37MG    C(37MG,36MGG):XUNDL-1         2014KO14                           201412
 37MG c  Includes Pb({+37}Mg,{+36}Mg|g)                                         
 37MG c  Compiled (unevaluated) dataset from 2014Ko14:                          
 37MG c  Phys Rev Lett 112, 242501 (2014)                                       
 37MG c  Compiled by J. C. Batchelder (ORNL/ORAU) and C.D. Nesaraja (ORNL),     
 37MG2c  November 24, 2014                                                      
 37MG d  Edited by B. Singh (McMaster), Nov 25, 2014                            
 37MG c  Coulomb and nuclear dominated 1 neutron removal reaction:              
 37MG c  Projectile: {+37}Mg secondary beam produced by projectile              
 37MG2c  fragmentation at RIKEN with E({+37}Mg)=240 MeV/u mid target            
 37MG3c  energy for C target (thickness 2.54 g/cm{+2}) and ({+37}Mg)=244 MeV/u  
 37MG4c  mid target energy for Pb target (thickness 3.37 g/cm{+2}) with typical 
 37MG5c  intensity of 6 pps                                                     
 37MG c  Detectors: {+36}Mg residues produced were identified by their          
 37MG2c  B|r, tof, and |DE using the Zero Degree Spectrometer and the           
 37MG3c  |g-rays detected with the DALI2 detector array at RIBF-RIKEN facility. 
 37MG c  Measured: E|g, I|g, ({+36}Mg residue)|g-coin and cross-section based   
 37MG2c  on known 2+ |) 0+ and 4+ |) 2+ |g-rays in {+36}Mg.                     
 37MG c  Combined analysis of the data from Coulomb- and nuclear-               
 37MG2c  dominated 1n-removal reactions from {+37}Mg was performed              
 37MG3c  to extract S(n), J|p and C{+2}S.                                       
 37MG c  Theory: Large scale shell model calculations using the {Isd}-{Ipf}     
 37MG2c  cross shell- modified monopole (SDPF-M) Sm effective interaction.      
 37MG c                                                                         
 37MG c  Experimental S(n)({+37}Mg)=0.22 MeV {I+12-9} for 2p{-3/2} or 2p{-1/2}  
 37MG2c  neutron removal; 0.40 MeV {I+19-13} for 2s{-1/2} neutron removal       
 37MG3c  (2014K014). These values are consistent with S(n)=0.16 MeV {I68}       
 37MG4c  (systematic trends, 2012Wa38)                                          
 37MG  L 0.0         (3/2-)                                                     
 37MG cL J$3/2- is more likely but 1/2- is not fully excluded, whereas 1/2+     
 37MG2cL is very unlikely when compared to shell-model calculations. The        
 37MG3cL J|p assignment is made from comparisons of measured inclusive and      
 37MG4cL partial one-neutron-removal cross sections and the measured parallel   
 37MG5cL momentum distribution of {+36}Mg residues with eikonal-model           
 37MG6cL predictions using C{+2}S value noted below. From consistency of the    
 37MG7cL measured data with large scale shell model calculations, {+37}Mg is    
 37MG8cL identified as deformed and having a significant(|?40%) p-wave neutron  
 37MG9cL halo component with a {+36}Mg(0+,g.s.)~#(|n2p{-3/2} or |n2p{-1/2})     
 37MGAcL configuration, and lies within the "island of inversion".              
 37MG cL $Experimental C{+2}S=0.42 {I+14-12} for 2p{-3/2} or 2p{-1/2} neutron   
 37MG2cL removal; 0.40 {I+16-13} for 2s{-1/2} neutron removal                   
                                                                                
 37MG    9BE(48CA,XG):T1/2:XUNDL-2     2022CR03                           202304
 37MG c  Compiled (unevaluated) dataset from 2022Cr03: Phys Rev Lett. 129,      
 37MG2c  212501 (2022)                                                          
 37MG c  Compiled by E. J. Gass (NNDC,BNL) (February 28, 2023).                 
 37MG c  {+48}Ca beam was accelerated to 172.3 MeV/u through the FRIB linac.    
 37MG2c  Fully-stripped 120 particle-nA beam of {+48}Ca{+20+} collided with     
 37MG3c  8.89mm {+9}Be fragmentation target. Preseparator selected nuclei with  
 37MG4c  B|r of 5.100 Tm to optimize {+42}Si. Additional separation was         
 37MG5c  carried out by the ARIS. The cocktail beam of fragments was delivered  
 37MG6c  to FDSi at 4.904 Tm. In the center of FDSi was a 5 mm-thick            
 37MG7c  fast-response YSO scintillation detector sandwiched by two plastic     
 37MG8c  scintillator veto detectors. This was surrounded by 11 HPGe clover     
 37MG9c  detectors and 15 fast-timing LaBr{-3} detectors in a hemisphere to     
 37MGac  the north. On the south side were 88 neutron detectors of the VANDLE   
 37MGbc  array in two layers 90 and 96 cm from the implantation detector. Two   
 37MGcc  large-area Si PIN detectors and a 2-mm-thick plastic scintillator      
 37MGdc  were positioned 1.5 m upstream in the last diagnostic detector box of  
 37MGec  the beamline. Ions were identified using event-by-event energy loss    
 37MGfc  in the PIN detector (to determine Z) and time-of-flight from a         
 37MGgc  plastic timing scintillator in ARIS to the timing scintillator in the  
 37MGhc  diagnostic detector box (to determine A/Q). Half-lives were obtained   
 37MGic  by fitting decay curves to a function considering the decay of the     
 37MGjc  parent, growth and decay of daughters, potential |bn and |b2n decay    
 37MGkc  branches, and constant background.                                     
 37MG  L 0.0                            6.4 MS    15                            
 37MG cL T$from fit to decay curve with function that included decay of parent, 
 37MG2cL exponential growth and decay of daughters (including |bn and |b2n      
 37MG3cL branches) and a constant background (2022Cr03). Reported as            
 37MG4cL 6.4 ms {I4} (stat) {I14} (syst).