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 /* NRDF D0363 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D363;
 TITLE=/A STUDY OF THE 58NI,90ZR AND 208PB(P,D) REACTIONS AT 121 MEV/;
 PURPOSE=/IN ORDER TO INVESTIGATE THE EXTENT TO WHICH THE DISTORTED WAVE
          METHOD CAN BE EXTENDED TO HIGHER BOMBARDING ENERGIES, THE
          58NI, 9/ZR AND 208PB(P,D) REACTIONS WERE STUDIED AT 121 MEV.
          THE MAJOR EMPHASIS IN THE PRESENT WAS TO STUDY THE LOW-LYING
          STATES THAT ARE STRONGLY EXCITED AND HENCE HAVE SPECTROSCOPIC
          FACTORS THAT WERE RATHER WELL DETERMINDED IN EARLIER WORK DONE
          AT LOWER BOMBARDING ENERGIES./;
 ATH=(R.E.ANDERSON'1',J.J.KRAUSHAAR'1',J.R.SHEPARD'1',J.R.COMFORT'2');
 INST-ATH=(1USACLU'1',1USAINU'2');
 REF=NP/A;
 VLP=311(1978)93;
 RCTS=(58NI(P,D)57NI,90ZR(P,D)89ZR,208PB(P,D)207PB);
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 /* Experimental Conditions                                           */
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 \\EXP,1;
 RCT=58NI(P,D)57NI;
 ENR=>99%;
 CHM=ELM;
 THK-TGT=11.1MG/CM**2;
 BAC=SELF;
 POL-TGT=NO;
 ALGN-TGT=NO;
 ACC=(CYC);
 INST-ACC=1USAINU;
 INC-ENGY-LAB-RANGE=(121.2MEV);
 DELTA-INC-ENGY-LAB=XKEV;
 ERS-PRJ=XKEV;
 BEAM-INTNSTY=XUA;
 POL-PRJ=NO;
 DET-SYS=(MAG+PS-PC+PLST-SCT);
 SOLID-ANGL=2.55MSR;
 ERS-DET=125KEV;
 ANL=(OPT-MODEL,CC,DWBA);
 PHQ=(XSECTN,ANGL-DSTRN,DSIGMA/DOMEGA,OPT-POTL-PARA,SPEC-FCTR);
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 PRJ=P;
 TGT=58NI;
 INC-ENGY-LAB=121.2MEV;
 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 WS RIS AIS VSO RRSO ARSO WSO RISO AISO
 (MEV) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM)
 (MEV) (FM) (FM)
 121.2 -11.29 1.13 -9.86 1.49 0.32 0  3.40 1.27 0.65 0
 121.2 -22.0 1.23 0.76 -7.29 1.47 0.51 0  4.46 1.05 0.61 -1.59 1.05 0.61
 \END;
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