/*===================================================================*/ /* NRDF D1118 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; D#=D1118; TITLE=/ Analyzing power as a probe for clarifying nuclear reaction mechanisms: Study of the two-step unbound channel contribution ATH=(K.YAGI'1', Y.AOKI'1', K.HASHIMOTO'1', H.IIDA'1', H.SAKAMOTO'1', Y.TAGISHI'1', M.MATOBA'2', M.IGARASHI'3', K.-I.KUBO'4'); INST-ATH=(2JPNTSU'1', 2JPNKYU'2', 2JPNJPN'3', 2JPNTMU'4'); /* '1' Institute for Physics and Tandem Accelerator Center */ /* '2' Department of Energy Conversion Engineering */ /* '3' Tokyo Medical College, Tokyo */ /* '4' Department of Physics */ REF=PR/C; VLP=31(1985)676; RCTS=208PB(P,T)206PB; PHQS=(VCTR-ANALPW, ANGL-DSTRN); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,3; /* 2007-05-09 : Converted, N.Otuka. Converted to EXFOR E1118 */ ENR=99.1%; CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC; INST-ACC=2JPNRCN; DET-PARTCL=T; COINC=NO; ANT-COINC=NO; DET-SYS=MAG'5'; /* '5' To detect emitted tritons (RAIDEN) */ ANL=DWBA'6'; /* '6' Code TWOFNR/PTFF */ /* 2007-06-19 : Altered, At. Re-digitized */ RCT=208PB(P,T)206PB; PHQ=VCTR-ANALPW; THK-TGT=4.0MG/CM**2; INC-ENGY-LAB-RANGE=50.2MEV; BEAM-INTNSTY=80NA; POL-PRJ=83%; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; INC-ENGY-LAB=50.2MEV; EXC-ENGY=1.34MEV; J-PTY=3+; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTL AY DELTA-AY (DEG) (NODIM) (NODIM) 5.204E+00 1.728E-01 +-5.277E-02 9.975E+00 2.372E-01 +-5.279E-02 1.480E+01 6.268E-02 +-4.724E-02 2.041E+01 -1.645E-01 +-5.002E-02 2.532E+01 -1.640E-01 +-5.002E-02 3.049E+01 -1.413E-01 +-4.725E-02 3.551E+01 -1.018E-02 +-5.000E-02 \END; /*===================================================================*/ |