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/* NRDF D1273 Data No.26 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,26;
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,26;
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,26;
INC-MOM-LAB=11GEV/C;
DATA3=2'33';
DATA4=2'34';
/*@33@*/ /*@34@*/
/*FIG.3-A*/
/* D1273 FIG.3-(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))
0.828 -4.623E+02 +3.386E+02-2.110E+02
0.843 -1.054E+03 +4.660E+02-4.654E+02
0.854 -5.455E+02 +4.662E+02-2.536E+02
0.866 -2.661E+03 +3.384E+02-4.656E+02
0.877 -2.195E+03 +4.656E+02-3.388E+02
0.885 -4.057E+03 +5.501E+02-6.351E+02
0.893 -6.216E+03 +5.926E+02-5.505E+02
0.903 -4.776E+03 +8.468E+02-4.656E+02
0.904 -6.681E+03 +7.196E+02-6.349E+02
0.929 -4.986E+03 +4.656E+02-7.196E+02
0.935 -2.700E+03 +4.235E+02-6.773E+02
0.949 -1.175E+03 +5.928E+02-4.229E+02
0.953 -2.318E+03 +7.196E+02-3.810E+02
0.982 -1.131E+03 +5.082E+02-3.810E+02
0.993 -6.647E+02 +3.810E+02-4.662E+02
1.018 -5.786E+02 +XXXXXXXXX-XXXXXXXXX
1.043 1.424E+02 +XXXXXXXXX-XXXXXXXXX
1.066 -2.373E+02 +XXXXXXXXX-XXXXXXXXX
1.080 5.984E+01 +XXXXXXXXX-XXXXXXXXX
1.102 -1.082E+02 +XXXXXXXXX-XXXXXXXXX
1.120 1.468E+02 +XXXXXXXXX-XXXXXXXXX
1.142 -3.600E+02 +XXXXXXXXX-XXXXXXXXX
1.153 2.163E+01 +XXXXXXXXX-XXXXXXXXX
1.186 1.505E+02 +XXXXXXXXX-XXXXXXXXX
1.197 -5.685E+02 +XXXXXXXXX-XXXXXXXXX
1.219 -2.286E+02 +XXXXXXXXX-XXXXXXXXX
1.233 2.378E+02 +XXXXXXXXX-XXXXXXXXX
1.255 7.470E+02 +XXXXXXXXX-XXXXXXXXX
1.277 -9.835E+01 +XXXXXXXXX-XXXXXXXXX
1.306 4.112E+02 +XXXXXXXXX-XXXXXXXXX
1.325 7.364E+01 +3.388E+02-2.540E+02
1.361 -9.362E+01 +XXXXXXXXX-XXXXXXXXX
1.376 -8.970E+02 +3.388E+02-2.540E+02
1.394 -1.150E+03 +XXXXXXXXX-XXXXXXXXX
1.427 -1.021E+03 +XXXXXXXXX-XXXXXXXXX
1.442 -8.087E+02 +XXXXXXXXX-XXXXXXXXX
1.463 -5.958E+02 +XXXXXXXXX-XXXXXXXXX
1.493 -4.248E+02 +XXXXXXXXX-XXXXXXXXX
1.518 -2.964E+02 +XXXXXXXXX-XXXXXXXXX
1.540 -4.645E+02 +XXXXXXXXX-XXXXXXXXX
1.558 2.165E+00 +XXXXXXXXX-XXXXXXXXX
1.595 -2.498E+02 +XXXXXXXXX-XXXXXXXXX
\END;
/*===================================================================*/
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