1994Be24, 1997Be70, 1998Do08: ¹¹³Mo produced and identified in Pb,Be(²³⁸U,F), E=750 MeV/nucleon, followed by on-line fragment separator and time of flight method at GSI facility. Identification was marked as uncertain in 1994Be24 and 1997Be70

2008Be33: ¹¹³Mo produced in ⁹Be(¹³⁶Xe,X),E=1 GeV/nucleon reaction at GSI facility. Products identified in-flight by using the Fragment Separator (FRS). Measured cross section

2011Ni01: ¹¹³Mo 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 ¹¹³Mo 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 ¹¹³Mo 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: ¹¹³Mo 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 ¹¹³Mo 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 ¹¹³Mo 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

2014Sa18, 2013Fa05: theoretical calculation of T_1/2 and %β^-n

Q-value: Estimated uncertainties (2012Wa38): 300 for Q(β^-), 360 for S(n), 420 for S(p), 590 for Q(α)

Q-value: Q(β^-n)=4420 300, S(2n)=8970 300, S(2p)=29790 360 (syst,2012Wa38).