27F     9BE(29NE,N26F)                2012CH12                           201108
 27F   H TYP=MOD$AUT=M.S. BASUNIA$DAT=26-Jun-2012$COM=added this dataset$       
 27F   H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 112, 1875 (2011)$           
 27F 2 H CUT=30-Nov-2010$                                                       
 27F  c  {+29}Ne beam, E=62 MeV/nucleon, was produced by fragmentation          
 27F 2c  of {+48}Ca beam, E=140 MeV/nucleon, on a Be target at                  
 27F 3c  NSCL facility. Fragments were separated by a1900 Fragment separator    
 27F 4c  and identified by time-of-flight and energy loss information.          
 27F 5c  Detected charged fragments, neutrons and |g-rays in coin mode. The     
 27F 6c  |g-rays were detected using a Caesium Iodide detector array. The       
 27F 7c  charged fragments were deflected by a Sweeper magnet and passed        
 27F 8c  through a pair of cathode readout drift chambers, ionization chamber,  
 27F 9c  and plastic scintillators. Neutrons were detected in Modular Neutron   
 27F ac  array. Identified a neutron-unbound state at 2.50 MeV in {+27}F.       
 27F bc  The unbound states in {+27}F was deduced from the measured relative    
 27F cc  energy spectrum for 26f+n coincidences. No |g-ray events were          
 27F dc  recorded in the Caesium Iodide detector array in the coincidence mode. 
 27F   L 0.0          (5/2+)                                                    
 27F  cL $|G{-0}=5.0 ms {I2}                                                    
 27F  cL J,T$From Adopted Levels                                                
 27F   L 2.50E3    22                                                           
 27F  cL $|G{-0}=10 keV                                                         
 27F  cL E$resonance energy=380 keV 60 from fit of energy spectrum for          
 27F 2cL 26f+n coincidence spectrum with Maxwellian distribution and L=2        
 27F 3cL Breit-Wigner resonance. Comparisons with shell-model calculations.     
                                                                                
 27F     ADOPTED LEVELS, GAMMAS                                  11NDS    201108
 27F   H TYP=MOD$AUT=M.S. BASUNIA$DAT=27-Jun-2012$COM=1231 keV level            
 27F 2 H and 504G are added from the 1H(27F,27F'G) dataset. Also updated with   
 27F 3 H the 9BE(29NE,N26F) dataset$                                            
 27F   H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 112, 1875 (2011)$           
 27F 2 H CUT=30-Nov-2010$                                                       
 27F   Q 1.759E4   202.11E3  211.739E4 25-1.61E4 SY    2012WA38                 
 27F  cQ $Note: Current evaluation has used the following Q record              
 27F 2cQ 17.6E3    2 {I2}.1E3   2 {I17802}   syst -16238 syst    2011AuZZ       
 27F  cQ           |DS(p)=241 (syst); |DQ(|a)=353 (syst) (2011AuZZ)             
 27F  cQ $Q(|b{+-})=17900 {I400}, S(n)=1400 {I400}, S(p)=18100 {I500}(syst),    
 27F 2cQ Q(|a)=-15900 {I500}(syst) 2003Au03                                     
 27F  c  Some recent nuclear structure calculations: 2006Ko02, 2004La24,        
 27F 2c  2004Mi31, 2002Ka73, 2002St29.                                          
 27F  c  Atomic mass excess measurement: 24630 keV 190 (2007Ju03)               
 27F  c  Measured {+27}F production cross-sections: |s{-f}=2.1 nb 7 from        
 27F 2c  {+40}Ar fragmentation, E=1.06 GeV/u, on Be target (2000Oz01).          
 27F  c  38.97 MeV/u and 34.00 MeV/u beams of {+27}F on a Si target,            
 27F 2c  measured |s=2096 (164) mb and |s=2468 (256) mb, respectively, for the  
 27F 3c  Si({+27}F,x) reaction (2006Kh08). A squared reduced absorption radius  
 27F 4c  of r{-0}{+2}=1.16 (7) fm{+2} is deduced and used to study the isospin  
 27F 5c  dependence.                                                            
 27F   XA1H(27F,27F'G)                                                          
 27F   XB9BE(29NE,N26F)                                                         
 27F  PN                                                                     6  
 27F   L 0.0          (5/2+)           5.0 MS    2                              
 27F 2 L XREF=AB                                                                
 27F 2 L %B-=100$%B-N=77 21                                                     
 27F  cL %B-N$From 1999Re16. Other: 90 {I30} (1999Dl01).                        
 27F  cL J$From systematics of odd mass fluorine isotopes (2003Au02)            
 27F  cL T$Weighted average of 5.3 ms {I9} (|b-decay time spectrum-1997Ta22),   
 27F 2cL 5.2 ms {I3} (1999Dl01), 6.5 ms {I11} (1999Re16), and 4.9 ms {I2}       
 27F xcL (1998NoZW).                                                            
 27F   L 777          (1/2+)                                                    
 27F 2 L XREF=A                                                                 
 27F  cL E,J$The shell model calculation predicts a level energy for the 1/2+   
 27F 2cL excited state at 1100 keV. An excited state closer to this energy      
 27F 3cL can be constructed using the 504|g and 777|g in cascade. However, a    
 27F 4cL state directly feeding the g.s. is more likely (2004El10).             
 27F   G 777       19  100                                                      
 27F   L 1281         (1/2-)                                                   ?
 27F 2 L XREF=A                                                                 
 27F  cL E,J$From 777 keV + 504 keV |g-rays. Spin/parity assignment from a      
 27F 2cL comparison to other fluorine isotopes, however was not supported by    
 27F 3cL theoretical calculations. The derived octapole deformation             
 27F 4cL parameter |b{-3}=0.7 {I2} do not contradict with the assumption of the 
 27F 5cL existence of a deformed 1/2- state in {+27}F.                          
 27F   G 504       15                                                          ?
 27F   L 2.50E3    22                  10 KEV                                   
 27F 2 L XREF=B                                                                 
                                                                                
 27F     1H(27F,27F'G)                 2004EL10                  11NDS    201108
 27F   H TYP=MOD$AUT=M.S. BASUNIA$DAT=26-Jun-2012$COM=added 1281 keV level and  
 27F 2 H placement of 504G$                                                     
 27F   H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 112, 1875 (2011)$           
 27F 2 H CUT=30-Nov-2010$                                                       
 27F  c  2004El10: {+1}H({+27}F,{+27}F'|g); {+27}F was obtained by bombarding a 
 27F 2c  {+181}Ta target with a primary beam of {+40}Ar, E=94 MeV/u; reaction   
 27F 3c  products were momentum and mass analyzed using the RIPS fragment       
 27F 4c  separator at RIKEN, and identified by energy loss, time-of-flight and  
 27F 5c  magnetic rigidity; the secondary beam of {+27}F, E=40 MeV/u, directed  
 27F 6c  to a liquid hydrogen target; E|g was measured using a setup of 146     
 27F 7c  NaI(Tl) scintillator detectors.                                        
 27F  cL J$From Adopted Levels.                                                 
 27F   L 0.0          (5/2+)                                                    
 27F   L 777          (1/2+)                                                    
 27F   G 777       19                                                           
 27F   L 1281         (1/2-)                                                   ?
 27F  cL E,J$From 777 keV + 504 keV |g-rays. Spin/parity assignment from a      
 27F 2cL comparison with other fluorine isotopes, however was not supported by  
 27F 3cL theoretical calculations. The derived octapole deformation             
 27F 4cL parameter |b{-3}=0.7 {I2} do not contradict to the assumption of the   
 27F 5cL existence of a deformed 1/2- state in {+27}F.                          
 27F   G 504       15                                                          ?