Characterization of the low-lying 0+ and 2+ states in Ni 68 via β decay of the low-spin Co 68 isomer

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Abstract

The low-energy structure of the neutron-rich nucleus Ni68 has been investigated by measuring the β decay of the low-spin isomer in Co68 selectively produced in the decay chain of Mn68. A revised level scheme has been built based on the clear identification of β-γ-E0 delayed coincidences. Transitions between the three lowest-lying 0+ and 2+ states are discussed on the basis of measured intensities or their upper limits for unobserved branches and state-of-the-art shell model calculations.

Figures

  • FIG. 1. Time spectrum between two consecutive signals in the plastic detectors in the time region [−1000, −125] ns and [+50, +1000] ns, outside the prompt time distribution to exclude β scattering from one detector to another.
  • FIG. 2. Gamma spectrum in coincidence with the decay radiation from the 0+2 to 0 + 1 in 68Ni. The time condition required is that the γ ray is detected within 600 ns after one of the two plastic signals (68Coβ rays or delayed E0 signal, see text).
  • FIG. 3. (Color online) β-gated γ -ray spectrum in the time window [350, 2200] ms after the proton pulse impinged on the target when (blue) lasers are tuned to resonantly ionize Mn and (red) lasers are off. The laser-off spectrum was scaled to the laser-on one using the 1313-keV peak from 136I for comparison. Symbols indicate lines associated with: 68Co decay (stars), 68Fe decay (squares), 67Fe and 67Co decay after β-delayed neutron emission (triangles), laser off 68Ga and 136I contaminants decay (circles).
  • FIG. 4. Decay scheme of 68Co. All the β-feeding percentages should be considered as upper limits (see text) and the missed feeding (possibly β, E0, or γ feeding) was determined using the method of Ref. [27]. Tentative spin-parity assignments in brackets for higher spin states (4−,3−,4+) comes from Refs. [12,23]. When indicated with a 1u exponent, logf t values were taken assuming a first-forbidden unique transition. Asterisk (∗) from Ref. [11], upsidedown triangle (∇ ) from Ref. [32].
  • TABLE I. (top) Summary of γ energies and intensities in 68Ni relative to the (2+1 → 0+1 ) γ -ray transition obtained in this work compared to the published results of Muelleret al. for the decay of the low-spin isomer of 68Co [11]. (bottom) Intensities and 2σ upper limits (95% CL) determined for different 0+ to 0+ decays.
  • TABLE II. Absolute B(E2) in e2fm 4 and B(E2) ratios R(Eγ ) for low-lying transitions in 68Ni. Theoretical values for MCSM calculations using the revised A3DA interaction (see Ref. [6] for details) and SM calculations using the LNPS interaction from Ref. [8] are compared to experimental values. Effective charges en = 0.5e and ep = 1.5e were used in the A3DA calculations.
  • FIG. 5. (Color online) Level scheme of 68Ni focused on the lowlying 0+ and 2+ states with their experimental B(E2) ratios [R(Eγ )] normalized to ground state transitions for each level. For the 0+3 state at 2511 keV, limits on branching ratios are quoted instead of B(E2) ratios (indicated with an asterisk).
  • FIG. 6. (Color online) Potential energy surfaces (PESs) obtained fromMCSM calculations [6] for the 0+ and 2+ states of 68Ni, coordinated by the usual quadrupole momentsQ0 andQ2 (or γ ). Circles on the PES represent shapes of MCSM basis vectors (see Ref. [6] for more details).

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Flavigny, F., Pauwels, D., Radulov, D., Darby, I. J., De Witte, H., Diriken, J., … Wimmer, K. (2015). Characterization of the low-lying 0+ and 2+ states in Ni 68 via β decay of the low-spin Co 68 isomer. Physical Review C - Nuclear Physics, 91(3). https://doi.org/10.1103/PhysRevC.91.034310

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