/*===================================================================*/ /* NRDF D1765 Data No.16 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,16; D#=D1765; TITLE=/Measurement of neutron-production double-differential cross sections for intermediate energy pion incident reaction/; PURPOSE=/To measure the neutron-production double-differential cross section for 870-MeV (momentum of 1.0-GeV/c) pi+ and pi- and 2.1-GeV (that of 2.25-GeV/c) pi+ mesons incident on iron and lead targets at the pi2 beam line of the 12GeV proton synchrotron at High Energy Accelerator Research Organization (KEK)./; ATH=(Y.IWAMOTO'1', N.SHIGYO'1', H.KITSUKI'1', H.TENZOU'1', S.ISHIMOTO'1', K.MAEHATA'1', K.ISHIBASHI'1', T.NAKAMOTO'2', M.NUMAJIRI'2', S.MEIGO'3', H.TAKADA'3'); INST-ATH=(2JPNKYU'1', 2JPNKEK'2', 2JPNJAE'3'); /* '1' Department of Applied Quantum Physics and Nuclear Engineering */ REF=(NST'4', PR/C'5'); VLP=(38(2001)363'4', 70(2004)024602'5'); /* '5' Y.Iwamoto+, Analysis with in-medium nucleon-nucleon elastic cross section */ RCTS=(FE(PIP,N)X, FE(PIN,N)X, PB(PIP,N)X, PB(PIN,N)X); PHQS=ENGY-SPEC; /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,16; /* 2004-10-13 : Converted, Converted from EXFOR E1765 */ /* 2002-11-19 : Compiled */ RTY=SPAL; PHQ=ENGY-SPEC; ENR=NAT; CHM=ELM; PHYS-FORM=SLD; BAC=X; POL-TGT=0%; ALGN-TGT=0%; ACC=SYN'6'; /* '6' The pi-2 beam line of KEK */ INST-ACC=2JPNKEK; ERS-PRJ=XKEV'7'; /* '7' The momentum resolution of the secondary beam is about 1 % BEAM-INTNSTY=XMA'8'; /* '8' 10**5 particles/2.5 s */ POL-PRJ=0%; ION-SOURCE=/ Incident particles were generated as a secondary beam from an internal target mounted in the accelertor ring.For the positive beam incidence, the Time-of-Flight of incident particles was measured for separating pi+ mesons from other particles by the use of a pair of Pilot U scintillators.Cerenkov counter was set up at the beam line to distinguish pi+ and mu+ particles. /; DET-PARTCL=N; COINC=NO; ANT-COINC=NO; DET-SYS=(SCT'9',SCT'10',TOF); /* '9' NE213 liquid scintillators of 12.7 cm in diameter and 12.7 cm thick were placed in directions of 15 degree, 30 degree, 60 degree, 90 degree, 120 degree for the neutron TOF measurements /* '10' NE102A plastic scintillators of 1 cm thick were mounted as veto detectors to eliminate charged-particle enents by the anticoincidence method */ EFCN-DET=/ The neutron detection efficiencies were obtained by calculation results obtained from the SCINFUL (J.K.Dickens, SCINFUL: A monte Carlo Based Computer Program to Determine a Scintillator Full Energy Response to Neutron Detection for En between 0.1 and 80MeV: User's Manual and Fortran Program Listing, ORNL-6462,(1988).) and the CECIL(R.A.Cecil, et al., Nucl. Instrum. Methods., 161, 439(1979).) codes. Calculated results of the neutron detection efficiencies for the four threshold levels are plotted in Fig. 6, p366 in reference. /; /* Experimental Method: - Time-of-flight RCT=FE(PIP,N)X; THK-TGT=XMG/CM**2'26'; /* '26' 4.9cm in diameter and 3.0cm thick */ INC-ENGY-LAB=2.1GEV; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,16; INC-ENGY-LAB=2.1GEV; EMT=N; THTL=90DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) (MB/SR/MEV) 1.25 23.2 7.0059 1.75 20.3 6.1402 2.5 15.6 4.7059 3.5 13.004 2.9629 4.5 10.926 2.4863 5.5 8.7574 2.0016 7 6.6262 1.5036 9 4.909 1.1219 12.5 2.9391 0.66921 17.5 1.9506 0.44854 22.5 1.2922 0.30528 27.5 1.1727 0.27988 35 1.0638 0.2478 45 0.83888 0.19823 55 0.81218 0.19411 65 0.71927 0.17444 75 0.58175 0.14411 90 0.43395 0.10899 125 0.23742 0.058791 175 0.079733 0.022224 250 0.040363 0.01103 350 0.016472 0.0050562 450 0.011612 0.0037467 550 0.0079636 0.0029743 650 0.0019622 0.001112 \END; /*===================================================================*/ |