2+	85 fs 17	3294.4 7	[E2]		0.000912	B(E2)(W.u.)=0.028 +8-6, α=0.000912 13, α(K)=3.67E-6 5, α(L)=2.73E-7 4, α(M)=2.075E-8 29
3414.58	7/2+	208 fs 56	1181.0 2	M1+E2	-0.35 7	2.57×10^-5	B(E2)(W.u.)=0.64 +38-25, B(M1)(W.u.)=0.0017 +7-4, α=2.57E-5 5, α(K)=1.94E-5 4, α(L)=1.443E-6 27, α(M)=1.097E-7 21
	7/2+	208 fs 56	2148.4 1	E2		0.000395	B(E2)(W.u.)=9.9 +38-21, α=0.000395 6, α(K)=7.41E-6 10, α(L)=5.51E-7 8, α(M)=4.19E-8 6
	7/2+	208 fs 56	3414.4	[M3]		0.000457	α=0.000457 6, α(K)=6.27×10^-6 9, α(L)=4.66E-7 7, α(M)=3.55E-8 5
3506.1	3/2+	8.8 fs +16-12	1272.3	(M1(+E2))	+0.05 11	3.33×10^-5	B(E2)(W.u.)<5.01, B(M1)(W.u.)<0.074, α=3.33E-5 5, α(K)=1.639E-5 25, α(L)=1.220E-6 19, α(M)=9.27E-8 14
	3/2+	8.8 fs +16-12	2239.9	(M1(+E2))	-0.06 19	0.000352	B(E2)(W.u.)<5.9, B(M1)(W.u.)=0.088 25, α=0.000352 7, α(K)=6.31E-6 9, α(L)=4.69E-7 7, α(M)=3.57E-8 5
	3/2+	8.8 fs +16-12	3505.9	M1+E2	+0.41 3	0.000878	B(E2)(W.u.)=1.74 +37-35, B(M1)(W.u.)=0.0287 +47-45, α=0.000878 13, α(K)=3.23E-6 5, α(L)=2.400E-7 34, α(M)=1.824E-8 26
4191.01	5/2+	4.9 fs 21	1957.2 6	(M1(+E2))	+0.09 14	0.000237	B(E2)(W.u.)<16, B(M1)(W.u.)=0.15 +14-6, α=0.000237 4, α(K)=7.84E-6 12, α(L)=5.83E-7 9, α(M)=4.43E-8 7
4191.01	5/2+	4.9 fs 21	2924.7 6	M1+E2	-0.12 5	0.000637	B(E2)(W.u.)=1.0 +14-7, B(M1)(W.u.)=0.13 +10-4, α=0.000637 9, α(K)=4.19E-6 6, α(L)=3.11E-7 4, α(M)=2.366E-8 33
4260.4	3/2+	10.4 fs 42	2994.1	M1+E2	+0.25 5	0.000670	B(E2)(W.u.)=0.7 +6-3, B(M1)(W.u.)=0.023 +15-8, α=0.000670 10, α(K)=4.05E-6 6, α(L)=3.01E-7 4, α(M)=2.291E-8 32
4260.4	3/2+	10.4 fs 42	4260.1	M1+E2	+0.35 4	1.13×10^-3	B(E2)(W.u.)=0.50 +36-17, B(M1)(W.u.)=0.017 +11-5, α=1.13E-3 2, α(K)=2.449E-6 34, α(L)=1.820E-7 26, α(M)=1.383E-8 19
4430.84	7/2-	0.424 ps 31	239.8 2	[E1]			B(E1)(W.u.)=0.00087 +19-18
	7/2-	0.424 ps 31	1016.4 1	(E1)			B(E1)(W.u.)=6.8E-5 +11-10
	7/2-	0.424 ps 31	1135.7 2	(E1+M2)	-0.04 3	3.75×10^-5	B(E1)(W.u.)=4.30E-4 +38-34, B(M2)(W.u.)=2.5 +50-22, α=3.75E-5 5, α(K)=1.274E-5 20, α(L)=9.48E-7 15, α(M)=7.20E-8 11
	7/2-	0.424 ps 31	1296.9	[E3]		4.80×10^-5	α=4.80×10^-5 7, α(K)=3.74E-5 5, α(L)=2.79E-6 4, α(M)=2.117E-7 30
	7/2-	0.424 ps 31	2197.0 2	(E1+M2)	-0.03 2	0.000782	B(E1)(W.u.)=8.0E-5 +7-6, B(M2)(W.u.)=0.07 +12-6, α=0.000782 11, α(K)=4.46E-6 6, α(L)=3.31E-7 5, α(M)=2.52E-8 4
	7/2-	0.424 ps 31	3164.6 7	[M2]		0.000516	B(M2)(W.u.)=0.51 13, α=0.000516 7, α(K)=5.26×10^-6 7, α(L)=3.91E-7 5, α(M)=2.97E-8 4
	7/2-	0.424 ps 31	4431.0 7	[E3]		1.02×10^-3	B(E3)(W.u.)=13.1 +28-26, α=1.02E-3 1, α(K)=3.06E-6 4, α(L)=2.275E-7 32, α(M)=1.729E-8 24
4592.5	3/2+	13 fs 4	2358.6	[M1,E2]		0.00045	α=0.00045 5, α(K)=6.06×10^-6 26, α(L)=4.50E-7 19, α(M)=3.42E-8 14
	3/2+	13 fs 4	3326.2	M1+E2	-0.8 4	0.00084	B(E2)(W.u.)=4.1 +29-27, B(M1)(W.u.)=0.016 +10-6, α=0.00084 4, α(K)=3.52E-6 6, α(L)=2.62E-7 5, α(M)=1.99E-8 4
	3/2+	13 fs 4	4592.1	(M1+E2)		0.00129	α=0.00129 8, α(K)=2.23×10^-6 4, α(L)=1.659E-7 32, α(M)=1.261E-8 25
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
4633.58	7/2+	70 fs 14	1128.1	[E2]		3.19×10^-5	B(E2)(W.u.)<48, α=3.19E-5 4, α(K)=2.75E-5 4, α(L)=2.049E-6 29, α(M)=1.556E-7 22
	7/2+	70 fs 14	1218.8 4	M1+E2	+0.33 6	2.84×10^-5	B(E2)(W.u.)=18 +8-6, B(M1)(W.u.)=0.055 +14-10, α=2.84E-5 5, α(K)=1.822E-5 31, α(L)=1.356E-6 23, α(M)=1.030E-7 18
	7/2+	70 fs 14	1339.2 4	M1+E2	+0.38 4	4.49×10^-5	B(E2)(W.u.)=13.6 +45-32, B(M1)(W.u.)=0.038 +10-7, α=4.49E-5 7, α(K)=1.542E-5 23, α(L)=1.148E-6 17, α(M)=8.72E-8 13
	7/2+	70 fs 14	1499.9	[M3]		5.07×10^-5	α=5.07×10^-5 7, α(K)=3.83E-5 5, α(L)=2.86E-6 4, α(M)=2.173E-7 30
	7/2+	70 fs 14	2399.7 5	(M1+E2)	+0.45 6	0.000435	B(E2)(W.u.)=0.75 +27-20, B(M1)(W.u.)=0.0048 +12-8, α=0.000435 7, α(K)=5.74E-6 8, α(L)=4.27E-7 6, α(M)=3.24E-8 5
	7/2+	70 fs 14	3367.6 7	[E2]		0.000941	B(E2)(W.u.)=0.095 +39-31, α=0.000941 13, α(K)=3.55E-6 5, α(L)=2.64E-7 4, α(M)=2.007E-8 28
	7/2+	70 fs 14	4633.8	[M3]		0.000785	α=0.000785 11, α(K)=3.58×10^-6 5, α(L)=2.66E-7 4, α(M)=2.023E-8 28
4784.7	5/2+	6.9 fs 28	1368.8	[M1,E2]		5.7×10^-5	α=5.7×10^-5 9, α(K)=1.61E-5 17, α(L)=1.20E-6 13, α(M)=9.1E-8 10
	5/2+	6.9 fs 28	1488.4	(M1(+E2))	+0.04 10	7.38×10^-5	B(E2)(W.u.)<22, B(M1)(W.u.)=0.30 +28-12, α=7.38E-5 11, α(K)=1.243E-5 18, α(L)=9.25E-7 13, α(M)=7.03E-8 10
	5/2+	6.9 fs 28	1649.1	[E2]		0.0001636	B(E2)(W.u.)<22, α=0.0001636 23, α(K)=1.214E-5 17, α(L)=9.04E-7 13, α(M)=6.87E-8 10
	5/2+	6.9 fs 28	2549.5	(M1+E2)		0.00053	α=0.00053 5, α(K)=5.34×10^-6 20, α(L)=3.97E-7 15, α(M)=3.02E-8 11
	5/2+	6.9 fs 28	3517.1	[M1,E2]		0.00093	α=0.00093 7, α(K)=3.26×10^-6 8, α(L)=2.42E-7 6, α(M)=1.84E-8 5
	5/2+	6.9 fs 28	4783.0	E2		1.43×10^-3	B(E2)(W.u.)=2.3 +15-7, α=1.43E-3 2, α(K)=2.139E-6 30, α(L)=1.589E-7 22, α(M)=1.208E-8 17
5014.9	(3/2+)	40 fs 12	1508.8	[M1,E2]		9.3×10^-5	α=9.3×10^-5 14, α(K)=1.33E-5 12, α(L)=9.9E-7 9, α(M)=7.5E-8 7
	(3/2+)	40 fs 12	1719.8	[M1,E2]		0.000170	α=0.000170 24, α(K)=1.04×10^-5 8, α(L)=7.8E-7 6, α(M)=5.9E-8 4
	(3/2+)	40 fs 12	3748.5	[M1,E2]		0.00101	α=0.00101 7, α(K)=2.97×10^-6 7, α(L)=2.21E-7 5, α(M)=1.68E-8 4
	(3/2+)	40 fs 12	5014.5	(M1(+E2))	-0.2 5	0.00134	B(E2)(W.u.)<0.28, B(M1)(W.u.)=0.0030 +18-15, α=0.00134 5, α(K)=1.959E-6 31, α(L)=1.455E-7 23, α(M)=1.106E-8 17
5015.2	3/2-	7.6 fs 51	1880.8	[E1]		0.000563	B(E1)(W.u.)=0.00030 +34-14, α=0.000563 8, α(K)=5.56E-6 8, α(L)=4.14E-7 6, α(M)=3.14E-8 4
	3/2-	7.6 fs 51	3748.8	[E1]		1.58×10^-3	B(E1)(W.u.)=0.0011 +13-5, α=1.58E-3 2, α(K)=2.224E-6 31, α(L)=1.653E-7 23, α(M)=1.256E-8 18
	3/2-	7.6 fs 51	5014.8	[E1]		2.02×10^-3	B(E1)(W.u.)=0.00021 +23-11, α=2.02E-3 3, α(K)=1.575E-6 22, α(L)=1.170E-7 16, α(M)=8.89E-9 12
5115.2	5/2+	10.4 fs 44	1701.3	M1+E2	+1.6 11	0.000173	B(E2)(W.u.)=57 +36-37, B(M1)(W.u.)=0.015 +27-9, α=0.000173 24, α(K)=1.10E-5 8, α(L)=8.2E-7 6, α(M)=6.2E-8 5
	5/2+	10.4 fs 44	1820.9	[M1,E2]		0.000211	α=0.000211 28, α(K)=9.4×10^-6 6, α(L)=7.0E-7 5, α(M)=5.33E-8 35
	5/2+	10.4 fs 44	2882.1	M1+E2	+0.65 55	0.00065	B(E2)(W.u.)=3.2 +42-27, B(M1)(W.u.)=0.014 +11-7, α=0.00065 4, α(K)=4.35E-6 9, α(L)=3.23E-7 7, α(M)=2.46E-8 5
	5/2+	10.4 fs 44	3849.6	M1+E2	+0.30 6	0.000992	B(E2)(W.u.)=0.44 +37-19, B(M1)(W.u.)=0.016 +11-5, α=0.000992 15, α(K)=2.82E-6 4, α(L)=2.095E-7 29, α(M)=1.592E-8 22
	5/2+	10.4 fs 44	5115.5	[E2]		1.52×10^-3	B(E2)(W.u.)<0.25, α=1.52E-3 2, α(K)=1.951E-6 27, α(L)=1.449E-7 20, α(M)=1.102E-8 15
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
5256.8	1/2+	≤ 10 fs	1842.1	[M3]		7.34×10^-5	α=7.34×10^-5 10, α(K)=2.329E-5 33, α(L)=1.737E-6 24, α(M)=1.320E-7 18
5256.8	1/2+	≤ 10 fs	5256.3	(M1)		1.41×10^-3	B(M1)(W.u.)≥0.014, α=1.41×10^-3 2, α(K)=1.838E-6 26, α(L)=1.366E-7 19, α(M)=1.038E-8 15
5342.84	9/2+	38 fs 11	709.4 2	[M1+E2]			B(M1)(W.u.)=0.021 +9-5
	9/2+	38 fs 11	1928.0 1	(M1(+E2))	+0.04 6	0.0002250	B(E2)(W.u.)<1.1, B(M1)(W.u.)=0.064 +32-18, α=0.0002250 32, α(K)=8.03E-6 11, α(L)=5.97E-7 8, α(M)=4.54E-8 6
	9/2+	38 fs 11	2048.3 4	E2		0.000347	B(E2)(W.u.)=4.0 +19-11, α=0.000347 5, α(K)=8.07E-6 11, α(L)=6.00E-7 8, α(M)=4.56E-8 6
	9/2+	38 fs 11	3110.2 8	E2		0.000836	B(E2)(W.u.)=0.97 +43-24, α=0.000836 12, α(K)=4.01E-6 6, α(L)=2.98E-7 4, α(M)=2.268E-8 32
	9/2+	38 fs 11	4076.5	[M3]		0.000640	α=0.000640 9, α(K)=4.50×10^-6 6, α(L)=3.35E-7 5, α(M)=2.54E-8 4
5530.0	(5/2)+	11 fs 5	2115.3	M1+E2	+1.0 5	0.000340	B(E2)(W.u.)=35 +29-23, B(M1)(W.u.)=0.036 +38-17, α=0.000340 24, α(K)=7.26E-6 23, α(L)=5.40E-7 18, α(M)=4.11E-8 13
5530.0	(5/2)+	11 fs 5	3296.0	M1+E2	+0.12 5	0.000782	B(E2)(W.u.)=0.09 +13-6, B(M1)(W.u.)=0.016 +12-5, α=0.000782 11, α(K)=3.51E-6 5, α(L)=2.61E-7 4, α(M)=1.984E-8 28
5772.7	7/2+	22 fs 9	1139.3	[M1+E2]		2.8×10^-5	B(M1)(W.u.)=0.08 +6-3, α=2.8×10^-5 4, α(K)=2.34E-5 34, α(L)=1.75E-6 26, α(M)=1.33E-7 20
	7/2+	22 fs 9	1513.1	[E2]		0.0001090	B(E2)(W.u.)<52, α=0.0001090 15, α(K)=1.444E-5 20, α(L)=1.075E-6 15, α(M)=8.17E-8 11
	7/2+	22 fs 9	1582.6	[M1,E2]		0.000119	α=0.000119 18, α(K)=1.22×10^-5 10, α(L)=9.1E-7 8, α(M)=6.9E-8 6
	7/2+	22 fs 9	2267.3	[E2]		0.000453	B(E2)(W.u.)<8.6, α=0.000453 6, α(K)=6.74E-6 9, α(L)=5.01E-7 7, α(M)=3.81E-8 5
	7/2+	22 fs 9	2358.0 10	[M1,E2]		0.00045	α=0.00045 5, α(K)=6.06×10^-6 26, α(L)=4.51E-7 19, α(M)=3.42E-8 15
	7/2+	22 fs 9	2639.1	[M3]		0.0002413	α=0.0002413 34, α(K)=1.051×10^-5 15, α(L)=7.83E-7 11, α(M)=5.95E-8 8
	7/2+	22 fs 9	3539.5	[M1,E2]		0.00094	α=0.00094 7, α(K)=3.23×10^-6 8, α(L)=2.40E-7 6, α(M)=1.83E-8 4
	7/2+	22 fs 9	4507.0	[E2]		1.35×10^-3	B(E2)(W.u.)=0.44 +33-15, α=1.35E-3 2, α(K)=2.323E-6 33, α(L)=1.726E-7 24, α(M)=1.312E-8 18
	7/2+	22 fs 9	5772.9	[M3]		1.05×10^-3	α=1.05×10^-3 2, α(K)=2.465E-6 35, α(L)=1.833E-7 26, α(M)=1.393E-8 20
5892.1	9/2+	24 fs 8	2477.3 6	M1+E2	+0.23 6	0.000457	B(E2)(W.u.)=0.18 +15-9, B(M1)(W.u.)=0.0047 +25-15, α=0.000457 7, α(K)=5.41E-6 8, α(L)=4.02E-7 6, α(M)=3.06E-8 4
	9/2+	24 fs 8	2596.8	[E2]		0.000609	B(E2)(W.u.)<1.6, α=0.000609 9, α(K)=5.36E-6 8, α(L)=3.98E-7 6, α(M)=3.03E-8 4
	9/2+	24 fs 8	3658.2 5	E2		1.05×10^-3	B(E2)(W.u.)=5.1 +25-13, α=1.05E-3 2, α(K)=3.14E-6 4, α(L)=2.332E-7 33, α(M)=1.772E-8 25
	9/2+	24 fs 8	4625.4	[M3]		0.000783	α=0.000783 11, α(K)=3.59×10^-6 5, α(L)=2.67E-7 4, α(M)=2.029E-8 28
6046.4	7/2+	22 fs 12	1412.2	[M1+E2]		6.6×10^-5	B(M1)(W.u.)=0.051 +51-24, α=6.6×10^-5 10, α(K)=1.51E-5 15, α(L)=1.13E-6 12, α(M)=8.6E-8 9
	7/2+	22 fs 12	1615.2	[E1]		0.000365	B(E1)(W.u.)=0.00035 +40-19, α=0.000365 5, α(K)=7.01E-6 10, α(L)=5.21E-7 7, α(M)=3.96E-8 6
	7/2+	22 fs 12	1785.9	[E2]		0.0002229	B(E2)(W.u.)=6 +7-3, α=0.0002229 31, α(K)=1.040E-5 15, α(L)=7.74E-7 11, α(M)=5.88E-8 8
	7/2+	22 fs 12	2631.7	(M1(+E2))	-0.4 6	0.00053	B(E2)(W.u.)<20, B(M1)(W.u.)=0.019 +42-13, α=0.00053 4, α(K)=4.95E-6 14, α(L)=3.68E-7 10, α(M)=2.80E-8 8
	7/2+	22 fs 12	2751.3	[M1,E2]		0.00062	α=0.00062 6, α(K)=4.73×10^-6 16, α(L)=3.52E-7 12, α(M)=2.67E-8 9
	7/2+	22 fs 12	3812.3	M1+E2	+1.2 6	0.00105	B(E2)(W.u.)=0.6 +5-4, B(M1)(W.u.)=0.0013 +18-7, α=0.00105 5, α(K)=2.91E-6 5, α(L)=2.16E-7 4, α(M)=1.644E-8 30
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
6078.53	9/2+	22 fs 12	1444.4 9	M1+E2	+0.13 8	6.34×10^-5	B(E2)(W.u.)=2.2 +47-19, B(M1)(W.u.)=0.06 +6-3, α=6.34E-5 11, α(K)=1.313E-5 20, α(L)=9.77E-7 15, α(M)=7.43E-8 11
	9/2+	22 fs 12	2664.1	[M1,E2]		0.00058	α=0.00058 6, α(K)=4.98×10^-6 17, α(L)=3.70E-7 13, α(M)=2.81E-8 10
	9/2+	22 fs 12	2783.7	[E2]		0.000693	B(E2)(W.u.)=1.5 +17-8, α=0.000693 10, α(K)=4.78E-6 7, α(L)=3.56E-7 5, α(M)=2.70E-8 4
	9/2+	22 fs 12	3844.6 2	E2		1.12×10^-3	B(E2)(W.u.)=3.3 +31-12, α=1.12E-3 2, α(K)=2.92E-6 4, α(L)=2.167E-7 30, α(M)=1.647E-8 23
	9/2+	22 fs 12	4812.3	[M3]		0.000830	α=0.000830 12, α(K)=3.35×10^-6 5, α(L)=2.491E-7 35, α(M)=1.894E-8 27
6233.4	(7/2)+		3098.9	[M3]		0.000368	α=0.000368 5, α(K)=7.58×10^-6 11, α(L)=5.64E-7 8, α(M)=4.29E-8 6
6399.0	7/2(-)	27 fs 12	1283.0	[E1]		0.0001244	B(E1)(W.u.)=0.00058 +49-23, α=0.0001244 17, α(K)=1.022E-5 14, α(L)=7.61E-7 11, α(M)=5.78E-8 8
	7/2(-)	27 fs 12	1967.7	(M1(+E2))	+0.15 14	0.000242	B(E2)(W.u.)=2.1 +66-18, B(M1)(W.u.)=0.08 +6-3, α=0.000242 5, α(K)=7.79E-6 12, α(L)=5.79E-7 9, α(M)=4.40E-8 7
	7/2(-)	27 fs 12	2208.0	[E1]		0.000789	B(E1)(W.u.)<1.8E-4, α=0.000789 11, α(K)=4.42E-6 6, α(L)=3.29E-7 5, α(M)=2.497E-8 35
	7/2(-)	27 fs 12	2984.2	[E1]		1.24×10^-3	B(E1)(W.u.)=1.8E-5 +15-7, α=1.24E-3 2, α(K)=2.96E-6 4, α(L)=2.197E-7 31, α(M)=1.670E-8 23
	7/2(-)	27 fs 12	3103.8	[E1]		1.30×10^-3	B(E1)(W.u.)=5.3E-5 +44-21, α=1.30E-3 2, α(K)=2.81E-6 4, α(L)=2.090E-7 29, α(M)=1.588E-8 22
	7/2(-)	27 fs 12	3264.5	[E3]		0.000644	α=0.000644 9, α(K)=5.13×10^-6 7, α(L)=3.81E-7 5, α(M)=2.90E-8 4
	7/2(-)	27 fs 12	4164.9	[E1]		1.74×10^-3	B(E1)(W.u.)=1.0E-5 +9-4, α=1.74E-3 2, α(K)=1.959E-6 27, α(L)=1.456E-7 20, α(M)=1.106E-8 15
	7/2(-)	27 fs 12	6398.3	[E3]			B(E3)(W.u.)<69
6453.49	11/2+	23 fs 12	1110.2 3	M1+E2	+0.27 3	2.41×10^-5	B(E2)(W.u.)=19 +18-7, B(M1)(W.u.)=0.07 +6-3, α=2.41E-5 4, α(K)=2.149E-5 32, α(L)=1.601E-6 24, α(M)=1.216E-7 18
	11/2+	23 fs 12	1819.6 6	[E2]		0.0002382	B(E2)(W.u.)=4.8 +43-17, α=0.0002382 33, α(K)=1.004E-5 14, α(L)=7.47E-7 10, α(M)=5.68E-8 8
	11/2+	23 fs 12	3039.3 4	E2		0.000806	B(E2)(W.u.)=14 +12-5, α=0.000806 11, α(K)=4.16E-6 6, α(L)=3.09E-7 4, α(M)=2.351E-8 33
	11/2+	23 fs 12	4220.6	[M3]		0.000679	α=0.000679 10, α(K)=4.22×10^-6 6, α(L)=3.14E-7 4, α(M)=2.388E-8 33
6501.3	9/2-	38 fs 14	2070.6 5	M1+E2	+1.3 3	0.000330	B(E2)(W.u.)=36 +20-12, B(M1)(W.u.)=0.021 +16-7, α=0.000330 11, α(K)=7.63E-6 14, α(L)=5.68E-7 11, α(M)=4.31E-8 8
6501.3	9/2-	38 fs 14	3086.4 6	[E1]		1.29×10^-3	B(E1)(W.u.)=1.0E-4 +6-3, α=1.29E-3 2, α(K)=2.83E-6 4, α(L)=2.105E-7 29, α(M)=1.600E-8 22
6796.0	9/2-	139 fs 41	2364.8 6	M1+E2	+0.29 4	0.000411	B(E2)(W.u.)=0.54 +30-17, B(M1)(W.u.)=0.0081 +34-19, α=0.000411 6, α(K)=5.83E-6 8, α(L)=4.33E-7 6, α(M)=3.29E-8 5
6796.0	9/2-	139 fs 41	3380.8 6	(E1)		1.42×10^-3	B(E1)(W.u.)=3.5E-5 +16-9, α=1.42E-3 2, α(K)=2.526E-6 35, α(L)=1.877E-7 26, α(M)=1.426E-8 20
6823.91	11/2-	62 fs 26	1480.8 2	E1		0.000260	B(E1)(W.u.)=0.0013 +9-4, α=0.000260 4, α(K)=8.05E-6 11, α(L)=5.98E-7 8, α(M)=4.55E-8 6
	11/2-	62 fs 26	2393.8 3	E2		0.000513	B(E2)(W.u.)=12 +8-4, α=0.000513 7, α(K)=6.14E-6 9, α(L)=4.57E-7 6, α(M)=3.47E-8 5
	11/2-	62 fs 26	3529.0	[E3]		0.000737	α=0.000737 10, α(K)=4.47×10^-6 6, α(L)=3.33E-7 5, α(M)=2.528E-8 35
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
6931.4	5/2+	< 28 fs	2500.1	[E1]		0.000970	B(E1)(W.u.)>1.5E-4, α=0.000970 14, α(K)=3.73E-6 5, α(L)=2.77E-7 4, α(M)=2.106E-8 29
	5/2+	< 28 fs	4697.2	M1+E2	-1.3 3	1.34×10^-3	B(E2)(W.u.)>0.54, B(M1)(W.u.)>0.0015, α=1.34E-3 3, α(K)=2.172E-6 31, α(L)=1.614E-7 23, α(M)=1.227E-8 18
	5/2+	< 28 fs	6930.6	[E2]			B(E2)(W.u.)>9.5E-7
7117.7	9/2+	≤ 17 fs	3703.1	M1+E2	-0.18 2	0.000932	B(E2)(W.u.)≥0.21, B(M1)(W.u.)≥0.025, α=0.000932 13, α(K)=2.97E-6 4, α(L)=2.209E-7 31, α(M)=1.679E-8 24
7442.1	11/2+	12 fs 10	988.1 6	(M1(+E2))	+0.3 3
	11/2+	12 fs 10	4027.5 4	E2		1.18×10^-3	B(E2)(W.u.)=6 +7-3, α=1.18E-3 2, α(K)=2.73E-6 4, α(L)=2.026E-7 28, α(M)=1.540E-8 22
	11/2+	12 fs 10	5207	[M3]		0.000925	α=0.000925 13, α(K)=2.93×10^-6 4, α(L)=2.177E-7 30, α(M)=1.655E-8 23
7781.17	3/2-		4649.1 7	E1+M2	-0.05 2	1.91×10^-3	α=1.91×10^-3 3, α(K)=1.723E-6 24, α(L)=1.280E-7 18, α(M)=9.73E-9 14
7781.17	3/2-		7780.9 12	E1+M2	+0.045 5
7859.6	11/2(-)		2516.8 6	(E1)		0.000980	α=0.000980 14, α(K)=3.70×10^-6 5, α(L)=2.75E-7 4, α(M)=2.087E-8 29
7859.6	11/2(-)		3428.6 6	(E2)		0.000966	α=0.000966 14, α(K)=3.46×10^-6 5, α(L)=2.57E-7 4, α(M)=1.953E-8 27
8031.2	5/2+		3840.0	(M1)		0.000977	α=0.000977 14, α(K)=2.82×10^-6 4, α(L)=2.096E-7 29, α(M)=1.593E-8 22
8031.2	5/2+		4524.7	(M1+E2)	+0.033	1.20×10^-3	α=1.20×10^-3 2, α(K)=2.247E-6 31, α(L)=1.670E-7 23, α(M)=1.269E-8 18
8103.6	5/2+		3912.4	(M1+E2)	+0.06 1	1.00×10^-3	α=1.00×10^-3 1, α(K)=2.75E-6 4, α(L)=2.042E-7 29, α(M)=1.552E-8 22
8207.9	3/2+	2.6 eV 2	5973.5	(M1+E2)	+0.028 18	1.58×10^-3	α=1.58×10^-3 2, α(K)=1.555E-6 22, α(L)=1.156E-7 16, α(M)=8.78E-9 12
8224.4	7/2(-)		1825.3	(M1(+E2))	-0.11 28	0.000186	α=0.000186 7, α(K)=8.80×10^-6 19, α(L)=6.55E-7 14, α(M)=4.98E-8 11
8224.4	7/2(-)		4929.0	(E1+M2)	-0.03 1	2.00×10^-3	α=2.00×10^-3 3, α(K)=1.607E-6 23, α(L)=1.194E-7 17, α(M)=9.08E-9 13
8242.7	5/2-		2570.2	D(+Q)	+0.01 8
8242.7	5/2-		3811.2	(M1+E2)	-0.12 1	0.000968	α=0.000968 14, α(K)=2.85×10^-6 4, α(L)=2.119E-7 30, α(M)=1.611E-8 23
8343.5	(11/2+)	27 fs 7	4928.5 8	(E2)		1.47×10^-3	B(E2)(W.u.)=1.24 +44-26, α=1.47E-3 2, α(K)=2.052E-6 29, α(L)=1.525E-7 21, α(M)=1.159E-8 16
8355.6	5/2-		7088.6	(E1+M2)	+0.010 4
8414.2	11/2(-)		1590.1 5	(M1)		0.0001034	α=0.0001034 15, α(K)=1.109×10^-5 16, α(L)=8.25E-7 12, α(M)=6.27E-8 9
8414.2	11/2(-)		3983.3 7	(E2)		1.17×10^-3	α=1.17×10^-3 2, α(K)=2.77E-6 4, α(L)=2.058E-7 29, α(M)=1.564E-8 22
8433.9	7/2-		4242.7	(E1+M2)	+0.11 3	1.76×10^-3	α=1.76×10^-3 3, α(K)=1.932E-6 29, α(L)=1.435E-7 21, α(M)=1.091E-8 16
	7/2-		5138.4	(E1+M2)	+0.021 3	2.06×10^-3	α=2.06×10^-3 3, α(K)=1.531E-6 21, α(L)=1.138E-7 16, α(M)=8.65E-9 12
	7/2-		6199.4	(E1+M2)	+0.03 2
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
8461.0	5/2+	2 eV 1	4200.3	(M1(+E2))	-0.26 GT	0.00117	α=0.00117 7, α(K)=2.53×10^-6 5, α(L)=1.88E-7 4, α(M)=1.429E-8 29
	5/2+	2 eV 1	4954.5	(M1+E2)	+0.11 3	1.32×10^-3	α=1.32×10^-3 2, α(K)=1.989E-6 28, α(L)=1.478E-7 21, α(M)=1.123E-8 16
	5/2+	2 eV 1	5165.5	(M1(+E2))	+0.01 5	1.38×10^-3	α=1.38×10^-3 2, α(K)=1.881E-6 26, α(L)=1.398E-7 20, α(M)=1.062E-8 15
	5/2+	2 eV 1	6226.5	(M1+E2)	+0.100 11
	5/2+	2 eV 1	7194.0	(M1(+E2))	-0.02 3
8470.4	5/2		7203.4	D+Q	-0.06 3
8543.6	1/2-	54 eV 10	5408.8	(E1)		2.14×10^-3	α=2.14×10^-3 3, α(K)=1.443E-6 20, α(L)=1.072E-7 15, α(M)=8.15E-9 11
8555.4	3/2-	210 eV 25	3540	(M1+E2)	-0.09 8	0.000871	α=0.000871 13, α(K)=3.17×10^-6 4, α(L)=2.354E-7 33, α(M)=1.789E-8 25
8575.6	5/2+	7 eV 5	4314.9	(M1(+E2))	+0.28 33	1.14×10^-3	α=1.14×10^-3 3, α(K)=2.40E-6 4, α(L)=1.786E-7 27, α(M)=1.357E-8 21
	5/2+	7 eV 5	5069.1	(M1+E2)	+0.18 2	1.35×10^-3	α=1.35×10^-3 2, α(K)=1.930E-6 27, α(L)=1.434E-7 20, α(M)=1.090E-8 15
	5/2+	7 eV 5	5440.8	(E2(+M3))	-0.04 5	1.61×10^-3	α=1.61×10^-3 2, α(K)=1.796E-6 26, α(L)=1.335E-7 19, α(M)=1.014E-8 15
	5/2+	7 eV 5	6341.1	(M1+E2)	-0.09 5
	5/2+	7 eV 5	7308.5	(M1(+E2))	+0.01 1
8584.2	5/2(+)	50 eV 10	7317.1	(M1(+E2))	+0.008 6
8641.2	5/2+	5 eV 3	4450.0	(M1+E2)	+0.6	1.22×10^-3	α=1.22×10^-3 2, α(K)=2.316E-6 32, α(L)=1.721E-7 24, α(M)=1.308E-8 18
	5/2+	5 eV 3	5134.6	(M1(+E2))	+0.09 9	1.37×10^-3	α=1.37×10^-3 2, α(K)=1.896E-6 27, α(L)=1.409E-7 20, α(M)=1.071E-8 15
	5/2+	5 eV 3	5345.7	(M1+E2)	-0.13 6	1.43×10^-3	α=1.43×10^-3 2, α(K)=1.798E-6 25, α(L)=1.336E-7 19, α(M)=1.016E-8 14
	5/2+	5 eV 3	6406.7	(M1(+E2))	-0.03 4
	5/2+	5 eV 3	7374.1	(M1+E2)	-0.042 3
8649.5	3/2+		4458.3	(M1+E2)	-1.1 8	0.00126	α=0.00126 7, α(K)=2.33×10^-6 4, α(L)=1.731E-7 33, α(M)=1.315E-8 25
	3/2+		5354.0	(M1+E2)	+0.10 6	1.43×10^-3	α=1.43×10^-3 2, α(K)=1.794E-6 25, α(L)=1.333E-7 19, α(M)=1.013E-8 14
	3/2+		5514.7	(M1+E2)	-3.7 3	1.62×10^-3	α=1.62×10^-3 2, α(K)=1.760E-6 25, α(L)=1.308E-7 18, α(M)=9.94E-9 14
	3/2+		6415.0	(M1+E2)	-0.28 5
	3/2+		7382.4	(M1+E2)	+0.045 3
8705.23	(13/2-)	159 fs 28	1881.9 9	M1+E2	+0.20 6	0.0002090	B(E2)(W.u.)=0.8 +6-4, B(M1)(W.u.)=0.0154 +32-24, α=0.0002090 33, α(K)=8.40E-6 12, α(L)=6.25E-7 9, α(M)=4.75E-8 7
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
8729.1	3/2+		6494.6	(M1+E2)	-0.20 7
8730.5	3/2+		6496.0	(M1+E2)	-0.01 13
	3/2+		7463.4	(M1+E2)	+0.12 5
	3/2+		8729.2	(M1(+E2))	+0.02 2
8738.0	3/2+	20 eV 5	3178.9	(M1(+E2))	-0.15 19	0.000738	α=0.000738 15, α(K)=3.70×10^-6 5, α(L)=2.75E-7 4, α(M)=2.092E-8 30
	3/2+	20 eV 5	3722.9	D+Q	-0.75 28
	3/2+	20 eV 5	3954.3	(M1(+E2))	-0.02 15	1.02×10^-3	α=1.02×10^-3 2, α(K)=2.71E-6 4, α(L)=2.011E-7 28, α(M)=1.529E-8 21
	3/2+	20 eV 5	5442.5	(M1+E2)	-0.24 6	1.46×10^-3	α=1.46×10^-3 2, α(K)=1.758E-6 25, α(L)=1.306E-7 18, α(M)=9.93E-9 14
	3/2+	20 eV 5	5603.2	(M1+E2)	+20 14	1.65×10^-3	α=1.65×10^-3 2, α(K)=1.726E-6 24, α(L)=1.282E-7 18, α(M)=9.75E-9 14
	3/2+	20 eV 5	6503.5	(M1+E2)	-0.8 4
	3/2+	20 eV 5	7470.9	(M1+E2)	+1.2 6
	3/2+	20 eV 5	8736.7	(M1+E2)	-0.20 7
8757.3	5/2+	3 eV 2	5342.2	(M1+E2)	-0.13 2	1.43×10^-3	α=1.43×10^-3 2, α(K)=1.800E-6 25, α(L)=1.337E-7 19, α(M)=1.016E-8 14
	5/2+	3 eV 2	6522.8	(M1+E2)	+0.09 5
	5/2+	3 eV 2	7490.2	(M1+E2)	+0.206 3
8840.0	7/2-	1 eV 1	2440.9	(M1(+E2))	+0.07 9	0.000437	α=0.000437 6, α(K)=5.51×10^-6 8, α(L)=4.10E-7 6, α(M)=3.12E-8 4
8840.0	7/2-	1 eV 1	6605.4	(E1+M2)	+0.03 2
8902.9	1/2+	92 eV 15	5396.3	(M1+E2)		0.00152	α=0.00152 8, α(K)=1.795×10^-6 32, α(L)=1.334E-7 24, α(M)=1.014E-8 18
8909.7	5/2+	1 eV 1	3237.1	D(+Q)	-0.01 9
	5/2+	1 eV 1	3350.6	(M1(+E2))	+0.03 6	0.000801	α=0.000801 11, α(K)=3.43×10^-6 5, α(L)=2.55E-7 4, α(M)=1.936E-8 27
	5/2+	1 eV 1	7642.6	(M1+E2)	+0.07 1
8935.8	3/2+	3 eV 2	4152.1	(M1(+E2))		0.00115	α=0.00115 8, α(K)=2.57×10^-6 5, α(L)=1.91E-7 4, α(M)=1.451E-8 30
8935.8	3/2+	3 eV 2	6701.2	(M1+E2)	-0.17 5
9009	5/2+	70 eV 20	5502.5	(M1+E2)	+0.15 2	1.47×10^-3	α=1.47×10^-3 2, α(K)=1.731E-6 24, α(L)=1.286E-7 18, α(M)=9.78E-9 14
9009	5/2+	70 eV 20	6774.5	(M1+E2)	+0.64 10
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
9046.1	3/2-	9.2 keV 9	9044.7	(E1(+M2))	-0.008 5
9067.1	5/2+	16 eV 5	3536.9	(M1+E2)	+0.52 12	0.000899	α=0.000899 17, α(K)=3.20×10^-6 5, α(L)=2.376E-7 34, α(M)=1.806E-8 26
9067.1	5/2+	16 eV 5	6832.5	(M1+E2)	-0.07 1
9113.4	7/2-	1 eV 1	6878.8	(E1(+M2))	-0.01 3
9115.5	5/2+	22 eV 7	6880.9	(M1+E2)	-0.07 1
9128.5	5/2+	3 eV 2	6893.9	(M1+E2)	+1.18 9
9130.9	5/2+	4 eV 2	7863.7	(M1+E2)	-0.03 1
9154.2	7/2(-)		6919.6	(E1+M2)	+0.20 2
9156.2	3/2(+)		6921.6	(M1(+E2))	+0.08 10
9175.9	(13/2)-	83 fs 28	1733.7 6	(E1)		0.000455	B(E1)(W.u.)=1.5E-4 +8-5, α=0.000455 6, α(K)=6.28E-6 9, α(L)=4.67E-7 7, α(M)=3.55E-8 5
	(13/2)-	83 fs 28	2351.6 6	[M1,E2]		0.00045	α=0.00045 5, α(K)=6.09×10^-6 26, α(L)=4.53E-7 19, α(M)=3.44E-8 15
	(13/2)-	83 fs 28	2722.6 6	(E1)		1.10×10^-3	B(E1)(W.u.)=0.00029 +15-8, α=1.10E-3 2, α(K)=3.33E-6 5, α(L)=2.475E-7 35, α(M)=1.881E-8 26
9176.2	3/2-	83 eV 15	1394.5	(M1(+E2))	+0.07 2	5.26×10^-5	α=5.26×10^-5 7, α(K)=1.393E-5 20, α(L)=1.037E-6 15, α(M)=7.88E-8 11
	3/2-	83 eV 15	2565.5	(M1(+E2))	-0.05 2	0.000489	α=0.000489 7, α(K)=5.10×10^-6 7, α(L)=3.80E-7 5, α(M)=2.88E-8 4
	3/2-	83 eV 15	2839.3	(E1(+M2))	+0.01 2	1.17×10^-3	α=1.17×10^-3 2, α(K)=3.15E-6 4, α(L)=2.343E-7 33, α(M)=1.781E-8 25
	3/2-	83 eV 15	3616.9	(E1(+M2))	0.00 2	1.53×10^-3	α=1.53×10^-3 2, α(K)=2.324E-6 33, α(L)=1.727E-7 24, α(M)=1.312E-8 18
	3/2-	83 eV 15	4161	D(+Q)	0.00 1
	3/2-	83 eV 15	5880.4	(E1+M2)	+0.06 2	2.26×10^-3	α=2.26×10^-3 3, α(K)=1.315E-6 18, α(L)=9.76E-8 14, α(M)=7.42E-9 10
	3/2-	83 eV 15	6941.4	(E1+M2)	+0.11 2
	3/2-	83 eV 15	7908.8	(E1+M2)	+0.05 2
	3/2-	83 eV 15	9174.5	(E1+M2)	+0.07 1
9206.1	7/2+		5910.5	(M1+E2)	+0.10 8	1.57×10^-3	α=1.57×10^-3 2, α(K)=1.577E-6 22, α(L)=1.172E-7 16, α(M)=8.91E-9 12
9240.7	3/2+	150 eV 15	7006.0	(M1+E2)	+0.14 3
9312.9	(13/2+)		2859.4 6	D+Q	+0.25 10
9319.5	3/2(+)		9318.0	D+Q	+0.27 1
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
9412.4	7/2-	0.50 keV 8	5997.2	(E1(+M2))	+0.02 3	2.29×10^-3	α=2.29×10^-3 3, α(K)=1.284E-6 18, α(L)=9.53E-8 13, α(M)=7.25E-9 10
9448.9	5/2+	0.45 keV 5	8181.6	(M1+E2)	+0.13 2
9449.86	(13/2)-	35 fs 14	745.3 6	(M1)			B(M1)(W.u.)=0.6 +4-2
	(13/2)-	35 fs 14	1106.4 4	[E1]		2.84×10^-5	B(E1)(W.u.)=0.00037 +30-17, α=2.84E-5 4, α(K)=1.331E-5 19, α(L)=9.91E-7 14, α(M)=7.53E-8 11
	(13/2)-	35 fs 14	2007.8 7	[E1]		0.000654	B(E1)(W.u.)=0.00012 +10-6, α=0.000654 9, α(K)=5.06E-6 7, α(L)=3.76E-7 5, α(M)=2.86E-8 4
	(13/2)-	35 fs 14	2627.3 16	M1+E2	+0.2 GE	0.00057	B(M1)(W.u.)<0.023, α=0.00057 5, α(K)=5.10×10^-6 18, α(L)=3.79E-7 13, α(M)=2.88E-8 10
9476.9	(7/2-)		5970.2	[M2]		1.28×10^-3	α=1.28×10^-3 2, α(K)=1.916E-6 27, α(L)=1.424E-7 20, α(M)=1.083E-8 15
9524.6	3/2+	22.0 keV 22	5333.2	M1+E2	-0.58 4	1.46×10^-3	α=1.46×10^-3 2, α(K)=1.813E-6 25, α(L)=1.347E-7 19, α(M)=1.024E-8 14
9524.6	3/2+	22.0 keV 22	9523.0	(M1+E2)	+1.7 10
9536.4	5/2+	15 eV 10	2712.1	[E3]		0.000442	α=0.000442 6, α(K)=7.21×10^-6 10, α(L)=5.36E-7 8, α(M)=4.08E-8 6
	5/2+	15 eV 10	3081.5	[M3]		0.000363	α=0.000363 5, α(K)=7.66×10^-6 11, α(L)=5.70E-7 8, α(M)=4.33E-8 6
	5/2+	15 eV 10	7301.7	(M1+E2)	-0.03 1
9577.8	7/2(-)	22 eV 10	7343.1	(E1(+M2))	-0.04 2
9585.0	(1/2+,3/2-)	3.7 keV 4	8317.7	D+Q	+0.36 2
9585.0	(1/2+,3/2-)	3.7 keV 4	9583.4	D(+Q)	0.00 2
9593.8	3/2		8326.5	D(+Q)	-0.01 3
9598.5	3/2(-)		8331.2	D+Q	+0.84 6
9598.5	3/2(-)		9596.9	D(+Q)	0.00 2
9765.2	3/2-	0.30 keV 7	8497.8	(E1+M2)	-0.24 2
9843.6		50 eV 10	8576.2	D(+Q)	+0.01 4
9843.6		50 eV 10	9841.9	D+Q	+0.65 2
9852.3	(7/2)		7617.5	D+Q	+0.27 2
9865.8	7/2		7631.0	D+Q	+0.01 1
9867.8	3/2-	0.35 keV 4	9866.1	(E1(+M2))	+0.04 1
9925.8	3/2		9924.1	D+Q	+0.60 1
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
10019.7	5/2-	1 eV 1	8752.2	(E1+M2)	-0.11 2
10046	5/2-	0.22 keV 3	8779.3	(E1+M2)	-0.03 2
10193.0	3/2(+)		4300.8	[M3]		0.000700	α=0.000700 10, α(K)=4.08×10^-6 6, α(L)=3.04E-7 4, α(M)=2.309E-8 32
10193.0	3/2(+)		8925.5	D(+Q)	+0.02 7
10210.4	3/2		8942.9	D+Q	-0.27 3
10210.4	3/2		10208.6	D+Q	+0.11 3
10212			7977	D+Q	-0.05 2
10216.95	(15/2)-	76 fs 21	903.9 3	[E1]			B(E1)(W.u.)=0.00033 +14-9
	(15/2)-	76 fs 21	1041.7 7	M1+E2	+0.30 GE		B(M1)(W.u.)<0.088
	(15/2)-	76 fs 21	1511.7 5	[M1,E2]		9.4×10^-5	α=9.4×10^-5 14, α(K)=1.33E-5 12, α(L)=9.9E-7 9, α(M)=7.5E-8 7
	(15/2)-	76 fs 21	1802.8 5	[E2]		0.0002305	B(E2)(W.u.)=5.0 +21-14, α=0.0002305 32, α(K)=1.022E-5 14, α(L)=7.60E-7 11, α(M)=5.78E-8 8
	(15/2)-	76 fs 21	2139.6 5	[E2]		0.000391	B(E2)(W.u.)=1.9 +8-5, α=0.000391 5, α(K)=7.46E-6 10, α(L)=5.55E-7 8, α(M)=4.22E-8 6
	(15/2)-	76 fs 21	2356.8 6	[E2]		0.000496	B(E2)(W.u.)=1.7 +8-6, α=0.000496 7, α(K)=6.31E-6 9, α(L)=4.69E-7 7, α(M)=3.56E-8 5
	(15/2)-	76 fs 21	3392.8 6	E2		0.000951	B(E2)(W.u.)=1.4 +6-3, α=0.000951 13, α(K)=3.51E-6 5, α(L)=2.61E-7 4, α(M)=1.984E-8 28
10226	7/2		7990	D+Q	+0.04 2
10233	5/2		8964	D(+Q)	-0.05 6
10267	3/2		8999	D(+Q)	-0.04 9
10271	3/2		9003	D+Q	-0.12 2
10287	5/2		8052	D(+Q)	-0.02 4
10304	3/2		8068	D+Q	-0.65 18
10304	3/2		10301	D+Q	+0.23 5
10335	3/2		10332	D+Q	+0.18 3
10385	5/2		8149	D+Q	+0.40 14
10401	5/2		8165	D+Q	+0.23 18
10483	5/2		9214	D+Q	-0.42 25
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
10485	3/2		10482	D+Q	+0.19 1
10487	3/2		10484	D(+Q)	+0.02 3
10520.16	(15/2+)	0.67 ps 7	1070.1 4	[E1]			B(E1)(W.u.)=2.35E-4 +40-35
	(15/2+)	0.67 ps 7	1207.3 4	[M1,E2]		3.1×10^-5	α=3.1×10^-5 5, α(K)=2.08E-5 28, α(L)=1.55E-6 21, α(M)=1.17E-7 16
	(15/2+)	0.67 ps 7	1344.3 5	[E1]		0.0001651	B(E1)(W.u.)=5.0E-6 +19-17, α=0.0001651 23, α(K)=9.44E-6 13, α(L)=7.02E-7 10, α(M)=5.34E-8 7
	(15/2+)	0.67 ps 7	1815.2 7	(E1)		0.000516	B(E1)(W.u.)=9.6E-5 +13-11, α=0.000516 7, α(K)=5.86E-6 8, α(L)=4.36E-7 6, α(M)=3.31E-8 5
	(15/2+)	0.67 ps 7	2176.4 6	[E2]		0.000409	B(E2)(W.u.)=0.035 +10-9, α=0.000409 6, α(K)=7.24E-6 10, α(L)=5.39E-7 8, α(M)=4.09E-8 6
	(15/2+)	0.67 ps 7	3078.1 6	[E2]		0.000823	B(E2)(W.u.)=0.0128 +29-25, α=0.000823 12, α(K)=4.08E-6 6, α(L)=3.03E-7 4, α(M)=2.305E-8 32
	(15/2+)	0.67 ps 7	4066	[E2]		1.20×10^-3	B(E2)(W.u.)<0.0014, α=1.20E-3 2, α(K)=2.69E-6 4, α(L)=1.998E-7 28, α(M)=1.519E-8 21
10537	3/2		10535	D+Q	-0.07 3
10564	3/2		10562	D+Q	+0.63 9
10607	3/2		10605	D+Q	+0.35 3
10645	3/2		10643	D+Q	-0.18 5
10650	3/2		9382	D+Q	+0.08 5
10659	3/2	24 keV	10657	D+Q	-1.04 9
10672	5/2		9404	D+Q	+0.06 5
10698	3/2		10696	D+Q	+0.02 1
10703	3/2		10701	D+Q	+0.09 1
10706	3/2		10704	D+Q	-0.27 5
10774	3/2		10772	D(+Q)	+0.01 1
10801	3/2		10799	D+Q	+0.05 1
10818	3/2		9550	D+Q	-0.34 8
10818	3/2		10816	D+Q	+0.27 2
10834	3/2		10832	D+Q	+0.33 3
10882	3/2		10880	D+Q	+0.63 7
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
10948	3/2		10946	D+Q	+0.11 2
11075	3/2		11073	D+Q	-0.14 1
11135	3/2		11133	D+Q	+0.51 2
11173	5/2	< 20 keV	9904	D+Q	+0.042 7
11296.98	(17/2+)	1.32 ps 14	537.5 2	[E1]			B(E1)(W.u.)=1.89E-4 +50-44
	(17/2+)	1.32 ps 14	776.8 2	M1+E2	+0.17 10		B(E2)(W.u.)=3.3 +46-27, B(M1)(W.u.)=0.0154 22
	(17/2+)	1.32 ps 14	1080.3 3	[E1]			B(E1)(W.u.)=1.21E-4 +21-19
	(17/2+)	1.32 ps 14	1259.6 4	[E2]		4.33×10^-5	B(E2)(W.u.)=4.2 +8-7, α=4.33E-5 6, α(K)=2.136E-5 30, α(L)=1.591E-6 22, α(M)=1.209E-7 17
	(17/2+)	1.32 ps 14	1697	[E2]		0.0001840	B(E2)(W.u.)<0.061, α=0.0001840 26, α(K)=1.148E-5 16, α(L)=8.54E-7 12, α(M)=6.49E-8 9
	(17/2+)	1.32 ps 14	1984	[E2]		0.000316	B(E2)(W.u.)<0.028, α=0.000316 4, α(K)=8.55E-6 12, α(L)=6.36E-7 9, α(M)=4.83E-8 7
	(17/2+)	1.32 ps 14	4472.7 9	[E3]		1.03×10^-3	B(E3)(W.u.)=8.0 +30-27, α=1.03E-3 1, α(K)=3.01E-6 4, α(L)=2.241E-7 31, α(M)=1.703E-8 24

Mass measurements: 2009Kw02, 2008Re16, 2006Re19

Other measurements:

2018De02: ¹²C(¹⁹F,X) E=127 MeV at the Pelletron Linac Facility, Mumbai. Measured high-energy γ-ray spectra of giant dipole resonance (GDR). Deduced GDR parameters.

2018Mo22,2016Mo35: ²⁷Al(α,X) E=28, 35, 42 MeV at the Variable Energy Cyclotron Centre (VECC), Kolkata. Measured high-energy γ-ray spectra of GDR. Deduced GDR parameters. Systematic study of ground parameters.

2012Zh06: ⁹Be(⁴⁰Ar,X) E=57 MeV/nucleon. Measured fragment yield, momentum distributions at HIRFL facility; deduced target dependence on production cross section

1982Ve13: ³¹P(³He,³He) E=25 MeV. Measured σ(θ) Deduced optical model parameters, matter and charge radii.

1983Gl07: ³¹P(n,n) E=thermal, measured phase shift, scattering length

1968Bu10: ³¹P(α,α’) E-25 MeV. Measured σ(Eα,θ)

1972Ko36, 1962La26: measured hyperfine structure

Theoretical calculations: 73 primary references for structure retrieved from the NSR database (www.nndc.bnl.gov/nsr/) are listed under ’document records’.

Levels: Adopted proton pickup spectroscopic factors from 1977En02 evaluation listed below were averaged (by 1977En02) with corresponding neutron pickup spectroscopic factors for ³¹S

Q-value: S(2n)=23630.3 4, S(2p)=20810.7 3 (2021Wa16)

Q(β-)=-5398.01 keV 23	S(n)= 12311.01 keV 7	S(p)= 7296.553 keV 22	Q(α)= -9668.60 keV 5
Reference: 2021WA16

References:
A	³¹Si β^- decay (157.24 M)	B	³¹S ε decay (2.5534 S)
C	³²Cl εp decay (300.1 MS)	D	¹²C(²⁰Ne,pγ),¹⁶O(¹⁶O,pγ)
E	²⁰Ne(¹²C,p)	F	²⁴Mg(¹²C,αpγ)
G	²⁴Mg(¹⁶O,2APG)	H	²⁷Al(α,γ):Resonances
I	²⁷Al(α,p):Resonances	J	²⁷Al(⁶Li,d)
K	²⁸Si(α,p),⁴He(²⁸Si,p)	L	²⁸Si(α,pγ),⁴He(²⁸Si,pγ)
M	²⁸Si(¹⁸O,¹⁵N)	N	²⁸Si(¹⁹F,¹⁶O)
O	²⁹Si(³He,p)	P	²⁹Si(α,d)
Q	³⁰Si(p,γ)	R	³⁰Si(p,p):Resonances
S	³⁰Si(p,α):Resonances	T	³⁰Si(d,n)
U	³⁰Si(³He,d),(pol ³He,d)	V	³⁰Si(α,t)
W	³⁰Si(¹⁶O,¹⁵N)	X	³¹P(γ,γ’)
Y	³¹P(E,E’)	Z	³¹P(n,n’γ)
a	³¹P(p,p’)	b	³¹P(p,p’γ)
c	³¹P(d,d’)	d	³²S(γ,pγ’)
e	³²S(E,E’p)	f	³²S(n,d)
g	³²S(d,³He),(pol d,³He)	h	³²S(¹³C,¹⁴N)
i	³³S(p,³He)	j	³³S(d,α)
k	³⁴S(p,α)	l	Coulomb Excitation

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2+	STABLE	μ=+1.130925 5 (2011La24,2019StZV) g_J=-2.00165 39 (1964Pe11), atomic beam magnetic resonance.
1266.08	3/2+	510 fs 24	μ=+0.30 8 (1982Ho06,2020StZV), B(E2)=0.0070 8 Adopted (1977En02) proton stripping spectroscopic factor=0.97 14. E(level): Adopted (1977En02) proton stripping spectroscopic factor=0.97 14.
2233.63	5/2+	256 fs 17	μ=+2.8 6 (1982Ho06,2020StZV), B(E2)=0.0118 7 Adopted (1977En02) proton stripping spectroscopic factor=0.10 2. E(level): Adopted (1977En02) proton stripping spectroscopic factor=0.10 2.
3134.3	1/2+	7.1 fs 4	Adopted (1977En02) proton stripping spectroscopic factor=0.04 2. E(level): Adopted (1977En02) proton stripping spectroscopic factor=0.04 2.
3294.90	5/2+	85 fs 17	Adopted (1977En02) proton stripping spectroscopic factor<0.01. E(level): Adopted (1977En02) proton stripping spectroscopic factor<0.01. J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
3414.58	7/2+	208 fs 56	B(E2)\|^=0.0039 8 for 3415⁺3506 doublet in (e,e’). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
3506.1	3/2+	8.8 fs +16-12	Adopted (1977En02) proton stripping spectroscopic factor <0.01. E(level): Adopted (1977En02) proton stripping spectroscopic factor <0.01. J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
4191.01	5/2+	4.9 fs 21	Adopted (1977En02) proton stripping spectroscopic factor=0.03 2. E(level): Adopted (1977En02) proton stripping spectroscopic factor=0.03 2. J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
4260.4	3/2+	10.4 fs 42	Adopted (1977En02) proton stripping spectroscopic factor=0.06 2. E(level): Adopted (1977En02) proton stripping spectroscopic factor=0.06 2. J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
4430.84	7/2-	0.424 ps 31	Adopted (1977En02) proton stripping spectroscopic factor=0.45 7. E(level): Adopted (1977En02) proton stripping spectroscopic factor=0.45 7. J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
4592.5	3/2+	13 fs 4	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
4784.7	5/2+	6.9 fs 28	XREF: a(4740)k(4730). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
5342.84	9/2+	38 fs 11	XREF: a(5310).
5558.9	3/2+	< 17 fs	XREF: a(5600). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
5672.4	5/2	25 fs 6	XREF: a(5630). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
5892.1	9/2+	24 fs 8	XREF: d(5910).
5987.9	(3/2)+		XREF: L(?).
6158	(1/2,3/2,5/2)		XREF: t(6180?).
6399.0	7/2(-)	27 fs 12	XREF: a(6360). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
6668	(11/2-)		XREF: a(6690)i(6690).
6841.9	(5/2)-		XREF: U(6844.0).
6909.6	(3/2)-		XREF: U(6911.3).
6931.4	5/2+	< 28 fs	XREF: U(6933.2).
7079.9	(3/2)-		XREF: U(7082.4).
7214.3	1/2-,3/2-		XREF: k(7240).
E(level)	J^π(level)	T_1/2(level)	Comments
7347.1	(3/2)-		XREF: j(7356).
7572			XREF: i(7600).
7687.2			XREF: Q(?).
7717.2	(5/2)-		XREF: U(7719.4).
7781.17	3/2-		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
7859.6	11/2(-)		XREF: U(7863.8).
7897.9	1/2-	64 eV 9	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
7944.6	3/2+,5/2+		XREF: U(7946.2).
8031.2	5/2+		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8047.7	3/2-		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8076.91	11/2(-)		XREF: U(8078.0).
8103.6	5/2+		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8207.9	3/2+	2.6 eV 2	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8224.4	7/2(-)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8242.7	5/2-		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8355.6	5/2-		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8433.9	7/2-		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8461.0	5/2+	2 eV 1	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8470.4	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8543.6	1/2-	54 eV 10	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
8552.2	1/2+	0.31 keV 4	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
8555.4	3/2-	210 eV 25	XREF: t(8564). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
8575.6	5/2+	7 eV 5	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8584.2	5/2(+)	50 eV 10	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8641.2	5/2+	5 eV 3	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
E(level)	J^π(level)	T_1/2(level)	Comments
8649.5	3/2+		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8729.1	3/2+		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8730.5	3/2+		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8738.0	3/2+	20 eV 5	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
8757.3	5/2+	3 eV 2	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8763.3	1/2+	1.45 keV 15	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
8840.0	7/2-	1 eV 1	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8902.9	1/2+	92 eV 15	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
8909.7	5/2+	1 eV 1	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8935.8	3/2+	3 eV 2	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
8985.9	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9009	5/2+	70 eV 20	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9046.1	3/2-	9.2 keV 9	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9052.7	(5/2)+		XREF: O(9044).
9067.1	5/2+	16 eV 5	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9113.4	7/2-	1 eV 1	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9115.5	5/2+	22 eV 7	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9128.5	5/2+	3 eV 2	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9130.9	5/2+	4 eV 2	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9154.2	7/2(-)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9156.2	3/2(+)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9176.2	3/2-	83 eV 15	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9206.1	7/2+		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9226.3	1/2-	3.6 keV 5	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9240.7	3/2+	150 eV 15	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
E(level)	J^π(level)	T_1/2(level)	Comments
9290.8	3/2-	10.0 keV 8	parity from L(³He,d)=1 from 0⁺. J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9319.5	3/2(+)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9362	3/2-	10.0 keV 10	XREF: U(9353). J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9399.7	1/2+	0.50 keV 8	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9412.4	7/2-	0.50 keV 8	XREF: U(9406). J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9440.8	3/2(+)	180 eV 20	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9448.9	5/2+	0.45 keV 5	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9524.6	3/2+	22.0 keV 22	XREF: R(9522.2).
9536.4	5/2+	15 eV 10	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9570.5	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9579	3/2-	20.0 keV 20	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9593.8	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9598.5	3/2(-)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9659	(3/2,5/2)+		XREF: d(9680)g(9680).
9756.5	5/2+	3 eV 2	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9760.4	5/2+	20 eV 7	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9765	(3/2)+	0.20 keV 5	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9765.2	3/2-	0.30 keV 7	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9786	3/2-	50 keV 5	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9814	(5/2,7/2)-	12 eV 5	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9816.5	3/2-	150 eV 20	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9819.4	3/2-	4.5 keV 5	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9840.7	(7/2)-	66 eV 15	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9852.3	(7/2)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9865.8	7/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
E(level)	J^π(level)	T_1/2(level)	Comments
9867.8	3/2-	0.35 keV 4	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9925.8	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
9928	5/2+	170 eV 20	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9946.2	(5/2)-	125 eV 15	XREF: U(9950). J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9963.6	1/2+	5.0 keV 5	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
9999.4	1/2+	7.5 keV 11	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
10019.7	5/2-	1 eV 1	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10046	5/2-	0.22 keV 3	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ). From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
10092	1/2+	180 eV 20	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
10093	3/2-	270 eV 30	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
10116.5	1/2-	3.4 keV 3	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
10153.3	1/2+	3.9 keV 4	J^π(level): From R-Matrix analysis of experimental cross sections for resonances observed in ³⁰Si(p,p):resonances (1976Ou01).
10193.0	3/2(+)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10210.4	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10226	7/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10233	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10267	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10271	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10287	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10304	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10335	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10385	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10401	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10425	(1/2,3/2)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10483	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
E(level)	J^π(level)	T_1/2(level)	Comments
10485	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10487	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10537	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10564	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10607	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10645	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10650	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10659	3/2	24 keV	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10672	5/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10698	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10703	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10706	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10774	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10801	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10818	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10834	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10846	(1/2,3/2)		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10882	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
10948	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
11075	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
11135	3/2		J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
11173	5/2	< 20 keV	J^π(level): Spin from (p,γ), based on γ(θ) and γγ(θ), and RUL for strong transitions where measured T_1/2 is also available in (p,γ).
11282	3/2	< 8 keV	XREF: Q(11285). J^π(level): From measured p(θ) data in (α,p):resonances.
11317	(3/2,7/2-,9/2-)	< 6 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
11364		< 8 keV	XREF: Q(11363).
E(level)	J^π(level)	T_1/2(level)	Comments
11400		< 8 keV	XREF: Q(11392).
11605	3/2	10 keV 5	J^π(level): From measured p(θ) data in (α,p):resonances.
11654	(7/2-,9/2+)	< 5 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
11733	3/2	< 5 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
11929	3/2	< 5 keV	XREF: I(11931). J^π(level): From measured p(θ) data in (α,p):resonances.
12002	(3/2,7/2-)	< 6 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
12028	(3/2,7/2-)	< 8 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
12052	3/2	4 keV 2	J^π(level): From measured p(θ) data in (α,p):resonances.
12092.4	7/2-	< 3 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
12126	9/2+	< 5 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
12204	11/2-	< 3 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
12329	5/2-	6 keV 3	J^π(level): From measured p(θ) data in (α,p):resonances.
12447	7/2-	< 3 keV	J^π(level): From measured p(θ) data in (α,p):resonances.
12629	(3/2,5/2-,7/2)	< 6 keV	J^π(level): From measured α(θ) data in (p,α):resonances.
12643	5/2(-)	4 keV 2	J^π(level): From measured α(θ) data in (p,α):resonances.
12806	(3/2+,7/2-)	6 keV 3	J^π(level): From measured α(θ) data in (p,α):resonances.
12830	3/2	< 3 keV	J^π(level): From measured α(θ) data in (p,α):resonances.
13099	(5/2-,7/2-)	5 keV 2	J^π(level): From measured α(θ) data in (p,α):resonances.
13107	(3/2+,7/2-)	< 6 keV	J^π(level): From measured α(θ) data in (p,α):resonances.

E(level)	E(gamma)	Comments
1266.08	1266.1	E(γ): others: 1266.4 5 from (¹²C,αpγ) and 1266.1 4 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): From (²⁰Ne,pγ)
2233.63	967.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
2233.63	2233.6	E(γ): others: 2234.2 7 from (¹²C,αpγ) and 2233.5 4 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): from (¹⁶O,2αpγ)
3134.3	1868.1	I(γ): other: <5.9 from ³¹S ε decay
3134.3	3134.1	E(γ): other: 3133 5 from (γ,γ’) I(γ): other: 100.0 28 from ³¹S ε decay M(γ): D+Q with multiple δ(Q/d) values from γ(θ) in (p,γ’), but 1/2 to 1/2 transition should be pure dipole; M1 from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
3294.90	1061.5	E(γ): weighted average of 1061.6 2 from (²⁰Ne,pγ), 1061.9 5 from (¹²C,αpγ), and 1061.0 3 from (¹⁶O,2αpγ) I(γ): weighted average of 28.6 23 from (²⁰Ne,pγ), 38 10 from (¹²C,αpγ), 28.2 12 from (¹⁶O,2αpγ), 19.1 24 from (α,γ):resonances, 24 6 from (α,pγ), and 26.5 13 from (p,γ)
	2028.8	E(γ): others: 2028.9 6 from (¹²C,αpγ) and 2028.6 4 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): others: 100 6 from (²⁰Ne,pγ), 100 14 from (¹²C,αpγ), 100.0 35 from (¹⁶O,2αpγ), 100.0 24 from (α,γ):resonances, and 100 6 from (α,pγ)
	3294.4	E(γ): weighted average of 3293.6 12 from (¹²C,αpγ) and 3294.7 7 from (¹⁶O,2αpγ) I(γ): weighted average of 1.08 19 from (¹⁶O,2αpγ) and 1.41 26 from (p,γ)
3414.58	1181.0	E(γ): weighted average of 1180.9 2 from (²⁰Ne,pγ) and 1181.1 3 from (¹⁶O,2αpγ) I(γ): weighted average of 2.6 4 from (²⁰Ne,pγ), 3.20 27 from (¹⁶O,2αpγ), 4.2 11 from (α,pγ), and 2.5 5 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
3414.58	2148.4	E(γ): others: 2148.3 8 from (¹²C,αpγ) and 2148.6 4 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): others: 100 4 from (¹⁶O,2αpγ) and 100.0 11 from (α,pγ) M(γ): Q with ΔJ=2 from γγ(DCO) in (²⁰Ne,pγ), (¹²C,αpγ) and (¹⁶O,2αpγ); M2 ruled out by RUL
3506.1	2239.9	I(γ): weighted average of 67 11 from ³¹S ε decay, 56 6 from (α,pγ), and 75 4 from (p,γ)
3506.1	3505.9	I(γ): from (p,γ). Others: 100 6 from ³¹S ε decay (2.5534 s) and 100 6 from (α,pγ)
4191.01	1957.2	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 37 4 from (¹⁶O,2αpγ), 31.6 26 from (α,γ):resonances, 32 4 from (α,pγ), and 34.7 28 from (p,γ)
4191.01	2924.7	E(γ): From (¹⁶O,2αpγ) I(γ): from (α,γ):resonances. Others: 100 7 from (¹⁶O,2αpγ), 100 5 from (α,pγ), and 100.0 28 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
4260.4	2994.1	I(γ): unweighted average of 56 6 from (α,pγ) and 34.8 20 from (p,γ)
4260.4	4260.1	I(γ): from (p,γ). Other: 100 6 from (α,pγ)
4430.84	239.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1016.4	E(γ): others: 1016.5 5 from (¹²C,αpγ) and 1016.4 2 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): weighted average of 8.4 14 from (²⁰Ne,pγ), 8.6 11 from (¹⁶O,2αpγ), 7.3 18 from (α,γ):resonances, 7.7 28 from (p,γ), and 13 5 from (α,pγ) M(γ): d with ΔJ=0 from γγ(DCO) in (²⁰Ne,pγ), (¹²C,αpγ), and (¹⁶O,2αpγ); E1 from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
	1135.7	E(γ): weighted average of 1135.6 2 from (²⁰Ne,pγ), 1136.4 5 from (¹²C,αpγ), and 1135.7 3 from (¹⁶O,2αpγ) I(γ): weighted average of 64 4 from (²⁰Ne,pγ), 72 10 from (¹²C,αpγ), 87 5 from (¹⁶O,2αpγ), 75 4 from (α,γ):resonances, and 76 4 from (p,γ). Other: 109 9 from (α,pγ) is discrepant M(γ): D+Q and δ from γ(θ) in (p,γ); d with ΔJ=1 from γγ(DCO) in (²⁰Ne,pγ), (¹²C,αpγ), and (¹⁶O,2αpγ); E1⁺M2 from level scheme
	2197.0	E(γ): others: 2197.9 9 from (¹²C,αpγ) and 2197.0 4 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): from (²⁰Ne,pγ) and (¹⁶O,2αpγ). Other: 100 4 from (α,γ):resonances, 100 9 from (α,pγ), and 100 6 from (p,γ), 100 15 from (¹²C,αpγ). From (²⁰Ne,pγ) M(γ): D+Q and δ from γ(θ) in (p,γ); d with ΔJ=1 from γγ(DCO) in (²⁰Ne,pγ) and (¹⁶O,2αpγ); E1⁺M2 from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
	3164.6	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 4.8 11 from (¹⁶O,2αpγ) and 3.6 10 from (p,γ)
	4431.0	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 1.51 32 from (¹⁶O,2αpγ) and 1.9 4 from (p,γ)
4592.5	2358.6	I(γ): other: 31 5 from (α,pγ)
	3326.2	I(γ): other: 100 7 from (α,pγ)
	4592.1	I(γ): unweighted average of 31 5 from (α,pγ) and 46 4 from (p,γ)
E(level)	E(gamma)	Comments
4633.58	1218.8	E(γ): unweighted average of 1219.4 1 from (²⁰Ne,pγ), 1218.2 5 from (¹²C,αpγ), and 1218.8 3 from (¹⁶O,2αpγ) I(γ): others: 100 7 from (²⁰Ne,pγ), 100 4 from (¹⁶O,2αpγ), 100 9 from (α,γ):resonances, 100 5 from (α,pγ), 100 42 from (¹²C,αpγ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	1339.2	E(γ): weighted average of 1339.6 3 from (²⁰Ne,pγ), 1338.6 6 from (¹²C,αpγ), and 1338.7 4 from (¹⁶O,2αpγ) I(γ): others: 101 8 from (²⁰Ne,pγ), 70 16 from (¹²C,αpγ), 96 8 from (¹⁶O,2αpγ), and 92 8 from (α,pγ); 167 18 from (α,γ):resonances is discrepant M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	2399.7	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 68 8 from (¹⁶O,2αpγ), 88 10 from (α,γ):resonances, 56 10 from (α,pγ), and 72.7 28 from (p,γ)
	3367.6	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 10 4 from (¹⁶O,2αpγ), 7.7 26 from (α,pγ), and 8.3 28 from (p,γ)
	4633.8	I(γ): <11 from (p,γ) but from RUL expected value is 0.015, thus this transition most likely does not occur. γ not seen in (¹⁶O,2αpγ).
4784.7	1488.4	I(γ): weighted average of 74 7 from (α,γ):resonances, 76 9 from (α,pγ), and 73 5 from (p,γ)
	2549.5	I(γ): weighted average of 36 7 from (α,γ):resonances, 41 7 from (α,pγ), and 52 5 from (p,γ)
	3517.1	I(γ): unweighted average of 29 7 from (α,γ):resonances and 11 4 from (p,γ). Other: \|<17 from (α,pγ)
	4783.0	I(γ): others: 100 7 from (α,γ):resonances and 100 9 from (α,pγ)
5014.9	3748.5	I(γ): other: 33 7 from (α,pγ)
5014.9	5014.5	I(γ): other: 100 7 from (α,pγ)
5015.2	3748.8	I(γ): other: 100 13 from (α,pγ)
5015.2	5014.8	I(γ): unweighted average of 25 13 from (α,pγ) and 66 5 from (p,γ). Iγ from (α,pγ) is inconsistent.
5115.2	1701.3	I(γ): weighted average of 21 5 from (α,pγ) and 28 4 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	2882.1	I(γ): weighted average of 40 7 from (α,pγ) and 50 4 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	3849.6	I(γ): other: 100 7 from (α,pγ). See comment for 3845γ from 6078 level
5256.8	5256.3	E(γ): other: 5255 4 from (γ,γ’) M(γ): d from pγ(θ) in (α,pγ); M1 from level scheme
5342.84	709.4	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1928.0	E(γ): others: 1927.8 5 from (¹²C,αpγ) and 1928.4 4 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): from (p,γ). Others: 100 6 from (²⁰Ne,pγ), 100 4 from (¹⁶O,2αpγ), 100 20 from (α,γ):resonances, and 100 5 from (α,pγ)
	2048.3	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 8.6 12 from (¹⁶O,2αpγ), 9.8 25 from (α,pγ), and 4.9 12 from (p,γ). Other: 42 16 from (α,γ):resonances is discrepant M(γ): Q from γγ(ADO) in (¹⁶O,2αpγ) and pγ(θ) in (α,pγ); M2 ruled out by RUL
	3110.2	E(γ): weighted average of 3110.9 6 from (²⁰Ne,pγ) and 3109.4 6 from (¹⁶O,2αpγ) I(γ): unweighted average of 10.3 11 from (²⁰Ne,pγ), 14.0 9 from (¹⁶O,2αpγ), 12.2 25 from (α,pγ), and 18.5 25 from (p,γ). Other: 58 16 from (α,γ):resonances is discrepant M(γ): Q from γγ(ADO) in (¹⁶O,2αpγ) and pγ(θ) in (α,pγ); M2 ruled out by RUL
5530.0	2115.3	I(γ): from (α,pγ). Others: 100 60 from (α,γ):resonances and 100 14 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
5530.0	3296.0	I(γ): from (α,pγ). Others: 100 60 from (α,γ):resonances and 86 14 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
5558.9	5558.4	E(γ): other: 5559 4 from (γ,γ’)
5772.7	1139.3	I(γ): weighted average of 63 25 from (α,γ):resonances, 20 10 from (α,pγ), and 51 14 from (p,γ)
	1582.6	I(γ): weighted average of 30 10 from (α,pγ) and 34 12 from (p,γ)
	2358.0	E(γ): from (¹²C,αpγ). I(γ): from (α,pγ). Others: 100 38 from (α,γ):resonances and 100 26 from (p,γ)
	3539.5	I(γ): from (p,γ). Others: 38 13 from (α,γ):resonances and 50 16 from (α,pγ)
	4507.0	I(γ): weighted average of 50 25 from (α,γ):resonances and 57 14 from (p,γ)
E(level)	E(gamma)	Comments
5892.1	2477.3	E(γ): From (¹⁶O,2αpγ) I(γ): weighted average of 9.6 29 from (¹⁶O,2αpγ), 11.1 22 from (α,pγ), and 8.7 33 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
5892.1	3658.2	E(γ): From (¹⁶O,2αpγ) I(γ): from (α,pγ). Others: 100 8 from (¹⁶O,2αpγ) and 100.0 33 from (p,γ) M(γ): Q, ΔJ=2 also from γγ(ADO) in (¹⁶O,2αpγ). From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
6046.4	1412.2	I(γ): weighted average of 53 12 from (α,pγ) and 27 9 from (p,γ)
	2631.7	I(γ): from (α,pγ). Other: 100 15 from (p,γ) M(γ): D+Q from pγ(θ) in (α,pγ); M1⁺E2 from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
	3812.3	I(γ): from (α,pγ). Other: 42 12 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
6078.53	1444.4	E(γ): unweighted average of 1445.0 3 from (²⁰Ne,pγ), 1445.6 4 from (¹⁶O,2αpγ), 1442.7 8 from (¹²C,αpγ). Others: 1444.6 from (p,γ) I(γ): unweighted average of 42 4 from (²⁰Ne,pγ), 50 8 from (¹⁶O,2αpγ), 13.6 34 from (α,pγ) and 13 4 from (p,γ). Note that while values from (α,pγ) and (p,γ) are consistent, and so are those from the other two studies, the two pairs of values are discrepant. The evaluators consider it is likely because the 3845γ from 6078 level is unresolved with the 3850γ from the 5116 level due to poor resolution in (p,γ) and (α,pγ), and the 5116 level is however not populated in the more recent studies of (²⁰Ne,pγ) and (¹⁶O,2αpγ).
6078.53	3844.6	E(γ): weighted average of 3844.6 1 from (²⁰Ne,pγ), 3846 4 from (¹²C,αpγ), and 3846.3 7 from (¹⁶O,2αpγ) I(γ): from (α,pγ). Others: 100 9 from (²⁰Ne,pγ), 100 8 from (¹⁶O,2αpγ), and 100 13 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
6453.49	1110.2	E(γ): weighted average of 1110.1 3 from (²⁰Ne,pγ), 1109.5 5 from (¹²C,αpγ), and 1110.5 3 from (¹⁶O,2αpγ) I(γ): unweighted average of 9.9 9 from (²⁰Ne,pγ), 13.1 28 from (¹²C,αpγ), 16.9 18 from (¹⁶O,2αpγ), and 12 5 from (α,pγ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	1819.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3039.3	E(γ): weighted average of 3039.7 4 from (²⁰Ne,pγ), 3038.9 19 from (¹²C,αpγ), and 3038.7 5 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ). Others: 100 5 from (²⁰Ne,pγ), 100 29 from (¹²C,αpγ), 100 5 from (α,pγ), and 100 12 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	4220.6	I(γ): other: 11 11 (α,γ):res.
6501.3	2070.6	E(γ): unweighted average of 2071.5 2 from (²⁰Ne,pγ), 2069.9 7 from (¹²C,αpγ), and 2070.4 4 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ). Others: 100 40 from (α,γ):resonances, 100 20 from (α,pγ), and 100 13 from (p,γ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
6796.0	2364.8	E(γ): weighted average of 2363.3 10 from (¹²C,αpγ) and 2365.0 4 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ). Others: 100 11 from (α,pγ), 100 16 from (¹²C,αpγ) M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
6796.0	3380.8	E(γ): weighted average of 3381.6 16 from (¹²C,αpγ) and 3380.7 6 from (¹⁶O,2αpγ) I(γ): weighted average of 38 7 from (¹⁶O,2αpγ), and 33 11 from (α,pγ). Other: 114 32 from (¹²C,αpγ) is discrepant M(γ): D+Q from pγ(θ) in (α,pγ); E1⁺M2 from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments; M2 component unlikely from RUL
6823.91	1480.8	E(γ): others: 1480.5 5 from (¹²C,αpγ) and 1480.8 3 from (¹⁶O,2αpγ). From (²⁰Ne,pγ) I(γ): weighted average of 65.9 26 from (¹⁶O,2αpγ), 67 17 from (α,pγ), and 54 15 from (p,γ). Other: 114 4 from (²⁰Ne,pγ) is discrepant M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
6823.91	2393.8	E(γ): weighted average of 2394.0 2 from (²⁰Ne,pγ), 2393.6 7 from (¹²C,αpγ), and 2393.0 4 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ). Others: 100 7 from (²⁰Ne,pγ), 100 17 from (α,pγ), and 100 23 from (p,γ) M(γ): Q with ΔJ=2 from γγ(DCO) in (²⁰Ne,pγ) and (¹⁶O,2αpγ); M2 ruled out by RUL
6828	2397	E(γ): From (α,γ):resonances I(γ): From (α,γ):resonances
	3414	E(γ): From (α,γ):resonances I(γ): From (α,γ):resonances
	4595	E(γ): From (α,γ):resonances I(γ): From (α,γ):resonances
6909.6	6908.8	E(γ): other: 6909 4 from (γ,γ’)
6931.4	2297.1	I(γ): other: 32 16 from (α,γ):resonances is inconsistent
	2500.1	I(γ): weighted average of 27 10 from (α,γ):resonances and 16 5 from (p,γ)
	4697.2	I(γ): other: 100 19 from (α,γ):resonances M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
7117.7	3703.1	M(γ): From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
7141.1	5874.4	I(γ): from (γ,γ’). Other: 19 from (p,γ)
7141.1	7140.2	E(γ): other: 7140 4 from (γ,γ’) I(γ): from (γ,γ’)
E(level)	E(gamma)	Comments
7214.3	7213.4	E(γ): other: 7214 4 from (γ,γ’)
7313.7	7312.8	E(γ): other: 7316 4 from (γ,γ’)
7442.1	988.1	E(γ): unweighted average of 988.9 3 from (²⁰Ne,pγ), 987.0 4 from (¹²C,αpγ), and 988.4 2 from (¹⁶O,2αpγ). This γ is not seen in (α,γ):resonances due to the high detector threshold (>2 MeV) I(γ): unweighted average of 36 4 from (²⁰Ne,pγ), 18.9 19 from (¹⁶O,2αpγ), and 9.9 22 from (α,pγ)
	2807	E(γ): From (α,γ):resonances
	4027.5	E(γ): weighted average of 4027.8 3 from (²⁰Ne,pγ), 4027 3 from (¹²C,αpγ), and 4026.6 5 from (¹⁶O,2αpγ) I(γ): from (α,pγ). Others: 100 8 from (²⁰Ne,pγ), 100 4 from (¹⁶O,2αpγ), and 100 25 from (α,γ):resonances M(γ): ΔJ=2 also supported by γγ(DCO) in (²⁰Ne,pγ) and (¹⁶O,2αpγ). From pγ(θ) in (α,pγ) with magnetic/electric nature determined by measured γ(lin pol) and/or by RUL based on measured lifetimes
	5207	E(γ): From (α,γ):resonances
7687.2	5452.9	E(γ): from (p,γ)
7851.2	7850	E(γ): from (γ,γ’)
7859.6	1063.4	E(γ): weighted average of 1063.2 6 from (¹²C,αpγ) and 1063.5 4 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ)
	2516.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): d with ΔJ=1 from γγ(ADO) in (¹⁶O,2αpγ); (M1) from level scheme
	3428.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): Q with ΔJ=2 from γγ(ADO) in (¹⁶O,2αpγ); M2 is less likely
7897.9	7898.1	E(γ): other: 7896 6 from (γ,γ’)
8076.91	1253.4	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): d from (¹⁶O,2αpγ). ΔJ=0 from γγ(ADO)
	2733.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3645.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): from (¹⁶O,2αpγ). ΔJ=2 from γγ(ADO)
8207.9	8206.7	E(γ): other: 8209 4 from (γ,γ’)
8343.5	4928.5	E(γ): From (¹⁶O,2αpγ) M(γ): Q with ΔJ=2 from γγ(ADO) in (¹⁶O,2α,pγ); M2 is less likely
8345.5	4154.3	E(γ): From (α,γ):resonances I(γ): From (α,γ):resonances
	4930.5	E(γ): From (α,γ):resonances I(γ): From (α,γ):resonances
	6111.1	E(γ): From (α,γ):resonances I(γ): From (α,γ):resonances
8414.2	1590.1	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): from (¹⁶O,2αpγ) with ΔJ=0 from γγ(ADO)
	1913.1	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3983.3	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): from (¹⁶O,2αpγ), with ΔJ=2 from γγ(ADO)
8543.6	5408.8	M(γ): D+Q from (p,γ); E1 from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
8555.4	3540	M(γ): D+Q from (p,γ), (M1⁺E2) from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
E(level)	E(gamma)	Comments
8705.23	628.4	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1881.9	E(γ): unweighted average of 1883.7 4 from (²⁰Ne,pγ), 1880.8 5 from (¹²C,αpγ), and 1881.3 4 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ). Others: 100 10 from (²⁰Ne,pγ) and 100 16 from (¹²C,αpγ)
	1909.2	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	2203.9	E(γ): weighted average of 2205.3 15 from (²⁰Ne,pγ), 2204.2 9 from (¹²C,αpγ), and 2203.6 6 from (¹⁶O,2αpγ) I(γ): unweighted average of 4.7 8 from (²⁰Ne,pγ) and 9.5 21 from (¹⁶O,2αpγ)
	2251.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
8738.0	3722.9	M(γ): it is E1⁺M2 from level scheme, but the strong M2 component is inconsistent with measured proton resonance strength and RUL. It is possible this transition could feed the 5014.9, (3/2⁺) level instead of 5015.2, 3/2- level as claimed by 2005Vo24 in (p,γ), if δ can be confirmed.
9175.9	1099.2	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1733.7	E(γ): weighted average of 1733.4 7 from (²⁰Ne,pγ) and 1733.9 6 from (¹⁶O,2αpγ) I(γ): weighted average of 12.5 26 from (²⁰Ne,pγ) and 18 6 from (¹⁶O,2αpγ) M(γ): ΔJ=1 from γγ(DCO) in (²⁰Ne,pγ); E1⁺M2 from level scheme, but δ(M2/E1)<0.15 from RUL=3 for M2.
	2351.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	2722.6	E(γ): weighted average of 2723.5 8 from (²⁰Ne,pγ) and 2722.3 5 from (¹⁶O,2αpγ) I(γ): from (²⁰Ne,pγ). Other: 100 8 from (¹⁶O,2αpγ) M(γ): ΔJ=1 from γγ(DCO) in (²⁰Ne,pγ) and (¹⁶O,2αpγ); E1 from level scheme
9312.9	1871.0	E(γ): weighted average of 1870.6 9 from (¹²C,αpγ) and 1871.1 6 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ)
	2859.4	E(γ): weighted average of 2860.6 12 from (¹²C,αpγ) and 2859.1 6 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ)
	3233.3	E(γ): weighted average of 3232 3 from (¹²C,αpγ) and 3233.4 7 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ)
9449.86	745.3	E(γ): unweighted average of 745.8 2 from (²⁰Ne,pγ) and 744.7 2 from (¹⁶O,2αpγ) I(γ): from (¹⁶O,2αpγ). Other: 100 19 from (²⁰Ne,pγ) M(γ): d from ΔJ=0 from γγ(DCO) in (²⁰Ne,pγ) and (¹⁶O,2αpγ); M1 from Δπ=(no)
	1106.4	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1373.2	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	2007.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	2627.3	E(γ): unweighted average of 2628.8 9 from (²⁰Ne,pγ) and 2625.7 6 from (¹⁶O,2αpγ) I(γ): <32 in (²⁰Ne,pγ).
9524.6	5333.2	M(γ): D+Q from γγ(θ) in (p,γ); E1⁺M2 ruled out based on measured proton resonance and RUL
9536.4	2712.1	E(γ): could belong to a different level at similar energy
9536.4	3081.5	E(γ): could belong to a different level at similar energy
9599.8	3145.7	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3707.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	4257.1	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
9611.9	8344.6	M(γ): γ(θ) from (p,γ) consistent with ΔJ=0 or ΔJ=2
E(level)	E(gamma)	Comments
10019.7	8752.2	M(γ): D+Q from γ(θ); (E1⁺M2) from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
10037.0	2594.7	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3582.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	4144.5	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	4693.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): Q from γγ(ADO) in (¹⁶O,2αpγ)
10046	8779.3	M(γ): D+Q from γ(θ); (E1⁺M2) from Δπ, where parity assignments of connecting levels are uniquely established from independent arguments
10216.95	767.3	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	903.9	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1041.7	E(γ): unweighted average of 1042.4 2 from (²⁰Ne,pγ) and 1041.0 2 from (¹⁶O,2αpγ) I(γ): unweighted average of 52 5 from (²⁰Ne,pγ) and 25 5 from (¹⁶O,2αpγ)
	1511.7	E(γ): weighted average of 1511.4 6 from (¹²C,αpγ) and 1511.9 5 from (¹⁶O,2αpγ) I(γ): weighted average of 1.3 13 from (¹²C,αpγ) and 4.0 10 from (¹⁶O,2αpγ)
	1802.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	2139.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	2356.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3392.8	E(γ): weighted average of 3392.3 7 from (²⁰Ne,pγ), 3394.8 11 from (¹²C,αpγ), and 3392.5 6 from (¹⁶O,2αpγ) I(γ): from (²⁰Ne,pγ). Others: 100 20 from (¹²C,αpγ) and 100 23 from (¹⁶O,2αpγ) M(γ): Q from γγ(ADO) in (¹⁶O,2αpγ); M2 ruled out by RUL. Other: D+Q in (²⁰Ne,pγ) is inconsistent
10520.16	483.1	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	920.4	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1070.1	E(γ): weighted average of 1070.7 4 from (²⁰Ne,pγ) and 1069.8 3 from (¹⁶O,2αpγ) I(γ): unweighted average of 57 5 from (²⁰Ne,pγ) and 43 5 from (¹⁶O,2αpγ)
	1207.3	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1344.3	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1815.2	E(γ): unweighted average of 1815.9 4 from (²⁰Ne,pγ) and 1814.5 4 from (¹⁶O,2αpγ) I(γ): from (²⁰Ne,pγ) M(γ): d with ΔJ=1 from γγ(DCO) in (²⁰Ne,pγ) and (¹⁶O,2αpγ); (E1) from level scheme
	2176.4	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3078.1	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	4066	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
10759.4	3934.6	E(γ): From (¹⁶O,2αpγ) M(γ): Q from (¹⁶O,2αpγ), ΔJ=2 from γγ(ADO); E2 from level scheme
11296.98	537.5	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	776.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1080.3	E(γ): weighted average of 1080.9 6 from (²⁰Ne,pγ) and 1080.1 3 from (¹⁶O,2αpγ) I(γ): weighted average of 73 10 from (²⁰Ne,pγ) and 53 13 from (¹⁶O,2αpγ)
	1259.6	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1697	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	1984	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	4472.7	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
E(level)	E(gamma)	Comments
11733.8	1516.8	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): d from ΔJ=0 from γγ(ADO) in (¹⁶O,2αpγ); Δπ=yes from level scheme
	2557.7	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	3028.5	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ)
	5280.3	E(γ): From (¹⁶O,2αpγ) I(γ): From (¹⁶O,2αpγ) M(γ): Q from ΔJ=2 from γγ(ADO) in (¹⁶O,2αpγ); E2 from level scheme
12170.6	2994.6	E(γ): From (²⁰Ne,pγ)
13879.2	2582.1	E(γ): From (¹⁶O,2αpγ)