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 /* NRDF D0350 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D350;
 TITLE=/ELASTIC AND INELASTIC SCATTERING OF 185 MEV PROTONS FROM 12C/;
 PURPOSE=/THE MAIN MOTIVATION FOR THE WISH TO OBTAIN A MORE RELIABLE
          OPTICAL POTENTIAL WAS THE FACT THAT DISTORTION EFFECTS IN
          CALCULATIONS ON INELASTIC SCATTERING OF MEDIUM ENERGY PROTONS
          IN THE DISTORTED-WAVE IMPULSE APPROXIMATION HAVE BEEN FOUND TO
          BE VERY LARGE. THIS MEANS THAT IT IS VERY DIFFICULT TO EXTRACT
          INFORMATION ON NUCLEAR STRUCTURE AND THE MODE OF EXCITATION
          UNLESS THE DISTORTING POTENTIAL IS RATHER WELL KNOWN./;
 ATH=(A.INGEMARSSON'1',O.JONSSON'1',A.HALLGREN'1');
 INST-ATH=(2SWDUPP'1');
 REF=NP/A;
 VLP=319(1979)377;
 RCTS=(12C(P,P)12C);
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 ENR=X%;
 CHM=ELM;
 THK-TGT=(0.16G/CM**2,0.48G/CM**2);
 BAC=SELF;
 POL-TGT=NO;
 ALGN-TGT=NO;
 ACC=(SYNCYC);
 INST-ACC=2SWDUPP;
 INC-ENGY-LAB-RANGE=(185MEV);
 DELTA-INC-ENGY-LAB=XKEV;
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XUA;
 POL-PRJ=NO;
 DET-PARTCL=(P);
 DET-SYS=(MAG);
 SOLID-ANGL=XMSR;
 ERS-DET=(400KEV,550KEV);
 ANL=(OPT-MODEL,DWIA,DWBA);
 PHQ=(XSECTN,ANGL-DSTRN,DSIGMA/DOMEGA,POL,OPT-POTL-PARA);
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 PRJ=P;
 TGT=12C;
 INC-ENGY=185MEV;
 POTL-FORM=/-(V*F(XR)+I*(WV*F(XIV)-4*WS*DIF(1!XIS)F(XIS)+WG*G(XIG)))+
 (HBAR/(MPI*C))**2*1/R*(VSO*DIF(1!R)F(XRSO)+I*WSO*DIF(1!R)
 F(XISO))*SIGMA*L+UC(R):
 F(XI)=1/(1+EXP(XI)): G(XG)=EXP(-XG**2):
 XI=(R-RI*A**(1/3))/AI:
 UNIFORM  CHARGE OF RAIDUS RC*A**(1/3):/;
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB V RR AR WV RIV AIV VSO RRSO ARSO WSO RISO AISO DATA1'1'
 (MEV) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM)
 (NODIM)
 185 15.79 1.213 0.633  9.00 1.221 0.695 2.31 0.903 0.480 -3.41 0.903
 0.480 2.98
 185 10.37 1.353 0.614 18.61 1.041 0.627 3.63 0.870 0.463 -3.09 0.870
 0.463 3.82
 185 15.25 1.218 0.635 12.61 1.038 0.745 2.14 0.890 0.481 -3.76 0.890
 0.481 3.72
 185  7.78 1.452 0.448 25.74 0.878 0.723 4.04 0.866 0.489 -3.06 0.866
 0.489 3.52
 \END;
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