DARPE: Search Results
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 /* NRDF D1658 Data No.9                                              */
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 /* Bibliography                                                      */
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 \\BIB,9;
 D#=D1658;
 TITLE=/ Fusion and breakup at the barrier with 11Be /;
 PURPOSE=/ To measure the fusion cross-sections with unstable beams
 ATH=(A.YOSHIDA'1', C.SIGNORINI'2', T.FUKUDA'3', Y.WATANABE'1',
      N.AOI'4', M.HIRAI'4', M.ISHIHARA'1,4', H.KOBINATA'4', Y.MIZOI'3',
      L.MUELLER'2', Y.NAGASHIMA'5', J.NAKANO'3', T.NOMURA'3', Y.H.PU'1',
      F.SCARLASSARA'2');
 INST-ATH=(2JPNIPC'1', 2ITYPAD'2', 2JPNINS'3', 2JPNTOK'4',
           2JPNTSU'5');
      /* '2' Physics Department of the University and INFN */
      /* '4' Department of Physics */
      /* '5' College of Medical Technology */
 REF=PL/B;
 VLP=389(1996)457;
 RCTS=(209BI(11BE,4*N)216FR, 209BI(11BE,5*N)215FR,
       209BI(10BE,3*N)216FR, 209BI(10BE,4*N)215FR, 209BI(9BE,3*N)215FR,
       209BI(9BE,4*N)214FR, 209BI(9BE,5*N)213FR, 209BI(9BE,FISSN));
 PHQS=XSECTN;
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 /* Experimental Conditions                                           */
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 \\EXP,9;
 /* 2003-08-15 : Converted, Am + N.Otuka. Data converted to EXFOR
    E1658 */
 PHQ=XSECTN;
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 ANL=STATIST-MODEL'6';
 /* '6' Evaporation code CASCADE [E.Pulhofer, Nucl. Phys.
        A280(1977)267]. */
 /* 2006-11-13 : Altered, Mh. Re-digitized */
 RCT=209BI(9BE,FISSN);
 RTY=FISSN;
 THK-TGT=0.370MG/CM**2;
 BAC=X'62';
 /* '62' Kapton foil, in order to stop all of the recoil
         evaporation residues produced by the reaction. */
 THK-BAC=2.0MG/CM**2;
 ACC=VDGT'63';
 /* '63' 12UD Tandem */
 INST-ACC=2JPNTSU'64';
 /* '64' Tandem Accelerator Center */
 INC-ENGY-CM-RANGE=35[70MEV;
 DET-SYS=SI'65';
 /* '65' to measure alpha-particles, 150 mm2 silicon detector
         located 135 deg to the beam direction and 11 cm from the
         target */
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 /* Descriptive Parameters                                            */
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 \\DATA,9;
 TOT-ERR=<5%;
 NORM=/ Absolute cross-section normalization was deduced by the known
        Rutherford cross section and the ratio between the solid angles
        of the two detectors, measured with a point alpha-source
        positioned at the target site. /;
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM XSECTN
 (MEV) (MB)
 4.125E+01 8.038E+00
 4.316E+01 1.806E+01
 4.602E+01 3.557E+01
 4.919E+01 7.084E+01
 5.371E+01 1.577E+02
 \END;
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