39AR 27AL(14C,PNG):XUNDL-2 2019Ab05 202112 39AR c Compiled (unevaluated) dataset from 2019Ab05: Phys. Rev. C 100, 39AR2c 014310 (2019). 39AR c Compiled by S. Zhu, NNDC-BNL; October 23, 2021. 39AR c 2019Ab05: High spin states in {+39}Ar were populated via 39AR2c {+27}Al({+14}C, pn|g) reaction at a beam energy of 25.6 MeV. |g rays 39AR3c were detected by the FSU |g detector array with three 4-crystal 39AR4c clover and 7single-crystal Compton suppressed HPGe detectors grouped 39AR5c in 3 angles at 35|', 90|' and 145|' with respect to the beam 39AR6c direction. Evaporated light ions were identified by Si E-|DE 39AR7c telescope. Comparison with the shell model calculations using FSU 39AR8c cross-shell interaction including {Ispsd pf} orbitals. 39AR cG M$From measurements of R{-DCO}=I|g{-2}(at 135|' gated by |g{-1} at 39AR2cG 90|')/I|g{-2}(at 90|' gated by |g{-1} at 135|'). 39AR cL J$From the Adopted Levels (2018Ch17), unless otherwise stated. 39AR L 0 7/2- 39AR L 1267 3/2- 39AR G 1267 39AR L 1517 3/2+ 39AR G 250 39AR L 2093 5/2- 39AR G 2093 39AR L 2342.5 17 9/2- 39AR cL J$from 2019Ab05. 39AR G 2342.5 17 26 39AR L 2358 1/2+ 39AR G 841 39AR G 1092 39AR L 2481 7/2- 39AR G 388 39AR G 2481 39AR L 2503 (5/2)+ 39AR G 986 39AR L 2524 (5/2-,7/2,9/2-) 39AR G 2523 39AR L 2650.1 12 11/2- 39AR G 308.2 5 10 D 39AR cG M$from R{-DCO}=0.97 {I17} (gate: 551|g) and 1.02 {16} (gate: 1341|g). 39AR G 2649.9 12 100 39AR L 3062 (5/2-,7/2-) 39AR G 969 39AR G 3062 39AR L 3160 5/2-,7/2- 39AR G 636 39AR L 3450.7 20 11/2+ 39AR cL J$from 2019Ab05. 39AR G 1108.2 10 12 39AR L 3748 39AR G 588 39AR L 3991.0 14 13/2+ 39AR cL J$from 2019Ab05. 39AR G 540.5 2 3 D 39AR cG M$from R{-DCO}=0.95 {I28} (gate: 551|g). 39AR G 1340.6 8 84 D 39AR cG M$from R{-DCO}=0.97 {I7} (gate: 551|g) and 1.01 {I18} (gate: 992|g). 39AR L 4541.5 15 15/2+ 39AR cL J$from 2019Ab05. 39AR G 550.6 5 73 D 39AR cG M$from R{-DCO}=1.04 {I6} (gate: 992|g) and 1.02 {I5} (gate: 1341|g). 39AR L 5031 4 39AR G 1580 3 2 39AR L 5247 4 39AR G 1796 3 2 39AR L 5533.4 20 17/2+ 39AR cL J$from 2019Ab05. 39AR G 992.1 13 26 39AR L 5812.6 21 15/2+ 39AR cL J$from 2019Ab05. 39AR G 280.1 3 39AR G 1271.7 15 15 D+Q 39AR cG M$from R{-DCO}=2.0 {I15} (gate: 551|g). 39AR L 6960 3 39AR G 2418 3 2 39AR L 7072 2 39AR G 1540.2 19 2 39AR G 2530 4 2 39AR L 7380 3 39AR G 2838 4 2 39AR L 7919 3 39AR G 2386 3 2 39AR L 7980 4 39AR G 3438 4 1 39AR L 8285 3 39AR G 2752 3 2 39AR L 8357 4 39AR G 2824 3 3 39AR L 8706 3 39AR G 3173 2 8 39AR L 9024 4 39AR G 3491 3 1 39AR L 9188 3 39AR G 3655 3 5 39AR L 10183 5 39AR G 1474 3 3 39AR L 11132 5 39AR G 1944 3 2 39AR 39AR B-:XUNDL-3 2025Ad02 202509 39AR c Compiled (unevaluated) dataset from 2025Ad02: 39AR c Eur. Phys. J C 85, 728 (2025) 39AR c Compiled by E.A. McCutchan (NNDC,BNL) September 5, 2025 39AR c Direct measurement of {+39}Ar half-life using the DEAP-3600 detector. 39AR2c DEAP-3600 is located 2 km underground in the SNOLAB, Canada. 39AR3c It consists of 3269 kg of liquid argon distilled from the 39AR4c atmosphere, surrounded by 255 PMT's which observed scintillation 39AR5c light from the LAr. Used pulse-shape discrimination to 39AR6c distinguish nuclear and electron recoils. Measurement performed 39AR7c over 3.4 years. 39AR cL J$From the Adopted Levels (2018Ch17), unless otherwise stated. 39AR L 0 7/2- 302 Y 10 39AR cL T$reported as 302 y {I8} (stat) {I6} (syst) (2025Ad02), uncertainty 39AR2cL combined in quadrature by compiler.