/*===================================================================*/
 /* NRDF D1797 Data No.2                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1797;
 TITLE=/Isobaric analog state of 14Be/;
 PURPOSE=/To measure the Isobaric Analog State (IAS) of the
          neutron-dripline nucleus 14Be for the first time in a
          charge-exchange reactino 14Be(p,n)14B* in inverse kinematics
          at E(14Be) = 74 AMeV./;
 ATH=(S.TAKEUCHI'1', S.SHIMOURA'2', T.MOTOBAYASHI'1', H.AKIYOSHI'3',
      Y.ANDO'1', N.AOI'4', ZS.FULOP'5', T.GOMI'1', Y.HIGURASHI'1',
      M.HIRAI'6', N.IWASA'7', H.IWASAKI'2', Y.IWATA'6',
      H.KOBAYASHI'1', M.KUROKAWA'2', Z.LIU'8', T.MINEMURA'3',
      S.OZAWA'3', H.SAKURAI'4', M.SERATA'1', T.TERANISHI'2',
      K.YAMADA'1', Y.YANAGISAWA'3', M.ISHIHARA'3');
 INST-ATH=(2JPNYOK'1', 2JPNTOK'2', 2JPNIPC'3', 2JPNTOK'4', 3HUNDEB'5',
           2JPNIRS'6', 2JPNTOH'7', 3CPRIMP'8');
      /* '1' Department of Physics */
      /* '2' Center for Nuclear Study (CNS) */
      /* '4' Department of Physics */
      /* '7' Department of Physics */
 REF=PL/B;
 VLP=515(2001)255;
 RCTS=(P(14BE,14B)N, D(14BE,14B)X);
 PHQS=(ENGY-SPEC, ANGL-DSTRN, X'9', X'10', COULOMB-DISP-ENGY'11');
 /* '9' Energy and width of the peak of the decay energy spectra of
    the 12Be + p + n channel for the (p,n) reaction */
 /* '10' Excitation energy of the IAS */
 /* '11' Coulomb displacement energy for the pair of 14Be and its
    IAS. */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2003-07-09 : Compiled */
 ENR=X%;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'12',PRJFS'13');
 /* '12' Primary beam of 100 AMeV 18O on a 1110 mg/cm**2 thic 9Be
        target */
 /* '13' Secondary beam of 14Be selected by the RIKEN Projectile
        Fragment Separator (RIPS) [T.Kubo et al., Nucl. Instrum. Methods
        B70(1992)309]. */
 INST-ACC=(2JPNIPC'12',2JPNIPC'13');
 INC-ENGY-LAB=74MEV/A;
 ERS-PRJ=8MEV/A;
 BEAM-INTNSTY=1e4PPS'14';
 /* '14' Typical intensity of the 14Be beam with a purity of
         around 80% */
 POL-PRJ=0%;
 DET-PARTCL=(P,N,12BE);
 COINC=(P,N,12BE);
 ANT-COINC=NO;
 DET-SYS=(PLST-SCT'15',TOF'16');
 /* '15' To detect decay particles from 14B*. Resolutions of TOF
         were about 1.2% (FWHM) for charged particles and about
         1.5%(FWHM) for neutrons at the energies of 74 AMeV. */
 /* '16' To determine velocities of the decay particles */
 ERS-DET=0.15MEV'17';
 /* '17' Resolution of decay energy at 0.3 MeV */
 /* Experimental Method:
    - Time-of-flight (To determine velocities of the decay particles)
 /* Analysis:
    - Invariant mass method
 RCT=D(14BE,14B)X;
 PHQ=ENGY-SPEC;
 CHM=CD2'26';
 /* '26' (CD2)n and C target are used, C target was used to
         subtract the contributions ofcarbon nuclei in the (CD2)n
         target. */
 THK-TGT=XMG/CM**2'27';
 /* '27' 204 and 152 mg/cm2 for (CD2)n and C target, respectively.
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=74MEV/A;
 SYS-ERR=10%'28';
 /* '28' Uncertainties in neutron detection efficiency and the
         reaction losses of the charged particles in hodoscope. */
 EMT-1=12BE;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 ENGY-EMT'29' DATA1'30' DATA2'31' DELTA-DATA2'31,32' FLAG'33'
 (MEV) (MEV) (MB/MEV) (MB/MEV) (NODIM)
 16.770 0.000  0.000 +-X         1
 16.845 0.075 -0.023 +-0.023     2
 16.900 0.130  0.000 +-X         1
 16.945 0.175  0.035 +-0.047     X
 16.995 0.225  0.100 +-0.072     X
 17.045 0.275  0.077 +-0.086     X
 17.095 0.325  0.013 +-0.080     X
 17.170 0.400  0.114 +-0.059     X
 17.270 0.500  0.090 +-0.040     X
 17.370 0.600  0.047 +-0.037     X
 17.495 0.725  0.033 +-0.043     X
 17.645 0.875  0.014 +-0.033     X
 17.820 1.050  0.017 +-0.028     X
 18.020 1.250  0.056 +-0.034     X
 18.220 1.450  0.025 +-0.030     X
 18.445 1.675  0.039 +-0.041     X
 18.695 1.925  0.076 +-0.049     X
 18.970 2.200  0.090 +-0.039     X
 19.270 2.500  0.057 +-0.038     X
 19.595 2.825  0.026 +-0.026     X
 \END;
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