/*===================================================================*/ /* NRDF D1943 Data No.25 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,25; D#=D1943; TITLE=/ Angular distributions of protons from the alpha particle bombardment of 10B, 14N, 16O and 20Ne /; ATH=(H.YAMAGUCHI'1'); INST-ATH=(2JPNINS'1'); REF=JPJ; VLP=16(1961)583; /* Secondary reference - INS-J, 35(1960) (H.Yamaguchi et al., Numerical data) RCTS=(10B(ALPHA,P)13C, 14N(ALPHA,P)17O, 16O(ALPHA,P)19F, 20NE(ALPHA,P)23NA); PHQS=(XSECTN-RATIO, XSECTN, ANGL-DSTRN); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,25; /* 2005-07-22 : Compiled, C.Kurokawa + N.Otuka */ /* Related references - I.Nonaka et al., JPJ, 14(1959)1260. (Details of scattering chamber given). See also NRDF D1942. POL-TGT=0%; ALGN-TGT=0%; ACC=CYC; INST-ACC=2JPNINS; DELTA-INC-ENGY-LAB=XMEV'2'; /* '2' Absolute value of beam energy is in accuracy of a few per-cent. */ ERS-PRJ=0.5%; POL-PRJ=0%; DET-PARTCL=P; COINC=NO; ANT-COINC=NO; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,25; DELTA-INC-ENGY-LAB=XMEV'3'; /* '3' Absolute value of beam energy is in accuracy of a few per-cent. */ INC-ENGY-LAB=6.25MEV; EXC-ENGY=6.05MEV'4',6.13MEV'5'; J-PI=0+'4',3-'5'; /*FIG.6-(4)*/ /* D892 FIG.6-(4) */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (UB/SR) (UB/SR) 44.269 3.589E+00 +-0.122E+00 54.710 3.233E+00 +-0.156E+00 73.086 2.422E+00 +-0.222E-01 89.791 2.033E+00 +-0.556E-01 111.926 2.078E+00 +-0.111E+00 126.125 1.833E+00 +-0.111E+00 137.401 2.078E+00 +-0.889E-01 \END; /*===================================================================*/ |