/*===================================================================*/
 /* NRDF D1821 Data No.1                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1821;
 TITLE=/ In-beam gamma spectroscopy of 34Si with deuteron inelastic
         scattering using reverse kinematics /;
 ATH=(N.IWASA'1', T.MOTOBAYASHI'2', H.SAKURAI'3', H.AKIYOSHI'2',
      Y.ANDO'4', N.AOI'3', H.BABA'4', N.FUKUDA'3', Z.FULOP'5',
      U.FUTAKAMI'4', T.GOMI'4', Y.HIGURASHI'4', K.IEKI'4', H.IWASAKI'3',
      T.KUBO'2', S.KUBONO'6', H.KINUGAWA'4', H.KUMAGAI'2', M.KUNIBU'4',
      S.MICHIMASA'6', T.MINEMURA'4', H.MURAKAMI'4', K.SAGARA'7',
      A.SAITO'4', S.SHIMOURA'6', S.TAKEUCHI'2', Y.YANAGISAWA'2',
      K.YONEDA'2', M.ISHIHARA'2');
 INST-ATH=(2JPNTOH'1', 2JPNIPC'2', 2JPNTOK'3', 2JPNRIK'4', 3HUNDEB'5',
           2JPNTOK'6', 2JPNKYU'7');
      /* '1' Department of Physics */
      /* '3' Department of Physics */
      /* '4' Department of Physics */
      /* '6' Center for Nuclear Study (CNS) */
      /* '7' Department of Physics */
 REF=PR/C;
 VLP=67(2003)064315;
 RCTS=2H(34SI,34SI)2H;
 PHQS=GAMMA-SPEC;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2003-08-22 : Compiled, St + On. */
 RTY=INEL-SCATT;
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=LIQD;
 THK-TGT=150+-5MG/CM**2'8';
 /* '8' Target has two windows. Thickness was decreasing to 97+-8
        mg/cm2 at the edges of the windows. */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'9',PRJFS'10');
 /* '9' 40Ar primary beam at 95A MeV on Be target */
 /* '10' 34Si secondary beam */
 INST-ACC=(2JPNIPC'9',2JPNIPC'10');
 /* '10' RIKEN projectile-fragment separator */
 INC-ENGY-LAB=38.4MEV/A'11';
 /* '11' Average beam energy in the center of the target. */
 POL-PRJ=0%;
 ANT-COINC=NO;
 DET-SYS=(CNTR-TLSCP'12',SCT'13',PPAC'14',NAI'15',TOF'16',EDE);
 /* '12' To detect and identify reaction products */
 /* '13' To obtain TOF between target and telescope */
 /* '14' To obtain TOF between target and telescope */
 /* '15' To detect deexcitation gamma. Typical energy resolution
         is 9% for 0.661 MeV gamma rays from 137Cs. Total detection
         efficiency is 4.9% for a 3.326 MeV photon emitted from a
         source moving with a velocity of 0.28c. */
 /* '16' To identify beam particles event by event */
 ERS-DET=9%;
 ANL=DSA;
 /* Experimental Method:
    - Time-of-flight (To identify beam particles event by event)
    - Particle identification by 'E/Delta E' measurement
 /* 2006-10-05 : Altered, Is. Re-digitized */
 RCT=2H(34SI,34SI)2H;
 PHQ=GAMMA-SPEC;
 DET-PARTCL=(GAMMA'18',34SI);
 /* '18' Prompt gamma from 34Si */
 COINC=(GAMMA,34SI);
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-ENGY-LAB=38.4MEV/A'17';
 /* '17' Average beam energy in the center of the target. */
 EMT-2=GAMMA'19';
 THTL-2=40[138DEG;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 ENGY-GAMMA'19' COUNTS DELTA-COUNTS
 (KEV) (ARB) (ARB)
 2.297E+02 1.428E+04 +-NEGLIGIBLE
 2.777E+02 1.488E+04 +-NEGLIGIBLE
 3.296E+02 1.338E+04 +-NEGLIGIBLE
 3.775E+02 1.192E+04 +-NEGLIGIBLE
 4.295E+02 1.154E+04 +-NEGLIGIBLE
 4.774E+02 1.107E+04 +-NEGLIGIBLE
 5.334E+02 1.019E+04 +-NEGLIGIBLE
 5.773E+02 1.023E+04 +-NEGLIGIBLE
 6.332E+02 8.786E+03 +-NEGLIGIBLE
 6.812E+02 7.473E+03 +-NEGLIGIBLE
 7.291E+02 6.386E+03 +-NEGLIGIBLE
 7.851E+02 5.768E+03 +-NEGLIGIBLE
 8.290E+02 5.482E+03 +-NEGLIGIBLE
 8.809E+02 6.657E+03 +-NEGLIGIBLE
 9.249E+02 8.745E+03 +-NEGLIGIBLE
 9.808E+02 8.950E+03 +-NEGLIGIBLE
 1.029E+03 8.122E+03 +-NEGLIGIBLE
 1.081E+03 5.407E+03 +-NEGLIGIBLE
 1.129E+03 4.193E+03 +-NEGLIGIBLE
 1.181E+03 4.311E+03 +-NEGLIGIBLE
 1.229E+03 4.351E+03 +-NEGLIGIBLE
 1.279E+03 4.154E+03 +-7.480E+01
 1.329E+03 3.746E+03 +-6.744E+01
 1.381E+03 3.614E+03 +-6.508E+01
 1.427E+03 3.719E+03 +-6.696E+01
 1.480E+03 3.719E+03 +-6.696E+01
 1.532E+03 3.563E+03 +-6.416E+01
 1.576E+03 3.343E+03 +-5.872E+01
 1.628E+03 3.550E+03 +-6.393E+01
 1.683E+03 3.706E+03 +-6.672E+01
 1.732E+03 3.876E+03 +-7.578E+01
 1.782E+03 3.550E+03 +-6.393E+01
 1.828E+03 3.353E+03 +-6.038E+01
 1.881E+03 3.167E+03 +-5.703E+01
 1.930E+03 3.078E+03 +-5.542E+01
 1.979E+03 3.111E+03 +-5.602E+01
 2.029E+03 3.013E+03 +-4.332E+01
 2.078E+03 2.845E+03 +-5.124E+01
 2.127E+03 2.775E+03 +-6.007E+01
 2.180E+03 2.785E+03 +-5.015E+01
 2.226E+03 2.897E+03 +-6.270E+01
 2.278E+03 2.981E+03 +-5.367E+01
 2.328E+03 2.866E+03 +-6.203E+01
 2.383E+03 2.775E+03 +-6.007E+01
 2.426E+03 2.707E+03 +-4.874E+01
 2.479E+03 2.566E+03 +-5.554E+01
 2.528E+03 2.668E+03 +-5.776E+01
 2.582E+03 2.586E+03 +-5.367E+01
 2.627E+03 2.723E+03 +-5.187E+01
 2.682E+03 2.970E+03 +-5.348E+01
 2.726E+03 3.213E+03 +-5.785E+01
 2.781E+03 3.256E+03 +-6.103E+01
 2.829E+03 3.231E+03 +-6.321E+01
 2.880E+03 3.056E+03 +-7.742E+01
 2.929E+03 2.886E+03 +-6.248E+01
 2.983E+03 2.617E+03 +-6.062E+01
 3.031E+03 2.297E+03 +-4.972E+01
 3.083E+03 2.108E+03 +-5.334E+01
 3.130E+03 2.139E+03 +-4.629E+01
 3.182E+03 2.206E+03 +-4.426E+01
 3.230E+03 2.546E+03 +-5.106E+01
 3.275E+03 2.891E+03 +-4.630E+01
 3.330E+03 2.937E+03 +-5.892E+01
 3.378E+03 2.638E+03 +-5.292E+01
 3.426E+03 2.278E+03 +-5.494E+01
 3.474E+03 1.738E+03 +-4.193E+01
 3.526E+03 1.275E+03 +-4.118E+01
 3.577E+03 1.119E+03 +-3.612E+01
 3.629E+03 1.013E+03 +-2.856E+01
 3.677E+03 9.098E+02 +-2.938E+01
 3.731E+03 9.890E+02 +-3.193E+01
 3.776E+03 9.244E+02 +-3.365E+01
 3.831E+03 8.640E+02 +-3.145E+01
 3.879E+03 9.062E+02 +-2.926E+01
 3.931E+03 8.606E+02 +-3.132E+01
 3.979E+03 7.670E+02 +-3.108E+01
 4.030E+03 7.255E+02 +-2.940E+01
 4.078E+03 6.440E+02 +-2.610E+01
 4.130E+03 7.226E+02 +-2.928E+01
 4.174E+03 8.044E+02 +-2.928E+01
 4.229E+03 7.226E+02 +-2.630E+01
 4.274E+03 6.835E+02 +-2.770E+01
 4.332E+03 6.862E+02 +-2.781E+01
 4.373E+03 6.288E+02 +-2.548E+01
 4.432E+03 5.386E+02 +-2.405E+01
 4.480E+03 5.135E+02 +-2.294E+01
 4.528E+03 4.522E+02 +-2.208E+01
 4.576E+03 4.363E+02 +-2.130E+01
 4.627E+03 4.312E+02 +-2.285E+01
 4.675E+03 4.030E+02 +-2.136E+01
 4.727E+03 4.160E+02 +-2.031E+01
 4.775E+03 4.193E+02 +-2.222E+01
 4.830E+03 3.782E+02 +-2.004E+01
 4.874E+03 3.998E+02 +-2.119E+01
 4.929E+03 3.737E+02 +-2.137E+01
 4.977E+03 3.479E+02 +-1.887E+01
 \END;
 /*===================================================================*/