25P ADOPTED LEVELS 25NDS 202508 25P H TYP=FUL$AUT=M. Shamsuzzoha Basunia, Anagha Chakraborty$ 25P 2 H CIT=NDS 205, 1 (2025)$CUT=31-May-2025$ 25P d Dataset by A. CHAKRABORTY 25P Q 2.19E4 SY-2.16E3 SY-9.32E3 SY 2021Wa16 25P XA9BE(32S,XG) 25P L 0.0 (1/2+) 38 NS LT ? 25P 2 L %P=100 25P X L XREF=A 25P cL T$from 2011Fo08 25P cL J$from mirror analog 1/2{++} ground state of {+25}Ne (2010Ca10); 25P 2cL predicted result from shell model calculation (2015Fe02) 25P 9BE(32S,XG) 2011FO08 25NDS 202508 25P H TYP=FUL$AUT=M. Shamsuzzoha Basunia, Anagha Chakraborty$ 25P 2 H CIT=NDS 205, 1 (2025)$CUT=31-May-2025$ 25P d Dataset by A. CHAKRABORTY 25P c Adapted/Edited the XUNDL data set compiled by B. Singh (McMaster), 25P 2c Oct 20, 2011. 25P c Search for {+25}P nuclide and its possible proton decay mode was made. 25P c E=50.3 MeV/nucleon {+32}S beam from U400M cyclotron bombarded a 25P 2c {+9}Be target of 92.4 mg/cm{+2} thickness. Fragments were separated 25P 3c by ACCULINNA fragment separator at JINR, Dubna. Time-of-flight-|DE and 25P 4c |DE-E techniques using plastic scintillators and Si strip detectors 25P 5c were used to identify the fragments. The fragment separator was 25P 6c sequentially tuned for optimum transmission of {+26}S, {+27}S, {+28}S, 25P 7c and {+29}S. Total time of flight through the separator was 314-322 ns. 25P 8c From systematics of fragmentation cross sections, the expected events 25P 9c due to {+25}P are 360 {I+85-70}, but no events could be ascribed to 25P ac this nuclide in the concerned experiment. 25P L 0 38 NS LT ? 25P cL T$from 2011Fo08; estimated (with 63% confidence level) from flight 25P 2cL time of 314-322 ns, Poisson statistics of the observed distribution 25P 3cL (2011Fo08) of one to four events. At 98% confidence level, 25P 4cL the estimation gives T{-1/2}<50 ns (2011Fo08). 25P 5cL Others: <30 ns (1996PoZZ).