1997Be70: ¹¹⁴Mo produced in Pb(²³⁸U,F),E=750 MeV/nucleon reaction and identified by time-of-flight at GSI

2011Ni01: ¹¹⁴Mo 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 ¹¹⁴Mo 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 ¹¹⁴Mo 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: ¹¹⁴Mo 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 ¹¹⁴Mo 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 ¹¹⁴Mo 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

Structure calculations: 2010Bo12, 2010Ou01, 1997Sk01

Q-value: Estimated uncertainties (2012Wa38): ΔQ(β^-)=320, ΔS(n)=420, ΔS(p)=500, ΔQ(α)=670

Q-value: Q(β^-n)=4930 300, S(2n)=8490 360, S(2p)=30570 760 (syst, 2012Wa38)