14F     ADOPTED LEVELS                                                   201405
 14F   H TYP=FUL$AUT=J. Kelley, C.G. Sheu$CUT=01-MARCH-2014$CIT=ENSDF$          
 14F   Q                       -1556   41-9.26e3 40    2012WA38                 
 14F   XA1H(13O,P)                                                              
 14F  c  Theoretical works:                                                     
 14F  c  2011Sh17: Simple potential model comparison of {+14}F and its mirror   
 14F 2c  nucleus {+14}B, and a critical analysis of the 2010Go11 results. The   
 14F 3c  main critique is connected with the suggestion that in 2010Go16 the    
 14F 4c  observed J|p=3- state at E({+13}O+p)=3.05 MeV is at too low an energy  
 14F 5c  and that its deduced spectroscopic factor is not appropriate; the      
 14F 6c  authors suggest the E({+13}O+p)=3.05 MeV state is the J|p=1+ state and 
 14F 7c  mirror of {+14}B*(1.28 MeV).                                           
 14F  c  2011Sh21: Comparison of ab initio no-core Shell Model calculations     
 14F 2c  with data on {+14}F and its mirror {+14}B nucleus.                     
 14F  c  2010Ma06: Performed ab initio no-core Shell Model calculations of the  
 14F 2c  mass of {+14}F and its mirror {+14}B nucleus along with the {+13}O     
 14F 3c  nucleus. In addition they calculated the predicted excitation energies 
 14F 4c  for {+14}F and {+14}B.                                                 
 14F  c  See earlier predictions on {+14}F ground state properties reported in  
 14F 2c  1978Gu10, 1984An18, 1993Po11, 2000Po32, 2008Va13.                      
 14F  cL E$ S(p)({+14}F)=1.56 MeV {I4}.                                         
 14F   L 0            2-               910 KEV   100                            
 14F  cL $|G/|G{-s.p.}=0.85 {I}                                                 
 14F  cL E$mass excess=31960 keV {I50}.                                         
 14F 2 L XREF=A                                                                 
 14F   L 0.54E3    18 1-               1 MEV     AP                             
 14F  cL $|G/|G{-s.p.}=0.6 {I}                                                  
 14F 2 L XREF=A                                                                 
 14F   L 1490      72 3-               210 KEV   40                             
 14F  cL $|G/|G{-s.p.}=0.55 {I}                                                 
 14F 2 L XREF=A                                                                 
 14F   L 2.79E3    11 4-               550 KEV   100                            
 14F  cL $|G/|G{-s.p.}=0.5 {I}                                                  
 14F 2 L XREF=A                                                                 
                                                                                
 14F     1H(13O,P)                     2010GO16,2012Go11                  201405
 14F   H TYP=FUL$AUT=J. Kelley, C.G. Sheu$CUT=01-MARCH-2014$CIT=ENSDF$          
 14F  c  The authors measured the excitation function for {+1}H+{+13}O elastic  
 14F 2c  scattering. Resonances observed in 2010Go16 indicate the first         
 14F 2c  observation of {+14}F. The work was also reported in 2012Go11.         
 14F  c  A beam of 31 MeV/A {+13}O ions was produced via the                    
 14F 2c  {+1}H({+14}N,{+13}O) reaction at the TAMU Cyclotron Institute. The     
 14F 3c  beam energy was degraded to |?10 MeV/A at the entrance of a methane    
 14F 4c  (CH{-4}) filled scattering chamber. A thin plastic scintillator along  
 14F 5c  with a windowless ionization chamber provided identification of {+13}O 
 14F 6c  particles at the entrance of the scattering chamber. As the {+13}O     
 14F 7c  ions passed through the chamber, {+1}H({+13}O,p) scattering reactions  
 14F 8c  occurred. A pair of silicon |DE-E telescopes located |?51 cm from the  
 14F 9c  chamber entrance detected the scattered protons. The energy spectrum   
 14F ac  of scattered protons, which reflects the elastic scattering excitation 
 14F bc  function, was evaluated by R-matrix analysis to determine {+14}F       
 14F cc  resonances involved in the reaction.                                   
 14F  cL E$ S(p)({+14}F)=1.56 MeV {I4}.                                         
 14F   L 0            2-               910 KEV   100                            
 14F  cL $|G/|G{-s.p.}=0.85                                                     
 14F  cL E$mass excess=31960 keV {I50}.                                         
 14F  cL E$E{-res}({+13}O+p)=1.56 MeV {I4}.                                     
 14F   L 0.54E3    18 1-               1 MEV     AP                             
 14F  cL $|G/|G{-s.p.}=0.6                                                      
 14F  cL E$E{-res}({+13}O+p)=2.10 MeV {I17}.                                    
 14F   L 1490      72 3-               210 KEV   40                             
 14F  cL $|G/|G{-s.p.}=0.55                                                     
 14F  cL E$E{-res}({+13}O+p)=3.05 MeV {I6}.                                     
 14F   L 2.79E3    11 4-               550 KEV   100                            
 14F  cL $|G/|G{-s.p.}=0.5                                                      
 14F  cL E$E{-res}({+13}O+p)=4.35 MeV {I10}.