ENTRY O1305 20090814 O040O130500000001 SUBENT O1305001 20090814 O040O130500100001 BIB 13 64 O130500100002 TITLE Charged-particle evaporation and pre-equilibrium O130500100003 emission in 1.2 GeV proton-induced spallation reactionsO130500100004 REFERENCE (J,NP/A,765,426,2006) O130500100005 AUTHOR (C.-M.Herbach, D.Hilscher, U.Jahnke, V.G.Tishchenko, O130500100006 J.Galin, A.Letourneau, A.Peghaire, D.Filges, O130500100007 F.Goldenbaum, L.Pienkowski, W.U.Schroeder, J.Toke) O130500100008 INSTITUTE (2GERBER,2GERJUL,2FR GAN,1USAROC) O130500100009 (3POLWWA) Heavy Ion Laboratory. O130500100010 REL-REF (R,O0678001,M.ENKE+,J,NP/A,657,317,1999) O130500100011 (R,O0277001,R.MICHEL+,J,NIM/B,103,183,1995) O130500100012 (R,O0839001,I.LEYA+,J,NIM/B,229,1,2005) O130500100013 Experimental data from the publications were used O130500100014 for a comparison with presented data. O130500100015 The results of Enke+ have been corrected for a reduced O130500100016 geometrical efficiency of ~7.7%, for counting losses O130500100017 due to double hits, and for lower energy cut-offs by O130500100018 (R,,C.-M.HERBACH+,J,NIM/A,508,315,2003). The paper and O130500100019 (R,,U.JAHNKE+,J,NIM/A,508,295,2003) Contain detailed O130500100020 description of the NESSI detector. O130500100021 SAMPLE The targets of natural isotopic composition used in theO130500100022 present experiments were self-supporting metallic filmsO130500100023 of 1-10 mg/cm2 thickness, prepared by mechanical O130500100024 rolling. The layer thicknesses have been determined byO130500100025 weighing and by energy-loss measurements with alpha O130500100026 particles. The non-uniformity has been investigated byO130500100027 energy-loss measurements afar from the target centre. O130500100028 DETECTOR (SPEC) The experiments utilised the 4pi-detector NESSIO130500100029 (NEutron Scintillator tank and SIlicon ball) for an O130500100030 efficient and simultaneous detection of neutrons and O130500100031 charged particles. In addition to the Berlin Neutron O130500100032 Ball (BNB), and the Berlin Silicon Ball (BSiB), the O130500100033 setup has been equipped with six ancillary four-elementO130500100034 detector-telescopes and a set of plastic scintillationO130500100035 detectors for beam diagnostics purposes. O130500100036 For the present experiment six position in the BSIB O130500100037 array, selected at polar angles 30, 2X75, 2X105, and O130500100038 150 degrees, have been equipped with 4-element O130500100039 Si/CsI(Tl) detector telescopes. Each telescope O130500100040 consists of a stack of three delta-e Si detectors with O130500100041 thicknesses of 25-27 mum, 80-90 mum, and approximately O130500100042 1000 mum, backed by a 7-cm thick CsI(Tl) crystal of 4 O130500100043 cm in diameter. O130500100044 FACILITY (SYNCH,2GERGSI) The Cooler Synchrotron Facility COSY. O130500100045 METHOD (EXTB) O130500100046 (TOF) Particle identification with BSiB detectors wasO130500100047 obtained by means of energy and time-of-flight O130500100048 measurements; O130500100049 (EDE) For the Si/CsI(Tl) telescopes. O130500100050 HISTORY (20060203C) By F.Ch. O130500100051 (20090623A).New subentries were added, according O130500100052 N.Otsuka comments. O130500100053 ADD-RES (COMP) Results of simulation calculations with the O130500100054 intra-nuclear cascade code INCL2.0 coupled to the O130500100055 statistical model GEMINI. O130500100056 (ANGD) See figure 4 for example. O130500100057 (E-DIS) See figure 2 for example. O130500100058 CORRECTION The cross sections are corrected for the counting O130500100059 losses below the lower energy threshold of 2 MeV. O130500100060 Used correction for particle identification see in O130500100061 REFERENCE. O130500100062 COMMENT -By authors: O130500100063 1. Product kinetic energies of 0