/*===================================================================*/ /* NRDF D1060 Data No.25 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,25; D#=D1677; TITLE=/A NEW APPROACH TO A 'MODEL-INDEPENDENT' OPTICAL POTENTIAL AND ITS APPLICATION TO PROTON ELASTIC SCATTERING NEAR THE (P,N) THRESHOLD ENERGY REGION/; PURPOSE=/A NEW APPROACH TO A "MODEL INDEPENDENT" OPTICAL POTENTIAL IS PROPOSED, WHICH FEATURES THE ADAPTIVE IMPROVEMENT OF EXPANSION BASE AND PRACTICAL ESTIMATION OF THE ERRORS OF TEH DERIVED POTENTIAL/; ATH=(Y.AOKI'1',K.HIROTA'1',H.KISHITA'1',K.KOYAMA'1',M.MASAKI'1', K.MIURA'1',Y.MUKOUHARA'1',S.NAKAGAWA'1',N.OKUMURA'1', Y.TAGISHI'1'); INST-ATH=(2JPNTSU'1'); REF=NP/A; VLP=599(1996)417; RCTS=(28SI(P,P)28SI,40CA(P,P)40)CA; PHQS=(ANALPW,DSIGMA/DOMEGA-RATIO); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,25; RCT=40CA(P,P)40CA; RTY=(ELA-SCATT); ENR=NAT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=1.5MG/CM**2; ACC=(VDGT); INC-ENGY-LAB=(12.5MEV,14.5MEV,15.4MEV,16.5MEV,18.5MEV,20.5MEV); DELTA-INC-ENGY-LAB=800KEV; CHRG-INC-ION=1; DET-PARTCL=(P); COINC=NO; ANT-COINC=NO; /*@12@*/ SOLID-ANGL=1.1[1.4MSR; ERS-DET=80KEV; ANL=(OPT-MODEL); PHQ=(ANALPW, DSIGMA/DOMEGA-RATIO); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,25; INC-ENGY-LAB=14.5MEV; EMT=P; RSD=40CA; STATIST-ERR=<5%; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC ANALPW DELTA-ANALPW (DEG) (NODIM) (NODIM) 2.434E+01 -1.401E-02 +0.000E+00-0.000E+00 3.036E+01 2.034E-02 +0.000E+00-0.000E+00 3.660E+01 1.275E-01 +0.000E+00-0.000E+00 4.168E+01 2.040E-01 +0.000E+00-0.000E+00 4.602E+01 9.181E-02 +0.000E+00-0.000E+00 5.087E+01 -4.309E-02 +0.000E+00-0.000E+00 5.417E+01 -2.749E-01 +2.012E-02-1.643E-02 5.928E+01 -4.228E-01 +3.313E-02-5.952E-02 6.555E+01 -5.599E-01 +4.943E-02-2.976E-02 7.062E+01 -6.188E-01 +2.640E-02-2.957E-02 7.603E+01 -7.037E-01 +2.640E-02-3.979E-02 8.019E+01 -6.444E-01 +1.643E-02-3.947E-02 8.464E+01 -3.076E-01 +1.656E-02-6.599E-03 8.669E+01 -4.521E-02 +0.000E+00-0.000E+00 8.887E+01 1.182E-01 +0.000E+00-0.000E+00 9.221E+01 1.505E-01 +0.000E+00-0.000E+00 9.635E+01 8.767E-02 +0.000E+00-0.000E+00 9.996E+01 8.385E-02 +0.000E+00-0.000E+00 1.033E+02 6.004E-02 +0.000E+00-0.000E+00 1.076E+02 4.023E-02 +0.000E+00-0.000E+00 1.115E+02 8.280E-02 +0.000E+00-0.000E+00 1.152E+02 5.595E-02 +0.000E+00-0.000E+00 1.208E+02 -2.882E-02 +0.000E+00-0.000E+00 1.261E+02 -2.691E-01 +1.980E-02-6.729E-03 1.319E+02 -4.956E-01 +1.980E-02-2.950E-02 1.379E+02 -8.442E-01 +5.273E-02-3.287E-02 1.429E+02 -9.064E-01 +2.646E-02-2.653E-02 1.466E+02 -4.843E-01 +2.310E-02-3.287E-02 1.507E+02 6.023E-02 +0.000E+00-0.000E+00 1.554E+02 5.557E-01 +1.320E-02-1.637E-02 1.614E+02 7.914E-01 +2.983E-02-1.993E-02 1.669E+02 8.616E-01 +3.960E-02-2.627E-02 1.731E+02 7.806E-01 +2.290E-02-3.979E-02 \END; /*===================================================================*/ |