101SN 105TE A DECAY:0.62 US:XUNDL-4 2010DA17 201012 101SN c Compiled (unevaluated) dataset from 2010Da17: 101SN2c Phys Rev Lett 105, 162502 (2010) 101SN c Compiled by J. Chen and B. Singh (McMaster); Dec 9, 2010 101SN c {+109}Xe was produced from heavy ion fusion evaporation reactions 101SN2c at the Holifield Radioactive Ion Beam Facility, Oak Ridge National 101SN3c Laboratory. Mass A=109 products were resolved by atomic mass-to-ionic 101SN4c charge ratio and separated using Recoil Mass Spectrometer. The 101SN5c recoiling fusion evaporation residues were implanted into a 101SN6c double-sided silicon strip detector (DSSD). |g-rays detected by the 101SN7c ancillary detector suite CARDS, comprising four large volume HPGe 101SN8c Clover detectors. Measured E|g, E|a, I|a. Deduced levels, J|p for 101SN9c {+105}Te and {+101}Sn. 101SN c Study of {+109}Xe --> {+105}Te --> {+101}Sn superallowed |a-decay chain 105TE P 0 (5/2+) 0.62 US 7 5073 21 105TE cP T$ From timing of |a decay (2006Li41) 105TE cP QP$ From E|a=4880 {I20} 101SN N 1 AP 101SN cN BR$ %|a|?100 assumed 101SN L 0.0 (7/2+) 101SN A 4880 20 11 4 101SN cA $|DL=2 transition 101SN L 172 2 (5/2+) 101SN A 4711 3 89 4 101SN cA $|DL=0 transition 101SN G 172 2 101SN 9BE(112SN,XG):T1/2,B+P:XUNDL-52012LO08 201207 101SN c Compiled (unevaluated) data set from 2012Lo08: 101SN2c Phys Rev C 86, 014313 (2012) 101SN c Compiled by E. Thiagalingam and B. Singh (McMaster); July 15, 2012. 101SN c {+101}Sn produced from fragmentation of a {+112}Sn beam at E=120 101SN2c MeV/nucleon on a 195 mg/cm{+2} {+9}Be target at the National 101SN3c Superconducting Cyclotron Laboratory (NSCL). Fragments separated by 101SN4c the A1900 Fragment Separator and the Radio Frequency Fragment 101SN5c Separator (RFFS). Ions were implanted in the double-sided silicon strip 101SN6c detector (DSSD). Detection system: NSCL Beta Counting System in 101SN7c conjunction with the SeGA Array of 16 HPGe detectors. 101SN8c Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 101SN9c |g|bp-coin, half-life, |b-delayed proton emission probability. 101SN c Total of 458 |bp coin events identified. 101SN L 0 (5/2+) 2.1 S 2 101SN2 L %B+P=22 1 (2012Lo08) 101SN cL T$ measured by 2012Lo08 from decay curves of time correlations between 101SN2cL implantations and decay radiation. Decay curves were fitted with 101SN3cL Poisson distribution using log-likelihood function by consideration 101SN4cL of decay of parent, daughter and grand-daughter. 101SN2cL correlated with implanted nuclei 101SN cL J$ from {+101}Sn Adopted Levels in ENSDF database 101SN cL %B+P$ Measured by 2012Lo08 based on observation of 458 |bp coincidence 101SN2cL events. 101SN 9BE(124XE,XG):T1/2,B+P:XUNDL-62019PA16 202006 101SN c Compiled (unevaluated) dataset from 2019Pa16: 101SN2c Phys Rev C 99, 034313 (2019) 101SN c Compiled by E.A. McCutchan (NNDC,BNL) August 16, 2019 101SN c {+101}Sn produced from fragmentation of a {+124}Xe beam at E=345 101SN2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 101SN3c Fragments separated by B|r-|DE-B|r method in the first stages 101SN4c of BigRIPS and then B|r-tof-B|r measurements using later stage of 101SN5c BigRIPS and the ZeroDegree spectrometer. Ions were implanted in 101SN6c WAS3ABi consisting of three double-sided silicon strip detectors 101SN7c and ten single-sided silicon strip detectors. Gamma rays were 101SN8c detected using the Euroball-RIKEN Cluster Array (EURICA) consisting 101SN9c of 84 HPGe crystals arranged in 12 clusters. 101SNac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 101SNbc |g|bp-coin, half-life, |b-delayed proton emission probability. 101SN L 0.0 2.22 S 5 101SN2 L %B+P=23.6 8 (2019Pa16) 101SN cL T$weighted average of 2.18 s {I9} from implant-|b(t) and 2.24 s {I6} 101SN2cL from implant-|bp(t); both analyses used multiparameter 101SN3cL fits to total decay time distribution with a Bateman equation 101SN cL %B+P$from the number of |bp events divided by the total number of 101SN2cL decays as determined from the T{-1/2} analysis (2019Pa16). 101SN 105TE A DECAY:XUNDL-7 2019XI06 202101 101SN c Compiled (unevaluated) dataset from 2019Xi06: 101SN2c Phys Rev C 100, 034315 (2019) 101SN c Compiled by J. Chen (NSCL, MSU), October 24, 2019 101SN c 2019Xi06: source of {+105}Te was from |a decay of {+109}Xe ions 101SN2c produced from fusion evaporation E=250 MeV {+58}Ni beam on 550 101SN3c |mg/cm{+2} enriched {+54}Fe target, with the beam from the tandem 101SN4c accelerator of the Japan Atomic Energy Agency (JAEA). Ions were 101SN5c separated by the Recoil Mass Separator (RMS) and implanted into the 101SN6c YAP:Ce detector at the focal plane of RMS. Measured energy spectra, 101SN7c implant-decay energy and time correlations. 101SN N 1 105TE P 0.0 (5/2+) 0.62 US 7 5069 3 105TE cP J,T$From Adopted Levels of {+105}Te in ENSDF database (2006 update) 105TE cP QP$From 2017Wa10 101SN L 0.0 101SN A 4872 101SN cA E$measured as the |a-decay energy of {+105}Te to {+101}Sn in 2019Xi06 101SN 9BE(124XE,XG):T1/2,B+P:XUNDL-82025AP05 202510 101SN c Compiled (unevaluated) dataset from 2025Ap05: 101SN2c Phys. Rev. C 112, 034310 (2025) 101SN c Compiled by E.A. McCutchan (NNDC,BNL) October 14, 2025 101SN c {+101}Sn produced from fragmentation of a {+124}Xe beam at E=345 101SN2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 101SN3c Fragments separated by BigRIPS separator 101SN4c and then |DE-B|r-tof measurements using 101SN5c plastic scintillators and MUSIC. Ions implanted into 101SN6c AIDA an array of six DSSDs. 101SN7c Gamma rays were detected 101SN8c using the Decay Total Absorption Spectrometer (DTAS) 101SN9c consisting of 16 NaI detectors. 101SNac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 101SNbc |g|bp-coin, half-life, |b-delayed proton emission probability. 101SN L 0.0 2.24 S 8 101SN2 L %B+P=20 1 (2025Ap05) 101SN cL T$weighted average of 2.3 s {I3} from implant-|b(t) and 2.24 s {I8} 101SN2cL from implant-|bp(t); both analyses used multiparameter 101SN3cL fits to total decay time distribution with a Bateman equation 101SN cL %B+P$from the number of |bp events divided by the total number of 101SN2cL decays as determined from the T{-1/2} analysis (2025Ap05).