List of levels for 91ZR

ADOPTED LEVELS, GAMMAS for ⁹¹Zr

Author: Coral M. Baglin | Citation: Nucl. Data Sheets 114, 1293 (2013) | Cutoff date: 1-Sep-2013

Full ENSDF file | Adopted Levels (PDF version)

Q(β-)=-1258 keV 3	S(n)= 7193.9 keV 4	S(p)= 8690.3 keV 17	Q(α)= -5441.0 keV 20
Reference: 2012WA38

References:
A	⁸⁸Sr(α,nγ)	B	⁸⁸Sr(⁶Li,2npγ)
C	⁹⁰Zr(n,γ) E=THERMAL	D	⁹¹Zr(γ,γ’)
E	⁹¹Zr(n,n’γ)	F	⁹⁰Zr(α,³He)
G	⁹⁰Zr(d,p)	H	⁹⁰Zr(pol d,p)
I	⁹¹Zr(α,α’)	J	⁹¹Zr(d,d’)
K	⁹¹Zr(p,p’)	L	⁹²Zr(d,t)
M	⁹²Zr(p,d)	N	⁹³Nb(d,α)
O	Coulomb Excitation	P	⁹¹Zr(n,n’)
Q	⁹⁰Zr(¹²C,¹¹C)	R	⁹⁰Zr(¹³C,¹²C)
S	⁹⁰Zr(¹³C,¹²CG)	T	⁹⁰Zr(¹⁶O,¹⁵O)
U	⁹⁰Zr(⁷Li,⁶Li)	V	⁹¹Nb ε decay (6.8×10² Y)
W	⁹¹Nb ε decay (60.86 d)	X	⁹¹Y β^- decay
Y	⁹¹Zr(¹⁸O,¹⁸O’)	Z	⁹¹Zr(³He,³He’), (pol ³He,³He)
a	⁹²Zr(pol p,d)	b	⁹²Zr(³He,α)
c	⁹³Nb(μ^-,2nγ)	d	⁸⁸Sr(¹²C,⁹Be)
e	⁹⁰Zr(²⁰Ne,¹⁹Ne)	f	⁸²Se(¹³C,4nγ)
g	⁹⁰Zr(n,γ) E=RES	h	⁹¹Zr IT decay

Other Reactions:

²H(⁹⁰Zr,pγ), E=360 MeV: 2007Ci05. Proposed measurement of γ-rays in coincidence with (d,p) reaction protons in inverse kinematics to serve as surrogate for (n,γ) reaction (feasibility study).

⁹¹Zr(α,³Heγ), E=51 MeV: 2005Ch53. Observed 90γ from 2260 level.

⁹²Mo(n,2pγ), E(n)|<800 MeV: 2000Ga46. 99% ⁹²Mo target, pulsed beam; 15 coaxial HPGe detectors (for Eγ|<4 MeV) and 11 planar Ge detectors (for Eγ|<1 MeV), BGO suppression shields for all planar and 9 coaxial detectors; measured 2131γ and 2170γ excitation functions for E(n)=10-250 MeV.

⁹³Nb(pol p,³He), E=100.0 MeV 5: 2000Co29. Beam polarization ≈80%, 2 Si detector telescopes, particle identification, θ(lab)=15|’-140|’; measured double differential cross section and analyzing power for E(³He)=38-90 MeV (6 energies); investigated reaction mechanism; multistep direct reaction theory.

Other measurements:

n-resonances: 2008Ta04, 2006MuZX, 2000Le01. Note that neutron resonance data have not been included in Adopted Levels; please see the ⁹¹Zr(n,γ) E=res dataset for these.

Charge distribution from (e,e): 1971Fa16.

Isotopic shift and mean square charge radius: 1988Ga26, 1988GaZS, 1999GaZX.

Hfs: 1993Yo11, 1999Be77, 2000Bo31, 2003Th03.

Theory (list not complete):

Nuclear structure: 2000Ho15, 1979Ch18, 1975Gl07, 1975Ip01, 1971Pa18, 1966Ve02, 1965Au04 (shell-model calculations).

Magnetic moment: 1998Jo17 (core polarization and meson exchange current), 1981Na12, 1973Va10 (core polarization), 1983Na10 (meson exchange contributions).

1989Fu05 (relativistic self-consistent calculation of baryon-meson dynamics)

n-resonances: 1987St13.

Level density: 1974So04.

|L hyperon binding energy (2013Lo03).

Gammas: E(f) From ⁸²Se(¹³C,4nγ)

E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
0.0	A B C D E F G H I J K L M N O P Q R S T U V W X Y Z a b c d e f g h	5/2+	STABLE
1204.81 13	A C D E G H I J K L M N O P R S U W X Y a c	1/2+	0.62 ps 14	1204.80 13	100	E2	0.0	5/2+
1466.4 4	A C D E G H I J K L M N P S a c	5/2+	0.32 ps 3	1466.3 4	100	[M1,E2]	0.0	5/2+
1882.20 17	A C D E F G H I J K L M P a	7/2+	76 fs 11	1882.18 19	100	(M1+E2)	0.0	5/2+
2042.35 19	A C D E F G H I J K L M N P S U a	3/2+	11.1 fs 11	2042.33 19	100	(M1(+E2))	0.0	5/2+
2131.49 15	A B D E G J K L M N P f h	(9/2)+	127 fs 17	2131.54 18	100	(E2)	0.0	5/2+
2170.15 15	A B E F G H I J K M P Q S T Z f	(11/2)-	> 5.5 ps	38.7 2 2170.04 18	2.5 14 100 10	[E1] (E3)	2131.49 0.0	(9/2)+ 5/2+
2189.5 6	A D E F K N U	(5/2)-	≤ 1.8 ps	2189.0 7	100	[E1]	0.0	5/2+
2200.5 3	A D E F G H J K L M N Q U	7/2+	0.33 ps +9-6	2200.5 3	100	(M1+E2)	0.0	5/2+
2259.92 21	A B G J K N f	(13/2)-		89.55 19	100		2170.15	(11/2)-
2287.8 3	A B J K N f h	(15/2)-	29.0 ns 8	28.0 2	100	(M1)	2259.92	(13/2)-
2320.5 3	A B E F G H J K M h	(11/2)-		60.33 20 151.1 4			2259.92 2170.15	(13/2)- (11/2)-
2356.4 7	A E G J K L M N	(1/2)-		1151.6 6	100		1204.81	1/2+
2366.56 19	A C D E G J K N		105 fs +18-14	2366.53 19	100		0.0	5/2+
2394.9 8	A J K	(9/2)-		224.8 7	100		2170.15	(11/2)-
2534.69 22	A E G J K	(3/2+,5/2+)	78 fs +19-15	652.49 20 1068.0 5 2534.8 4	77 20 48 9 100 18		1882.20 1466.4 0.0	7/2+ 5/2+ 5/2+
2557.8 5	A C D E G H J K S	1/2+	0.13 ps +6-4	2557.8 5	100	[E2]	0.0	5/2+
2577.9 5	A C D E G I J K M N	(3/2)-	84 fs 21	2577.9 5	100	[E1]	0.0	5/2+
2640.2 4	A C D E G J K M	(3/2)-	92 fs +32-21	2640.1 4	100	[E1]	0.0	5/2+
2693.7 4	A C D E F G H J K M N T	(3/2)-	25 fs 4	2693.7 4	100	(E1(+M2))	0.0	5/2+
2764.6 5	A B E J K L N	(13/2,15/2)-		443.8 5 477.2 6	29 100		2320.5 2287.8	(11/2)- (15/2)-
2775.2 5	A C D E G J K L N Z	(5/2)-	0.13 ps +5-3	732.4 5 ? 2775.2 5	86 25 100 25	[E1]	2042.35 0.0	3/2+ 5/2+
2791.46 25	A E	(GE5/2)		659.97 20	100		2131.49	(9/2)+
2810.9 7	A D E F H M	(7/2+)	24 fs +5-4	415.9 7 ? 770.5 10 2810.9 7	36 19 7 100 21	[E1] [E2] [M1]	2394.9 2042.35 0.0	(9/2)- 3/2+ 5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2813 3	J K M	-
2826.0 16	A G L N	3/2+,5/2+		2826.0 16	100		0.0	5/2+
2835.7 5	E F G I J K N	(3/2,5/2,7/2)-		1369.2 3 ?	100		1466.4	5/2+
2857.06 25	B J K f h	(13/2)+	≤ 7 ns	537 1 570 1 596.9 3 725.7 3	27 3 20.3 20 61 6 100 9	E2	2320.5 2287.8 2259.92 2131.49	(11/2)- (15/2)- (13/2)- (9/2)+
2871.5 7	C E F G H J K	3/2+		2871.0 8	100		0.0	5/2+
2902.3 7	E G K L M N b	(7/2)+		712.6 5 2903.1 10	100 30 80 30		2189.5 0.0	(5/2)- 5/2+
2914.2 5	A E J K N b	(9/2+)		782.7 4	100		2131.49	(9/2)+
2928.4 10	E G H J K M	3/2+,5/2+	61 fs +15-11	2928.3 10	100		0.0	5/2+
2992.1 7	E L			791.6 6	100		2200.5	7/2+
3007.7 8	A E G J K L	5/2-,7/2-	94 fs +43-26	3007.6 8	100	[E1]	0.0	5/2+
3017.1 20	A J			3017.0 20	100		0.0	5/2+
3034 3	G I J K L N	-
3053 5	F G K L N
3083.3 6	A C E F G H J K	3/2+	17 fs +6-4	3083.3 7	100		0.0	5/2+
3107.9 8	D E G J K L M	7/2+,9/2+	38 fs +8-6	3107.8 8	100		0.0	5/2+
3146.9 3	B K f h	(17/2)+	≤ 7 ns	289.8 3 859.0 3	13.3 13 100 10	E2	2857.06 2287.8	(13/2)+ (15/2)-
3167.3 4	B K N f h	(21/2+)	4.35 µs 14 % IT = 100 % IT = 100	20.4 2 S 879.4 3	7.0 7 100 11	[E2] [E3]	3146.9 2287.8	(17/2)+ (15/2)-
3234.8 10	C D E G I J K L M	(3/2)-	27 fs +6-5	3234.7 10	100	[E1]	0.0	5/2+
3262 8	K
3276.6 6	E F K M	(3/2-)		1810.1 4 ?	100		1466.4	5/2+
3290.4 5	C E F G H J K M N	3/2+		1248.0 4 ?	100		2042.35	3/2+
3312 4	D J K N	(+)
3321 4	D J K
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3331.1 15	E G K L	1/2+		3331.0 15	100		0.0	5/2+
3356 8	K
3378 6	K M	(1/2-,3/2-)
3410 8	K
3456 5	G K	9/2-,11/2-
3469 5	F G H I J K N Q T	7/2+
3476.1 10	C D I K L M N	1/2-,3/2-		3476 1 ?	100		0.0	5/2+
3476.3 8	C D G I J K N	3/2+,5/2+		3476 1 ?	100		0.0	5/2+
3489 4	J K N
3555 6	F G H K	(7/2)+
3576.1 10	D F K L M	(3/2)-	7.6 fs 13	3576 1	100	[E1]	0.0	5/2+
3597 6	K M N	5/2-,7/2-
3636 6	F G K	3/2+,5/2+
3652 4	J K N	(-)
3667 7	F G K N
3681 3	D F G H J K M	3/2+	6.6 fs 26	3681 3	100		0.0	5/2+
3704 3	D J K L M	7/2+,9/2+		3704 3	100		0.0	5/2+
3725 8	K L	1/2-,3/2-
3750 4	G J K M N	3/2+,5/2+
3776 4	G J K N	(+)
3820 4	F G J K L M	(7/2+,9/2+)
3829 8	K N
3850 4	G H J K N	(5/2)+
3884 6	K M	(1/2-,3/2-)
3898 4	F G J K L M	7/2+,9/2+
3908 4	G H J K N	9/2-,11/2-
3924 6	F G K N	3/2+,5/2+
3949 5	J K
3962 4	J K L M	7/2+,9/2+
3984.2 8	C G J K M N	3/2+,5/2+		3984.5	100		0.0	5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4007 4	F G H J K	7/2+,9/2+
4025.6 11	C K L M	(3/2+,5/2+)
4040 4	G J K	(3/2+,5/2+)
4070 4	F G J K M T	9/2-,11/2-
4114 4	F G J K N T	7/2+,9/2+
4148 2	G J K N	(3/2+,5/2+)
4162.4 8	C G J K	3/2+,5/2+		4162.6	100		0.0	5/2+
4180.0 6	C J	1/2(+),3/2,5/2+		2713.6 4180.2	100 15		1466.4 0.0	5/2+ 5/2+
4192 4	G J K	(3/2+,5/2,7/2-)
4210 10	M	1/2-,3/2-
4230 8	K
4245 8	F K
4268 4	F G J K	(1/2-,3/2-)
4279 5	G J K N	7/2+,9/2+
4296 4	I J K M N	1/2-,3/2-
4319.8 8	C D G I K M	3/2-	4.1 fs 18	4319.8	100	[E1]	0.0	5/2+
4338 5	J K
4354 6	G K	3/2+,5/2+
4380 6	G K N	7/2+,9/2+
4400 4	G J K M	(3/2+,5/2+)
4414 5	G J T	9/2-,11/2-
4437 5	J K N
4450 8	K N
4464 4	G J K	3/2+,5/2+
4504 5	G J M	1/2-,3/2-
4532.7 11	C G J N	3/2+,5/2+
4549 7	J N
4588 5	G J	(3/2+,5/2,7/2-)
4611 8	G
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4653 5	G J	(1/2,3/2-)
4685 5	D G J	(1/2+,3/2-)		4685 5			0.0	5/2+
4704?	D			4704.1 10 ?	100		0.0	5/2+
4712.1 8	D G J f			1545	100		3167.3	(21/2+)
4735 8	G M N	(1/2,3/2)-
4786 5	G J	(-)
4808 8	G	(3/2+,5/2+)
4833 10	G M	1/2-,3/2-
4876 10	G
4928 10	G
4953 10	G	(5/2-,7/2-)
4989 10	G
5017 10	G
5095 10	G	(1/2-,3/2-)
5132 10	G N
5158 10	G
5176 10	G
5217 10	G	(3/2+,5/2+)
5254 10	G
5308.2 8	f			596 2141			4712.1 3167.3	(21/2+)
5312 10	G N	(3/2+,5/2+)
5357 10	G
5382 10	G
5426 10	G N
5450 10	G
5472 10	G
5495.6 9	f			2328	100		3167.3	(21/2+)
5496 10	G
5530 10	G
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5550 10	G
5598 10	G I N	(-)
5613.1 8	f			305 901			5308.2 4712.1
5645 10	G
5674 10	G N
5716 10	G
5741.3 8	f			128 2574			5613.1 3167.3	(21/2+)
5744 10	G
5781 10	G
5804 10	G
5843 10	G
5877 10	G
5894 10	G
5933 10	G
5954 10	G
6003 10	G
6027 10	G
6081 10	G
6103 10	G
6156 10	G
6179 10	G
6210 10	G
6262 10	G
6297 10	G
6352 10	G
6390 10	G
6431 10	G
6457 10	G
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6773.2 9	f			1032 1160			5741.3 5613.1
7014.3 9	f			241 1273 1401			6773.2 5741.3 5613.1
7194.4 5	C	1/2+		2662.12? 2875.00 3015.12 3032.53 3169.20? 3210.85 3718.15 3906.30? 3960.14? 4111.5 4322.4 4553.9 4617.0 4636.8 4828.5? 5152.4 5989.8 7194.4	23 35 100 28 10 35 49 10 28 11 35 15 43 23 19 19 13 2.4	[E1] [E1] [E1] [E1] [E2]	4532.7 4319.8 4180.0 4162.4 4025.6 3984.2 3290.4 3234.8 3083.3 2871.5 2640.2 2577.9 2557.8 2366.56 2042.35 1204.81 0.0	3/2+,5/2+ 3/2- 1/2(+),3/2,5/2+ 3/2+,5/2+ (3/2+,5/2+) 3/2+,5/2+ 3/2+ (3/2)- 3/2+ 3/2+ (3/2)- (3/2)- 1/2+ 3/2+ 1/2+ 5/2+
7198.7188 4	g	1/2
7198.86427 6	g	3/2
7202.0805 2	g	3/2
7203.6578 4	g	1/2
7204.39652 7	g	1/2
7206.97387 2	g	1/2
7207.16354 7	g	1/2
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7207.20615 1	g	1/2
7208.118 3	g	1/2
7208.19616 1	g	1/2
7211.608 1	g	1/2
7211.64354 2	g	1/2
7211.6926 1	g	1/2
7212.11 2	g	1/2
7213.76964 1	g	1/2
7213.788 2	g	1/2
7213.8 9	f			1601 1718 2502			5613.1 5495.6 4712.1
7214.396 2	g	1/2
7221.078 3	g	3/2
7221.146 1	g	3/2
7223.410 3	g	3/2
7229.867 4	g	1/2
7233.973 3	g	3/2
7234.86 1	g	1/2
7235.84 1	g	3/2
7236.5076 1	g	3/2
7236.65 6	g	1/2
7236.888 6	g	1/2
7237.071 20	g	1/2
7239.229 8	g	3/2
7247.579 7	g	1/2
7247.685 8	g	1/2
7247.982 1	g	1/2
7248.656 1	g	1/2
7248.847 1	g	1/2
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7250.09 2	g	1/2
7250.80 1	g	1/2
7252.055 4	g	1/2
7252.570 8	g	1/2
7256.1198 2	g	3/2
7256.624 2	g	1/2
7258.1392 3	g	1/2
7259.14 6	g	1/2
7259.36 2	g	3/2
7259.544 2	g	1/2
7262.737 7	g	3/2
7264.96 8	g	1/2
7266.57 5	g	3/2
7267.42 5	g	1/2
7268.57 5	g	3/2
7269.59 5	g
7270.06 5	g
7273.70 5	g
7274.18 5	g
7274.46 8	g
7275.48 8	g
7276.16 5	g	3/2
7277.22 5	g	[1/2]
7279.69 5	g	1/2
7284.28 5	g	1/2
7286.77 5	g	3/2
7288.16 5	g	(1/2)
7288.68 5	g
7289.63 5	g	3/2
7291.17 95	g	3/2
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7292.99 5	g	3/2
7294.20 10	g	3/2
7298.45 10	g	1/2
7298.94 10	g	3/2
7302.01 20	g
7302.90 10	g	3/2
7303.89 10	g	3/2
7305.08 10	g	3/2
7307.75 10	g	1/2
7312.39 10	g	1/2
7315.06 10	g	(3/2)
7315.76 10	g	[3/2]
7316.15 10	g
7317.74 10	g	1/2
7320.21 10	g
7320.70 10	g	3/2
7323.08 10	g	1/2
7323.77 10	g
7324.36 10	g
7325.05 10	g	3/2
7327.13 10	g
7327.53 10	g	3/2
7332.47 10	g	3/2
7337.61 10	g	1/2
7338.70 10	g
7341.57 10	g
7343.55 10	g	1/2
7344.44 10	g	1/2
7348.8 5	g	1/2
7349.8 5	g	3/2
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7352.85 10	g	1/2
7353.14 10	g
7354.23 10	g	[3/2]
7356.41 10	g	1/2
7357.39 10	g	1/2
7359.37 10	g	3/2
7361.85 10	g	1/2
7365.41 10	g	3/2
7367.5 11	f			1626	100		5741.3
7369.06 10	g	1/2
7370.55 10	g	3/2
7372.72 10	g	[1/2]
7374.41 10	g	3/2
7377.17 10	g	3/2
7378.86 10	g	1/2
7381.23 20	g
7381.92 20	g
7382.71 10	g	1/2
7385.58 10	g	1/2
7386.17 10	g	1/2
7391.12 10	g	1/2
7392.70 10	g
7394.48 10	g
7396.66 10	g
7399.43 10	g
7400.42 10	g
7400.71 10	g	1/2
7403.68 20	g	3/2
7407.54 20	g	3/2
7411.7 3	g	1/2
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
7412.8 3	g	3/2
7415.3 3	g	1/2
7416.0 3	g	[3/2]
7419.70 20	g	3/2
7423.56 20	g	1/2
7430.4 5	g	3/2
7432.3 5	g	1/2
7436.61 20	g
7438.89 20	g
7440.67 20	g	1/2
7445.91 20	g	3/2
7448.09 20	g	1/2
7456.00 20	g	1/2
7456.89 20	g	1/2
7464.2 3	g	3/2
7464.6 3	g	1/2
7472.5 3	g	[3/2]
7475.9 3	g
7478.8 3	g	3/2
7481.1 3	g	3/2
7482.6 3	g
7485.4 3	g	3/2
7492.5 3	g	1/2
7645.3 10	f			872 1904			6773.2 5741.3
7665.5 10	f			452 1924			7213.8 5741.3
8359.3 11	f			694	100		7665.5
8471.3 11	f			1104 1457			7367.5 7014.3
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8627.8 12	f			1260	100		7367.5
8889.2 11	f			261 418 530 1244			8627.8 8471.3 8359.3 7645.3
9132.3 12	f			773 1487			8359.3 7645.3
9188.3 14	f			829	100		8359.3
9465.2 15	f			576	100		8889.2
9596.2 15	f			707	100		8889.2
10068.3 14	f			880 936			9188.3 9132.3
10442.3 14	f			374	100		10068.3
10531.2 18	f			935	100		9596.2
10659.2 18	f			1194	100		9465.2
11063.2 21	f			404	100		10659.2
11165.3 20	f			723	100		10442.3
11639.3 22 ?	f			474?	100		11165.3
12136.4 22 ?	f			971?	100		11165.3
12773.4 23	f			1710	100		11063.2
14.40E3 15	U

E(level): Level energies with ΔE|<3 keV are calculated from the Adopted Gammas by means of a least-squares fit. The others are weighted averages from reaction data (see XREF column).

J^π(level): Target spins for (d,p), (p,d), and (d,t) reactions are 0⁺.

E(γ): From (n,n’γ), except as noted.

I(γ): γ branching ratios for each level; from (n,n’γ), except as noted.

M(γ): From γ(θ) observed in (n,n’γ), if not indicated otherwise.

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
1204.81	1/2+	0.62 ps 14	1204.80 13	E2			B(E2)(W.u.)=15 4
1882.20	7/2+	76 fs 11	1882.18 19	(M1+E2)	+1.25 15		B(E2)(W.u.)=7.7 13, B(M1)(W.u.)=0.017 4
2131.49	(9/2)+	127 fs 17	2131.54 18	(E2)			B(E2)(W.u.)=4.2 6
2170.15	(11/2)-	> 5.5 ps	38.7 2	[E1]		1.75	B(E1)(W.u.)<0.025, α=1.75 4
2189.5	(5/2)-	≤ 1.8 ps	2189.0 7	[E1]			B(E1)(W.u.)>1.8E-5
2287.8	(15/2)-	29.0 ns 8	28.0 2	(M1)		7.92	B(M1)(W.u.)=0.00388 17, α=7.92 21
2557.8	1/2+	0.13 ps +6-4	2557.8 5	[E2]			B(E2)(W.u.)=1.6 +5-8
2577.9	(3/2)-	84 fs 21	2577.9 5	[E1]			B(E1)(W.u.)=0.00023 6
2640.2	(3/2)-	92 fs +32-21	2640.1 4	[E1]			B(E1)(W.u.)=0.00023 12
2693.7	(3/2)-	25 fs 4	2693.7 4	(E1(+M2))	-0.3 +3-7		B(E1)(W.u.)=0.00068 11
2775.2	(5/2)-	0.13 ps +5-3	2775.2 5	[E1]			B(E1)(W.u.)=6.E-5 +3-4
2810.9	(7/2+)	24 fs +5-4	415.9 7	[E1]			B(E1)(W.u.)=0.045 +10-12
	(7/2+)	24 fs +5-4	770.5 10	[E2]			B(E2)(W.u.)=440 +190-200
	(7/2+)	24 fs +5-4	2810.9 7	[M1]			B(M1)(W.u.)=0.027 +8-9
2857.06	(13/2)+	≤ 7 ns	725.7 3	E2			B(E2)(W.u.)>0.0079
3007.7	5/2-,7/2-	94 fs +43-26	3007.6 8	[E1]			B(E1)(W.u.)=0.00013 +4-6
3146.9	(17/2)+	≤ 7 ns	289.8 3	E2		0.0244	B(E2)(W.u.)>0.19, α=0.0244
3167.3	(21/2+)	4.35 µs 14 % IT = 100 % IT = 100	20.4 2	[E2]		341	B(E2)(W.u.)=4.3 7, α=341 14
3167.3	(21/2+)	4.35 µs 14 % IT = 100 % IT = 100	879.4 3	[E3]		0.00202	B(E3)(W.u.)=0.056 9, α=0.00202
3234.8	(3/2)-	27 fs +6-5	3234.7 10	[E1]			B(E1)(W.u.)=0.00037 +7-9
3576.1	(3/2)-	7.6 fs 13	3576 1	[E1]			B(E1)(W.u.)=0.00096 17
4319.8	3/2-	4.1 fs 18	4319.8	[E1]			B(E1)(W.u.)=0.0010 5

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	5/2+	STABLE	Q=-0.176 3, μ=-1.30362 2 Δ<r²>(90,91)=0.096 11 (1988GaZS), 0.137 16 (1999GaZX); from LASER resonance fluorescence. E(level): Δ<r²>(90,91)=0.096 11 (1988GaZS), 0.137 16 (1999GaZX); from LASER resonance fluorescence.
1204.81	1/2+	0.62 ps 14	β₂=0.21 3 from (n,n’), 0.16 from (α,α’). E(level): β₂=0.21 3 from (n,n’), 0.16 from (α,α’).
1466.4	5/2+	0.32 ps 3	β₂=0.076 16 from (n,n’), 0.05 from (α,α’). E(level): β₂=0.076 16 from (n,n’), 0.05 from (α,α’).
1882.20	7/2+	76 fs 11	β₂=0.103 12 from (n,n’), 0.08 from (α,α’). E(level): β₂=0.103 12 from (n,n’), 0.08 from (α,α’).
2042.35	3/2+	11.1 fs 11	β₂=0.082 11 from (n,n’). E(level): β₂=0.082 11 from (n,n’).
2131.49	(9/2)+	127 fs 17	β₂=0.052 7 from (n,n’). E(level): β₂=0.052 7 from (n,n’).
2170.15	(11/2)-	> 5.5 ps	β₃=0.180 15 from (n,n’). Other: (α,α’). E(level): β₃=0.180 15 from (n,n’). Other: (α,α’).
2200.5	7/2+	0.33 ps +9-6	XREF: F(2203)L(2186).
2320.5	(11/2)-		XREF: F(2333).
2577.9	(3/2)-	84 fs 21	β₃≈0.21 from (α,α’). E(level): β₃≈0.21 from (α,α’).
2775.2	(5/2)-	0.13 ps +5-3	XREF: Z(2770).
2826.0	3/2+,5/2+		XREF: γ(2812)L(2817).
2835.7	(3/2,5/2,7/2)-		β₃≈0.22 from (α,α’). E(level): β₃≈0.22 from (α,α’).
2902.3	(7/2)+		XREF: L(2896).
3053			XREF: F(3063).
3167.3	(21/2+)	4.35 µs 14 % IT = 100 % IT = 100	Q=(-)0.86 5, μ=+9.82 8 J^π(level): From γ(θ) observed in (⁶Li,2npγ) (1976Br14), together with the arguments given under comments.
3276.6	(3/2-)		XREF: K(3283)M(3287).
3331.1	1/2+		XREF: L(3314).
3469	7/2+		XREF: F(3475)K(3466).
3476.1	1/2-,3/2-		XREF: L(3468).
3555	(7/2)+		XREF: F(3558).
3576.1	(3/2)-	7.6 fs 13	XREF: L(3568).
3725	1/2-,3/2-		XREF: L(3739).
3898	7/2+,9/2+		XREF: F(3917)K(3893).
3908	9/2-,11/2-		XREF: K(3903).
E(level)	J^π(level)	T_1/2(level)	Comments
3962	7/2+,9/2+		XREF: L(3952).
4007	7/2+,9/2+		XREF: F(4018)γ(4018).
4025.6	(3/2+,5/2+)		XREF: L(4005).
4180.0	1/2(+),3/2,5/2+		XREF: J(4174).
4268	(1/2-,3/2-)		XREF: γ(4262)J(4273)K(4265).
4279	7/2+,9/2+		XREF: γ(4272)J(4287)K(4273).
4685	(1/2+,3/2-)		XREF: d(4674)γ(4679)J(4690).
4735	(1/2,3/2)-		XREF: n(4752).
4833	1/2-,3/2-		XREF: M(4820).
5312	(3/2+,5/2+)		XREF: n(5294).
5426			XREF: n(5408).
5598	(-)		L(α,α’)=(3). E(level): L(α,α’)=(3).
7198.7188	1/2		Γ_γ=0.0780 eV 23, Γ_n=10.8 eV 5, Γ_nΓ_γ/Γ=0.0770 eV 23 (2008Ta04). E(level): Γ_γ=0.0780 eV 23, Γ_n=10.8 eV 5, Γ_nΓ_γ/Γ=0.0770 eV 23 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7198.86427	3/2		Γ_γ=0.250 eV 22, Γ_n=0.089 eV 4, gΓ_nΓ_γ/Γ=0.130 eV 5 (2008Ta04). E(level): Γ_γ=0.250 eV 22, Γ_n=0.089 eV 4, gΓ_nΓ_γ/Γ=0.130 eV 5 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7202.0805	3/2		Γ_γ=0.150 eV 5, Γ_n=3.20 eV 19, gΓ_nΓ_γ/Γ=0.287 eV 9 (2008Ta04). E(level): Γ_γ=0.150 eV 5, Γ_n=3.20 eV 19, gΓ_nΓ_γ/Γ=0.287 eV 9 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7203.6578	1/2		Γ_γ=0.218 eV 8, Γ_n=6.0 eV 4, Γ_nΓ_γ/Γ=0.211 eV 7 (2008Ta04). E(level): Γ_γ=0.218 eV 8, Γ_n=6.0 eV 4, Γ_nΓ_γ/Γ=0.211 eV 7 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7204.39652	1/2		Γ_γ=0.44 eV 4, Γ_n=0.0200 eV 16, Γ_nΓ_γ/Γ=0.0190 eV 14 (2008Ta04). E(level): Γ_γ=0.44 eV 4, Γ_n=0.0200 eV 16, Γ_nΓ_γ/Γ=0.0190 eV 14 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7206.97387	1/2		Γ_γ=0.241 eV 20, Γ_n=0.0070 eV 6, Γ_nΓ_γ/Γ=0.0067 eV 6 (2008Ta04). E(level): Γ_γ=0.241 eV 20, Γ_n=0.0070 eV 6, Γ_nΓ_γ/Γ=0.0067 eV 6 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7207.16354	1/2		Γ_γ=0.081 eV 8, Γ_n=0.049 eV 4, Γ_nΓ_γ/Γ=0.0310 eV 20 (2008Ta04). E(level): Γ_γ=0.081 eV 8, Γ_n=0.049 eV 4, Γ_nΓ_γ/Γ=0.0310 eV 20 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7207.20615	1/2		Γ_γ=0.057 eV 5, Γ_n=0.046 eV 4, Γ_nΓ_γ/Γ=0.0260 eV 17 (2008Ta04). E(level): Γ_γ=0.057 eV 5, Γ_n=0.046 eV 4, Γ_nΓ_γ/Γ=0.0260 eV 17 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7208.118	1/2		Γ_γ=0.068 eV 5, Γ_n=30 eV 3, Γ_nΓ_γ/Γ=0.0.068 eV 5 (2008Ta04). E(level): Γ_γ=0.068 eV 5, Γ_n=30 eV 3, Γ_nΓ_γ/Γ=0.0.068 eV 5 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7208.19616	1/2		Γ_γ=0.053 eV 4, Γ_n=53 eV 5, Γ_nΓ_γ/Γ=0.053 eV 5 (2008Ta04). E(level): Γ_γ=0.053 eV 4, Γ_n=53 eV 5, Γ_nΓ_γ/Γ=0.053 eV 5 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7211.608	1/2		Γ_γ=0.099 eV 7, gΓ_n=1.46 eV 15, Γ_nΓ_γ/Γ=0.092 eV 6 (2008Ta04). E(level): Γ_γ=0.099 eV 7, gΓ_n=1.46 eV 15, Γ_nΓ_γ/Γ=0.092 eV 6 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7211.64354	1/2		Γ_γ=0.279 eV 26, Γ_n=0.0260 eV 25. Γ_nΓ_γ/Γ=0.0240 eV 20 (2008Ta04). E(level): Γ_γ=0.279 eV 26, Γ_n=0.0260 eV 25. Γ_nΓ_γ/Γ=0.0240 eV 20 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7211.6926	1/2		Γ_γ=0.246 eV 21, Γ_n=0.020 eV 2, Γ_nΓ_γ/Γ=0.0.0180 eV 17 (2008Ta04). E(level): Γ_γ=0.246 eV 21, Γ_n=0.020 eV 2, Γ_nΓ_γ/Γ=0.0.0180 eV 17 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
E(level)	J^π(level)	T_1/2(level)	Comments
7212.11	1/2		Γ_γ=0.162 eV 12, Γ_n=241 eV 18, Γ_nΓ_γ/Γ=0.162 eV 12 (2008Ta04). E(level): Γ_γ=0.162 eV 12, Γ_n=241 eV 18, Γ_nΓ_γ/Γ=0.162 eV 12 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7213.76964	1/2		Γ_γ=0.0200 eV 18, Γ_n=0.105 eV 11. Γ_nΓ_γ/Γ=0.0170 eV 13 (2008Ta04). E(level): Γ_γ=0.0200 eV 18, Γ_n=0.105 eV 11. Γ_nΓ_γ/Γ=0.0170 eV 13 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7213.788	1/2		Γ_γ=0.11 eV 1, Γ_n=0.70 eV 7, Γ_nΓ_γ/Γ=0.097 eV 7 (2008Ta04). E(level): Γ_γ=0.11 eV 1, Γ_n=0.70 eV 7, Γ_nΓ_γ/Γ=0.097 eV 7 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7214.396	1/2		Γ_γ=0.270 eV 15, Γ_n=13.0 eV 12, Γ_nΓ_γ/Γ=0.267 eV 15 (2008Ta04). E(level): Γ_γ=0.270 eV 15, Γ_n=13.0 eV 12, Γ_nΓ_γ/Γ=0.267 eV 15 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7221.078	3/2		Γ_γ=0.065 eV 6, Γ_n=1.30 eV 13, gΓ_nΓ_γ/Γ=0.124 eV 10 (2008Ta04). E(level): Γ_γ=0.065 eV 6, Γ_n=1.30 eV 13, gΓ_nΓ_γ/Γ=0.124 eV 10 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7221.146	3/2		Γ_γ=0.210 eV 13, Γ_n=5.8 eV 6, gΓ_nΓ_γ/Γ=0.410 eV 25 (2008Ta04). E(level): Γ_γ=0.210 eV 13, Γ_n=5.8 eV 6, gΓ_nΓ_γ/Γ=0.410 eV 25 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7223.410	3/2		Γ_γ=0.150 eV 15, Γ_n=1.10 eV 11, gΓ_nΓ_γ/Γ=0.270 eV 24 (2008Ta04). E(level): Γ_γ=0.150 eV 15, Γ_n=1.10 eV 11, gΓ_nΓ_γ/Γ=0.270 eV 24 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7229.867	1/2		Γ_γ=0.59 eV 4, Γ_n=38 eV 4, Γ_nΓ_γ/Γ=0.58 eV 4 (2008Ta04). E(level): Γ_γ=0.59 eV 4, Γ_n=38 eV 4, Γ_nΓ_γ/Γ=0.58 eV 4 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7233.973	3/2		Γ_γ=0.180 eV 15, Γ_n=1.30 eV 13, gΓ_nΓ_γ/Γ=0.329 eV 24 (2008Ta04). E(level): Γ_γ=0.180 eV 15, Γ_n=1.30 eV 13, gΓ_nΓ_γ/Γ=0.329 eV 24 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7234.86	1/2		Γ_γ=0.160 eV 15, Γ_n=58 eV 6, Γ_nΓ_γ/Γ=0.162 eV 15 (2008Ta04). E(level): Γ_γ=0.160 eV 15, Γ_n=58 eV 6, Γ_nΓ_γ/Γ=0.162 eV 15 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7235.84	3/2		Γ_γ=0.98 eV 5, Γ_n=236 eV 17, gΓ_nΓ_γ/Γ=1.96 eV 11 (2008Ta04). E(level): Γ_γ=0.98 eV 5, Γ_n=236 eV 17, gΓ_nΓ_γ/Γ=1.96 eV 11 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7236.5076	3/2		Γ_γ=0.040 eV 4, Γ_n=0.20 eV 2, gΓ_nΓ_γ/Γ=0.068 eV 6 (2008Ta04). E(level): Γ_γ=0.040 eV 4, Γ_n=0.20 eV 2, gΓ_nΓ_γ/Γ=0.068 eV 6 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7236.65	1/2		Γ_γ=0.200 eV 19, Γ_n=285 eV 28, Γ_nΓ_γ/Γ=0.203 eV 19 (2008Ta04). E(level): Γ_γ=0.200 eV 19, Γ_n=285 eV 28, Γ_nΓ_γ/Γ=0.203 eV 19 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7236.888	1/2		Γ_γ=0.071 eV 7, Γ_n=0.49 eV 5, Γ_nΓ_γ/Γ=0.062 eV 5 (2008Ta04). E(level): Γ_γ=0.071 eV 7, Γ_n=0.49 eV 5, Γ_nΓ_γ/Γ=0.062 eV 5 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7237.071	1/2		Γ_γ=0.200 eV 17, Γ_n=116 eV 11, Γ_nΓ_γ/Γ=0.200 eV 17 (2008Ta04). E(level): Γ_γ=0.200 eV 17, Γ_n=116 eV 11, Γ_nΓ_γ/Γ=0.200 eV 17 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7239.229	3/2		Γ_γ=0.310 eV 22, Γ_n=83 eV 8, gΓ_nΓ_γ/Γ=0.63 eV 5 (2008Ta04). E(level): Γ_γ=0.310 eV 22, Γ_n=83 eV 8, gΓ_nΓ_γ/Γ=0.63 eV 5 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7247.579	1/2		Γ_γ=0.0250 eV 25, Γ_n=0.81 eV 8, Γ_nΓ_γ/Γ=0.0250 eV 24 (2008Ta04). E(level): Γ_γ=0.0250 eV 25, Γ_n=0.81 eV 8, Γ_nΓ_γ/Γ=0.0250 eV 24 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7247.685	1/2		Γ_γ=0.094 eV 9, Γ_n=1.50 eV 15, Γ_nΓ_γ/Γ=0.088 eV 8 (2008Ta04). E(level): Γ_γ=0.094 eV 9, Γ_n=1.50 eV 15, Γ_nΓ_γ/Γ=0.088 eV 8 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7247.982	1/2		Γ_γ=0.190 eV 19, Γ_n=0.48 eV 5, Γ_nΓ_γ/Γ=0.134 eV 10 (2008Ta04). E(level): Γ_γ=0.190 eV 19, Γ_n=0.48 eV 5, Γ_nΓ_γ/Γ=0.134 eV 10 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7248.656	1/2		Γ_γ=0.240 eV 24, Γ_n=0.098 eV 10, Γ_nΓ_γ/Γ=0.070 eV 5 (2008Ta04). E(level): Γ_γ=0.240 eV 24, Γ_n=0.098 eV 10, Γ_nΓ_γ/Γ=0.070 eV 5 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7248.847	1/2		Γ_γ=0.250 eV 25, Γ_n=0.22 eV 2, Γ_nΓ_γ/Γ=0.117 eV 8 (2008Ta04). E(level): Γ_γ=0.250 eV 25, Γ_n=0.22 eV 2, Γ_nΓ_γ/Γ=0.117 eV 8 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7250.09	1/2		Γ_γ=0.190 eV 18, Γ_n=64 eV 6, Γ_nΓ_γ/Γ=0.192 eV 18 (2008Ta04). E(level): Γ_γ=0.190 eV 18, Γ_n=64 eV 6, Γ_nΓ_γ/Γ=0.192 eV 18 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7250.80	1/2		Γ_γ=0.250 eV 22, Γ_n=41 eV 4, Γ_nΓ_γ/Γ=0.244 eV 21 (2008Ta04). E(level): Γ_γ=0.250 eV 22, Γ_n=41 eV 4, Γ_nΓ_γ/Γ=0.244 eV 21 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7252.055	1/2		Γ_γ/Γ=0.42 eV 4, Γ_n=0.65 eV 6, Γ_nΓ_γ/Γ=0.257 eV 18 (2008Ta04). E(level): Γ_γ/Γ=0.42 eV 4, Γ_n=0.65 eV 6, Γ_nΓ_γ/Γ=0.257 eV 18 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7252.570	1/2		Γ_γ/Γ=0.180 eV 16, Γ_n=9.4 eV 9, Γ_nΓ_γ/Γ=0.174 eV 15 (2008Ta04). E(level): Γ_γ/Γ=0.180 eV 16, Γ_n=9.4 eV 9, Γ_nΓ_γ/Γ=0.174 eV 15 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
E(level)	J^π(level)	T_1/2(level)	Comments
7256.1198	3/2		Γ_γ=0.200 eV 20, gΓ_n=0.70 eV 7, gΓ_nΓ_γ/Γ=0.313 eV 25 (2008Ta04). E(level): Γ_γ=0.200 eV 20, gΓ_n=0.70 eV 7, gΓ_nΓ_γ/Γ=0.313 eV 25 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7256.624	1/2		Γ_γ=0.150 eV 15, Γ_n=1.0 eV 1, Γ_nΓ_γ/Γ=0.128 eV 11 (2008Ta04). E(level): Γ_γ=0.150 eV 15, Γ_n=1.0 eV 1, Γ_nΓ_γ/Γ=0.128 eV 11 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7258.1392	1/2		Γ_γ=0.160 eV 16, Γ_n=0.70 eV 7, Γ_nΓ_γ/Γ=0.133 eV 11 (2008Ta04). E(level): Γ_γ=0.160 eV 16, Γ_n=0.70 eV 7, Γ_nΓ_γ/Γ=0.133 eV 11 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7259.14	1/2		Γ_γ=0.079 eV 8, Γ_n=127 eV 13, Γ_nΓ_γ/Γ=0.079 eV 8 (2008Ta04). E(level): Γ_γ=0.079 eV 8, Γ_n=127 eV 13, Γ_nΓ_γ/Γ=0.079 eV 8 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7259.36	3/2		Γ_γ=0.47 eV 4, gΓ_n=129 eV 13, gΓ_nΓ_γ/Γ=0.94 eV 7 (2008Ta04). E(level): Γ_γ=0.47 eV 4, gΓ_n=129 eV 13, gΓ_nΓ_γ/Γ=0.94 eV 7 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7259.544	1/2		Γ_γ=0.30 eV 3, Γ_n=0.70 eV 7, Γ_nΓ_γ/Γ=0.212 eV 16 (2008Ta04). E(level): Γ_γ=0.30 eV 3, Γ_n=0.70 eV 7, Γ_nΓ_γ/Γ=0.212 eV 16 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7262.737	3/2		Γ_γ=0.43 eV 4, gΓ_n=5.5 eV 5, gΓ_nΓ_γ/Γ=0.80 eV 7 (2008Ta04). E(level): Γ_γ=0.43 eV 4, gΓ_n=5.5 eV 5, gΓ_nΓ_γ/Γ=0.80 eV 7 (2008Ta04). All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7264.96	1/2		Γ_γ=0.139 eV 20, Γ_n=205 eV 25, gΓ_nΓ_γ/Γ=0.139 eV. E(level): Γ_γ=0.139 eV 20, Γ_n=205 eV 25, gΓ_nΓ_γ/Γ=0.139 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7266.57	3/2		Γ_γ=0.121 eV 15, gΓ_n=300 eV 20, gΓ_nΓ_γ/Γ=0.241 eV. E(level): Γ_γ=0.121 eV 15, gΓ_n=300 eV 20, gΓ_nΓ_γ/Γ=0.241 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7267.42	1/2		Γ_γ=0.135 eV 20, Γ_n=170 eV 20, Γ_nΓ_γ/Γ=0.134 eV. E(level): Γ_γ=0.135 eV 20, Γ_n=170 eV 20, Γ_nΓ_γ/Γ=0.134 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7268.57	3/2		Γ_γ=0.105 eV 11, gΓ_n=42 eV 8, gΓ_nΓ_γ/Γ=0.209 eV. E(level): Γ_γ=0.105 eV 11, gΓ_n=42 eV 8, gΓ_nΓ_γ/Γ=0.209 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7269.59			gΓ_n=2 eV 1, gΓ_nΓ_γ/Γ=0.086 eV. E(level): gΓ_n=2 eV 1, gΓ_nΓ_γ/Γ=0.086 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7270.06			gΓ_n=1.5 eV 10, gΓ_nΓ_γ/Γ=0.175 eV. E(level): gΓ_n=1.5 eV 10, gΓ_nΓ_γ/Γ=0.175 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7273.70			gΓ_n=0.5 eV 5, gΓ_nΓ_γ/Γ=0.1 eV. E(level): gΓ_n=0.5 eV 5, gΓ_nΓ_γ/Γ=0.1 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7274.18			gΓ_n=0.5 eV 5. E(level): gΓ_n=0.5 eV 5. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7274.46			gΓ_nΓ_γ/Γ=0.251 eV. E(level): gΓ_nΓ_γ/Γ=0.251 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7275.48			gΓ_nΓ_γ/Γ=0.36 eV. E(level): gΓ_nΓ_γ/Γ=0.36 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7276.16	3/2		Γ_γ=0.28 eV 4, gΓ_n=210 eV 10, gΓ_nΓ_γ/Γ=0.557 eV. E(level): Γ_γ=0.28 eV 4, gΓ_n=210 eV 10, gΓ_nΓ_γ/Γ=0.557 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7277.22	[1/2]		Γ_γ=0.102 eV 11, gΓ_n=14 eV 3, gΓ_nΓ_γ/Γ=0.102 eV. E(level): Γ_γ=0.102 eV 11, gΓ_n=14 eV 3, gΓ_nΓ_γ/Γ=0.102 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7279.69	1/2		Γ_γ=0.127 eV 22, Γ_n=6.5 eV 10, Γ_nΓ_γ/Γ=0.125 eV. E(level): Γ_γ=0.127 eV 22, Γ_n=6.5 eV 10, Γ_nΓ_γ/Γ=0.125 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7284.28	1/2		Γ_γ=0.249 eV 25, Γ_n=19 eV 3, Γ_nΓ_γ/Γ=0.246 eV. E(level): Γ_γ=0.249 eV 25, Γ_n=19 eV 3, Γ_nΓ_γ/Γ=0.246 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7286.77	3/2		Γ_γ=0.19 eV 4, gΓ_n=4.00 eV 14, gΓ_nΓ_γ/Γ=0.345 eV. E(level): Γ_γ=0.19 eV 4, gΓ_n=4.00 eV 14, gΓ_nΓ_γ/Γ=0.345 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7288.16	(1/2)		Γ_γ=0.31 eV 3, gΓ_n=2 eV 1, gΓ_nΓ_γ/Γ=0.272 eV. E(level): Γ_γ=0.31 eV 3, gΓ_n=2 eV 1, gΓ_nΓ_γ/Γ=0.272 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7288.68			gΓ_n=4 eV 1, gΓ_nΓ_γ/Γ=0.418 eV. E(level): gΓ_n=4 eV 1, gΓ_nΓ_γ/Γ=0.418 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7289.63	3/2		Γ_γ=0.21 eV 4, gΓ_n=30 eV 4, gΓ_nΓ_γ/Γ=0.408 eV. E(level): Γ_γ=0.21 eV 4, gΓ_n=30 eV 4, gΓ_nΓ_γ/Γ=0.408 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
E(level)	J^π(level)	T_1/2(level)	Comments
7291.17	3/2		Γ_γ=0.38 eV 5, gΓ_n=42 eV 4, gΓ_nΓ_γ/Γ=0.745 eV. E(level): Γ_γ=0.38 eV 5, gΓ_n=42 eV 4, gΓ_nΓ_γ/Γ=0.745 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7292.99	3/2		Γ_γ=0.46 eV 5, gΓ_n=7 eV 2, gΓ_nΓ_γ/Γ=0.82 eV. E(level): Γ_γ=0.46 eV 5, gΓ_n=7 eV 2, gΓ_nΓ_γ/Γ=0.82 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7294.20	3/2		Γ_γ=0.36 eV 3, gΓ_n=2 eV 1, gΓ_nΓ_γ/Γ=0.533 eV. E(level): Γ_γ=0.36 eV 3, gΓ_n=2 eV 1, gΓ_nΓ_γ/Γ=0.533 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7298.45	1/2		Γ_γ=1.38 eV 20, Γ_n=210 eV 15, Γ_nΓ_γ/Γ=1.373 eV. E(level): Γ_γ=1.38 eV 20, Γ_n=210 eV 15, Γ_nΓ_γ/Γ=1.373 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7298.94	3/2		Γ_γ=0.63 eV 10, gΓ_n=300 eV 30, gΓ_nΓ_γ/Γ=1.26 eV. E(level): Γ_γ=0.63 eV 10, gΓ_n=300 eV 30, gΓ_nΓ_γ/Γ=1.26 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7302.01			gΓ_n<0.5 eV. gΓ_nΓ_γ/Γ=0.372 eV. E(level): gΓ_n<0.5 eV. gΓ_nΓ_γ/Γ=0.372 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7302.90	3/2		Γ_γ=0.41 eV 6, gΓ_n=116 eV 14, gΓ_nΓ_γ/Γ=0.806 eV. E(level): Γ_γ=0.41 eV 6, gΓ_n=116 eV 14, gΓ_nΓ_γ/Γ=0.806 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7303.89	3/2		Γ_γ=0.53 eV 6, gΓ_n=150 eV 15, gΓ_nΓ_γ/Γ=1.049 eV. E(level): Γ_γ=0.53 eV 6, gΓ_n=150 eV 15, gΓ_nΓ_γ/Γ=1.049 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7305.08	3/2		Γ_γ=0.40 eV 6, gΓ_n=238 eV 20, gΓ_nΓ_γ/Γ=0.806 eV. E(level): Γ_γ=0.40 eV 6, gΓ_n=238 eV 20, gΓ_nΓ_γ/Γ=0.806 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7307.75	1/2		gΓ_n=136 eV 12, Γ_nΓ_γ/Γ=0.577 eV. E(level): gΓ_n=136 eV 12, Γ_nΓ_γ/Γ=0.577 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7312.39	1/2		Γ_γ=0.206 eV 21, gΓ_n=142 eV 14, Γ_nΓ_γ/Γ=0.206 eV. E(level): Γ_γ=0.206 eV 21, gΓ_n=142 eV 14, Γ_nΓ_γ/Γ=0.206 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7315.06	(3/2)		Γ_γ=0.272 eV 24, gΓ_n=3 eV 1, gΓ_nΓ_γ/Γ=0.461 eV. E(level): Γ_γ=0.272 eV 24, gΓ_n=3 eV 1, gΓ_nΓ_γ/Γ=0.461 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7315.76	[3/2]		Γ_γ=0.225 eV 25, gΓ_n=23 eV 3, gΓ_nΓ_γ/Γ=0.442 eV. E(level): Γ_γ=0.225 eV 25, gΓ_n=23 eV 3, gΓ_nΓ_γ/Γ=0.442 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7316.15			gΓ_nΓ_γ/Γ=0.605 eV. E(level): gΓ_nΓ_γ/Γ=0.605 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7317.74	1/2		Γ_γ=0.50 eV 8, Γ_n=26 eV 3, Γ_nΓ_γ/Γ=0.49 eV. E(level): Γ_γ=0.50 eV 8, Γ_n=26 eV 3, Γ_nΓ_γ/Γ=0.49 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7320.21			gΓ_n=34 eV 5. E(level): gΓ_n=34 eV 5. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7320.70	3/2		Γ_γ=0.65 eV 20, gΓ_n=426 eV 30, gΓ_nΓ_γ/Γ=1.3 eV. E(level): Γ_γ=0.65 eV 20, gΓ_n=426 eV 30, gΓ_nΓ_γ/Γ=1.3 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7323.08	1/2		Γ_γ=0.25 eV 9, Γ_n=140 eV 10, gΓ_nΓ_γ/Γ=0.252 eV. E(level): Γ_γ=0.25 eV 9, Γ_n=140 eV 10, gΓ_nΓ_γ/Γ=0.252 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7323.77			gΓ_nΓ_γ/Γ=0.312 eV. E(level): gΓ_nΓ_γ/Γ=0.312 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7324.36			gΓ_nΓ_γ/Γ=0.486 eV. E(level): gΓ_nΓ_γ/Γ=0.486 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7325.05	3/2		Γ_γ=0.32 eV 5, gΓ_n=342 eV 16, gΓ_nΓ_γ/Γ=0.641 eV. E(level): Γ_γ=0.32 eV 5, gΓ_n=342 eV 16, gΓ_nΓ_γ/Γ=0.641 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7327.13			gΓ_nΓ_γ/Γ=0.448 eV. E(level): gΓ_nΓ_γ/Γ=0.448 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7327.53	3/2		Γ_γ=0.35 eV 8, gΓ_n=334 eV 14, gΓ_nΓ_γ/Γ=0.7 eV. E(level): Γ_γ=0.35 eV 8, gΓ_n=334 eV 14, gΓ_nΓ_γ/Γ=0.7 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7332.47	3/2		Γ_γ=0.30 eV 8, gΓ_n=14 eV 2, gΓ_nΓ_γ/Γ=0.57 eV. E(level): Γ_γ=0.30 eV 8, gΓ_n=14 eV 2, gΓ_nΓ_γ/Γ=0.57 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7337.61	1/2		Γ_n=325 eV 15, Γ_nΓ_γ/Γ=0.57 eV. E(level): Γ_n=325 eV 15, Γ_nΓ_γ/Γ=0.57 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
E(level)	J^π(level)	T_1/2(level)	Comments
7338.70			gΓ_n=29 eV 3, gΓ_nΓ_γ/Γ=0.473 eV. E(level): gΓ_n=29 eV 3, gΓ_nΓ_γ/Γ=0.473 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7341.57			gΓ_n=3 eV 2, gΓ_nΓ_γ/Γ=0.464 eV. E(level): gΓ_n=3 eV 2, gΓ_nΓ_γ/Γ=0.464 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7343.55	1/2		Γ_γ=0.47 eV 5, Γ_n=190 eV 15, Γ_nΓ_γ/Γ=0.464 eV. E(level): Γ_γ=0.47 eV 5, Γ_n=190 eV 15, Γ_nΓ_γ/Γ=0.464 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7344.44	1/2		Γ_n=225 eV 25. E(level): Γ_n=225 eV 25. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7348.8	1/2		Γ_γ=0.70 eV 15, gΓ_n=1900 eV 250, gΓ_nΓ_γ/Γ=0.697 eV. E(level): Γ_γ=0.70 eV 15, gΓ_n=1900 eV 250, gΓ_nΓ_γ/Γ=0.697 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7349.8	3/2		Γ_γ=0.64 eV 10, gΓ_n=720 eV 60, gΓ_nΓ_γ/Γ=1.271 eV. E(level): Γ_γ=0.64 eV 10, gΓ_n=720 eV 60, gΓ_nΓ_γ/Γ=1.271 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7352.85	1/2		gΓ_n=49 eV 6. E(level): gΓ_n=49 eV 6. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7353.14			gΓ_n=10 eV 5. gΓ_nΓ_γ/Γ=0.895 eV. E(level): gΓ_n=10 eV 5. gΓ_nΓ_γ/Γ=0.895 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7354.23	[3/2]		Γ_γ=0.36 eV 4, gΓ_n=42 eV 5, gΓ_nΓ_γ/Γ=0.716 eV. E(level): Γ_γ=0.36 eV 4, gΓ_n=42 eV 5, gΓ_nΓ_γ/Γ=0.716 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7356.41	1/2		Γ_γ=0.83 eV 16, gΓ_n=1090 eV 200, gΓ_nΓ_γ/Γ=0.83 eV. E(level): Γ_γ=0.83 eV 16, gΓ_n=1090 eV 200, gΓ_nΓ_γ/Γ=0.83 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7357.39	1/2		Γ_n=350 eV 50. E(level): Γ_n=350 eV 50. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7359.37	3/2		Γ_γ=1.40 eV 2, gΓ_n=860 eV 60, gΓ_nΓ_γ/Γ=2.799 eV. E(level): Γ_γ=1.40 eV 2, gΓ_n=860 eV 60, gΓ_nΓ_γ/Γ=2.799 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7361.85	1/2		Γ_n=130 eV 20. E(level): Γ_n=130 eV 20. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7365.41	3/2		Γ_γ=1.33 eV 20, gΓ_n=600 eV 50, gΓ_nΓ_γ/Γ=2.648 eV. E(level): Γ_γ=1.33 eV 20, gΓ_n=600 eV 50, gΓ_nΓ_γ/Γ=2.648 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7369.06	1/2		Γ_n=170 eV 20. E(level): Γ_n=170 eV 20. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7370.55	3/2		Γ_γ=0.46 eV 9, gΓ_n=1750 eV 300, gΓ_nΓ_γ/Γ=0.911 eV. E(level): Γ_γ=0.46 eV 9, gΓ_n=1750 eV 300, gΓ_nΓ_γ/Γ=0.911 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7372.72	[1/2]		Γ_n=90 eV 9. E(level): Γ_n=90 eV 9. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7374.41	3/2		Γ_γ=0.33 eV 6, gΓ_n=544 eV 40, gΓ_nΓ_γ/Γ=0.663 eV. E(level): Γ_γ=0.33 eV 6, gΓ_n=544 eV 40, gΓ_nΓ_γ/Γ=0.663 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7377.17	3/2		Γ_γ=0.55 eV 16, gΓ_n=820 eV 60, gΓ_nΓ_γ/Γ=1.098 eV. E(level): Γ_γ=0.55 eV 16, gΓ_n=820 eV 60, gΓ_nΓ_γ/Γ=1.098 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7378.86	1/2		Γ_n=50 eV 7. E(level): Γ_n=50 eV 7. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7381.23			gΓ_nΓ_γ/Γ=0.406 eV. E(level): gΓ_nΓ_γ/Γ=0.406 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7381.92			gΓ_nΓ_γ/Γ=0.499 eV. E(level): gΓ_nΓ_γ/Γ=0.499 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7382.71	1/2		Γ_γ=0.76 eV 25, Γ_n=78 eV 8, Γ_nΓ_γ/Γ=0.756 eV. E(level): Γ_γ=0.76 eV 25, Γ_n=78 eV 8, Γ_nΓ_γ/Γ=0.756 eV. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7385.58	1/2		Γ_n=92 eV 10. E(level): Γ_n=92 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7386.17	1/2		Γ_n=106 eV 10. E(level): Γ_n=106 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
E(level)	J^π(level)	T_1/2(level)	Comments
7391.12	1/2		Γ_n=470 eV 30. E(level): Γ_n=470 eV 30. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7392.70			gΓ_n=30 eV 10. E(level): gΓ_n=30 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7394.48			gΓ_n=10 eV 5. E(level): gΓ_n=10 eV 5. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7396.66			gΓ_n=50 eV 10. E(level): gΓ_n=50 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7399.43			gΓ_n=67 eV 10. E(level): gΓ_n=67 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7400.42			gΓ_n=24 eV 10. E(level): gΓ_n=24 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7400.71	1/2		Γ_n=96 eV 10. E(level): Γ_n=96 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7403.68	3/2		gΓ_n=1300 eV 200. E(level): gΓ_n=1300 eV 200. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7407.54	3/2		gΓ_n=750 eV 140. E(level): gΓ_n=750 eV 140. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7411.7	1/2		Γ_n=2400 eV 300. E(level): Γ_n=2400 eV 300. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7412.8	3/2		gΓ_n=1510 eV 150. E(level): gΓ_n=1510 eV 150. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7415.3	1/2		Γ_n=345 eV 35. E(level): Γ_n=345 eV 35. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7416.0	[3/2]		gΓ_n=320 eV 40. E(level): gΓ_n=320 eV 40. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7419.70	3/2		gΓ_n=466 eV 50. E(level): gΓ_n=466 eV 50. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7423.56	1/2		Γ_n=413 eV 45. E(level): Γ_n=413 eV 45. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7430.4	3/2		gΓ_n=3000 eV 300. E(level): gΓ_n=3000 eV 300. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7432.3	1/2		Γ_n=3250 eV 300. E(level): Γ_n=3250 eV 300. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7436.61			gΓ_n=42 eV 6. E(level): gΓ_n=42 eV 6. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7438.89			gΓ_n=164 eV 20. E(level): gΓ_n=164 eV 20. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7440.67	1/2		Γ_n=96 eV 10. E(level): Γ_n=96 eV 10. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7445.91	3/2		gΓ_n=580 eV 50. E(level): gΓ_n=580 eV 50. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7448.09	1/2		Γ_n=300 eV 30. E(level): Γ_n=300 eV 30. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7456.00	1/2		Γ_n=200 eV 20. E(level): Γ_n=200 eV 20. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7456.89	1/2		Γ_n=170 eV 25. E(level): Γ_n=170 eV 25. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7464.2	3/2		gΓ_n=1100 eV 100. E(level): gΓ_n=1100 eV 100. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
E(level)	J^π(level)	T_1/2(level)	Comments
7464.6	1/2		Γ_n=290 eV 30. E(level): Γ_n=290 eV 30. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7472.5	[3/2]		gΓ_n=2190 eV 300. E(level): gΓ_n=2190 eV 300. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7475.9			gΓ_n=360 eV 50. E(level): gΓ_n=360 eV 50. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7478.8	3/2		gΓ_n=2140 eV 200. E(level): gΓ_n=2140 eV 200. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7481.1	3/2		gΓ_n=480 eV 80. E(level): gΓ_n=480 eV 80. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7482.6			gΓ_n=420 eV 50. E(level): gΓ_n=420 eV 50. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7485.4	3/2		gΓ_n=492 eV 60. E(level): gΓ_n=492 eV 60. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
7492.5	1/2		Γ_n=410 eV 50. E(level): Γ_n=410 eV 50. All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level). J^π(level): All data are from (n,γ) E=res. Note that the systematic uncertainty of 0.4 keV arising from the adopted S(n) value needs to be combined in quadrature with the uncertainties shown here for E(level).
14.40E3			Not a discrete state; Γ=6 MeV. E(level): Not a discrete state; Γ=6 MeV.

E(level)	E(gamma)	Comments
1204.81	1204.80	E(γ): unweighted average of 1204.67 8 from ε decay (60.86 d) and 1204.92 10 from (n,n’γ). M(γ): from Coulomb excitation.
1466.4	1466.3	E(γ): Weighted average from (α,nγ), (n,n’γ), (¹³C,¹²Cγ), (γ,γ’).
1882.20	1882.18	E(γ): Weighted average from (α,nγ), (n,n’γ), (γ,γ’).
2042.35	2042.33	E(γ): Weighted average from (α,nγ), (n,n’γ), (¹³C,¹²Cγ), (γ,γ’).
2131.49	2131.54	E(γ): Weighted average from (α,nγ), (n,n’γ), (⁶Li,2npγ), (γ,γ’). M(γ): stretched (Q) from γ(θ) in (n,n’γ), not M2 from RUL.
2170.15	38.7	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ).
2170.15	2170.04	E(γ): Weighted average from (α,nγ), (n,n’γ), (⁶Li,2npγ), (¹³C,¹²Cγ). I(γ): from (⁶Li,2npγ). M(γ): γ(θ) in (⁶Li,2npγ) and (n,n’γ) consistent with octupole; Δπ from level scheme.
2189.5	2189.0	E(γ): Weighted average from (n,n’γ) and (α,nγ).
2259.92	89.55	E(γ): Weighted average from (α,nγ) and (⁶Li,2npγ). M(γ): not stretched Q (from γ(θ) in (α,nγ)).
2287.8	28.0	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ). M(γ): from α(exp) in (⁶Li,2npγ).
2320.5	60.33	E(γ): Weighted average from (α,nγ) and (⁶Li,2npγ).
2320.5	151.1	E(γ): Weighted average from (α,nγ), (n,n’γ), and (⁶Li,2npγ).
2356.4	1151.6	E(γ): Weighted average from (n,n’γ) and (α,nγ).
2366.56	2366.53	E(γ): Weighted average from (α,nγ), (n,n’γ), (γ,γ’).
2394.9	224.8	E(γ): from (α,nγ).
2534.69	652.49	E(γ): Weighted average from (n,n’γ) and (α,nγ).
2557.8	2557.8	E(γ): Weighted average from (α,nγ), (n,n’γ), (¹³C,¹²Cγ).
2577.9	2577.9	E(γ): Weighted average from (α,nγ), (n,n’γ), (γ,γ’).
2640.2	2640.1	E(γ): Weighted average from (n,n’γ) and (α,nγ).
2693.7	2693.7	E(γ): Weighted average from (α,nγ), (n,n’γ), (γ,γ’).
2764.6	443.8	E(γ): Weighted average from (n,n’γ) and (α,nγ). I(γ): average of 33 and 25 from (α,nγ) at E(p)=11.8 and 13.5 MeV, respectively.
2764.6	477.2	E(γ): Weighted average from (α,nγ) and (⁶Li,2npγ). M(γ): not stretched Q (from γ(θ) in (⁶Li,2npγ)).
2791.46	659.97	E(γ): Weighted average from (n,n’γ) and (α,nγ).
2810.9	415.9	M(γ): not pure E2 from RUL.
2810.9	2810.9	E(γ): Weighted average from (α,nγ), (n,n’γ), (γ,γ’).
E(level)	E(gamma)	Comments
2826.0	2826.0	E(γ): from (α,nγ).
2857.06	537	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ).
	570	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ).
	596.9	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ).
	725.7	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ). M(γ): Q from γ(θ) in (⁶Li,2npγ), not M2 from RUL.
3017.1	3017.0	E(γ): from (α,nγ).
3083.3	3083.3	E(γ): Weighted average from (n,n’γ) and (α,nγ).
3146.9	289.8	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ). M(γ): Q from γ(θ) in (⁶Li,2npγ), not M2 from RUL.
3146.9	859.0	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ). M(γ): not stretched Q from γ(θ) in (⁶Li,2npγ).
3167.3	20.4	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ).
3167.3	879.4	E(γ): From (⁶Li,2npγ). I(γ): From (⁶Li,2npγ).
3476.1	3476	E(γ): from (γ,γ’); 3476.7 in (n,γ).
3476.3	3476	E(γ): from (γ,γ’); 3476.7 in (n,γ).
3576.1	3576	E(γ): from (γ,γ’).
3681	3681	E(γ): from (γ,γ’).
3704	3704	E(γ): from (γ,γ’).
3984.2	3984.5	E(γ): from (n,γ).
4162.4	4162.6	E(γ): from (n,γ).
4319.8	4319.8	E(γ): from (n,γ) E=thermal; Eγ=4322 2 in (γ,γ’).
4685	4685	E(γ): from level energy difference. Possibly the 4674γ from (γ,γ’).
4704	4704.1	E(γ): from (γ,γ’) alone so shown as tentative.
7194.4	2662.12	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	2875.00	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3015.12	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3032.53	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3169.20	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3210.85	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3718.15	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3906.30	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	3960.14	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	4111.5	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	4322.4	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	4553.9	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	4617.0	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	4636.8	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	4828.5	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	5152.4	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	5989.8	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
	7194.4	E(γ): Primary γ from (n,γ) E=thermal. I(γ): Primary γ from (n,γ) E=thermal.
E(level)	E(gamma)	Comments