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 /* NRDF D1670 Data No.5                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,5;
 D#=D1670;
 TITLE=/ Isobalic analog state of 11Li /;
 ATH=(T.TERANISHI'1', S.SHIMOURA'2', Y.ANDO'2', M.HIRAI'3', N.IWASA'2',
      T.KIKUCHI'2', S.MORIYA'2', T.MOTOBAYASHI'2', H.MURAKAMI'2',
      T.NAKAMURA'3', T.NISHIO'2', H.SAKURAI'1', T.UCHIBORI'2',
      Y.WATANABE'1', Y.YANAGISAWA'2', M.ISHIHARA'1,3');
 INST-ATH=(2JPNIPC'1', 2JPNRIK'2', 2JPNTOK'3', 2GERGSI'4');
      /* '2' Department of Physics */
      /* '3' Department of Physics */
 REF=(PL/B'5');
 VLP=(407(1997)110'5');
 /* Secondary reference 
    - NP/A, 630(1998)387 (S.Shimoura et al., Proceedings of The Sixth
      International Conference on Nucleus-Nucleus Collisions
      (Gatlinburg, 1997))
 RCTS=(P(11LI,11BE)N, D(11LI,11BE)N);
 PHQS=(ENGY-SPEC, ENGY-SPEC'6', ANGL-DSTRN'7', X'8');
 /* '6' Fermi transition part */
 /* '7' Fermi transition part */
 /* '8' Excitation energy and width of IAS of 11Li. This is obtained
    by fitting Fermi part of energy spectrum (Fig.2c) with Gaussian
    function over the region of 0.4 MeV < Ed < 1.6 MeV. Effects of the
    detector acceptance and the Ed resolution were taken into account
    in the fitting procedure. */
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 /* Experimental Conditions                                           */
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 \\EXP,5;
 /* 2003-08-18 : Converted, Data converted to EXFOR E1670 */
 ENR=X%;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=PRJFS'9';
 /* '9' A primary 18O beam of 100 AMeV bombarded a 9Be target of
        1.4 g/cm2 thickness. Reaction products were analyzed by the
        projectile fragment separator RIPS [T.Kubo et al., Nucl. Instr.
        Meth. B70(1992)309] to obtain a radioactive 11Li beam. */
 INST-ACC=2JPNIPC;
 INC-ENGY-LAB=64MEV/A'10';
 /* '10' at the middle of the target */
 ERS-PRJ=6%;
 BEAM-INTNSTY=20000PPS;
 POL-PRJ=0%;
 DET-PARTCL=(N,P,9LI);
 COINC=(P,N,9LI);
 ANT-COINC=NO;
 DET-SYS=(SCT'11',TOF'12');
 /* '11' To detect decay particles from 11Be. The hodoscope
         consisted of a 5-mm thick Delta E plane and two 60-mm thick E
         planes. */
 /* '12' To determine velocities of charged particles and neutrons
         over the 3.1 m flight path between the target and the
         hodoscope. */
 /* Experimental Method:
    - Time-of-flight (To determine velocities of charged particles
      and neutrons over the 3.1 m flight path between the target and
      the hodoscope.)
 /* Analysis:
    - Invariant mass method
 /* In the reference data given are not corrected for acceptance. In
    this work, 11Be*(IAS) decays in two ways: 11Be*(IAS) -> 9Li+p+n
    (direct decay) and 11Be*(IAS) -> 10Li+p ->9Li+p+n (Sequential
    decay). The author assumed direct decay in the evaluation of
    acceptance. To avoid ambiguity due to this assumption, authors gave
    raw data (not corrected by acceptance) in the reference. */
 /* none */
 /* none */
 RCT=P(11LI,11BE)N;
 PHQ=X'45';
 /* '45' Excitation energy and width of IAS of 11Li. This is
         obtained by fitting Fermi part of energy spectrum (Fig.2c)
         with Gaussian function over the region of 0.4 MeV < Ed < 1.6
         MeV. Effects of the detector acceptance and the Ed resolution
         were taken into account in the fitting procedure. */
 CHM=CH2'46';
 /* '46' (CH2)n and C target are used, C target was used to
         subtract the contributions of carbon nuclei in the (CH2)n
         target. */
 THK-TGT=XMG/CM**2'47';
 /* '47' 191 and 188 mg/cm2 for (CH2)n and C target, respectively.
 /* Analysis:
    - a Gaussian fit
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 /* Descriptive Parameters                                            */
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 \\DATA,5;
 INC-ENGY-LAB=64MEV/A;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY DELTA-EXC-ENGY WDTH DELTA-WDTH
 (MEV) (MEV) (MEV) (MEV)
 1.02 +-0.02 0.49 +-0.07
 \END;
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