/*===================================================================*/
 /* NRDF D0163 Data No.46                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,46;
 D#=D163;
 TITLE=/DEEPLY BOUND HOLE STATES AND ISOBARIC ANALOG STATES OBSERVED
        BY NEUTRON PICKUP REACTIONS ON EVEN TIN ISOTOPES/;
 ATH=(M.SEKIGUCHI'1',Y.SHIDA'1',F.SOGA'1',Y.HIRAO'1',M.SAKAI'1');
 INST-ATH=(2JPNINS'1');
 REF=NP/A;
 VLP=278(1977)231;
 RCTS=(116SN(3HE,ALPHA)115SN,118SN(3HE,ALPHA)117SN,
       120SN(3HE,ALPHA)119SN,124SN(3HE,ALPHA)123SN,
       116SN(P,D)115SN,      118SN(P,D)117SN,
       120SN(P,D)117SN,      120SN(P,D)119SN,
       122SN(P,D)121SN,124SN(P,D)123SN);
 /* '11' TO '31' ARE COMMENTS ON DATA HEADINGS' */
 /* '11': YARGET ISOSPIN*/
 /* '12': C2SN BY SEPARATION ENERGY METHOD */
 /* '13': (2T0+1)C2SN BY SEPARATION ENERGY METHOD */
 /* '14': C2SN BY COUPLED CHANNEL METHOD */
 /* '15': (2T0+1)C2SN BY COUPLED CHANNEL METHOD*/
 /* '21': VALUES FROM PHYS.REV.C3(1971)1168 EXC-ENGY FOR RSD OF SN */
 /* '22': EXC-ENGY FOR RSD OF IN*/
 /* '23': NUCL.DATA A9(1971)267 HASBEEN USED TO DEDUCE*/
 /* '31': MAX-DSIGMA/DOMEGA VALUE AT MAXMUM AROUND 24 OF DWBA CURVE
          AFTER NORMARIZATION TO DATA FROM THE (P,D) REACTION */
 /* IN THE COSE OF COUPLED-CHANNEL CALCULATION,AN ISOSPIN-DEPENDENT
    POTENTIAL OF THE FORM (T.T)U1 IS ADDED TO THE BINDING POTENTIAL WITH
    U1=-4V1'/A*(D/DR:F(XR)),F(X)=(1+E**X)**(-1),XR=(R-RR*A**(1/3))/AR,
    GAMMA R=1.25 GAMMA R=0.65,V1'=225MEV */
 /* DWBA CALCULATIONS WERE CATTIED OUT WITH THE CODE DWUCK AND THE
    TOSBAC-3400 */
 /* THE COUPLED-CHANNEL CALCULATIONS WERE CARRIED OUT WITH CODE SUMIT
    AND SYBER 74-16 AT THE UNIVERSITY OF GRONIGEN */
 /* IN THE CASED OS DWBA AND C-C CALCULATIONS,NORMALIZATION FACTOR
    N=2.33 WAS USED.*/
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 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,46;
 POL-TGT=NO;
 ALGN-TGT=NO;
 ACC=(SYNCYC);
 INST-ACC=2JPNINS;
 INC-ENGY-RANGE=(51.9MEV);
 DELTA-INC-ENGY=XKEV;
 POL-PRJ=NO;
 DET-PARTCL=(P);
 DET-SYS=(MAG,PROP-CNTR'1');
 /* '1' BACKED WITH SCINTILLATION COUNTERS */
 SOLID-ANGL=XMSR;
 ERS-DET=(90KEV'1',100KEV'2');
 /* '1' FOR THE GROUND STATE '2' FOR THE ISOBARIC ANALOG STATES */
 ANL=(CC,DWBA,SHELL-MODEL);
 PHQ=(EXC-FUNCT,ANGL-DSTRN,ENGY-SPEC,EXC-ENGY,ISOSPIN,IAS,OPT-POTL-PARA,
      COULOMB-DISPLACEMENT-ENGY);
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,46;
 PRJ=D;
 TGT=(115SN,117SN,119SN,121SN,123SN);
 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):/;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY V  RR   AR   WV    RIV  AIV  WS      RIS  AIS   VSO   RRSO
 ARSO  RC
 (MEV) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV)   (FM) (FM)  (MEV) (FM)
 (FM)  (FM)
 X     VD'1' 1.17 0.75 WD'2' 1.32 AD'3' WSD'4' 1.32 AD'3' 6.2   1.01
 0.75  1.30
 /* '1'VD=110.3-0.64(1/2ED)+0.4Z/(A-1)**(1/3)
    '2'WD=0.44(1/2ED)-4.26
    '3'AD=0.51+0.7(N-Z-1)/(A-1)
    '4'WSD=24.8-0.50(1/2ED)
 \END;
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