ENTRY 23045 20220218 23102304500000001 SUBENT 23045001 20220218 23102304500100001 BIB 16 105 2304500100002 TITLE Production of protons, deuterons, and tritons from 2304500100003 carbon bombarded by 175 MeV quasi mono-energetic 2304500100004 neutrons 2304500100005 AUTHOR (S.Hirayama,Y.Watanabe,M.Hayashi,Y.Naito,R.Bevilacqua, 2304500100006 J.Blomgren,L.Nilsson, A.Oehrn, M.Oesterlund, S.Pomp, 2304500100007 A.Prokofiev, V.Simutkin, P.A.Soederstroem, U.Tippawan) 2304500100008 INSTITUTE (2SWDUPP) 2304500100009 (2JPNKYU) 2304500100010 (3TAICHM) 2304500100011 REFERENCE (J,NSTP,1,69,2011) C data as plots of particle 2304500100012 double-differential yield. 2304500100013 (C,2007NICE,2,1091,2007) First author M.Hayashi. 2304500100014 #doi:10.1051/ndata:07747 2304500100015 (S,JAEA-C-2008-008,62,2008) Two measurements for carbon2304500100016 First author M.Hayashi. Preliminary results. 2304500100017 REL-REF (I,,S.Pomp+,C,2004SANTA,,780,2004) 2304500100018 Details of Uppsala neutron beam facility. 2304500100019 (I,,S.Dangtip+,J,NIM/A,452,484,2000) 2304500100020 Exp. setup of MEDLEY . 2304500100021 (M,,U.Tippawan+,J,PR/C,69,064609,2004) 2304500100022 (M,,U.Tippawan+,J,PR/C,73,034611,2006) 2304500100023 (M,,P.A.Soederstroem,T,Soederstroem,200702) 2304500100024 Three references for data reduction procedure. 2304500100025 SAMPLE Polyethylene (CH2) sample of 25 mm diameter, 1.0 mm 2304500100026 thickness - for absolute cross section normalization. 2304500100027 Instrumental background was measured without samples. 2304500100028 FACILITY (CYCLO,2SWDUPP) Gustav Werner cyclotron. 2304500100029 INC-SOURCE (P-LI7) Enriched 99.99% Li-7 target. 2304500100030 Neutrons transported to MEDLEY chamber through 100-cm 2304500100031 long conical collimator of 54 mm diameter at the end. 2304500100032 Faraday cap - to monitor proton beam current. 2304500100033 Distance from Li target to the center of MEDLEY chamber2304500100034 3.74 m. 2304500100035 INC-SPECT Relative neutron beam intensity was monitored by 2304500100036 integrated proton beam current and by both thin film 2304500100037 breakdown counter and ionization chamber . 2304500100038 1 98.5 MeV protons produce neutrons with peak energy 2304500100039 94 MeV using lithium target of 8 mm thick. 2304500100040 Neutron flux 3.1E+5 n/(cm**2*sec), proton beam 2304500100041 intensity of 3.4 microA. 2304500100042 2 180 MeV protons produce neutrons with peak energy of 2304500100043 175 MeV using 23.5 mm thick Li target. 2304500100044 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500100045 intensity 0.3 microA. 2304500100046 Measured (from data analysis of recoil protons from np 2304500100047 scattering in CH2 measurement) and calculated incident 2304500100048 neutron spectrum is presented on Fig.7 of C,2007NICE. 2304500100049 METHOD (EDE) deltaE - E technique. 2304500100050 (TOF) Used to reject the tail neutrons produced in Li 2304500100051 target. 2304500100052 DETECTOR (TELES,SIBAR,CSICR) MEDLEY consists of eight 2304500100053 three-element telescopes mounted inside vacuum chamber 2304500100054 of 90 cm diameter.Each telescope consists of two fully 2304500100055 depleted silicon surface barrier detectors ( first of 2304500100056 thickness 50-60 microm, 23.9 mm diameter, second - 2304500100057 400-600 microm, 23.9 mm diameter) 2304500100058 serving as deltaE detector and CsI(Tl) scintillator 2304500100059 100 mm total length, cylindrical shape of 50 mm 2304500100060 diameter; last 30 mm are tapered to 18 mm diameter to 2304500100061 match size of Hamamatsu S3204-08 photodiode, serving as2304500100062 E detector. 2304500100063 Energy calibration of detectors was obtained using the 2304500100064 data themselves. 2304500100065 MONITOR (1-H-1(N,EL)1-H-1,,DA) For neutron spectrum, using CH2 2304500100066 target and kinematics calculation. 2304500100067 n,p scattering c-s were taken from NN-online SAID: 2304500100068 SAID Nucleon-Nucleon scattering database - 2304500100069 http://gwdac.phys.gwu.edu/ 2304500100070 ANALYSIS Events in deltaE-E bands were fitted with respect to 2304500100071 the energy deposited in two deltaE detectors, which was2304500100072 determined from thickness and energy loses calculated 2304500100073 by SRIM code. 2304500100074 Measured TOF data were used for selection of light-ion 2304500100075 events induced by neutrons in the main peak of source 2304500100076 neutron spectrum. 2304500100077 Number of net counts due to np scattering was obtained 2304500100078 using measurements of the (n,P) spectrum at 20 degrees 2304500100079 for both samples -CH2 and C. 2304500100080 Absolute values of c-s were determined using reference 2304500100081 np cross section in the same method as in REL-REFs of 2304500100082 U.Tippawan+. The np scattering cross sections from 2304500100083 NN-online of SAID Nucleon-Nucleon scattering database. 2304500100084 http://gwdac.phys.gwu.edu - G.Washington Un., USA. 2304500100085 CORRECTION Background was subtracted after normalization to the 2304500100086 same neutron fluence. 2304500100087 For finite efficiency of CsI(Tl) scintillator by Monte 2304500100088 Carlo simulation method. 2304500100089 For the finite target thickness by method of REL-REF 2304500100090 U.Tippawan+,J,PR/C,69 -not applied for 175 MeV . 2304500100091 It was assumed that target is treated as a point source2304500100092 -it was confirmed by comparison of PHITS simulation 2304500100093 between a point source and a plane source, in which the2304500100094 difference is only 1.%. 2304500100095 STATUS (UNOBT) Request for the data was sent 03.07.2009 to 2304500100096 Y.Watanabe (Subents 002-006) 2304500100097 HISTORY (20090702C) M.M. 2304500100098 (20110715A) M.M. Ref. J,NSTP,1,69,2011 was added. 2304500100099 Authors' names were added. BIB information was added. 2304500100100 Subents 007-009 were added. 2304500100101 Request of data was sent to author Shusuke Hirayama 2304500100102 hirayama@aees.kyushu-u.ac.jp 18-07-2011. 2304500100103 (20130203A) SD: Headings and units to col. 3 were 2304500100104 added in Subents 5,6. Title corrected according to 2304500100105 first ref. 2304500100106 (20220218U) SD: JAEA-C-2008-08,62 -> JAEA-C-2008-008,622304500100107 ENDBIB 105 0 2304500100108 COMMON 1 3 2304500100109 ANG-NRM 2304500100110 ADEG 2304500100111 20. 2304500100112 ENDCOMMON 3 0 2304500100113 ENDSUBENT 112 0 2304500199999 SUBENT 23045002 20090624 22142304500200001 BIB 6 15 2304500200002 REACTION (20-CA-0(N,X)1-H-1,,DA/DE) 2304500200003 SAMPLE Calcium sample of 29 mm diameter, 230 microm thickness.2304500200004 INC-SPECT Relative neutron beam intensity was monitored by 2304500200005 integrated proton beam current and by both thin film 2304500200006 breakdown counter and ionization chamber . 2304500200007 98.5 MeV protons produce neutrons with peak energy 2304500200008 94 MeV using lithium target of 8 mm thick. 2304500200009 Neutron flux 3.1E+5 n/(cm**2*sec), proton beam 2304500200010 intensity of 3.4 microA. 2304500200011 ANALYSIS Detail of data analysis and model calculation - see 2304500200012 REL-REF of P.A.Soederstroem . 2304500200013 ERR-ANALYS (E-ERR-DIG) Digitizing error of E . 2304500200014 (ERR-DIG) Digitizing error of DATA . 2304500200015 (DATA-ERR) Error bar for DATA. 2304500200016 STATUS (CURVE) Fig.6 of C,2007NICE. 2304500200017 ENDBIB 15 0 2304500200018 COMMON 3 3 2304500200019 EN E-ERR-DIG ERR-DIG 2304500200020 MEV MEV PER-CENT 2304500200021 94. 0.11 0.0062 2304500200022 ENDCOMMON 3 0 2304500200023 DATA 4 157 2304500200024 ANG E DATA DATA-ERR 2304500200025 ADEG MEV MB/SR/MEV MB/SR/MEV 2304500200026 20. 2.64 0.0580 0.245 2304500200027 20. 3.59 5.674 2304500200028 20. 5.51 7.814 2304500200029 20. 6.71 6.660 2304500200030 20. 7.43 5.103 2304500200031 20. 8.63 3.910 2304500200032 20. 9.59 3.515 2304500200033 20. 10.79 2.694 2304500200034 20. 12.96 2.555 0.490 2304500200035 20. 15.12 1.668 0.456 2304500200036 20. 16.80 1.857 0.441 2304500200037 20. 18.72 1.279 0.528 2304500200038 20. 21.61 1.670 0.390 2304500200039 20. 25.93 1.280 0.444 2304500200040 20. 30.01 1.215 0.421 2304500200041 20. 33.86 1.765 0.549 2304500200042 20. 37.94 1.587 0.494 2304500200043 20. 41.78 1.767 0.550 2304500200044 20. 45.87 1.768 0.550 2304500200045 20. 49.95 1.677 0.459 2304500200046 20. 53.79 1.867 0.510 2304500200047 20. 57.88 1.771 0.414 2304500200048 20. 61.00 1.869 0.358 2304500200049 20. 62.68 1.972 0.378 2304500200050 20. 64.84 2.194 0.513 2304500200051 20. 67.01 2.315 0.541 2304500200052 20. 68.93 2.316 2304500200053 20. 70.85 1.872 2304500200054 20. 73.01 1.683 2304500200055 20. 74.94 1.099 0.300 2304500200056 20. 76.86 1.597 2304500200057 20. 79.02 0.718 0.223 2304500200058 20. 80.46 3.028 2304500200059 20. 81.42 2.086 2304500200060 20. 82.38 0.758 0.263 2304500200061 20. 83.58 1.515 2304500200062 20. 84.54 1.044 0.285 2304500200063 20. 85.50 1.292 2304500200064 20. 86.23 1.101 2304500200065 20. 87.19 0.890 0.243 2304500200066 20. 88.39 0.800 2304500200067 20. 89.35 0.445 0.183 2304500200068 20. 90.55 0.551 0.130 2304500200069 20. 91.51 0.469 0.163 2304500200070 20. 92.47 0.890 2304500200071 20. 93.68 0.341 0.154 2304500200072 20. 94.39 0.891 2304500200073 20. 95.60 0.400 0.124 2304500200074 20. 96.32 0.400 0.093 2304500200075 20. 98.50 0.00481 0.00464 2304500200076 20. 99.21 0.02381 0.12988 2304500200077 40. 2.64 4.891 2.692 2304500200078 40. 3.60 6.735 2304500200079 40. 4.32 3.953 2304500200080 40. 5.28 8.336 2304500200081 40. 6.00 6.056 2304500200082 40. 7.20 4.640 2304500200083 40. 8.40 3.956 2304500200084 40. 9.36 3.556 2304500200085 40. 10.81 2.584 2304500200086 40. 12.73 1.877 0.439 2304500200087 40. 14.89 1.439 0.499 2304500200088 40. 16.81 1.601 0.498 2304500200089 40. 18.98 1.103 0.420 2304500200090 40. 21.86 0.940 0.219 2304500200091 40. 25.94 1.295 0.302 2304500200092 40. 29.79 1.165 0.318 2304500200093 40. 33.87 1.105 0.383 2304500200094 40. 37.71 .9426 0.293 2304500200095 40. 41.80 .7226 0.275 2304500200096 40. 45.88 .9954 0.345 2304500200097 40. 49.73 .8048 0.250 2304500200098 40. 54.05 .7636 0.315 2304500200099 40. 57.89 .7244 0.275 2304500200100 40. 60.78 .9459 0.360 2304500200101 40. 62.94 .7249 0.251 2304500200102 40. 64.86 .6518 0.202 2304500200103 40. 67.02 .6182 0.192 2304500200104 40. 68.94 .7256 0.225 2304500200105 40. 71.10 .8982 0.210 2304500200106 40. 72.79 .9476 0.181 2304500200107 40. 74.95 .4496 0.199 2304500200108 40. 76.87 .8523 0.233 2304500200109 40. 79.03 .4745 0.195 2304500200110 40. 80.48 .4266 0.176 2304500200111 40. 81.44 .7269 0.226 2304500200112 40. 82.40 .3448 0.162 2304500200113 40. 83.36 .0910 0.134 2304500200114 40. 84.32 .6895 0.161 2304500200115 40. 85.28 .5877 0.137 2304500200116 40. 86.24 .3838 0.133 2304500200117 40. 87.44 .4271 0.148 2304500200118 40. 88.41 .0776 0.114 2304500200119 40. 89.37 .2254 0.124 2304500200120 40. 90.33 .2789 0.106 2304500200121 40. 91.29 .4507 0.123 2304500200122 40. 92.25 .1822 0.068 2304500200123 40. 93.45 .3105 0.107 2304500200124 40. 94.42 .0166 0.069 2304500200125 40. 95.37 .3843 0.089 2304500200126 40. 96.57 .3276 0.089 2304500200127 40. 98.26 .0778 0.077 2304500200128 40. 99.22 .1071 0.040 2304500200129 140. 2.66 0.0409 0.1409 2304500200130 140. 3.37 3.231 0.756 2304500200131 140. 4.57 2.347 0.451 2304500200132 140. 5.29 5.506 0.814 2304500200133 140. 6.25 4.219 0.426 2304500200134 140. 7.45 2.906 0.429 2304500200135 140. 8.41 2.477 0.579 2304500200136 140. 9.61 2.349 0.549 2304500200137 140. 11.06 1.379 0.265 2304500200138 140. 12.98 0.7676 0.1795 2304500200139 140. 14.90 0.6902 0.2395 2304500200140 140. 16.82 0.5015 0.2071 2304500200141 140. 18.75 0.1923 0.1145 2304500200142 140. 21.87 0.2946 0.1392 2304500200143 140. 25.96 0.0963 0.0695 2304500200144 140. 30.04 0.1130 0.1012 2304500200145 140. 33.89 0.0482 0.0482 2304500200146 140. 37.97 0.0121 0.0194 2304500200147 140. 42.06 0.0463 0.0120 2304500200148 140. 49.99 0.0121 0.0230 2304500200149 140. 54.07 0.0218 0.0381 2304500200150 140. 57.91 0.0255 0.0486 2304500200151 140. 60.80 0.0027 0.0027 2304500200152 140. 62.96 0.0167 0.0246 2304500200153 140. 64.87 0.0568 0.0156 2304500200154 140. 66.80 0.0352 0.0145 2304500200155 140. 68.96 0.0969 0.0143 2304500200156 140. 70.88 0.0285 0.0151 2304500200157 160. 2.90 0.0920 2304500200158 160. 3.37 4.044 0.776 2304500200159 160. 4.57 4.045 0.946 2304500200160 160. 5.29 4.500 0.864 2304500200161 160. 6.49 2.939 0.434 2304500200162 160. 7.46 2.787 0.535 2304500200163 160. 8.42 2.506 0.481 2304500200164 160. 9.62 1.920 0.369 2304500200165 160. 10.82 1.127 0.216 2304500200166 160. 12.75 0.6617 0.1811 2304500200167 160. 14.91 0.4808 0.1669 2304500200168 160. 17.07 0.4560 0.1718 2304500200169 160. 18.99 0.2677 0.1595 2304500200170 160. 21.88 0.1572 0.0826 2304500200171 160. 25.96 0.1205 0.0851 2304500200172 160. 30.05 0.0974 0.0895 2304500200173 160. 33.89 0.1342 0.1488 2304500200174 160. 37.98 0.09250 0.12446 2304500200175 160. 42.07 0.00936 0.02252 2304500200176 160. 45.91 0.01223 0.02726 2304500200177 160. 61.04 0.05165 0.08313 2304500200178 160. 62.96 0.04404 0.07087 2304500200179 160. 65.12 0.1422 0.0333 2304500200180 160. 67.04 0.1501 0.0288 2304500200181 160. 68.96 0.2558 0.0258 2304500200182 160. 71.12 0.2300 0.1370 2304500200183 ENDDATA 159 0 2304500200184 ENDSUBENT 183 0 2304500299999 SUBENT 23045003 20090624 22142304500300001 BIB 5 18 2304500300002 REACTION (6-C-0(N,X)1-H-1,,DA/DE) 2304500300003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500300004 INC-SPECT Relative neutron beam intensity was monitored by 2304500300005 integrated proton beam current and by both thin film 2304500300006 breakdown counter and ionization chamber . 2304500300007 178.7 MeV protons produce neutrons with peak energy of2304500300008 174.3 MeV using 23.5 mm thick Li target. 2304500300009 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500300010 intensity 0.3 microA. 2304500300011 Measured (from data analysis of recoil protons from np 2304500300012 scattering in CH2 measurement) and calculated incident 2304500300013 neutron spectrum is presented on Fig.7 of C,2007NICE, 2304500300014 Fig.5 of S,JAEA-C-2008-008. 2304500300015 Effective beam time 15hours. Neutron flight path 374cm.2304500300016 ANALYSIS Detail of data analysis and model calculation - see 2304500300017 REL-REF of P.A.Soederstroem . 2304500300018 STATUS (PRELM) Fig.8 of C,2007NICE . 2304500300019 (CURVE) Fig.6 of S,JAEA-C-2008-8 , Exp. I . 2304500300020 ENDBIB 18 0 2304500300021 COMMON 4 3 2304500300022 EN ANG E-ERR-DIG ERR-DIG 2304500300023 MEV ADEG MEV PER-CENT 2304500300024 175. 20. 0.26822 0.10905E-01 2304500300025 ENDCOMMON 3 0 2304500300026 DATA 3 30 2304500300027 E DATA DATA-ERR 2304500300028 MEV MB/SR/MEV MB/SR/MEV 2304500300029 22.066 0.96356 0.11421 2304500300030 26.937 1.0045 0.10025 2304500300031 32.295 1.0694 0.86268E-01 2304500300032 37.165 1.1148 0.11126 2304500300033 42.024 0.92219 0.10931 2304500300034 46.899 1.0457 0.63974E-01 2304500300035 51.762 0.94094 0.75907E-01 2304500300036 57.114 0.88298 0.77524E-01 2304500300037 61.967 0.64383 0.71379E-01 2304500300038 66.837 0.67119 0.67012E-01 2304500300039 72.198 0.76107 0.75924E-01 2304500300040 77.071 0.82748 0.53882E-01 2304500300041 81.933 0.72907 0.63976E-01 2304500300042 86.800 0.71358 0.79147E-01 2304500300043 91.669 0.72842 0.80720E-01 2304500300044 97.011 0.55392 0.75796E-01 2304500300045 101.89 0.68324 0.80987E-01 2304500300046 106.76 0.66873 0.53947E-01 2304500300047 111.63 0.79089 0.69400E-01 2304500300048 116.49 0.64061 0.51679E-01 2304500300049 121.85 0.68199 0.55017E-01 2304500300050 126.72 0.72608 0.47279E-01 2304500300051 131.58 0.57588 0.57473E-01 2304500300052 136.92 0.48648 0.57663E-01 2304500300053 141.79 0.49659 0.43576E-01 2304500300054 146.64 0.29343 0.40162E-01 2304500300055 151.99 0.29328 0.34763E-01 2304500300056 156.86 0.29315 0.34748E-01 2304500300057 162.16 0.10026 0.26098E-01 2304500300058 166.93 0.13884E-010.72585E-02 2304500300059 ENDDATA 32 0 2304500300060 ENDSUBENT 59 0 2304500399999 SUBENT 23045004 20090624 22142304500400001 BIB 5 18 2304500400002 REACTION (6-C-0(N,X)1-H-1,,DA/DE) 2304500400003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500400004 INC-SPECT Relative neutron beam intensity was monitored by 2304500400005 integrated proton beam current and by both thin film 2304500400006 breakdown counter and ionization chamber . 2304500400007 178.7 MeV protons produce neutrons with peak energy of2304500400008 174.3 MeV using 23.5 mm thick Li target. 2304500400009 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500400010 intensity 0.3 microA. 2304500400011 Measured (from data analysis of recoil protons from np 2304500400012 scattering in CH2 measurement) and calculated incident 2304500400013 neutron spectrum is presented on Fig.7 of C,2007NICE, 2304500400014 Fig.5 of S,JAEA-C-2008-008. 2304500400015 Effective beam time 15hours. Neutron flight path 374cm.2304500400016 ANALYSIS Detail of data analysis and model calculation - see 2304500400017 REL-REF of P.A.Soederstroem . 2304500400018 STATUS (PRELM) 2304500400019 (CURVE) Fig.6 of S,JAEA-C-2008-8 , EXP. I . 2304500400020 ENDBIB 18 0 2304500400021 COMMON 4 3 2304500400022 EN ANG E-ERR-DIG ERR-DIG 2304500400023 MEV ADEG MEV PER-CENT 2304500400024 175. 40. 0.18665 0.96923E-02 2304500400025 ENDCOMMON 3 0 2304500400026 DATA 3 30 2304500400027 E DATA DATA-ERR 2304500400028 MEV MB/SR/MEV MB/SR/MEV 2304500400029 22.560 0.66742 0.58567E-01 2304500400030 27.386 0.42012 0.46577E-01 2304500400031 32.227 0.42893 0.47540E-01 2304500400032 37.554 0.46642 0.40929E-01 2304500400033 42.378 0.27565 0.50498E-01 2304500400034 47.227 0.37776 0.41881E-01 2304500400035 52.555 0.41951 0.36812E-01 2304500400036 57.390 0.35446 0.39297E-01 2304500400037 62.220 0.25850 0.44571E-01 2304500400038 67.551 0.32567 0.28588E-01 2304500400039 72.390 0.31218 0.42729E-01 2304500400040 77.223 0.24764 0.42699E-01 2304500400041 82.539 0.19235 0.36479E-01 2304500400042 87.386 0.23730 0.36743E-01 2304500400043 91.743 0.24744 0.33874E-01 2304500400044 97.547 0.21803 0.33754E-01 2304500400045 102.38 0.18814 0.29130E-01 2304500400046 107.22 0.19616 0.30373E-01 2304500400047 112.53 0.11593 0.27725E-01 2304500400048 116.88 0.90050E-010.24360E-01 2304500400049 122.20 0.81039E-010.23152E-01 2304500400050 127.04 0.67047E-010.20152E-01 2304500400051 132.36 0.72908E-010.18591E-01 2304500400052 136.72 0.89948E-010.18577E-01 2304500400053 142.05 0.80947E-010.18054E-01 2304500400054 146.88 0.64213E-010.14320E-01 2304500400055 152.17 0.20194E-010.10557E-01 2304500400056 157.47 0.11685E-010.10740E-01 2304500400057 162.33 0.20182E-010.63447E-02 2304500400058 172.97 0.12699E-010.58435E-02 2304500400059 ENDDATA 32 0 2304500400060 ENDSUBENT 59 0 2304500499999 SUBENT 23045005 20130203 22342304500500001 BIB 8 26 2304500500002 REACTION (6-C-0(N,X)1-H-1,,DA/DE) 2304500500003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500500004 INC-SPECT Neutron beam line was reinforced by installing an 2304500500005 additional iron shielding (wall of 50 cm thickness, 2304500500006 placed in front of MEDLEY) to reduce background 2304500500007 neutrons. 2304500500008 Relative neutron beam intensity was monitored by 2304500500009 integrated proton beam current and by both thin film 2304500500010 breakdown counter and ionization chamber . 2304500500011 179.3 MeV protons produce neutrons with peak energy of 2304500500012 174.9 MeV using 23.5 mm thick Li target. 2304500500013 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500500014 intensity 0.3 microA. 2304500500015 Effective beam time 30hours. Neutron flight path 460cm.2304500500016 Measured (from data analysis of recoil protons from np 2304500500017 scattering in CH2 measurement) and calculated incident 2304500500018 neutron spectrum is presented on Fig.5 of 2304500500019 S,JAEA-C-2008-008 2304500500020 DETECTOR DeltaE detectors of 50 microm thickness were replaced2304500500021 by those of 1000 microm . 2304500500022 ANALYSIS Detail of data analysis and model calculation - see 2304500500023 REL-REF of P.A.Soederstroem. 2304500500024 ERR-ANALYS (DATA-ERR) Experimental error 2304500500025 STATUS (PRELM) Fig.6 of S,JAEA-C-2008-008, Exp II. 2304500500026 (CURVE) 2304500500027 HISTORY (20130203A) SD: Headings and units to col. 3 were added2304500500028 ENDBIB 26 0 2304500500029 COMMON 4 3 2304500500030 EN ANG E-ERR-DIG ERR-DIG 2304500500031 MEV ADEG MEV PER-CENT 2304500500032 175. 20. 0.26822 0.10905E-01 2304500500033 ENDCOMMON 3 0 2304500500034 DATA 3 32 2304500500035 E DATA DATA-ERR 2304500500036 MEV MB/SR/MEV MB/SR/MEV 2304500500037 22.532 0.61956 0.98249E-01 2304500500038 26.922 0.74834 0.12903 2304500500039 32.281 0.79667 0.10904 2304500500040 37.141 0.67302 0.12763 2304500500041 42.013 0.73175 0.10016 2304500500042 47.365 0.68668 0.11840 2304500500043 51.744 0.65813 0.12483 2304500500044 57.105 0.73074 0.12599 2304500500045 61.967 0.64383 0.99687E-01 2304500500046 66.841 0.73008 0.11578 2304500500047 72.198 0.76107 0.10414 2304500500048 77.064 0.72940 0.11294 2304500500049 82.406 0.55467 0.95595E-01 2304500500050 86.800 0.71358 0.97698E-01 2304500500051 92.149 0.62869 0.97343E-01 2304500500052 97.022 0.69808 0.93871E-01 2304500500053 101.89 0.72773 0.63859E-01 2304500500054 106.76 0.71227 0.78966E-01 2304500500055 111.62 0.65452 0.89587E-01 2304500500056 116.50 0.69683 0.77219E-01 2304500500057 121.85 0.72640 0.63742E-01 2304500500058 126.72 0.69617 0.82519E-01 2304500500059 132.07 0.65329 0.72427E-01 2304500500060 136.44 0.55192 0.61161E-01 2304500500061 141.31 0.48628 0.53887E-01 2304500500062 146.65 0.35456 0.64955E-01 2304500500063 152.00 0.35438 0.56198E-01 2304500500064 156.86 0.31224 0.57202E-01 2304500500065 161.67 0.92177E-010.26452E-01 2304500500066 166.98 0.33578E-010.25664E-01 2304500500067 171.81 0.16769E-010.10430E-01 2304500500068 182.01 0.11235E-010.90082E-02 2304500500069 ENDDATA 34 0 2304500500070 ENDSUBENT 69 0 2304500599999 SUBENT 23045006 20130203 22342304500600001 BIB 8 26 2304500600002 REACTION (6-C-0(N,X)1-H-1,,DA/DE) 2304500600003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500600004 INC-SPECT Neutron beam line was reinforced by installing an 2304500600005 additional iron shielding (wall of 50 cm thickness, 2304500600006 placed in front of MEDLEY) to reduce background 2304500600007 neutrons. 2304500600008 Relative neutron beam intensity was monitored by 2304500600009 integrated proton beam current and by both thin film 2304500600010 breakdown counter and ionization chamber . 2304500600011 179.3 MeV protons produce neutrons with peak energy of 2304500600012 174.9 MeV using 23.5 mm thick Li target. 2304500600013 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500600014 intensity 0.3 microA. 2304500600015 Effective beam time 30hours. Neutron flight path 460cm.2304500600016 Measured (from data analysis of recoil protons from np 2304500600017 scattering in CH2 measurement) and calculated incident 2304500600018 neutron spectrum is presented on Fig.5 of 2304500600019 S,JAEA-C-2008-008 2304500600020 DETECTOR DeltaE detectors of 50 microm thickness were replaced2304500600021 by those of 1000 microm . 2304500600022 ANALYSIS Detail of data analysis and model calculation - see 2304500600023 REL-REF of P.A.Soederstroem . 2304500600024 STATUS (PRELM) Fig.6 of S,JAEA-C-2008-008, Exp. II . 2304500600025 (CURVE) 2304500600026 ERR-ANALYS (DATA-ERR) Experimental error 2304500600027 HISTORY (20130203A) SD: Headings and units to col. 3 were added2304500600028 ENDBIB 26 0 2304500600029 COMMON 4 3 2304500600030 EN ANG E-ERR-DIG ERR-DIG 2304500600031 MEV ADEG MEV PER-CENT 2304500600032 175. 40. 0.18665 0.96923E-02 2304500600033 ENDCOMMON 3 0 2304500600034 DATA 3 29 2304500600035 E DATA DATA-ERR 2304500600036 MEV MB/SR/MEV MB/SR/MEV 2304500600037 22.544 0.38633 0.33913E-01 2304500600038 27.383 0.37819 0.37744E-01 2304500600039 32.223 0.37022 0.43892E-01 2304500600040 37.063 0.37798 0.51745E-01 2304500600041 42.389 0.40247 0.35317E-01 2304500600042 47.709 0.34728 0.47533E-01 2304500600043 52.068 0.38568 0.45716E-01 2304500600044 56.904 0.33280 0.45560E-01 2304500600045 62.227 0.32577 0.36117E-01 2304500600046 67.065 0.29941 0.40982E-01 2304500600047 72.393 0.34679 0.46633E-01 2304500600048 77.223 0.24764 0.33301E-01 2304500600049 82.068 0.29293 0.32476E-01 2304500600050 86.904 0.25814 0.40927E-01 2304500600051 92.227 0.24743 0.33272E-01 2304500600052 97.067 0.24736 0.27424E-01 2304500600053 102.39 0.23710 0.26294E-01 2304500600054 107.22 0.20033 0.22210E-01 2304500600055 112.06 0.17287 0.31675E-01 2304500600056 116.90 0.15233 0.20485E-01 2304500600057 121.74 0.14912 0.23643E-01 2304500600058 127.06 0.13420 0.21281E-01 2304500600059 131.89 0.10207 0.16190E-01 2304500600060 137.21 0.10204 0.21263E-01 2304500600061 142.05 0.80947E-010.18943E-01 2304500600062 146.88 0.64213E-010.15027E-01 2304500600063 151.71 0.48841E-010.12711E-01 2304500600064 157.04 0.61533E-010.12820E-01 2304500600065 162.36 0.53094E-010.13819E-01 2304500600066 ENDDATA 31 0 2304500600067 ENDSUBENT 66 0 2304500699999 SUBENT 23045007 20110715 22282304500700001 BIB 6 23 2304500700002 REACTION (6-C-0(N,X)1-H-1,,PY/DA/DE) 2304500700003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500700004 INC-SPECT Neutron beam line was reinforced by installing an 2304500700005 additional iron shielding (wall of 50 cm thickness, 2304500700006 placed in front of MEDLEY) to reduce background 2304500700007 neutrons. 2304500700008 Relative neutron beam intensity was monitored by 2304500700009 integrated proton beam current and by both thin film 2304500700010 breakdown counter and ionization chamber . 2304500700011 179.3 MeV protons produce neutrons with peak energy of 2304500700012 174.9 MeV using 23.5 mm thick Li target. 2304500700013 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500700014 intensity 0.3 microA. 2304500700015 Effective beam time 30hours. Neutron flight path 460cm.2304500700016 Measured (from data analysis of recoil protons from np 2304500700017 scattering in CH2 measurement) and calculated incident 2304500700018 neutron spectrum is presented on Fig.3 of 2304500700019 J,NSTP,1,69,2011. 2304500700020 DETECTOR DeltaE detectors of 50 microm thickness were replaced2304500700021 by those of 1000 microm . 2304500700022 ADD-RES (COMP) Compared with calculations of JENDL/HE2007, QMD,2304500700023 INC models. 2304500700024 STATUS Fig.4 of J,NSTP,1,69,2011 -20,60,100,140 deg. 2304500700025 ENDBIB 23 0 2304500700026 COMMON 1 3 2304500700027 EN 2304500700028 MEV 2304500700029 175. 2304500700030 ENDCOMMON 3 0 2304500700031 NODATA 0 0 2304500700032 ENDSUBENT 31 0 2304500799999 SUBENT 23045008 20110715 22282304500800001 BIB 6 23 2304500800002 REACTION (6-C-0(N,X)1-H-2,,PY/DA/DE) 2304500800003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500800004 INC-SPECT Neutron beam line was reinforced by installing an 2304500800005 additional iron shielding (wall of 50 cm thickness, 2304500800006 placed in front of MEDLEY) to reduce background 2304500800007 neutrons. 2304500800008 Relative neutron beam intensity was monitored by 2304500800009 integrated proton beam current and by both thin film 2304500800010 breakdown counter and ionization chamber . 2304500800011 179.3 MeV protons produce neutrons with peak energy of 2304500800012 174.9 MeV using 23.5 mm thick Li target. 2304500800013 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500800014 intensity 0.3 microA. 2304500800015 Effective beam time 30hours. Neutron flight path 460cm.2304500800016 Measured (from data analysis of recoil protons from np 2304500800017 scattering in CH2 measurement) and calculated incident 2304500800018 neutron spectrum is presented on Fig.3 of 2304500800019 J,NSTP,1,69,2011. 2304500800020 DETECTOR DeltaE detectors of 50 microm thickness were replaced2304500800021 by those of 1000 microm . 2304500800022 ADD-RES (COMP) Compared with calculations of JENDL/HE2007, 2304500800023 QMD model. 2304500800024 STATUS Fig.5 of J,NSTP,1,69,2011 -20,40,60,80 deg. 2304500800025 ENDBIB 23 0 2304500800026 COMMON 1 3 2304500800027 EN 2304500800028 MEV 2304500800029 175. 2304500800030 ENDCOMMON 3 0 2304500800031 NODATA 0 0 2304500800032 ENDSUBENT 31 0 2304500899999 SUBENT 23045009 20110715 22282304500900001 BIB 6 23 2304500900002 REACTION (6-C-0(N,X)1-H-2,,PY/DA/DE) 2304500900003 SAMPLE Carbon sample of 22 mm diameter, 1.0 mm thickness. 2304500900004 INC-SPECT Neutron beam line was reinforced by installing an 2304500900005 additional iron shielding (wall of 50 cm thickness, 2304500900006 placed in front of MEDLEY) to reduce background 2304500900007 neutrons. 2304500900008 Relative neutron beam intensity was monitored by 2304500900009 integrated proton beam current and by both thin film 2304500900010 breakdown counter and ionization chamber . 2304500900011 179.3 MeV protons produce neutrons with peak energy of 2304500900012 174.9 MeV using 23.5 mm thick Li target. 2304500900013 Neutron flux 4.3E+4 n/(cm**2*sec), proton beam 2304500900014 intensity 0.3 microA. 2304500900015 Effective beam time 30hours. Neutron flight path 460cm.2304500900016 Measured (from data analysis of recoil protons from np 2304500900017 scattering in CH2 measurement) and calculated incident 2304500900018 neutron spectrum is presented on Fig.3 of 2304500900019 J,NSTP,1,69,2011. 2304500900020 DETECTOR DeltaE detectors of 50 microm thickness were replaced2304500900021 by those of 1000 microm . 2304500900022 ADD-RES (COMP) Compared with calculations of JENDL/HE2007, 2304500900023 QMD model. 2304500900024 STATUS Fig.6 of J,NSTP,1,69,2011 -20,40,60,80 deg. 2304500900025 ENDBIB 23 0 2304500900026 COMMON 1 3 2304500900027 EN 2304500900028 MEV 2304500900029 175. 2304500900030 ENDCOMMON 3 0 2304500900031 NODATA 0 0 2304500900032 ENDSUBENT 31 0 2304500999999 ENDENTRY 9 0 2304599999999