/*===================================================================*/ /* NRDF D1725 Data No.9 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,9; D#=D1725; TITLE=/ Reaction mechanism of 6Li scattering at 600 MeV /; PURPOSE=/ To study the role of the breakup channels and its feedback to the elastic scattering at intermediate energy /; ATH=(K.SCHWARZ'1,2', C.SAMANTA'1,3', M.FUJIWARA'1,6', H.REBEL'2', R.DE.LEO'4', N.MATSUOKA'1', H.UTSUNOMIYA'5', H.AKIMUNE'6', I.DAITO'1', H.FUJIMURA'1', F.IHARA'1', K.ISHIBASHI'1', Y.MAEDA'1', T.YAMANAKA'1', H.YOSHIDA'1', A.OKIHANA'7', T.YOSHIMURA'7', P.K.J.VAN AARLE'1,8', W.A.T.UIJEN'1,8', M.ITO'9', Y.SAKURAGI'9'); INST-ATH=(2JPNRCN'1', 2GERKFK'2', 3INDSAH'3', 2ITYBAU'4', 2JPNKON'5', 2JPNJAE'6', 2JPNKUE'7', 2NEDENT'8', 2JPNJPN'9'); /* '4' Dipartimento di Fisica */ /* '6' Advanced Science Research Center */ /* '9' Department of Physcics, Osaka City University, Osaka */ REF=EPJ/A; VLP=7(2000)367; RCTS=(12C(6LI,6LI)X, 58NI(6LI,6LI)X, 90ZR(6LI,6LI)X, 208PB(6LI,6LI)X, 12C(6LI,ALPHA)X, 58NI(6LI,ALPHA)X, 90ZR(6LI,ALPHA)X, 208PB(6LI,ALPHA)X); PHQS=(ANGL-DSTRN, X'10', DATA'11', DATA'12'); /* '10' Transverse momentum distribution */ /* '11' Double differential cross section against logitudinal momentum of alpha. */ /* '12' squared of absolute value of momentum distribution */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,9; /* 2002-09-27 : Converted, Ay + On. Data converted to EXFOR E1725 ENR=X%; CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'13'; /* '13' Ring Cyclotron */ INST-ACC=2JPNRCN; INC-ENGY-LAB=100MEV/A; BEAM-INTNSTY=1NA; POL-PRJ=0%; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'14',MWDC,SCT'15',EDE); /* '14' Grand Gaiden [M.Fujiwara et al., Nucl.Instr.and Meth.in Phys.Res.A422(1999)484] */ /* '15' To measure energy loss Delta E and the residual energy E to particle identification */ /* Experimental Method: - Particle identification by 'E/Delta E' measurement /* 2006-08-08 : Altered, At. Re-digitized */ RCT=208PB(6LI,ALPHA)X; RTY=X'35'; /* '35' inclusive breakup */ PHQ=DATA'36'; /* '36' Double differential cross section against logitudinal momentum of alpha. */ THK-TGT=12.99MG/CM**2; DET-PARTCL=ALPHA; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,9; INC-ENGY-LAB=100MEV/A; THTL=5.5DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; MOM-LNGTD'37' DATA1'38' DELTA-DATA1'38' (MEV/C) (UNIT2) (UNIT2) -5.095E+02 5.764E-03 +-NEGLIGIBLE -4.500E+02 7.147E-03 +-NEGLIGIBLE -3.970E+02 8.069E-03 +-NEGLIGIBLE -3.427E+02 1.061E-02 +-NEGLIGIBLE -2.845E+02 1.476E-02 +-1.153E-03 -2.198E+02 2.398E-02 +-2.536E-03 -1.500E+02 3.919E-02 +-4.150E-03 -8.017E+01 8.138E-02 +-8.300E-03 -1.034E+01 1.326E-01 +-1.337E-02 5.819E+01 5.671E-02 +-5.764E-03 1.319E+02 1.268E-02 +-1.383E-03 2.095E+02 2.305E-03 +-NEGLIGIBLE \END; /*===================================================================*/ |