ENTRY            A0715   20041226
SUBENT        A0715001   20041226                                 
BIB                 13         41                                 
TITLE      Measurement of reaction cross section for proton-rich  
           nuclei (A<30) at intermediate energies.                
REFERENCE  (J,NP/A,707,303,2002)                                  
AUTHOR     (H.Y.Zhang, W.Q.Shena, Z.Z.Ren, Y.G.Ma, W.Z.Jiang,     
           Z.Y.Zhu, X.Z.Cai, D.Q.Fang, C.Zhong, L.P.Yua, Y.B.Wei, 
           W.L.Zhan, Z.Y.Guo, G.Q.Xiao, J.S.Wang, J.C.Wang,       
           Q.J.Wang, J.X.Li, M.Wang, Z.Q.Chen)                    
INSTITUTE  (3CPRCPR) Shanghai Institute of Nuclear Research and   
            College of Sciences, Ningbo University.               
           (3CPRIMP) Institute of Modern Physics.                 
           (3CPRNAN) Department of physics.                       
METHOD     (ASEP,EDE,TOF) All details in original paper           
DETECTOR   (SPEC) All details in original paper.                  
FACILITY   (FRS,3CPRIMP) Radioactive Ion Beam Line                
           (ACCEL,3CPRIMP) Heavy Ion Research Facility.           
INC-SOURCE (SPALL) 36-Ar primary beam on a 9-Be target.           
HISTORY    (20041222C) by F.Ch                                    
           (20041226U) Last checking has been done.               
ERR-ANALYS (DATA-ERR) The error bars include not only the         
           statistic errors but also systematic errors, because   
           the energy resolution and particle identification      
           limited by the response function of Si detectors and   
           noise of electronics equipment, etc.                   
REL-REF    (R,,W.Q.SHEN+,J,NP/A,491,130,1989)                     
MISC-COL   (MISC1) The experimental reaction cross section        
           transferred to 30 MeV/nucleon was listed in the same   
           table also by using Shen's formula for a consistent    
           comparison.  In this formula, the radius parameter is  
           the only adjustable parameter.  By adjusting the radius
           parameter, we can fit the experimental reaction cross  
           section at the experimental energy point.  Then we     
           change the incident energy to 30 MeV/nucleon and get   
           the reaction cross section with this fitted radius     
           parameter.                                             
           (MISC-ERR) The uncertainty of MISC1.                   
           An analysis is not given.                              
           (MISC2) Energy/nucleon                                 
ADD-RES    (COMP) A detailed comparison between the experimental  
           reaction cross sections at intermediate energies and   
           the calculation with Glauber model was made.           
           (STRUC) Proton halo structure.                         
ENDBIB              41                                            
NOCOMMON                                                          
ENDSUBENT           44