218AC 222PA A DECAY:XUNDL-3 2021Hu18 202108 218AC c Compiled (unevaluated) dataset from 2021Hu18: Chin. Phys. C 45, 218AC2c 044001 (2021). 218AC c Compiled by S. Zhu, NNDC-BNL, July 14, 2021 218AC c 2021Hu18: {+222}Pa was produced in {+186}W({+40}Ar,p3n) with a beam 218AC2c at 198.7 MeV bombarding a {+186}W target with a thickness of 200 218AC3c |mg/cm{+2}; evaporation residues (Er) were separated in-flight by the 218AC4c gas-filled recoil separator SHANS and implanted in three 16-strip 218AC5c position-sensitive silicon detectors (PSSDs) mounted side-by-side at 218AC6c the focal plane. {+222}Pa was identified by Er-|a-|a-|a time and 218AC7c position correlations. Measured E|a, I|a and T{-1/2}. 218AC cA HF$r{-0}({+218}Ac)=1.561 {I16}, unweighted average of 218AC2cA r{-0}({+218}Ra)=1.5571 {I17}, r{-0}({+216}Ra)=1.6051 {I43}, 218AC3cA r{-0}({+220}Th)=1.5514 {I30}, r{-0}({+218}Th)=1.529 {I15} from 218AC4cA 2020Si16. 218AC cL E$Level energies are deduced from E|a1=8636 keV {I15}, which is 218AC2cL consistent with Q|a=8790 keV {I60}, as g.s. to g.s. decay and E|a 218AC3cL values given here. 218AC cA E$From 2021Hu18. 222PA P 0 2.76 MS +43-33 8.79E+3 6 222PA cP QP$from 2021Wa16. 222PA cP T$from 2021Hu18. 218AC N 1.0 1.0 218AC PN 2 218AC L 0 0.87 US +18-7 218AC cL T$from 2021Hu18. 218AC A 8636 1524.9 188 218AC L 113 22 218AC A 8525 1615.9 147 218AC L 203 22 S 218AC A 8437 1619.9 67 S 218AC L 303 22 218AC A 8338 1614.4 49 218AC L 393 22 218AC A 8250 1619.2 20 218AC L 589 24 218AC A 8058 185.7 18 218AC 184W(40CA,X):T,EA:XUNDL-4 2019YA04 202205 218AC c Compiled (unevaluated) dataset from 2019Ya04: 218AC2c Eur. Phy. J A 55, 8 (2019) 218AC c Compiled by E.A. McCutchan (NNDC,BNL) April 28, 2022 218AC c E({+40}Ca)=206 MeV from the Sector-Focusing Cyclotron (SFC) 218AC2c of the Heavy Ion Research Facility in Lanzhou (HIRFL). 218AC3c Evaporation residues were identified 218AC4c and separated using SHANS separator and implanted into three 300-|mm 218AC5c double-sided silicon strip detectors. Measured E|a, I|a, 218AC6c (evaporation residue)|a correlations. Deduced T{-1/2} using digital 218AC7c pulse fitting method. 218AC L 0 1.04 US 12 218AC cL T$from 9204|a(t) (2019Ya04) 218AC cL $Measured E|a=9204 keV {I25} (2019Ya04) extracted from pile-up traces. 218AC 186W(40AR,X):T,EA:XUNDL-5 2023LU04 202403 218AC c Compiled (unevaluated) dataset from 2023Lu04: 218AC2c Phys. Rev. C 108, 014302 (2023) 218AC c Compiled by E.A. McCutchan (NNDC,BNL) January 29, 2024 218AC c E({+40}Ar)=188 MeV from the Sector-Focusing Cyclotron (SFC) 218AC2c of the Heavy Ion Research Facility in Lanzhou (HIRFL). 218AC3c Evaporation residues were identified 218AC4c and separated using SHANS separator and implanted into a 218AC5c double-sided silicon strip detector. Measured E|a, I|a, 218AC6c (evaporation residue)|a correlations. Deduced T{-1/2}. 218AC L 0 1.22 US 12 218AC cL T$from 9219|a(t) (2023Lu04) 218AC cL $Measured E|a=9219 keV {I6} (2023Lu04) extracted from 218AC2cL general least-square superpulse fitting algorithm.