DARPE: Search Results
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 /* NRDF D1883 Data No.11                                             */
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 /* Bibliography                                                      */
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 \\BIB,11;
 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,11;
 /* 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=28.2MEV;
 ANL=SMTRX-THEORY;
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 /* Descriptive Parameters                                            */
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 \\DATA,11;
 TOT-ERR=20%'8';
 /* '8' Including uncertainties of the charge collection, target
        thickness, and detection efficiency */
 INC-ENGY-CM=28.2MEV;
 EXC-ENGY=6.049MEV;
 J-PTY=0+;
 EXC-ENGY-EMT=0.0MEV;
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 /* Data Table                                                        */
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 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 1.292E+01 5.397E-01 +3.646E-02-3.646E-02
 1.304E+01 4.967E-01 +3.419E-02-3.419E-02
 1.359E+01 6.083E-01 +2.047E-02-2.047E-02
 1.464E+01 6.570E-01 +4.857E-02-4.857E-02
 1.470E+01 6.033E-01 +3.556E-02-3.556E-02
 1.560E+01 4.162E-01 +3.333E-02-3.333E-02
 1.620E+01 3.389E-01 +3.240E-02-3.045E-02
 1.685E+01 2.178E-01 +1.957E-02-1.957E-02
 1.808E+01 1.679E-01 +1.668E-02-1.668E-02
 1.891E+01 1.416E-01 +1.985E-02-1.382E-02
 2.052E+01 1.443E-01 +1.345E-02-1.345E-02
 2.132E+01 1.633E-01 +1.408E-02-1.210E-02
 2.232E+01 2.306E-01 +1.989E-02-2.251E-02
 2.307E+01 3.220E-01 +3.178E-02-3.635E-02
 2.503E+01 3.516E-01 +2.328E-02-2.328E-02
 2.709E+01 3.360E-01 +3.848E-02-2.756E-02
 2.914E+01 1.779E-01 +2.150E-02-2.150E-02
 3.167E+01 1.640E-01 +1.679E-02-1.679E-02
 \END;
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