92RH 9BE(124XE,XG):XUNDL-3 2017PA35 201712 92RH c Compiled (unevaluated) dataset from 2017Pa35: 92RH2c Phys Rev C 96, 044311 (2017) 92RH c Compiled by Y. Ichikawa (RIKEN) and F.G. Kondev (ANL); 92RH2c November 9, 2017 92RH c 2017Pa35: The {+92}Rh nucleus was produced by fragmentation reaction 92RH2c using {+124}Xe beam at E=345 MeV/nucleon incident on a 740 mg/cm{+2} 92RH3c thick {+9}Be target at the RIKEN-RIBF facility. The identification of 92RH4c the nuclide of interest was made through the BigRIPS separator and the 92RH5c ZeroDegree spectrometer by determining the atomic number and the 92RH6c mass-to-charge ratio of the ion using the tof-B|r-|DE method. The 92RH7c secondary beam was stopped in the double-sided silicon strip detector 92RH8c of the WAS3ABi spectrometer. The |g rays were detected by EURICA array 92RH9c comprising of 84 HP Ge detectors. Measured: E|g, I|g and T{-1/2}. 92RH D ------------------------------------------------------ 92RH cL E$From least-squares fit to E|g. 92RH cL J,T$From adopted levels in ENSDF, unless otherwise stated 92RH L 0.0 (GE6+) 4.66 S 25 92RH L 0.0+X (2+) 0.53 S 37 92RH L 55.3+X 3 (4+) 0.23 US 6 92RH cL E$Isomeric ratio R=6.8 % {I32} (2017Pa35) 92RH cL J$Proposed in 2017Pa35 92RH cL T$From 55.3|g(t) in 2017Pa35 92RH G 55.3 3 100 [E2] 11.2 3 92RH cG E,RI,M$From 2017Pa35 92RH cG $B(E2)(W.u.)=16 {I5} (by compilers) 92RH 9BE(124XE,XG):T1/2,B+P:XUNDL-42019PA16 202006 92RH c Compiled (unevaluated) dataset from 2019Pa16: 92RH2c Phys Rev C 99, 034313 (2019) 92RH c Compiled by E.A. McCutchan (NNDC,BNL) August 16, 2019 92RH c {+92}Rh produced from fragmentation of a {+124}Xe beam at E=345 92RH2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 92RH3c Fragments separated by B|r-|DE-B|r method in the first stages 92RH4c of BigRIPS and then B|r-tof-B|r measurements using later stage of 92RH5c BigRIPS and the ZeroDegree spectrometer. Ions were implanted in 92RH6c WAS3ABi consisting of three double-sided silicon strip detectors 92RH7c and ten single-sided silicon strip detectors. Gamma rays were 92RH8c detected using the Euroball-RIKEN Cluster Array (EURICA) consisting 92RH9c of 84 HPGe crystals arranged in 12 clusters. 92RHac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 92RHbc |g|bp-coin, half-life, |b-delayed proton emission probability. 92RH L 0.0 5.61 S 8 92RH2 L %B+P=2.2 1 (2019Pa16) 92RH cL T$weighted average of 5.60 s {I9} from implant-|b(t) and 5.67 s 92RH2cL {I26} from implant-|bp(t); both analyses used multiparameter fits 92RH3cL to total decay time distribution with a Bateman equation (2019Pa16). 92RH cL %B+P$from the number of |bp events divided by the total number of 92RH2cL decays as determined from the T{-1/2} analysis (2019Pa16). 92RH L 0.0+X 3.18 S 22 92RH2 L %B+P=1.7 3 (2019Pa16) 92RH cL T$weighted average of 3.18 s {I22} from implant-|b(t) and 2.6 s 92RH2cL {I+14-7} from implant-|bp(t); both analyses used multiparameter fits 92RH3cL to total decay time distribution with a Bateman equation (2019Pa16). 92RH cL %B+P$from the number of |bp events divided by the total number of 92RH2cL decays as determined from the T{-1/2} analysis (2019Pa16). 92RH 92PD EC DECAY:XUNDL-5 2019PA16 202006 92RH c Compiled (unevaluated) dataset from 2019Pa16 92RH c Phys. Rev. C 99, 034313 (2019) 92RH c Compiled by E.A. McCutchan (NNDC,BNL), August 16, 2019 92RH c {+92}Pd produced from fragmentation of a {+124}Xe beam at E=345 92RH2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 92RH3c Fragments separated by B|r-|DE-B|r method in the first stages of 92RH4c BigRIPS and then B|r-tof-B|r measurements using later stage of 92RH5c BigRIPS and the ZeroDegree spectrometer. Ions were implanted in 92RH6c WAS3ABi consisting of three double-sided silicon strip detectors and 92RH7c ten single-sided silicon strip detectors. Gamma rays were detected 92RH8c using the Euroball-RIKEN Cluster Array (EURICA) consisting of 84 HPGe 92RH9c crystals arranged in 12 clusters. Measured E|g, I|g, |b spectra, 92RHac E(p), I(p), |b|g-coin, |bp-coin, |g|bp-coin, half-life, |b-delayed 92RHbc proton emission probability. 92RH cL J$As proposed by 2019Pa16 92RH cL E$From E|g 92PD P 0.0 0+ 1.06 S 3 8.17E3 33 92PD cP QP$from beta endpoint measurement in 2019Pa16 92PD cP T$from 2019Pa16 92RH N 0.984 0.984 1.0 1.0 92RH cN NR$considering %|b{++}p=1.6 {I2} 92RH L X (2+) 92RH L 256.7+X 1 (1+) 92RH G 256.7 1 [M1] 85 5 92RH E 82 5 0.96 164.10 11 83 5 92RHS E EAV=3.23E3 17$CK=0.0100 16$CL=0.00123 19$CM+=0.00029 5 92RH cE LOGFT$calculated assuming x=0 92RH 9BE(124XE,XG):XUNDL-6 2019HA26 202404 92RH c Compiled (unevaluated) dataset from 2019Ha26: 92RH2c Phys Rev C 100, 024302 (2019) 92RH c Compiled by E.A. McCutchan (NNDC,BNL) February 21, 2024 92RH c {+92}Rh nucleus was produced in fragmentation of a 92RH2c {+124}Xe beam at E=345 MeV/nucleon incident on a 4-mm 92RH3c thick {+9}Be target at the RIKEN-RIBF facility. Identification of 92RH4c the nuclei of interest was made through the BigRIPS separator and the 92RH5c ZeroDegree spectrometer. The secondary ions were implanted into 92RH6c modified SIMBA active stopper detector. 92RH7c |g rays were measured by EURICA array 92RH8c consisting of 84 HP Ge detectors. Measured: E|g, I|g and T{-1/2}. 92RH L 0.0 92RH L 0.0+X (2+) 92RH L 55+X (4+) 0.232 US 15 92RH cL T$from 55|g(t) (2019Ha26) 92RH G 55 92RH 9BE(124XE,XG):XUNDL-7 2025AP05 202510 92RH c Compiled (unevaluated) dataset from 2025Ap05: 92RH2c Phys. Rev. C 112, 034310 (2025) 92RH c Compiled by E.A. McCutchan (NNDC,BNL) October 14, 2025 92RH c {+92}Rh produced from fragmentation of a {+124}Xe beam at E=345 92RH2c MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan. 92RH3c Fragments separated by BigRIPS separator 92RH4c and then |DE-B|r-tof measurements using 92RH5c plastic scintillators and MUSIC. Ions implanted into 92RH6c AIDA an array of six DSSDs. 92RH7c Gamma rays were detected 92RH8c using the Decay Total Absorption Spectrometer (DTAS) 92RH9c consisting of 16 NaI detectors. 92RHac Measured E|g, I|g, |b spectra, E(p), I(p), |b|g-coin, |bp-coin, 92RHbc |g|bp-coin, half-life, |b-delayed proton emission probability. 92RH L 0.0 5.6 S 1 92RH cL T$weighted average of 5.6 s {I1} from implant-|b(t) and 5.6 s 92RH2cL {I5} from implant-|bp(t); both analyses used multiparameter fits 92RH3cL to total decay time distribution with a Bateman equation (2025Ap05). 92RH L 0.0+X 3.5 S 4 92RH cL T$from implant-|bp(t) using 92RH2cL multiparameter fits 92RH3cL to total decay time distribution with a Bateman equation (2025Ap05).