Extended Data Table 1 States populated in 62Cr in the two-proton removal from 64Fe projectiles

From: In-beam spectroscopy reveals competing nuclear shapes in the rare isotope 62Cr

  1. Listed are the excitation energy EJ and its spin-parity J, measured (exp) and calculated (th) cross sections σ, transition energy Eγ, final-state energy Ef and spin-parity Jf. Spin-parity assignments in brackets are based on comparison with theory. There are unplaced γ rays at 2095, 2125, 2213, and 2965 keV that, in total, carry 0.029 mb of cross section. States in italic are tentative – a coincidence of the corresponding transition with the \({4}_{1}^{+}\) was firmly observed but, due to low statistics, the possibility that these transitions are actually feeding the 6+ state cannot be excluded. The partial cross section to the ground state was obtained from the inclusive one via subtraction. In addition to the uncertainty originating from unplaced, observed potential feeders, the possibility of unobserved feeding will make all partial cross sections upper limits except for \(\sigma ({0}_{2}^{+})\) for which the absence of any significant feeding is argued via Fig. 2. The inclusive cross section is 0.59(4) mb.
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