36P 208PB(36S,XG):XUNDL-1 2015CH56 201511 36P c Compiled (unevaluated) dataset from 2015Ch56: Phys Rev C 92, 044308 36P 2c (2015) 36P c Compiled by: J. Chen (NSCL, MSU), October 15, 2015 36P c 2015Ch56: E= 215 MeV {+36}S beam was produced using the combination 36P 2c of XTU tandem Van de Graaff accelerator and ALPI superconducting 36P 3c linear accelerator at the INFN Legnaro National Laboratory, Italy. 36P 4c Target was 99.7% enriched {+208}Pb with a thickness of 300 |mg/cm{+2} 36P 5c on a 20 |mg/cm{+2} carbon backing. Fragments were separated and 36P 6c identified by the PRISMA spectrometer and |g rays were detected with 36P 7c the CLARA array of 25 EUROBALL escape-suppressed HPGe clover 36P 8c detectors. Measured E|g, I|g. Deduced levels, J,|p. Comparisons with 36P 9c shell-model calculations. 36P cL E$From a least-squares fit to |g-ray energies (by compiler) 36P cL E(A),J$Level proposed by 2015Ch56, unless otherwise noted. 36P PN 5 36P G 152 1 2.7 6 36P G 471 1 5.9 9 36P L 0 4- 36P cL J$from Adopted Levels of {+36}P in ENSDF database 36P L 249.0 9 (3-) 36P G 249 1 100 4 36P L 423.0 9 (2-) 36P cL J$(1+) from Adopted Levels of {+36}P in ENSDF database. 2015Ch56 36P 2cL argue that J|p =(1+) would result in E3 and M2 depopulating 36P 3cL transitions and a level lifetime long enough that the de-excitation 36P 4cL |g-rays would not have been observed at the target position. 36P G 174 1 18.8 9 36P G 423 1 8.4 9 36P L 1344.0 13 (1-) 36P G 921 1 13.4 14 36P L 2030 1 (5-) A 36P G 2030 1 36.2 20 ? 36P L 2644 1 (4-) 36P G 614 1 12.1 13 ? 36P L 5212 1 (7+) A 36P G 3182 1 18.6 17 ? 36P 208PB(36S,XG):XUNDL-2 2019GR08 202003 36P c Compiled (unevaluated) dataset from 2019Gr08: 36P 2c Phys Rev C 100, 064308 (2019) 36P c Compiled by B. Singh (McMaster), December 31, 2019 36P c 2019Gr08: E({+36}S)=225 MeV beam was provided by Tandem-ALPI 36P 2c accelerator complex at the INFN Legnaro National Laboratory. 36P 4c Target was 99.7% enriched in {+208}Pb with a thickness of 1 mg/cm{+2} 36P 5c deposited on 1 mg/cm{+2} Nb backing, and mounted onto Cologne 36P 6c differential plunger. Recoiling projectile-like fragments were 36P 7c separated and identified by the PRISMA magnetic spectrometer. 36P 8c The |g rays were detected with the AGATA demonstrator array of 36P 9c five triple cluster modules of 36-fold segmented Ge crystals 36P Ac at a distance of 18 cm from the reaction target position, covering 36P Bc backward angles 135|' to 175|'. Measured E|g, ({+36}P)|g-coin, and 36P Cc and level lifetimes using differential recoil-distance method. 36P Dc Comparison with shell-model calculations using PSDPF effective 36P Ec interaction. 36P c Level scheme, including J|p values, is from a previous paper by the 36P 2c same experimental group: 2015Ch56: Phys. Rev. C 92, 044308 (2015) 36P cG E(x)$This |g is not shown in spectral Fig. 22 of 2019Gr08 36P cL T$From differential recoil-distance method (DRDM) 36P 2cL (2019Gr08) 36P G 471 36P L 0 4- 36P L 249 (3-) 36P G 249 36P L 423 (2-) 36P G 174 x 36P G 423 36P L 1344 (1-) 36P G 921 36P L 2030 (5-) 0.69 PS LT 36P cL T$estimated mean lifetime |t<1 ps. Correction due to feeding from 36P 2cL (4-) and (7+) levels could not be applied due to poor statistics 36P 3cL (2019Gr08) 36P G 2030 ? 36P L 2644 (4-) 36P G 614 x ? 36P L 5212 (7+) 1.87 PS 42 36P cL T$measured mean lifetime |t=2.7 ps {I6} (2019Gr08). There is no 36P 2cL observed feeding from higher levels. 36P G 3182 ?