119RH BE(238U,F):T1/2:XUNDL-2 2015LO04 201506 119RH c Compiled (unevaluated) dataset from 2015Lo04: 119RH2c Phys Rev Lett 114, 192501 (2015) 119RH c Compiled by B. Singh (McMaster); June 17, 2015 119RH c 2015Lo04: {+119}Rh nuclide produced at RIBF-RIKEN facility in 119RH2c {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon with an average 119RH3c intensity of 6|*10{+10} ions/s. Identification of {+119}Rh was made by 119RH4c determining atomic Z and mass-to-charge ratio A/Q, where Q=charge state 119RH5c of the ions. The selectivity of ions was based on magnetic rigidity, 119RH6c time-of-flight and energy loss. The separated nuclei were implanted at 119RH7c a rate of 50 ions/s in a stack of eight double-sided silicon-strip 119RH8c detector (WAS3ABi), surrounded by EURICA array of 84 HPGe detectors. 119RH9c Correlations were recorded between the implanted ions and |b rays. The 119RHAc half-life of {+119}Rh isotope was measured from the correlated ion-|b 119RHBc decay curves and maximum likelihood analysis technique as described in 119RHCc 2014Xu07 (Phys. Rev. Lett. 113, 032505). Comparison of measured 119RHDc half-lives with FRDM+QRPA, KTUY+GT2 and DF3+CQRPA theoretical 119RHEc calculations 119RH L 0 (7/2+) 190 MS 6 119RH2 L %B-=100$ %B-N=6.4 16 119RH cL J,%B-N$from Adopted Levels of {+119}Rh in ENSDF database; J|p 119RH2cL from systematics 119RH cL $Theoretical T{-1/2}{-1/2}=107.6 ms, %|b{+-}n=3.77 (2003Mo09) 119RH cL E$the measured half-life is assumed to correspond to the ground state 119RH2cL of {+119}Rh 119RH cL T$measured by 2015Lo04 from the analysis of the (implanted ions)|b 119RH2cL correlated decay curve in time and position. Earlier value: 119RH3cL 171 ms {I18} (Adopted Levels of {+119}Rh in ENSDF database, value 119RH4cL taken from 2006Mo07: Phys. Rev. C73, 035801) 119RH 9BE(238U,FG):XUNDL-3 2017NA04 201707 119RH c Compiled (unevaluated) data set from 2017Na04: 119RH2c Phys Lett B 767, 480 (2017) 119RH c Compiled by B. Singh (McMaster); July 2, 2017. 119RH c 2017Na04: excited states in {+119}Rh were studied by their 119RH2c population in the fission of 6.2 MeV/nucleon {+238}U beam by 10 |mm 119RH3c thick {+9}Be target at GANIL accelerator facility. The fission 119RH4c fragments were identified by mass and charge numbers through energy 119RH5c loss |DE, time-of flight and magnetic rigidity using VAMOS++ magnetic 119RH6c spectrometer. The gamma rays were detected using EXOGAM array of 11 119RH7c Compton-suppressed segmented clover HPGe detectors. Measured E|g, I|g 119RH8c and |g|g- and (fission fragment)|g-coin. Deduced levels, J|p, and 119RH9c band. Comparison with triaxial projected shell model (TPSM) 119RHAc calculations. 119RH d Details of |g-ray data were requested from the authors by compiler, 119RH2d March 31, 2017, but no response received. 119RH cL E$From E|g data, assuming uncertainty of 1 keV for each |g ray 119RH CL BAND(A)$|DJ=1 yrast band 119RH L 0 (7/2+) 190 MS 6 A 119RH cL T$from 2015Lo04: Phys. Rev. Lett. 114, 192501 119RH L 155 1 (9/2+) A 119RH G 155 119RH L 341 2 (11/2+) A 119RH G 186 119RH 9BE(238U,F):T1/2,%B-N:XUNDL-4 2021HA19 202105 119RH c Compiled (unevaluated) dataset from 2021Ha19: 119RH2c Phys Lett B816, 136266 (2021) 119RH c Compiled by B. Singh (McMaster); May 7, 2021 119RH c 2021Ha19: {+119}Rh produced in {+9}Be({+238}U,F) reaction with {+238}U 119RH2c beam of 345 MeV/nucleon from the cascade operation of the RBIF 119RH3c complex of accelerators at RIKEN. Identification of {+119}Rh made on 119RH4c the basis of magnetic rigidity, time-of-flight and energy loss using 119RH5c the BigRIPS separator and ZeroDegree spectrometer. The separated nuclei 119RH6c were sent to the Advanced Implantation Detector Array (AIDA) for the 119RH7c detection of implanted ions and subsequent |b{+-} and |b{+-}-delayed 119RH8c neutrons using six double-sided silicon-strip detector (DSSDs) for 119RH9c particles, and BRIKEN neutron counter array of 140 {+3}He proportional 119RHAc counters embedded in a high-density polyethylene (HDPE) matrix. 119RHBc Measured and analyzed (implanted ions)-|b and (implanted ions)-|b-n 119RHCc correlated events to deduce half-life of decay and delayed-neutron 119RHDc emission probability (%|b{+-}n or (P{-1n}). In the analysis, Bateman 119RHEc equation was used to fit the decay curve for the isotope of interest, 119RHFc subsequent daughters and grand-daughters in the decay chain to reach 119RHGc the final stable isotope. For details of the experimental arrangement, 119RHHc and analysis methodology, consult 2019To09 (Nucl. Instr. Meth. A925, 119RHIc 133) article for commissioning of BRIKEN facility at RIKEN. 119RH c Comparison of measured half-lives and P{-n} values with previous 119RH2c experimental results, and with FRDM+QRPA, FRDM+QRPA+HF, RHB+pn:RQRPA 119RH3c and EDM calculations, where FRDM=Finite range droplet model; 119RH4c QRPA=Quasiparticle random phase approximation; HF=Hauser-Feshbach 119RH5c framework; RHB+pn:RQRPA=Relativistic Hartree-Bogoliubov mass model 119RH6c with the proton-neutron relativistic QRPA; and EDM=semi-empirical 119RH7c Effective density model. 119RH L 0 192 MS 12 119RH2 L %B-=100 $ %B-N=3.4 9 (2021Ha19) 119RH cL $%|b{+-}n or P{-n} measured by 2021Ha19 from 119RH2cL (implanted ions)-|b-n correlated events. Earlier value: 6.4 {I16} 119RH3cL (2006Mo07: Phys. Rev. C 73, 035801). Weighted average of the two 119RH4cL values is 4.1 {I13} (compiler's note) 119RH cL E$the observed activity is assigned to the g.s. of {+119}Rh, but 119RH2cL there is the possibility of two activities, based on systematics 119RH3cL odd-A Rh nuclei. 119RH cL T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b 119RH2cL and (implanted ions)-|b-n correlated events. Earlier values: 190 ms 119RH3cL {I6} (2015Lo04: Phys. Rev. Lett. 114, 192501); 171 ms {I18} 119RH4cL (2006Mo07, also 190 ms {I10} in 2006ToZW (thesis from Michigan State 119RH5cL Univ.). Weighted average of the three values is 189 ms {I6}, as it 119RH6cL is heavily weighted by the value in 2015Lo04 (compiler's note)