2010Oh02: ¹²⁵Rh nuclide identified in Be(²³⁸U,F) and Pb(²³⁸U,F) reactions with a ²³⁸U⁸⁶⁺ beam energy of 345 MeV/nucleon produced by the cascade operation of the RBIF accelerator complex of the linear accelerator RILAC and four cyclotrons RRC, fRC, IRC and SRC. Identification of ¹²⁵Rh nuclei was made on the basis of magnetic rigidity, time-of-flight and energy loss of the fragments using BigRIPS fragment separator. Experiments performed at RIKEN facility. Based on α/Q spectrum and Z versus α/Q plot, 13 counts were assigned to ¹²⁵Rh isotope (Q=charge state)

2015Lo04: ¹²⁵Rh nuclide produced at RIBF-RIKEN facility in ⁹Be(²³⁸U,F) reaction at E=345 MeV/nucleon with an average intensity of 6×10¹⁰ ions/s. Identification of ¹²⁵Rh was made by determining atomic Z and mass-to-charge ratio α/Q, where Q=charge state of the ions. The selectivity of ions was based on magnetic rigidity, time-of-flight and energy loss. The separated nuclei were implanted at a rate of 50 ions/s in a stack of eight double-sided silicon-strip detector (WAS3ABi), surrounded by EURICA array of 84 HPGe detectors. Correlations were recorded between the implanted ions and β rays. The half-life of ¹²⁵Rh isotope was measured from the correlated ion-β decay curves and maximum likelihood analysis technique as described in 2014Xu07. Comparison of measured half-lives with FRDM+QRPA, KTUY+GT2 and DF3⁺CQRPA theoretical calculations

2013Fa08: theoretical calculations of T_1/2 and %β^-n

Q-value: Q(β^-), S(n) and S(p) from 2012Wa38; Q(α) from 1997Mo25

Q-value: Estimated uncertainties (2012Wa38): 640 for Q(β^-) and S(n), 780 for S(p)

Q-value: S(2n)=8840 640, Q(β^-n)=8280 590 (syst,2012Wa38). S(2p)=33780 (1997Mo25,theory)