26P BE(32S,X):T1/2:XUNDL-1 2017JA05 201704 26P c Compiled (unevaluated) dataset from 2017Ja05: 26P 2c Phy. Rev. C 95, 034315 (2017) 26P c M.S. Basunia (LBNL): Apr 17, 2017 26P c {+26}P obtained from {+32}S fragmentation from Be({+32}S,X), E=51.3 26P 2c MeV/nucleon, reaction; isotopes were separated using the ACCULINNA 26P 3c fragment separator at JINR, Dubna, Russia facility. Fragments were 26P 4c identified by time-of-flight (tof) and energy-loss technique using 26P 5c plastic scintillator and a silicon detector, respectively. Selected 26P 6c fragments were analyzed by Optical Time Projection Chamber (OTPC), 26P 7c filled with 49.5% Ar, 49.5% He, and 1% Co{-2} at atmospheric pressure. 26P 8c Light produced in the gas was recorded by a digital camera (CCD) and a 26P 9c photomultiplier (PMT) connected to an oscilloscope; the combination 26P ac of data from the CCD and the PMT was used to reconstruct particle 26P bc tracks in three dimensions. 26P c Setup was tuned for {+27}S ions, but {+26}P was also accepted. In total 26P 2c 2497 events of {+26}P were identified, of which 2463 events based on 26P 3c depth profile were inspected to select decay events. 26P L 0.0 (3)+ 50 MS +23-12 26P cL $%|e+%|b+=100; %|ep=33.5 {I20}; %|e2p=1.5 {I4}; %|ep+%|e2p=35 {I2} 26P cL J$From {+26}P Adopted Levels in the ENSDF database. 26P cL T$Measured by 2017Ja05 from 477 {+26}P implant-p(t) analysis by 26P 2cL maximum likelihood method. 26P cL $%|e2p and %|ep+%|e2p values from 2017Ja05. %|ep by compiler - 26P 2cL subtracted value of %|e2p from %|ep+%|e2p. 26P BE(36AR,X):XUNDL-2 2017PE09 201711 26P c Compiled (unevaluated) dataset from 2017Pe09: 26P 2c Phy. Rev. C 96, 014306 (2017) 26P c M.S. Basunia (LBNL): Aug 30, 2017 26P c {+26}P obtained from {+36}Ar fragmentation from Be({+36}Ar,X), E=150 26P 2c MeV/nucleon, reaction; Isotopes were separated using the A1900 26P 3c fragment separator at NSCL. The secondary beam was purified by means 26P 4c of the Radio-Frequency Fragment Separator and implanted into a planar 26P 5c germanium double-sided strip detector (GeDSSD). Isotopic identification 26P 6c of the secondary beam particle was done by time-of-flight (tof) and 26P 7c energy-loss technique using plastic scintillator and a pair of silicon 26P 8c detectors, respectively. |g rays were detected in coincidence with the 26P ac implantation signal using high-purity segmented Ge array (SeGA - 26P bc 32-fold segmented germanium detectors). 26P cc Measured E|g, half-life of excited state, isomeric state production 26P dc probability. 26P c Estimated Sp ({+26}P) |> -135 keV (2017Pe09). 26P 2c Sp ({+26}P) = 140 (sys) {I200} (sys) (AME2016 - 2017Wa10). 26P L 0.0 (3)+ 26P cL J$From {+26}P Adopted Levels in the ENSDF database. 26P L 164.4 4 104 NS 14 26P cL E$From E|g, assuming g.s. feeding by the compiler. 26P cL T$Deduced by fitting 164|g(t) using maximum likelihood method 26P 2cL (2017Pe04). 26P cL $An isomeric ratio R, probability of {+26}P production in an isomeric 26P 2cL state, 14% {I10} (2017Pe09). This value is much lower than 97% {I+3-10} 26P 3cL measured by 2014NiZZ. This difference may be due to different 26P 4cL production mechanism of {+26}P, noted in 2017Pe09. 26P cL $|G{-|g}=4.39 neV {I59}, 2017Pe09 deduce from measured half-life to 26P 2cL estimate proton separation energy. 26P G 164.4 4 26P cG E$Reported as 164.4 {I3} (sys) {I2} (stat) (2017Pe09) 26P BE(26SI,X):XUNDL-3 2019LO06 202006 26P c Compiled (unevaluated) dataset from 2019Lo06: 26P c Phy. Rev. C 99, 064330 (2019) 26P c Compiled by E.A. McCutchan (NNDC,BNL) April 1, 2020 26P c Includes {+9}Be({+27}P,X) 26P c {+26}Si obtained from {+36}Ar fragmentation with E({+36}Ar)=150 26P 2c MeV/nucleon. Secondary beam contained 14% {+26}Si at 118 26P 3c MeV/nucleon. Isotopes were separated using the A1900 26P 4c fragment separator at NSCL. The secondary beam was incident on 26P 5c a 287 mg/cm{+2} Be target placed at the reaction target position of 26P 6c the S800 spectrograph. Isotopic identification 26P 7c of the secondary beam particle was done by time-of-flight (tof) and 26P 8c energy-loss technique using plastic scintillator and a pair of silicon 26P 9c detectors, respectively. Measured E|g, I|g, |g(t) using the 26P ac CAESAR array consisting of 192 closely-packed CsI(Na) scintillators. 26P bc Additionally, data were taken with the SeGA array consisting of 32- 26P cc fold segmented HPGe detectors. 26P L 0.0 (3)+ 26P cL J$From {+26}P Adopted Levels in the ENSDF database. 26P L 164 3 (1+) 26P cL E$transition from this level not observed as decay occurred far beyond 26P 2cL the target position. 26P cL J$proposed by 2019Lo06 based on shell model calculations and comparison 26P 2cL to mirror nuclei. 26P L 244 3 (2+) 26P cL J$proposed by 2019Lo06 based on shell model calculations and comparison 26P 2cL to mirror nuclei. 26P G 80 3 100 11 26P cG E$weighted average of 79.5 {I35} from SeGA measurement and 81 {I6} from 26P 2cG CAESAR measurement 26P G 244 3 46 11 26P cG E$weighted average of 242.5 {I40} from SeGA measurement and 246 {I5} 26P 2cG from CAESAR measurement 26P cG RI$branching from 244-keV level is I|g(80):I|g(244)=s100 {I13}:49 {I13} 26P 2cG from SeGA measurement and 100 {I21} : 39 {I21} from CAESAR measurement. 26P 3cG 2019Lo06 give a weighted average of the two values. 26P BE(32S,X):T1/2:XUNDL-4 2020LI06 202011 26P c Compiled (unevaluated) dataset from 2020Li06: 26P 2c Phy. Rev. C 101, 024305 (2020) 26P c Compiled by E.A. McCutchan (NNDC,BNL) November 30, 2020 26P c {+26}P from fragmentation of {+32}S with E=80.6 MeV/nucleon. 26P 2c Reaction products separated and purified by RIBLL1 in Lanzhou. 26P 3c Ions identified by time-of-flight and energy loss. 26P 4c Detection system consisted of three double sided-silicon strip 26P 5c detectors, five Clover-type HPGe detectors, and five quadrant 26P 6c silicon detectors. Deduced T{-1/2} of ground state. 26P L 0.0 (3)+ 43.6 MS 3 26P cL J$From {+26}P Adopted Levels in the ENSDF database. 26P cL T$from {+26}P implant-|b-p(t) events fitted with an exponential 26P 2cL and a constant background (2020Li06).