DARPE: Search Results
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 /* NRDF D1895 Data No.7                                              */
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 /* Bibliography                                                      */
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 \\BIB,7;
 D#=D1895;
 TITLE=/ Subbarrier fusion in the systems 11,10Be+209Bi /;
 PURPOSE=/ To observe fusion cross sections of Halo nuclei beam and Bi
          target /;
 ATH=(C.SIGNORINI'1', A.YOSHIDA'2', Y.WATANABE'2', D.PIERROUTSAKOU'3',
      L.STROE'4', T.FUKUDA'5', M.MAZZOCCO'1', N.FUKUDA'2,6', Y.MIZOI'2',
      M.ISHIHARA'2,6', H.SAKURAI'6', A.DIAZ-TORRES'7', K.HAGINO'8');
 INST-ATH=(2ITYITY'1', 2JPNIPC'2', 2ITYNAP'3', 2ITYPAD'4', 2JPNKEK'5',
           2JPNTOK'6', 2GERFRK'7', 2JPNKTO'8');
      /* '1' Physics Department and INFN, Padova */
      /* '6' Physics Department */
      /* '7' Institut fuer Theoretische Physik */
      /* '8' Yukawa Institute for Theoretical Physics */
 REF=NP/A;
 VLP=735(2004)329;
 RCTS=(209BI(11BE,5*N)215FR, 209BI(11BE,4*N)216FR, 209BI(11BE,FISSN),
       209BI(10BE,4*N)215FR, 209BI(10BE,3*N)216FR, 209BI(10BE,FISSN),
       209BI(11BE,FUSN), 209BI(10BE,FUSN));
 PHQS=XSECTN;
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 /* Experimental Conditions                                           */
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 \\EXP,7;
 /* 2004-05-12 : Compiled, Ic + On */
 /* Related references 
    - C.Signorini et al., EPJ/A, 5(1999)7.
    (9Be+209Bi data given in this reference are compared with present
    11, 10Be+209Bi data.)
 PHQ=XSECTN;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.7[0.8MG/CM**2;
 BAC=MYLAR;
 THK-BAC=XMG/CM**2'9';
 /* '9' 0.07 micro-gram/cm**2 or 0.9 micro-meter thick */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(CYC'10',PRJFS'11');
 /* '10' Around 65 AMeV 13C beam with about 100 pnA or 450 pnA
        intensity onto a 12 mm thick beryllium target to produce
        fragmentation of Be nuclei as secondary beam */
 /* '11' RIPS fragment separator [T.Kubo et al., Nucl. Instrum.
        Meth. B70(1992)309]. */
 INST-ACC=(2JPNIPC'10',2JPNIPC'11');
 INC-ENGY-CM=30[55MEV'12';
 /* '12' Energy of secondary beam measured by time-of-flight
        method using plastic scintillator */
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=SI'13';
 /* '13' To detect fission fragments and alpha particles emitted
         from the ground states of evaporation residues */
 RCT=209BI(11BE,FUSN);
 RTY=FUSN;
 ANL=CC'44';
 /* '44' CDCC [N. Austern et al., Phys. Rep. 154(1987)125] and
         CCFUL [H. Hagino et al., Comput. Phys. Commun. 123(1999)143]
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 /* Descriptive Parameters                                            */
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 \\DATA,7;
 TOT-ERR=[30%'45';
 /* '45' Absolute uncertainty evaluated from the comparison of the
         cross sections for the 3n evaporation channel leading to 215Fr
         in the system 9Be+209Bi measured in [C. Signorini et al., Eur.
         Phys. J. A5(1999)7] and in a calibration run during this
         experiment */
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM XSECTN'46' DELTA-XSECTN'46,47'
 (MEV) (MB) (MB)
 35.9 10.8 +-7.6
 37.6 56 +-13.5
 38 65.7 +-34.8
 39.2 106.5 +-16.4
 40 149.2 +-45.7
 40.9 221 +-23.8
 42 356.8 +-62.896
 42.6 287.9 +-27.3
 44 340 +-53.984
 44.3 429.3 +-31.5
 46 676.1 +-66.537
 46.01 547.6 +-34.3
 47.7 675.5 +-37.9
 48 898.7 +-73.544
 49.4 752.7 +-39.2
 50 1047.1 +-76.413
 51.1 680.7 +-39.8
 52 1060.9 +-78.182
 52.9 850.2 +-45.8
 54 1436.4 +-136.9
 54.7 788.9 +-45.5
 \END;
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