ENTRY F1195 20130626 F052F119500000001 SUBENT F1195001 20130626 F052F119500100001 BIB 10 16 F119500100002 TITLE Boron analysis of thin layers using prompt nuclear F119500100003 techniques. F119500100004 AUTHOR (N.Moncoffre,N.Millard,H.Jaffrezic,J.Tousset) F119500100005 INSTITUTE (2FR LYO) F119500100006 REFERENCE (J,NIM/B,45,81,1990) F119500100007 #doi:10.1016/0168-583X(90)90789-W F119500100008 FACILITY (VDG,2FR LYO) F119500100009 DETECTOR (SIBAR) The alpha particle detector was made with a F119500100010 surface barrier silicon detector of 16 keV overall F119500100011 resolution. F119500100012 SAMPLE A thick boron target was used. F119500100013 MONITOR The cross section was normalized from the Rutherford F119500100014 scattering cross section of alpha particles on nickel. F119500100015 ERR-ANALYS (EN-ERR-DIG) Energy digitizing error F119500100016 (ERR-DIG) Data digitizing error F119500100017 HISTORY (20130626C) F119500100018 ENDBIB 16 0 F119500100019 COMMON 3 3 F119500100020 ANG EN-ERR-DIG ERR-DIG F119500100021 ADEG MEV B/SR F119500100022 172. 0.0024 0.00053 F119500100023 ENDCOMMON 3 0 F119500100024 ENDSUBENT 23 0 F119500199999 SUBENT F1195002 20130626 F052F119500200001 BIB 2 2 F119500200002 REACTION (5-B-11(A,EL)5-B-11,,DA) F119500200003 STATUS (CURVE) Fig.1 F119500200004 ENDBIB 2 0 F119500200005 NOCOMMON 0 0 F119500200006 DATA 2 83 F119500200007 EN DATA F119500200008 MEV B/SR F119500200009 3.8504 0.16984 F119500200010 3.8952 0.08172 F119500200011 3.9514 0.04229 F119500200012 4.0019 0.04114 F119500200013 4.0525 0.03649 F119500200014 4.1031 0.03649 F119500200015 4.1480 0.04924 F119500200016 4.1986 0.03996 F119500200017 4.2267 0.04924 F119500200018 4.2491 0.04808 F119500200019 4.2772 0.05039 F119500200020 4.2941 0.04923 F119500200021 4.3896 0.05966 F119500200022 4.4458 0.06778 F119500200023 4.4964 0.07241 F119500200024 4.5413 0.07357 F119500200025 4.5919 0.07356 F119500200026 4.6480 0.06429 F119500200027 4.6930 0.05037 F119500200028 4.7491 0.03414 F119500200029 4.7940 0.02718 F119500200030 4.8446 0.03065 F119500200031 4.8952 0.08398 F119500200032 4.9457 0.00862 F119500200033 4.9963 0.02833 F119500200034 5.0469 0.05383 F119500200035 5.0975 0.06426 F119500200036 5.1424 0.08745 F119500200037 5.1987 0.12222 F119500200038 5.2491 0.04686 F119500200039 5.2941 0.04802 F119500200040 5.3447 0.09671 F119500200041 5.3953 0.12337 F119500200042 5.4515 0.14076 F119500200043 5.4965 0.14655 F119500200044 5.5473 0.32858 F119500200045 5.5977 0.22423 F119500200046 5.6481 0.13031 F119500200047 5.6986 0.08741 F119500200048 5.7492 0.08046 F119500200049 5.7998 0.12567 F119500200050 5.8505 0.20566 F119500200051 5.8786 0.26015 F119500200052 5.9011 0.26943 F119500200053 5.9236 0.31580 F119500200054 5.9517 0.28913 F119500200055 5.9627 0.14421 F119500200056 5.9967 0.31000 F119500200057 6.0360 0.30652 F119500200058 6.0584 0.27985 F119500200059 6.0809 0.26942 F119500200060 6.0977 0.23579 F119500200061 6.1201 0.19869 F119500200062 6.1368 0.09203 F119500200063 6.1537 0.08159 F119500200064 6.1762 0.11405 F119500200065 6.1987 0.12796 F119500200066 6.2493 0.14187 F119500200067 6.2998 0.15926 F119500200068 6.3504 0.16622 F119500200069 6.4009 0.15114 F119500200070 6.4515 0.11404 F119500200071 6.5023 0.30997 F119500200072 6.5474 0.46301 F119500200073 6.5980 0.45025 F119500200074 6.6540 0.30069 F119500200075 6.6989 0.29837 F119500200076 6.7495 0.32387 F119500200077 6.8001 0.32155 F119500200078 6.8507 0.37372 F119500200079 6.9068 0.31227 F119500200080 6.9517 0.29140 F119500200081 7.0078 0.26473 F119500200082 7.0584 0.26009 F119500200083 7.1034 0.26936 F119500200084 7.1539 0.22298 F119500200085 7.2044 0.20095 F119500200086 7.2549 0.20095 F119500200087 7.3055 0.15804 F119500200088 7.3561 0.19051 F119500200089 7.4010 0.21369 F119500200090 7.4517 0.26238 F119500200091 7.5023 0.31107 F119500200092 ENDDATA 85 0 F119500200093 ENDSUBENT 92 0 F119500299999 ENDENTRY 2 0 F119599999999