93RH    93PD EC DECAY:XUNDL-2         2019PA16                           202006
 93RH c  Compiled (unevaluated) dataset from 2019Pa16                           
 93RH c  Phys. Rev. C 99, 034313 (2019)                                         
 93RH c  Compiled by E.A. McCutchan (NNDC,BNL), May 16, 2020                    
 93RH c  {+93}Pd produced from fragmentation of a {+124}Xe beam at E=345        
 93RH2c  MeV/nucleon on a 740 mg/cm{+2} {+9}Be target at RIKEN, Japan.          
 93RH3c  Fragments separated by B|r-|DE-B|r method in the first stages of       
 93RH4c  BigRIPS and then B|r-tof-B|r measurements using later stage of         
 93RH5c  BigRIPS and the ZeroDegree spectrometer. Ions were implanted in        
 93RH6c  WAS3ABi consisting of three double-sided silicon strip detectors and   
 93RH7c  ten single-sided silicon strip detectors. Gamma rays were detected     
 93RH8c  using the Euroball-RIKEN Cluster Array (EURICA) consisting of 84 HPGe  
 93RH9c  crystals arranged in 12 clusters. Measured E|g, I|g, |b spectra,       
 93RHac  E(p), I(p), |b|g-coin, |bp-coin, |g|bp-coin, half-life, |b-delayed     
 93RHbc  proton emission probability.                                           
 93RH cL E$From a least-squares fit to E|g, by compiler                         
 93RH cL J$As proposed by 2019Pa16                                              
 93RH D  CC$FROM BrIcc v2.3b (16-Dec-2014) 2008Ki07, "Frozen Orbitals" appr.    
 93PD  P 0.0          (7/2+)            1.17 S    2              10.03E3  37    
 93PD cP QP$from beta endpoint measurement in 2019Pa16                          
 93PD cP J,T$from 2019Pa16                                                      
 93RH  N 0.926        0.926     1.0       1.0                                   
 93RH cN NR$2019Pa16 report absolute intensities.  Additionally they report     
 93RH2cN relative intensities which are included in the comments. Value         
 93RH3cN given here considers the %|b{++}p=7.4 {I2} branch.                     
 93RH  L 0.0          (9/2+)                                                    
 93RH  E             4.8     240.025   135.93    24             4.8       24    
 93RHS E EAV=4.27E3 19$CK=0.0046 6$CL=0.00057 8$CM+=0.000134 18                 
 93RH  L 240.17    8  (7/2+)                                                    
 93RH  G 240.1     1            [M1]                    0.0319   82.2     18    
 93RHS G KC=0.0279 4$LC=0.00332 5$MC=0.000618 9$NC=0.0001025 15$OC=5.19E-6 8    
 93RH cG RI$I|g{-rel}=100                                                       
 93RH cG TI$total intensity corrected for assumed M1 multipolarity.             
 93RH  E             53.0    200.31    4 4.83    9              53.3      20    
 93RHS E EAV=4.15E3 19$CK=0.0050 7$CL=0.00061 9$CM+=0.000145 20                 
 93RH  L 622.54    8  (5/2+)                                                    
 93RH  G 382.3     1  24.5   11                                                 
 93RH cG RI$I|g{-rel}=29.8 {I15}                                                
 93RH  G 622.6     1  8.2    7                                                  
 93RH cG RI$I|g{-rel}=10.0 {I9}                                                 
 93RH  E             30.1    120.20    3 4.98    10             30.3      12    
 93RHS E EAV=3.96E3 19$CK=0.0057 8$CL=0.00070 10$CM+=0.000165 24                
 93RH  L 894.1     4  (11/2+)                                                   
 93RH  G 894.1     4  2.4    6                                                  
 93RH cG RI$I|g{-rel}=2.9 {I7}                                                  
 93RH  E             2.3     5 0.017   4 6.03    14             2.3       5     
 93RHS E EAV=3.83E3 19$CK=0.0062 9$CL=0.00077 12$CM+=0.00018 3                  
 93RH  L 1300.7    6  (7/2,9/2+)                                                
 93RH  G 1300.7    6  1.9    6                                                  
 93RH cG RI$I|g{-rel}=2.3 {I7}                                                  
 93RH  E             1.8     5 0.015   5 6.04    16             1.8       5     
 93RHS E EAV=3.63E3 19$CK=0.0073 12$CL=0.00089 14$CM+=0.00021 4                 
                                                                                
 93RH    9BE(112SN,X):ISOMER E:XUNDL-3 2023Xi01                           202302
 93RH c  Compiled (unevaluated) dataset from 2023Xi01: Phys. Rev. C 107,        
 93RH2c  014304 (2023).                                                         
 93RH c  Compiled by G. G~urdal, Jan 26, 2023                                   
 93RH c  2023Xi01: Neutron deficient {+93}Rh was produced via projectile        
 93RH2c  fragmentation of primary {+112}Sn beam and studied using Isochronous   
 93RH3c  Mass Spectrometry (IMS). The experiment was performed at the           
 93RH4c  HIRFL-CSR accelerator complex at the Institute of Modern Physics in    
 93RH5c  Lanzhou, China. The primary {+112}Sn{++35} ions were accelerated to a  
 93RH6c  relativistic energy of  |J400.88 MeV/u by the main Cooler Storage      
 93RH7c  Ring (CSRm) and impinged on a 10 mm thick {+9}Be target at the         
 93RH8c  entrance of Radioactive Ion Beam Line at Lanzhou (RIBLL2). The         
 93RH9c  fragments emerged from the target were separated in flight with        
 93RHac  RIBLL2 and the experimental Cooler Storage Ring (CSRe). To measure     
 93RHbc  the revolution times of the stored ions a tof detector equipped with   
 93RHcc  a carbon foil and a set of multichannel plates were used. Measured:    
 93RHdc  E{-x} of the isomer. Comparison with the shell model calculations.     
 93RH  L 0            9/2+              12.2 S    7                             
 93RH cL J,T$from the Adopted Levels of {+93}Rh in ENSDF database.              
 93RH  L 267       48 1/2-                                                   M  
 93RH cL E$recommended value obtained from the analysis of the shape of the     
 93RH2cL peaks in the revolution time spectrum using exponentially modified     
 93RH3cL Gaussian (EMG) function in 2023Xi01.                                   
 93RH cL J$based on the systematics of the J|p of the observed isomers in the   
 93RH2cL neighboring isotopes and the isotones in 2023Xi01. The authors of      
 93RH3cL 2023Xi01 states that the isomeric state is a proton-hole state.