93BR 9BE(136XE,X):T1/2:XUNDL-1 2012QU01 201204 93BR c Compiled (unevaluated) dataset from 2012Qu01: 93BR2c Phys Rev C 85, 035807 (2012). 93BR c Compiled by M. Birch and B. Singh (McMaster); April 23, 2012. 93BR c {+136}Xe primary beam, E=120 MeV/nucleon, impinged on a 235 mg/cm{+2} 93BR2c Be target. Experiment performed at the NSCL Coupled Cyclotron 93BR3c Facility. Fragments were separated by the A1900 fragment separator 93BR4c using the B|r-|DE-B|r technique. Beta decays measured in the NSCL Beta 93BR5c Counting System (BCS) consisting of four silicon PIN detectors, a 93BR6c double sided silicon strip detector (DSSD), and a single sided silicon 93BR7c strip detector (SSSD). Measured energy loss, total kinetic energy 93BR8c (TKE), time of flight, and isotopic half-life 93BR cL J$ From Adopted dataset for {+93}Br in ENSDF database 93BR L 0.0 (5/2-) 69 MS +40-25 93BR cL $ Total of 45 implantations observed, and 20 correlated decay 93BR2cL sequences. 93BR cL T$ value listed in table I is: 69 ms {I1} (syst) {I+40-25} (stat); 93BR2cL maximum-likelihood method for T{-1/2} analysis. 93BR3cL Value in Adopted dataset for {+93}Br in ENSDF database is 102 ms {I10}. 93BR 9BE(238U,FG):XUNDL-2 2024DU09 202410 93BR c Compiled (unevaluated) dataset from 2024Du09: 93BR2c Phys Rev C 110, 034304 (2024) 93BR c Compiled by E.A. McCutchan (NNDC,BNL) October 18, 2024 93BR c Two experiments were performed. In the first, {+238}U beam with 93BR2c 6.2 MeV/nucleon was incident on a {+9}Be target. VAMOS++ was 93BR3c used to separate fission fragments and E|g, I|g, recoil-|g was 93BR4c measured using the AGATA array. In the second experiment 93BR5c fission fragments were produced from thermal neutron induced fission 93BR6c of {+235}U at the ILL in Grenoble. Measured E|g, I|g, |g|g using 93BR7c 16 HPGe Clover detectors. 93BR cL E$From a least-squares fit to |g-ray energies (by compiler) 93BR cL J$As given in 2024Du09 93BR cG E$From AGATA experiment. Uncertainty includes a systematic 0.2 93BR2cG keV uncertainty. 93BR cL $Level scheme is tentative due to low statistics and lack of 93BR2cL gamma-gamma coincidences. Deduced from systematic comparison with 93BR3cL Se isotopes. 93BR G 233 2 93BR G 619 2 93BR G 883 2 93BR L 0.0 (5/2-) ? 93BR L 426 2 (7/2-) ? 93BR G 426 2 ? 93BR L 741 2 (9/2-) ? 93BR G 741 2 ? 93BR L 1116 3 (11/2-) ? 93BR G 690 2 ?