/*===================================================================*/ /* NRDF D1725 Data No.7 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,7; 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,7; /* 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=58NI(6LI,ALPHA)X; RTY=X'27'; /* '27' inclusive breakup */ PHQ=DATA'28'; /* '28' Double differential cross section against logitudinal momentum of alpha. */ THK-TGT=(4.00MG/CM**2,5.86MG/CM**2); DET-PARTCL=ALPHA; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,7; INC-ENGY-LAB=100MEV/A; THTL=5.5DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; MOM-LNGTD'29' DATA1'30' DELTA-DATA1'30' (MEV/C) (UNIT2) (UNIT2) -8.141E+02 6.967E-03 +-NEGLIGIBLE -7.687E+02 1.066E-02 +-NEGLIGIBLE -7.295E+02 1.311E-02 +-NEGLIGIBLE -6.871E+02 1.680E-02 +-NEGLIGIBLE -6.433E+02 1.721E-02 +-NEGLIGIBLE -5.978E+02 1.516E-02 +-NEGLIGIBLE -5.492E+02 1.516E-02 +-NEGLIGIBLE -5.006E+02 1.803E-02 +-NEGLIGIBLE -4.505E+02 2.049E-02 +-NEGLIGIBLE -3.940E+02 2.500E-02 +-2.869E-03 -3.392E+02 3.156E-02 +-3.279E-03 -2.796E+02 4.426E-02 +-4.508E-03 -2.185E+02 6.230E-02 +-6.557E-03 -1.558E+02 9.303E-02 +-9.426E-03 -8.997E+01 1.549E-01 +-1.557E-02 -2.100E+01 2.311E-01 +-2.336E-02 4.796E+01 1.770E-01 +-1.803E-02 1.185E+02 5.615E-02 +-5.738E-03 1.937E+02 1.434E-02 +-NEGLIGIBLE 2.721E+02 2.049E-03 +-NEGLIGIBLE \END; /*===================================================================*/ |