List of levels for 89Y

ADOPTED LEVELS, GAMMAS for ⁸⁹Y

Author: Balraj Singh | Citation: Nucl. Data Sheets 114, 1 (2013) | Cutoff date: 20-Oct-2012

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-2833 keV 3	S(n)= 11482 keV 3	S(p)= 7076.8 keV 24	Q(α)= -7966.7 keV 23
Reference: 2012WA38

References:
A	⁸⁹Sr β^- decay (50.563 d)	B	⁸⁹Y IT decay (15.663 S)
C	⁸⁹Zr ε decay (4.161 M)	D	⁸⁹Zr ε decay (78.41 H)
E	⁷⁴Ge(¹⁸O,2npγ),⁷⁶Ge(¹⁸O,4NPG)	F	⁸⁷Rb(α,2nγ)
G	⁸⁸Sr(p,γ)	H	⁸⁸Sr(p,p’),(pol p,p) IAR
I	⁸⁸Sr(d,n)	J	⁸⁸Sr(³He,d)
K	⁸⁸Sr(¹⁶O,¹⁵N)	L	⁸⁹Y(γ,γ’)
M	⁸⁹Y(E,E’)	N	⁸⁹Y(n,n’)
O	⁸⁹Y(n,n’γ)	P	⁸⁹Y(p,p’),(pol p,p’)
Q	⁸⁹Y(p,p’γ)	R	⁸⁹Y(d,d’)
S	⁸⁹Y(³He,³He’)	T	⁸⁹Y(α,α’)
U	⁹⁰Zr(E,E’p)	V	⁹⁰Zr(n,d)
W	⁹⁰Zr(d,³He),(pol d,³He)	X	⁹²Zr(p,α),(pol p,α)
Y	⁸⁸Sr(p,γ) IAR	Z	⁸⁸Sr(p,n) IAR
a	⁸⁹Y(γ,p) IAR	b	⁸⁹Y(γ,p),(γ,XN):GDR
c	⁸⁹Y(E,E’p) IAR	d	⁸⁹Y(E,p): GIANT RES
e	⁸⁹Y(π⁺,π⁺’),(π^-,π^-’)	f	⁸⁹Y(π⁺,K+):HYPERNUCLEUS
g	⁸⁹Y(HI,HI)	h	⁹⁰Zr(pol t,α),(t,α)
i	⁹⁰Zr(α,α’p)	j	⁹⁰Zr(⁶Li,⁷Be)
k	⁹⁰Zr(¹²C,¹³N),(¹³C,¹⁴N)	l	⁹¹Zr(d,α)
m	⁹³Nb(³He,⁷Be)

Other reactions:

⁸⁹Y(e,γ) E=50-100 keV: 1987Am01

⁸⁹Y(K^-,K^-) (analysis): 1983Ba71

⁸⁹Y(γ,γ) E=35.86, 39.36 keV: 1996Ra30, 1996Ra29

⁸⁹Y(π⁺,K⁺) E=1060 MeV/c: 1996Ha05, 1996Ha47, 1995Aj01, 1991Pi07, 1989Pi11, 1989Ch32, 1988Ch48. Measured |L hypernuclei spectra.

⁸⁹Y(K^-,π^-) E=720 MeV/c: 1981Be17 (also 1981Bo09)

⁹⁰Zr(p,2p): 1967Ar11 (E=156 MeV), 1971La16 (E=600 MeV)

⁹⁰Zr(π+,pπ+), (π^-,pπ-) E=500 MeV: 1998Mo09

⁹³Nb(γ,α) E=16-25 MeV: 1991An07, 1991An22

NMR studies (recent): 1997Se12, 1997Au07, 1996Oh03, 1996Wi28, 1996St23, 1995So19, 1995Go39, 1994Ma25, 1993Al02

Hyperfine structure measurements (selected): 2010Ba31, 2006Ca38, 1994Ri10, 1992Vi04, 1988Go04

Structure calculations (selected references only): 2011Ro08, 1997He24, 1996Ri01, 1995Re08, 1995Gu09, 1992Si14, 1990Va13. C. Sharma et al., Eur. Phys. J. A48, 138 (2012) analyzed structures of positive-parity bands by projected shell-model calculations

⁸⁹Y isotope identified using mass spectrometry technique by F.W. Aston, Nature 112, 449 (1923)

Levels: Levels marked with XREF=Y in the level table refer to the following reactions and levels populated therein:

Levels: ⁸⁸Sr(p,γ) IAR: 12076, 13070, 14060, 14492, 15837

Levels: ⁸⁸Sr(p,n) IAR: 12076, 13070, 13991, 14060, 14492, 14781

Levels: ⁸⁹Y(γ,p),(γ,xn):GDR: 16790, 21800

Levels: ⁸⁹Y(γ,p) IAR: 14060, 15800, 16800, 17000 (GDR), 17400, 21000 (GDR)

Levels: ⁸⁹Y(e,e’p) IAR: 13000, 14500, 14900, 15800, 16700, 17700, 18900, 20300, 21700

Levels: ⁸⁹Y(e,p): giant res: 16800, 27000

Levels: ⁸⁹Y(π⁺,π⁺’),(π^-,π^-’): 0

Levels: ⁸⁹Y(π⁺,K⁺):hypernucleus: 0, 6010, 7380, 12790, 14420, 19980, 21680, 27000

Levels: ⁸⁹Y(HI,HI): 0

Levels: ⁹⁰Zr(pol t,α),(t,α): 0, 909, 1507, 1745

Levels: ⁹⁰Zr(α,α’p): 0, 910, 1600

Levels: ⁹⁰Zr(⁶Li,⁷Be): 0, 909, 1507, 1745

Levels: ⁹⁰Zr(¹²C,¹³N),(¹³C,¹⁴N): 0, 910, 1510, 1740, 2220

Levels: ⁹¹Zr(d,α): 0, 910, 1510, 1740, 4310

Levels: ⁹³Nb(³He,⁷Be): 0, 910

Q-value: Note: Current evaluation has used the following Q record -2833.0 28 11482.229 7077.2 25-7967.2 25 2011AuZZ

Q-value: S(2n)=20833.9 28, S(2p)=17689.8 25 (2011AuZZ)

Q-value: Values in 2003Au03: Q(β^-)=-2832.9 28, S(n)=11474 3, S(p)=7069.0 26, Q(α)=-7959.3 26, S(2n)=20825.7 28, S(2p)=17681.9 26

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F G I J K L M N O P Q R S T U V W X e f g h i j k l m	1/2-	STABLE
908.97 3	A B D E F G I J K L M N O P Q S T U W X h i j k l m	9/2+	15.663 s 5 % IT = 100	908.960 25	100	M4+E5	0.0	1/2-
1507.41 9	C F G I J K L M N O P Q R S T U V W X h i j k l	3/2-	23.9 fs +25-21	1507.42 10	100	M1+E2	0.0	1/2-
1744.74 18	D F G I J K L M N O P Q R S T U W X h i j k l	5/2-	0.64 ps 6	1744.7 2	100	E2	0.0	1/2-
2222.43 18	F G I J K M N O P Q R S T X k	5/2+	0.97 ps 28	715.2 3 1313.2 3	46.0 9 100.0 9	[E1] [E2]	1507.41 908.97	3/2- 9/2+
2529.80 20	D F G M N O P Q R S T X	7/2+	0.08 ps 4	1620.8 2	100		908.97	9/2+
2566.55 15	D E F G N O P	11/2+	0.35 ps 7	1657.5 2	100	M1+E2	908.97	9/2+
2622.1 3	D F G J K N O P Q W X	9/2+	0.21 ps 10	1713.1 3	100	(M1+E2)	908.97	9/2+
2687?	G
2871.7 4	G I J M N O P Q R S T V X	(7/2)+	< 0.2 ps	1962.8 4	100		908.97	9/2+
2881.53 10	G I J K L N O P R U V X	(3/2)-	19.9 fs +21-19	2881.48 10	100		0.0	1/2-
2892.98 15	E F O P	13/2+	0.18 ps 3	326.5 5 1984.1 2	≈1.4 100 3	E2	2566.55 908.97	11/2+ 9/2+
3067.76 10	G I J K L N O P	3/2-	45.0 fs +15-11	1559.8 5 3067.7 1	10.6 8 100.0 8	(M1+E2)	1507.41 0.0	3/2- 1/2-
3107.26 24	F G I L M N O P R S T W X	(5/2)-	0.034 ps 3	1361.8 9 1599.8 4 3107.3 3	11.0 9 10.2 10 100.0 13	(M1+E2) (M1+E2) [E2]	1744.74 1507.41 0.0	5/2- 3/2- 1/2-
3138.9 3	G L N O P R V X	(5/2)-	0.11 ps +7-3	916.1 5 1631.6 4 3139.1 5	12.1 10 16.3 8 100.0 12	[E1] [E2]	2222.43 1507.41 0.0	5/2+ 3/2- 1/2-
3247.6 5	G O P	(3/2,5/2)		1740.2 5 3247.5 9	100.0 19 7.4 19	D+Q	1507.41 0.0	3/2- 1/2-
3343.44 15	E F O	13/2-	0.42 ps 14	450.5 1 776.89 6	6.2 6 100 3	E1 E1	2892.98 2566.55	13/2+ 11/2+
3360	X
3410.7 4	G O P	(5/2+)		2501.4 5	100		908.97	9/2+
3451.3 6	G O P	(7/2+)		2542.3 6	100	D+Q	908.97	9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3503.6 4	G O P	(7/2-)		364.7 5 1996.2 5	6.3 10 100.0 10		3138.9 1507.41	(5/2)- 3/2-
3515.9 3	G I J K L O P V	(3/2)-		1770.0 10 ? 3515.9 3	100	(M1+E2)	1744.74 0.0	5/2- 1/2-
3557.4 5	G O P V	(7/2-)		1812.5 9 2050.1 8 2648.3 6	25 4 100 3 76 3	D+Q	1744.74 1507.41 908.97	5/2- 3/2- 9/2+
3560	X	(1/2)
3621.1 6	G O Y i j l	(11/2)		2712.1 6	100	D+Q	908.97	9/2+
3630.3 6	O P	(11/2)+		2721.3 6	100	(M1+E2)	908.97	9/2+
3715.3 4	G I J K M O P R S T Y Z e l m	5/2+		843.6 5 1492.7 4 2806.7 8	31.1 23 80 4 100 5	(M1+E2)	2871.7 2222.43 908.97	(7/2)+ 5/2+ 9/2+
3747.7 8	O P	(9/2)+		2838.7 8	100	(M1+E2)	908.97	9/2+
3752.9 4	O	(5/2+)		341.9 5 2008.3 6 2844.2 8	12.0 12 100 3 35 3		3410.7 1744.74 908.97	(5/2+) 5/2- 9/2+
3790	X
3810	X
3848.3 4	G O P	(3/2-,5/2-)		2103.5 5 2340.8 6	100.0 14 17.8 14	(M1+E2) (M1+E2)	1744.74 1507.41	5/2- 3/2-
3862.4 5	G O P	(3/2,5/2)-		2355.1 5 3861.8 9	100.0 24 31.1 24		1507.41 0.0	3/2- 1/2-
3924 5	P
3976.8 6	O P	(11/2)+		1447.0 5	100		2529.80	7/2+
3992.2 1	G I L M O P S T U	3/2-	9.3 fs +11-10	3992.1 1	100	(M1+E2)	0.0	1/2-
4015.3 7	G I J O P	1/2+		1792.8 7 4015.4 15	75 7 100 7		2222.43 0.0	5/2+ 1/2-
4022.96 23	I O P R	(3/2)-		955.0 3 1800.8 4 2278.6 7 2515.3 6 4022.9 15	57 3 73 4 77 4 100 4 40 4	(M1+E2) (M1+E2) (M1+E2)	3067.76 2222.43 1744.74 1507.41 0.0	3/2- 5/2+ 5/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4060	X
4104.9 5	O P	(7/2+)		1574.9 7 1882.5 8 3196.3 12	100 6 78 6 61 5	(M1+E2) (M1+E2)	2529.80 2222.43 908.97	7/2+ 5/2+ 9/2+
4132.22 16	E F	15/2-	1.59 ps 28	788.6 1 1239.28 7	49 3 100 3	M1+E2 E1	3343.44 2892.98	13/2- 13/2+
4171.3 1	G L M O P S T e i m	3/2-,5/2-	10.1 fs +15-11	4171.2 1	100		0.0	1/2-
4188.1 6	I J K O P R	5/2+		2680.9 7 3278.7 9	100.0 22 19.2 22		1507.41 908.97	3/2- 9/2+
4230.4 12	O P R	(7/2)		3321.4 12	100		908.97	9/2+
4251 5	L P
4254.40 23	F	(15/2+)	1.4 ps 7	1361.2 2	100		2892.98	13/2+
4309.3 6	O P T e i l	(7/2)-		2086.7 7 3400.5 9	100.0 14 13.1 14		2222.43 908.97	5/2+ 9/2+
4334.1 12	O P R S			3425.1 12	100		908.97	9/2+
4354.7 10	O P R S			3445.7 10	100		908.97	9/2+
4383 5	P
4408.4 8	O P	1/2,3/2,5/2-		2901.0 10 4408.2 13	67 8 100 8		1507.41 0.0	3/2- 1/2-
4449.75 16	E F	17/2-	4.5 ps 10	317.5 1 1106.5 1	50.0 20 100.0 10	M1 E2	4132.22 3343.44	15/2- 13/2-
4457.6 7	I O P T	7/2-,9/2-		1927.8 6	100		2529.80	7/2+
4460 20	I J T	(1/2+)
4476.3 13	I J O P R S T	(5/2+)		2253.8 12	100		2222.43	5/2+
4489 5	P R S T
4508 5	P R
4529.3 16	O P X e g	5/2+,7/2+		3620.3 16	100		908.97	9/2+
4537.5 20	O P	3/2-,5/2-		4537.4 20	100		0.0	1/2-
4555 5	P T	7/2-,9/2-
4588 5	I J K P T	5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4603 5	P T	7/2-,9/2-
4616.8 5	L	1/2,3/2,5/2-		4616.7 5			0.0	1/2-
4625.8 5	L	1/2,3/2,5/2-		4625.7 5			0.0	1/2-
4636 5	P
4654 5	P
4682 5	P
4737 5	P	3/2-,5/2-
4770 5	P R S
4785 5	P R
4817 5	P R
4825.38 17	E F	17/2+	≥ 3.5 ps	570.5 3 693.2 2 1931.9 3	11 6 100 7 14 4	E1 (E2)	4254.40 4132.22 2892.98	(15/2+) 15/2- 13/2+
4831 5	J P e m	3/2+,5/2+
4838.59 17	F	19/2-	21 ps 8	388.9 1 706.3 1	100 1 51 9	M1+E2 E2	4449.75 4132.22	17/2- 15/2-
4849 5	I P	3/2-,5/2-
4862 5	I P X
4888 5	P X
4907 5	P X
4920.46 17	E F	(19/2+)	6.2 ps 21	95.07 3 470.72 5	38 3 100 5	(M1+E2) E1	4825.38 4449.75	17/2+ 17/2-
4927 5	J K P
4954 5	J K P
4973 5	P
4992 1	L	1/2,3/2,5/2-		4991 1			0.0	1/2-
5006 8	P U W g	(5/2)-
5026 8	P U
5046 8	P U
5075 8	I J K P g i m	(1/2+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5085.4 6	L P b g m	1/2,3/2,5/2-		5085.3 6			0.0	1/2-
5099 8	P X
5115 8	P S X
5125 8	P S X
5152.1 8	L P e g i m	1/2,3/2,5/2-		5151.9 8			0.0	1/2-
5167.7 3	L P Z g i	1/2,3/2,5/2-		3660.6 10 5167.5 3	4 2 100 2		1507.41 0.0	3/2- 1/2-
5183 8	J P b g i	3/2+,5/2+
5211 8	P X g j	(3/2-)
5257 8	P
5263.88 20	E F	(21/2+)	1.46 ps 28	343.37 12 425.6 3	100.0 18 1.55 24	M1 [E1]	4920.46 4838.59	(19/2+) 19/2-
5275 8	J P Z g j	(1/2+)
5289 8	P	3/2-,5/2-
5303 8	P
5309.83 20	F	(21/2-)	4.5 ps 9	471.1 2 860.1 1	100 10 5.3 6	(M1) (E2)	4838.59 4449.75	19/2- 17/2-
5321 8	P
5343 8	I J P e g l	(1/2+)
5362 8	I P
5382 8	P X g l m	(1/2)
5412.1 4	F	(19/2-)	1.25 ps 28	962.3 3	100		4449.75	17/2-
5419.4 5	L P e g i j	1/2,3/2,5/2-		5419.2 5			0.0	1/2-
5430 8	J P	(3/2+,5/2+)
5455 8	P
5476 8	P
5506 8	P
5542 8	P
5562 8	P
5582 8	P
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5592 8	P X
5614.4 15	L	1/2,3/2,5/2-		5614.2 15			0.0	1/2-
5625.8 2	I J L P X Y g j	1/2,3/2,5/2-		4117.4 5 5625.6 2	9 2 100 2		1507.41 0.0	3/2- 1/2-
5631 8	I J P X
5647 8	I P
5653.9 15	L	1/2,3/2,5/2-		5653.7 15			0.0	1/2-
5668 8	P X
5694 8	P S X
5725 8	J P
5739 8	J P
5753 8	P
5774 8	P
5789.4 8	L P Z b g l	1/2,3/2,5/2-		5789.2 8			0.0	1/2-
5796.4 8	L	1/2,3/2,5/2-		5796.2 8			0.0	1/2-
5801 8	P
5820 8	P
5843 8	P
5853 8	P
5879.4 4	F	(19/2+)	0.14 ps 10	615.5 3	100	(M1)	5263.88	(21/2+)
5888 8	I J K P Z g m	3/2+,5/2+
5910.7 2	L P b g i	1/2,3/2,5/2-		3028 2 5910.5 2	4 3 100 3		2881.53 0.0	(3/2)- 1/2-
5923.4 9	L	1/2,3/2,5/2-		5923.2 9			0.0	1/2-
5950 8	P
5981 8	P
6004 8	P
6.01E3 13	f
6100 20	I J	3/2+,5/2+
6122.9 2	L	1/2,3/2,5/2-		6122.7 2			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6158.9 4 ?	F			895.0 3 ?			5263.88	(21/2+)
6198.90 21	E F	(23/2+)	0.19 ps 4	935.01 5 1360.3 3 ?	100	M1+E2	5263.88 4838.59	(21/2+) 19/2-
6200 20	I J	7/2+,9/2+
6201.9 8	I L	1/2,3/2,5/2-		6201.7 8			0.0	1/2-
6206.3 3	I L	1/2,3/2,5/2-		6206.1 3			0.0	1/2-
6275.6 2	J K L	1/2,3/2,5/2-		6275.4 2			0.0	1/2-
6297.6 3	J K L	1/2,3/2,5/2-		6297.4 3			0.0	1/2-
6300 20	I	1/2+
6331.6 2	L	1/2,3/2,5/2-		6331.4 2			0.0	1/2-
6359.1 2	L	1/2,3/2,5/2-		6358.9 2			0.0	1/2-
6398.2 2	L	1/2,3/2,5/2-		6398.0 2			0.0	1/2-
6441.5 2	L	1/2,3/2,5/2-		2925 3 6441.2 2	10 8 100 8		3515.9 0.0	(3/2)- 1/2-
6472.3 18	I J L	1/2,3/2,5/2-		6472.0 18			0.0	1/2-
6479 3	L	1/2,3/2,5/2-		6479 3			0.0	1/2-
6493.5 8	I J L	1/2,3/2,5/2-		6493.5 8			0.0	1/2-
6.5E3 3	U	(7/2-)
6532.3 3	L	1/2,3/2,5/2-		6532.0 3			0.0	1/2-
6592.2 3	J L	1/2,3/2,5/2-		6591.9 3			0.0	1/2-
6608.9 5	J L	1/2,3/2,5/2-		6608.6 5			0.0	1/2-
6651.6 8	L	1/2,3/2,5/2-		6651.3 8			0.0	1/2-
6666.8 8	L	1/2,3/2,5/2-		6666.5 8			0.0	1/2-
6674.4 3	F	(23/2+)	≤ 0.7 ps	1410.5 2	100		5263.88	(21/2+)
6680 20	J
6728 2	L	1/2,3/2,5/2-		6728 2			0.0	1/2-
6750	M		1.0 MeV 2
6751.1 12	L	1/2,3/2,5/2-		6750.8 12			0.0	1/2-
6772.0 14	L	1/2,3/2,5/2-		6771.7 14			0.0	1/2-
6780 20	J K W Y m	7/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6782.9 6	L	1/2,3/2,5/2-		6782.6 6			0.0	1/2-
6798.2 5	L	1/2,3/2,5/2-		6797.9 5			0.0	1/2-
6852.4 8	L	1/2,3/2,5/2-		6852.1 8			0.0	1/2-
6866 2	L	1/2,3/2,5/2-		6866 2			0.0	1/2-
6880	S
6921 2	L	1/2,3/2,5/2-		6921 2			0.0	1/2-
6934.7 11	L	1/2,3/2,5/2-		6934.4 11			0.0	1/2-
6944.5 12	L	1/2,3/2,5/2-		6944.2 12			0.0	1/2-
6959.6 14	L	1/2,3/2,5/2-		6959.3 14			0.0	1/2-
6987.4 15	L	1/2,3/2,5/2-		6987.1 15			0.0	1/2-
7003.8 3	L	1/2,3/2,5/2-		7003.5 3			0.0	1/2-
7066.8 15	L	1/2,3/2,5/2-		7066.5 15			0.0	1/2-
7077.7 3	L	1/2,3/2,5/2-		7077.4 3			0.0	1/2-
7.1E3	T
7106 3	L	1/2,3/2,5/2-		7106 3			0.0	1/2-
7118.2 6	L	1/2,3/2,5/2-		7117.9 6			0.0	1/2-
7147.1 6	L	1/2,3/2,5/2-		7146.8 6			0.0	1/2-
7178.6 3	L	1/2,3/2,5/2-		7178.3 3			0.0	1/2-
7183.7 3	F	(25/2+)	0.21 ps 7	985 1 ? 1920.2 3	≈36 100 22	[E2]	6198.90 5263.88	(23/2+) (21/2+)
7190?	J
7193.8 4	F	(23/2+)	0.35 ps 14	994.5 5 1930 1	100 22 ≈89		6198.90 5263.88	(23/2+) (21/2+)
7198 2	L	1/2,3/2,5/2-		7198 2			0.0	1/2-
7225.3 8	L	1/2,3/2,5/2-		7225.0 8			0.0	1/2-
7240 3	L	1/2,3/2,5/2-		7240 3			0.0	1/2-
7255 3	L	1/2,3/2,5/2-		7255 3			0.0	1/2-
7259.5 3	F	(23/2+)		1995.6 4	100		5263.88	(21/2+)
7.3E3 40	W
7304.4 5	L	1/2,3/2,5/2-		7304.1 5			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7325.4 9	L	1/2,3/2,5/2-		7325.1 9			0.0	1/2-
7.38E3 21	f
7383.7 5	L	1/2,3/2,5/2-		7383.4 5			0.0	1/2-
7420.4 8	L	1/2,3/2,5/2-		7420.1 8			0.0	1/2-
7431.6 3	E F	(25/2+)	0.49 ps 14	172.1 1 757.1 2 1232.6 2	34 4 ≈42 100 8	(M1) (M1) (M1)	7259.5 6674.4 6198.90	(23/2+) (23/2+) (23/2+)
7452.1 8	L	1/2,3/2,5/2-		7451.8 8			0.0	1/2-
7475.2 15	L	1/2,3/2,5/2-		7474.9 15			0.0	1/2-
7484.1 11	L	1/2,3/2,5/2-		7483.8 11			0.0	1/2-
7527.9 14	L	1/2,3/2,5/2-		7527.6 14			0.0	1/2-
7536 3	L	1/2,3/2,5/2-		7536 3			0.0	1/2-
7548 5	L	1/2,3/2,5/2-		7548 5			0.0	1/2-
7556 4	L	1/2,3/2,5/2-		7556 4			0.0	1/2-
7566 3	L	1/2,3/2,5/2-		7566 3			0.0	1/2-
7588.1 18	L	1/2,3/2,5/2-		7587.8 18			0.0	1/2-
7590.0 3	F	(25/2+)	0.35 ps 14	396.1 2	100	(M1)	7193.8	(23/2+)
7618.4 9	L	1/2,3/2,5/2-		7618.1 9			0.0	1/2-
7640.8 11	L	1/2,3/2,5/2-		7640.4 11			0.0	1/2-
7652.3 20	L	1/2,3/2,5/2-		7651.9 20			0.0	1/2-
7666.1 6	L	1/2,3/2,5/2-		7665.7 6			0.0	1/2-
7692.2 8	L	1/2,3/2,5/2-		7691.8 8			0.0	1/2-
7703.3 15	L	1/2,3/2,5/2-		7702.9 15			0.0	1/2-
7714.0 14	L	1/2,3/2,5/2-		7713.6 14			0.0	1/2-
7722.2 9	J K L Z i j	(1/2+)		7721.8 9			0.0	1/2-
7750.5 5	L	1/2,3/2,5/2-		7750.1 5			0.0	1/2-
7774.4 5	L	1/2,3/2,5/2-		7774.0 5			0.0	1/2-
7787.5 3	L	1/2,3/2,5/2-		7787.1 3			0.0	1/2-
7799.2 8	L	1/2,3/2,5/2-		7798.8 8			0.0	1/2-
7811.8 17	L	1/2,3/2,5/2-		7811.4 17			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7830.2 6	L	1/2,3/2,5/2-		7829.8 6			0.0	1/2-
7834.6 3	E F	(27/2+)	1.25 ps 28	244.6 1 402.9 2 650.9 1	58 8 ≈226 100 13	(M1) M1 (M1)	7590.0 7431.6 7183.7	(25/2+) (25/2+) (25/2+)
7838.7 8	L	1/2,3/2,5/2-		7838.3 8			0.0	1/2-
7866.8 17	L	1/2,3/2,5/2-		7866.4 17			0.0	1/2-
7902.5 5	L	1/2,3/2,5/2-		7902.1 5			0.0	1/2-
7920.5 3	L	1/2,3/2,5/2-		7920.1 3			0.0	1/2-
7922.7 2	L	1/2,3/2,5/2-		7922.3 2			0.0	1/2-
7937.8 9	L	1/2,3/2,5/2-		7937.4 9			0.0	1/2-
7961.7 11	L	1/2,3/2,5/2-		7961.3 11			0.0	1/2-
7968.8 9	L	1/2,3/2,5/2-		7968.4 9			0.0	1/2-
7986.0 8	L	1/2,3/2,5/2-		7985.6 8			0.0	1/2-
7996.1 5	L	1/2,3/2,5/2-		7995.7 5			0.0	1/2-
8018 2	L	1/2,3/2,5/2-		8018 2			0.0	1/2-
8027.7 8	L	1/2,3/2,5/2-		8027.3 8			0.0	1/2-
8050	M		1.2 MeV 2
8067.3 5	L	1/2,3/2,5/2-		8066.9 5			0.0	1/2-
8099.0 14	L	1/2,3/2,5/2-		8098.6 14			0.0	1/2-
8129.3 3	L	1/2,3/2,5/2-		8128.9 3			0.0	1/2-
8142.1 12	L	1/2,3/2,5/2-		8141.7 12			0.0	1/2-
8150.8 17	L	1/2,3/2,5/2-		8150.4 17			0.0	1/2-
8159.7 9	L	1/2,3/2,5/2-		8159.3 9			0.0	1/2-
8175.6 9	L	1/2,3/2,5/2-		8175.2 9			0.0	1/2-
8198.9 5	L	1/2,3/2,5/2-		8198.5 5			0.0	1/2-
8210.9 8	L	1/2,3/2,5/2-		8210.5 8			0.0	1/2-
8221.2 3	L	1/2,3/2,5/2-		8220.8 3			0.0	1/2-
8264.2 3	E F	(29/2+)	0.97 ps 21	429.6 1 832.9?	100 16 <15	M1+E2 [E2]	7834.6 7431.6	(27/2+) (25/2+)
8270.7 6	L	1/2,3/2,5/2-		8270.3 6			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8285.4 17	L	1/2,3/2,5/2-		8285.0 17			0.0	1/2-
8311.0 5	L	1/2,3/2,5/2-		8310.6 5			0.0	1/2-
8320.1 6	L	1/2,3/2,5/2-		8319.7 6			0.0	1/2-
8330.4 14	L	1/2,3/2,5/2-		8330.0 14			0.0	1/2-
8338.1 8	L	1/2,3/2,5/2-		8337.7 8			0.0	1/2-
8369 2	J L	1/2,3/2,5/2-		8369 2			0.0	1/2-
8380.0 9	L	1/2,3/2,5/2-		8379.6 9			0.0	1/2-
8403.1 9	L	1/2,3/2,5/2-		8402.7 9			0.0	1/2-
8438.0 8	L	1/2,3/2,5/2-		8437.6 8			0.0	1/2-
8455 4	L	1/2,3/2,5/2-		8455 4			0.0	1/2-
8466.9 8	L	1/2,3/2,5/2-		8466.5 8			0.0	1/2-
8483.2 9	L	1/2,3/2,5/2-		8482.8 9			0.0	1/2-
8495.2 8	L	1/2,3/2,5/2-		8494.8 8			0.0	1/2-
8513.5 5	L	1/2,3/2,5/2-		8513.1 5			0.0	1/2-
8530.6 8	L	1/2,3/2,5/2-		8530.2 8			0.0	1/2-
8548.3 12	L	1/2,3/2,5/2-		8547.9 12			0.0	1/2-
8556.0 9	L	1/2,3/2,5/2-		8555.6 9			0.0	1/2-
8568.0 6	L	1/2,3/2,5/2-		8567.6 6			0.0	1/2-
8586.9 6	L	1/2,3/2,5/2-		8586.5 6			0.0	1/2-
8603 3	L	1/2,3/2,5/2-		8603 3			0.0	1/2-
8610.8 12	L	1/2,3/2,5/2-		8610.4 12			0.0	1/2-
8642.1 8	L	1/2,3/2,5/2-		8641.6 8			0.0	1/2-
8668.0 5	L	1/2,3/2,5/2-		8667.5 5			0.0	1/2-
8720.4 4	E F	(31/2+)	0.48 ps 14	456.2 2 885.9?	100 16 <23	(M1) [E2]	8264.2 7834.6	(29/2+) (27/2+)
8764.2 3	L	1/2,3/2,5/2-		8763.7 3			0.0	1/2-
8779.3 11	L	1/2,3/2,5/2-		8778.8 11			0.0	1/2-
8843.4 5	L	1/2,3/2,5/2-		8842.9 5			0.0	1/2-
8864 4	L	1/2,3/2,5/2-		8864 4			0.0	1/2-
8877.3 5	L	1/2,3/2,5/2-		8876.8 5			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8899.3 6	L	1/2,3/2,5/2-		8898.8 6			0.0	1/2-
8926.3 14	L	1/2,3/2,5/2-		8925.8 14			0.0	1/2-
8981 3	L	1/2,3/2,5/2-		8981 3			0.0	1/2-
8994.5 17	L	1/2,3/2,5/2-		8994.0 17			0.0	1/2-
9002.8 15	L	1/2,3/2,5/2-		9002.3 15			0.0	1/2-
9024.2 9	L	1/2,3/2,5/2-		9023.7 9			0.0	1/2-
9043.4 6	L	1/2,3/2,5/2-		9042.9 6			0.0	1/2-
9057.8 15	L	1/2,3/2,5/2-		9057.3 15			0.0	1/2-
9069.0 11	L	1/2,3/2,5/2-		9068.5 11			0.0	1/2-
9082 2	L	1/2,3/2,5/2-		9082 2			0.0	1/2-
9093.4 8	L	1/2,3/2,5/2-		9092.9 8			0.0	1/2-
9112.7 19	L	1/2,3/2,5/2-		9112.2 19			0.0	1/2-
9121.4 8	L	1/2,3/2,5/2-		9120.9 8			0.0	1/2-
9147.0 9	L	1/2,3/2,5/2-		9146.5 9			0.0	1/2-
9161.2 14	L	1/2,3/2,5/2-		9160.7 14			0.0	1/2-
9175.7 9	L	1/2,3/2,5/2-		9175.2 9			0.0	1/2-
9191.2 8	L	1/2,3/2,5/2-		9190.7 8			0.0	1/2-
9204.5 5	L	1/2,3/2,5/2-		9204.0 5			0.0	1/2-
9240.0 6	L	1/2,3/2,5/2-		9239.5 6			0.0	1/2-
9256.1 6	L	1/2,3/2,5/2-		9255.6 6			0.0	1/2-
9280.2 15	L	1/2,3/2,5/2-		9279.7 15			0.0	1/2-
9290.8 15	L	1/2,3/2,5/2-		9290.3 15			0.0	1/2-
9301.1 12	L	1/2,3/2,5/2-		9300.6 12			0.0	1/2-
9308.4 14	L	1/2,3/2,5/2-		9307.9 14			0.0	1/2-
9320 2	L	1/2,3/2,5/2-		9319 2			0.0	1/2-
9326.7 11	L	1/2,3/2,5/2-		9326.2 11			0.0	1/2-
9351.2 8	L	1/2,3/2,5/2-		9350.7 8			0.0	1/2-
9374.7 8	L	1/2,3/2,5/2-		9374.2 8			0.0	1/2-
9401.8 18	L	1/2,3/2,5/2-		9401.3 18			0.0	1/2-
9410.0 17	L	1/2,3/2,5/2-		9409.5 17			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
9449.6 9	L	1/2,3/2,5/2-		9449.1 9			0.0	1/2-
9471 3	L	1/2,3/2,5/2-		9470 3			0.0	1/2-
9482.0 15	L	1/2,3/2,5/2-		9481.5 15			0.0	1/2-
9503 3	L	1/2,3/2,5/2-		9502 3			0.0	1/2-
9532 4	L	1/2,3/2,5/2-		9531 4			0.0	1/2-
9541 3	L	1/2,3/2,5/2-		9540 3			0.0	1/2-
9575.6 18	L	1/2,3/2,5/2-		9575.0 18			0.0	1/2-
9593.6 15	L	1/2,3/2,5/2-		9593.0 15			0.0	1/2-
9623.7 11	L	1/2,3/2,5/2-		9623.1 11			0.0	1/2-
9660.9 8	L	1/2,3/2,5/2-		9660.3 8			0.0	1/2-
9679.4 2	L	1/2,3/2,5/2-		9678.8 2			0.0	1/2-
9901.0 8	L	1/2,3/2,5/2-		9900.4 8			0.0	1/2-
9912.0 8	L	1/2,3/2,5/2-		9911.4 8			0.0	1/2-
9964.2 9	L	1/2,3/2,5/2-		9963.6 9			0.0	1/2-
9973.2 6	L	1/2,3/2,5/2-		9972.6 6			0.0	1/2-
9990.3 12	L	1/2,3/2,5/2-		9989.7 12			0.0	1/2-
10005.8 15	L	1/2,3/2,5/2-		10005.2 15			0.0	1/2-
10017.6 18	L	1/2,3/2,5/2-		10017.0 18			0.0	1/2-
10037.4 15	L	1/2,3/2,5/2-		10036.8 15			0.0	1/2-
10049 2	L	1/2,3/2,5/2-		10048 2			0.0	1/2-
10065 4	L	1/2,3/2,5/2-		10064 4			0.0	1/2-
10073.9 19	L	1/2,3/2,5/2-		10073.3 19			0.0	1/2-
10091.3 14	L	1/2,3/2,5/2-		10090.7 14			0.0	1/2-
10108.2 14	L	1/2,3/2,5/2-		10107.6 14			0.0	1/2-
10141.3 12	L	1/2,3/2,5/2-		10140.7 12			0.0	1/2-
10173.0 11	L	1/2,3/2,5/2-		10172.4 11			0.0	1/2-
10194.5 24	L	1/2,3/2,5/2-		10193.9 24			0.0	1/2-
10276.2 19	L	1/2,3/2,5/2-		10275.6 19			0.0	1/2-
10286.9 19	L	1/2,3/2,5/2-		10286.3 19			0.0	1/2-
10307.1 11	L	1/2,3/2,5/2-		10306.5 11			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
10324.5 12	L	1/2,3/2,5/2-		10323.9 12			0.0	1/2-
10340.5 15	L	1/2,3/2,5/2-		10339.9 15			0.0	1/2-
10379.3 9	L	1/2,3/2,5/2-		10378.7 9			0.0	1/2-
10395.0 12	L	1/2,3/2,5/2-		10394.3 12			0.0	1/2-
10412.7 7	L	1/2,3/2,5/2-		10412.0 7			0.0	1/2-
10424.8 9	L	1/2,3/2,5/2-		10424.1 9			0.0	1/2-
10460.9 18	L	1/2,3/2,5/2-		10460.2 18			0.0	1/2-
10469 6	L	1/2,3/2,5/2-		10468 6			0.0	1/2-
10504 5	L	1/2,3/2,5/2-		10503 5			0.0	1/2-
10513.8 15	L	1/2,3/2,5/2-		10513.1 15			0.0	1/2-
10538.1 19	L	1/2,3/2,5/2-		10537.4 19			0.0	1/2-
10641.6 11	L	1/2,3/2,5/2-		10640.9 11			0.0	1/2-
10659.7 18	L	1/2,3/2,5/2-		10659.0 18			0.0	1/2-
10668.2 11	L	1/2,3/2,5/2-		10667.5 11			0.0	1/2-
10697.4 8	L	1/2,3/2,5/2-		10696.7 8			0.0	1/2-
10736.8 14	L	1/2,3/2,5/2-		10736.1 14			0.0	1/2-
10744.5 18	L	1/2,3/2,5/2-		10743.8 18			0.0	1/2-
10753 3	L	1/2,3/2,5/2-		10752 3			0.0	1/2-
10937 3	G	(5/2+)		9193 6 9431 6 10025 6 10937 6	34 9 47 12 11 3 100 25		1744.74 1507.41 908.97 0.0	5/2- 3/2- 9/2+ 1/2-
10967.5 11	L	1/2,3/2,5/2-		10966.8 11			0.0	1/2-
11058.9 15	L	1/2,3/2,5/2-		11058.2 15			0.0	1/2-
11069 2	L	1/2,3/2,5/2-		11068 2			0.0	1/2-
11081.8 9	L	1/2,3/2,5/2-		11081.1 9			0.0	1/2-
11106.9 18	L	1/2,3/2,5/2-		11106.2 18			0.0	1/2-
11192.5 19	L	1/2,3/2,5/2-		11191.7 19			0.0	1/2-
11200 2	L	1/2,3/2,5/2-		11199 2			0.0	1/2-
11419.3 14	L	1/2,3/2,5/2-		11418.5 14			0.0	1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
11463.0 18	L	1/2,3/2,5/2-		11462.2 18			0.0	1/2-
11474 3	L	1/2,3/2,5/2-		11473 3			0.0	1/2-
11498 3	L	1/2,3/2,5/2-		11497 3			0.0	1/2-
11517 2	L	1/2,3/2,5/2-		11516 2			0.0	1/2-
11535.9 5	L	1/2,3/2,5/2-		11535.1 5			0.0	1/2-
11560.7 6	L	1/2,3/2,5/2-		11559.9 6			0.0	1/2-
11571.2 8	L	1/2,3/2,5/2-		11570.4 8			0.0	1/2-
11601.8 17	L	1/2,3/2,5/2-		11601.0 17			0.0	1/2-
11611 2	L	1/2,3/2,5/2-		11610 2			0.0	1/2-
11623 3	L	1/2,3/2,5/2-		11622 3			0.0	1/2-
11646.0 19	L	1/2,3/2,5/2-		11645.2 19			0.0	1/2-
11660.4 14	L	1/2,3/2,5/2-		11659.6 14			0.0	1/2-
11669.3 18	L	1/2,3/2,5/2-		11668.5 18			0.0	1/2-
11691.4 18	L	1/2,3/2,5/2-		11690.6 18			0.0	1/2-
11739.8 12	L	1/2,3/2,5/2-		11739.0 12			0.0	1/2-
11770.0 12	L	1/2,3/2,5/2-		11769.2 12			0.0	1/2-
11802 2	L	1/2,3/2,5/2-		11801 2			0.0	1/2-
11817 3	L	1/2,3/2,5/2-		11816 3			0.0	1/2-
11832.1 15	L	1/2,3/2,5/2-		11831.3 15			0.0	1/2-
11843 2	L	1/2,3/2,5/2-		11842 2			0.0	1/2-
11854 2	L	1/2,3/2,5/2-		11853 2			0.0	1/2-
11873.5 19	L	1/2,3/2,5/2-		11872.7 19			0.0	1/2-
11913.2 14	L	1/2,3/2,5/2-		11912.3 14			0.0	1/2-
11946.9 18	L	1/2,3/2,5/2-		11946.0 18			0.0	1/2-
11962.3 14	L	1/2,3/2,5/2-		11961.4 14			0.0	1/2-
11984 2	L	1/2,3/2,5/2-		11983 2			0.0	1/2-
11991 2	L	1/2,3/2,5/2-		11990 2			0.0	1/2-
12E3 2	U	(1/2+,3/2+)
12076 15	H Y Z	5/2+	16 keV 2
12.79E3 12	f
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
13070 15	H Y Z c	(1/2+)	70 keV
13.8E3 2	M P		1.2 MeV 2
13991 15	H Z	5/2+	50 keV
14.0E3 2	M		4.5 MeV 4
14060 15	H Y Z a	3/2+	50 keV
14369 15	H	(1/2-)
14.42E3 16	f
14492 15	H Y Z c	3/2+	65 keV 7
14655 15	H	(3/2-)	30 keV
14.7E3 3	R T		4.4 MeV 4
14781 15	H Z	7/2+	20 keV
14833 15	H		25 keV
14912 15	H	(7/2-)	30 keV
15E3 2	W
15006 15	H c	(3/2+,5/2+)	25 keV
15176 15	H	3/2+	55 keV 21
15293 15	H	5/2+	45 keV 7
15323 15	H
15478 15	H		40 keV
15787 15	H	(7/2-)	55 keV
15837 15	H Y a c	(1/2+)	78 keV 15
16127 15	H	(1/2+)	80 keV 15
16247 15	H
16317 15	H
16.4E3	L		3.95 MeV
16527 15	H		50 keV 15
16607 15	H		50 keV 15
16647 15	H		50 keV 15
16717 15	H	(5/2-)	65 keV 15
16729 15	a c	(1/2+)
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
16767 15	H		50 keV 15
16790 40	L M a b d		3.9 MeV 2
16917 15	H	(7/2-)	40 keV 15
17E3 2	U	(3/2+,5/2+)
17127 15	H		50 keV 15
17427 15	H a c	(1/2+)	65 keV 15
17507 15	H
18.9E3	c
19.98E3 12	f
20.3E3?	c
21.5E3 2	L a		4.0 MeV 3
21.68E3 12	f
21.8E3 3	b c
27E3 1	f
28.0E3 5	M Z d j		8 MeV

E(level): From least-squares fit to Eγ data for levels populated in γ-ray studies. Others are generally from individual reactions

T_1/2(level): From ΔS(a) in (α,2nγ), unless otherwise stated. For IAR and giant resonances, values given are widths

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
908.97	9/2+	15.663 s 5 % IT = 100	908.960 25	M4+E5	0.00041 4	0.00851	B(E5)(W.u.)=0.147 15, B(M4)(W.u.)=3.995 2, α=0.00851
1507.41	3/2-	23.9 fs +25-21	1507.42 10	M1+E2	-0.13 2		B(E2)(W.u.)=2.1 2, B(M1)(W.u.)=0.26 3
1744.74	5/2-	0.64 ps 6	1744.7 2	E2			B(E2)(W.u.)=2.3 2
2222.43	5/2+	0.97 ps 28	715.2 3	[E1]			B(E1)(W.u.)=0.00030 9
2222.43	5/2+	0.97 ps 28	1313.2 3	[E2]			B(E2)(W.u.)=4.3 13
2566.55	11/2+	0.35 ps 7	1657.5 2	M1+E2	-15 8		B(E2)(W.u.)=5.5 11, B(M1)(W.u.)=6.E-5 5
2622.1	9/2+	0.21 ps 10	1713.1 3	(M1+E2)			B(E2)(W.u.)=(3.9), B(M1)(W.u.)=(0.010)
2892.98	13/2+	0.18 ps 3	1984.1 2	E2			B(E2)(W.u.)=4.3 8
3067.76	3/2-	45.0 fs +15-11	3067.7 1	(M1+E2)	+0.05		B(E2)(W.u.)=(0.89), B(M1)(W.u.)=(0.0077)
3107.26	(5/2)-	0.034 ps 3	1361.8 9	(M1+E2)	+0.6		B(E2)(W.u.)=(6.8), B(M1)(W.u.)=(0.0116)
	(5/2)-	0.034 ps 3	1599.8 4	(M1+E2)	-0.25		B(E2)(W.u.)=(2.8), B(M1)(W.u.)=(0.0067)
	(5/2)-	0.034 ps 3	3107.3 3	[E2]			B(E2)(W.u.)=2.0 2
3138.9	(5/2)-	0.11 ps +7-3	916.1 5	[E1]			B(E1)(W.u.)=0.00038 25
3138.9	(5/2)-	0.11 ps +7-3	3139.1 5	[E2]			B(E2)(W.u.)=0.6 4
3247.6	(3/2,5/2)		1740.2 5	D+Q	-0.24
3343.44	13/2-	0.42 ps 14	450.5 1	E1			B(E1)(W.u.)=0.00052 18
3343.44	13/2-	0.42 ps 14	776.89 6	E1			B(E1)(W.u.)=0.0016 6
3451.3	(7/2+)		2542.3 6	D+Q	-0.03
3515.9	(3/2)-		3515.9 3	(M1+E2)	-0.65 +15-30
3557.4	(7/2-)		2648.3 6	D+Q	-0.08
3621.1	(11/2)		2712.1 6	D+Q	+0.10
3630.3	(11/2)+		2721.3 6	(M1+E2)	+0.19
3715.3	5/2+		1492.7 4	(M1+E2)	-0.15
3747.7	(9/2)+		2838.7 8	(M1+E2)	+0.40
3848.3	(3/2-,5/2-)		2103.5 5	(M1+E2)	+1.8
3848.3	(3/2-,5/2-)		2340.8 6	(M1+E2)	-0.50
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
3992.2	3/2-	9.3 fs +11-10	3992.1 1	(M1+E2)	-0.90		B(E2)(W.u.)=(1.27), B(M1)(W.u.)=(0.0186)
4022.96	(3/2)-		955.0 3	(M1+E2)	-0.10
	(3/2)-		1800.8 4	(M1+E2)	-1.25
	(3/2)-		2515.3 6	(M1+E2)	-0.80
4104.9	(7/2+)		1882.5 8	(M1+E2)	+0.28
4104.9	(7/2+)		3196.3 12	(M1+E2)	-0.15
4132.22	15/2-	1.59 ps 28	788.6 1	M1+E2	+0.08 4		B(E2)(W.u.)=0.10 9, B(M1)(W.u.)=0.0092 18
4132.22	15/2-	1.59 ps 28	1239.28 7	E1			B(E1)(W.u.)=7.5E-5 14
4449.75	17/2-	4.5 ps 10	317.5 1	M1		0.00867	B(M1)(W.u.)=0.051 12, α=0.00867
4449.75	17/2-	4.5 ps 10	1106.5 1	E2			B(E2)(W.u.)=2.1 5
4825.38	17/2+	≥ 3.5 ps	693.2 2	E1			B(E1)(W.u.)<0.00023
4825.38	17/2+	≥ 3.5 ps	1931.9 3	(E2)			B(E2)(W.u.)<0.029
4838.59	19/2-	21 ps 8	388.9 1	M1+E2	+0.20 5	0.00540	B(E2)(W.u.)=3.3 21, B(M1)(W.u.)=0.011 5, α=0.00540 11
4838.59	19/2-	21 ps 8	706.3 1	E2			B(E2)(W.u.)=2.2 10
4920.46	(19/2+)	6.2 ps 21	95.07 3	(M1+E2)	-0.05 3	0.212	B(M1)(W.u.)>1.1 4, α=0.212
4920.46	(19/2+)	6.2 ps 21	470.72 5	E1			B(E1)(W.u.)>0.00036 13
5263.88	(21/2+)	1.46 ps 28	343.37 12	M1		0.00714	B(M1)(W.u.)=0.36 7, α=0.00714
5263.88	(21/2+)	1.46 ps 28	425.6 3	[E1]			B(E1)(W.u.)=4.6E-5 12
5309.83	(21/2-)	4.5 ps 9	471.1 2	(M1)			B(M1)(W.u.)=0.044 11
5309.83	(21/2-)	4.5 ps 9	860.1 1	(E2)			B(E2)(W.u.)=0.57 15
5879.4	(19/2+)	0.14 ps 10	615.5 3	(M1)			B(M1)(W.u.)=0.7 5
6198.90	(23/2+)	0.19 ps 4	935.01 5	M1+E2	-0.12 4		B(E2)(W.u.)=2.5 18, B(M1)(W.u.)=0.14 3
7183.7	(25/2+)	0.21 ps 7	1920.2 3	[E2]			B(E2)(W.u.)=4.4 18
7431.6	(25/2+)	0.49 ps 14	172.1 1	(M1)		0.0417	B(M1)(W.u.)=3.0 10, α=0.0417
7431.6	(25/2+)	0.49 ps 14	1232.6 2	(M1)			B(M1)(W.u.)=0.024 8
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
7590.0	(25/2+)	0.35 ps 14	396.1 2	(M1)			B(M1)(W.u.)=1.0 4
7834.6	(27/2+)	1.25 ps 28	244.6 1	(M1)		0.0167	B(M1)(W.u.)=0.70 19, α=0.0167
7834.6	(27/2+)	1.25 ps 28	650.9 1	(M1)			B(M1)(W.u.)=0.064 17
8264.2	(29/2+)	0.97 ps 21	429.6 1	M1+E2	-0.07 4		B(E2)(W.u.)=8 7, B(M1)(W.u.)=0.27 9
8264.2	(29/2+)	0.97 ps 21	832.9	[E2]			B(E2)(W.u.)<8
8720.4	(31/2+)	0.48 ps 14	456.2 2	(M1)			B(M1)(W.u.)=0.43 17
8720.4	(31/2+)	0.48 ps 14	885.9	[E2]			B(E2)(W.u.)<19

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2-	STABLE	μ=-0.1374154 3 (1977Ha12,1989Ra17,2011StZZ) Configuration=πp_1/2.
908.97	9/2+	15.663 s 5 % IT = 100	μ=+6.37 4 (2007Ch07,2011StZZ), Q=-0.43 6 (2007Ch07,2011StZZ) BE5\|^=0.00056 5 (e,e’); β₅=0.055 (p,p’).
1507.41	3/2-	23.9 fs +25-21	B(E2)\|^=0.0097 11 (e,e’); β₂=0.079 13 (n,n’); 0.060 (p,p’).
1744.74	5/2-	0.64 ps 6	B(E2)\|^=0.0164 15 (e,e’). β₂=0.079 10 (n,n’); 0.072 (p,p’).
2222.43	5/2+	0.97 ps 28	B(E3)\|^=0.0258 23 (e,e’). β₃=0.160 17 (n,n’); 0.156 (p,p’).
2529.80	7/2+	0.08 ps 4	B(E3)\|^=0.037 3 (e,e’). β₃=0.14 3 (n,n’); 0.146 (p,p’).
2566.55	11/2+	0.35 ps 7	β₅=0.027 (p,p’).
2622.1	9/2+	0.21 ps 10	β₅=0.047 (p,p’).
2871.7	(7/2)+	< 0.2 ps	β₃=0.079 13 (n,n’); 0.111 (p,p’).
2881.53	(3/2)-	19.9 fs +21-19	β₂=0.087 16 (n,n’); 0.066 (p,p’).
3107.26	(5/2)-	0.034 ps 3	β₂=0.065 8 (n,n’); 0.046 (p,p’).
3621.1	(11/2)		XREF: γ(3612).
3715.3	5/2+		XREF: R(3740)S(3680).
4171.3	3/2-,5/2-	10.1 fs +15-11	XREF: S(4180).
4251			XREF: L(?).
4309.3	(7/2)-		XREF: l(4310).
4408.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
4529.3	5/2+,7/2+		XREF: X(4550).
4616.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
4625.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
4831	3/2+,5/2+		XREF: J(4840).
4992	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5006	(5/2)-		XREF: W(5000).
5075	(1/2+)		XREF: I(5100)J(5080).
5085.4	1/2,3/2,5/2-		XREF: p(5089). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
5152.1	1/2,3/2,5/2-		XREF: p(5148). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5167.7	1/2,3/2,5/2-		XREF: p(5170). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5183	3/2+,5/2+		XREF: J(5190).
5211	(3/2-)		XREF: X(5220).
5275	(1/2+)		XREF: J(5270).
5343	(1/2+)		XREF: J(5340).
5382	(1/2)		XREF: X(5380).
5419.4	1/2,3/2,5/2-		XREF: p(5421). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5614.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5625.8	1/2,3/2,5/2-		XREF: p(5622). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5653.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5789.4	1/2,3/2,5/2-		XREF: p(5793). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5796.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5888	3/2+,5/2+		XREF: K(5870).
5910.7	1/2,3/2,5/2-		XREF: p(5915). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
5923.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6.01E3			E(level): Hypernuclear state.
6122.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6201.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6206.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6275.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6297.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6331.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6359.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6398.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
6441.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6472.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6479	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6493.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6.5E3	(7/2-)		E(level): Wide structure due to deep hole states.
6532.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6592.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6608.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6651.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6666.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6728	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6750		1.0 MeV 2	E(level): Giant resonance.
6751.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6772.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6780	7/2-		XREF: W(6800).
6782.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6798.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6852.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6866	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6921	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6934.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6944.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6959.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
6987.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7003.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
7066.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7077.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7.1E3			E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
7106	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7118.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7147.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7178.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7198	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7225.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7240	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7255	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7.3E3			E(level): Wide structure due to deep hole states.
7304.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7325.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7.38E3			E(level): Hypernuclear state.
7383.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7420.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7452.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7475.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7484.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7527.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7536	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7548	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7556	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7566	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
7588.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7618.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7640.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7652.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7666.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7692.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7703.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7714.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7722.2	(1/2+)		XREF: J(7720)K(7710). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7750.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7774.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7787.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7799.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7811.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7830.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7838.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7866.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7902.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7920.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7922.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7937.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7961.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7968.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7986.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
7996.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
8018	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8027.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8050		1.2 MeV 2	E(level): Giant resonance.
8067.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8099.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8129.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8142.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8150.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8159.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8175.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8198.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8210.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8221.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8270.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8285.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8311.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8320.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8330.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8338.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8369	1/2,3/2,5/2-		XREF: J(?). J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8380.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8403.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8438.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8455	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8466.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
8483.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8495.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8513.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8530.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8548.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8556.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8568.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8586.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8603	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8610.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8642.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8668.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8764.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8779.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8843.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8864	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8877.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8899.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8926.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8981	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
8994.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9002.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9024.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9043.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9057.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
9069.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9082	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9093.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9112.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9121.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9147.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9161.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9175.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9191.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9204.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9240.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9256.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9280.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9290.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9301.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9308.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9320	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9326.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9351.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9374.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9401.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9410.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9449.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9471	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9482.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
9503	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9532	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9541	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9575.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9593.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9623.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9660.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9679.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9901.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9912.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9964.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9973.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
9990.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10005.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10017.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10037.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10049	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10065	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10073.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10091.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10108.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10141.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10173.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10194.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10276.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
10286.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10307.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10324.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10340.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10379.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10395.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10412.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10424.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10460.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10469	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10504	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10513.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10538.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10641.6	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10659.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10668.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10697.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10736.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10744.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10753	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
10967.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11058.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11069	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11081.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11106.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
11192.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11200	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11419.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11463.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11474	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11498	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11517	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11535.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11560.7	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11571.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11601.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11611	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11623	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11646.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11660.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11669.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11691.4	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11739.8	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11770.0	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11802	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11817	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11832.1	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11843	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11854	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11873.5	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)	J^π(level)	T_1/2(level)	Comments
11913.2	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11946.9	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11962.3	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11984	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
11991	1/2,3/2,5/2-		J^π(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
12E3	(1/2+,3/2+)		E(level): Wide structure due to deep hole states.
12076	5/2+	16 keV 2	Γ_γ0=7 2, Γ_p=5.5 5 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
12.79E3			E(level): Hypernuclear state.
13070	(1/2+)	70 keV	Γ_γ0=16 3, Γ_p=46 KEV E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
13.8E3		1.2 MeV 2	E(level): Giant resonance.
13991	5/2+	50 keV	Γ_p=8 4 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
14.0E3		4.5 MeV 4	E(level): Giant resonance.
14060	3/2+	50 keV	Γ_γ0=7 3, Γ_p=26 4 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
14369	(1/2-)		E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
14.42E3			E(level): Hypernuclear state.
14492	3/2+	65 keV 7	Γ_γ0=11.3 19, Γ_p=20 3 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
14655	(3/2-)	30 keV	E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
14.7E3		4.4 MeV 4	E(level): Giant resonance.
14781	7/2+	20 keV	Γ_p=4 KEV E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
14912	(7/2-)	30 keV	E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
15E3			E(level): Wide structure due to deep hole states.
15006	(3/2+,5/2+)	25 keV	E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
15176	3/2+	55 keV 21	Γ_p=6.3 10 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
15293	5/2+	45 keV 7	Γ_p=4 3 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
15837	(1/2+)	78 keV 15	Γ_γ0=40 8 E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
E(level)	J^π(level)	T_1/2(level)	Comments
16127	(1/2+)	80 keV 15	E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
16.4E3		3.95 MeV	E(level): Giant resonance.
16729	(1/2+)		E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
16790		3.9 MeV 2	E(level): Giant resonance.
17E3	(3/2+,5/2+)		E(level): Wide structure due to deep hole states.
17427	(1/2+)	65 keV 15	E(level): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p).
19.98E3			E(level): Hypernuclear state.
21.5E3		4.0 MeV 3	E(level): Giant resonance.
21.68E3			E(level): Hypernuclear state.
21.8E3			XREF: c(?).
27E3			E(level): Hypernuclear state.
28.0E3		8 MeV	XREF: d(27000). E(level): Giant resonance.

E(level)	E(gamma)	Comments
908.97	908.960	M(γ): α(exp) in ⁸⁹Y IT decay. E5 admixture is suggested by L=5 in (e,e’), (p,p’), (n,n’) and (α,α’) from 1/2-
1744.74	1744.7	M(γ): ΔJ=2 γ to 1/2- and RUL
2222.43	715.2	I(γ): from (n,n’γ). Iγ=22 4 in (α,2nγ), 43 in (p,p’γ)
2622.1	1713.1	M(γ): ce data in ⁸⁹Zr ε decay
4449.75	317.5	E(γ): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p) M(γ): From (¹⁸O,2npγ), (¹⁸O,4npγ)
4920.46	470.72	E(γ): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p) M(γ): From (¹⁸O,2npγ), (¹⁸O,4npγ)
5263.88	343.37	E(γ): IAR of ⁸⁹Sr, confirmed by comparison of Γ_p with S-factors in ⁸⁸Sr(d,p) M(γ): From (¹⁸O,2npγ), (¹⁸O,4npγ)