List of levels for 57FE

Author: M. R. Bhat | Citation: Nucl. Data Sheets 85, 415 (1998) | Cutoff date: 24-Sep-1998

Resonance parameters: see 1984Fi09, 1983Ma54, 1983Ka09, 1981MuZQ, and the (n,γ) and (γ,n) references cited below

Levels: Configuration: see discussion in (n,γ) E=thermal on the configurations of the g.s., 14.4, 1627.3 and 1725.4, and capture states

Levels: Note: Jπ arguments based on γ(θ) from (α,nγ) are considered tentative by the evaluator since a Gaussian distribution of the magnetic substates was assumed and this is model dependent (see (¹³C,4nγ))

Levels: B(E2): see Coulomb excitation

Gammas: See (¹³C,4nγ), (α,nγ), and (n,γ) for unplaced gammas

Gammas: B(M1)(W.u.),B(E1)(W.u.),B(E2)(W.u.): calculated by evaluators from adopted T_1/2 and γ properties, except as noted

Q-value: Note: Current evaluation has used the following Q record -836.0 4 7646.03 1010559.1 4 -7320.0 4 1995Au04

E(level): For states connected by gammas, calculated using least-square adjustment procedures with the energy of the s- and p-wave capture states held fixed and uncertain gammas not included in the calculation. Uncertainty in ¹⁹⁸Au reference scale (|+1.1 eV) for 122γ and 136γ added in quadrature after adjustment. Other energies from ⁵⁶Fe(d,p),⁵⁷Fe(p,p’),⁵⁹Co(d,α), except as noted

J^π(level): From angular momentum transfer in (d,p), except as noted

T_1/2(level): From DSAM or RDM in (¹³C,4nγ), except as noted

I(γ): Relative-photon branching from each level

E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
14.4129	3/2-	98.3 ns 3	14.4129 6	M1+E2	0.00223 18	8.56	B(E2)(W.u.)=0.37 7, B(M1)(W.u.)=0.0078 3, α=8.56 26, α(K)=7.35 19, α(L)=0.779 42
136.4743	5/2-	8.7 ns 3	122.0614 4	M1+E2	+0.120 1	0.0240	B(E2)(W.u.)=2.3 4, B(M1)(W.u.)=0.00118 17, α=0.0240 14, α(K)=0.0214 12, α(L)=0.00224 20
136.4743	5/2-	8.7 ns 3	136.4743 5	E2		0.137	B(E2)(W.u.)=10.9 16, α=0.137 15, α(K)=0.134, α(L)=0.0139
366.759	3/2-	10.5 ps 14	230.29 2	(M1+E2)	+0.02 8		B(E2)(W.u.)=0.2 +15-2, B(M1)(W.u.)=0.0124 25
	3/2-	10.5 ps 14	352.36 1	M1+E2	+0.025 9		B(E2)(W.u.)=0.4 3, B(M1)(W.u.)=0.038 8
	3/2-	10.5 ps 14	366.75 1	M1+E2	-0.45 5		B(E2)(W.u.)=15 4, B(M1)(W.u.)=0.0049 10
706.416	5/2-	4.1 ps 11	339.54 18	M1+E2	+0.083 5		B(E2)(W.u.)=0.23 9, B(M1)(W.u.)=0.0020 7
	5/2-	4.1 ps 11	569.92 4	M1+E2	+0.097 8		B(E2)(W.u.)=0.15 6, B(M1)(W.u.)=0.0027 9
	5/2-	4.1 ps 11	692.03 2	M1+E2	-0.465 8		B(E2)(W.u.)=10 3, B(M1)(W.u.)=0.011 4
	5/2-	4.1 ps 11	706.4 2	[E2]			B(E2)(W.u.)=2.9 15
1007.13	7/2-	0.13 ps 7	640.20 14	E2			B(E2)(W.u.)=9.×10¹ 9
	7/2-	0.13 ps 7	870.68 5	M1+E2	-0.6 +2-5		B(E2)(W.u.)=1.1×10² 9, B(M1)(W.u.)=0.12 7
	7/2-	0.13 ps 7	992.68 8	E2			B(E2)(W.u.)=1.1×10² 7
1197.81	9/2-	2.9 ps 4	1061.60 17	E2			B(E2)(W.u.)=11.1 16
1356.83	7/2-	0.18 ps 7	650.4 19	M1+E2	+1.1 +6-3		B(E2)(W.u.)=6.×10² 4, B(M1)(W.u.)=0.11 8
	7/2-	0.18 ps 7	990.1 21	E2			B(E2)(W.u.)=6.×10¹ 3
	7/2-	0.18 ps 7	1342.7 22	E2			B(E2)(W.u.)=12 5
1627.256	3/2-	56 fs 8	1612.78 2	M1+E2	-0.35 5		B(E2)(W.u.)=4.7 16, B(M1)(W.u.)=0.051 10
1725.38	3/2-	31 fs 4	1725.09 6	M1+E2	+0.04 5		B(E2)(W.u.)=0.1 +3-10, B(M1)(W.u.)=0.094 18
1989.66	9/2-	0.18 ps +17-6	983.0 3	M1+E2	-4.5 5		B(E2)(W.u.)=8.×10¹ 8, B(M1)(W.u.)=0.0019 19
1989.66	9/2-	0.18 ps +17-6	1282.85 27	E2(+M3)	0.00 2		B(E2)(W.u.)=(3.×10¹ 3)
2118.6	5/2-	46 fs 12	1412.1 5	M1+E2	-0.08 5		B(E2)(W.u.)=0.5 7, B(M1)(W.u.)=0.09 3
2355.96	(11/2)-	0.06 ps 2	1158.37 18	M1+E2	-0.45 5		B(E2)(W.u.)=17 7, B(M1)(W.u.)=0.057 21
2355.96	(11/2)-	0.06 ps 2	1348.86 19	(E2)			B(E2)(W.u.)=1.1×10² 4
2455.55	9/2+	> 1.4 ps	1448.52 20	(E1+M2)	0.00 4		B(E1)(W.u.)<0.00011
E(level) (keV)	J^π(level)	T_1/2(level)	E(γ) (keV)	Multipolarity	Mixing Ratio	Conversion Coefficient	Additional Data
2878.7	(13/2)-	< 0.14 ps	1680.58 21	(E2)			B(E2)(W.u.)>23
3134.8	(15/2)-	160 ps 7	256.03 11	M1+E2	-0.07 2		B(E2)(W.u.)=1.2 7, B(M1)(W.u.)=0.0082 4
3269.26	(13/2)+	0.37 ps +21-11	813.73 15	(E2)			B(E2)(W.u.)=1.1×10² 7
3269.26	(13/2)+	0.37 ps +21-11	913.37 16	(E1+M2)	0.00 3		B(E1)(W.u.)=0.0011 7
4525.54	(17/2+)	0.29 ps 9	1256.27 19	(E2)			B(E2)(W.u.)=48 15
6187.1	(21/2+)	0.11 ps 4	1661.54 20	(E2)			B(E2)(W.u.)=31 12
8323.0	(25/2+)	< 0.14 ps	2135.9 3	(E2)			B(E2)(W.u.)>7.0

Q(β-)=-836.2 keV 5	S(n)= 7646.08 keV 4	S(p)= 10559.31 keV 21	Q(α)= -7320.2 keV 4
Reference: 2012WA38

References:
A	⁵⁷Mn β^- decay	B	⁵⁷Co ε decay
C	⁵⁷Fe(γ,γ): MOSSBAUER	D	⁴⁸Ca(¹³C,4nγ) E=25-65 MeV
E	⁵⁶Fe(n,n’γ)	F	⁵⁴Cr(α,nγ), (pol α,nγ)
G	⁵⁵Mn(t,nγ), ⁵⁶Fe(t,dγ):?	H	⁵⁵Mn(α,pnγ) E=25,28.6 MeV
I	⁵⁶Fe(n,γ), (pol n,γ) E=THERMAL	J	⁵⁶Fe(n,γ) E=1151.5 EV RES
K	⁵⁶Fe(d,p), ⁵⁷Fe(p,p’),	L	⁵⁶Fe(pol d,p) E=10 MeV
M	⁵⁶Fe(d,pγ) E=6 MeV	N	Coulomb Excitation
O	⁵⁸Fe(p,d), (d,t), (³He,α)	P	⁵⁹Co(μ^-,2nγ), (π^-,xγ),
Q	⁵⁸Ni(¹⁴C,¹⁵O) E=72 MeV	R	⁶⁰Ni(p,xγ), ⁶²Ni(p,xγ)

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	1/2-	STABLE
14.4129 6	A B C D E F G H I J K L M N O P R	3/2-	98.3 ns 3	14.4129 6	100	M1+E2	0.0	1/2-
136.4743 5	A B C D E F G H I J K L M N O P Q R	5/2-	8.7 ns 3	122.0614 4 136.4743 5	100 10 12.0 12	M1+E2 E2	14.4129 0.0	3/2- 1/2-
366.759 7	A B D E F G H I J K L M N O P Q R	3/2-	10.5 ps 14	230.29 2 352.36 1 366.75 1	9.2 11 100 11 17.7 20	(M1+E2) M1+E2 M1+E2	136.4743 14.4129 0.0	5/2- 3/2- 1/2-
706.416 16	A B D E F G H I J K M N O P R	5/2-	4.1 ps 11	339.54 18 569.92 4 692.03 2 706.4 2	1.7 3 11.0 13 100 11 5.7 24	M1+E2 M1+E2 M1+E2 [E2]	366.759 136.4743 14.4129 0.0	3/2- 5/2- 3/2- 1/2-
1007.13 4	A D E F H I K M	7/2-	0.13 ps 7	640.20 14 870.68 5 992.68 8	4.7 32 100.0 16 51.6 16	E2 M1+E2 E2	366.759 136.4743 14.4129	3/2- 5/2- 3/2-
1139.9 10 ?	J
1197.81 13	D E F H I K M	9/2-	2.9 ps 4	1061.60 17	100	E2	136.4743	5/2-
1265.52 13	A E I J K L M O P Q R	1/2-	82 fs 19	898.4 20 1250.6 22 1265.0 22	100 4.8 7 2.7 7		366.759 14.4129 0.0	3/2- 3/2- 1/2-
1356.83 18	D E F H I K L M	7/2-	0.18 ps 7	650.4 19 990.1 21 1342.7 22	100 43 7 40 5	M1+E2 E2 E2	706.416 366.759 14.4129	5/2- 3/2- 3/2-
1627.256 24	A E I J K L M	3/2-	56 fs 8	920.85 2 1260.60 3 1612.78 2 1627.05 8	14.1 16 46 5 100 11 3.9 5	M1+E2	706.416 366.759 14.4129 0.0	5/2- 3/2- 3/2- 1/2-
1725.38 3	A E I J K L M	3/2-	31 fs 4	460.1 4 1019.02 4 1358.71 6 1710.2 3 1725.09 6	0.48 17 27.6 29 14.3 16 4.0 9 100 11	M1+E2	1265.52 706.416 366.759 14.4129 0.0	1/2- 5/2- 3/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
1976.63 20	E I	(1/2-,3/2,5/2-)		251.1 3 1840.2 1976.4 11	25 100 24		1725.38 136.4743 0.0	3/2- 5/2- 1/2-
1989.66 20	D E F H	9/2-	0.18 ps +17-6	791.6 983.0 3 1282.85 27	66 78 100	M1+E2 E2(+M3)	1197.81 1007.13 706.416	9/2- 7/2- 5/2-
1991 5	K	1/2-,3/2-
2113.11 17	I	(1/2,3/2,5/2-)		849.5 5 2113.4 3	27 8 100 17		1265.52 0.0	1/2- 1/2-
2118.6 5	E K L M	5/2-	46 fs 12	1111.6 1412.1 5 2104.4 11	29 100 15 69 13	M1+E2	1007.13 706.416 14.4129	7/2- 5/2- 3/2-
2206.88 14	E I K L O	5/2-	10 fs 3	942.0 14 1199.9 1841 3 ? 2192.8 4 2206.8 6	8 4 42 100 19 84 22		1265.52 1007.13 366.759 14.4129 0.0	1/2- 7/2- 3/2- 3/2- 1/2-
2217.66 18	I K	(5/2+)		1851.3 4 2081.2 3 2202.7 8	46 10 77 17 100 32		366.759 136.4743 14.4129	3/2- 5/2- 3/2-
2220.2	E O	(7/2-)	> 0.3 ps	1853.3 2083.8 2205.8	10 94 100	(M1+E2)	366.759 136.4743 14.4129	3/2- 5/2- 3/2-
2330.41 16	I J	(1/2,3/2,5/2+)		703.4 4	100		1627.256	3/2-
2355.96 5	D E F H	(11/2)-	0.06 ps 2	1158.37 18 1348.86 19	41 4 100 10	M1+E2 (E2)	1197.81 1007.13	9/2- 7/2-
2358 12	K	1/2-,3/2-
2455.55 15	D E F H I M	9/2+	> 1.4 ps	1448.52 20	100	(E1+M2)	1007.13	7/2-
2456 5	K L	1/2+,7/2+,9/2+
2505.29 12	E I K L M	5/2+	78 fs 18	780.0 1798.1 3 2138.63 18 2368.6 3 2490.8 13	5 10 2 100 12 47 2 18 6		1725.38 706.416 366.759 136.4743 14.4129	3/2- 5/2- 3/2- 5/2- 3/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2564.22 21	I K L	3/2-		837.9 3 2562.4 5	100 17 57 16		1725.38 0.0	3/2- 1/2-
2574.5 4	E K M	(1/2,3/2,5/2-)	18 fs 4	2207.6 8 2574.4 4	38 15 100 13		366.759 0.0	3/2- 1/2-
2593.6 6	E	(3/2-,5/2-)	37 fs 10	1586.4 1887.1 2593.5	82 100 18		1007.13 706.416 0.0	7/2- 5/2- 1/2-
2599.4 3	I K	(1/2,3/2,5/2+)		2462.1 7 2598.1 11	100 17 43 15		136.4743 0.0	5/2- 1/2-
2697.17 17	E I J K L M Q	1/2-	6 fs 2	1991.0 10 2330.6 5 2682.5 3 2696.6 3	7 2 15 2 100 5 65 3		706.416 366.759 14.4129 0.0	5/2- 3/2- 3/2- 1/2-
2758.30 11	I K			1492.4 4 2391.80 20	27 5 100 14		1265.52 366.759	1/2- 3/2-
2821.07 23	E I K	(1/2,3/2,5/2+)	60 fs +20-10	603.54 19 1812.9 5	100 16 44 13		2217.66 1007.13	(5/2+) 7/2-
2835.89 7	E I J K	3/2,5/2		723.0 20 1828.9 10 2129.48 9 2469.17 16 2821.5 6 2835.43 19	1.5 15 4.5 30 100 11 90 17 15 3 37 6		2113.11 1007.13 706.416 366.759 14.4129 0.0	(1/2,3/2,5/2-) 7/2- 5/2- 3/2- 3/2- 1/2-
2855.0 4	I K
2878.7 4	D E F H	(13/2)-	< 0.14 ps	1680.58 21	100	(E2)	1197.81	9/2-
2904.28 24	E I			2198.2 5 2537.1 5	100 26 47 13		706.416 366.759	5/2- 3/2-
2921.20 10	I K L M	1/2-,3/2-	33 fs 6	1655.37 19 2216.2 5 2554.3 5 2906.0 4 2920.5 4	42 3 31 3 45 4 100 9		1265.52 706.416 366.759 14.4129 0.0	1/2- 5/2- 3/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
2970.89 22	I J K	(1/2,3/2,5/2+)		2603.1 15	100		366.759	3/2-
2987.95 15	I K	(1/2,3/2,5/2+)		657.56 9 1722.40 13 2618.9 9	76 12 100 14 15 6		2330.41 1265.52 366.759	(1/2,3/2,5/2+) 1/2- 3/2-
3059.1 3	E I K	1/2+		2691.6 5 2922.5 10	50 16 100 10		366.759 136.4743	3/2- 5/2-
3098.95 15	I K			2091.85 16	100		1007.13	7/2-
3110 5	K
3122.76 21	I K			2755.90 21	100		366.759	3/2-
3134.8 4	D F H	(15/2)-	160 ps 7	256.03 11	100	M1+E2	2878.7	(13/2)-
3182.77 20	I J K	1/2-,3/2-		211.87 9 977.1 7 1457.4 5 1825.9 3 2815.0 6 3166.9 11	50 8 31 19 25 7 56 14 56 14 100 82		2970.89 2206.88 1725.38 1356.83 366.759 14.4129	(1/2,3/2,5/2+) 5/2- 3/2- 7/2- 3/2- 3/2-
3205.6 5	I K O	5/2-,7/2-		988.2 5	100		2217.66	(5/2+)
3239.89 12	I J K M	1/2+		735.1 3 1022.0 3 1263.3 3 2873.7 3 3103.1 4 3225.3 4 3239.30 20	6.0 16 7.5 17 14.9 21 55 6 100 15 45 9 52 7		2505.29 2217.66 1976.63 366.759 136.4743 14.4129 0.0	5/2+ (5/2+) (1/2-,3/2,5/2-) 3/2- 5/2- 3/2- 1/2-
3269.26 13	D F H	(13/2)+	0.37 ps +21-11	813.73 15 913.37 16	49 3 100 3	(E2) (E1+M2)	2455.55 2355.96	9/2+ (11/2)-
3284 5	K
3301.77 10	I K	(5/2-,7/2-)		1674.62 13 2104.5 5 2935.8 8	57 15 100 24 36 15		1627.256 1197.81 366.759	3/2- 9/2- 3/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3322.48 11	I K	1/2-,3/2-		564.19 6 1115.64 15 1345.2 5 1965.3 2	76 8 31 5 21 4 100 14		2758.30 2206.88 1976.63 1356.83	5/2- (1/2-,3/2,5/2-) 7/2-
3336.59 25	I			2970.0 3	100		366.759	3/2-
3340.33 18	I			884.78 10	100		2455.55	9/2+
3345	K	7/2+,9/2+
3371.11 16	I J K L Q	3/2-		1041.1 5 1646.0 3 3356.3 2	9 3 21 4 100 12		2330.41 1725.38 14.4129	(1/2,3/2,5/2+) 3/2- 3/2-
3427.68 8	I J K L M Q	3/2-	3.0 fs +6-29	2721.17 9 3060.90 17 3291.1 2 3414.3 13	85 9 9.3 16 19 4 100 11		706.416 366.759 136.4743 14.4129	5/2- 3/2- 5/2- 3/2-
3452 5	K
3473 5	K	5/2-,7/2-
3513.8 4	D	(17/2)	< 0.14 ps	379.06 13	100		3134.8	(15/2)-
3535 5	K	7/2+,9/2+
3535.92 18	I			1810.51 17	100		1725.38	3/2-
3548 5	K	7/2+,9/2+
3561.34 12	I			803.09 8 1447.0 3	100 11 38 10		2758.30 2113.11	(1/2,3/2,5/2-)
3608 5	K	7/2+,9/2+
3608.51 21	I			1982.1 4	100		1627.256	3/2-
3661 5	K
3752 5	K	7/2+,9/2+
3784 10	K	7/2+,9/2+
3791.59 9	I J	3/2+		1460.9 3 1584.6 3 2066.17 12 2164.69 18 2526.2 3 3776.6 2 3791.7 10 ?	16.3 26 14.3 25 100 12 41 6 59 14 16 6 33		2330.41 2206.88 1725.38 1627.256 1265.52 14.4129 0.0	(1/2,3/2,5/2+) 5/2- 3/2- 3/2- 1/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
3827 10	K	5/2-,7/2-
3862.42 19	I			1655.51 12	100		2206.88	5/2-
3881 10	K
3902 10	K	5/2-,7/2-
3926.0 20	J	(1/2,3/2,5/2-)
3936.1 7	I K	5/2-,7/2-		3921.5 7	100		14.4129	3/2-
3981.18 24	I K L M	3/2-	7 fs 12	1159.5 13 1284.0 5 1381.7 2 3615.3 11 3981.7 4	15 8 77 39 100 13 77 17		2821.07 2697.17 2599.4 366.759 0.0	(1/2,3/2,5/2+) 1/2- (1/2,3/2,5/2+) 3/2- 1/2-
4042.60 24	I K	5/2-,7/2-		2415.1 3	100		1627.256	3/2-
4081 10	K
4093 10	K
4136.62 10	I	(1/2,3/2,5/2+)		575.09 19 834.91 8 1077.3 3 1215.38 5 1282.3 6 1300.9 4 1931.8 7	90 48 100 11 19 5 48 11 43 20 43 10 29 10		3561.34 3301.77 3059.1 2921.20 2855.0 2835.89 2206.88	(5/2-,7/2-) 1/2+ 1/2-,3/2- 3/2,5/2 5/2-
4138.57 18	K L M	5/2+	15 fs 8	1632.94 16 2783.8 5 3774.0 8 4002.4 9	100 6 81 15 22 5 17 4		2505.29 1356.83 366.759 136.4743	5/2+ 7/2- 3/2- 5/2-
4144.3 5	I	(1/2,3/2,5/2+)		2517.0 5	100		1627.256	3/2-
4209.59 12	I K	(3/2)-		601.3 2 1026.4 3 1110.9 3 1305.3 3 1705.0 8 2097 2 2582.0 3 2943.4 5 3842.4 3 4073.3 3 4194.8 4 4210.2 10	48 8 17 4 17 4 24 7 38 8 17 10 31 8 28 7 100 12 72 10 45 11 24 7		3608.51 3182.77 3098.95 2904.28 2505.29 2113.11 1627.256 1265.52 366.759 136.4743 14.4129 0.0	1/2-,3/2- 5/2+ (1/2,3/2,5/2-) 3/2- 1/2- 3/2- 5/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4239 10	K	3/2+,5/2+
4316 10	K	7/2+,9/2+
4363 10	K	5/2-,7/2-
4378.68 21	I	(1/2,3/2,5/2-)		335.9 3 1006.9 5 1255.5 8 2654.3 4 4378.3 4	25 7 19 7 13 7 31 13 100 16		4042.60 3371.11 3122.76 1725.38 0.0	5/2-,7/2- 3/2- 3/2- 1/2-
4379.44 19	J K L M	(1/2,3/2,5/2-)	3 fs 4	1458.09 21 1681.3 5 4013.6 4	22 3 12 4 100 9		2921.20 2697.17 366.759	1/2-,3/2- 1/2- 3/2-
4432.4 8	D F		< 0.14 ps	1297.8 5	100		3134.8	(15/2)-
4459.70 14	I K Q	5/2-,7/2-		1119.8 6 1351.8 10 1700.8 3 2348.9 9 2734.2 3 2832.46 18	3.8 19 9.4 39 21 4 11 6 28 5 100 13		3340.33 3110 2758.30 2113.11 1725.38 1627.256	(1/2,3/2,5/2-) 3/2- 3/2-
4492	K L	5/2+
4525	K	7/2+,9/2+
4525.54 23	D F H	(17/2+)	0.29 ps 9	1256.27 19	100	(E2)	3269.26	(13/2)+
4544 10	K	1/2+
4572.8 5	I K	1/2+		1973.4 4	100		2599.4	(1/2,3/2,5/2+)
4597.4 3	I K L M	5/2+	5 fs 8	2033.2 2 2870.8 11	100		2564.22 1725.38	3/2- 3/2-
4652 10	K	5/2-,7/2-
4680 10	K
4691.75 15	I K	(5/2+)		1355.6 4 1369.1 2 1487.2 9 1836.4 4 1855.9 4 2186.4 4 2486.0 6 4555.3 3	100 25 100 18 23 8 46 9 46 9 31 8 62 17 69 17		3336.59 3322.48 3205.6 2855.0 2835.89 2505.29 2206.88 136.4743	1/2-,3/2- 5/2-,7/2- 3/2,5/2 5/2+ 5/2- 5/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
4719 10	K
4753 10	K	5/2-,7/2-
4771 10	K	3/2+,5/2+
4823.9 5	K L M		< 10 fs	1584.0 4	100		3239.89	1/2+
4902 10	K
4922.9 7	K L M	5/2+	7 fs 10	2418.3 10 3565.4 8	100 13 70 9		2505.29 1356.83	5/2+ 7/2-
4970 20	O	(5/2-,7/2-)
4976 10	K	3/2+,5/2+
5019 10	K	5/2-,7/2-
5064 10	K L	(1/2+)&(7/2-)
5085 10	K
5099	K
5115 10	K	1/2+
5140.25 20	I K L	(1/2,3/2,5/2+)		1899.5 5 2574.3 3 3027.55 15	55 20 100 21 100 14		3239.89 2564.22 2113.11	1/2+ 3/2- (1/2,3/2,5/2-)
5178.44 25	I K	1/2+		1197.27 7 2480.2 6 5042.1 8	100 11 17 6 50 15		3981.18 2697.17 136.4743	3/2- 1/2- 5/2-
5195	K
5221.6 3	I K	(1/2-,3/2,5/2+)		2385.3 4 3014.7 3 4856.6 13	75 18 100 19 83 34		2835.89 2206.88 366.759	3/2,5/2 5/2- 3/2-
5238.7 4	I K	(1/2,3/2,5/2+)
5250	K	1/2+
5271 10	K	1/2+
5289	K L O	5/2+
5334	K	7/2+,9/2+
5362.1 9	K L M	5/2+	6 fs +15-6	2856.7 9	100		2505.29	5/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
5404 10	K
5422 10	K	3/2+,5/2+
5445 10	K	7/2+,9/2+
5472 10	K	3/2+,5/2+
5500 10	K	1/2+
5512 10	K
5525 10	K	1/2+
5545	K
5564 10	K	3/2+,5/2+
5590 10	K
5623 10	K
5641 10	K
5675 10	K
5688 10	K
5721 10	K	1/2+&(7/2+,9/2+)
5737 10	K	1/2+
5769 10	K
5802 10	K	3/2+,5/2+
5825	K	3/2+,5/2+
5844	K	1/2+
5864	K	3/2+,5/2+
5900	K
5918	K
5936	K
5956	K	3/2+,5/2+
5983	K	3/2+ TO (9/2+)
6025	K	3/2+,5/2+
6044	K	3/2+,5/2+
6083	K
6103	K	7/2+,9/2+
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
6130	K	1/2+
6148	K
6171	K	3/2+,5/2+
6187.1 3	D H	(21/2+)	0.11 ps 4	1661.54 20	100 10	(E2)	4525.54	(17/2+)
6194	K	7/2+,9/2+
6212	K	1/2+
6230	K	3/2+,5/2+
6252	K	7/2+,9/2+
6270	K	7/2+,9/2+
6305	K
6323	K
6340	K
6370	K	3/2+,5/2+
6408	K	3/2+,5/2+
6427	K	3/2+,5/2+
6496	K
6512	K	3/2+,5/2+
6542	K	1/2+
6571	K	3/2+,5/2+
6589	K	3/2+,5/2+
6640	K	3/2+,5/2+
6672	K	3/2+,5/2+
6703	K	3/2+,5/2+
6725	K
7646.7 7	J	1/2-		3267.0 20 ? 3721.3 20 ? 3854.3 35 4217.9 25 4276.5 30 4408.0 30 4463.5 20 4810.0 30 ? 4950.1 20 5920.8 30 6017.8 30 6381.8 20 6507.0 10 ? 7279.6 30 7508.8 20 7631.7 20 7645.5 20	1.9 10 1.9 12 1.9 11 1.2 8 1.7 8 1.3 8 5.5 10 1.5 10 5.0 14 5.6 13 1.1 5 35 5 <1.0 1.9 7 5.2 8 100 4 41 4	E1 M1,E2 M1,E2 E1 M1,E2 M1 M1,E2 M1,E2 M1 M1,E2 E2 M1,E2 M1	4379.44 3926.0 3791.59 3427.68 3371.11 3239.89 3182.77 2835.89 2697.17 1725.38 1627.256 1265.52 1139.9 366.759 136.4743 14.4129 0.0	(1/2,3/2,5/2-) (1/2,3/2,5/2-) 3/2+ 3/2- 3/2- 1/2+ 1/2-,3/2- 3/2,5/2 1/2- 3/2- 3/2- 1/2- 3/2- 5/2- 3/2- 1/2-
E(level) (keV)	XREF	J^π(level)	T_1/2(level)	E(γ) (keV)	I(γ)	M(γ)	Final Levels
8323.0 5	D H	(25/2+)	< 0.14 ps	2135.9 3	100 17	(E2)	6187.1	(21/2+)
10.45E+3 5 ?	O	(7/2-)

E(level)	J^π(level)	T_1/2(level)	Comments
0.0	1/2-	STABLE	μ=+0.09044 7 (1989Ra17), T=5/2 Small spectroscopic factor in (d,p) implies that ⁵⁷Fe g.s. is deformed (1973De23).
1007.13	7/2-	0.13 ps 7	T_1/2(level): From DSAM in (α,pnγ).
1139.9			Based on existence of primary γ in res (n,γ).
1265.52	1/2-	82 fs 19	J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
1356.83	7/2-	0.18 ps 7	T_1/2(level): From DSAM in (α,pnγ).
1627.256	3/2-	56 fs 8	J^π(level): L(n)=1 in (d,p). J\|=1/2 from γγ(θ) in (n,γ) E=thermal and CP in (pol n,γ) E=thermal.
1725.38	3/2-	31 fs 4	J^π(level): L(n)=1 in (d,p). J\|=1/2 from γγ(θ) in (n,γ) E=thermal and CP in (pol n,γ) E=thermal.
1989.66	9/2-	0.18 ps +17-6	T_1/2(level): From DSAM in (n,n’γ).
2118.6	5/2-	46 fs 12	J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From DSAM in (n,n’γ).
2206.88	5/2-	10 fs 3	T_1/2(level): From DSAM in (n,n’γ).
2220.2	(7/2-)	> 0.3 ps	T_1/2(level): From DSAM in (n,n’γ).
2355.96	(11/2)-	0.06 ps 2	T_1/2(level): From DSAM in (α,pnγ).
2455.55	9/2+	> 1.4 ps	T_1/2(level): From DSAM in (α,pnγ).
2505.29	5/2+	78 fs 18	J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
2564.22	3/2-		E(level): From (α,nγ). J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
2593.6	(3/2-,5/2-)	37 fs 10	T_1/2(level): From DSAM in (n,n’γ).
2697.17	1/2-	6 fs 2	E(level): From ⁵⁷Mn β^- decay. J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
2821.07	(1/2,3/2,5/2+)	60 fs +20-10	T_1/2(level): From DSAM in (n,n’γ).
2921.20	1/2-,3/2-	33 fs 6	E(level): From ⁵⁷Mn β^- decay. T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
3098.95			L(n)=2⁺4 doublet in (d,p). E(level): L(n)=2⁺4 doublet in (d,p).
3269.26	(13/2)+	0.37 ps +21-11	E(level): ΔJ=2 POSITIVE-PARITY band. T_1/2(level): From DSAM in (α,pnγ).
3371.11	3/2-		E(level): From (α,nγ). J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
3427.68	3/2-	3.0 fs +6-29	E(level): From (α,nγ). J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
3535	7/2+,9/2+		L(n)=4 in (d,p) inconsistent with 1811γ to 3/2- state. Therefore, state observed in (n,γ) is probably different.
3535.92			See comment on preceding state.
E(level)	J^π(level)	T_1/2(level)	Comments
3981.18	3/2-	7 fs 12	E(level): From ⁵⁷Mn β^- decay. From (α,nγ). J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
4138.57	5/2+	15 fs 8	E(level): From ⁵⁷Mn β^- decay. J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
4379.44	(1/2,3/2,5/2-)	3 fs 4	E(level): From ⁵⁷Mn β^- decay. T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
4492	5/2+		J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
4525.54	(17/2+)	0.29 ps 9	E(level): ΔJ=2 POSITIVE-PARITY band.
4597.4	5/2+	5 fs 8	E(level): From ⁵⁷Mn β^- decay. J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
4823.9		< 10 fs	Jπ=(1/2⁺) & (3/2⁺) from analyzing power(θ) and σ(θ) in (pol d,p) based on empirical curves. Data clearly show this level to be a doublet. E(level): Jπ=(1/2⁺) & (3/2⁺) from analyzing power(θ) and σ(θ) in (pol d,p) based on empirical curves. Data clearly show this level to be a doublet. From ⁵⁷Mn β^- decay. T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
4922.9	5/2+	7 fs 10	E(level): From ⁵⁷Mn β^- decay. J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
4970	(5/2-,7/2-)		E(level): From ε decay. J^π(level): From angular momentum transfer in (p,d) and (d,p) and Coulomb excitation.
5289	5/2+		J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
5362.1	5/2+	6 fs +15-6	E(level): From ⁵⁷Mn β^- decay. J^π(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p). T_1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
6187.1	(21/2+)	0.11 ps 4	E(level): ΔJ=2 POSITIVE-PARITY band. T_1/2(level): From DSAM in (α,pnγ).
7646.7	1/2-		γΓ_nΓ_γ/Γ=68.7 meV 15; σ₀Γ_γ=161 b×eV 4 from 1983Ma13; not consistent with 1981MuZQ. E(level): γΓ_nΓ_γ/Γ=68.7 meV 15; σ₀Γ_γ=161 b×eV 4 from 1983Ma13; not consistent with 1981MuZQ.
8323.0	(25/2+)	< 0.14 ps	E(level): ΔJ=2 POSITIVE-PARITY band.
10.45E+3	(7/2-)		IAS?(⁵⁷Mn) from ⁵⁸Fe(p,d). E(level): IAS?(⁵⁷Mn) from ⁵⁸Fe(p,d).

E(level)	E(gamma)	Comments
14.4129	14.4129	E(γ): from ε decay. From ε decay I(γ): From ε decay M(γ): from Γ and adopted Jπ. See also 1984Pl05.
136.4743	122.0614	E(γ): Recommended γ-ray calibration energy from ε decay.
136.4743	136.4743	E(γ): Recommended γ-ray calibration energy from ε decay. M(γ): Q from γ(θ,H,t) in ε decay and Coulomb excitation; E2 from RUL
366.759	230.29	M(γ): D+Q from γ(θ) in Coul. ex. and ε decay; and ΔJπ
1007.13	640.20	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ) M(γ): From comparison to RUL and ΔJπ
	870.68	E(γ): From ⁵⁷Mn β^- decay I(γ): From (¹³C,4nγ)
	992.68	E(γ): From ⁵⁷Mn β^- decay I(γ): From (¹³C,4nγ) M(γ): From comparison to RUL and ΔJπ
1197.81	1061.60	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ) M(γ): From comparison to RUL and ΔJπ
1265.52	898.4	E(γ): From γ-inelastic scattering I(γ): From γ-inelastic scattering
	1250.6	E(γ): From γ-inelastic scattering I(γ): From γ-inelastic scattering
	1265.0	E(γ): From γ-inelastic scattering I(γ): From γ-inelastic scattering
1356.83	650.4	E(γ): From γ-inelastic scattering I(γ): From γ-inelastic scattering
	990.1	E(γ): From γ-inelastic scattering I(γ): From γ-inelastic scattering M(γ): From comparison to RUL and ΔJπ
	1342.7	E(γ): From γ-inelastic scattering I(γ): From γ-inelastic scattering M(γ): From comparison to RUL and ΔJπ
1976.63	251.1	I(γ): From (n,n’γ)
	1840.2	E(γ): From (n,n’γ) I(γ): From (n,n’γ)
	1976.4	I(γ): From (n,n’γ)
1989.66	791.6	E(γ): From (α,pnγ) I(γ): From (n,n’γ)
	983.0	E(γ): From (¹³C,4nγ) I(γ): From (n,n’γ) M(γ): D+Q from γ(θ) in (n,n’γ); M1⁺E2 from RUL. From γ(θ) in (α,nγ) and (pol α,nγ) and final Jπ
	1282.85	E(γ): From (¹³C,4nγ) I(γ): intensity ratios for these three gammas from (n,n’γ) do not agree with results from (α,pnγ) indicating that a different level is being populated in (n,n’γ) compared to other reactions.. From (n,n’γ) M(γ): Q(+O) from γ(θ) in (n,n’γ); E2(+M3) from RUL
2118.6	1111.6	E(γ): from (n,n’γ); added 0.75 to conform to (d,pγ) energy scale I(γ): From (n,n’γ)
	1412.1	E(γ): From (d,pγ) I(γ): From (d,pγ) M(γ): D+Q from γ(θ) in (n,n’γ); M1⁺E2 from RUL
	2104.4	E(γ): From (d,pγ) I(γ): From (d,pγ)
2206.88	1199.9	E(γ): From (n,n’γ) I(γ): From (n,n’γ)
2206.88	1841	E(γ): From γ-inelastic scattering
E(level)	E(gamma)	Comments
2220.2	2083.8	M(γ): from γ(θ) in (n,n’γ) and ΔJπ.
2355.96	1158.37	E(γ): From (¹³C,4nγ) I(γ): consistent with Iγ=43 in (α,nγ), but not with Iγ=92 in (¹³C,4nγ) or Iγ=67 in (n,n’γ). From (α,pnγ)
2355.96	1348.86	E(γ): From (¹³C,4nγ) I(γ): From (α,pnγ) M(γ): From comparison to RUL and ΔJπ
2455.55	1448.52	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ) M(γ): M1⁺E2 (1978Kr19); disagrees with the adopted decay scheme
2505.29	780.0	E(γ): From (n,n’γ) I(γ): From (n,n’γ)
	1798.1	E(γ): From (d,pγ) I(γ): From (d,pγ)
	2368.6	E(γ): From (d,pγ) I(γ): From (d,pγ)
2574.5	2207.6	E(γ): From (d,pγ) I(γ): From (d,pγ)
2574.5	2574.4	E(γ): From (d,pγ) I(γ): From (d,pγ)
2593.6	1586.4	E(γ): From (n,n’γ) I(γ): From (n,n’γ)
	1887.1	E(γ): From (n,n’γ) I(γ): From (n,n’γ)
	2593.5	E(γ): From (n,n’γ) I(γ): From (n,n’γ)
2697.17	2330.6	E(γ): From (d,pγ) I(γ): From (d,pγ)
2697.17	2696.6	I(γ): From (d,pγ)
2878.7	1680.58	E(γ): From (α,nγ) I(γ): From (α,nγ) M(γ): from comparison to RUL and γ(θ) in (¹³C,4nγ)
2921.20	1655.37	E(γ): From (d,pγ) I(γ): From (d,pγ)
	2554.3	E(γ): From (d,pγ) I(γ): From (d,pγ)
	2906.0	E(γ): From (d,pγ) I(γ): From (d,pγ)
	2920.5	E(γ): From (d,pγ) I(γ): From (d,pγ)
3134.8	256.03	E(γ): From (¹³C,4nγ) M(γ): D+Q from γ(θ) in (α,nγ); M1⁺E2 from RUL
3269.26	813.73	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ) M(γ): Q from γ(θ) in (¹³C,4nγ); E2 from RUL
3269.26	913.37	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ) M(γ): M1⁺E2 (1978Kr19); disagrees with the adopted decay scheme. From γ(θ) in (α,nγ) and (pol α,nγ) and final Jπ
3513.8	379.06	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ)
3981.18	3615.3	E(γ): From (d,pγ)
4138.57	1632.94	E(γ): From (d,pγ) I(γ): From (d,pγ)
	2783.8	E(γ): From (d,pγ) I(γ): From (d,pγ)
	3774.0	E(γ): From (d,pγ) I(γ): From (d,pγ)
	4002.4	E(γ): From (d,pγ) I(γ): From (d,pγ)
E(level)	E(gamma)	Comments
4379.44	1458.09	E(γ): From (d,pγ) I(γ): From (d,pγ)
	1681.3	E(γ): From (d,pγ) I(γ): From (d,pγ)
	4013.6	E(γ): From (d,pγ) I(γ): From (d,pγ)
4432.4	1297.8	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ)
4525.54	1256.27	E(γ): From (¹³C,4nγ) I(γ): From (¹³C,4nγ) M(γ): Stretched-quadrupole radiation pattern in (¹³C,4nγ)
4597.4	2870.8	E(γ): From (d,pγ)
4823.9	1584.0	E(γ): From (d,pγ)
4922.9	2418.3	E(γ): From (d,pγ) I(γ): From (d,pγ)
4922.9	3565.4	E(γ): From (d,pγ) I(γ): From (d,pγ)
5362.1	2856.7	E(γ): From (d,pγ) I(γ): From (d,pγ)
6187.1	1661.54	E(γ): From (¹³C,4nγ) I(γ): From (α,pnγ) M(γ): Stretched-quadrupole radiation pattern in (¹³C,4nγ)
7646.7	3854.3	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	4217.9	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	4276.5	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	4408.0	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	4463.5	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	4950.1	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	5920.8	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	6017.8	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	6381.8	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	7279.6	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	7508.8	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	7631.7	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
	7645.5	M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
8323.0	2135.9	E(γ): From (¹³C,4nγ) I(γ): From (α,pnγ) M(γ): Stretched-quadrupole radiation pattern in (¹³C,4nγ)