/*===================================================================*/ /* NRDF D1273 Data No.14 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,14; D#=D1273; TITLE=/A STUDY OF K-PI+ SCATTERING IN THE REACTION K- P -> K- PI+ N AT 11 GEV/C/; ATH=(D.ASTON'1',N.AWAJI'2',T.BIENZ'1',F.BIRD'1',J.D'AMORE'3', W.DUNWOODIE'1',R.ENDORF'3',K.FUJII'2',H.HAYASHI'2',S.IWATA'2', W.B.JOHNSON'1',R.KAJIKAWA'2',P.KUNZ'1',D.W.G.S.LEITH'1', L.LEVINSON'1',T.MATSUI'2',B.T.MEADOWS'3',A.MIYAMOTO'2', M.NUSSBAUM'3',H.OZAKI'2',C.O.PAK'2',B.N.RATCLIFF'1',D.SCHULTZ'1', S.SHAPIRO'1',T.SHIMOMURA'2',P.K.SINERVO'1',A.SUGIYAMA'2', S.SUZUKI'2',G.TARNOPOLSKY'1',T.TAUCHI'2',N.TOGE'1',K.UKAI'4', A.WAITE'1',S.WILLIAMS'1'); INST-ATH=(1USASTF'1',2JPNNAG'2',1USAUCN'3',2JPNINS'4'); REF=NP/B; VLP=296(1988)493; RCTS=(P(KN,KN,PIP)N); PHQS=(ENGY-SPEC); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,14; RCT=P(KN,KN,PIP)N; CHM=ELM; PHYS-FORM=LIQD; INC-MOM-LAB=(11GEV/C); ERS-PRJ=0.4%; DET-PARTCL=(KN,PIP); DET-SYS=(MAG+PLST-SCT+SPK+MWPC+X'21'+TOF+EDE); /*@21@*/ SOLID-ANGL=4*PISR; ANL=(X'22'); /*@22@*/ PHQ=(ENGY-SPEC); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,14; INC-MOM-LAB=11GEV/C; DATA3=1'33'; DATA4=1'34'; /*@33@*/ /*@34@*/ /*FIG.2-A*/ /* D1273 FIG.2-(A) */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA1'31' DATA2'32' DELTA-DATA2'32' (GEV/C**2) (1/(MEV/C**2)) (1/(MEV/C**2)) 0.832 -1.920E+03 +5.480E+02-4.106E+02 0.840 -2.332E+03 +4.791E+02-4.110E+02 0.848 -3.634E+03 +4.110E+02-3.425E+02 0.860 -4.114E+03 +4.106E+02-4.793E+02 0.868 -5.758E+03 +5.478E+02-6.165E+02 0.889 -6.238E+03 +4.795E+02-8.220E+02 0.898 -3.978E+03 +4.110E+02-7.535E+02 0.906 -1.033E+03 +6.163E+02-7.535E+02 0.915 -2.802E+02 +XXXXXXXXX-XXXXXXXXX 0.940 -1.103E+03 +5.480E+02-5.480E+02 0.940 2.666E+02 +XXXXXXXXX-XXXXXXXXX 0.956 6.768E+02 +5.482E+02-4.110E+02 0.973 -7.740E+01 +XXXXXXXXX-XXXXXXXXX 0.998 1.702E+03 +4.793E+02-4.110E+02 1.023 2.628E+02 +XXXXXXXXX-XXXXXXXXX 1.039 -2.859E+02 +4.795E+02-3.425E+02 1.068 -2.187E+02 +XXXXXXXXX-XXXXXXXXX 1.089 -3.567E+02 +XXXXXXXXX-XXXXXXXXX 1.114 -8.373E+02 +XXXXXXXXX-XXXXXXXXX 1.139 -8.496E+01 +XXXXXXXXX-XXXXXXXXX 1.176 -5.662E+02 +XXXXXXXXX-XXXXXXXXX 1.184 -8.405E+02 +XXXXXXXXX-XXXXXXXXX 1.205 -1.565E+02 +XXXXXXXXX-XXXXXXXXX 1.221 -1.572E+02 +XXXXXXXXX-XXXXXXXXX 1.238 -1.459E+03 +XXXXXXXXX-XXXXXXXXX 1.271 -1.598E+03 +4.112E+02-5.480E+02 1.296 -5.716E+02 +XXXXXXXXX-XXXXXXXXX 1.313 -3.669E+02 +XXXXXXXXX-XXXXXXXXX 1.317 -1.189E+03 +6.161E+02-4.112E+02 1.354 -1.670E+03 +6.165E+02-4.797E+02 1.387 -1.535E+03 +4.110E+02-3.425E+02 1.408 -1.536E+03 +5.476E+02-3.425E+02 1.429 -5.777E+02 +XXXXXXXXX-XXXXXXXXX 1.445 -1.606E+03 +4.793E+02-4.110E+02 1.457 -1.469E+03 +XXXXXXXXX-XXXXXXXXX 1.474 -1.333E+03 +XXXXXXXXX-XXXXXXXXX 1.487 -1.128E+03 +XXXXXXXXX-XXXXXXXXX 1.499 -9.234E+02 +XXXXXXXXX-XXXXXXXXX 1.528 -7.192E+02 +XXXXXXXXX-XXXXXXXXX 1.540 -6.513E+02 +XXXXXXXXX-XXXXXXXXX 1.553 -6.519E+02 +XXXXXXXXX-XXXXXXXXX 1.569 -7.896E+02 +XXXXXXXXX-XXXXXXXXX 1.603 -1.065E+03 +XXXXXXXXX-XXXXXXXXX 1.636 -1.067E+03 +XXXXXXXXX-XXXXXXXXX 1.677 -1.137E+03 +XXXXXXXXX-XXXXXXXXX 1.706 -1.823E+03 +XXXXXXXXX-XXXXXXXXX 1.756 -9.351E+02 +XXXXXXXXX-XXXXXXXXX 1.793 -1.690E+03 +XXXXXXXXX-XXXXXXXXX 1.843 -1.556E+03 +XXXXXXXXX-XXXXXXXXX 1.868 -1.214E+03 +XXXXXXXXX-XXXXXXXXX 1.909 -1.148E+03 +XXXXXXXXX-XXXXXXXXX 1.934 -1.560E+03 +XXXXXXXXX-XXXXXXXXX 1.971 -1.698E+03 +XXXXXXXXX-XXXXXXXXX 2.013 -1.769E+03 +XXXXXXXXX-XXXXXXXXX 2.050 -1.839E+03 +XXXXXXXXX-XXXXXXXXX 2.091 -1.841E+03 +XXXXXXXXX-XXXXXXXXX 2.129 -1.774E+03 +XXXXXXXXX-XXXXXXXXX 2.170 -1.913E+03 +XXXXXXXXX-XXXXXXXXX 2.207 -1.778E+03 +XXXXXXXXX-XXXXXXXXX 2.253 -1.643E+03 +XXXXXXXXX-XXXXXXXXX 2.294 -1.987E+03 +XXXXXXXXX-XXXXXXXXX 2.332 -1.920E+03 +XXXXXXXXX-XXXXXXXXX 2.390 -1.649E+03 +XXXXXXXXX-XXXXXXXXX 2.448 -1.583E+03 +XXXXXXXXX-XXXXXXXXX 2.522 -1.176E+03 +XXXXXXXXX-XXXXXXXXX \END; /*===================================================================*/ |