/* 2005-12-19 File is generated by HENDEL. */
 \\BIB,1[8;
 D#=D1573;
 TITLE=/ Coulomb dissociation of a halo nucleus 11Be at 72A MeV /;
 PURPOSE=/ To perform the coincidence measurement of 11Be
           dissociation /;
 ATH=(T.NAKAMURA'1', S.SHIMOURA'1', T.KOBAYASHI'2', T.TERANISHI'1',
      K.ABE'3', N.AOI'1', Y.DOKI'1', M.FUJIMAKI'2', N.INABE'2',
      N.IWASA'4', K.KATORI'3', T.KUBO'2', H.OKUNO'1', T.SUZUKI'2',
      I.TANIHATA'2', Y.WATANABE'2', A.YOSHIDA'2', M.ISHIHARA'1,2');
 INST-ATH=(2JPNTOK'1', 2JPNIPC'2', 2JPNOSA'3', 2JPNRIK'4');
      /* '1' Department of Physics */
      /* '3' Department of Physics */
      /* '4' Department of Physics */
 REF=PL/B;
 VLP=331(1994)296;
 RCTS=(PB(11BE,11BE)PB, 12C(11BE,11BE)12C, PB(11BE,N,10BE)PB);
 PHQS=(ENGY-SPEC, STRGTH-FUNCT, ANGL-DSTRN'5', MOM-DSTRN'6',
       ANGL-DSTRN'7', ANGL-DSTRN'8');
 /* '5' dsigma/db (b=impact parameter. b is related to the
    scattering angle theta of the c.m. of 10Be+n system as b=a cot
    (theta/2), where a represents half the distance of closest approach
    in the classical Coulomb head-on collision) */
 /* '6' Mean values of longitudinal momentum distributions */
 /* '7' dsigma/dphi (azimuthal angular distibution of 10Be in 11Be
    rest frame) */
 /* '8' dsigma/dcos(theta) (polar angular distibution of 10Be in
    11Be rest frame) */

 \\EXP,1[8;
 /* 2005-09-13 : Converted, Sr + On. Converted to EXFOR E1573 */
 /* 2005-10-18 : Altered, Ah + Sr. Re-digitized */
 CHM=ELM;
 PHYS-FORM=SLD;
 ACC=PRJFS'9';
 /* '9' 11Be is provided by using a projectile fragmentation of
        100A MeV 18O */
 INST-ACC=2JPNIPC'10';
 /* '10' RIPS */
 INC-ENGY-LAB=72.0MEV/A;
 ERS-PRJ=0.2MEV/A'11';
 /* '11' FWHM */
 DET-PARTCL=(N,10BE);
 COINC=(N,10BE);
 ANT-COINC=NO;
 DET-SYS=(MAG'12',SCT'12',X'13',SCT'14',EDE'15',TOF'16');
 /* '12' To detect 10Be */
 /* '13' Drift chamber (To detect 10Be) */
 /* '14' To detect neutron */
 /* '15' To identify 10Be */
 /* '16' To determine momentum vector of 10Be and neutron */
 ERS-DET=XKEV'17';
 /* '17' Energy resolution is proportional to square root of
         relative energy between 10Be and neutron. 450 keV FWHM is
         estimated at 1 MeV (relative energy). */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement (To identify
      10Be)
    - Time-of-flight (To determine momentum vector of 10Be and
      neutron)
 */

 \\EXP,1;
 RCT=PB(11BE,11BE)PB;
 RTY=INEL-SCATT;
 PHQ=ENGY-SPEC;
 THK-TGT=104MG/CM**2;

 \\DATA,1;
 INC-ENGY-LAB=72.0MEV/A;
 SYS-ERR=[20%'18';
 /* '18' Total systematic error. Uncertainty in the absolute
         normalization (mainly coming from uncertainties in neutron
         detection efficiency) */
 EMT-2=N;
 \DATA;
 EXC-ENGY-EMT DSIGMA/DE DELTA-DSIGMA/DE'19'
 (MEV) (B/MEV) (B/MEV)
 5.560E-02 6.831E-01 +-1.752E-01
 1.577E-01 1.546E+00 +-2.234E-01
 2.621E-01 1.837E+00 +-2.565E-01
 3.634E-01 1.724E+00 +-2.684E-01
 4.655E-01 1.609E+00 +-2.686E-01
 5.676E-01 1.426E+00 +-2.612E-01
 7.119E-01 1.121E+00 +-1.947E-01
 9.151E-01 1.058E+00 +-1.814E-01
 1.108E+00 9.117E-01 +-1.879E-01
 1.306E+00 6.756E-01 +-1.998E-01
 1.501E+00 2.883E-01 +-2.160E-01
 1.807E+00 4.268E-01 +-1.529E-01
 2.207E+00 1.301E-01 +-1.462E-01
 2.607E+00 1.653E-01 +-1.573E-01
 3.000E+00 -1.760E-01 +-1.718E-01
 3.500E+00 -6.344E-02 +-1.298E-01
 \END;
 /* Data scanned from Fig.1(a), p298 in reference */
 /* '19' Statistical error */

 \\EXP,2;
 RCT=12C(11BE,11BE)12C;
 RTY=INEL-SCATT;
 PHQ=ENGY-SPEC;
 THK-TGT=184MG/CM**2;

 \\DATA,2;
 INC-ENGY-LAB=72.0MEV/A;
 SYS-ERR=[20%'20';
 /* '20' Total systematic error. Uncertainty in the absolute
         normalization (mainly coming from uncertainties in neutron
         detection efficiency) */
 EMT-2=N;
 \DATA;
 EXC-ENGY-EMT DSIGMA/DE
 (MEV) (B/MEV)
 5.095E-02 1.449E-02
 1.459E-01 3.532E-02
 2.495E-01 3.603E-02
 3.531E-01 4.079E-02
 4.524E-01 3.341E-02
 5.517E-01 3.410E-02
 6.985E-01 2.706E-02
 9.014E-01 5.267E-02
 1.100E+00 6.212E-02
 1.299E+00 3.931E-02
 1.497E+00 5.279E-02
 1.804E+00 3.073E-02
 2.210E+00 4.162E-02
 2.607E+00 3.229E-02
 3.004E+00 2.296E-02
 3.500E+00 2.642E-02
 \END;
 /* Data scanned from Fig.1(a), p298 in reference */

 \\EXP,3;
 RCT=(PB(11BE,11BE)PB, 12C(11BE,11BE)12C);
 RTY=(INEL-SCATT,X'21');
 /* '21' Coulomb breakup reaction */
 PHQ=STRGTH-FUNCT;
 THK-TGT=XMG/CM**2'22';
 /* '22' 104 mg/cm**2 for Pb target, 184 mg/cm**2 for C target */
 ANL=X'23';
 /* '23' Direct breakup model */
 /* Analysis:
    - Coulomb part of the dissociation on Pb is obtained by
      subtraction the nuclear contribution from the original spectrum.
      Cross section for C target is used to estimate the nuclear
      contribution.
    - Equivalent photon method [C.A. Bertulani and G. Banr, Phys.
      Rep. 163 (1988) 299.]
 */

 \\DATA,3;
 INC-ENGY-LAB=72.0MEV/A;
 SYS-ERR=[20%'24';
 /* '24' Total systematic error. Uncertainty in the absolute
         normalization (mainly coming from uncertainties in neutron
         detection efficiency) */
 EMT-2=N;
 \DATA;
 EXC-ENGY-EMT BE-L'25' DELTA-BE-L'25,26'
 (MEV) (UNIT) (UNIT)
 5.452E-01 2.996E-01 +-8.126E-02
 6.592E-01 7.202E-01 +-1.308E-01
 7.618E-01 9.108E-01 +-1.308E-01
 8.610E-01 9.091E-01 +-1.427E-01
 9.603E-01 9.014E-01 +-1.546E-01
 1.064E+00 8.442E-01 +-1.546E-01
 1.213E+00 7.158E-01 +-1.269E-01
 1.412E+00 7.124E-01 +-1.308E-01
 1.611E+00 6.535E-01 +-1.487E-01
 1.806E+00 5.390E-01 +-1.789E-01
 1.997E+00 1.966E-01 +-2.064E-01
 2.310E+00 4.183E-01 +-1.633E-01
 2.706E+00 8.928E-02 +-1.847E-01
 3.104E+00 1.734E-01 +-2.345E-01
 3.504E+00 8.450E-03 +-2.816E-01
 3.999E+00 8.077E-03 +-2.628E-01
 \END;
 /* Data scanned from Fig.1(b), p298 in reference */
 /* '25' dB(E1)/dE (dipole strength distribtuion) [e**2fm**2] */
 /* '26' Statistical error */

 \\EXP,4;
 RCT=PB(11BE,11BE)PB;
 RTY=INEL-SCATT;
 PHQ=ANGL-DSTRN'27';
 /* '27' dsigma/db (b=impact parameter. b is related to the
         scattering angle theta of the c.m. of 10Be+n system as b=a cot
         (theta/2), where a represents half the distance of closest
         approach in the classical Coulomb head-on collision) */
 THK-TGT=104MG/CM**2;
 ANL=X'28';
 /* '28' Direct breakup model */

 \\DATA,4;
 INC-ENGY-LAB=72.0MEV/A;
 SYS-ERR=[20%'29';
 /* '29' Total systematic error. Uncertainty in the absolute
         normalization (mainly coming from uncertainties in neutron
         detection efficiency) */
 EMT-2=N;
 \DATA;
 DATA1'30' DATA2'31' DELTA-DATA2'31,32'
 (FM) (UNIT) (UNIT)
 7.551E+00 1.510E+01 +-3.890E+01
 1.048E+01 1.386E+01 +-2.593E+01
 1.341E+01 6.868E+01 +-2.507E+01
 1.650E+01 7.899E+01 +-1.849E+01
 1.948E+01 7.764E+01 +-1.667E+01
 2.248E+01 9.640E+01 +-1.539E+01
 2.550E+01 4.109E+01 +-1.635E+01
 2.845E+01 3.917E+01 +-1.427E+01
 3.148E+01 4.267E+01 +-1.394E+01
 3.443E+01 2.907E+01 +-1.411E+01
 3.755E+01 1.785E+01 +-1.363E+01
 4.055E+01 3.136E+00 +-1.372E+01
 4.361E+01 1.065E+01 +-1.154E+01
 4.661E+01 2.212E+01 +-1.082E+01
 4.972E+01 1.216E+01 +-1.085E+01
 5.260E+01 1.466E+01 +-1.010E+01
 5.570E+01 1.771E+01 +-1.010E+01
 5.866E+01 2.195E+01 +-8.892E+00
 6.151E+01 1.182E+01 +-7.291E+00
 6.454E+01 2.237E+01 +-8.401E+00
 6.755E+01 2.759E+00 +-7.469E+00
 7.060E+01 3.140E+00 +-6.574E+00
 7.355E+01 4.426E+00 +-7.536E+00
 7.665E+01 7.636E+00 +-5.772E+00
 7.968E+01 5.846E-01 +-5.451E+00
 8.269E+01 1.886E+00 +-7.647E+00
 9.177E+01 7.812E+00 +-5.131E+00
 9.464E+01 3.487E+00 +-5.131E+00
 9.767E+01 4.392E+00 +-4.446E+00
 \END;
 /* Data scanned from Fig.1(c), p298 in reference */
 /* '30' Impact parameter b. b is related to the scattering angle
         theta of the c.m. of 10Be+n system as b=a cot (theta/2), where
         a represents half the distance of closest approach in the
         classical Coulomb head-on collision */
 /* '31' dsigma/b [mb/fm] */
 /* '32' Statistical error */

 \\EXP,5;
 RCT=PB(11BE,N,10BE)PB;
 PHQ=MOM-DSTRN'33';
 /* '33' Mean values of longitudinal momentum distributions */
 THK-TGT=104MG/CM**2;
 ANL=X'34';
 /* '34' First-order perturbation theory */

 \\DATA,5;
 INC-ENGY-LAB=72.0MEV/A;
 EMT-2=N;
 INTRM=11BE;
 \DATA;
 THTL-INTRM'35' MOM-LNGTD'36' DELTA-DATA1'37'
 (DEG) (MEV/C) (MEV/C)
 4.991E-01 -6.097E-01 +-1.198E+00
 1.495E+00 2.453E+00 +-1.363E+00
 2.500E+00 4.359E+00 +-3.056E+00
 \END;
 /* Data scanned from Fig.2, p300 in reference */
 /* '35' Scattering angle theta of the c.m. of 10Be+n system */
 /* '36' Mean values of longitudinal momentum of 10Be in the rest
         frame of incident 11Be */
 /* '37' Error in mean values of longitudinal momentum of 10Be
         (Statistical error) */

 \\EXP,6;
 RCT=PB(11BE,N,10BE)PB;
 PHQ=MOM-DSTRN'38';
 /* '38' Mean values of longitudinal momentum distributions */
 THK-TGT=104MG/CM**2;
 ANL=X'39';
 /* '39' First-order perturbation theory */

 \\DATA,6;
 INC-ENGY-LAB=72.0MEV/A;
 EMT-2=N;
 INTRM=11BE;
 \DATA;
 THTL-INTRM'40' MOM-LNGTD'41' DELTA-DATA1'42'
 (DEG) (MEV/C) (MEV/C)
 4.980E-01 -9.367E-01 +-9.429E-01
 1.492E+00 -3.611E+00 +-1.162E+00
 2.496E+00 -8.602E+00 +-1.966E+00
 \END;
 /* Data scanned from Fig.2, p300 in reference */
 /* '40' Scattering angle theta of the c.m. of 10Be+n system */
 /* '41' Mean values of longitudinal momentum of neutron in the
         rest frame of incident 11Be */
 /* '42' Error in mean values of longitudinal momentum of neutron
         (Statistical error) */

 \\EXP,7;
 RCT=PB(11BE,N,10BE)PB;
 PHQ=ANGL-DSTRN'43';
 /* '43' dsigma/dphi (azimuthal angular distibution of 10Be in
         11Be rest frame) */
 THK-TGT=104MG/CM**2;
 ANL=X'44';
 /* '44' First-order time-dependent perturbation theory */

 \\DATA,7;
 INC-ENGY-LAB=72.0MEV/A;
 EMT-2=N;
 INTRM=11BE;
 EXC-ENGY-INTRM-MAX=4MEV'45';
 /* '45' Relative energy between 10Be and neutron */
 \DATA;
 DATA1'46' DATA2'47' DELTA-DATA2'47,48'
 (DEG) (UNIT) (UNIT)
 8.770E+00 2.424E-01 +-5.498E-02
 2.571E+01 1.793E-01 +-5.778E-02
 4.265E+01 3.135E-01 +-5.812E-02
 5.959E+01 3.532E-01 +-6.155E-02
 7.726E+01 4.370E-01 +-6.751E-02
 9.429E+01 4.251E-01 +-6.693E-02
 1.117E+02 4.651E-01 +-6.337E-02
 1.286E+02 2.483E-01 +-5.778E-02
 1.458E+02 1.647E-01 +-5.964E-02
 1.635E+02 1.556E-01 +-5.509E-02
 1.814E+02 1.588E-01 +-5.964E-02
 1.977E+02 3.070E-01 +-6.553E-02
 2.150E+02 2.116E-01 +-6.989E-02
 2.321E+02 3.239E-01 +-8.098E-02
 2.490E+02 2.626E-01 +-1.016E-01
 2.663E+02 4.648E-01 +-1.121E-01
 2.826E+02 3.596E-01 +-1.012E-01
 3.002E+02 4.944E-01 +-8.591E-02
 3.172E+02 3.281E-01 +-7.827E-02
 3.347E+02 3.033E-01 +-6.243E-02
 3.522E+02 2.309E-01 +-5.497E-02
 \END;
 /* Data scanned from Fig.3(a), p300 in reference */
 /* '46' Scattering angle phi of 10Be in 11Be rest frame */
 /* '47' dsigma/dphi [b/rad] */
 /* '48' Statistical error */

 \\EXP,8;
 RCT=PB(11BE,N,10BE)PB;
 PHQ=ANGL-DSTRN'49';
 /* '49' dsigma/dcos(theta) (polar angular distibution of 10Be in
         11Be rest frame) */
 THK-TGT=104MG/CM**2;
 ANL=X'50';
 /* '50' First-order time-dependent perturbation theory */

 \\DATA,8;
 INC-ENGY-LAB=72.0MEV/A;
 EMT-2=N;
 INTRM=11BE;
 EXC-ENGY-INTRM-MAX=4MEV'51';
 /* '51' Relative energy between 10Be and neutron */
 \DATA;
 COS-CM'52' DATA1'53' DELTA-DATA1'53,54'
 (NODIM) (B) (B)
 -9.521E-01 8.147E-01 +-1.723E-01
 -8.541E-01 6.946E-01 +-1.811E-01
 -7.628E-01 9.050E-01 +-1.764E-01
 -6.673E-01 8.867E-01 +-1.978E-01
 -5.710E-01 5.895E-01 +-2.145E-01
 -4.761E-01 8.333E-01 +-2.264E-01
 -3.823E-01 7.744E-01 +-2.431E-01
 -2.879E-01 1.176E+00 +-2.336E-01
 -1.920E-01 1.038E+00 +-2.574E-01
 -9.435E-02 1.568E+00 +-2.645E-01
 3.409E-03 1.397E+00 +-2.717E-01
 9.640E-02 9.949E-01 +-2.526E-01
 1.935E-01 1.065E+00 +-2.693E-01
 2.882E-01 1.375E+00 +-2.550E-01
 3.797E-01 8.231E-01 +-2.717E-01
 4.727E-01 1.084E+00 +-2.359E-01
 5.691E-01 7.673E-01 +-2.359E-01
 6.638E-01 1.071E+00 +-2.073E-01
 7.621E-01 6.806E-01 +-2.097E-01
 8.567E-01 1.029E+00 +-1.954E-01
 9.517E-01 1.192E+00 +-1.883E-01
 \END;
 /* Data scanned from Fig.3(b), p300 in reference */
 /* '52' Cosine of scattering angle theta of 10Be in 11Be rest
         frame */
 /* '53' dsigma/dcos(theta) */
 /* '54' Statistical error */
 \\END;