ADOPTED LEVELS for 243Bk

Authors: C.D. Nesaraja, E.A. Mccutchan |  Citation: Nucl. Data Sheets 121, 695 (2014) |  Cutoff date: 30-Sep-2013 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-2300 keV SYS(n)= 7115 keV SYS(p)= 3403 keV 4Q(α)= 6874 keV 4
Reference: 2012WA38

References:
  A  247Es α decay (4.55 M) 

General Comments:

S(2n)=13485 syst 200; S(2p)=8823 4 (2012Wa38)

First identification: 1950Th52 in α particle bombardment of Americium, chemical separation.

Theoretical calculations:

2013Zd01: T1/2 for α decay calculated with a phenomenological model based on Gamow theory with WKB approximation for Coulomb barrier penetration.

2012Ni16: α decay T1/2 and fine structure calculated with Multichannel cluster model

2012Po01: calculated α decay T1/2 with a universal decay law using α-like R matrix theory.

2012Sa05,2011Sa40: calculated T1/2 and α decay fine structure using Coulomb and proximity potential model.

2012Zh01: β2, β4, moment of inertia, and alignments calculated with a particle conserving method based on the cranked shell model.

2011Zh36: partial α decay T1/2 to members of favored band calculated with a microscopic quantum tunneling theory.

2010Ni02: T1/2 and branching ratios calculated using generalized density dependent cluster model.

2008Do12: calculated binding energies with additional terms beyond standard Bethe Weizsacker formula

2004Pa40: deformation parameters, pairing gap, and single particle energy levels calculated with a macroscopic-microscopic model.

2002Lo05: calculated binding energies, Q(α), pairing gap, ground state deformation and single-particle levels with a relativistic mean field approach.

1985Lo17,1978Po09: calculated spontaneous-fission half-life of ground state.

1984Ku05: systematic study of fission-barrier parameters

1980Ka41: hindrance factors for α’s from 243Bk were calculated with R-matrix method.

Q-value: ΔQ(β-)=114; ΔS(n)=200 (2012Wa38)






E(level)
(keV)
XREFJπ(level) T1/2(level)
      0.0  (3/2-) 4.6 h 2 
% ε ≈ 99.85
% α ≈ 0.15
    ≈18A (7/2+)  
     67 20 A (9/2+)  
    131 20 A (11/2+)  
  ≈2200  5 ns
% SF ≤ 100

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)
Band 1 - 7/2[633] band. α=5.7 FOR B=0.0.
    ≈18 (7/2+)  
     67 20  (9/2+)  
    131 20  (11/2+)  

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
      0.0(3/2-) 4.6 h 2 
% ε ≈ 99.85
% α ≈ 0.15
Partial half-life for spontaneous-fission decay calculated by 1985Lo17 and 1978Po09: log[T1/2(SF in years)]≈3.6 and ≈5.0 from plots in 1985Lo17 and 1978Po09, respectively, yield spontaneous fission branchings≈1.3×10-5% and ≈5.1×10-7%.
E(level): Partial half-life for spontaneous-fission decay calculated by 1985Lo17 and 1978Po09: log[T1/2(SF in years)]≈3.6 and ≈5.0 from plots in 1985Lo17 and 1978Po09, respectively, yield spontaneous fission branchings≈1.3×10-5% and ≈5.1×10-7%.
     18(7/2+)   E(level): 7/2[633] band. α=5.7 FOR B=0.0.
Jπ(level): Hindrance factors for α decay from (7/2+) 247Es and the level spacings imply that these levels are probably members of a rotational band. From the unhindered character of the α transition (HF≈2.4) to the ≈18 keV level, the bandhead member should be the same state as that of the parent. Systematics of Nilsson states (see, for example, 1972El21) suggest either the 3/2[521] or the 7/2[633] orbital for 247Es g.s. If the α decay was to the 3/2[521] orbital, the band parameter would be 9.4 which would not fit the local trend. By assuming a rotational band built on the 7/2[633] state, the rotational band parameter of 5.7 is consistent with band parameters for 7/2[633] bands in the region.
     67(9/2+)   E(level): 7/2[633] band. α=5.7 FOR B=0.0.
Jπ(level): Hindrance factors for α decay from (7/2+) 247Es and the level spacings imply that these levels are probably members of a rotational band. From the unhindered character of the α transition (HF≈2.4) to the ≈18 keV level, the bandhead member should be the same state as that of the parent. Systematics of Nilsson states (see, for example, 1972El21) suggest either the 3/2[521] or the 7/2[633] orbital for 247Es g.s. If the α decay was to the 3/2[521] orbital, the band parameter would be 9.4 which would not fit the local trend. By assuming a rotational band built on the 7/2[633] state, the rotational band parameter of 5.7 is consistent with band parameters for 7/2[633] bands in the region.
    131(11/2+)   E(level): 7/2[633] band. α=5.7 FOR B=0.0.
Jπ(level): Hindrance factors for α decay from (7/2+) 247Es and the level spacings imply that these levels are probably members of a rotational band. From the unhindered character of the α transition (HF≈2.4) to the ≈18 keV level, the bandhead member should be the same state as that of the parent. Systematics of Nilsson states (see, for example, 1972El21) suggest either the 3/2[521] or the 7/2[633] orbital for 247Es g.s. If the α decay was to the 3/2[521] orbital, the band parameter would be 9.4 which would not fit the local trend. By assuming a rotational band built on the 7/2[633] state, the rotational band parameter of 5.7 is consistent with band parameters for 7/2[633] bands in the region.
   2200 5 ns
% SF ≤ 100
Assignment: 241Am(α,2n) systematics (1972Ga42).
E(level): Assignment: 241Am(α,2n) systematics (1972Ga42).

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