/*===================================================================*/ /* NRDF D1895 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; 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,3; /* 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,FISSN); RTY=FISSN; DET-PARTCL=X'24'; /* '24' Fission Fragments */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; INC-ENGY-CM XSECTN'25' DELTA-XSECTN'25,26' XSECTN'27' DELTA-XSECTN'27,28' (MEV) (MB) (MB) (MB) (MB) 35.9 10.8 +-7.6 X +-X 37.6 13.5 +-7.8 X +-X 39.2 16 +-8 X +-X 40.9 39.7 +-12 X +-X 42 X +-X 28.8 +-12.7 42.6 35.3 +-11.2 X +-X 44 X +-X 10.3 +-7.3 44.3 45.5 +-12.6 X +-X 46 X +-X 36.9 +-13.7 46.01 103.4 +-19.2 X +-X 47.7 150.7 +-23 X +-X 48 X +-X 19.7 +-11.2 49.4 193.6 +-26.8 X +-X 50 X +-X 108.7 +-31.7 51.1 185 +-26.7 X +-X 52 X +-X 226.5 +-52.9 52.9 294.3 +-35.2 X +-X 54 X +-X 149.1 +-49.7 54.7 337 +-38.2 X +-X \END; /*===================================================================*/ |