/*===================================================================*/ /* NRDF D1594 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; D#=D1594; TITLE=/ Elastic scattering of 3He particles at 450 MeV /; PURPOSE=/ To measure elastic scattering of 3He particles at an incident energy of 150 MeV/nucleon for several target nuclei in a wide mass region. /; ATH=(T.YAMAGATA'1', H.UTSUNOMIYA'1', M.TANAKA'2', S.NAKAYAMA'3', N.KOORI'3', A.TAMII'4', Y.FUJITA'5', K.KATORI'5', M.INOUE'6', M.FUJIWARA'7', H.OGATA'7'); INST-ATH=(2JPNKON'1', 2JPNKTJ'2', 2JPNTKS'3', 2JPNKTO'4', 2JPNOSA'5', 2JPNKTO'6', 2JPNRCN'7'); /* '1' Department of Physics */ /* '3' Department of Physics */ /* '4' Department of Physics */ /* '5' Department of Physics */ /* '6' Institute for Chemical Research */ REF=(NP/A'8'); VLP=(589(1995)425'8'); /* Secondary reference - PR/C, 50(1994)2606 (Brief report for 90Zr and 208Pb target) RCTS=(12C(3HE,3HE)12C, 28SI(3HE,3HE)28SI, 58NI(3HE,3HE)58NI, 90ZR(3HE,3HE)90ZR, 208PB(3HE,3HE)208PB); PHQS=(ANGL-DSTRN, OPT-POTL-PARA); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,4; /* 2005-09-09 : Converted, Sr + On. Converted to EXFOR E1594 */ /* 2005-09-26 : Altered, At + Ot + Sr. Re-digitized */ RTY=ELA-SCATT; CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'9'; /* '9' K = 400 MeV ring cyclotron */ INST-ACC=2JPNRCN; INC-ENGY-LAB=450MEV; BEAM-INTNSTY=1[30NA; POL-PRJ=0%; DET-PARTCL=3HE; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'10',MWDC'11',SCT'12',TOF); /* '10' Grand RAIDEN: To analyze 3He [M.Fujiwara, et al., Nucl. Instr. Meth. A, to be published]. */ /* '11' To detect 3He by two 2-dimensional position-sensitive multiwire-drift-chambers */ /* '12' To detect 3He by two plastic scintillators (delta E) [T.Noro, et al., RCNP annual report (1991) p.177, unpublished.] */ ERS-DET=400KEV'13'; /* '13' Mainly due to energy spread of incident beam */ ANL=OPT-MODEL'14'; /* '14' Analysis using the code 'ECIS' [Ref: J. Raynal, Code ECIS88, unpublished.] */ /* Experimental Method: - Time-of-flight RCT=90ZR(3HE,3HE)90ZR; PHQ=ANGL-DSTRN; ENR=>99%; THK-TGT=11.3MG/CM**2; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,4; INC-ENGY-LAB=450MEV; SYS-ERR=15%'27'; /* '27' Total systematic error. Uncertainty in absolute value, mainly due to the uncertainty in target thickness and the charge-collection efficiency of Faraday cup */ EMT=3HE; DELTA-THTL=0.05DEG; DATA1=0.3DEG'28'; /* '28' Overall angular resolution */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC RUTH-RATIO DELTA-RUTH-RATIO'29' (DEG) (NODIM) (NODIM) 4.214E+00 4.246E-02 +-NEGLIGIBLE 4.786E+00 1.265E-01 +-NEGLIGIBLE 5.357E+00 2.451E-01 +-NEGLIGIBLE 5.929E+00 2.973E-01 +-NEGLIGIBLE 6.477E+00 1.488E-01 +-NEGLIGIBLE 7.030E+00 5.090E-02 +-NEGLIGIBLE 7.592E+00 1.602E-02 +-NEGLIGIBLE 7.878E+00 3.847E-02 +-NEGLIGIBLE 8.384E+00 1.176E-01 +-NEGLIGIBLE 9.380E+00 9.589E-02 +-NEGLIGIBLE 1.006E+01 6.483E-02 +-NEGLIGIBLE 1.070E+01 2.164E-02 +-NEGLIGIBLE 1.130E+01 2.053E-02 +-NEGLIGIBLE 1.171E+01 2.682E-02 +-NEGLIGIBLE 1.264E+01 4.606E-02 +-NEGLIGIBLE 1.316E+01 2.594E-02 +-NEGLIGIBLE 1.379E+01 1.424E-02 +-NEGLIGIBLE 1.432E+01 8.935E-03 +-NEGLIGIBLE 1.490E+01 9.778E-03 +-NEGLIGIBLE 1.529E+01 1.259E-02 +-NEGLIGIBLE 1.579E+01 1.257E-02 +-NEGLIGIBLE 1.643E+01 1.072E-02 +-NEGLIGIBLE 1.686E+01 5.958E-03 +-NEGLIGIBLE 1.737E+01 3.729E-03 +-NEGLIGIBLE 1.788E+01 2.202E-03 +-NEGLIGIBLE 1.838E+01 2.484E-03 +-NEGLIGIBLE 1.895E+01 3.530E-03 +-NEGLIGIBLE 1.950E+01 2.807E-03 +-NEGLIGIBLE 2.000E+01 2.050E-03 +-NEGLIGIBLE 2.050E+01 1.683E-03 +-NEGLIGIBLE 2.100E+01 6.840E-04 +-NEGLIGIBLE 2.143E+01 5.841E-04 +-4.746E-05 2.214E+01 4.982E-04 +-4.048E-05 2.257E+01 4.973E-04 +-4.041E-05 2.314E+01 2.986E-04 +-5.060E-05 2.357E+01 3.769E-04 +-3.062E-05 2.414E+01 3.910E-04 +-6.599E-05 2.457E+01 2.747E-04 +-4.635E-05 2.529E+01 8.160E-05 +-2.566E-05 2.571E+01 7.835E-05 +-2.069E-05 2.629E+01 8.452E-05 +-4.039E-05 2.671E+01 1.348E-04 +-4.244E-05 2.729E+01 6.925E-05 +-2.178E-05 2.771E+01 9.826E-05 +-3.604E-05 2.836E+01 2.597E-05 +-1.890E-05 2.879E+01 2.696E-05 +-1.962E-05 \END; /*===================================================================*/ |