/*===================================================================*/ /* NRDF D1601 Data No.1 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,1; D#=D1601; TITLE=/ Core-excited states of 12(Lambda)C hypernuclei formed in the (pi+,K+) reaction /; PURPOSE=/ The present letter reports on a high-quality 12(lamda) hypernuclear spectrum /; ATH=(T.HASEGAWA'1', O.HASHIMOTO'1', S.HOMMA'1', T.MIYACHI'1', T.NAGAE'1', M.SEKIMOTO'1', T.SHIBATA'1', H.SAKAGUCHI'2', T.TAKAHASHI'2', K.AOKI'3', H.NOUMI'3', H.BHANG'4', M.YOUN'4', Y.GAVRILOV'5', S.AJIMURA'6', T.KISHIMOTO'6', A.OHKUSU'6', K.MAEDA'7', R.SAWAFTA'8', R.P.REDWINE'9'); INST-ATH=(2JPNINS'1', 2JPNKTO'2', 2JPNKEK'3', 3KORNSU'4', 4RUSJIA'5', 2JPNOSA'6', 2JPNTOH'7', 1USABNL'8', 1USAMIT'9'); /* '2' Department of Physics */ /* '4' Department of Physics */ /* '6' Department of Physics */ /* '7' Department of Physics */ /* '8' Physics Department */ /* '9' Laboratory for Nuclear Science */ REF=PRL; VLP=74(1995)224; RCTS=12C(PIP,KP)X; PHQS=(ENGY-SPEC'10', XSECTN); /* '10' Excitation spectrum of 12(Lambda)C */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,1; /* 2003-08-22 : Converted, Am + On. Data converted to EXFOR E1601 /* 2005-08-12 : Altered, On. REACTION corrected (CP-D/430) */ /* 2005-11-03 : Converted, On. Converted from EXFOR E1601 */ ENR=NAT; CHM=ELM; PHYS-FORM=SLD; THK-TGT=890MG/CM**2; POL-TGT=0%; ALGN-TGT=0%; ACC=SYN; INST-ACC=2JPNKEK'11'; /* '11' K6 beam channel */ INC-MOM-LAB=1.06GEV/C; BEAM-INTNSTY=XNA'12'; /* '12' 3*10**6/spill */ POL-PRJ=0%; DET-PARTCL=KP; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'13',X'14',CRNKOV'15'); /* '13' Large superconducting dipole magnet spectrometer SKS [T. Shintomi et al., IEEE Trans. Magnetics, MAG-28(1992)585] to determines the momenta of kaons from target. */ /* '14' Drift chamber */ /* '15' Used as trigger counters in the identification of kaons SOLID-ANGL=100MSR; ERS-DET=[1.9MEV'16'; /* '16' 1.9+-0.1 MeV - full width at half minimum */ /* 2006-11-06 : Altered, Is. Re-digitized */ RCT=12C(PIP,KP)X; PHQ=ENGY-SPEC'17'; /* '17' Excitation spectrum of 12(Lambda)C */ /* Analysis: - Integration of angular distribution (integrated from 2 to 14 deg) /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,1; INC-MOM-LAB=1.06GEV/C; THTL=2[14DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY'18' DSIGMA/DE DELTA-DSIGMA/DE (MEV) (UB/MEV) (UB/MEV) -1.369E+01 5.887E-04 +-NEGLIGIBLE -1.320E+01 6.021E-04 +-NEGLIGIBLE -1.266E+01 -1.563E-04 +-NEGLIGIBLE -1.217E+01 -1.428E-04 +-NEGLIGIBLE -1.168E+01 -1.294E-04 +-NEGLIGIBLE -1.115E+01 -1.148E-04 +-NEGLIGIBLE -1.066E+01 2.024E-03 +-NEGLIGIBLE -1.016E+01 -8.793E-05 +-NEGLIGIBLE -9.673E+00 2.244E-03 +-NEGLIGIBLE -9.180E+00 1.678E-03 +-NEGLIGIBLE -8.645E+00 -4.649E-05 +-NEGLIGIBLE -8.195E+00 7.388E-04 +-NEGLIGIBLE -7.702E+00 -2.072E-05 +-NEGLIGIBLE -7.292E+00 -9.521E-06 +-NEGLIGIBLE -6.882E+00 1.680E-06 +-NEGLIGIBLE -6.636E+00 8.401E-06 +-NEGLIGIBLE -6.189E+00 3.692E-03 +-2.126E-03 -5.695E+00 1.580E-03 +-NEGLIGIBLE -5.202E+00 1.207E-03 +-NEGLIGIBLE -4.750E+00 4.464E-04 +-NEGLIGIBLE -4.216E+00 -1.187E-04 +-NEGLIGIBLE -3.728E+00 2.793E-03 +-1.546E-03 -3.239E+00 4.932E-03 +-2.512E-03 -2.787E+00 4.172E-03 +-1.739E-03 -2.213E+00 4.380E-03 +-1.739E-03 -1.740E+00 2.043E-02 +-4.251E-03 -1.278E+00 4.460E-02 +-6.956E-03 -8.176E-01 1.035E-01 +-1.005E-02 -3.248E-01 1.696E-01 +-1.198E-02 2.146E-01 1.644E-01 +-1.179E-02 6.547E-01 1.067E-01 +-9.662E-03 1.268E+00 7.481E-02 +-8.309E-03 1.724E+00 3.715E-02 +-5.797E-03 2.203E+00 4.817E-02 +-6.763E-03 2.668E+00 3.659E-02 +-5.797E-03 3.196E+00 4.066E-02 +-6.570E-03 3.678E+00 1.536E-02 +-3.863E-03 4.176E+00 1.113E-02 +-3.092E-03 4.669E+00 1.037E-02 +-2.898E-03 5.200E+00 1.173E-02 +-3.092E-03 5.678E+00 2.353E-02 +-4.831E-03 6.210E+00 2.432E-02 +-4.638E-03 6.656E+00 2.800E-02 +-5.217E-03 7.200E+00 1.894E-02 +-3.865E-03 7.682E+00 2.765E-02 +-5.217E-03 8.169E+00 3.133E-02 +-5.797E-03 8.657E+00 3.502E-02 +-5.792E-03 9.189E+00 6.885E-02 +-7.343E-03 9.612E+00 9.185E-02 +-8.889E-03 1.020E+01 1.433E-01 +-1.121E-02 1.067E+01 1.642E-01 +-1.237E-02 1.117E+01 1.611E-01 +-1.217E-02 1.172E+01 1.489E-01 +-1.121E-02 1.219E+01 9.540E-02 +-8.890E-03 1.267E+01 7.203E-02 +-8.119E-03 1.321E+01 6.664E-02 +-7.729E-03 1.367E+01 5.969E-02 +-7.536E-03 1.415E+01 6.589E-02 +-7.536E-03 1.468E+01 7.190E-02 +-8.117E-03 1.518E+01 6.630E-02 +-7.344E-03 1.560E+01 9.105E-02 +-8.889E-03 1.609E+01 9.010E-02 +-9.083E-03 1.664E+01 7.620E-02 +-8.309E-03 1.710E+01 1.077E-01 +-1.005E-02 1.761E+01 8.705E-02 +-8.889E-03 1.809E+01 9.827E-02 +-9.469E-03 1.862E+01 1.064E-01 +-1.005E-02 1.912E+01 9.308E-02 +-9.082E-03 1.962E+01 8.961E-02 +-9.082E-03 2.012E+01 1.136E-01 +-1.024E-02 2.064E+01 9.602E-02 +-9.468E-03 2.113E+01 1.300E-01 +-1.102E-02 2.171E+01 1.274E-01 +-1.101E-02 2.217E+01 1.169E-01 +-1.044E-02 2.262E+01 1.139E-01 +-1.024E-02 2.312E+01 1.115E-01 +-1.044E-02 2.368E+01 1.222E-01 +-1.044E-02 2.414E+01 1.154E-01 +-1.024E-02 2.468E+01 1.116E-01 +-1.063E-02 2.519E+01 1.313E-01 +-1.082E-02 2.563E+01 1.043E-01 +-9.663E-03 2.615E+01 1.139E-01 +-1.043E-02 2.666E+01 1.041E-01 +-9.662E-03 2.722E+01 1.428E-01 +-1.159E-02 2.773E+01 1.302E-01 +-1.082E-02 2.816E+01 1.113E-01 +-1.043E-02 2.867E+01 1.013E-01 +-9.468E-03 2.925E+01 1.312E-01 +-1.082E-02 2.971E+01 1.204E-01 +-1.043E-02 3.020E+01 1.204E-01 +-1.043E-02 3.076E+01 1.355E-01 +-1.159E-02 3.130E+01 1.313E-01 +-1.140E-02 3.177E+01 1.497E-01 +-1.256E-02 3.223E+01 1.408E-01 +-1.159E-02 3.277E+01 1.335E-01 +-1.159E-02 3.324E+01 1.182E-01 +-1.082E-02 3.373E+01 1.501E-01 +-1.237E-02 3.425E+01 1.625E-01 +-1.295E-02 3.469E+01 1.424E-01 +-1.179E-02 3.522E+01 1.426E-01 +-1.217E-02 3.570E+01 1.179E-01 +-1.063E-02 \END; /*===================================================================*/ |