2010Oh02: ¹¹⁵Mo 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 ¹¹⁵Mo 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, 933 counts were assigned to ¹¹⁵Mo isotope. (Q=charge state)

2011Ni01: ¹¹⁵Mo nuclide produced in Be(²³⁸U,F) reactions at E=345 MeV/nucleon produced by the cascade operation of the RBIF complex of accelerators at RIKEN. Target=550 mg/cm². Identification of ¹¹⁵Mo made on the basis of magnetic rigidity, time-of-flight and energy loss. The separated nuclei were implanted in a nine-layer double-sided silicon-strip detector (DSSSD). Correlations were recorded between the heavy ions and β rays. The half-life of ¹¹⁵Mo isotope was measured from the correlated ion-β decay curves and maximum likelihood analysis technique. In the analysis of the decay curve, β-detection efficiency, background rate, daughter and granddaughter (including those populated in delayed neutron decays) half-lives, and β-delayed neutron emission probabilities were considered. Comparison of measured half-lives with FRDM+QRPA and KTUY+GT2 calculations

2015Lo04: ¹¹⁵Mo 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 ¹¹⁵Mo 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 ¹¹⁵Mo 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

1995CzZZ: preliminary report suggesting formation of ¹¹⁵Mo (figure 2 in 1995CzZZ) produced in ²⁰⁸Pb(U,F) reaction at E=750 MeV/nucleon; on-line fragment separator at GSI; time of flight and energy loss technique. However, this isotope was not listed in authors’ later publications of the same or similar studies: 1997Be70 and 1997Be12. This would suggest that identification of ¹¹⁵Mo was probably uncertain in this study

2013Fa05: theoretical calculations of T_1/2 and %β^-n

Q-value: Estimated uncertainties (2012Wa38): ΔQ(β^-)=450, ΔS(n)=500, ΔS(p)=640, ΔQ(α)=810

Q-value: Q(β^-n)=5950 410, S(2n)=8120 500 (syst,2012Wa38). S(2p)=31950 (theory,1997Mo25)