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 /* NRDF D1799 Data No.5                                              */
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 /* Bibliography                                                      */
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 \\BIB,5;
 D#=D1799;
 TITLE=/ Measurement of the 24Mg(p,t)22Mg reaction for the states
         near the 21Na+p threshold /;
 ATH=(S.MICHIMASA'1', S.KUBONO'1', S.H.PARK'2', T.TERANISHI'1',
      Y.YANAGISAWA'3', N.IMAI'4', ZS.FULOP'5', X.LIU'1', T.MINEMURA'3',
      C.C.YUN'1', J.M.D'AURIA'6', K.P.JACKSON'7');
 INST-ATH=(2JPNTOK'1', 3KORNSU'2', 2JPNIPC'3', 2JPNTOK'4', 3HUNDEB'5',
           1CANSFU'6', 1CANTMF'7');
      /* '1' Center for Nuclear Study(CNS) */
      /* '2' School of Physics */
      /* '4' Department of Physics */
      /* '6' Department of Chemistry */
 REF=(EPJ/A'8');
 VLP=(14(2002)275'8');
 /* Secondary reference 
    - NP/A, 718(2003)581 (S.Michimasa et al., Proc. of the 7th
      International Symposium on Nuclei in the Cosmos (NIC7))
 RCTS=24MG(P,T)22MG;
 PHQS=ANGL-DSTRN;
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 /* Experimental Conditions                                           */
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 \\EXP,5;
 /* 2004-03-22 : Compiled, St + Am */
 /* 2006-10-04 : Altered, On. Reference (NIC7) added */
 RTY=PKUP;
 PHQ=ANGL-DSTRN;
 ENR=99.9%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.358+-0.012MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'9';
 /* '9' CNS-SF cyclotron */
 INST-ACC=2JPNTOK'10';
 /* '10' Center for Nuclear Study */
 INC-ENGY-LAB=34.68MEV;
 BEAM-INTNSTY=[100NA'11';
 /* '11' The beam current on the target was monitored by a Faraday
         cup placed just after the target. */
 POL-PRJ=0%;
 DET-PARTCL=T;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'12',SWPC'13',SCT'14',TOF'15',EDE'16');
 /* '12' High-resolution magnetic spectrograph, PA [S. Kato et
         al., Nucl. Instrum. Methods 154, 19 (1978)] */
 /* '13' Hybrid-gas counter [M.H. Tanaka et al., Nucl. Instrum.
         Methods 195, 509 (1976)] */
 /* '14' Plastic scintillator */
 /* '15' Particle Identification */
 /* '16' Particle Identification */
 SOLID-ANGL=5.0MSR;
 ERS-DET=[37.5KEV'17';
 /* '17' FWHM for tritons */
 ANL=DWBA'18';
 /* '18' The analysis is made with the code TWOFNR [M. Igarashi,
         unpublished] for spin assignments. The optical potential
         parameters of the initial and final channels are taken from
         R.A.Paddock[Phys. Rev. C5, 485(1972)]. A Woods-Saxon form
         factor with r=1.2fm and a=0.65fm is used for the bound-state
         potential, where the depth was determined to reproduce the
         separation energy. */
 /* Experimental Method:
    - Time-of-flight (Particle Identification)
    - Particle identification by 'E/Delta E' measurement (Particle
      Identification)
 RCT=24MG(P,T)22MG;
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 /* Descriptive Parameters                                            */
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 \\DATA,5;
 INC-ENGY-LAB=34.68MEV;
 EXC-ENGY=5.7139MEV;
 DELTA-EXC-ENGY=0.0012MEV;
 J-PTY=2+;
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 /* Data Table                                                        */
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 \DATA;
 THTC DELTA-THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (DEG) (UB/SR) (UB/SR)
 14.95 +-0.04 7.14 +-1.66
 22.97 +-0.08 3.87 +-0.59
 38.86 +-0.18 3.41 +-0.35
 54.47 +-0.23 2.86 +-0.20
 62.13 +-0.21 1.78 +-0.12
 69.69 +-0.17 1.41 +-0.09
 \END;
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