2010Oh02: ¹²⁷Pd 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 ¹²⁷Pd 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, 70 counts in one setting and one count in another setting was assigned to ¹²⁷Pd isotope, Q=charge state

2015Lo04: ¹²⁷Pd 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 ¹²⁷Pd 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 ¹²⁷Pd 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, 2013Zh05: calculated Q values, half-life, %β^-n

Q-value: Estimated uncertainties (2012Wa38): ΔQ^-=540, ΔS(n)=ΔS(p)=ΔQ(α)=710

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

Q-value: S(2n)=9360 640, Q(β^-n)=5270 540 (syst, 2012Wa38). S(2p)=32400 (theory, 1997Mo25)