ADOPTED LEVELS, GAMMAS for 75Cu

Authors: Alexandru Negret, Balraj Singh |  Citation: Nucl. Data Sheets 114, 841 (2013) |  Cutoff date: 30-Jun-2013 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=8088 keV 3S(n)= 6536 keV 7S(p)= 13300 keV SYQ(α)= -1.253×104 keV 47
Reference: 2012WA38

References:
  A  BE(86Kr,xγ)  B  BE(238U,Fγ)

General Comments:

75Cu produced and identified in thermal neutron fission of 235U: 1985Re01, 1987Ar21, 1990Be13, 1991Kr15

2013Pe03: 75Cu was produced following the fragmentation of 86Kr (60.4 MeV/nucleon) beam on Be; Bρ-ΔE-tof technique was applied using LISE2000 spectrometer at GANIL to identify the fragments. Si and HPGe detectors used to measure particle and γ spectra, respectively. Deduced isomers, half-lives, and level scheme. α previous very similar experiment of the same group is presented in 2010Da06 and 1999DaZQ.

2010Vi07, 2009Fl03: 75Cu was produced at ISOLDE-CERN facility by 1 GeV proton induced fission of uranium carbide target. Resonance Ionization laser ion source (RILIS) used to laser ionize the atoms followed by high-resolution isotope separation (HRS) and ISCOOL Paul trap. Measured hyperfine structure. Deduced spin, magnetic dipole moment and electric quadrupole moment of the ground state. Collinear and in-source laser spectroscopic technique. Comparison with large-scale shell-model calculations using 56Ni core.

2011Il01: 75Cu beam produced from fission of 238U (using UCx target with protons at Holifield Radioactive Ion beam facility). Isotopic half-life measured from decay curves of 8 γ rays from decay of 75Cu

2012Ka36: 75Cu isomers produced in 9Be(238U,X) at 345 MeV/nucleon using BigRIPS separator at RIKEN facility. Measured delayed γ rays and isomer half-life. Total of 5.4×105 75Cu fragments detected

Mass measurement (Penning-trap system): 2007Ra27, 2005Gu36

Structure calculations: 2010Si11 (levels, J, π, μ), 2005Bo19 (half-life and delayed-neutron emission probability), 2005Li54 (calculated 5/2- and 3/2- levels), 2004Sm03 (levels, shell model), 2012Sr02, 2012Sr03 (shell model).

Q-value: Estimated ΔS(p)=400 (2012Wa38)

Q-value: S(2n)=11627 3, S(2p)=32150 500 (syst), Q(β-n)=3214 3 (2012Wa38)










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   0.0AB 5/2(-) 1.224 s 3 
% β- = 100
% β-n = 3.5 6
     
  61.7 4 AB (1/2-,3/2-) 310 ns 8 
% IT = 100
  61.7 4 
  100
[M1,E2]
   0.0
5/2(-)
  66.2 4 AB (1/2-,3/2-) 149 ns 6 
% IT = 100
   4.5 6 S
  66.2 4 
 
  100
[M1]
[M1,E2]
  61.7
   0.0
(1/2-,3/2-)
5/2(-)

E(γ): From 2013Pe03; the values from 2010Da06 and 2012Ka36 are in good agreement.

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Additional Gamma Data:













E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityConversion
Coefficient
Additional Data
  61.7 (1/2-,3/2-) 310 ns 8 
% IT = 100
  61.7 4 [M1,E2]2.0α=2.0 18
  66.2 (1/2-,3/2-) 149 ns 6 
% IT = 100
   4.5 6 [M1]54α=54 20
(1/2-,3/2-) 149 ns 6 
% IT = 100
  66.2 4 [M1,E2]1.5α=1.5 13

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
   0.05/2(-) 1.224 s 3 
% β- = 100
% β-n = 3.5 6
μ=+1.0062 13 (2009Fl03,2010Vi07,2011StZZ), Q=-0.269 16 (2010Vi07,2011StZZ)
Dominant (≈90%) configuration=π1f5/2 (2010Da06), with significant coupling to the 2+ vibrational excitation, as suggested by the deviation of measured magnetic moment from Schmidt value. Measurements of spin=3/2 and magnetic moments for 71Cu and 73Cu suggest inversion of π2p3/2 to π1f5/2 orbitals in νg9/2 mid-shell.
  61.7(1/2-,3/2-) 310 ns 8 
% IT = 100
Jπ(level): 1/2- and 3/2- doublet expected from large-scale shell model calculations, corresponding to p1/2 and p3/2 orbitals, respectively. The ordering of the two Jπ’s could not be established (2013Pe03).
T1/2(level): From time difference between the implantation of the heavy ions in Si detectors and the delayed γ rays detected with three HPGe detectors (2013Pe03) in Be(86Kr,Xγ).
  66.2(1/2-,3/2-) 149 ns 6 
% IT = 100
Jπ(level): 1/2- and 3/2- doublet expected from large-scale shell model calculations, corresponding to p1/2 and p3/2 orbitals, respectively. The ordering of the two Jπ’s could not be established (2013Pe03).
T1/2(level): From time difference between the implantation of the heavy ions in Si detectors and the delayed γ rays detected with three HPGe detectors (2013Pe03) in Be(86Kr,Xγ).

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Additional Gamma Comments:

E(level)E(gamma)Comments
  66.2   4.5E(γ): γ not observed directly. Its existence is assumed based on the decay and population time pattern of the two observed gammas, 61.7 and 66.2 in 2013Pe03.

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