/*===================================================================*/ /* NRDF D1895 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; 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,2; /* 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,4*N)216FR; DET-PARTCL=ALPHA'19'; /* '19' Alpha from 216Fr */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; RSD=216FR; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; INC-ENGY-CM XSECTN'20' DELTA-XSECTN'20,21' XSECTN'22' DELTA-XSECTN'22,23' (MEV) (MB) (MB) (MB) (MB) 37.6 42.5 +-11.1 X +-X 38 X +-X 65.7 +-34.8 39.2 90.5 +-14.3 X +-X 40 X +-X 149.2 +-45.7 40.9 172.5 +-20.2 X +-X 42 X +-X 328 +-61.6 42.6 223.5 +-24.1 X +-X 44 X +-X 276.6 +-50 44.3 282.3 +-27 X +-X 46 X +-X 492.4 +-60.8 46.01 261.7 +-24.7 X +-X 47.7 13.6 +-24.3 X +-X 48 X +-X 580.9 +-67.8 49.4 141.5 +-19.4 X +-X 50 X +-X 504.5 +-64.8 51.1 34.4 +-18 X +-X 52 X +-X 345.1 +-53.6 52.9 73.6 +-16.5 X +-X 54 X +-X 750.4 +-118.7 \END; /*===================================================================*/ |