ADOPTED LEVELS, GAMMAS for 58Zn

Author: Balraj Singh |  Citation: ENSDF |  Cutoff date: 31-JUL-2014 

Authors: Caroline D. Nesaraja, Scott D. Geraedts and Balraj Singh |  Citation: Nucl. Data Sheets 111, 897 (2010) |  Cutoff date: 12-Jan-2010 

 Full ENSDF file | Adopted Levels (PDF version) 


S(n)= 17820 keV SYS(p)= 2280 keV 50Q(α)= -5510 keV 70
Reference: 2012WA38

References:
  A  2H(57Cu,58ZnG) 

General Comments:

58Zn nucleus is of astrophysical interest since it is deemed as a waiting-point nucleus in rp process in X-ray bursts

1998Jo18 (also 2000Oi04): 58Zn produced and identified in Nb(p,X) E=1 GeV at ISOLDE at CERN using selective laser-ion source. Measured Eγ, Iγ, βγ coin, isotopic half-life

2002Lo13 (also 2002Bl17): 58Zn obtained from fragmentation of 78Kr beam at 73 MeV/nucleon at GANIL using LISE spectrometer. Measured isotopic half-life

2005Ka46: 58Zn produced and identified in Nb(p,X) E=1.4 GeV at ISOLDE at CERN using selective laser-ion source. Measured Eγ, Iγ, βγ coin, isotopic half-life. No delayed protons were observed from 58Zn isotope. The authors state that analysis of 58Ni(3He,3n) (same reaction as was used by 1983HoZY) experiment is in progress to detect protons

2007Bl09: fragmentation of 70Ge beam at 71.6 MeV/nucleon with Ni target. Measured production cross section.

2009Fu15: fragmentation of 64Zn+29 beam at 79 MeV/nucleon with natural Ni target at LISE3, GANIL facility. Measured half-life by measuring β-delayed γ-ray activity.

2012OrZY: 58Zn produced in Ni(58Ni,X),E=74.5 MeV/nucleon using LISE3 facility at GANIL. Detected 58Zn fragments through tof, E-ΔE measurements followed by detection of β particles. Half-life of ground state was measured from β-decay curve. This is an independent experiment by the same group as 2009Fu15. Through an e-mail communication of July 30, 2014 with Professor B. Rubio at University of Valencia, another experiment had been done for a precise measurement of ground-state half-life, results of which were communicated to the evaluator

Others:

1983HoZY: possible identification in 58Ni(3He,3n) reaction, claimed to have observed delayed protons. This work remains unpublished.

1994Fo07 (also 1996Fo08,1987Zu03): 58Ni(π+-) E=120-292 MeV; measured excitation function for double charge exchange reaction on t=1 target: 58Ni(π+-)58Zn, leading to double isobaric analog states and compared data with theoretical calculations

1986Se04: 58Ni(π+-) E=292 MeV, deduced mass excess

2001Fo07: reaction rates of 57Cu(p,γ)58Zn and levels of 58Zn from shell-model calculations. The first 2+ state is predicted at 1400

2006Va21, 2004Va38: Structure calculation for Pseudo-orbital SO(6) symmetry in 58Zn, 58Cu and 58Ni

Q-value: Estimated uncertainty=210 in S(n) (2012Wa38).

Q-value: Q(εp)=6500 50, S(2n)=32860 510 (syst), S(2p)=2970 50 (2012Wa38)









E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)Final Levels
     0.0A 0+ 86.7 ms 24 
% ε = 100
% εp < 3
    
  1356 3 A (2+)     1356 3 
  100
     0.0
0+
  2499 4 A (4+)     1143 3 
  100
  1356
(2+)
  2609 6 A (2+)     1253 5 
  100
  1356
(2+)
  2862 3 A (2+)     1507 4 
  2861 4 
  100 25 
   88 25 
  1356
     0.0
(2+)
0+
  2902 3 A (1+)     1545 3 
  2904 5 
  100 15 
   23 8 
  1356
     0.0
(2+)
0+
  3263 4 A (2+)     1906 4 
  3265 6 
   57 29 
  100 29 
  1356
     0.0
(2+)
0+
  3378 6 A (3+)      879 4 
  100
  2499
(4+)

E(level): From least-squares fit to Eγ data. All levels listed here above the first 2+ level at 1356 keV are proton unbound.

Jπ(level): From systematics of even-even nuclei, shell-model predictions, and mirror analogy with 58Ni nucleus

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments

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