142TE    9BE(238U,F):T1/2:XUNDL-1      2020WU04                           202101
142TE c  Compiled (unevaluated) dataset from 2020Wu04:                          
142TE2c  Phys Rev C 101, 042801(R) (2020)                                       
142TE c  Compiled by B. Singh (McMaster), Jan 23, 2021                          
142TE c  2020Wu04: {+142}Te nuclide produced at the RIBF-RIKEN facility in      
142TE2c  {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon and an intensity of    
142TE3c  5pnA. Identification of fission fragments of interest was made based on
142TE4c  time-of-flight (tof), magnetic rigidity (B|r), and energy loss (|DE)   
142TE5c  using the BigRIPS spectrometer, determining atomic Z and mass-to-charge
142TE6c  ratio A/Q, where Q=charge state of the ions. The separated nuclei      
142TE7c  were implanted at a rate of 100 ions/s in the beta counting system     
142TE8c  of the Wide range Active Silicon-Strip Stopper Array for Beta and      
142TE9c  ion detection (WAS3ABi), which included a stack of five Double Sided   
142TEAc  Silicon Strip Detectors (DSSSDs). The WAS3ABi setup was surrounded     
142TEBc  by Euroball RIken Cluster Array (EURICA) array of 84 HPGe detectors    
142TECc  for |g detection. Half-life of the separated and implanted ions        
142TEDc  was determined by fitting the time distribution of |b(implants)- and/or
142TEEc  |b|g(implants)-correlated decay curves to the sum of activities of     
142TEFc  parent nuclei, daughter nuclei, grand-daughter nuclei, |b-delayed      
142TEGc  neutron daughter and grand-daughter nuclei, and a constant background. 
142TEHc  Comparison of measured half-lives with FRDM+QRPA (2003), FRDM+QRPA     
142TEIc  (2019), KTUY+GT2, RHB+pn-RQRPA, and DF+CQRPA theoretical calculations. 
142TE  L 0            0+                  147 MS 8                              
142TE2 L %B-=100 $ %B-N=? $ %B-2N=?                                             
142TE cL %B-$only the |b{+-} decay mode is expected and detected, followed by   
142TE2cL |b-delayed neutron decay                                               
142TE cL T$from 2020Wu04, fitting the time distribution of                      
142TE2cL (implanted ions)|b|g-correlated decay curves to the sum of activities  
142TE3cL of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n      
142TE4cL daughter and grand-daughter nuclei, and a constant background.         
                                                                                
142TE    9BE(238U,F):T1/2:XUNDL-2      2023MO01                           202303
142TE c  Compiled (unevaluated) dataset from 2023Mo01:                          
142TE2c  Phys Rev C 107, 014311 (2023)                                          
142TE c  Compiled by E.A. McCutchan (NNDC,BNL)                                  
142TE c  {+142}Te nuclide produced at the RIBF-RIKEN facility in                
142TE2c  {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon.                       
142TE3c  Identification of fission fragments of interest was made based on      
142TE4c  time-of-flight (tof), magnetic rigidity (B|r), and energy loss (|DE)   
142TE5c  using the BigRIPS spectrometer and Zero-degree spectrometer.           
142TE6c  Fragments implanted into WAS3ABi detector. Measured E|g, I|g, |g|g     
142TE7c  |b-|g using the EURICA array consisting of 12 cluster HPGe detectors.  
142TE  L 0            0+                  148 MS 18                             
142TE cL T$from fitting  of the time distribution of 191|g, 276|g and 877|g.