116RH 9BE(238U,FG):XUNDL-1 2017NA04 201707 116RH c Compiled (unevaluated) data set from 2017Na04: 116RH2c Phys Lett B 767, 480 (2017) 116RH c Compiled by B. Singh (McMaster); July 2, 2017. 116RH c First level scheme for {+116}Rh proposed in the present work. 116RH c 2017Na04: high-spin excited states in {+116}Rh were studied by their 116RH2c population in the fission of 6.2 MeV/nucleon {+238}U beam by 10 |mm 116RH3c thick {+9}Be target at GANIL accelerator facility. The fission 116RH4c fragments were identified by mass and charge numbers through energy 116RH5c loss |DE, time-of flight and magnetic rigidity using VAMOS++ magnetic 116RH6c spectrometer. The gamma rays were detected using EXOGAM array of 11 116RH7c Compton-suppressed segmented clover HPGe detectors. Measured E|g, I|g 116RH8c and |g|g- and (fission fragment)|g-coin. Deduced high-spin levels, J|p, 116RH9c band, and energy signature splitting. Comparison with triaxial 116RHAc projected shell model (TPSM) calculations. 116RH d Details of |g-ray data were requested from the authors by compiler, 116RH2d March 31, 2017, but no response received. 116RH cG E(X)$From spectral Fig. 1 in 2017Na04 116RH cL E$From least-squares fit to E|g data (by compiler), assuming 116RH2cL uncertainty of 1 keV for each |g ray 116RH CL BAND(A)$|DJ=1 yrast band based on (7-) 116RH G 143 X 116RH G 310 X 116RH L 0+X (7-) 0.57 S 5 AM 116RH DL E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 116RH cL T$from {+116}Rh Adopted Levels in the ENSDF database (Dec 2009 update). 116RH2 L %B-=100 116RH L 173+X 1 (8-) A 116RH G 173 116RH L 386+X 1 (9-) A 116RH G 213 116RH G 386 116RH L 614+X 1 (10-) A 116RH G 228 116RH G 441 116RH L 902+X 1 (11-) A 116RH G 288 116RH G 516 116RH L 1150+X 1 (12-) A 116RH G 248 116RH G 536 116RH U(P,F):MASS,ISOMER:XUNDL-2 2023HU01 202303 116RH c Compiled (unevaluated) dataset from 2023Hu01: 116RH2c Phys Rev C 107, 014306 (2023). 116RH c Compiled by B. Singh (McMaster), February 01, 2023 116RH c 2023Hu01: {+116}Rh produced in U(p,F),E(p)=25 MeV using IGISOL facility 116RH2c and the JYFLTRAP double Penning trap system at the K130 116RH3c cyclotron of the University of Jyvaskyla. Measured mass excesses of the 116RH4c ground state and isomer in {+116}Rh using the 116RH5c phase-imaging ion-cyclotron-resonance (|p{+-}ICR) technique. Comparison 116RH6c BSkG1 mass model theoretical calculations, and with mass excesses from 116RH7c systematics in AME2020. Discussed triaxial deformation of {+116}Rh. 116RH cL J,T$From {+116}Rh Adopted Levels in the ENSDF database 116RH2cL (December 2009 update) 116RH L 0.0 1+ 0.68 S 6 116RH cL $Measured mass excess=-70729 keV {I2} (2023Hu01), with reference to 116RH2cL mass of {+133}Cs. 116RH cL T$2023Hu01 cite value of 685 ms {I39} from 2021Ko07 (NUBASE2020) 116RH L 120.8 19 (6-) 0.57 S 5 116RH cL $Measured mass excess=-70608.3 keV {I28} (2023Hu01), with reference to 116RH2cL mass of {+116}Rh g.s. 116RH cL E$from 2023Hu01, difference of measured mass excesses of the g.s. and 116RH2cL the isomer. 116RH 252CF SF DECAY:XUNDL-3 2025Li19 202512 116RH c Compiled (unevaluated) dataset from 2025Li19: 116RH2c Phys Rev C 111, 034308 (2025). 116RH c Compiled by E.A. McCutchan (NNDC,BNL) April 10, 2025 116RH c 2025Li19: {+116}Rh produced in {+252}Cf SF decay at CARIBU facility. 116RH2c Helium filled gas catcher collects fission products, followed by an 116RH3c isobar separator. Measured mass excesses of the 116RH4c ground state and isomer in using the Canadian Penning trap. 116RH cL J,T$From {+116}Rh Adopted Levels in the ENSDF database 116RH2cL (December 2009 update) 252CF P 0 0+ 2.647 Y 3 252CF cP T$From {+252}Cf Adopted Levels in the ENSDF database (Jan 2021 update) 116RH L 0.0 1+ 0.68 S 6 116RH cL $Measured mass excess=-70733 keV {I5} (2025Li19), with reference to 116RH2cL mass of {+116}Cd. 116RH L 121.2 65 (6-) 0.57 S 5 116RH cL $Measured mass excess=-70611.8 keV {I41} (2025Li19), with reference to 116RH2cL mass of {+116}Cd. 116RH cL E$from 2025Li19, difference of measured mass excesses of the g.s. and 116RH2cL the isomer.