ENTRY E1869 20120614 E069E186900000001 SUBENT E1869001 20120614 E069E186900100001 BIB 9 16 E186900100002 TITLE The 14N(d,n)15O reaction in the energy range from 1.5- E186900100003 to 2.9-MeV E186900100004 AUTHOR (S.Morita, N.Kawai, Y.Goto, T.Maki, M.Mukae) E186900100005 INSTITUTE (2JPNKYU) Department of Physics, Faculty of Science E186900100006 REFERENCE (J,JPJ,15,(12),2170,196012) E186900100007 PART-DET (N) E186900100008 SAMPLE - Chemical-form of target is element. E186900100009 - Physical-form of target is gas. E186900100010 - Target-thickness: pressure is 20.0 cm Hg E186900100011 FACILITY (VDG,2JPNKYU) E186900100012 DETECTOR (SCIN) Disk of thin plastic scintillator. Angular E186900100013 resolutions ranged from +-4 deg at 0 deg, to E186900100014 +-6 deg at 90 deg. E186900100015 HISTORY (20040218C) Sr + On E186900100016 (20120405A) Nf. Subentries 002-008: PAR added in SF5, E186900100017 E-LVL added, ERR-S corrected E186900100018 ENDBIB 16 0 E186900100019 NOCOMMON 0 0 E186900100020 ENDSUBENT 19 0 E186900199999 SUBENT E1869002 20120614 E069E186900200001 BIB 6 13 E186900200002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900200003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900200004 (E-LVL,8-O-15) E186900200005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900200006 neutron scatterings in materials E186900200007 between the target and detector and so E186900200008 on is less than 10% (<10%) E186900200009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900200010 to 2% (2-5%) E186900200011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900200012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900200013 STATUS (CURVE) Scanned from Fig.2(a), p2172 in reference E186900200014 HISTORY (20061005A) Is. Re-digitized E186900200015 ENDBIB 13 0 E186900200016 COMMON 2 3 E186900200017 EN E-LVL E186900200018 MEV MEV E186900200019 1.53 0. E186900200020 ENDCOMMON 3 0 E186900200021 DATA 2 13 E186900200022 ANG-CM DATA-CM E186900200023 ADEG MB/SR E186900200024 1.150E-01 2.393E+00 E186900200025 1.039E+01 2.565E+00 E186900200026 1.650E+01 2.663E+00 E186900200027 3.264E+01 2.557E+00 E186900200028 4.654E+01 1.824E+00 E186900200029 6.318E+01 1.558E+00 E186900200030 7.889E+01 1.077E+00 E186900200031 9.290E+01 9.418E-01 E186900200032 1.078E+02 7.679E-01 E186900200033 1.220E+02 9.163E-01 E186900200034 1.375E+02 1.309E+00 E186900200035 1.514E+02 1.565E+00 E186900200036 1.618E+02 1.960E+00 E186900200037 ENDDATA 15 0 E186900200038 ENDSUBENT 37 0 E186900299999 SUBENT E1869003 20120614 E069E186900300001 BIB 6 13 E186900300002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900300003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900300004 (E-LVL,8-O-15) E186900300005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900300006 neutron scatterings in materials E186900300007 between the target and detector and so E186900300008 on is less than 10% (<10%) E186900300009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900300010 to 2% (2-5%) E186900300011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900300012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900300013 STATUS (CURVE) Scanned from Fig.2(b), p2172 in reference E186900300014 HISTORY (20061005A) Is. Re-digitized E186900300015 ENDBIB 13 0 E186900300016 COMMON 2 3 E186900300017 EN E-LVL E186900300018 MEV MEV E186900300019 1.72 0. E186900300020 ENDCOMMON 3 0 E186900300021 DATA 2 13 E186900300022 ANG-CM DATA-CM E186900300023 ADEG MB/SR E186900300024 6.494E-01 2.151E+00 E186900300025 1.093E+01 2.047E+00 E186900300026 2.087E+01 2.180E+00 E186900300027 3.097E+01 2.076E+00 E186900300028 4.638E+01 1.703E+00 E186900300029 6.217E+01 1.511E+00 E186900300030 7.720E+01 9.472E-01 E186900300031 9.300E+01 7.790E-01 E186900300032 1.079E+02 8.009E-01 E186900300033 1.219E+02 1.036E+00 E186900300034 1.366E+02 2.023E+00 E186900300035 1.501E+02 2.354E+00 E186900300036 1.603E+02 3.800E+00 E186900300037 ENDDATA 15 0 E186900300038 ENDSUBENT 37 0 E186900399999 SUBENT E1869004 20120614 E069E186900400001 BIB 6 13 E186900400002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900400003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900400004 (E-LVL,8-O-15) E186900400005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900400006 neutron scatterings in materials E186900400007 between the target and detector and so E186900400008 on is less than 10% (<10%) E186900400009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900400010 to 2% (2-5%) E186900400011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900400012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900400013 STATUS (CURVE) Scanned from Fig.2(c), p2172 in reference E186900400014 HISTORY (20061005A) Is. Re-digitized E186900400015 ENDBIB 13 0 E186900400016 COMMON 2 3 E186900400017 EN E-LVL E186900400018 MEV MEV E186900400019 1.97 0. E186900400020 ENDCOMMON 3 0 E186900400021 DATA 2 6 E186900400022 ANG-CM DATA-CM E186900400023 ADEG MB/SR E186900400024 7.676E-02 1.711E+00 E186900400025 1.022E+01 1.749E+00 E186900400026 2.037E+01 1.772E+00 E186900400027 3.161E+01 1.651E+00 E186900400028 9.369E+01 8.970E-01 E186900400029 1.502E+02 4.701E+00 E186900400030 ENDDATA 8 0 E186900400031 ENDSUBENT 30 0 E186900499999 SUBENT E1869005 20120614 E069E186900500001 BIB 6 13 E186900500002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900500003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900500004 (E-LVL,8-O-15) E186900500005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900500006 neutron scatterings in materials E186900500007 between the target and detector and so E186900500008 on is less than 10% (<10%) E186900500009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900500010 to 2% (2-5%) E186900500011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900500012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900500013 STATUS (CURVE) Scanned from Fig.2(d), p2172 in reference E186900500014 HISTORY (20061005A) Is. Re-digitized E186900500015 ENDBIB 13 0 E186900500016 COMMON 2 3 E186900500017 EN E-LVL E186900500018 MEV MEV E186900500019 2.24 0. E186900500020 ENDCOMMON 3 0 E186900500021 DATA 2 13 E186900500022 ANG-CM DATA-CM E186900500023 ADEG MB/SR E186900500024 1.696E-01 2.263E+00 E186900500025 1.092E+01 3.425E+00 E186900500026 2.110E+01 3.090E+00 E186900500027 3.227E+01 2.921E+00 E186900500028 4.693E+01 1.305E+00 E186900500029 6.216E+01 1.260E+00 E186900500030 7.681E+01 1.165E+00 E186900500031 9.263E+01 1.178E+00 E186900500032 1.067E+02 1.059E+00 E186900500033 1.218E+02 1.587E+00 E186900500034 1.361E+02 2.964E+00 E186900500035 1.502E+02 3.568E+00 E186900500036 1.600E+02 4.996E+00 E186900500037 ENDDATA 15 0 E186900500038 ENDSUBENT 37 0 E186900599999 SUBENT E1869006 20120614 E069E186900600001 BIB 6 13 E186900600002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900600003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900600004 (E-LVL,8-O-15) E186900600005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900600006 neutron scatterings in materials E186900600007 between the target and detector and so E186900600008 on is less than 10% (<10%) E186900600009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900600010 to 2% (2-5%) E186900600011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900600012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900600013 STATUS (CURVE) Scanned from Fig.2(e), p2172 in reference E186900600014 HISTORY (20061005A) Is. Re-digitized E186900600015 ENDBIB 13 0 E186900600016 COMMON 2 3 E186900600017 EN E-LVL E186900600018 MEV MEV E186900600019 2.54 0. E186900600020 ENDCOMMON 3 0 E186900600021 DATA 2 12 E186900600022 ANG-CM DATA-CM E186900600023 ADEG MB/SR E186900600024 2.660E-01 3.564E+00 E186900600025 1.071E+01 3.994E+00 E186900600026 2.131E+01 4.208E+00 E186900600027 3.090E+01 4.047E+00 E186900600028 6.229E+01 1.698E+00 E186900600029 7.707E+01 1.478E+00 E186900600030 9.204E+01 1.291E+00 E186900600031 1.068E+02 1.303E+00 E186900600032 1.215E+02 1.483E+00 E186900600033 1.362E+02 2.129E+00 E186900600034 1.508E+02 2.441E+00 E186900600035 1.600E+02 3.122E+00 E186900600036 ENDDATA 14 0 E186900600037 ENDSUBENT 36 0 E186900699999 SUBENT E1869007 20120614 E069E186900700001 BIB 6 13 E186900700002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900700003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900700004 (E-LVL,8-O-15) E186900700005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900700006 neutron scatterings in materials E186900700007 between the target and detector and so E186900700008 on is less than 10% (<10%) E186900700009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900700010 to 2% (2-5%) E186900700011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900700012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900700013 STATUS (CURVE) Scanned from Fig.2(f), p2172 in reference E186900700014 HISTORY (20061005A) Is. Re-digitized E186900700015 ENDBIB 13 0 E186900700016 COMMON 2 3 E186900700017 EN E-LVL E186900700018 MEV MEV E186900700019 2.675 0. E186900700020 ENDCOMMON 3 0 E186900700021 DATA 2 13 E186900700022 ANG-CM DATA-CM E186900700023 ADEG MB/SR E186900700024 -4.130E-01 4.191E+00 E186900700025 1.041E+01 4.539E+00 E186900700026 2.027E+01 4.680E+00 E186900700027 3.093E+01 4.292E+00 E186900700028 4.627E+01 3.030E+00 E186900700029 6.178E+01 2.139E+00 E186900700030 7.746E+01 1.859E+00 E186900700031 9.255E+01 1.984E+00 E186900700032 1.065E+02 1.844E+00 E186900700033 1.218E+02 2.044E+00 E186900700034 1.361E+02 2.474E+00 E186900700035 1.510E+02 2.649E+00 E186900700036 1.598E+02 3.483E+00 E186900700037 ENDDATA 15 0 E186900700038 ENDSUBENT 37 0 E186900799999 SUBENT E1869008 20120614 E069E186900800001 BIB 6 13 E186900800002 REACTION (7-N-14(D,N)8-O-15,PAR,DA) E186900800003 EN-SEC ANG-CM is polar angle (c.m.) between beam and neutron E186900800004 (E-LVL,8-O-15) E186900800005 ERR-ANALYS (ERR-SYS,,10.) Uncertainty in neutron intensity, E186900800006 neutron scatterings in materials E186900800007 between the target and detector and so E186900800008 on is less than 10% (<10%) E186900800009 (ERR-S,2.,5.) Statistical uncertainty ranges from 5% E186900800010 to 2% (2-5%) E186900800011 ADD-RES (COMP) Heavy particle stripping theory [G.E. Owen and E186900800012 L. Madansky, Phys. Rev. 105(1957)1766]. E186900800013 STATUS (CURVE) Scanned from Fig.2(g), p2172 in reference E186900800014 HISTORY (20061005A) Is. Re-digitized E186900800015 ENDBIB 13 0 E186900800016 COMMON 2 3 E186900800017 EN E-LVL E186900800018 MEV MEV E186900800019 2.90 0. E186900800020 ENDCOMMON 3 0 E186900800021 DATA 2 13 E186900800022 ANG-CM DATA-CM E186900800023 ADEG MB/SR E186900800024 2.212E-01 2.406E+00 E186900800025 1.050E+01 3.147E+00 E186900800026 2.057E+01 3.438E+00 E186900800027 3.119E+01 3.548E+00 E186900800028 4.596E+01 2.583E+00 E186900800029 6.147E+01 1.738E+00 E186900800030 7.701E+01 1.665E+00 E186900800031 9.259E+01 2.201E+00 E186900800032 1.074E+02 1.702E+00 E186900800033 1.216E+02 1.748E+00 E186900800034 1.365E+02 2.189E+00 E186900800035 1.510E+02 2.495E+00 E186900800036 1.656E+02 3.141E+00 E186900800037 ENDDATA 15 0 E186900800038 ENDSUBENT 37 0 E186900899999 SUBENT E1869009 20061121 E040E186900900001 BIB 5 10 E186900900002 REACTION (7-N-14(D,N)8-O-15,,SIG) E186900900003 ERR-ANALYS (ERR-SYS) Maxium uncertainty in neutron intensity, E186900900004 neutron scatterings in materials between the E186900900005 target and detector and so on E186900900006 COMMENT Absolute value of cross section was determined by E186900900007 normalizing the angular distribution to the absolute E186900900008 cross section obtained at the direction of 30 deg by E186900900009 Retz-Schmidt and Weil (private communication). E186900900010 STATUS (CURVE) Data scanned from Fig.4, p2174 in reference E186900900011 HISTORY (20061005A) Is. Re-digitized E186900900012 ENDBIB 10 0 E186900900013 COMMON 1 3 E186900900014 ERR-SYS E186900900015 PER-CENT E186900900016 15. E186900900017 ENDCOMMON 3 0 E186900900018 DATA 2 7 E186900900019 EN DATA E186900900020 MEV MB E186900900021 1.538E+00 1.718E+01 E186900900022 1.722E+00 1.824E+01 E186900900023 1.971E+00 2.308E+01 E186900900024 2.224E+00 2.320E+01 E186900900025 2.529E+00 2.538E+01 E186900900026 2.681E+00 3.143E+01 E186900900027 2.905E+00 2.721E+01 E186900900028 ENDDATA 9 0 E186900900029 ENDSUBENT 28 0 E186900999999 ENDENTRY 9 0 E186999999999