/*===================================================================*/
 /* NRDF D1895 Data No.8                                              */
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 /* Bibliography                                                      */
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 \\BIB,8;
 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;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,8;
 /* 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(10BE,FUSN);
 RTY=FUSN;
 ANL=CC'48';
 /* '48' CDCC [N. Austern et al., Phys. Rep. 154(1987)125] and
         CCFUL [H. Hagino et al., Comput. Phys. Commun. 123(1999)143]
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 TOT-ERR=[30%'49';
 /* '49' 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 */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM XSECTN'50' DELTA-XSECTN'50,51'
 (MEV) (MB) (MB)
 34.4 4.8 +-4.8
 36.1 12.2 +-7
 37.7 95.4 +-15.036
 38 39.9 +-29.1
 39.4 107 +-14.825
 40 126.4 +-37.1
 41 240.6 +-34.969
 42 204.57 +-35.183
 42.7 426.7 +-34.32
 44 464.7 +-32.844
 44.4 518.1 +-29.657
 46 612.2 +-23.956
 46.2 544.7 +-32.936
 47.9 679.8 +-32.737
 48 920 +-32.676
 49.6 660.1 +-32.51
 50 895.3 +-33.147
 51.3 706.9 +-38.618
 52 936.7 +-42.854
 53 556.7 +-36.344
 54 734 +-51.565
 54.7 460.1 +-36.592
 \END;
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