114RH 9BE(238U,FG):XUNDL-2 2017NA04 201707 114RH c Compiled (unevaluated) data set from 2017Na04: 114RH2c Phys Lett B 767, 480 (2017) 114RH c Compiled by B. Singh (McMaster); July 2, 2017. 114RH c 2017Na04: high-spin excited states in {+114}Rh were studied by their 114RH2c population in the fission of 6.2 MeV/nucleon {+238}U beam by 10 |mm 114RH3c thick {+9}Be target at GANIL accelerator facility. The fission 114RH4c fragments were identified by mass and charge numbers through energy 114RH5c loss |DE, time-of flight and magnetic rigidity using VAMOS++ magnetic 114RH6c spectrometer. The gamma rays were detected using EXOGAM array of 11 114RH7c Compton-suppressed segmented clover HPGe detectors. Measured E|g, I|g 114RH8c and |g|g- and (fission fragment)|g-coin. Deduced high-spin levels, J|p, 114RH9c bands, and energy signature splitting. Comparison with triaxial 114RHAc projected shell model (TPSM) calculations. 114RH d Details of |g-ray data were requested from the authors by compiler, 114RH2d March 31, 2017, but no response received. 114RH cG E(X)$From spectral Fig. 1 in 2017Na04 114RH cL $The side band as proposed earlier (see {+114}Rh Adopted Levels in 114RH2cL the ENSDF database) was also confirmed in this work. 114RH cL E$From least-squares fit to E|g data (by compiler), assuming 114RH2cL uncertainty of 1 keV for each |g ray 114RH cL E(B),J(B)$from {+114}Rh Adopted Levels in the ENSDF database 114RH CL BAND(A)$|DJ=1 yrast band based on (7-) 114RH G 148 X 114RH G 176 X 114RH G 255.2 114RH cG $This |g ray is mentioned in the text as belonging to the side band, 114RH2cG but no such transition was reported in an earlier study from SF decay 114RH L 0+X (7-) 1.85 S 5 AM 114RH DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 114RH cL T$From {+114}Rh Adopted Levels in the ENSDF database (Jan 2012 update). 114RH2cL The half-life, taken from 1988Ay02 (Nucl. Phys. A480, 104), is the same 114RH3cL as for the 1+ g.s. 114RH2 L %B- AP 100 114RH L 211+X 1 (8-) A 114RH G 211 114RH L 407+X 1 (9-) A 114RH G 196 114RH G 407 114RH L 489+X 2 (9-) B 114RH G 278 X 114RH L 671+X 1 (10-) A 114RH G 264 114RH G 460 114RH L 813+X 2 (10-) B 114RH G 324 X 114RH L 969+X 1 (11-) A 114RH G 297 114RH G 562 114RH L 1285+X 1 (12-) A 114RH G 317 114RH G 614 114RH L 1705+X 1 (13-) A 114RH G 420 114RH G 737 114RH U(P,F):MASS,ISOMER:XUNDL-3 2023HU01 202303 114RH c Compiled (unevaluated) dataset from 2023Hu01: 114RH2c Phys Rev C 107, 014306 (2023). 114RH c Compiled by B. Singh (McMaster), February 01, 2023 114RH c 2023Hu01: {+114}Rh produced in U(p,F),E(p)=25 MeV using IGISOL facility 114RH2c and the JYFLTRAP double Penning trap system at the K130 114RH3c cyclotron of the University of Jyvaskyla. Measured mass excesses of the 114RH4c ground state and isomer in {+114}Rh using the 114RH5c phase-imaging ion-cyclotron-resonance (|p{+-}ICR) technique. Comparison 114RH6c BSkG1 mass model theoretical calculations, and with mass excesses from 114RH7c systematics in AME2020. Discussed triaxial deformation of {+114}Rh. 114RH cL J,T$From {+114}Rh Adopted Levels in the ENSDF database 114RH2cL (January 2012 update) 114RH L 0.0 1+ 1.85 S 5 114RH cL $Measured mass excess=-75662.7 keV {I26} (2023Hu01), with reference to 114RH2cL mass of {+133}Cs. 114RH L 110.9 32 (7-) 1.85 S 5 114RH cL $Measured mass excess=-75551.8 keV {I41} (2023Hu01), with reference to 114RH2cL mass of {+114}Rh g.s. 114RH cL E$from 2023Hu01, difference of measured mass excesses of the g.s. and 114RH2cL the isomer. 114RH 238U(P,X):XUNDL-4 2025ST02 202509 114RH c Compiled (unevaluated) dataset from 2025St02: Phys Lett B 862, 139359 114RH2c (2025) 114RH c Compiled by V. Cheung (LLNL) Apr 7, 2025. 114RH c E(p)=25 MeV on 15mg/cm{+2} {+nat}U target. Fission fragments were 114RH2c stopped, thermalized, accelerated, mass-separated, and injected into 114RH3c a cooler-buncher. The bunched beam was delivered to the JYFLTRAP 114RH4c double Penning-trap mass spectrometer. Deduced J|p and half-lives of 114RH5c {+114}Rh isomers. 114RH cL E$From measured mass difference between g.s. and isomer of {+114}Rh 114RH2cL from Penning-trap mass measurement (2025St02). 114RH cL J$From observed population in fission and through the decay of 114RH2cL {+114}Ru ground state. 114RH L 0.0 (6-) 1.85 S 6 114RH cL T$from weighted average of partial half-lives determined from the |g 114RH2cL rays in 2003Lh01 114RH L 94.5 23 (0-) 1 S AP M1 114RH cL T$from 2025St02 where isomer observed to survive the 1.18s fission 114RH2cL cycle and 0.9s in-trap decay cycle. Ion ratio between isomers was 114RH3cL observed to be constant over accumulation times from 220 to 620 ms. 114RH L 117.2 21 (3+) 1 S AP M2 114RH cL T$from 2025St02 where isomer observed to survive the 1.18s fission 114RH2cL cycle and 0.9s in-trap decay cycle. Ion ratio between isomers was 114RH3cL observed to be constant over accumulation times from 220 to 620 ms. 114RH 252CF SF DECAY:XUNDL-5 2025Li19 202512 114RH c Compiled (unevaluated) dataset from 2025Li19: 114RH2c Phys Rev C 111, 034308 (2025). 114RH c Compiled by E.A. McCutchan (NNDC,BNL) April 10, 2025 114RH c 2025Li19: {+114}Rh produced in {+252}Cf SF decay at CARIBU facility. 114RH2c Helium filled gas catcher collects fission products, followed by an 114RH3c isobar separator. Measured mass excesses of the 114RH4c ground state and isomer in using the Canadian Penning trap. 252CF P 0 0+ 2.647 Y 3 252CF cP T$From {+252}Cf Adopted Levels in the ENSDF database (Jan 2021 update) 114RH L 0.0 114RH cL $Measured mass excess=-75660.7 keV {I7} (2025Li19), with reference to 114RH2cL mass of {+112}Sn. 114RH L 93.0 11 114RH cL $Measured mass excess=-75567.7 keV {I8} (2025Li19), with reference to 114RH2cL mass of {+112}Sn g.s. 114RH L 114.2 11 114RH cL $Measured mass excess=-75546.5 keV {I8} (2025Li19), with reference to 114RH2cL mass of {+112}Sn g.s. 114RH cL E$from 2025Li19, difference of measured mass excesses of the g.s. and 114RH2cL the isomer.