2008Oh06: ¹²⁵Pd nuclide identified in ⁹Be(²³⁸U,X) reaction 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 ¹²⁵Pd 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, 22 counts were assigned to ¹²⁵Pd isotope. (Q=charge state)

2008Be33: identification and production of ¹²⁵Pd nuclide in Be(¹³⁶Xe,X) reaction at E(¹³⁶Xe)=1 GeV/nucleon, beam provided by SIS18 synchrotron at GSI facility. The fragments were analyzed using FRS magnetic separator on the basis of magnetic rigidity and time-of-flight. Atomic number of residual nucleus was determined from energy loss in an ionization chamber MUSIC

2015Lo04: ¹²⁵Pd 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 ¹²⁵Pd 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 ¹²⁵Pd 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

Q-value: Estimated uncertainties (2012Wa38): 720 for Q(β^-), 500 for S(n), 570 for S(p) and Q(α)

Q-value: S(2n)=9950 450, S(2p)=31440 640, Q(β^-n)=3910 470 (syst,2012Wa38)