88TC 9BE(124XE,XG):T1/2,B+P:XUNDL-32019PA16 202006 88TC c Compiled (unevaluated) dataset from 2019Pa16: 88TC2c Phys Rev C 99, 034313 (2019) 88TC c Compiled by E.A. McCutchan (NNDC,BNL) August 16, 2019 88TC c {+88}Tc produced from fragmentation of a {+124}Xe beam at E=345 88TC2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 88TC3c Fragments separated by B|r-|DE-B|r method in the first stages 88TC4c of BigRIPS and then B|r-tof-B|r measurements using later stage of 88TC5c BigRIPS and the ZeroDegree spectrometer. Ions were implanted in 88TC6c WAS3ABi consisting of three double-sided silicon strip detectors 88TC7c and ten single-sided silicon strip detectors. Gamma rays were 88TC8c detected using the Euroball-RIKEN Cluster Array (EURICA) consisting 88TC9c of 84 HPGe crystals arranged in 12 clusters. 88TCac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 88TCbc |g|bp-coin, half-life, |b-delayed proton emission probability. 88TC L 0.0 5.8 S 4 88TC2 L %B+P LT 0.3 (2019Pa16) 88TC cL T$from implant-|b(t) using multiparameter fits 88TC2cL to total decay time distribution with a Bateman equation (2019Pa16). 88TC3cL Value is combined result for the ground state and the isomer. 88TC cL %B+P$from the number of |bp events divided by the total number of 88TC2cL decays as determined from the T{-1/2} analysis (2019Pa16). 88TC3cL Value is combined result for the ground state and the isomer. 88TC L 0.0+X 5.8 S 4 88TC2 L %B+P LT 0.3 (2019Pa16) 88TC cL T$from implant-|b(t) using multiparameter fits 88TC2cL to total decay time distribution with a Bateman equation (2019Pa16). 88TC3cL Value is combined result for the ground state and the isomer. 88TC cL %B+P$from the number of |bp events divided by the total number of 88TC2cL decays as determined from the T{-1/2} analysis (2019Pa16). 88TC3cL Value is combined result for the ground state and the isomer. 88TC 88RU EC DECAY:XUNDL-4 2019PA16 202006 88TC c Compiled (unevaluated) dataset from 2019Pa16 88TC c Phys. Rev. C 99, 034313 (2019) 88TC c Compiled by E.A. McCutchan (NNDC,BNL), August 16, 2019 88TC c {+88}Ru produced from fragmentation of a {+124}Xe beam at 88TC2c E=345 MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 88TC3c Fragments separated by B|r-|DE-B|r method in the first stages of 88TC4c BigRIPS and then B|r-tof-B|r measurements using later stage of 88TC5c BigRIPS and the ZeroDegree spectrometer. Ions were implanted in 88TC6c WAS3ABi consisting of three double-sided silicon strip detectors and 88TC7c ten single-sided silicon strip detectors. Gamma rays were detected 88TC8c using the Euroball-RIKEN Cluster Array (EURICA) consisting of 84 HPGe 88TC9c crystals arranged in 12 clusters. Measured E|g, I|g, |b spectra, 88TCac E(p), I(p), |b|g-coin, |bp-coin, |g|bp-coin, half-life, |b-delayed 88TCbc proton emission probability. 88TC cL E$From E|g 88TC cL J$As proposed by 2019Pa16 based on shell model calculations and decay 88TC2cL pattern. 88TC D CC$FROM BrIcc v2.3b (16-Dec-2014) 2008Ki07, "Frozen Orbitals" appr. 88RU P 0.0 0+ 1.9 S 5 7.3E3 3 88RU cP T$From 2019Pa16 88RU cP QP$From AME-2016 (2017Wa10). Value is from systematics. 88TC N 1.0 1.0 1.0 1.0 88TC cN NT$Absolute intensity is reported by 2019Pa16 88TC PN 3 88TC L X (2+) 88TC L 146.0+X 5 (1+) 88TC G 146.0 5 94 66 M1 0.098317 103 76 88TCS G KC=0.0860 15$LC=0.01021 18$MC=0.00185 4$NC=0.000295 5$OC=1.94E-5 4 88TC cG RI,TI$2019Pa16 report total intensity assuming M1 multipolarity for 88TC2cG the 146|g. I|g deduced by compiler from total intensity. 88TC E 98.67 211.33 214.05 16 100 88TCS E EAV=2.86E3 15$CK=0.0115 18$CL=0.00140 22$CM+=0.00032 5 88TC cE LOGFT$calculated taking x=0. 88TC NI(36AR,XG):ISOMER E:XUNDL-5 2019VI05 202203 88TC c Compiled (unevaluated) dataset from 2019Vi05: 88TC c Phys Rev C 100, 054333 (2019) 88TC c Compiled by E.A. McCutchan (NNDC,BNL) February 18, 2021 88TC c E({+36}Ar)=222 MeV beam was incident on a natural Ni target 88TC2c at the HIGISOL facility. Recoil products stopped and thermalized 88TC3c in helium gas of the HIGISOL ion guide, then collected and guided 88TC4c to the high-vacuum region of the mass separator using a SPIG. 88TC5c Ions then accelerated to 30 keV, mass separated, followed by 88TC6c bunching and cooling in the RFQ. Ion bunches from the RFQ were 88TC7c injected into the double-Penning trap mass spectrometer (JYFLTRAP). 88TC8c Measured masses, deduced excitation energy of isomer. 88TC cL T$From the Adopted Levels of {+88}Tc in the ENSDF database 88TC2cL (November 2013 update). 88TC cL J$Spins are proposed by 2019Vi05 based on comparison to a number of 88TC2cL shell model calculations. 2019Vi05 note that these spin assignments 88TC3cL are in conflict with 97 % {I1} of the ions being detected in the 88TC4cL ground state, as heavy-ion fusion evaporation reactions would favor 88TC5cL production of high-spin levels. 88TC L 0.0 2+ 6.4 S 8 88TC L 70.4 31 6+ 5.8 S 2 88TC cL E$from difference in mass excess values of ME=-61670 keV {I4} for 88TC2cL the ground state and -61600 keV {I5} for the isomer (2019Vi05).