ENTRY D0369 20120201 D081D036900000001 SUBENT D0369001 20120201 D081D036900100001 BIB 10 15 D036900100002 TITLE Simulations of channeling spectra in the system p+28Si D036900100003 AUTHOR (X.A.Aslanoglou, P.A.Assimakopoulos, M.Kokkoris, D036900100004 E.Kossionides) D036900100005 INSTITUTE (2GRCIOA,2GRCATH) D036900100006 REFERENCE (J,NIM/B,140,294,1998) D036900100007 FACILITY (VDGT,2GRCATH) TN11 TANDEM Accelerator D036900100008 SAMPLE The target was a Si crystal wafer (0.9 mg/cm2 thick) D036900100009 DETECTOR (SIBAR) Single Si surface barrier detector placed at D036900100010 angle 160. deg. with respect to the beam, and an D036900100011 overall resolution of 16 keV. D036900100012 ERR-ANALYS No information on uncertainty given D036900100013 STATUS (TABLE) Data received from Dr. X.A.Aslanoglou D036900100014 (APRVD) Entry was approved by Dr. X.A.Aslanoglou D036900100015 HISTORY (20051104C) SD D036900100016 (20110201A) On. Formal correction only D036900100017 ENDBIB 15 0 D036900100018 NOCOMMON 0 0 D036900100019 ENDSUBENT 18 0 D036900199999 SUBENT D0369002 20120201 D081D036900200001 BIB 2 2 D036900200002 REACTION (14-SI-28(P,EL)14-SI-28,,DA,,RTH) D036900200003 HISTORY (20120201A) On. SF8=RTH added D036900200004 ENDBIB 2 0 D036900200005 COMMON 2 3 D036900200006 EN-RSL ANG D036900200007 KEV ADEG D036900200008 16. 160. D036900200009 ENDCOMMON 3 0 D036900200010 DATA 2 90 D036900200011 EN DATA D036900200012 KEV NO-DIM D036900200013 1304.43 0.98 D036900200014 1322.36 0.97 D036900200015 1340.19 1.01 D036900200016 1357.85 0.98 D036900200017 1375.37 1.06 D036900200018 1392.73 1.03 D036900200019 1409.98 0.97 D036900200020 1427.05 1.08 D036900200021 1444.01 1.09 D036900200022 1460.89 1.05 D036900200023 1477.57 0.97 D036900200024 1494.17 0.99 D036900200025 1510.67 0.98 D036900200026 1531.09 0.90 D036900200027 1547.29 0.89 D036900200028 1563.40 0.86 D036900200029 1579.39 0.74 D036900200030 1595.30 0.61 D036900200031 1615.04 0.51 D036900200032 1630.70 0.65 D036900200033 1642.40 1.23 D036900200034 1646.25 1.59 D036900200035 1650.10 1.71 D036900200036 1654.01 2.13 D036900200037 1657.88 2.33 D036900200038 1665.60 2.53 D036900200039 1672.64 2.50 D036900200040 1680.31 2.47 D036900200041 1687.95 2.39 D036900200042 1695.56 2.23 D036900200043 1703.16 2.08 D036900200044 1714.53 2.01 D036900200045 1729.59 1.87 D036900200046 1744.58 1.68 D036900200047 1759.50 1.57 D036900200048 1774.27 1.61 D036900200049 1788.43 1.57 D036900200050 1803.07 1.56 D036900200051 1817.65 1.55 D036900200052 1832.16 1.54 D036900200053 1846.57 1.47 D036900200054 1860.94 1.42 D036900200055 1875.19 1.30 D036900200056 1888.08 1.40 D036900200057 1902.20 1.38 D036900200058 1916.27 1.39 D036900200059 1930.27 1.42 D036900200060 1944.21 1.34 D036900200061 1958.08 1.31 D036900200062 1971.88 1.37 D036900200063 1985.64 1.28 D036900200064 1999.28 1.14 D036900200065 2012.90 1.10 D036900200066 2026.43 1.18 D036900200067 2040.98 1.01 D036900200068 2054.40 0.95 D036900200069 2067.77 1.03 D036900200070 2071.00 1.39 D036900200071 2074.42 1.95 D036900200072 2077.00 2.40 D036900200073 2081.08 3.01 D036900200074 2084.40 3.43 D036900200075 2087.70 3.43 D036900200076 2091.00 3.42 D036900200077 2094.31 3.11 D036900200078 2097.61 2.78 D036900200079 2100.91 2.71 D036900200080 2107.51 2.35 D036900200081 2117.36 2.11 D036900200082 2130.46 1.91 D036900200083 2141.14 1.85 D036900200084 2154.14 1.65 D036900200085 2167.08 1.57 D036900200086 2179.98 1.56 D036900200087 2192.82 1.60 D036900200088 2205.61 1.51 D036900200089 2218.36 1.42 D036900200090 2231.05 1.44 D036900200091 2245.97 1.50 D036900200092 2258.56 1.58 D036900200093 2271.09 1.48 D036900200094 2283.60 1.43 D036900200095 2296.03 1.39 D036900200096 2308.44 1.44 D036900200097 2320.79 1.41 D036900200098 2333.11 1.31 D036900200099 2345.36 1.35 D036900200100 2357.59 1.25 D036900200101 2369.75 1.47 D036900200102 2381.90 1.37 D036900200103 ENDDATA 92 0 D036900200104 ENDSUBENT 103 0 D036900299999 ENDENTRY 2 0 D036999999999