ENTRY C1669 20160701 C163C166900000001 SUBENT C1669001 20160701 C163C166900100001 BIB 8 11 C166900100002 TITLE The Reaction Cross Section of Nitrogen 14 for Protons C166900100003 between 220 keV and 600 keV C166900100004 AUTHOR (R.E.Pixley) C166900100005 REFERENCE (T,PIXLEY,1957) C166900100006 INSTITUTE (1USACAL) C166900100007 FACILITY (VDG,1USACAL) 650 keV electrostatic generator of C166900100008 the Kellogg Radiation Laboratory. C166900100009 DETECTOR (CSICR,NAICR) NaI(Tl) 1.5 in.x1.5 in. for annihilation C166900100010 gamma radiation, thin CsI(Tl) crystal for positrons. C166900100011 DECAY-DATA (8-O-15,2.MIN,B+,,,AR) C166900100012 HISTORY (20160701C) BP C166900100013 ENDBIB 11 0 C166900100014 NOCOMMON 0 0 C166900100015 ENDSUBENT 14 0 C166900199999 SUBENT C1669002 20160701 C163C166900200001 BIB 5 17 C166900200002 REACTION (7-N-14(P,G)8-O-15,,SIG,,,DERIV) C166900200003 SAMPLE Be3N2 (Actual composition: Be3-N1.7-O0.4) and C166900200004 TaN targets. C166900200005 ANALYSIS (TTUNF) The cross section in terms of a thick target C166900200006 yield (Y) is: sigma (E)= epsilon (E) dY/dE, where C166900200007 epsilon is the stopping cross section per nitrogen C166900200008 atom of the target expressed in keV-cm2. For thin C166900200009 targets: sigma (E)= epsilon Y /delta E. C166900200010 ERR-ANALYS (ERR-T) The relative probable error. C166900200011 (ERR-S) Number of counts. C166900200012 (ERR-1,10.,14.) Stopping cross sections for Be and Ta C166900200013 nitride targets. C166900200014 (ERR-2) Correction for target nonuniformity. C166900200015 (ERR-3) Proton current. C166900200016 (ERR-4) Timing. C166900200017 (ERR-5) Mean life. C166900200018 STATUS (CURVE) Fig. 11, page 65. C166900200019 ENDBIB 17 0 C166900200020 COMMON 5 3 C166900200021 ERR-S ERR-2 ERR-3 ERR-4 ERR-5 C166900200022 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT C166900200023 4.0 4.0 3.0 1.0 1.0 C166900200024 ENDCOMMON 3 0 C166900200025 DATA 3 16 C166900200026 EN DATA ERR-T C166900200027 KEV B B C166900200028 218.705 3.324E-09 1.749E-09 C166900200029 231.851 6.583E-09 C166900200030 240.659 1.477E-08 C166900200031 250.919 3.313E-08 C166900200032 261.202 8.959E-08 1.976E-08 C166900200033 269.401 5.008E-07 C166900200034 276.318 1.056E-05 C166900200035 279.412 4.799E-05 1.210E-05 C166900200036 282.153 1.354E-05 C166900200037 284.161 3.588E-06 C166900200038 401.969 1.021E-07 C166900200039 451.324 1.199E-07 C166900200040 502.149 1.628E-07 3.323E-08 C166900200041 551.536 2.453E-07 C166900200042 600.915 3.472E-07 6.267E-08 C166900200043 650.291 4.814E-07 C166900200044 ENDDATA 18 0 C166900200045 ENDSUBENT 44 0 C166900299999 SUBENT C1669003 20160701 C163C166900300001 BIB 3 5 C166900300002 REACTION 1(7-N-14(P,0),,EN) C166900300003 2(7-N-14(P,G),,WID) C166900300004 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C166900300005 STATUS (DEP,C1669002) C166900300006 (TABLE) page 28-29. C166900300007 ENDBIB 5 0 C166900300008 NOCOMMON 0 0 C166900300009 DATA 5 1 C166900300010 DATA 1DATA-ERR 1DATA 2+DATA-ERR 2-DATA-ERR 2 C166900300011 KEV KEV KEV KEV KEV C166900300012 278.14 0.53 1.9 0.4 0.5 C166900300013 ENDDATA 3 0 C166900300014 ENDSUBENT 13 0 C166900399999 SUBENT C1669004 20160701 C163C166900400001 BIB 4 10 C166900400002 REACTION (7-N-14(P,EL)7-N-14,,DA,,RTH) C166900400003 SAMPLE Melamine (N2CH2)3, a thick layer of melamine on an C166900400004 aluminum backing. C166900400005 ERR-ANALYS (ERR-T) The relative probable error. C166900400006 (ERR-S) Counting statistics. C166900400007 (ERR-1) Stopping cross section. C166900400008 (ERR-2) Reproducibility of the integrator. C166900400009 (ERR-3) Uncertainty in spectrometer and target angles. C166900400010 (ERR-4) Spectrometer energy. C166900400011 STATUS (CURVE) Fig. 15, page 68. C166900400012 ENDBIB 10 0 C166900400013 COMMON 7 6 C166900400014 ANG-CM ERR-T ERR-S ERR-1 ERR-2 ERR-3 C166900400015 ERR-4 C166900400016 ADEG PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT C166900400017 PER-CENT C166900400018 152.0 7.0 2.0 3.0 1.0 1.0C166900400019 0.5 C166900400020 ENDCOMMON 6 0 C166900400021 DATA 2 14 C166900400022 EN DATA C166900400023 KEV NO-DIM C166900400024 269.342 0.955 C166900400025 271.898 0.938 C166900400026 274.581 0.897 C166900400027 276.552 0.830 C166900400028 277.139 0.834 C166900400029 277.473 0.868 C166900400030 277.596 0.957 C166900400031 278.095 1.113 C166900400032 278.719 1.248 C166900400033 279.349 1.198 C166900400034 279.768 1.211 C166900400035 281.237 1.110 C166900400036 285.262 1.039 C166900400037 288.529 1.065 C166900400038 ENDDATA 16 0 C166900400039 ENDSUBENT 38 0 C166900499999 SUBENT C1669005 20160701 C163C166900500001 BIB 4 10 C166900500002 REACTION (7-N-14(P,EL)7-N-14,,DA,,RTH) C166900500003 SAMPLE Melamine (N2CH2)3, a thick layer of melamine on an C166900500004 aluminum backing. C166900500005 ERR-ANALYS (ERR-T) The relative probable error. C166900500006 (ERR-S) Counting statistics. C166900500007 (ERR-1) Stopping cross section. C166900500008 (ERR-2) Reproducibility of the integrator. C166900500009 (ERR-3) Uncertainty in spectrometer and target angles. C166900500010 (ERR-4) Spectrometer energy. C166900500011 STATUS (CURVE) Fig. 16, page 68. C166900500012 ENDBIB 10 0 C166900500013 COMMON 7 6 C166900500014 ANG-CM ERR-T ERR-S ERR-1 ERR-2 ERR-3 C166900500015 ERR-4 C166900500016 ADEG PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT C166900500017 PER-CENT C166900500018 125.0 7.0 2.0 3.0 1.0 1.0C166900500019 0.5 C166900500020 ENDCOMMON 6 0 C166900500021 DATA 2 14 C166900500022 EN DATA C166900500023 KEV NO-DIM C166900500024 268.506 0.928 C166900500025 270.894 0.919 C166900500026 273.868 0.893 C166900500027 274.832 0.901 C166900500028 276.130 0.858 C166900500029 276.925 0.804 C166900500030 277.596 0.824 C166900500031 278.269 0.917 C166900500032 278.859 1.072 C166900500033 279.572 1.097 C166900500034 280.410 1.084 C166900500035 281.498 1.021 C166900500036 284.765 0.990 C166900500037 287.489 0.994 C166900500038 ENDDATA 16 0 C166900500039 ENDSUBENT 38 0 C166900599999 SUBENT C1669006 20160701 C163C166900600001 BIB 4 10 C166900600002 REACTION (7-N-14(P,EL)7-N-14,,DA,,RTH) C166900600003 SAMPLE Melamine (N2CH2)3, a thick layer of melamine on an C166900600004 aluminum backing. C166900600005 ERR-ANALYS (ERR-T) The relative probable error. C166900600006 (ERR-S) Counting statistics. C166900600007 (ERR-1) Stopping cross section. C166900600008 (ERR-2) Reproducibility of the integrator. C166900600009 (ERR-3) Uncertainty in spectrometer and target angles. C166900600010 (ERR-4) Spectrometer energy. C166900600011 STATUS (CURVE) Fig. 17, page 68. C166900600012 ENDBIB 10 0 C166900600013 COMMON 7 6 C166900600014 ANG-CM ERR-T ERR-S ERR-1 ERR-2 ERR-3 C166900600015 ERR-4 C166900600016 ADEG PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT C166900600017 PER-CENT C166900600018 90.0 7.0 2.0 3.0 1.0 1.0C166900600019 0.5 C166900600020 ENDCOMMON 6 0 C166900600021 DATA 2 10 C166900600022 EN DATA C166900600023 KEV NO-DIM C166900600024 270.614 0.990 C166900600025 273.044 0.990 C166900600026 274.594 0.964 C166900600027 275.977 0.968 C166900600028 277.524 0.854 C166900600029 278.194 0.825 C166900600030 278.992 0.896 C166900600031 280.376 0.975 C166900600032 281.718 0.987 C166900600033 283.896 0.991 C166900600034 ENDDATA 12 0 C166900600035 ENDSUBENT 34 0 C166900699999 SUBENT C1669007 20160701 C163C166900700001 BIB 3 6 C166900700002 REACTION (7-N-14(P,EL),,WID) C166900700003 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. C166900700004 STATUS (DEP,C1669004) C166900700005 (DEP,C1669005) C166900700006 (DEP,C1669006) C166900700007 (TABLE) page 44. C166900700008 ENDBIB 6 0 C166900700009 NOCOMMON 0 0 C166900700010 DATA 2 1 C166900700011 DATA DATA-ERR C166900700012 KEV KEV C166900700013 1.5 0.5 C166900700014 ENDDATA 3 0 C166900700015 ENDSUBENT 14 0 C166900799999 ENDENTRY 7 0 C166999999999