1992Ay02: ¹¹³Tc produced and identified in ²³⁸U(p,F),E=20 MeV reaction followed by on-line isotopic separator at IGISOL facility in JYFL, measured half-life

1999Wa09: measured T_1/2 and %β^-n, source from ²³⁸U(p,F) at the IGISOL facility in JYFL. Earlier T_1/2 measurement by 1998Ku17

2009Pe06: ¹¹³Tc formed by fragmentation of ¹³⁶Xe beam at 120 MeV/nucleon at NSCL-MSU facility using Coupled Cyclotrons and A1900 fragment separator. The time-of-flight and transversal positions of each particle was measured using two plastic scintillators. The ΔE energy loss in a Si PIN detector was measured which, when combined with time-of-flight (tof) and transversal position measurements, allowed for an event-by-event identification of the transmitted nuclei. Transmitted nuclei and their β decays were measured using the β counting system consisting of four Si PIN detectors and a double-sided Si strip detector. β-delayed neutrons were measured in coincidence with β-decay precursor using neutron emission ratio observer (NERO) detector consisting of 60 proportional gas counter tubes embedded in polyethylene moderator matrix. The γ rays were measured with SeGA Ge detectors. Measured isotopic half-lives and delayed neutron emission probabilities Isotopic half-life was measured by 2009Pe06 from maximum likelihood method of time differences of implantations and correlated β decay events.

2015Lo04: ¹¹³Tc 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 ¹¹³Tc 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 ¹¹³Tc 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

Mass measurement: 2011Ha48

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

Q-value: Estimated uncertainty=200 for S(p) (2012Wa38)

Q-value: Q(β^-)n=4746 10, S(2n)=9932 11, S(2p)=28510 300 (syst) (2012Wa38)