DARPE: Search Results
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 /* NRDF D1883 Data No.13                                             */
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 /* Bibliography                                                      */
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 \\BIB,13;
 D#=D1883;
 TITLE=/ Alpha-particle doorway states in 28Si /;
 ATH=(K.KATORI'1', K.FURUNO'1', T.OOI'1', S.HANASHIMA'1');
 INST-ATH=(2JPNTSU'1');
      /* '1' Institute of Physics and Tandem Accelerator Center */
 REF=PR/C;
 VLP=21(1980)1387;
 RCTS=12C(16O,16O)12C;
 PHQS=(EXC-FUNCT, ANGL-DSTRN);
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 /* Experimental Conditions                                           */
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 \\EXP,13;
 /* 2004-04-13 : Compiled, Ic + On */
 RTY=INEL-SCATT;
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.029MG/CM**2'2';
 /* '2' Measured by the energy-loss method with an 241Am alpha
        source. */
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT'3';
 /* '3' 12 UD Pelletron */
 INST-ACC=2JPNTSU;
 CHRG-INC-ION=(5+, 6+, 7+);
 POL-PRJ=0%;
 DET-PARTCL=12C;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'4',SI'5');
 /* '4' ESP-90 magnetic spectrograph [J.E. Spencer et al., Nucl.
        Instrum. Methods 49(1976)181]. */
 /* '5' Two 47 mm Si position-sensitive detectors */
 SOLID-ANGL=0.94MSR'6';
 /* '6' Corresponding to Delta-theta (lab) = +-0.72 deg or
        Delta-theta(c.m.) = +-1.5 deg */
 ERS-DET=[70KEV;
 ANL=STATIST-MODEL'7';
 /* '7' Hauser-Feshbach theory */
 /* 2006-10-02 : Altered, Mt. Re-digitized */
 RCT=12C(16O,16O)12C;
 PHQ=ANGL-DSTRN;
 INC-ENGY-CM=24.3MEV;
 ANL=SMTRX-THEORY;
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 /* Descriptive Parameters                                            */
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 \\DATA,13;
 TOT-ERR=20%'8';
 /* '8' Including uncertainties of the charge collection, target
        thickness, and detection efficiency */
 INC-ENGY-CM=24.3MEV;
 EXC-ENGY=6.131MEV;
 J-PTY=3-;
 EXC-ENGY-EMT=0.0MEV;
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 /* Data Table                                                        */
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 \DATA;
 THTC DSIGMA/DOMEGA
 (DEG) (MB/SR)
 1.313E+01 1.373E+00
 1.443E+01 1.267E+00
 1.548E+01 1.356E+00
 1.658E+01 1.470E+00
 1.754E+01 1.602E+00
 1.911E+01 1.892E+00
 1.959E+01 2.013E+00
 2.146E+01 2.067E+00
 2.214E+01 1.825E+00
 2.334E+01 1.636E+00
 2.522E+01 1.479E+00
 2.657E+01 1.306E+00
 2.888E+01 1.162E+00
 2.989E+01 9.667E-01
 3.047E+01 1.003E+00
 3.129E+01 8.852E-01
 3.359E+01 9.182E-01
 3.546E+01 9.524E-01
 \END;
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