ADOPTED LEVELS, GAMMAS for 62Fe

Authors: Balraj Singh, Huang Xiaolong, and Wang Xianghan |  Citation: Nucl. Data Sheets 204, 1 (2025) |  Cutoff date: 30-Jun-2023 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=2546 keV 19S(n)= 8029 keV 4S(p)= 14425 keV 4Q(α)= -9311 keV 4
Reference: 2021WA16

References:
  A  62Mn β- decay (92 MS)  B  62Mn β- decay (671 MS+92 MS)
  C  9Be(62Fe,62Fe’γ)  D  64Ni(18O,20Ne),(14C,16O),
  E  64Ni(238U,xγ)  F  197Au(62Fe,62Fe’γ)
  G  208Pb(64Ni,xγ)  H  238U(64Ni,xγ),64Ni(238U,xγ)
  I  238U(70Zn,xγ)  J  Coulomb Excitation

General Comments:

1975Fr16: identification and production of 62Fe in 64Ni(n,2pn) reaction at E(n)=25-200 MeV, neutron beam of the 200-MeV LINAC at BNL. Identification from monitoring of decay of 62Fe and growth of 62Co. Measured Eγ, half-life

Delayed neutron decay of 63Mn is allowed and, in principle, can populate levels in 62Fe, but there is no experimental information available for this decay mode

Mass measurement: 2012Na15

Theoretical nuclear structure calculations:

2022Ho02: calculated quadrupole deformation parameter β2, S(2n), rms matter radius, hexadecapole deformation parameter β4, difference of the charge square radii, diffuseness parameters using Skyrme-Hartree-Fock method in three-dimensional coordinate space.

2022Ko04: calculated ground state energy, charge rms radius using coupled cluster (α) and ab-initio density functional theory, extended to open-shell deformed nuclei.

2021Ob02: calculated energy levels, Jπ, B(E2), deformation parameters, using shell model.

2017Sc04: calculated energy levels, Jπ B(E2), B(M1) using large-scale shall model.

2014Ji14: calculated levels, Jπ, deformation of ground state, B(E2) of collective states, potential energy surface using mean-field models.

2014Ko16: calculated levels, Jπ, B(E2), E(4+)/E(2+), E(6+)/E(4+), quadrupole moment, energy surface contour in (β-γ) plane using proton-neutron interacting boson model (IBM-2) and interacting shell model (ISM).

2012Lo04: calculated M1 transition strength distribution for ground and low-lying states using shell model with 40,48Ca core and KB3Gmod interaction; and compared with single-particle calculation and Kopecky formula.

2010Le20: calculated levels, Jπ, B(E2), quadrupole moment, occupation of neutron intruder orbitals and percentage of particle-hole excitations using interacting shell-model framework in full pf valence space with 48Ca core and G-matrix effective interaction.

2010Sr02, 2009Sr01: calculated levels, Jπ, quadrupole moments, B(E2), wave functions, occupation numbers using large-scale shell model with GXPF1A interaction.

2009Su20: calculated levels, Jπ, moment of inertia, B(E2), deformation parameters, yrast band up to 20+ using projected shell-model.

2002Ca48: calculated level energies, Jπ, B(E2) using large-scale shell model.

Other theory calculations: 19 references for structure and four for decays retrieved form the NSR database are listed in this dataset as ’document’ records.

Q-value: S(2n)=13608 4, S(2p)=26547 3 (2021Wa16)










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABCDEFGHIJ 0+ 68 s 2 
% β- = 100
     
   877.31 10 ABCDEFGHIJ 2+ 5.3 ps 6     877.3 1 
  100
E2
     0.0
0+
  1692.3 20 A          (0+)      815 2 
  100

   877.31
2+
  2016.98 18  B D       (1+,2+)     1139.8 2 
  2017.0 10 
  100 9 
   11 6 


   877.31
     0.0
2+
0+
  2176.47 14  B  E GHI  4+ 0.60 ps 17    1299.2 1 
  100
E2
   877.31
2+
  2691.62 16  B     H   (3+)      515.2 2 
   674.8 2 
  1814.0 2 
    5.0 13 
   16.9 25 
  100 8 


D
  2176.47
  2016.98
   877.31
4+
(1+,2+)
2+
  2849.72 24  B              673.3 2 
  100

  2176.47
4+
  3008.9 5  B    GH   (4-)      317.0 4 
   832.4 5 
    8.1 35 
  100 18 


  2691.62
  2176.47
(3+)
4+
  3015.7 5  B  E GHI  (5-)      839.3 5 
  100
D
  2176.47
4+
  3310.0 7  B    GH   (6-)      294.3 5 
   301.0 10 
  100 50 
  <33


  3015.7
  3008.9
(5-)
(4-)
  3360.3 15  B             1183.8 15 
  100

  2176.47
4+
  3387.84 17     E GHI  6+     1211.3 1 
  100
(E2)
  2176.47
4+
  3604.87 19       GH   (7-)      294.8 3 
   589.2 1 
    6.1 22 
  100 5 

(Q)
  3310.0
  3015.7
(6-)
(5-)
  3629.4 3       GH        241.6 2 
  100

  3387.84
6+
  3633.48 18  B         (4+)      941.8 2 
  1457.1 2 
  1616.4 3 
  2756.0 5 
  100 7 
   77 6 
    2.6 4 
    2.5 3 
(D)



  2691.62
  2176.47
  2016.98
   877.31
(3+)
4+
(1+,2+)
2+
  3661.7 15  B             1485.2 15 
  100

  2176.47
4+
  3713.7 15  B             1537.2 15 
  100

  2176.47
4+
  4050.7 4  B         (2+,3,4+)     1201.1 3 
  1874.0 15 
  3172.3 9 
  100 21 
   13 13 
   26 13 



  2849.72
  2176.47
   877.31

4+
2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4251.77 20       GH   (8+)      647.1 3 
   863.9 1 
    6.7 34 
  100 8 

(Q)
  3604.87
  3387.84
(7-)
6+
  4358.84 25        H   (8-)      754.0 2 
  1048.7 3 
   44 13 
  100 25 


  3604.87
  3310.0
(7-)
(6-)
  4902.2 4        H   (9-)     1297.3 3 
  100

  3604.87
(7-)
  4970 80    D              
  5319.5 3       GH   10+     1067.7 2 
  100

  4251.77
(8+)
  5474?       H       1222?
 

  4251.77
(8+)

E(level): From a least-squares fit to Eγ data

M(γ): From γγ(θ) in 62Mn β- decay and γ(θ) in 238U(64Ni,Xγ), combined with RUL (for E2 and M2)

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - Yrast band.
     0.0 0+ 68 s 2 
% β- = 100
     
   877.31 10  2+ 5.3 ps 6     877.3 1 
  100
E2
     0.0
0+
  2176.47 14  4+ 0.60 ps 17    1299.2 1 
  100
E2
   877.31
2+
  3387.84 17  6+     1211.3 1 
  100
(E2)
  2176.47
4+
  4251.77 20  (8+)      647.1 3 
   863.9 1 
    6.7 34 
  100 8 

(Q)
  3604.87
  3387.84
(7-)
6+
  5319.5 3  10+     1067.7 2 
  100

  4251.77
(8+)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - Band based on (4-),α=0
  3008.9 5  (4-)        
  3310.0 7  (6-)      294.3 5 
   301.0 10 
  100 50 
  <33


  3015.7
  3008.9
(5-)
(4-)
  4358.84 25  (8-)      754.0 2 
  1048.7 3 
   44 13 
  100 25 


  3604.87
  3310.0
(7-)
(6-)
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - Band based on (5-),α=1
  3015.7 5  (5-)        
  3604.87 19  (7-)      294.8 3 
   589.2 1 
    6.1 22 
  100 5 

(Q)
  3310.0
  3015.7
(6-)
(5-)
  4902.2 4  (9-)     1297.3 3 
  100

  3604.87
(7-)

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Additional Gamma Data:











E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityAdditional Data
   877.31 2+ 5.3 ps 6     877.3 1 E2B(E2)(W.u.)=14.1 16
  2176.47 4+ 0.60 ps 17    1299.2 1 E2B(E2)(W.u.)=17 +7-4

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.00+ 68 s 2 
% β- = 100
E(level): Yrast band.
   877.312+ 5.3 ps 6  Q=-0.08 40 (2015Ga38)
E(level): Yrast band.
  2176.474+ 0.60 ps 17  E(level): Yrast band.
  3008.9(4-)   E(level): Band based on (4-),α=0.
Jπ(level): Jπ assignments for the negative-parity states are based on band structures, systematics and γ(θ) data in 238U(64Ni,Xγ), and also shell-model calculations by 2009Su20.
  3015.7(5-)   ΔJ=1, dipole γ to 4+.
E(level): Band based on (5-),α=1.
Jπ(level): Jπ assignments for the negative-parity states are based on band structures, systematics and γ(θ) data in 238U(64Ni,Xγ), and also shell-model calculations by 2009Su20.
  3310.0(6-)   E(level): Band based on (4-),α=0.
Jπ(level): Jπ assignments for the negative-parity states are based on band structures, systematics and γ(θ) data in 238U(64Ni,Xγ), and also shell-model calculations by 2009Su20.
  3387.846+   E(level): Yrast band.
  3604.87(7-)   E(level): Band based on (5-),α=1.
Jπ(level): Jπ assignments for the negative-parity states are based on band structures, systematics and γ(θ) data in 238U(64Ni,Xγ), and also shell-model calculations by 2009Su20.
  4251.77(8+)   E(level): Yrast band.
  4358.84(8-)   E(level): Band based on (4-),α=0.
Jπ(level): Jπ assignments for the negative-parity states are based on band structures, systematics and γ(θ) data in 238U(64Ni,Xγ), and also shell-model calculations by 2009Su20.
  4902.2(9-)   E(level): Band based on (5-),α=1.
Jπ(level): Jπ assignments for the negative-parity states are based on band structures, systematics and γ(θ) data in 238U(64Ni,Xγ), and also shell-model calculations by 2009Su20.
  5319.510+   E(level): Yrast band.

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Additional Gamma Comments:

E(level)E(gamma)Comments
   877.31   877.3M(γ): ΔJ=2, quadrupole from γ(θ) and γγ(θ); RUL
  3387.84  1211.3E(γ): From 238U(64Ni,Xγ)
M(γ): ΔJ=(2), (Q) γ to (4+); (E2) from in-band transition
  3604.87   294.8E(γ): From 238U(64Ni,Xγ)
I(γ): From 238U(64Ni,Xγ)
   589.2E(γ): From 238U(64Ni,Xγ)
I(γ): From 238U(64Ni,Xγ)
  3629.4   241.6E(γ): From 238U(64Ni,Xγ)
  4251.77   647.1E(γ): From 238U(64Ni,Xγ)
I(γ): From 238U(64Ni,Xγ)
   863.9E(γ): From 238U(64Ni,Xγ)
I(γ): From 238U(64Ni,Xγ)
  4358.84   754.0E(γ): From 238U(64Ni,Xγ)
I(γ): From 238U(64Ni,Xγ)
  1048.7E(γ): From 238U(64Ni,Xγ)
I(γ): From 238U(64Ni,Xγ)
  4902.2  1297.3E(γ): From 238U(64Ni,Xγ)
  5319.5  1067.7E(γ): From 238U(64Ni,Xγ)
  5474  1222E(γ): From 238U(64Ni,Xγ)

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