DARPE: Search Results
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 /* NRDF D1803 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1803;
 TITLE=/Study of resonance states in 12N using a radioactive ion beam
        of 11C/;
 PURPOSE=/The authors report the first experimental result on the
          elastic resonance scattering of 11C+p using the RI beam of
          11C./;
 ATH=(T.TERANISHI'1', S.KUBONO'1', S.SHIMOURA'1', M.NOTANI'1',
      Y.YANAGISAWA'2', S.MICHIMASA'1', K.UE'1', H.IWASAKI'1',
      M.KUROKAWA'1', Y.SATOU'1', T.MORIKAWA'3', A.SAITO'4', H.BABA'4',
      J.H.LEE'5', C.S.LEE'5', ZS.FULOP'6', S.KATO'7');
 INST-ATH=(2JPNTOK'1', 2JPNIPC'2', 2JPNKYU'3', 2JPNYOK'4', 3KORKOR'5',
           3HUNDEB'6', 2JPNYMG'7');
      /* '1' Center for Nuclear Study (CNS) */
      /* '3' Department of Physics */
      /* '4' Department of Physics */
      /* '5' Department of Physics, Chun-Ang University, Seoul */
      /* '7' Department of Physics */
 REF=PL/B;
 VLP=556(2003)27;
 RCTS=1H(11C,11C)1H;
 PHQS=(EXC-FUNCT, PTY);
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2004-08-06 : Compiled */
 ENR=NAT;
 CHM=CH2'8';
 /* '8' Data with carbon target was also taken in a separate run to
        evaluate the background contribution from the reactions of 11C
        with C atoms in the (CH2)n target. */
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'9';
 /* '9' Thickness of (CH2)n target is 8.0 mg/cm2 and C target is
        10.7 mg/cm2 */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'10',PRJFS'11');
 /* '10' Isochronous cyclotron, Primary 10B beam with 7.8 MeV/A
 /* '11' To produce 11C secondary beam by the 3He(10B,12N*)n
        reaction, where the 11C particles were emitted from the unbound
        levels in 12N. */
 INST-ACC=(2JPNIPC'10',2JPNIPC'11');
 INC-ENGY-CM=0.3125[3.0375MEV'12';
 /* '12' Excitation function obtained by thick target method */
 BEAM-INTNSTY=17000PPS;
 POL-PRJ=0%;
 DET-PARTCL=P;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(PPAC'13',SI'14',TOF'15',EDE'16');
 /* '13' 2 parallel plate avalanche counters 1) to identify proton
         usign ToF information and 2) to determin scattering angle with
         a resolution of 0.6 deg (FWHM) */
 /* '14' To identify proton using E-Delta E infomation */
 /* '15' Particle identification, measured by 2 PPACs and Delta-E
         detector */
 /* '16' Particle identification */
 /* Experimental Method:
    - Time-of-flight (Particle identification, measured by 2 PPACs
      and Delta-E detector)
    - Particle identification by 'E/Delta E' measurement (Particle
      identification)
    - Thick-target method (11C beam particles were fully stopped in
      the (CH2)n target and energies of recoil protons, coming out from
      a thick target, are measured at a forward angle in the laboratory
      frame and the converted to the center-of-mass energies of
      scattering. Due to the thick target, a wide range of the
      excitation function for the elastic scattering can be measured
      with a beam of fixed energy. See S. Kubono, Nucl. Phys.
      A693(2001)221 for detail.)
 RCT=1H(11C,11C)1H;
 PHQ=PTY;
 /* Analysis:
    - Resonance formula based on [J.M. Blatt and L.C. Biedenharn,
      Rev. Mod. Phys. 24(1952)258]
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
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 /* Data Table                                                        */
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 \DATA;
 RESN-ENGY'21' EXC-ENGY'22' RESN-WDTH'23' SPIN'24' PTY
 (MEV) (MEV) (MEV) (NODIM) (NODIM)
 2.53  3.1   0.22   3   -1
 2.96  3.6   0.22   2   +1
 \END;
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