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 /* NRDF D1831 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D1831;
 TITLE=/Detailed analysis of the resonant backscattering spectrum for
        deeply penetrating protons in carbon/;
 PURPOSE=/To study the spectral response in Rutherford backscattering
          spectroscopy for deeply penetrating ions in matter/;
 ATH=(M.TOSAKI'1', S.ITO'1', N.MAEDA'2');
 INST-ATH=(2JPNKTO'1', 2JPNJPN'2');
      /* '1' Radioisotope Research Center */
      /* '2' Fukui College of Technology, Sabae, Fukui */
 REF=NIM/B;
 VLP=168(2000)543;
 RCTS=12C(P,P)12C;
 PHQS=EXC-FUNCT;
 /*===================================================================*/
 /* Experimental Conditions                                           */
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 \\EXP,1;
 /* 2003-12-18 : Compiled */
 RTY=ELA-SCATT;
 PHQ=EXC-FUNCT;
 /* Additional result not compiled:
    - Proton spectra (Energy spectra of proton for incident proton
      energy of 5.05, 5.5 and 6.0 MeV (Fig.4,5,6).)
 CHM=ELM;
 PHYS-FORM=SLD'3';
 /* '3' Carbon foil */
 THK-TGT=0.0227MG/CM**2'4';
 /* '4' Except 4.8 MeV proton for which 0.0083 mg/cm**2 thick
        carbon foil was used to avoid peak broadening due to energy
        loss in target */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNKTO'5';
 /* '5' Department of Physics */
 ERS-PRJ=+-2.5KEV'6';
 /* '6' at 6 MeV */
 POL-PRJ=0%;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=SI'7';
 /* '7' Passivated implanted planar silicon (PIPS) detector */
 SOLID-ANGL=1.83e-2MSR;
 ERS-DET=14.3KEV'8';
 /* '8' FWHM for protons in the energy range studied */
 RCT=12C(P,P)12C;
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 RSD=12C;
 THTL=179.2DEG;
 DELTA-THTL=0.2DEG;
 DELTA-DSIGMA/DOMEGA=10%'9';
 /* '9' Uncertainty due to thickness of target */
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB DSIGMA/DOMEGA
 (MEV) (B/SR)
  4.000  0.072
  4.100  0.066
  4.200  0.070
  4.300  0.082
  4.400  0.077
  4.500  0.094
  4.600  0.095
  4.650  0.089
  4.700  0.11
  4.760  0.14
  4.770  0.16
  4.780  0.22
  4.790  0.36
  4.795  0.69
  4.800  0.60
  4.805  0.20
  4.810  0.090
  4.830  0.086
  4.850  0.084
  4.900  0.092
  4.950  0.097
  5.000  0.11
  5.050  0.10
  5.100  0.13
  5.150  0.13
  5.200  0.15
  5.250  0.15
  5.300  0.15
  5.325  0.14
  5.350  0.093
  5.375  0.071
  5.400  0.059
  5.450  0.076
  5.500  0.087
  5.550  0.11
  5.600  0.11
  5.650  0.13
  5.700  0.12
  5.750  0.13
  5.800  0.14
  5.850  0.14
  5.875  0.14
  5.900  0.16
  5.925  0.17
  5.950  0.18
  5.975  0.18
  6.000  0.18
  6.050  0.19
  6.100  0.19
  6.150  0.19
  6.200  0.18
  6.300  0.20
  6.400  0.19
  6.500  0.18
  6.600  0.18
 \END;
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