DARPE: Search Results
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 /* NRDF D1640 Data No.3                                              */
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 /* Bibliography                                                      */
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 \\BIB,3;
 D#=D1640;
 TITLE=/ Anomaly in the 15N, 16O, 19F + 54,56Fe fusion cross sections
         around the Coulomb barrier energy /;
 PURPOSE=/ The determination of fusion corss sections /;
 ATH=(H.FUNAKI'1', E.ARAI'1');
 INST-ATH=(2JPNTIT'1');
 REF=NP/A;
 VLP=556(1993)307;
 RCTS=(54FE(19F,FUSN), 54FE(15N,FUSN), 56FE(15N,FUSN), 54FE(16O,FUSN),
       56FE(16O,FUSN), 56FE(19F,FUSN));
 PHQS=(ANGL-DSTRN'2', EXC-FUNCT'3');
 /* '2' Angular distribution of evaporation residues */
 /* '3' Excitation function of the fusion reaction */
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 /* Experimental Conditions                                           */
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 \\EXP,3;
 /* 2003-09-12 : Converted, Km + Am + On. Data converted to EXFOR
    E1640 */
 /* 2007-05-10 : Altered, On. MeV/u -> MeV/A in free text fields */
 /* Related references 
    - E.Arai et al., NIM/B, 64(1992)296.
    (Detailed description of the system is given)
 RTY=FUSN;
 CHM=X'4';
 /* '4' Fe2O3 */
 PHYS-FORM=SLD;
 BAC=C;
 THK-BAC=0.020MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=LINAC'5';
 /* '5' Heavy Ion Linac System */
 INST-ACC=2JPNTIT;
 POL-PRJ=0%;
 DET-PARTCL=X'6';
 /* '6' evaporation residues */
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(CNTR-TLSCP'7',SBD'8',TOF);
 /* '7' The t.o.f. counter telescope has two timing detectors which
        define a flight path of 50 cm. */
 /* '8' A 100 mm**2 surface-barrier detector (SBD) provides the
        kinetic energy (E) signal of particles. */
 ERS-DET=XKEV'9';
 /* '9' The mass separation of the spectrometer has been mainly
        determined by the energy resolution to be delta A = 4 in the
        A-region around 70. */
 CALB-DET=/ The beam energy analyzing magnet has been calibrated by
            measuring the sharp peak observed at 6.42 MeV in the
            1H(19F,alpha gamma)16O reaction. /;
 MONTR-RCT=/ , As a beam monitor a surface-barrier detector (SBD) was
             installed at 165 degrees with respect to the beam
             direction. /;
 /* 2006-11-22 : Altered, Mh. Re-digitized */
 RCT=54FE(15N,FUSN);
 PHQ=EXC-FUNCT'18';
 /* '18' Excitation function of the fusion reaction */
 ENR=97.21%;
 THK-TGT=0.110MG/CM**2'19';
 /* '19' The thickness was determined by the Rutherford
         backscattering technique. */
 INC-ENGY-LAB=2[3MEV/A'20';
 /* '20' The final energy of beams has been raised or lowered by
        the second linac in the range between 2 and 3 MeV/u. */
 ANL=CC'21';
 /* '21' the one-dimensional barrier-penetration model [C.H.Dasso
         et al. Comput.Phys.Commun.46(1987)187] */
 /* Analysis:
    - Integration of angular distribution (Integration of
      differential cross sections (angular distributions of evaporation
      residue))
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 /* Descriptive Parameters                                            */
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 \\DATA,3;
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM
 (MEV) (MB) (MB)
 2.482E+01 2.818E+01 +-6.670E+00
 2.601E+01 8.445E+01 +-1.176E+01
 2.661E+01 1.078E+02 +-6.528E+00
 2.751E+01 1.801E+02 +-NEGLIGIBLE
 2.771E+01 1.870E+02 +-NEGLIGIBLE
 2.841E+01 3.074E+02 +-3.444E+01
 2.954E+01 2.973E+02 +-5.003E+01
 3.270E+01 6.508E+02 +-7.294E+01
 3.436E+01 7.739E+02 +-7.339E+01
 3.568E+01 6.504E+02 +-4.128E+01
 \END;
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