/*===================================================================*/
 /* NRDF D1872 Data No.8                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 D#=D1872;
 TITLE=/ (d,alpha) reactions on 19F, 20Ne, 31P and 32S at 14.7 MeV /;
 ATH=(K.TAKAMATSU'1');
 INST-ATH=(2JPNKTO'1');
      /* '1' Department of Physics, Faculty of Science */
 REF=JPJ;
 VLP=17(1962)896;
 RCTS=(19F(D,ALPHA)17O, 31P(D,ALPHA)29SI, 20NE(D,ALPHA)18F,
       32S(D,ALPHA)30P, 24MG(D,ALPHA)22NA);
 PHQS=(ANGL-DSTRN, XSECTN);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,8;
 /* 2004-02-20 : Compiled, Ic + On */
 /* Related references 
    - K.Kimura et al., JPJ, 17(1962)9.
    (Details of beam handling and scattering chamber)
    - T.Yanabu et al., JPJ, 17(1962)914.
    (Details of detecting system)
    - M.el Nadi, PR, 119(1960)242.
    (Two-nucleon picjup process formula used in analysis)
    - H.C.Newns, PPS, 76(1960)489.
    (Two-nucleon picjup process formula used in analysis)
 /* Additional results shown but not compiled
    - Energy distribution (Typical pulse-height spectrum (channel
      number v.s. counts/channel) of alpha particlles are shown for
      19F, 20Ne, 31P and 32S target.)
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNKTO;
 POL-PRJ=0%;
 DET-PARTCL=ALPHA;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SI'2',CSI'3');
 /* '2' To detect alpha. Energy calibration was done with the alpha
        particles produced in the known reactions such as
        27Al(p,alpha)24Mg, 16O(d,alpha)14N and 27Al(d,alpha)25Mg etc.
 /* '3' CSI(Tl) scintillation counter to monitor the beam current
        of incident deuterons */
 ERS-DET=1.2%'4';
 /* '4' Value at 20 MeV */
 /* Experimental Method:
    - Beam current integrated (Conventional current integrator with
      an accuracy better than 10%)
 /* 2006-10-05 : Altered, Is. Re-digitized */
 RCT=20NE(D,ALPHA)18F;
 PHQ=ANGL-DSTRN;
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=GAS;
 THK-TGT=XMG/CM**2'28';
 /* '28' about 30 cmHg */
 INC-ENGY-LAB=14.5MEV;
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 /* Descriptive Parameters                                            */
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 \\DATA,8;
 INC-ENGY-LAB=14.5MEV;
 SYS-ERR=(<20%'29',<20%'30');
 /* '29' Maximum uncertainty of absolute values arise from
         spectrum analysis */
 /* '30' Maximum uncertainty of absolute values arise from beam
         current estimation */
 DELTA-THTL=+-3DEG;
 DATA1=1'31';
 /* '31' First to fourth excited states could not be resolved in
         author's detecting system. */
 DATA2=2;
 DATA3=3;
 DATA4=4;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA
 (DEG) (MB/SR)
 2.383E+01 2.428E+00
 3.447E+01 1.488E+00
 4.581E+01 1.147E+00
 5.599E+01 1.050E+00
 6.735E+01 5.173E-01
 7.712E+01 6.841E-01
 8.803E+01 7.371E-01
 9.293E+01 7.453E-01
 9.782E+01 7.697E-01
 1.087E+02 9.284E-01
 1.174E+02 9.814E-01
 1.268E+02 9.775E-01
 1.358E+02 1.404E+00
 1.463E+02 1.559E+00
 1.538E+02 1.405E+00
 1.628E+02 1.698E+00
 1.673E+02 2.076E+00
 \END;
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