/*===================================================================*/
 /* NRDF D1759 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 D#=D1759;
 TITLE=/ Measurements of secondary neutrons produced from thick
         targets bombarded by high energy neon ions /;
 PURPOSE=/ To perform a systematic study to measure the angular and
           energy distributions of neutrons produced from thick C, Al,
           Cu, and Pb targets bombarded by 100, 180 and 400 MeV/nucleon
           Ne ions. /;
 ATH=(T.KUROSAWA'1', N.NAKAO'2', T.NAKAMURA'1', Y.UWAMINO'3',
      T.SHIBATA'2', A.FUKUMURA'4', K.MURAKAMI'4');
 INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNIPC'3', 2JPNIRS'4');
      /* '1' Cyclotron and Radioisotope Center */
 REF=NST;
 VLP=36(1999)41;
 RCTS=(C(20NE,N)X, 27AL(20NE,N)X, CU(20NE,N)X, PB(20NE,N)X);
 PHQS=(ENGY-SPEC, N-MLT'5');
 /* '5' Thick target differential multiplicity of neutron with
    respect to angle integrated over partial angular range */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 /* 2002-02-24 : Compiled+Checked, R.Suzuki + sK */
 /* 2004-04-23 : Altered, N.Otuka. MLT in SF6 replaced by PY */
 /* 2008-01-30 : Altered, N.Otuka. EDE added under METHOD */
 /* 2009-08-23 : Altered, Nf. 014-017 corrected */
 RTY=HEAVY-ION-RCT;
 ENR=NAT'6';
 /* '6' The enrichments of targets are not given in the reference.
        But compiler asked T.Kurosawa. */
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'7';
 /* '7' Heavy Ion Medical Accelerator in Chiba (HIMAC) */
 INST-ACC=2JPNIRS'8';
 /* '8' The mass numbers of projectiles are not given in the
        reference. But compiler asked NIRS staff. */
 BEAM-INTNSTY=XMA'9';
 /* '9' The beam intensities were kept to be 100,000-1,000,000
        particles per pulse. */
 POL-PRJ=0%;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'10',SCT'11',TOF'12',EDE'13');
 /* '10' Plastic scintillator (NE102A) was used as the delta-E
         counter and the beam pick-up counter. Liquid scintillator
         (NE213) was used as the E counter. */
 /* '11' Liquid scintillator */
 /* '12' To measure the energy of neutron */
 /* '13' To eliminate charged particles */
 ERS-DET=XKEV'14';
 /* '14' The neutron energy resolutions is represented as a
         function of neutron energy at Fig. 2 in reference. */
 CALB-DET=/ Each E counter was calibrated with a 60Co Gamma-ray source.
 EFCN-DET=/ The neutron detection efficiencies were calculated with the
            Monte Carlo code of Cecil et al. for all energy ranges.
            Reference: R. A. Cecil, B. D. Anderson, and R. Madey, Nucl.
            Instrum. Methods 161, 439 (1979). /;
 /* 2003-09-22 : Altered, N.Otuka. Data are revised by author. */
 /* 2007-10-25 : Altered, N.Otuka. Superseded by data with new
    analysis */
 RCT=CU(20NE,N)X;
 PHQ=ENGY-SPEC;
 THK-TGT=4465MG/CM**2;
 INC-ENGY-LAB-RANGE=100MEV/A;
 ANL=(INCASC'24',X'25');
 /* '24' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
 /* '25' Phenomenological Hybrid analysis by the moving source
         model */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 SYS-ERR=(3%'15',10%'16',8%'17',14%'18');
 /* '15' Notmalization uncertainty due to number of accepted beam
         particles incident on target */
 /* '16' Normalization uncertainty due to solid angle uncertainty
 /* '17' Normalization uncertainty due to additional uncertainty
         in the efficiencies at neutron energies near threshold (8% in
         Table 2, but 7% in text) */
 /* '18' Total normalization uncertainty */
 STATIST-ERR=X%'19';
 /* '19' The statistical uncertainties vary in a range of 2 to 5 %
         for the low- to medium-energy (5-50 MeV) region of the spectra
         and increase to about 30% at the highest energies. */
 INC-ENGY-LAB=100MEV/A;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL ENGY-EMT-LAB DN/DOMEGA/DE
 (DEG) (MEV) (1/SR/MEV/PARTCL)
 0 6.509555 3.91168E-03
 0 7.20987 3.39817E-03
 0 7.983885 2.46233E-03
 0 8.83905 2.34032E-03
 0 9.799335 2.75929E-03
 0 10.85252 2.22099E-03
 0 12.00495 2.12740E-03
 0 13.28785 2.25228E-03
 0 14.71425 2.22130E-03
 0 16.2973 2.09035E-03
 0 18.04995 2.20035E-03
 0 19.9845 2.00920E-03
 0 22.1116 2.97640E-03
 0 24.52675 2.71813E-03
 0 27.26295 2.81058E-03
 0 30.2661 3.20003E-03
 0 33.53965 3.32666E-03
 0 37.2437 2.92991E-03
 0 41.4151 3.43915E-03
 0 45.9195 3.71139E-03
 0 50.99215 3.61384E-03
 0 56.66305 3.94170E-03
 0 63.0506 3.71793E-03
 0 70.1812 3.59795E-03
 0 78.2024 2.69976E-03
 0 87.1258 2.64204E-03
 0 97.1282 1.49537E-03
 0 108.1842 1.22484E-03
 0 120.4905 6.25320E-04
 0 133.945 3.68922E-04
 0 148.7405 1.70989E-04
 0 166.362 8.44259E-05
 0 185.5285 6.86112E-05
 0 206.4865 5.74794E-05
 0 231.6655 1.81525E-05
 7.5 6.621 3.84902E-03
 7.5 7.32574 4.02467E-03
 7.5 8.104965 2.99013E-03
 7.5 8.980295 2.30697E-03
 7.5 9.94192 2.23180E-03
 7.5 10.9965 1.78944E-03
 7.5 12.17275 2.29723E-03
 7.5 13.4836 2.27489E-03
 7.5 14.9427 1.92283E-03
 7.5 16.5641 2.31243E-03
 7.5 18.3616 1.90864E-03
 7.5 20.34845 2.29129E-03
 7.5 22.53615 2.07484E-03
 7.5 24.93355 2.27308E-03
 7.5 27.65065 2.51152E-03
 7.5 30.7209 2.12281E-03
 7.5 34.07185 2.84658E-03
 7.5 37.8688 2.52863E-03
 7.5 42.1511 2.67054E-03
 7.5 46.7825 3.36681E-03
 7.5 52.007 2.92545E-03
 7.5 57.85805 2.99800E-03
 7.5 64.4618 2.61487E-03
 7.5 71.8492 2.68864E-03
 7.5 80.1794 1.97452E-03
 7.5 89.4694 2.09801E-03
 7.5 99.91235 1.42111E-03
 7.5 111.489 1.09833E-03
 7.5 124.419 6.31933E-04
 7.5 138.604 3.95837E-04
 7.5 154.2645 1.85538E-04
 7.5 172.999 8.13194E-05
 7.5 193.473 5.58024E-05
 7.5 215.987 1.91442E-05
 7.5 243.205 1.31335E-05
 15 4.84016 2.63278E-03
 15 5.362725 3.65298E-03
 15 5.938045 2.63303E-03
 15 6.570545 3.58824E-03
 15 7.277525 2.21760E-03
 15 8.067445 2.28172E-03
 15 8.949435 2.03839E-03
 15 9.933125 1.93409E-03
 15 11.0283 1.77411E-03
 15 12.2448 1.36015E-03
 15 13.5921 1.49861E-03
 15 15.0785 1.35259E-03
 15 16.71045 1.35894E-03
 15 18.49175 1.75170E-03
 15 20.50545 1.54474E-03
 15 22.7727 1.39947E-03
 15 25.2291 1.51160E-03
 15 27.9967 1.33665E-03
 15 31.0958 1.57868E-03
 15 34.59105 1.40300E-03
 15 38.50345 1.55426E-03
 15 42.91525 1.45764E-03
 15 47.8445 1.42719E-03
 15 53.3926 1.19949E-03
 15 59.56585 1.32408E-03
 15 66.4838 1.04182E-03
 15 74.1249 1.01093E-03
 15 82.61885 7.71900E-04
 15 91.88785 5.79992E-04
 15 102.05195 4.04916E-04
 15 114.113 2.01863E-04
 15 127.1725 1.61404E-04
 15 141.3665 7.16716E-05
 15 158.292 4.85685E-05
 15 178.7615 2.02716E-05
 15 200.894 1.74253E-05
 30 6.05582 3.34792E-03
 30 6.71223 2.91718E-03
 30 7.43685 2.55832E-03
 30 8.23366 2.29206E-03
 30 9.138165 1.77672E-03
 30 10.16234 1.67290E-03
 30 11.2856 1.46058E-03
 30 12.5086 1.51098E-03
 30 13.8902 1.14749E-03
 30 15.44305 1.12257E-03
 30 17.1155 1.03310E-03
 30 18.9928 1.03788E-03
 30 21.0836 1.05535E-03
 30 23.4272 9.03872E-04
 30 26.0289 8.77824E-04
 30 28.93515 7.22306E-04
 30 32.14305 7.72980E-04
 30 35.704 7.29845E-04
 30 39.9057 5.62530E-04
 30 44.5456 5.65346E-04
 30 49.69945 4.29194E-04
 30 55.3166 4.44138E-04
 30 61.4639 3.47641E-04
 30 68.738 2.76589E-04
 30 76.5866 2.84755E-04
 30 85.07615 1.91980E-04
 30 95.1388 1.59212E-04
 30 107.2117 1.01478E-04
 30 120.145 8.49670E-05
 30 134.01 6.54254E-05
 30 150.63 3.75721E-05
 30 170.8515 1.61220E-05
 30 192.1105 1.91322E-05
 60 5.477085 2.93125E-03
 60 6.06999 2.08544E-03
 60 6.737265 1.33340E-03
 60 7.483335 1.20456E-03
 60 8.32293 9.20724E-04
 60 9.26031 8.55171E-04
 60 10.3137 6.86064E-04
 60 11.4859 5.74860E-04
 60 12.7985 4.86720E-04
 60 14.25045 4.28797E-04
 60 15.8655 3.33571E-04
 60 17.63485 3.65478E-04
 60 19.58175 3.34517E-04
 60 21.8742 2.59998E-04
 60 24.37135 2.79083E-04
 60 27.10095 2.24904E-04
 60 30.32485 1.59099E-04
 60 33.79465 1.74646E-04
 60 37.5345 1.38632E-04
 60 41.94735 1.04981E-04
 60 47.2093 6.69216E-05
 60 52.8062 6.41328E-05
 60 58.7506 5.09715E-05
 60 65.79795 3.42107E-05
 60 74.25065 2.92749E-05
 60 84.5273 1.24286E-05
 60 95.30805 9.45975E-06
 60 106.54125 6.74986E-06
 90 5.35326 1.50582E-03
 90 5.950925 1.09349E-03
 90 6.598485 1.35378E-03
 90 7.32781 7.71720E-04
 90 8.143945 7.65975E-04
 90 9.0634 5.09304E-04
 90 10.091015 4.69855E-04
 90 11.24715 3.33210E-04
 90 12.5351 3.16062E-04
 90 13.97925 2.36374E-04
 90 15.5789 1.93880E-04
 90 17.361 1.47725E-04
 90 19.31635 1.48767E-04
 90 21.47175 1.30628E-04
 90 24.0146 1.06250E-04
 90 26.78995 1.00763E-04
 90 29.83045 9.25140E-05
 90 33.4303 4.98296E-05
 90 37.3147 4.87863E-05
 90 41.5135 3.39078E-05
 90 46.4832 2.59039E-05
 90 52.4306 1.43801E-05
 90 58.78005 1.13615E-05
 90 65.5527 7.89835E-06
 90 73.6188 3.25640E-06
 90 83.3458 2.61930E-06
 90 93.46825 1.04873E-06
 \END;
 /*===================================================================*/