1994Be24, 1998Do08: Produced from ²⁰⁸Pb(U,f) E=750 MeV/nucleon. Identified with on-line fragment separator at GSI; time of flight and energy loss measurements, no half-life measurement.

2006Mo07: ⁹Be(¹³⁶Xe,X),E=121.8 MeV/nucleon. The A1900 fragment separator at NSCL-MSU facility was used to separate nuclei of interest. The secondary beam was implanted into β-decay arrangement consisting of Si(PIN) detectors and Si strip detectors (DSSD) and single-sided Si strip detectors (SSSD). Implantation and decay events were time stamped and correlated. Measured half-life from ion-β correlated spectrum

2008Be33: ¹¹⁵Tc produced in ⁹Be(¹³⁶Xe,X),E=1 GeV/nucleon, measured production σ at GSI 2011Ni01: ¹¹⁵Tc produced in Be(²³⁸U,F),E=345 MeV/nucleon, the beam produced by the cascade operation of the RBIF complex of accelerators at RIKEN. Target=550 mg/cm². Identification of ¹¹⁵Tc 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 ¹¹⁵Tc 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: ¹¹⁵Tc 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 ¹¹⁵Tc 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 ¹¹⁵Tc 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

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

Q-value: ΔQ(β^-)=210, ΔS(n)=220, ΔS(p)=360, ΔQ(α)=360 (2012Wa38)

Q-value: Q(β^-n)=6240 200, S(2n)=9240 200, S(2p)=29980 450 (syst,2012Wa38)