/*===================================================================*/
 /* NRDF D1610 Data No.1                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1610;
 TITLE=/ Lambda hyperon production at backward angles in the reaction
         6Li(pi-,Lambda)X at 4GeV/c /;
 PURPOSE=/ To measure invariant cross sections and polarizations of
           Lambda hyperons /;
 ATH=(K.TOMIZAWA'1', I.ARAI'1', H.KITAYAMA'1', N.KATO'1', Y.NAGASAKA'1',
      M.TANAKA'1', K.YAGI'1', J.CHIBA'2', T.KOBAYASHI'2', A.MANABE'2',
      T.NAGAE'3', M.SEKIMOTO'3', V.PANTUEV'4');
 INST-ATH=(2JPNTSU'1', 2JPNKEK'2', 2JPNINS'3', 4RUSJIA'4');
      /* '1' Institute of Physics */
 REF=PL/B;
 VLP=328(1994)264;
 RCTS=6LI(PIN,LAMDA)X;
 PHQS=(DATA'5', ENGY-SPEC'6', ANGL-DSTRN, POL);
 /* '5' Invariant-mass spectra of a (proton,pi-) pair */
 /* '6' Invariant cross sections */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2003-08-13 : Converted, Am + On. Data converted to EXFOR E1610
 /* 2005-11-03 : Converted, On. Converted from EXFOR E1610 */
 RTY=INCL;
 ENR=93%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'7';
 /* '7' 36 mm thick and 32 mm in diameter */
 ACC=SYN'8';
 /* '8' pi2 beam line of 12 GeV proton synchrotron (12GeV PS) */
 INST-ACC=2JPNKEK;
 INC-MOM-LAB=4GEV/C;
 ION-SOURCE=/ Spallation /;
 DET-PARTCL=(PIN,P);
 COINC=(P,PIN);
 ANT-COINC=NO;
 DET-SYS=(X'9',SCT'10',X'11');
 /* '9' Cylindrical drift chamber (CDC) for measuring the momentum
        and trajectory of the outgoing particles with a momentum
        resolution of Delta P/P is about 10%. */
 /* '10' Cylindrical hodoscope (CDH) which consists of 24 plastic
         scintillator counters used to measure the time-of-flight of
         the outgoing particle */
 /* '11' Cylindrical drift chamber (VC) used to detect a vertex
         point by measuring the trajectories of the Lambda hyperon's
         decay products (proton and pi-). */
 /* 2006-12-19 : Altered, At. Re-digitized */
 RCT=6LI(PIN,LAMDA)X;
 PHQ=DATA'12';
 /* '12' Invariant-mass spectra of a (proton,pi-) pair */
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-MOM-LAB=4GEV/C;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 DATA1'13' COUNTS'14' DELTA-COUNTS'14'
 (MEV/C**2) (UNIT1) (UNIT1)
 1.083E+03 4.013E+01 +-5.406E+00
 1.088E+03 8.811E+01 +-8.786E+00
 1.092E+03 9.620E+01 +-8.786E+00
 1.098E+03 1.124E+02 +-1.014E+01
 1.103E+03 1.813E+02 +-1.216E+01
 1.107E+03 2.678E+02 +-1.622E+01
 1.112E+03 3.077E+02 +-1.690E+01
 1.117E+03 2.523E+02 +-1.622E+01
 1.123E+03 1.671E+02 +-1.216E+01
 1.128E+03 1.211E+02 +-1.081E+01
 1.132E+03 1.333E+02 +-1.081E+01
 1.138E+03 1.150E+02 +-1.014E+01
 1.143E+03 1.137E+02 +-1.014E+01
 1.147E+03 9.540E+01 +-9.463E+00
 1.153E+03 8.052E+01 +-8.111E+00
 1.157E+03 9.538E+01 +-8.784E+00
 1.163E+03 8.388E+01 +-8.111E+00
 1.168E+03 6.832E+01 +-8.110E+00
 1.173E+03 8.656E+01 +-8.110E+00
 1.178E+03 8.384E+01 +-8.110E+00
 1.183E+03 6.288E+01 +-7.434E+00
 1.188E+03 6.287E+01 +-6.758E+00
 1.193E+03 5.745E+01 +-6.756E+00
 1.198E+03 5.339E+01 +-6.758E+00
 1.203E+03 4.121E+01 +-5.407E+00
 1.208E+03 4.255E+01 +-5.406E+00
 1.213E+03 5.741E+01 +-6.759E+00
 1.218E+03 5.199E+01 +-6.759E+00
 1.223E+03 4.319E+01 +-5.407E+00
 1.228E+03 3.845E+01 +-5.408E+00
 1.233E+03 4.114E+01 +-5.406E+00
 1.238E+03 2.964E+01 +-4.729E+00
 1.243E+03 3.098E+01 +-4.732E+00
 1.248E+03 3.232E+01 +-4.731E+00
 1.253E+03 3.231E+01 +-4.731E+00
 1.258E+03 3.568E+01 +-5.406E+00
 1.263E+03 3.094E+01 +-4.055E+00
 1.268E+03 2.822E+01 +-4.056E+00
 1.273E+03 2.483E+01 +-4.056E+00
 1.278E+03 2.820E+01 +-4.055E+00
 1.283E+03 2.819E+01 +-4.731E+00
 1.287E+03 1.872E+01 +-4.055E+00
 1.293E+03 2.681E+01 +-4.055E+00
 1.298E+03 2.680E+01 +-4.057E+00
 \END;
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