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 /* NRDF D1859 Data No.6                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,6;
 D#=D1859;
 TITLE=/ The angular distributions of the long-range alpha-particles
         from the reaction F19(p,alpha0)O16 /;
 PURPOSE=/ To report the experimental data on the long range
           alpha-particles, which will be used to ascertain the J-value
           and the other nuclear properties of the resonance levels. /;
 ATH=(A.ISOYA'1', H.OHMURA'1', T.MOMOTA'1');
 INST-ATH=(2JPNTOK'1');
      /* '1' Department of Physics, Faculty of Science */
 REF=NP;
 VLP=7(1958)116;
 RCTS=19F(P,ALPHA)16O;
 PHQS=(EXC-FUNCT, ANGL-DSTRN'2', ANGL-DSTRN);
 /* '2' Legendre coefficient */
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 /* Experimental Conditions                                           */
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 \\EXP,6;
 /* 2004-03-14 : Compiled, Kc + Km */
 ENR=NAT;
 CHM=X'3';
 /* '3' Calcium fluoride */
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'4';
 /* '4' About 8 keV at 840 keV */
 BAC=AL;
 THK-BAC=[0.05MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDG;
 INST-ACC=2JPNTOK;
 ERS-PRJ=0.2%;
 BEAM-INTNSTY=0.4[2UA;
 POL-PRJ=0%;
 DET-PARTCL=ALPHA;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(PROP-CNTR'5',PROP-CNTR'6');
 /* '5' Side-window type to count alpha-particles at various angle
        with angular resolution of 4-5 deg, which was considered to
        cause an error in the coefficients of the angular distribution
        not larger than 2%. */
 /* '6' End-window type to count long-range alpha-particles at 90
        deg. */
 ANL=LEGD;
 /* 2006-10-11 : Altered, Is. Re-digitized */
 RCT=19F(P,ALPHA)16O;
 PHQ=ANGL-DSTRN;
 INC-ENGY-LAB=831KEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,6;
 INC-ENGY-LAB=831KEV;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 COS-CM DSIGMA/DOMEGA
 (NODIM) (MB/SR)
 -9.598E-01 2.670E+00
 -8.649E-01 2.257E+00
 -7.601E-01 1.894E+00
 -6.427E-01 1.610E+00
 -4.954E-01 1.431E+00
 -3.481E-01 1.246E+00
 -1.759E-01 1.074E+00
 -3.613E-03 1.055E+00
 1.736E-01 1.080E+00
 3.468E-01 1.061E+00
 5.000E-01 1.284E+00
 6.405E-01 1.610E+00
 7.653E-01 2.042E+00
 8.652E-01 2.565E+00
 9.451E-01 3.009E+00
 9.925E-01 3.496E+00
 \END;
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