ENTRY F0401 20220604 F091F040100000001 SUBENT F0401001 20220604 F091F040100100001 BIB 8 16 F040100100002 TITLE A study of the Be9(He3,n)C11 reaction F040100100003 AUTHOR (L.van der Zwan,A.T.Stewart,J.Y.Park,E.Merzbacher) F040100100004 INSTITUTE (1USANCA) F040100100005 (1CANCAN) Dalhousie University, Halifax, Nova Scotia F040100100006 REFERENCE (J,CJP,41,1036,1963) F040100100007 FACILITY (VDG,1USANCA) 3-MeV F040100100008 SAMPLE The target was a thin layer of beryllium (~16 ug/cm2) F040100100009 evaporated onto a 0.02-in foil of Ta backing F040100100010 DETECTOR (CSICR) CsI scintillator covered by 0.004 inch of F040100100011 aluminium foil for protons F040100100012 (PLATE) the Ilford C-2 emulsions, 1in.x3in.x400 micronsF040100100013 to detect neutrons. (technique of observing proton F040100100014 recoils in photographic emulsions). F040100100015 HISTORY (19870414C) F040100100016 (19990409A) CNPD: corrected 4-dig. year F040100100017 (20220604A) SD: Corrections in all Subents. F040100100018 ENDBIB 16 0 F040100100019 NOCOMMON 0 0 F040100100020 ENDSUBENT 19 0 F040100199999 SUBENT F0401002 20220604 F091F040100200001 BIB 4 5 F040100200002 REACTION (4-BE-9(HE3,N)6-C-11,PAR,DA) F040100200003 ERR-ANALYS (DATA-ERR) No information about source of uncertainty F040100200004 STATUS (CURVE) Figs 3,4 from Canad.J.Phys.,41(1963)1036 F040100200005 HISTORY (20220603A) SD: SF9=EXP deleted from REACTION code. F040100200006 ANG-ERR -> ANG-ERR-D. F040100200007 ENDBIB 5 0 F040100200008 COMMON 2 3 F040100200009 EN ANG-ERR-D F040100200010 MEV ADEG F040100200011 2. 1.5 F040100200012 ENDCOMMON 3 0 F040100200013 DATA 4 42 F040100200014 E-LVL ANG-CM DATA-CM DATA-ERR F040100200015 MEV ADEG MB/SR MB/SR F040100200016 0. 0.6 0.89 0.13 F040100200017 0. 31.8 0.79 0.13 F040100200018 0. 46.3 1.23 0.11 F040100200019 0. 79.0 0.78 0.09 F040100200020 0. 92.6 0.73 0.13 F040100200021 0. 107.7 0.66 0.07 F040100200022 0. 137.3 0.82 0.07 F040100200023 2.01 1.2 0.35 0.07 F040100200024 2.01 30.1 0.53 0.04 F040100200025 2.01 45.3 0.42 0.04 F040100200026 2.01 76.7 0.41 0.07 F040100200027 2.01 93.0 0.57 0.04 F040100200028 2.01 108.2 0.44 0.07 F040100200029 2.01 136.8 0.77 0.04 F040100200030 4.319 2.4 0.16 0.07 F040100200031 4.319 31.8 0.23 0.04 F040100200032 4.319 46.8 0.45 0.09 F040100200033 4.319 78.6 0.31 0.02 F040100200034 4.319 93.5 0.70 0.15 F040100200035 4.319 109.0 0.42 0.07 F040100200036 4.319 138.2 0.37 0.04 F040100200037 4.804 2.6 0.35 0.08 F040100200038 4.804 30.4 0.42 0.08 F040100200039 4.804 47.9 0.69 0.12 F040100200040 4.804 78.6 0.41 0.06 F040100200041 4.804 94.7 0.86 0.16 F040100200042 4.804 109.0 0.43 0.06 F040100200043 4.804 137.0 0.32 0.06 F040100200044 6.34 1.5 2.74 0.32 F040100200045 6.34 31.9 1.75 0.30 F040100200046 6.34 47.6 2.23 0.24 F040100200047 6.34 79.7 1.26 0.21 F040100200048 6.34 95.8 1.48 0.21 F040100200049 6.34 109.4 1.00 0.09 F040100200050 6.34 137.9 0.67 0.08 F040100200051 6.905 2.5 1.11 0.15 F040100200052 6.905 31.8 1.34 0.11 F040100200053 6.905 38.7 1.98 0.15 F040100200054 6.905 82.9 1.57 0.13 F040100200055 6.905 96.7 1.81 0.26 F040100200056 6.905 111.5 1.30 0.19 F040100200057 6.905 141.0 0.46 0.02 F040100200058 ENDDATA 44 0 F040100200059 ENDSUBENT 58 0 F040100299999 ENDENTRY 2 0 F040199999999