/*===================================================================*/ /* NRDF D1658 Data No.9 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,9; D#=D1658; TITLE=/ Fusion and breakup at the barrier with 11Be /; PURPOSE=/ To measure the fusion cross-sections with unstable beams ATH=(A.YOSHIDA'1', C.SIGNORINI'2', T.FUKUDA'3', Y.WATANABE'1', N.AOI'4', M.HIRAI'4', M.ISHIHARA'1,4', H.KOBINATA'4', Y.MIZOI'3', L.MUELLER'2', Y.NAGASHIMA'5', J.NAKANO'3', T.NOMURA'3', Y.H.PU'1', F.SCARLASSARA'2'); INST-ATH=(2JPNIPC'1', 2ITYPAD'2', 2JPNINS'3', 2JPNTOK'4', 2JPNTSU'5'); /* '2' Physics Department of the University and INFN */ /* '4' Department of Physics */ /* '5' College of Medical Technology */ REF=PL/B; VLP=389(1996)457; RCTS=(209BI(11BE,4*N)216FR, 209BI(11BE,5*N)215FR, 209BI(10BE,3*N)216FR, 209BI(10BE,4*N)215FR, 209BI(9BE,3*N)215FR, 209BI(9BE,4*N)214FR, 209BI(9BE,5*N)213FR, 209BI(9BE,FISSN)); PHQS=XSECTN; /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,9; /* 2003-08-15 : Converted, Am + N.Otuka. Data converted to EXFOR E1658 */ PHQ=XSECTN; ENR=X%; CHM=ELM; PHYS-FORM=SLD; POL-TGT=0%; ALGN-TGT=0%; POL-PRJ=0%; COINC=NO; ANT-COINC=NO; ANL=STATIST-MODEL'6'; /* '6' Evaporation code CASCADE [E.Pulhofer, Nucl. Phys. A280(1977)267]. */ /* 2006-11-13 : Altered, Mh. Re-digitized */ RCT=209BI(9BE,FISSN); RTY=FISSN; THK-TGT=0.370MG/CM**2; BAC=X'62'; /* '62' Kapton foil, in order to stop all of the recoil evaporation residues produced by the reaction. */ THK-BAC=2.0MG/CM**2; ACC=VDGT'63'; /* '63' 12UD Tandem */ INST-ACC=2JPNTSU'64'; /* '64' Tandem Accelerator Center */ INC-ENGY-CM-RANGE=35[70MEV; DET-SYS=SI'65'; /* '65' to measure alpha-particles, 150 mm2 silicon detector located 135 deg to the beam direction and 11 cm from the target */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,9; TOT-ERR=<5%; NORM=/ Absolute cross-section normalization was deduced by the known Rutherford cross section and the ratio between the solid angles of the two detectors, measured with a point alpha-source positioned at the target site. /; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; INC-ENGY-CM XSECTN (MEV) (MB) 4.125E+01 8.038E+00 4.316E+01 1.806E+01 4.602E+01 3.557E+01 4.919E+01 7.084E+01 5.371E+01 1.577E+02 \END; /*===================================================================*/ |