ENTRY 32731 20191011 31923273100000001 SUBENT 32731001 20191011 31923273100100001 BIB 13 41 3273100100002 TITLE Experimental measurements with Monte Carlo correction 3273100100003 and theoretical calculations of neutron inelastic 3273100100004 scattering cross section of 115In 3273100100005 AUTHOR (Chao Wang,Jun Xiao,Xiaobing Luo) 3273100100006 INSTITUTE (3CPRSIU,3CPRNPC) 3273100100007 REFERENCE (J,RPC,127,177,2016) 3273100100008 FACILITY (VDGT,3CPRSIU) 2.5 MeV electrostatic accelerator 3273100100009 INC-SOURCE (D-D) The deuteron beam current of 300 mA and beam 3273100100010 energy of 2.0 MeV. The solid Tritium-Ti target had a 3273100100011 thickness of approximately 1.20 mg/cm2. 3273100100012 SAMPLE (49-IN-115,NAT=0.957) The 115In samples were pure 3273100100013 indium with a purity of higher than 99.99%. Disks of 3273100100014 pure indium, 0.5 mm in thickness and 10 mm in 3273100100015 diameter, were sandwiched between two Au foils of 0.3 3273100100016 mm in thickness. These foils were wrapped with 0.3 mm 3273100100017 in thickness cadmium box and put into 90 deg angle 3273100100018 relative to the deuteron beam direction. Samples at 3273100100019 the high energy neutron emitting direction between 0 3273100100020 deg and 60 deg, were not sandwiched between the Au 3273100100021 foils. 3273100100022 DETECTOR (HPGE) Well-calibrated coaxial high-purity germanium 3273100100023 detector (GEM30P4-76, ORTEC, USA), with an entrance 3273100100024 window thickness of 1.5 mm, a sensitive volume of 75 3273100100025 cm3 and a sensitive diameter of 60 mm. The detector 3273100100026 has 20% relative efficiency and an energy resolution 3273100100027 of 1.85 keV FWHM at 1.33 MeV. 3273100100028 METHOD (ACTIV) 8-h of irradiation. 3273100100029 CORRECTION Corrections were made for the multiple scattering (S) 3273100100030 and the flux attenuation (F). The total correction 3273100100031 factor was calculated by F = S x D. For 2.95 MeV, 3273100100032 3.94 MeV and 5.24 MeV, S were 1.013, 0.977 and 1.016, 3273100100033 D were 0.960, 0.970 and 0.966, F were 0.973, 0.948 3273100100034 and 0.981. 3273100100035 ERR-ANALYS (ERR-T) total typical uncertainty 2.5% 3273100100036 (ERR-S) Statistics of full energy peak 1.0% 3273100100037 (ERR-1) Detecting efficiency 1.5% 3273100100038 (ERR-2) Standard cross section of Au 1.5% 3273100100039 (ERR-3,,1.0) Decay scheme less than 1.0% 3273100100040 (ERR-4,,1.0) Background neutron less than 1.0% 3273100100041 STATUS (TABLE) Table 4 of Radiat.Phys.Chem.,127,177,2016 3273100100042 HISTORY (20191011C) Compiled by Liu Lile (CNDC) 3273100100043 ENDBIB 41 0 3273100100044 COMMON 3 3 3273100100045 ERR-S ERR-1 ERR-2 3273100100046 PER-CENT PER-CENT PER-CENT 3273100100047 1.0 1.5 1.5 3273100100048 ENDCOMMON 3 0 3273100100049 ENDSUBENT 48 0 3273100199999 SUBENT 32731002 20190101 31923273100200001 BIB 6 11 3273100200002 REACTION (49-IN-115(N,INL)49-IN-115-M,,SIG) 3273100200003 DECAY-DATA (49-IN-115-M,,DG,336.4) 3273100200004 MONITOR (79-AU-197(N,G)79-AU-198,,SIG) 3273100200005 DECAY-MON (79-AU-198,,DG,411.8) 3273100200006 METHOD Neutron flux at 2.95 MeV was determined by using the 3273100200007 198Au activity, while the neutron flux at 3.94 3273100200008 and 5.24 MeV were determined by the 2.95 MeV 198Au 3273100200009 activity and the (d,n) angular differential cross 3273100200010 section ratio. 3273100200011 MISC-COL (MISC1) D(d,n)3He neutron outgoing angle 3273100200012 (MISC2) D(d,n)3He angular differential cross section 3273100200013 ENDBIB 11 0 3273100200014 COMMON 1 3 3273100200015 EN-NRM 3273100200016 MEV 3273100200017 2.95 3273100200018 ENDCOMMON 3 0 3273100200019 DATA 5 3 3273100200020 EN DATA ERR-T MISC1 MISC2 3273100200021 MEV MB MB ADEG MB/SR 3273100200022 2.95 339.3 8.5 90. 5.15 3273100200023 3.94 313.2 7.8 60. 6.84 3273100200024 5.24 327.9 8.2 0. 43.3 3273100200025 ENDDATA 5 0 3273100200026 ENDSUBENT 25 0 3273100299999 ENDENTRY 2 0 3273199999999