ADOPTED LEVELS, GAMMAS for 56Fe
Authors: Huo Junde, Huo Su, Yang Dong | Citation: Nucl. Data Sheets 112, 1513 (2011) | Cutoff date: 29-Oct-2009
Full ENSDF file | Adopted Levels (PDF version)
Q(β-)=-4566.6 keV 5 | S(n)= 11197.10 keV 23 | S(p)= 10183.67 keV 16 | Q(α)= -7613.3 keV 4 | ||
Reference: 2012WA38 |
E(level): From 55Mn(p,p), (p,γ) E=res: IAR, except as noted. For resonance states E(level) are calculated by using E(level)=S(p)+0.9824×E(p), where E(p) is incident proton energy in lab system and S(p)=10183.74 17 (2003Au03); States of E(level)>13000 are unplaced in adopted levels, see 56Fe(e,e’), (3He,3He’), (α,α’), and 60Ni(p,Xγ),(e,e’αγ),(γ,α).
T1/2(level): From ΔS(a) measurement in 56Fe(n,n’γ), except as noted.
E(γ): From 56Fe(n,n’γ), except as noted. For resonance states primary γ’s are unplaced in adopted levels, see 55Mn(p,p), (p,γ) E=res: IAR.
I(γ): Relative photon branching from each level renormalized to 100 for the strongest branching; values from 56Fe(n,n’γ), except as noted.
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
846.7778 | 2+ | 6.07 ps 23 | 846.7638 19 | E2 | B(E2)(W.u.)=16.8 7 | ||
2085.1045 | 4+ | 0.64 ps 12 | 1238.2736 22 | E2 | B(E2)(W.u.)=24 5 | ||
2657.5894 | 2+ | 21 fs 1 | 1810.757 4 | M1+E2 | -0.18 1 | B(E2)(W.u.)=3.3 4, B(M1)(W.u.)=0.166 8 | |
2941.50 | 0+ | 0.45 ps +21-12 | 2094.9 3 | [E2] | B(E2)(W.u.)=2.4 +7-12 | ||
2959.972 | 2+ | 28 fs 3 | 2113.135 5 | M1+E2 | +0.27 3 | B(E2)(W.u.)=2.5 6, B(M1)(W.u.)=0.076 9 | |
3122.970 | 4+ | 47 fs 12 | 1037.8333 24 | M1(+E2) | 0.00 5 | B(M1)(W.u.)=(0.42 11) | |
4+ | 47 fs 12 | 2276.131 4 | E2 | B(E2)(W.u.)=0.13 4 | |||
3369.95 | 2+ | 17 fs 3 | 2523.06 5 | M1+E2 | +0.25 15 | B(E2)(W.u.)=1.3 +15-13, B(M1)(W.u.)=0.065 13 | |
3388.55 | 6+ | 2.9 ps 2 | 1303.4 1 | E2 | B(E2)(W.u.)=4.0 4 | ||
3445.348 | 3+ | 29 fs 5 | 787.743 5 | M1+E2 | +0.85 35 | B(E2)(W.u.)=30 16, B(M1)(W.u.)=0.013 5 | |
3+ | 29 fs 5 | 1360.212 4 | M1+E2 | -0.11 1 | B(E2)(W.u.)=0.79 20, B(M1)(W.u.)=0.060 11 | ||
3+ | 29 fs 5 | 2598.500 4 | M1+E2 | -0.28 2 | B(E2)(W.u.)=0.74 16, B(M1)(W.u.)=0.031 6 | ||
3755.57 | 6+ | 0.13 ps 2 | 367.0 1 | M1+E2 | +0.07 12 | 0.00141 | B(E2)(W.u.)=4.×101 +16-4, B(M1)(W.u.)=0.61 10, α=0.00141 8, α(K)=0.00125 7, α(L)=0.00012 |
6+ | 0.13 ps 2 | 1670.8 4 | E2 | B(E2)(W.u.)=21 4 | |||
3856.495 | 3+ | 25 fs 3 | 733.514 4 | M1 | B(M1)(W.u.)=0.025 4 | ||
3+ | 25 fs 3 | 1771.357 4 | M1(+E2) | -0.004 +5-2 | B(E2)(W.u.)=(0.0015 +38-15), B(M1)(W.u.)=(0.145 18) | ||
3+ | 25 fs 3 | 3009.645 4 | M1+E2 | +0.065 5 | B(E2)(W.u.)=0.0018 4, B(M1)(W.u.)=0.00190 24 | ||
4048.888 | 3+ | 7 fs 3 | 1088.894 9 | M1+E2 | +0.43 12 | B(E2)(W.u.)=9 6, B(M1)(W.u.)=0.028 13 | |
3+ | 7 fs 3 | 1963.741 8 | M1+E2 | +0.22 3 | B(E2)(W.u.)=1.8 9, B(M1)(W.u.)=0.07 3 | ||
3+ | 7 fs 3 | 3202.029 8 | M1+E2 | +0.50 1 | B(E2)(W.u.)=3.1 14, B(M1)(W.u.)=0.06 3 | ||
4100.363 | 4+ | 43 fs 5 | 977.372 5 | M1(+E2) | +0.07 +3-2 | B(E2)(W.u.)=(0.6 6), B(M1)(W.u.)=(0.061 8) | |
4+ | 43 fs 5 | 2015.215 5 | M1+E2 | +0.68 5 | B(E2)(W.u.)=2.3 4, B(M1)(W.u.)=0.0102 13 | ||
4+ | 43 fs 5 | 3253.503 4 | E2 | B(E2)(W.u.)=1.76 21 | |||
4119.936 | 3+ | 0.14 ps 4 | 996.948 5 | M1+E2 | B(E2)(W.u.)=3.8 11 | ||
3+ | 0.14 ps 4 | 1159.944 6 | M1+E2 | +0.064 +16-36 | B(E2)(W.u.)=0.006 4, B(M1)(W.u.)=0.0010 3 | ||
3+ | 0.14 ps 4 | 2034.791 5 | M1+E2 | -0.073 5 | B(E2)(W.u.)=0.038 12, B(M1)(W.u.)=0.015 5 | ||
3+ | 0.14 ps 4 | 3273.079 4 | M1+E2 | +0.420 4 | B(E2)(W.u.)=0.023 7, B(M1)(W.u.)=0.00068 20 | ||
E(level) (keV) | Jπ(level) | T1/2(level) | E(γ) (keV) | Multipolarity | Mixing Ratio | Conversion Coefficient | Additional Data |
4298.096 | 4+ | 110 fs 50 | 1175.101 4 | M1+E2 | +0.14 4 | B(E2)(W.u.)=2.1 16, B(M1)(W.u.)=0.07 4 | |
4+ | 110 fs 50 | 2212.948 4 | M1+E2 | -3.0 10 | B(E2)(W.u.)=0.7 4, B(M1)(W.u.)=0.00019 15 | ||
4+ | 110 fs 50 | 3451.232 4 | E2 | B(E2)(W.u.)=0.21 10 | |||
4394.93 | 3+ | 35 fs 17 | 3548.05 6 | M1+E2 | -0.30 2 | B(E2)(W.u.)=0.17 9, B(M1)(W.u.)=0.012 6 | |
4700.63 | 7+ | 0.083 ps +82-14 | 1312.2 1 | M1+E2 | -0.08 8 | B(E2)(W.u.)=0.7 +15-7, B(M1)(W.u.)=0.0981 13 | |
5255.7 | 8+ | 0.35 ps 4 | 1499.5 3 | E2 | B(E2)(W.u.)=4.7 7 | ||
8+ | 0.35 ps 4 | 1866.8 3 | E2 | B(E2)(W.u.)=4.0 6 | |||
5626.84 | 8+ | 0.069 ps +21-14 | 926.2 1 | M1+E2 | +0.25 10 | B(E2)(W.u.)=5.×101 4, B(M1)(W.u.)=0.332 16 | |
8+ | 0.069 ps +21-14 | 1871.3 | E2 | B(E2)(W.u.)=1.2 12 | |||
8+ | 0.069 ps +21-14 | 2238 2 | E2 | B(E2)(W.u.)=0.9 +3-4 | |||
9140.3 | 1- | 1.28 eV 17 | 9139.5 6 | E1 | B(E1)(W.u.)=0.0016983 4 |
Additional Level Data and Comments:
E(level) | Jπ(level) | T1/2(level) | Comments |
846.7778 | 2+ | 6.07 ps 23 | Q=-0.19 8 (2005St24), μ=1.22 16 (2005St24), G=+0.504 63 (2009Ea01) XREF: F(850)J(850)K(840)M(850)R(850)X(850)Y(840). E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
2085.1045 | 4+ | 0.64 ps 12 | XREF: F(2090)J(2090)K(2078)X(2100)Z(2090). E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
2657.5894 | 2+ | 21 fs 1 | XREF: M(2650)R(2650). E(level): From 56Co ε decay. From 54Fe(α,2pγ). From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
2941.50 | 0+ | 0.45 ps +21-12 | XREF: F(2950). |
2959.972 | 2+ | 28 fs 3 | XREF: O(2950)Z(2970). E(level): From 56Co ε decay. From 54Fe(α,2pγ). From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
3076.2 | (3-) | XREF: M(3100)W(3100). E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
3120.11 | (1+) | 19 fs 1 | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
3122.970 | 4+ | 47 fs 12 | XREF: Z(3150). E(level): From 56Co ε decay. From 54Fe(α,2pγ). From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
3369.95 | 2+ | 17 fs 3 | XREF: K(3375). E(level): From 56Co ε decay. From 54Fe(α,2pγ). From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
3388.55 | 6+ | 2.9 ps 2 | XREF: Z(3400). |
3445.348 | 3+ | 29 fs 5 | E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
3600.21 | (1,2+) | < 59 fs | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. |
3605.69 | 2+ | 0.15 ps 4 | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
3610.21 | 0(+) | 52 fs 21 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. |
3744.13 | 2+ | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
3759.6 | XREF: Z(3780). | ||
3829.77 | 2+ | 39 fs 5 | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
3856.495 | 3+ | 25 fs 3 | E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
4048.888 | 3+ | 7 fs 3 | XREF: Z(4080). E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
4085.93 | (1,2+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
4100.363 | 4+ | 43 fs 5 | E(level): From 56Co ε decay. From 54Fe(α,2pγ). From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
4119.936 | 3+ | 0.14 ps 4 | E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
4298.096 | 4+ | 110 fs 50 | E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
4302.0 | 0+ | E(level): From 56Fe(n,n’γ). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
4368.13 | 3- | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
4394.93 | 3+ | 35 fs 17 | E(level): From 54Fe(α,2pγ). From 56Co ε decay. |
4401.27 | 2+ | 56 fs +48-22 | XREF: Z(4420). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4447.7 | E(level): From 54Fe(α,2pγ). From 56Co ε decay. | ||
4458.532 | 4+ | 26 fs +12-8 | E(level): From 56Co ε decay. From 54Fe(α,2pγ). From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
4509.56 | 3- | 83 fs 28 | XREF: O(4530). E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
4539.5 | 1+,2+ | 25 fs +20-14 | XREF: O(4530). |
4554.77 | 4+ | 94 fs +43-24 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4608.56 | 2+ | 47 fs +33-18 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4610.82 | 4+ | 27 fs +45-15 | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4620 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
4658.26 | 2+,3+,4+ | 49 fs +8-7 | E(level): From 56Mn β- decay. Jπ(level): From angular momentum transfer in 57Fe(d,t). T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4683.04 | (2+),3+ | 66 fs +63-25 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4692.32 | 4+ | 33 fs +10-7 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4728.14 | 2+ | 63 fs +57-20 | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). |
4730.0 | 0+ | E(level): From 56Fe(n,n’γ). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
4737.33 | 2+ | 32 fs +7-6 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4784.12 | (1,2+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
4802 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
4812.68 | 4+,5+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
4820 | E(level): From 54Fe(t,p). | ||
4847.9 | (2+) | 64 fs 27 | E(level): From 56Fe(p,p’γ). Iγ unknown. Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
4866.52 | (1,2+) | 9.7 fs 20 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
4878.0 | 2+ | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
4887.1 | E(level): From 56Fe(n,n’γ). | ||
5023.49 | (1,2)+ | 6 fs 3 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
E(level) | Jπ(level) | T1/2(level) | Comments |
5033.02 | (4,5)+ | 10 fs +3-2 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5038.49 | 4+ | 78 fs +36-22 | XREF: F(5050). E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5055.87 | 4+,(3+) | 66 fs +63-25 | XREF: H(5062). E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5122.11 | 5- | XREF: W(5080). E(level): From 56Co ε decay. From 56Fe(n,n’γ). Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
5131.66 | 3+,4+,(2+) | 73 fs +28-17 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5149.54 | 2+ | XREF: K(5156). E(level): From 56Fe(p,p’γ). From 56Fe(n,n’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
5184.3 | 8(+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
5186.82 | 2+ | XREF: O(5200)Z(5200). | |
5194.80 | (1,2+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
5219 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
5227.3 | 1 | 12.3 fs 20 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). |
5232.57 | 2+,(3+) | 8 fs +6-5 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5235.89 | 4+ | 104 fs +55-28 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5249 | 4+ | E(level): From 56Co ε decay. From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
5255.7 | 8+ | 0.35 ps 4 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). |
5256.9 | 2+ | 20 fs 4 | E(level): Iγ unknown. Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
5296 | 0+ | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
5302.94 | 4+ | 28 fs +15-9 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5386 | 0+ | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
5402.3 | GE 1 | 17 fs 4 | E(level): From 56Fe(n,n’γ). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
5451.60 | 4+ | 98 fs +40-28 | XREF: K(5455). E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5479.15 | (4+) | 25 fs +24-9 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5488.24 | 2,3,4 | 3 fs 2 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5502.94 | (2,3,4)+ | 5 fs 2 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5511.6 | 2+ | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
5528 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
5538.07 | (1,2+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
5573.51 | 2+ | XREF: K(5591). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
5590.06 | 1+,2,3+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
5618.36 | 4+ | 76 fs +51-24 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5623.86 | (4,5)+ | 19 fs +14-10 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5626.84 | 8+ | 0.069 ps +21-14 | XREF: d(5621). |
5661.18 | < 14 fs | T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. | |
5670.33 | (2,3,4)+ | 16 fs +8-6 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5684 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
5697.98 | (2+) | 85 fs +42-33 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5705.43 | 2+ | 3 fs 2 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5725 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
5737 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
5774.00 | (4+) | 12 fs +9-6 | XREF: d(5768). E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5795.2 | XREF: d(5784). E(level): From 56Fe(n,n’γ). | ||
5853 | 19 fs 5 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
5861.5 | 4+ | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
5871.26 | (2,3,4) | 12 fs +27-10 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5913.51 | 2+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
5914.53 | (2,3,4)+ | 22 fs +14-8 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
5936.17 | 2+ | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
5965.81 | XREF: F(5970). | ||
6002 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6013 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
E(level) | Jπ(level) | T1/2(level) | Comments |
6041 | (7-) | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | |
6055 | 2+ | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
6061.79 | 4+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
6071.6 | 6+ | E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
6078 | 16 fs 3 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
6092.2 | (3-) | XREF: F(6080). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
6102.21 | (0 TO 3+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
6115.7 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). | ||
6131.24 | 2+ | 5 fs +4-3 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
6174 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6201 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6219 | 13 fs 3 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
6250.78 | 1 | 8.1 fs 15 | E(level): Iγ unknown. From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
6265 | 4+ | XREF: K(6273). E(level): From 56Co ε decay. From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
6289 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6316 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6351 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6363 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6397 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6446.92 | 2+,3+ | 11 fs +7-4 | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
6489 | (2+) | E(level): From 56Co ε decay. From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
6527 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6543 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6555 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6566.81 | 0+ | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
6593 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6613 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6625.10 | (0 TO 3+) | E(level): From 56Co ε decay. From 56Fe(p,p’γ). Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
6652 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6666.62 | 3- | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
6670 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6698 | 1 | 0.65 fs 10 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
6700 | 0+ | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
6725 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6742 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6781 | 3- | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
6800 | 0+ | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
6807.8 | XREF: K(6823). | ||
6843 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6850.9 | 9(+) | XREF: d(6856)K(6855). E(level): From 56Mn β- decay. From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From angular momentum transfer in 57Fe(d,t). | |
6869.73 | (3-) | XREF: F(6870). E(level): From 56Co ε decay. Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
6916 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6926 | 1- | 1.10 eV 29 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
6940 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
6981.68 | (0 TO 3+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
6994 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7010.8 | (>3-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
7029.8 | (>3-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
7055 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7061.6 | 1+ | 0.41 fs 8 | E(level): Iγ unknown. Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
E(level) | Jπ(level) | T1/2(level) | Comments |
7084.6 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). | ||
7090 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7102 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7124 | 0+ | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
7135 | 1 | 8.1 fs 15 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
7154 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7167.27 | 1 | 5.1 fs 9 | E(level): Iγ unknown. Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
7177.2 | (10+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
7204 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7211.5 | 1 | 0.77 eV 22 | Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
7220 | 0+ | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
7248 | 1 | 2.3 fs 3 | E(level): Iγ unknown. From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
7254.19 | 0+ | XREF: F(7290). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
7285.8 | 1.6 fs 7 | E(level): Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
7312 | E(level): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). | ||
7422.67 | (1,2+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
7446.5 | 1 | 2.7 fs 8 | E(level): Iγ unknown. From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
7468.5 | 1 | 2.5 fs 4 | E(level): Iγ unknown. Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
7475 | (3-) | E(level): From 56Co ε decay. From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). Jπ(level): From angular momentum transfer in 56Fe(d,d’), or 56Fe(p,p’), or 56Fe(α,α’), or 56Fe(e,e’). | |
7503.6 | 9(+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
7580 | E(level): From 54Fe(t,p). | ||
7630 | 3- | E(level): From 54Fe(t,p). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
7670 | E(level): From 54Fe(t,p). | ||
7720 | E(level): From 54Fe(t,p). | ||
7820.6 | 10(+) | XREF: F(7840). E(level): From 56Mn β- decay. From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From angular momentum transfer in 57Fe(d,t). | |
E(level) | Jπ(level) | T1/2(level) | Comments |
7875.8 | 2+ | Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
7886.54 | (1,2+) | 1.6 fs 3 | E(level): From 56Fe(p,p’γ). Iγ unknown. Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
8050 | E(level): From 54Fe(t,p). | ||
8110 | 0+ | E(level): From 54Cr(3He,n). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
8120 | 2+ | E(level): From 54Fe(t,p). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
8128 | 1 | 3.55 eV 74 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
8219 | 1.8 fs 3 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
8239.7 | 1 | 5.75 eV 92 | Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
8247.76 | (0 TO 3+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
8309.59 | (1,2+) | 1.9 fs 6 | E(level): From 56Fe(p,p’γ). Iγ unknown. Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
8414.8 | (10+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
8447.87 | (0 TO 3+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
8535.95 | 1 | 4.92 eV 95 | Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
8679.9 | 11(+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
8758.47 | (0 TO 3+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
8767 | 1.1 fs 2 | XREF: J(8800). E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
8879 | 1.5 fs 4 | XREF: J(8800). E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
8909.9 | (1,2+) | 0.97 fs 21 | E(level): From 56Fe(p,p’γ). Iγ unknown. Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
8962 | 1.2 fs 2 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
8989 | 1.5 fs 3 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9107 | 0.53 fs 11 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9140.3 | 1- | 1.28 eV 17 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
9154 | 0.47 fs 15 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9200 | 0+ | E(level): From 54Cr(3He,n). Jπ(level): From angular momentum transfer in 54Fe(t,p), or 54Fe(3He,n). | |
9287 | 0.61 fs 14 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
9311 | 0.71 fs 14 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9322 | 0.70 fs 15 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9344.7 | (11+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
9378.2 | (11+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
9402 | 0.70 fs 16 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9557.62 | (1,2+) | 1.2 fs 4 | E(level): From 56Fe(p,p’γ). Iγ unknown. Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. |
9666 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). | ||
9737 | 0.48 fs 13 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9768 | 1.0 fs 3 | XREF: J(9800). E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9895 | 1.1 fs 3 | XREF: J(9800). E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9948 | 0.61 fs 14 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
9969 | 1.5 fs 5 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
10060 | 0.81 fs 23 | XREF: J(10200). E(level): From 56Fe(γ,γ’), (pol γ,γ’). Iγ unknown. T1/2(level): Upper limit based upon the assumption that Γγ0/Γ=1. | |
10094.4 | (12+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
10497 | 1 | 3.44 eV 64 | XREF: J(10200). E(level): From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
10563.1 | (12+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
10898.9 | (13+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
11133 | 1 | 2.08 eV 52 | E(level): From 56Fe(γ,γ’), (pol γ,γ’). Jπ(level): Based on γ resonance ex. measurements in 56Fe(γ,γ’), (pol γ,γ’). T1/2(level): From 56Fe(γ,γ’), (pol γ,γ’) assuming 100% transition to g.s. |
11598.65 | 1+ | IAR of 1+ 110 in 56Mn. E(level): IAR of 1+ 110 in 56Mn. | |
11603.64 | 1+ | IAR of 1+ 110 in 56Mn. E(level): IAR of 1+ 110 in 56Mn. | |
11612.93 | 1+ | IAR of 1+ 110 in 56Mn. E(level): IAR of 1+ 110 in 56Mn. | |
11638.0 | 3(-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11640.7 | 3(-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11644.0 | 3(-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11664.0 | 3(-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
E(level) | Jπ(level) | T1/2(level) | Comments |
11678.0 | 4+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11680.6 | 4+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11688.2 | 4+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11692.1 | 2+ | ≈ 9 keV | Γp=2.0 2 E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
11832.8 | 3+ | ≈ 17 keV | Γp=1.0 2 E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
11840.8 | 3+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11850.0 | 3+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11879.6 | (5+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11886.8 | (5+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11913.3 | (4+) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11925.2 | 3+ | ≈ 11 keV | Γp=1.0 1 E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
11947.7 | (4-) | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11952.6 | 4+ | E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. | |
11958.1 | 3+ | ≈ 11 keV | Γp=1.0 1 E(level): From 56Fe(p,p’γ). Jπ(level): From 55Mn(p,p’), (p,γ) E=res: IAR based on reasonable assumption of the multipolarity of observed γ-transitions and application of corresponding selection rules, or analyses of IAR state in 56Mn. T1/2(level): From 55Mn(p,p), (p,γ) E=res: IAR. |
11964 | (13+) | E(level): From 56Fe(γ,γ’), (pol γ,γ’). From (HI,xnγ). Jπ(level): From γγ-coin and γ(θ) in (HI,xnγ). | |
12440 | E(level): From 56Fe(n,n’). | ||
12520 | E(level): From 56Fe(n,n’). |
E(level) | E(gamma) | Comments |
846.7778 | 846.7638 | E(γ): From 56Mn β- decay.. From 56Fe(n,n’).. From 56Fe(γ,γ’), (pol γ,γ’). I(γ): From 56Mn β- decay. M(γ): From 56Co ε decay. |
2085.1045 | 1238.2736 | E(γ): From 56Mn β- decay.. From 56Fe(n,n’).. From 56Fe(γ,γ’), (pol γ,γ’). I(γ): From 56Mn β- decay. M(γ): From 56Co ε decay. |
2657.5894 | 1810.757 | E(γ): From 56Co ε decay.. From 56Fe(n,n’). I(γ): From 56Mn β- decay. | 2657.527 | E(γ): From 56Co ε decay.. From 56Fe(n,n’). I(γ): %Branching=5.4 21 from B(E2)=0.0037 10 (e,e’) and adopted T1/2; %Branching=5 3 in 56Fe(p,p’γ).. From 56Mn β- decay. |
2941.50 | 2941 | E(γ): 2939 reported in (p,p’γ). |
2959.972 | 2113.135 | E(γ): From 56Co ε decay.. From 56Fe(n,n’). I(γ): From 56Mn β- decay. | 2959.92 | E(γ): From 56Mn β- decay.. From 56Fe(n,n’). I(γ): From 56Mn β- decay. |
3076.2 | 991.51 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2229 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3120.11 | 462 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2273.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3120 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3122.970 | 1037.8333 | E(γ): From 56Mn β- decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 2276.131 | E(γ): From 56Co ε decay.. From 56Fe(γ,γ’), (pol γ,γ’).. From 54Fe(t,p). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
3369.95 | 2523.06 | E(γ): From 56Mn β- decay.. From 56Fe(n,n’). I(γ): From 56Mn β- decay. | 3369.84 | E(γ): From 56Mn β- decay.. From 56Fe(n,n’). I(γ): From 56Mn β- decay. |
3388.55 | 265.5 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). | 1303.4 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). M(γ): From 54Fe(α,2pγ). |
3445.348 | 787.743 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 1360.212 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 2598.500 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
3448.41 | 790 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2601 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3448 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3600.21 | 942 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1515 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2753 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3600 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
3605.69 | 948 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1521 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2759 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3606 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3610.21 | 952 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1525 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2763 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3610 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3744.13 | 2897 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3755.57 | 367.0 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). M(γ): From 54Fe(α,2pγ). | 632.6 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). | 1670.8 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). |
3829.77 | 1172 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2983 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3830 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
3856.495 | 411.145 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 486.55 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 733.514 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 896.510 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 1198.888 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 1771.357 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 3009.645 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
4048.888 | 1088.894 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 1963.741 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 3202.029 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
E(level) | E(gamma) | Comments |
4085.93 | 3239 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4086 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4100.363 | 655.003 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 977.372 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 1140.368 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 1442.746 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 2015.215 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 3253.503 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
4119.936 | 263.434 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 674.579 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 996.948 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 1159.944 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 1462.322 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 2034.791 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 3273.079 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
4298.096 | 852.732 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 1175.101 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 1640.475 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 2212.948 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. | 3451.232 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
4394.93 | 1271.92 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 3548.05 | E(γ): From 56Co ε decay.. From 54Fe(t,p).. From 56Fe(γ,γ’), (pol γ,γ’).. From 56Fe(n,n’γ). I(γ): From 56Co ε decay. M(γ): From 56Co ε decay. |
4401.27 | 955.8 | I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1031 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1441 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2316 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3554.2 | I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
4447.7 | 3600.8 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. |
4458.532 | 1335.40 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 2373.24 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. | 3611.53 | E(γ): From 56Co ε decay.. From 54Fe(t,p). I(γ): From 56Co ε decay. |
4509.56 | 754.35 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1139.66 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1386.3 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1852.09 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2424.93 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3662.67 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4554.77 | 799.02 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 810.60 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1165.74 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1431.58 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1897.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2469.71 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3708.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4608.56 | 1485.60 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1667.07 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1949.9 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2523.09 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3761.5 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4610.82 | 756.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 781.20 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1651.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1954.11 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2525.75 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3763.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
4658.26 | 1213 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1288 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1698 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2000 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2573 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3811 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4658 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4683.04 | 1312.58 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1559.53 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2525.75 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3836.21 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4692.32 | 936.58 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 948.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1569.42 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2034.76 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2607.22 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3844.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4700.63 | 944.7 | E(γ): From 56Fe(p,p’γ). I(γ): From 56Fe(p,p’γ). | 1312.2 | E(γ): From 56Fe(p,p’γ). I(γ): From 56Fe(p,p’γ). M(γ): From (HI,xnγ). |
4728.14 | 3881 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4728 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4737.33 | 617.36 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2079.80 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3889.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4736.3 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
4784.12 | 1664 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3937 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4784 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4812.68 | 692.65 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1057.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1368.3 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4847.9 | 2190.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2763.24 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4847 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
4866.52 | 1267 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1419 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1422 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1497 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1747 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1907 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2209 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2782 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4020 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4867 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
4878.0 | 2793 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4031 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4878 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5023.49 | 903 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1575 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1653 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1903 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2063 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2365 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4176 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5023 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
5033.02 | 1277.00 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1643.9 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2947.86 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4188.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5038.49 | 1915.10 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5055.87 | 757.75 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2971.04 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5131.66 | 673.02 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1082.83 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1686.41 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2008.80 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4284.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5149.54 | 2026.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3064.04 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5184.3 | 1427.8 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
5186.82 | 3101.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5194.80 | 1585 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2075 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2253 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2537 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4348 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5227.3 | 5227 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
5232.57 | 1132.13 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1183.39 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1783.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1787.18 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3147.7 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4385.87 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
5235.89 | 543.39 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 777.14 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 936.58 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1135.68 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1186.29 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1480.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1790.44 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1847.49 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2276.3 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2578.56 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3150.70 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5255.7 | 1499.5 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). M(γ): From (HI,xnγ). | 1866.8 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). M(γ): From (HI,xnγ). |
5256.9 | 4410 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5257 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5302.94 | 757.75 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1005.1 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1915.10 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2180.12 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3217.61 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4456.9 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5307.81 | 1919.69 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5402.3 | 5404 | E(γ): Multiply placed with undivided intensity. From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). I(γ): Multiply placed with undivided intensity |
5451.60 | 1151.84 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1153.78 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1402.79 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1696.17 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2063.25 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4604.9 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
5479.15 | 3394.10 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5488.24 | 1120.27 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1368.41 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2042.65 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3401.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5502.94 | 1101.80 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1402.79 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2058.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2133.13 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2845.96 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3418.69 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5538.07 | 2168 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2880 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4691 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5538 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5590.06 | 2142 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2145 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2220 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2932 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4743 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5618.36 | 1223.46 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2173.89 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2230.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2658.19 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3535.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4772.5 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
5623.86 | 1523.26 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1575.21 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1867.89 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2500.52 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3539.14 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5626.84 | 926.2 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). M(γ): From 54Fe(α,2pγ). | 1871.3 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). M(γ): From 54Fe(α,2pγ). | 2238 | E(γ): From 54Fe(α,2pγ).. From 56Co ε decay. I(γ): From 54Fe(α,2pγ). M(γ): From 54Fe(α,2pγ). |
5661.18 | 5661.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5670.33 | 2711.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3585.25 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4822.9 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5697.98 | 1293.73 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5705.43 | 977.29 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2259.92 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2584.73 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2744.88 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3619.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 4857.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5774.00 | 1326.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3116.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5801.34 | 1972.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2859.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5806.3 | 4958.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5817.22 | 2447.5 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
5853 | 5853 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
5861.5 | 2902.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5871.26 | 1551.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2127.34 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3786.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5914.53 | 1222.38 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1312.42 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1455.5 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1519.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1615.91 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2058.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2792.65 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2794.13 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3829.64 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5068.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5936.17 | 2080 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5089 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
5986.86 | 1447 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2542 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5140 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6021.11 | 5174.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6047.53 | 1508.31 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5200.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6061.79 | 1612.96 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1667.07 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 1842.53 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2305.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2460.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3101.22 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3975.4 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5214.6 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
E(level) | E(gamma) | Comments |
6078 | 6078 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
6102.21 | 2496 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2654 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5255 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6110.6 | 4026.3 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6131.24 | 2010.77 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3171.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5284.61 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6219 | 6219 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
6250.78 | 5404 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 6251 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6312.75 | 1863.83 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6386.99 | 2286.5 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6446.92 | 2618 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2842 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 2848 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3328 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6454.4 | 5607.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6472.5 | 2352.2 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6625.10 | 3025 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3180 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 3665 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6698 | 5853 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). | 6698 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
6850.9 | 1221.7 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
E(level) | E(gamma) | Comments |
6854.67 | 1798.62 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6889.98 | 3949.0 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
6926 | 6926 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
6981.68 | 4324 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 6135 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7008.00 | 4923.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7010.8 | 3935.3 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7084.6 | 968.9 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
7135 | 7135 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
7167.27 | 6320 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 7167 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7177.2 | 1920.9 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
7211.5 | 6364 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 7211 | E(γ): Iγ unknown. |
7220 | 3619 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 6372 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7248 | 7248 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
7254.19 | 3643.8 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7422.67 | 6576 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 7423 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
7446.5 | 7446 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
7468.5 | 7468 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
7503.6 | 2247.1 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). | 2319.3 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
7820.6 | 969.6 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). | 2564.4 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
E(level) | E(gamma) | Comments |
7886.54 | 1951 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 7887 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
8128 | 8128 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
8219 | 8219 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
8239.7 | 8239 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
8247.76 | 7401 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
8309.59 | 7463 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 8310 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
8414.8 | 2785.7 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). | 3158.2 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
8447.87 | 7601 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
8679.9 | 265.1 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). | 859.2 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
8758.47 | 3974 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5158 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR | 5388 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
8767 | 8767 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
8879 | 8879 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
8909.9 | 8910 | E(γ): From 55Mn(p,p), (p,γ) E=res: IAR. From 56Fe(p,p’), (pol p,p’). I(γ): From 55Mn(p,p), (p,γ) E=res: IAR |
8962 | 8962 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
8989 | 8989 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9107 | 9107 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9140.3 | 9139.5 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ).. From 54Cr(3He,n). M(γ): From 56Fe(γ,γ’), (pol γ,γ’). |
9154 | 8307 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). | 9154 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
E(level) | E(gamma) | Comments |
9287 | 9287 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9311 | 9311 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9322 | 9322 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9378.2 | 963.4 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
9402 | 9402 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9557.62 | 9558 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9666 | 9666 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9737 | 9737 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9768 | 9768 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9895 | 9895 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9948 | 9948 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
9969 | 9969 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
10060 | 10060 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
10094.4 | 1414.5 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
10497 | 10497 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
10563.1 | 1184.9 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
10898.9 | 1554.2 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |
11133 | 11133 | E(γ): From 56Fe(γ,γ’), (pol γ,γ’).. From (HI,xnγ). |
11964 | 1401 | E(γ): From (HI,xnγ). I(γ): From (HI,xnγ). |