List of levels for 87Y

Authors: T.D. Johnson and W.D. Kulp | Citation: Nucl. Data Sheets 129, 1 (2015) | Cutoff date: 27-Jul-2015

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
380.82	9/2+	13.37 h 3 % IT = 98.43 11 % ε = 1.57 11	380.79 7	M4		0.256	B(M4)(W.u.)=2.705 12, α=0.256, α(K)=0.217 3, α(L)=0.0329 5, α(M)=0.00575 8, α(N)=0.000753 11, α(O)=4.46×10^-5 7
793.73	5/2-	≤ 10 ns	793.7 1	(E2)		1.09×10^-3	B(E2)(W.u.)>0.0078, α=1.09E-3 2, α(K)=0.000963 14, α(L)=0.0001073 15, α(M)=1.83E-5 3, α(N)=2.45E-6 4, α(O)=1.671E-7 24
1404.47	13/2+	≤ 10 ns	1024.0 3	E2		5.91×10^-4	B(E2)(W.u.)>0.0022, α=5.91E-4, α(K)=0.000522 8, α(L)=5.74E-5 8, α(M)=9.79E-6 14, α(N)=1.315E-6 19, α(O)=9.09E-8 13
1590.92	11/2+	≤ 10 ns	1210.0 2	D+Q	+1.0 4		B(E2)(W.u.)>0.00029, B(M1)(W.u.)>3.7E-7
2038.05	(11/2+)	≤ 10 ns	633.6 1	M1+E2	+0.37 7	0.00171	B(E2)(W.u.)>0.00098, B(M1)(W.u.)>3.6E-6, α=0.00171 3, α(K)=0.001514 24, α(L)=0.000167 3, α(M)=2.85E-5 5, α(N)=3.83E-6 7, α(O)=2.67E-7 4
2038.05	(11/2+)	≤ 10 ns	1657.2 1	[M1,E2]		3.48×10^-4	B(E2)(W.u.)>3.9E-6, B(M1)(W.u.)>1.5E-7, α=3.48E-4 6, α(K)=0.000194 3, α(L)=2.09E-5 3, α(M)=3.56E-6 5, α(N)=4.80E-7 7, α(O)=3.40E-8 5
2366.92	15/2-	≤ 10 ns	962.4 1	D			B(E1)(W.u.)>3.8E-8, α(K)=0.000257 11, α(L)=2.77E-5 13, α(M)=4.72E-6 21, α(N)=6.4E-7 3, α(O)=4.45E-8 20
2428.09	17/2+	≤ 10 ns	1023.6 1	E2		5.91×10^-4	B(E2)(W.u.)>0.0022, α=5.91E-4, α(K)=0.000522 8, α(L)=5.74E-5 8, α(M)=9.80E-6 14, α(N)=1.316E-6 19, α(O)=9.10E-8 13
2648.91	(15/2-)		169.9 1	D(+Q)	+0.05 2	0.0434	α=0.0434 7, α(K)=0.0382 6, α(L)=0.00435 7, α(M)=0.000745 12, α(N)=9.99×10^-5 16, α(O)=6.84E-6 11
2676.06	17/2-	0.25 ns 10	27.2 1	[M1]		7.79	α=7.79
	17/2-	0.25 ns 10	247.9 2	(E1+M2)	+0.19 11	0.010	B(E1)(W.u.)<1.4E-5, α=0.010 4, α(K)=0.009 3, α(L)=0.0010 4, α(M)=0.00018 7, α(N)=2.4E-5 9, α(O)=1.6E-6 6
	17/2-	0.25 ns 10	309.1 1	M1+E2	+0.20 4	0.00962	B(E2)(W.u.)=(1.1 7), B(M1)(W.u.)=(0.0024 11), α=0.00962 20, α(K)=0.00848 18, α(L)=0.000953 22, α(M)=0.000163 4, α(N)=2.19E-5 5, α(O)=1.51E-6 3
2827.20	21/2+	0.53 ns 3	399.1 1	E2		0.00792	B(E2)(W.u.)=4.6 3, α=0.00792, α(K)=0.00695 10, α(L)=0.000817 12, α(M)=0.0001395 20, α(N)=1.84E-5 3, α(O)=1.176E-6 17
2961.47	17/2-		285.4 1	M1(+E2)	+0.07 28	0.0114	α=0.0114 14, α(K)=0.0100 12, α(L)=0.00112 16, α(M)=0.00019 3, α(N)=2.6×10^-5 4, α(O)=1.79E-6 19
2961.47	17/2-		312.6 3	(M1+E2)	-0.4 3	0.0102	α=0.0102 17, α(K)=0.0090 15, α(L)=0.00102 19, α(M)=0.00018 4, α(N)=2.3×10^-5 5, α(O)=1.58E-6 23
2986.9	(19/2+)	< 49 ps	159.8 1	(M1+E2)	+0.06 2	0.0512	B(E2)(W.u.)>4.1, B(M1)(W.u.)>0.078, α=0.0512 9, α(K)=0.0451 8, α(L)=0.00515 10, α(M)=0.000882 16, α(N)=0.0001182 21, α(O)=8.08E-6 13
2986.9	(19/2+)	< 49 ps	558.7 5	[M1,E2]		0.00236	B(E2)(W.u.)>0.092, B(M1)(W.u.)>0.00041, α=0.00236 10, α(K)=0.00208 9, α(L)=0.000231 12, α(M)=3.94E-5 19, α(N)=5.29E-6 25, α(O)=3.66E-7 14
3402.4	(19/2-)		440.9 5	(M1)		0.00390	α=0.00390, α(K)=0.00344 5, α(L)=0.000381 6, α(M)=6.51×10^-5 10, α(N)=8.77E-6 13, α(O)=6.12E-7 9
3402.4	(19/2-)		726.4 3	(M1+E2)	+0.26 6	1.24×10^-3	α=1.24×10^-3, α(K)=0.001098 16, α(L)=0.0001202 18, α(M)=2.05E-5 3, α(N)=2.76E-6 4, α(O)=1.94E-7 3
3446.5	(19/2-)		770.5 3	(D+Q)	-0.19 17	1.08×10^-3	α=1.08×10^-3 2
3552.95	(23/2+)	0.083 ps 21	725.8 1	D(+Q)	-0.20 22	1.24×10^-3	B(M1)(W.u.)=(0.67 +23-14), α=1.24×10^-3 2, α(K)=0.001097 21, α(L)=0.0001200 25, α(M)=2.05E-5 5, α(N)=2.76E-6 6, α(O)=1.94E-7 4
3595.3	(21/2+)	0.5 ns 2	608.4 3	D+Q	+0.06 3		B(E2)(W.u.)=(2.1E-3 +15-6), B(M1)(W.u.)=(1.9E-4 +13-6)
3766.6	(21/2-)		364.1 5	D+(Q)	-0.15 20
3766.6	(21/2-)		1090.6 5	(E2)		5.12×10^-4	α=5.12×10^-4, α(K)=0.000453 7, α(L)=4.96E-5 7, α(M)=8.47E-6 12, α(N)=1.138E-6 16, α(O)=7.89E-8 11
4039.40	(25/2+)	0.17 ps 4	486.4 1	D(+Q)	-0.16 20		B(E2)(W.u.)<817, B(M1)(W.u.)=(1.1 +4-3), α(K)=0.00276 10, α(L)=0.000305 13, α(M)=5.21E-5 22, α(N)=7.0E-6 3, α(O)=4.89E-7 16
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
4555.0	(23/2+)		1568.2 5	(E2)		3.50×10^-4	α=3.50×10^-4, α(K)=0.000212 3, α(L)=2.29E-5 4, α(M)=3.91E-6 6, α(N)=5.27E-7 8, α(O)=3.70E-8 6
4564.1	(23/2-)		1011.4 5	(D)			α(K)=0.000232 4, α(L)=2.50×10^-5 4, α(M)=4.27E-6 6, α(N)=5.75E-7 8, α(O)=4.03E-8 6
4564.1	(23/2-)		1117.6 3	(E2)		4.86×10^-4	α=4.86×10^-4, α(K)=0.000429 6, α(L)=4.70E-5 7, α(M)=8.01E-6 12, α(N)=1.077E-6 15, α(O)=7.47E-8 11
4609.66	25/2+	0.12 ps 4	1056.8 1	D(+Q)	0.04 18
4609.66	25/2+	0.12 ps 4	1782.4 1	E2		3.91×10^-4	B(E2)(W.u.)=4.9 21, α=3.91E-4, α(K)=0.0001654 24, α(L)=1.785E-5 25, α(M)=3.04E-6 5, α(N)=4.10E-7 6, α(O)=2.89E-8 4
5228.2	(25/2-)		1319.4 5	D(+Q)	0.14 22
5319.7	(25/2-)		1553.0 5	(E2)		3.48×10^-4	α=3.48×10^-4, α(K)=0.000216 3, α(L)=2.34E-5 4, α(M)=3.99E-6 6, α(N)=5.37E-7 8, α(O)=3.77E-8 6
5495.2	(25/2+)		940.1 5	D+Q	-0.8 5
5495.2	(25/2+)		1942.2 5	D+Q	-0.8 3
5759.59	(27/2-)	> 2.1 ps	439.7 5	D(+Q)	+0.10 10
	(27/2-)	> 2.1 ps	1195.6 3	(E2)		4.26×10^-4	B(E2)(W.u.)<2.1, α=4.26E-4, α(K)=0.000370 6, α(L)=4.04E-5 6, α(M)=6.90E-6 10, α(N)=9.27E-7 13, α(O)=6.45E-8 9
	(27/2-)	> 2.1 ps	1720.0 3	(E1+M2)	-0.14 10	5.20×10^-4	B(E1)(W.u.)<1.3E-5, B(M2)(W.u.)<0.95, α=5.20E-4, α(K)=9.7E-5 10, α(L)=1.04E-5 11, α(M)=1.78E-6 18, α(N)=2.39E-7 24, α(O)=1.69E-8 17
5827.1	(27/2+)		1217.4 3	(M1+E2)	-1.0 3	4.14×10^-4	α=4.14×10^-4, α(K)=0.000358 5, α(L)=3.89E-5 6, α(M)=6.64E-6 10, α(N)=8.95E-7 13, α(O)=6.28E-8 10
5934.50	(29/2-)	1.8 ps 4	174.9 1	D+Q	-0.20 12
6535.5	(31/2-)	0.18 ps 4	601.0 1	(D+Q)	+0.14 14		B(E2)(W.u.)=(3.×10¹ +7-3), B(M1)(W.u.)=(0.55 13), α(K)=0.00168 3, α(L)=0.000184 4, α(M)=3.15E-5 6, α(N)=4.24E-6 8, α(O)=2.97E-7 5
7016.6	(33/2-)	0.11 ps 3	481.1 1	(D+Q)	-0.10 15		B(E2)(W.u.)=(9.×10¹ +26-9), B(M1)(W.u.)=(1.8 5), α(K)=0.00281 7, α(L)=0.000311 8, α(M)=5.31E-5 14, α(N)=7.15E-6 18, α(O)=4.99E-7 11

Q(β-)=-3672 keV 4	S(n)= 11806 keV 14	S(p)= 5784.1 keV 11	Q(α)= -6373 keV 3
Reference: 2012Wa38

References:
A	⁸⁵Rb(α,2nγ), ⁷⁴Ge(¹⁸O,4NPG)	B	⁸⁴Sr(α,p)
C	⁸⁶Sr(p,γ)	D	⁸⁶Sr(p,p’),(pol p,p’) IAR
E	⁸⁶Sr(³He,d), (d,n)	F	⁸⁷Y IT decay (13.37 H)
G	⁸⁷Zr β⁺ decay	H	⁸⁸Sr(p,2nγ)
I	⁸⁹Y(p,t)	J	⁹⁰Zr(p,α), (pol p,α)
K	⁸⁶Sr(p,γ) IAR	L	⁸⁰Se(¹¹B,4nγ)
M	⁸⁷Sr(p,nγ)

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 E F G H I J L M	1/2-	79.8 h 3 % ε = 100
380.82 7	A B C E F G H I J L M	9/2+	13.37 h 3 % IT = 98.43 11 % ε = 1.57 11	380.79 7	100	M4	0.0	1/2-
793.73 8	A B C E G H I J K L M	5/2-	≤ 10 ns	793.7 1	100	(E2)	0.0	1/2-
982.89 10	B C E I J K M	3/2-		982.9 1	100	M1,E2	0.0	1/2-
1152.71 11	B C E G J M	5/2+		771.9 1	100	E2	380.82	9/2+
1182.00 9	C I J M	3/2-		1182.1 1	100		0.0	1/2-
1203.01 9	B C H I J K M	5/2-		409.2 1 1203.0 2	9.8 4 100.0 16		793.73 0.0	5/2- 1/2-
1321 8	B
1404.47 12	A B E H J L M	13/2+	≤ 10 ns	1024.0 3	100	E2	380.82	9/2+
1405.3 4	B C E G	(7/2+,9/2+)	≤ 10 ns	1024.0 10	100		380.82	9/2+
1504 8	B
1590.92 14	A C G H L M	11/2+	≤ 10 ns	1210.0 2	100	D+Q	380.82	9/2+
1608.31 12	B C E G M	7/2+,9/2+		1227.5 1	100		380.82	9/2+
1609 5	I J	3/2-
1623.50 21	A C H J	(5/2,7/2)		444.0 643.0 829.5 2	16 100 100		1182.00 982.89 793.73	3/2- 3/2- 5/2-
1629.94 13	C L M	(1/2-,3/2-)		836.2 1	100	M1,E2	793.73	5/2-
1641 5	I	1/2-
1704.7 4	C J M			501.9 523.3 7 910.5 1704.5 4	18 75 13 94 100 18		1203.01 1182.00 793.73 0.0	5/2- 3/2- 5/2- 1/2-
1719 4	I	3/2-,5/2-
1756.08 11	B C J M	5/2		574.1 1 962.7 2	100 4 ≈36		1182.00 793.73	3/2- 5/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1768.2 5	L	(9/2-)		974.5 5	100		793.73	5/2-
1801.64 15	C J M	5/2-		598.1 619.8 2 818.5 1801.5 2	16 20 4 8 100 4		1203.01 1182.00 982.89 0.0	5/2- 3/2- 3/2- 1/2-
1814 5	I	3/2-,5/2-
1849 3	B C E I J	1/2-		665.2 864.1	67 100		1182.00 982.89	3/2- 3/2-
1979.95 12	C I J M	7/2-		574.0 776.9 1 827.3 2 1186.5 3	123 100 4 21 3 31 5		1405.3 1203.01 1152.71 793.73	(7/2+,9/2+) 5/2- 5/2+ 5/2-
2008.8 3	B H J L M	(7/2)		1215.1 3	100		793.73	5/2-
2021 5	B I	(7/2-,9/2-)
2038.05 11	A L M	(11/2+)	≤ 10 ns	633.6 1 1657.2 1	100.0 16 99.3 21	M1+E2 [M1,E2]	1404.47 380.82	13/2+ 9/2+
2072.7 10	C	(3/2,5/2,7/2)		1279.0	100		793.73	5/2-
2073.31 23	G M	(7/2+,9/2+)		920.6 2 1692.0 15	100 4		1152.71 380.82	5/2+ 9/2+
2083.0 5	B C E	(3/2)-		880.0 901.3 930.0 1100.1 2082.8	31 97 31 53 100		1203.01 1182.00 1152.71 982.89 0.0	5/2- 3/2- 5/2+ 3/2- 1/2-
2095 5	B I	3/2-,5/2-
2112.3 4	C J M	5/2+		706.3 930.0 959.7 4	55 27 100		1405.3 1182.00 1152.71	(7/2+,9/2+) 3/2- 5/2+
2122 5	I	5/2+,7/2+
2154.60 18	J M	(9/2-)		951.7 2 1773.5 3	38.8 14 100 4		1203.01 380.82	5/2- 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2158.9 10	C			2158.9	100		0.0	1/2-
2165 5	I	7/2,9/2-
2186.0 3	C J M	7/2-		1392.3 3	100		793.73	5/2-
2202 5	I	7/2-,9/2-
2202.17 17	B E G M	7/2+,9/2+		611.2 2 797.0 7 1048 1 1410.0 15 1821.4 2	30 3 100 5 33 17 17 8 29.8 20		1590.92 1405.3 1152.71 793.73 380.82	11/2+ (7/2+,9/2+) 5/2+ 5/2- 9/2+
2209 3	J	3/2-
2210.6 8	C	(1/2)		409.2 2210.4	47 100		1801.64 0.0	5/2- 1/2-
2216 5	I	9/2+,11/2+
2241.6 7	G	(7/2,9/2-)		633 1 836 1 1862.0 15	100 50 100 50 50 25		1608.31 1405.3 380.82	7/2+,9/2+ (7/2+,9/2+) 9/2+
2244.8 6	C			619.7 1042.6 1451.9	77 100 31		1623.50 1203.01 793.73	(5/2,7/2) 5/2- 5/2-
2249 3	J	9/2-
2256 5	I	3/2-,5/2-
2276 3	J	(9/2-&7/2+)
2277.53 17	B C E M	7/2-		1075.3 4 1483.8 2 1896.2 3	80 9 100 14 50 11		1203.01 793.73 380.82	5/2- 5/2- 9/2+
2279.4	C	(7/2-)		1126.9	100		1152.71	5/2+
2292.3 10	C I	5/2+,7/2+		1139.6	100		1152.71	5/2+
2302.61 15	D J M	13/2+		711.4 3 898.6 2 1921.6 2	100		1590.92 1404.47 380.82	11/2+ 13/2+ 9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2314 5	I	(5/2+,7/2+)
2344.61 17	M			940.0 2 1963.9 2	100 11 100 11		1404.47 380.82	13/2+ 9/2+
2353.55 21	C M	(7/2,9/2,11/2)		746.6 949.4 1559.7 2	100 47		1608.31 1405.3 793.73	7/2+,9/2+ (7/2+,9/2+) 5/2-
2365 3	J	7/2+
2366.92 15	A H I J L M	15/2-	≤ 10 ns	962.4 1	100	D	1404.47	13/2+
2400.0 3	M			2019.2 3	100		380.82	9/2+
2409 2	C E I J	3/2+		2408.3	100		0.0	1/2-
2428.09 15	A H L	17/2+	≤ 10 ns	1023.6 1	100	E2	1404.47	13/2+
2446 2	C I	(5/2)+
2449 3	J	9/2-
2479.07 15	A H I L	13/2-		441.1 5 888.2 1	26 3 100 5	(D+Q) (D)	2038.05 1590.92	(11/2+) 11/2+
2502 2	C	(5/2+)
2532 2	J	11/2-
2532 2	C
2552 2	C G I	9/2+		1400.0 15 2172 2	100 25 50 25		1152.71 380.82	5/2+ 9/2+
2563.7 7	C G I J	9/2,11/2+		973 1 1159 1 2183.0 15	50 13 100 13 38 13		1590.92 1404.47 380.82	11/2+ 13/2+ 9/2+
2572 2	C	(3/2-)
2599 3	J	9/2-
2602.3 11	G I	(7/2)+		1808.0 15 2222.0 15	33 11 100 22		793.73 380.82	5/2- 9/2+
2616 2	C	(3/2-)
2648.91 15	A L	(15/2-)		169.9 1	100	D(+Q)	2479.07	13/2-
2661 3	J	7/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2668	C	(5/2)
2676.06 15	A H I L	17/2-	0.25 ns 10	27.2 1 247.9 2 309.1 1	<5.9 20.0 18 100 12	[M1] (E1+M2) M1+E2	2648.91 2428.09 2366.92	(15/2-) 17/2+ 15/2-
2682 3	J	11/2+
2730 4	E	5/2-,7/2-
2737 5	I	9/2+,11/2+
2747 3	J	3/2+
2762	C	(3/2-)
2801 3	J	(3/2+&11/2+)
2808 5	I	9/2+,11/2+
2808.4 8	L	(13/2-)		1040.2 5	100		1768.2	(9/2-)
2827.20 18	A H L	21/2+	0.53 ns 3	399.1 1	100	E2	2428.09	17/2+
2828 5	I	(3/2,5/2)-
2831 3	J	9/2-
2871 5	I	11/2-,13/2-
2901 5	I J	3/2-,5/2-
2907 4	C E	3/2+,5/2+
2960 3	J	(5/2+)
2961.47 18	A I L	17/2-		285.4 1 312.6 3	100 6 40 4	M1(+E2) (M1+E2)	2676.06 2648.91	17/2- (15/2-)
2986.9 3	A L	(19/2+)	< 49 ps	159.8 1 558.7 5	100 5 35 4	(M1+E2) [M1,E2]	2827.20 2428.09	21/2+ 17/2+
2995.6 3	A	(17/2)		346.7 2	100		2648.91	(15/2-)
2996 2	C E I J	5/2+
2996.1 11	G	(7/2,9/2,11/2)		1388.0 15 2615.0 15	100 33 100 67		1608.31 380.82	7/2+,9/2+ 9/2+
3038 5	I	9/2+,11/2+
3043 4	E	3/2+,5/2+
3057 5	I	(5/2+,7/2+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3090 4	E	3/2+,5/2+
3093 5	I	9/2+,11/2+
3094.4 4	A	(21/2)	< 49 ps	107.5 2	100	D	2986.9	(19/2+)
3120 3	E I	5/2+,7/2+
3120 10	J	(13/2-)
3181 5	I	(13/2+,15/2+)
3195 4	E	(1/2+)
3245 5	I	9/2+,11/2+
3262.9 13	G I	9/2+,11/2+		1857.0 15 2883 2	100 50 100 75		1405.3 380.82	(7/2+,9/2+) 9/2+
3308 6	E J	3/2+,5/2+
3351 2	C E	3/2+,5/2+
3402.4 3	A L	(19/2-)		440.9 5 726.4 3	51 4 100 8	(M1) (M1+E2)	2961.47 2676.06	17/2- 17/2-
3405.2 11	E G	3/2+,5/2+		1203 1	100		2202.17	7/2+,9/2+
3446.5 3	A J L	(19/2-)		770.5 3	100	(D+Q)	2676.06	17/2-
3500	J	(11/2+)
3552.95 19	A L	(23/2+)	0.083 ps 21	725.8 1	100	D(+Q)	2827.20	21/2+
3595.2 4	A	(21/2,23/2,25/2+)		768.0 3	100		2827.20	21/2+
3595.3 5	A	(21/2+)	0.5 ns 2	608.4 3	100	D+Q	2986.9	(19/2+)
3640 20	J
3730	J	(7/2-)
3766.6 4	A L	(21/2-)		364.1 5 1090.6 5	100 8 67 8	D+(Q) (E2)	3402.4 2676.06	(19/2-) 17/2-
3840	J	(11/2-)
3908.8 4	L	(23/2-)		142.2 5 506.4 5	21 6 100 6	(D+Q) [Q]	3766.6 3402.4	(21/2-) (19/2-)
4039.40 21	A L	(25/2+)	0.17 ps 4	486.4 1	100	D(+Q)	3552.95	(23/2+)
4214.1 3	A	(27/2)		174.7 2	100	D	4039.40	(25/2+)
4555.0 4	L	(23/2+)		1568.2 5 1727.6 5	100 14 62 19	(E2)	2986.9 2827.20	(19/2+) 21/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4564.1 3	L	(23/2-)		1011.4 5 1117.6 3 1161.7 5	41 17 100 7 31 4	(D) (E2)	3552.95 3446.5 3402.4	(23/2+) (19/2-) (19/2-)
4609.66 19	L	25/2+	0.12 ps 4	569.0 5 1056.8 1 1782.4 1	11 3 100 25 83 17	D(+Q) E2	4039.40 3552.95 2827.20	(25/2+) (23/2+) 21/2+
5228.2 3	L	(25/2-)		1189.1 5 1319.4 5 1675.1 5	78 11 100 11 56 6	(D) D(+Q) (D)	4039.40 3908.8 3552.95	(25/2+) (23/2-) (23/2+)
5288.48 21	L	(27/2+)	0.10 ps 3	678.8 1 1249.0 5 1735.8 5	100 18 11.8 18 21 3	(D,Q) (D,Q)	4609.66 4039.40 3552.95	25/2+ (25/2+) (23/2+)
5319.7 4	L	(25/2-)		1553.0 5	100	(E2)	3766.6	(21/2-)
5495.2 4	L	(25/2+)		940.1 5 1942.2 5	82 9 100 9	D+Q D+Q	4555.0 3552.95	(23/2+) (23/2+)
5759.59 24	L	(27/2-)	> 2.1 ps	264.3 5 439.7 5 531.5 5 1195.6 3 1720.0 3	12.3 18 14 4 9 4 100 7 95 11	(D) D(+Q) (E2) (E1+M2)	5495.2 5319.7 5228.2 4564.1 4039.40	(25/2+) (25/2-) (25/2-) (23/2-) (25/2+)
5827.1 3	L	(27/2+)		331.7 5 1217.4 3 1787.8 5	6.8 17 100 14 44 7	(M1+E2)	5495.2 4609.66 4039.40	(25/2+) 25/2+ (25/2+)
5934.50 24	L	(29/2-)	1.8 ps 4	107.5 5 174.9 1 615.0 5 646.0 3 706.3 5	38 4 100 6 21 4 80 6 44 5	(D) D+Q (D)	5827.1 5759.59 5319.7 5288.48 5228.2	(27/2+) (27/2-) (25/2-) (27/2+) (25/2-)
6535.5 3	L	(31/2-)	0.18 ps 4	601.0 1	100	(D+Q)	5934.50	(29/2-)
7016.6 3	L	(33/2-)	0.11 ps 3	481.1 1	100	(D+Q)	6535.5	(31/2-)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
10537 11	D K	5/2+	23 keV 1
10923 11	D	1/2+	40 keV 2
11468 15	D	3/2+	21 keV 2
11739 11	D	1/2+	33 keV 2
11900 11	D	1/2+	34 keV 2
11966 23	D	(3/2)+	25 keV 8
11966 23	D	(5/2+)	25 keV 8
12371 11	D	3/2+	24 keV 1
12661 14	D	1/2+	44 keV 4
12968 15	D	3/2+
13076 15	D	5/2+

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2-	79.8 h 3 % ε = 100	μ=-0.19 2 Δ<r²>=+0.057 fm² relative to ⁸⁹Y (2007Ch07). E(level): 1/2- ground-state band.
380.82	9/2+	13.37 h 3 % IT = 98.43 11 % ε = 1.57 11	μ=6.24 2, Q=-0.50 6 %IT and %ε+%B calculated from measured I_β+=0.75 5 and theoretical ε/β+ ratio for decay to ⁸⁷Sr. E(level): %IT and %ε+%B calculated from measured I_β+=0.75 5 and theoretical ε/β+ ratio for decay to ⁸⁷Sr. yrast states, positive parity.
793.73	5/2-	≤ 10 ns	E(level): 1/2- ground-state band.
1182.00	3/2-		XREF: I(1177).
1405.3	(7/2+,9/2+)	≤ 10 ns	E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
1608.31	7/2+,9/2+		XREF: B(1618).
1629.94	(1/2-,3/2-)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
1756.08	5/2		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
1768.2	(9/2-)		E(level): 1/2- ground-state band.
1979.95	7/2-		XREF: C(1979)I(1991)J(1979).
2008.8	(7/2)		XREF: B(2012).
2021	(7/2-,9/2-)		XREF: B(2012).
2083.0	(3/2)-		XREF: B(2103).
2095	3/2-,5/2-		XREF: B(2103).
2158.9			E(level): From (p,γ), only determined by primary γ spectra.
2186.0	7/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2209	3/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2210.6	(1/2)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. From (p,γ), only determined by primary γ spectra. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
2244.8			E(level): From (p,γ), only determined by primary γ spectra.
2249	9/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2276	(9/2-&7/2+)		J^π(level): From (p,α) from angular distribution and analyzing powers .
2366.92	15/2-	≤ 10 ns	XREF: I(2374).
2428.09	17/2+	≤ 10 ns	E(level): yrast states, positive parity.
2449	9/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2479.07	13/2-		XREF: I(2486). E(level): ΔJ=1 band based on 13/2-.
E(level)	J^π(level)	T_1/2(level)	Comments
2502	(5/2+)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
2532	11/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2552	9/2+		XREF: I(2544).
2572	(3/2-)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
2599	9/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2616	(3/2-)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
2648.91	(15/2-)		E(level): ΔJ=1 band based on 13/2-.
2661	7/2+		J^π(level): From (p,α) from angular distribution and analyzing powers .
2668	(5/2)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
2682	11/2+		J^π(level): From (p,α) from angular distribution and analyzing powers .
2747	3/2+		J^π(level): From (p,α) from angular distribution and analyzing powers .
2762	(3/2-)		E(level): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. J^π(level): From comparison of primary γ strength with the γ strength to the 381 level in (p,γ).
2801	(3/2+&11/2+)		J^π(level): From (p,α) from angular distribution and analyzing powers .
2808.4	(13/2-)		E(level): 1/2- ground-state band.
2827.20	21/2+	0.53 ns 3	E(level): yrast states, positive parity.
2831	9/2-		J^π(level): From (p,α) from angular distribution and analyzing powers .
2960	(5/2+)		J^π(level): From (p,α) from angular distribution and analyzing powers .
2961.47	17/2-		E(level): ΔJ=1 band based on 13/2-.
2996	5/2+		XREF: C(2995)I(2997)J(2998).
3120	(13/2-)		J^π(level): From (p,α) from angular distribution and analyzing powers .
3262.9	9/2+,11/2+		XREF: I(3273).
3351	3/2+,5/2+		E(level): From (p,γ), only determined by primary γ spectra.
3402.4	(19/2-)		E(level): ΔJ=1 band based on 13/2-.
3500	(11/2+)		J^π(level): From (p,α) from angular distribution and analyzing powers .
3552.95	(23/2+)	0.083 ps 21	E(level): yrast states, positive parity.
E(level)	J^π(level)	T_1/2(level)	Comments
3730	(7/2-)		J^π(level): From (p,α) from angular distribution and analyzing powers .
3766.6	(21/2-)		E(level): ΔJ=1 band based on 13/2-.
3840	(11/2-)		J^π(level): From (p,α) from angular distribution and analyzing powers .
4039.40	(25/2+)	0.17 ps 4	E(level): yrast states, positive parity.
5288.48	(27/2+)	0.10 ps 3	E(level): yrast states, positive parity.
5759.59	(27/2-)	> 2.1 ps	E(level): Other positive parity yrast states.
5934.50	(29/2-)	1.8 ps 4	E(level): Other positive parity yrast states.
6535.5	(31/2-)	0.18 ps 4	E(level): Other positive parity yrast states.
7016.6	(33/2-)	0.11 ps 3	E(level): Other positive parity yrast states.
10537	5/2+	23 keV 1	Γ_p=3.44 20 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
10923	1/2+	40 keV 2	Γ_p=14.0 10 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
11468	3/2+	21 keV 2	Γ_p=1.6 2 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
11739	1/2+	33 keV 2	Γ_p=9.5 5 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
11900	1/2+	34 keV 2	Γ_p=11.5 6 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
11966	(3/2)+	25 keV 8	Γ_p=1.4 10 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
11966	(5/2+)	25 keV 8	Γ_p=1.0 8 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
12371	3/2+	24 keV 1	Γ_p=5.2 3 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
12661	1/2+	44 keV 4	Γ_p=11.9 7 J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
12968	3/2+		J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.
13076	5/2+		J^π(level): From analyzing power and shape of the resonance curve in (p,p’) IAR.

E(level)	E(gamma)	Comments
793.73	793.7	M(γ): α(K)(exp)=1.016×10^-3 97 gives mult=M1,E2. Placement in level scheme requires ΔJ=2. See dataset from (p,nγ).
982.89	982.9	M(γ): α(K)(exp)=0.55×10^-3 13 gives mult=M1,E2. See (p,ng) dataset.
1152.71	771.9	M(γ): α(K)(exp)=1.19×10^-3 33 gives mult=M1,E2. Placement in level scheme requires ΔJ=2. See dataset from (p,nγ).
1404.47	1024.0	M(γ): M1,E2 from α(K)exp, but placement in level scheme requires ΔJ=2
1623.50	444.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1623.50	643.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1629.94	836.2	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
1704.7	501.9	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	523.3	I(γ): Iγ=91 in (p,γ)
	910.5	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1801.64	598.1	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1801.64	818.5	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): Iγ=35 in (p,γ). From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1849	665.2	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1849	864.1	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
1979.95	574.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): from (p,γ); not reported in (p,nγ), so placement may be questionable.. From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2038.05	633.6	M(γ): Using δ from 1980Fi06 with the α(K)exp from 1980Ta13 and comparing with calculations from BrICC yields the M1⁺E2 multipolarity
2038.05	1657.2	I(γ): from (p,nγ); other: 49 4 from (⁸⁰Se(¹¹B,4nγ)).
2072.7	1279.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2073.31	920.6	I(γ): Not well determined. (p,nγ), In ⁸⁷Zr β⁺ there is only a weak 921γ, with the spectrum suggesting roughly half that of the 1692γ, whereas (p,nγ) shows the 920γ intensity as slightly less than the 1692γ. In (p,γ) the 920γ intensity is a little over 4 times as high as that of the 1692γ, suggesting, for this case at least, a doublet was observed. In β⁺, the 1279γ shown dexciting the 2072.7 was not observed, indicating another level close to this energy, as shown here.
2083.0	880.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	901.3	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	930.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.. Multiply placed with undivided intensity I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.. Multiply placed with undivided intensity
	1100.1	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	2082.8	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2112.3	706.3	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2112.3	930.0	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.. Multiply placed with undivided intensity I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.. Multiply placed with undivided intensity
E(level)	E(gamma)	Comments
2158.9	2158.9	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2202.17	611.2	I(γ): from (p,nγ); other: 67 17 from ⁸⁷Zr β+ decay.
	797.0	I(γ): 100 34 from β⁺
	1048	I(γ): From β⁺, as not seen in (p,nγ)
	1410.0	I(γ): From β⁺, as not seen in (p,nγ)
	1821.4	I(γ): from (p,nγ); other: 50 17 from ⁸⁷Zr β+ decay.
2210.6	409.2	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2210.6	2210.4	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2244.8	619.7	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	1042.6	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	1451.9	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2292.3	1139.6	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2302.61	711.4	I(γ): weak
2302.61	898.6	I(γ): weak
2353.55	746.6	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	949.4	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
	1559.7	E(γ): γ’s of 746 and 949 are reported in (p,γ) and 1559 is reported in (p,nγ).
2409	2408.3	E(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV. I(γ): From (p,γ); these values do not have uncertainties and the energies are quoted here to the nearest 0.1 keV.
2479.07	441.1	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
2648.91	169.9	M(γ): Supported by directional correlation of oriented states in (¹¹B,4nγ)
2676.06	309.1	M(γ): D+Q from (α,2nγ) angular distribution and E1⁺M2 for δ=+0.2 4 is eliminated from RUL
2808.4	1040.2	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
2961.47	312.6	I(γ): from ⁸⁰Se(¹¹B,4nγ).
2986.9	159.8	E(γ): Taken from (α,2nγ). From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
2986.9	558.7	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
E(level)	E(gamma)	Comments
3402.4	440.9	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3402.4	726.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3446.5	770.5	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3552.95	725.8	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3766.6	364.1	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3766.6	1090.6	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3908.8	142.2	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
3908.8	506.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
4039.40	486.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
4555.0	1568.2	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
4555.0	1727.6	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
4564.1	1011.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1117.6	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1161.7	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
4609.66	569.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1056.8	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1782.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
5228.2	1189.1	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1319.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1675.1	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
5288.48	678.8	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1249.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1735.8	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
5319.7	1553.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
5495.2	940.1	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
5495.2	1942.2	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
E(level)	E(gamma)	Comments
5759.59	264.3	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ) M(γ): Although a calculated mixing ratio of -0.20 20 for M2/E1 is reported in (¹¹β,4nγ), an M2 component is excluded by RUL for larger half-lives reasonably close to 2.1 ps
	439.7	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	531.5	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1195.6	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1720.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ) M(γ): (D+Q) from direction correlation of oriented nuclei in ⁸⁰Se(¹¹β,4nγ) and additional support from level scheme placement
5827.1	331.7	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1217.4	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	1787.8	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
5934.50	107.5	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	174.9	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	615.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	646.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
	706.3	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
6535.5	601.0	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)
7016.6	481.1	E(γ): From ⁸⁰Se(¹¹B,4nγ) I(γ): From ⁸⁰Se(¹¹B,4nγ)