/*===================================================================*/ /* NRDF D0152 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; D#=D152; TITLE=/(P,D) REACTIONS AT 52 MEV.I.58NI(P,D)57NI (EXPERIMENTAL)/; PURPOSE=/TO TEST THE VALIDITY OF CURRENT REACTION THEORIES,(P,D)ANGULAR DISTRIBUTION HAVE BEEN TAKEN AT THE INCIDENT ENERGY OF 52MEV, THE HIGHEST ENERGY SO FAR STUDIED,OVER A WIDE RANGE OF ANGLES AND IN SMALL STEPS'D'/; ATH=(H.OHNUMA'C',T.SUEHIRO'A,C',M.SEKIGUCHI'C',S.YAMADA'B,C'); INST-ATH=(2JPNINS'C'); /* 'A' PRESENT ADRESS:TOHOKU INSTITUTE OF TECHNOLOGY */ /* 'B' PRESENT ADRESS: TOKYO INSTITUTE OF TECHNOLOGY */ REF=JPJ; VLP=36(1974)1236; RCTS=(58NI(P,D)57NI); /* 'D'THE 58NI(P,D)REACTION,WHICH WE BELIEVE REQUIRE ANALYSIS FROM VARIOUS ASPECTS. BRIET DESCRIPTION OF ANALYSIS AND SPECTIOSCOPIC INFORMATION OBTAINED ARE ALSO GIVEN. DETAILS OF THE ANALYSIS WE HAVE DONE SO FAR WILL BE GIVEN IN A SUBSEQUENT PAPER: H.OHNUMA ET AL., J .PHYS.SOC.JAPAN 36(1974)1245 */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,2; RCT=58NI(P,D)57NI; CHM=ELM; THK-TGT=2.7MG/CM**2; BAC=SELF; ACC=(SYNCYC); INST-ACC=2JPNINS; INC-ENGY-RANGE=(51.93MEV); DET-PARTCL=(D); DET-SYS=(D); DET-SYS=(MAG+PROP-CNTR); ERS-DET=70KEV; ANL=(OPT-MODEL,DWBA); PHQ=(ANGL-DSTRN); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; INC-ENGY=51.93MEV; THTC=5.8[110.3DEG; EXC-ENGY=1.10MEV; J-PI=1/2-; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 6.0 1.04 0.02 8.0 0.95 0.02 10.6 0.73 0.02 13.1 0.42 0.02 15.7 0.24 0.01 18.3 0.19 0.01 20.8 0.20 0.01 23.4 0.20 0.01 26.0 0.16 0.01 28.5 0.11 0.01 31.1 0.083 0.004 33.7 0.059 0.004 36.2 0.064 0.004 38.8 0.054 0.003 41.3 0.039 0.003 43.9 0.025 0.002 46.4 0.018 0.002 49.0 0.015 0.002 51.5 0.013 0.0014 54.1 0.011 0.0013 56.6 0.013 0.0014 59.1 0.012 0.0014 61.7 0.010 0.0013 64.2 0.0085 0.0012 66.7 0.0087 0.0012 69.3 0.0084 0.0012 71.8 0.0057 0.0010 74.3 0.0062 0.0010 76.8 0.0048 0.0009 79.4 0.0043 0.0008 81.9 0.0048 0.0009 86.9 0.0033 0.0007 91.9 0.0033 0.0007 96.9 0.0024 0.0006 101.9 0.0024 0.0006 106.8 0.0014 0.0005 111.8 0.0016 0.0005 \END; /*===================================================================*/ |