DARPE: Search Results
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 /* NRDF D1902 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1902;
 TITLE=/ One- and two-proton removal from 15O /;
 ATH=(H.JEPPESEN'1,2', R.KANUNGO'1', B.ABU-IBRAHIM'3', S.ADHIKARI'4,5',
      M.CHIBA'1', D.FANG'1', N.IWASA'6', K.KIMURA'7', K.MAEDA'6',
      S.NISHIMURA'1', T.OHNISHI'1', A.OZAWA'1', C.SAMANTA'4,5',
      T.SUDA'1', T.SUZUKI'8', I.TANIHATA'1', Q.WANG'9', C.WU'1',
      Y.YAMAGUCHI'8', K.YAMADA'1', A.YOSHIDA'1', T.ZHENG'1,9');
 INST-ATH=(2JPNIPC'1', 2DENAAU'2', 3EGYEGY'3', 1USAUSA'4', 3INDSAH'5',
           2JPNTOH'6', 2JPNNIA'7', 2JPNNII'8', 3CPRBJG'9');
      /* '2' Department of Physics and Astronomy */
      /* '3' Department of Physics, Cairo University */
      /* '4' Physics Department, Virginia Commonwealth University */
      /* '6' Department of Physics */
      /* '7' Department of Electric, Electronics and Computer
            Engineering */
      /* '8' Department of Physics */
      /* '9' Department of Technical Physics */
 REF=NP/A;
 VLP=739(2004)57;
 RCTS=(9BE(15O,14N)X, 9BE(15O,13C)X);
 PHQS=(MOM-DSTRN, XSECTN'10', XSECTN'11');
 /* '10' one-proton removal cross section */
 /* '11' two-proton removal cross section */
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 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2004-11-27 : Compiled, Kc + Am + On */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'12';
 /* '12' A 0.5 mm thick target */
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'13',PRJFS'14');
 /* '13' 15O secondary beam was produced by the fragmentation of
        a 20Ne primary beam incident on a 0.5 mm Be production target.
 /* '14' RIKEN projectile fragment separator (RIPS) */
 INST-ACC=(2JPNIPC'13',2JPNIPC'14');
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(PPAC,SCT'15',IC'16',NAI'17',TOF'18');
 /* '15' To measure ToF for momentum distribution and fragment
         identification */
 /* '16' To measure energy loss for charge identification */
 /* '17' To measure total energy for mass identification */
 /* '18' To measure momentum distribution and fragment
         identification using newly developed TOF technique [R.Kanungo,
         et al., Phys. Rev. Lett. 88(2002)142502] */
 /* Experimental Method:
    - Time-of-flight (To measure momentum distribution and fragment
      identification using newly developed TOF technique [R.Kanungo, et
      al., Phys. Rev. Lett. 88(2002)142502])
 RCT=9BE(15O,13C)X;
 PHQ=MOM-DSTRN;
 INC-ENGY-LAB=56MEV/A;
 DET-PARTCL=13C;
 ANL=(GLAUBER'22',GLAUBER'23');
 /* '22' Simultaneous emission: 1-proton removal momentum
         distribution for 13C+p is obtained as first step, then which
         is folded by itself to generate momentum distribution for
         13C+p+p case. */
 /* '23' Sequential decay: Proton emission with 14N resonance at
         8.618 MeV or 8.980 MeV and from their decay is considered. */
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 INC-ENGY-LAB=56MEV/A;
 DATA1=253MEV/C'24';
 /* '24' Width (FWHM) of a single Gaussian distribution fit.
         Two-proton removal momentum distribution if connected by a
         smooth line including the asymmetric tail has a width of 285
         +65-10 MeV/c. */
 DELTA-DATA1=17MEV/C;
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 /* Data Table                                                        */
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 \DATA;
 MOM-LNGTD'25' COUNTS DELTA-COUNTS
 (MEV/C) (ARB) (ARB)
 -487.5 3 +-1.73
 -437.5 10 +-3.16
 -387.5 22 +-4.69
 -337.5 27 +-5.19
 -287.5 38 +-6.16
 -237.5 65 +-8.06
 -187.5 92 +-9.59
 -137.5 126 +-11.22
 -87.5 126 +-11.22
 -37.5 171 +-13.07
 12.5 172 +-13.13
 62.5 186 +-13.63
 112.5 118 +-10.86
 162.5 56 +-7.48
 212.5 29 +-5.38
 262.5 5 +-2.23
 \END;
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