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 /* NRDF D0358 Data No.60                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,60;
 D#=D358;
 TITLE=/HIGH RESOLUTION INVESTIGATION OF THE 87SR(P,P)REACTION/;
 PURPOSE=/THE PRESENT STUDY WAS UNDERTAKEN (A) TO INVESTIGATE THE LEVEL
          STRUCTURE ,ESPECIALLY THE CORE MULTIPLETS OF 87SR, WHICH WAS
          LARGELY UNKNOWN, AND (B) TO CHECK IF THE RULES OF THE
          WEAK-COUPLING APPROXIMATION ARE OBEYED IN THIS NUCLEUS./;
 ATH=(E.J.KAPTEIN'1',H.P.BLOK'1',J.BLOK'1');
 INST-ATH=(2NEDFUL'1');
 REF=NP/A;
 VLP=312(1978)97;
 RCTS=(87SR(P,P)87SR,88SR(P,P)88SR);
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 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,60;
 ENR=X%'1';
 /*@3@*/
 CHM=SRO;
 THK-TGT=0.098MG/CM**2;
 BAC=C;
 THK-BAC=0.020MG/CM**2;
 POL-TGT=NO;
 ACC=(CYC);
 INST-ACC=2NEDFUL;
 INC-ENGY-LAB-RANGE=(20.5MEV);
 POL-PRJ=NO;
 DET-PARTCL=(P);
 DET-SYS=(MAG+PS-SI);
 SOLID-ANGL=XMSR'2';
 /*@4@*/
 ERS-DET=9[14KEV;
 ANL=(DWBA'3');
 /*@5@*/
 RCT=87SR(P,P)87SR;
 PHQ=(OPT-POTL-PARA);
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 /* Descriptive Parameters                                            */
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 \\DATA,60;
 PRJ=P;
 TGT=87SR;
 INC-ENGY=20.55MEV;
 POTL-FORM=/-(V*F(ZR)+I*(WV*F(XIV)-4*WS*DIF(1!XIS)F(XIS)+WG*G(XG)))+(HBA
 R/(MPI*C))**2*1/RSO*(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 RADIUS RC*A**(1/3):/;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 V RR AR WV RIV AIV WS RIS AIS WG RIG AIG VSO
 RRSO ARSO WSO RISO AISO RC
 (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV)
 (FM) (FM) (MEV) (FM) (FM) (FM)
 -54.37 1.17 0.578 0 1.088 1.010 -6.654 1.088 1.010 X X X -6.78 1.01
 0.75 X X X 1.25
 -53.89 1.17 0.75 -1.82 1.32 0.60 -8.18 1.32 0.60 X X X -6.2 1.01
 0.75 X X X 1.25
 \END;
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