ENTRY 11174 20220315 14981117400000001 SUBENT 11174001 20220315 14981117400100001 BIB 10 22 1117400100002 TITLE Nuclear Cross Sections for 95-Mev Neutrons 1117400100003 AUTHOR (J.DeJuren,N.Knable) 1117400100004 REFERENCE (J,PR,77,606,1950) 1117400100005 #doi:10.1103/PhysRev.77.606 1117400100006 REL-REF (A,11146001,L.J.Cook+,J,PR,75,7,1949) 83-MeV data. 1117400100007 INSTITUTE (1USABRK) 1117400100008 FACILITY (CYCLO,1USABRK) 184-inch Berkeley cyclotron. 1117400100009 INC-SOURCE (D-BE) The neutron source was a 1/2" thick Be target 1117400100010 with 190 MeV deuteron beam. 1117400100011 DETECTOR (FISCH) Bi fission ionization chamber 1117400100012 SAMPLE Metal used in the experiments were usually machined 1117400100013 cylinders and were measured by two different 1117400100014 observers with micrometers or vernier calipers. The 1117400100015 liquids employed were weighed in a 500-ml volumetric 1117400100016 flask. Chemically pure materials were used. 1117400100017 HISTORY (19760924T) Translated from SCISRS. 1117400100018 (19800814A) Converted to reaction formalism 1117400100019 (20071108A) Title added, BIB update. 1117400100020 (20220315A) BP: Added doi, incoming source, error 1117400100021 analysis, status, related reference, sample, 1117400100022 inelastic cross section data (subs. 16-19). Corrected 1117400100023 errors (subs. 2-15). 1117400100024 ENDBIB 22 0 1117400100025 NOCOMMON 0 0 1117400100026 ENDSUBENT 25 0 1117400199999 SUBENT 11174002 20220315 14981117400200001 BIB 4 5 1117400200002 REACTION (1-H-1(N,TOT),,SIG) 1117400200003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400200004 standard deviations. 1117400200005 CORRECTION Corrected for diffraction scattering 1117400200006 STATUS (TABLE) Table I, page 611. 1117400200007 ENDBIB 5 0 1117400200008 NOCOMMON 0 0 1117400200009 DATA 4 1 1117400200010 EN EN-RSL DATA ERR-S 1117400200011 MEV MEV B B 1117400200012 9.5E+01 2.6E+01 7.3E-02 1.5E-03 1117400200013 ENDDATA 3 0 1117400200014 ENDSUBENT 13 0 1117400299999 SUBENT 11174003 20220315 14981117400300001 BIB 4 5 1117400300002 REACTION (1-H-2(N,TOT),,SIG) 1117400300003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400300004 standard deviations. 1117400300005 CORRECTION Corrected for diffraction scattering 1117400300006 STATUS (TABLE) Table I, page 611. 1117400300007 ENDBIB 5 0 1117400300008 NOCOMMON 0 0 1117400300009 DATA 4 1 1117400300010 EN EN-RSL DATA ERR-S 1117400300011 MEV MEV B B 1117400300012 9.5E+01 2.6E+01 1.04E-01 4.E-03 1117400300013 ENDDATA 3 0 1117400300014 ENDSUBENT 13 0 1117400399999 SUBENT 11174004 20220315 14981117400400001 BIB 4 5 1117400400002 REACTION (1-H-WTR(N,TOT),,SIG) 1117400400003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400400004 standard deviations. 1117400400005 CORRECTION Corrected for diffraction scattering. 1117400400006 STATUS (TABLE) Table I, page 611. 1117400400007 ENDBIB 5 0 1117400400008 NOCOMMON 0 0 1117400400009 DATA 4 1 1117400400010 EN EN-RSL DATA ERR-S 1117400400011 MEV MEV B B 1117400400012 9.5E+01 2.6E+01 8.11E-01 7.E-03 1117400400013 ENDDATA 3 0 1117400400014 ENDSUBENT 13 0 1117400499999 SUBENT 11174005 20220315 14981117400500001 BIB 4 5 1117400500002 REACTION (1-H-D2O(N,TOT),,SIG) 1117400500003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400500004 standard deviations. 1117400500005 CORRECTION Corrected for diffraction scattering. 1117400500006 STATUS (TABLE) Table I, page 611. 1117400500007 ENDBIB 5 0 1117400500008 NOCOMMON 0 0 1117400500009 DATA 4 1 1117400500010 EN EN-RSL DATA ERR-S 1117400500011 MEV MEV B B 1117400500012 9.5E+01 2.6E+01 8.68E-01 5.E-03 1117400500013 ENDDATA 3 0 1117400500014 ENDSUBENT 13 0 1117400599999 SUBENT 11174006 20220315 14981117400600001 BIB 4 5 1117400600002 REACTION (4-BE-9(N,TOT),,SIG) 1117400600003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400600004 standard deviations. 1117400600005 CORRECTION Corrected for diffraction scattering. 1117400600006 STATUS (TABLE) Table I, page 611. 1117400600007 ENDBIB 5 0 1117400600008 NOCOMMON 0 0 1117400600009 DATA 4 1 1117400600010 EN EN-RSL DATA ERR-S 1117400600011 MEV MEV B B 1117400600012 9.5E+01 2.6E+01 3.96E-01 4.E-03 1117400600013 ENDDATA 3 0 1117400600014 ENDSUBENT 13 0 1117400699999 SUBENT 11174007 20220315 14981117400700001 BIB 3 4 1117400700002 REACTION (6-C-0(N,TOT),,SIG) 1117400700003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400700004 standard deviations. 1117400700005 STATUS (TABLE) Table I, page 611. 1117400700006 ENDBIB 4 0 1117400700007 NOCOMMON 0 0 1117400700008 DATA 4 1 1117400700009 EN EN-RSL DATA ERR-S 1117400700010 MEV MEV B B 1117400700011 9.5E+01 2.6E+01 4.98E-01 3.E-03 1117400700012 ENDDATA 3 0 1117400700013 ENDSUBENT 12 0 1117400799999 SUBENT 11174008 20220315 14981117400800001 BIB 3 4 1117400800002 REACTION (7-N-0(N,TOT),,SIG) 1117400800003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400800004 standard deviations. 1117400800005 STATUS (TABLE) Table I, page 611. 1117400800006 ENDBIB 4 0 1117400800007 NOCOMMON 0 0 1117400800008 DATA 4 1 1117400800009 EN EN-RSL DATA ERR-S 1117400800010 MEV MEV B B 1117400800011 9.5E+01 2.6E+01 5.70E-01 7.E-03 1117400800012 ENDDATA 3 0 1117400800013 ENDSUBENT 12 0 1117400899999 SUBENT 11174009 20220315 14981117400900001 BIB 3 4 1117400900002 REACTION (8-O-0(N,TOT),,SIG) 1117400900003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117400900004 standard deviations. 1117400900005 STATUS (TABLE) Table I, page 611. 1117400900006 ENDBIB 4 0 1117400900007 NOCOMMON 0 0 1117400900008 DATA 4 1 1117400900009 EN EN-RSL DATA ERR-S 1117400900010 MEV MEV B B 1117400900011 9.5E+01 2.6E+01 6.63E-01 7.E-03 1117400900012 ENDDATA 3 0 1117400900013 ENDSUBENT 12 0 1117400999999 SUBENT 11174010 20220315 14981117401000001 BIB 3 4 1117401000002 REACTION (13-AL-27(N,TOT),,SIG) 1117401000003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117401000004 standard deviations. 1117401000005 STATUS (TABLE) Table I, page 611. 1117401000006 ENDBIB 4 0 1117401000007 NOCOMMON 0 0 1117401000008 DATA 4 1 1117401000009 EN EN-RSL DATA ERR-S 1117401000010 MEV MEV B B 1117401000011 9.5E+01 2.6E+01 9.93E-01 1.1E-02 1117401000012 ENDDATA 3 0 1117401000013 ENDSUBENT 12 0 1117401099999 SUBENT 11174011 20220315 14981117401100001 BIB 3 4 1117401100002 REACTION (17-CL-0(N,TOT),,SIG) 1117401100003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117401100004 standard deviations. 1117401100005 STATUS (TABLE) Table I, page 611. 1117401100006 ENDBIB 4 0 1117401100007 NOCOMMON 0 0 1117401100008 DATA 4 1 1117401100009 EN EN-RSL DATA ERR-S 1117401100010 MEV MEV B B 1117401100011 9.5E+01 2.6E+01 1.28 2.E-02 1117401100012 ENDDATA 3 0 1117401100013 ENDSUBENT 12 0 1117401199999 SUBENT 11174012 20220315 14981117401200001 BIB 3 4 1117401200002 REACTION (29-CU-0(N,TOT),,SIG) 1117401200003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117401200004 standard deviations. 1117401200005 STATUS (TABLE) Table I, page 611. 1117401200006 ENDBIB 4 0 1117401200007 NOCOMMON 0 0 1117401200008 DATA 4 1 1117401200009 EN EN-RSL DATA ERR-S 1117401200010 MEV MEV B B 1117401200011 9.5E+01 2.6E+01 2.00 2.E-02 1117401200012 ENDDATA 3 0 1117401200013 ENDSUBENT 12 0 1117401299999 SUBENT 11174013 20220315 14981117401300001 BIB 3 4 1117401300002 REACTION (50-SN-0(N,TOT),,SIG) 1117401300003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117401300004 standard deviations. 1117401300005 STATUS (TABLE) Table I, page 611. 1117401300006 ENDBIB 4 0 1117401300007 NOCOMMON 0 0 1117401300008 DATA 4 1 1117401300009 EN EN-RSL DATA ERR-S 1117401300010 MEV MEV B B 1117401300011 9.5E+01 2.6E+01 3.18 3.E-02 1117401300012 ENDDATA 3 0 1117401300013 ENDSUBENT 12 0 1117401399999 SUBENT 11174014 20220315 14981117401400001 BIB 3 4 1117401400002 REACTION (82-PB-0(N,TOT),,SIG) 1117401400003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117401400004 standard deviations. 1117401400005 STATUS (TABLE) Table I, page 611. 1117401400006 ENDBIB 4 0 1117401400007 NOCOMMON 0 0 1117401400008 DATA 4 1 1117401400009 EN EN-RSL DATA ERR-S 1117401400010 MEV MEV B B 1117401400011 9.5E+01 2.6E+01 4.48 3.E-02 1117401400012 ENDDATA 3 0 1117401400013 ENDSUBENT 12 0 1117401499999 SUBENT 11174015 20220315 14981117401500001 BIB 4 5 1117401500002 REACTION (92-U-0(N,TOT),,SIG) 1117401500003 ERR-ANALYS (ERR-S) Statistical errors are given in terms of 1117401500004 standard deviations. 1117401500005 CORRECTION Corrected for diffraction scattering. 1117401500006 STATUS (TABLE) Table I, page 611. 1117401500007 ENDBIB 5 0 1117401500008 NOCOMMON 0 0 1117401500009 DATA 4 1 1117401500010 EN EN-RSL DATA ERR-S 1117401500011 MEV MEV B B 1117401500012 9.5E+01 2.6E+01 4.89 6.E-02 1117401500013 ENDDATA 3 0 1117401500014 ENDSUBENT 13 0 1117401599999 SUBENT 11174016 20220315 14981117401600001 BIB 5 11 1117401600002 REACTION ((6-C-0(N,INL)6-C-0,,SIG)/(6-C-0(N,TOT),,SIG)) 1117401600003 METHOD The inelastic cross-section measurements are subject 1117401600004 to greater sources of error. The "poor geometry" 1117401600005 detector count inelastically scattered neutrons or 1117401600006 neutrons ejected from nuclei if their energies are 1117401600007 above the threshold for bismuth fission. The 1117401600008 inelastic cross sections obtained, therefore, 1117401600009 represent a lower limit to the true values. 1117401600010 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1117401600011 STATUS (TABLE) Table II, page 611. 1117401600012 HISTORY (20220315A) BP 1117401600013 ENDBIB 11 0 1117401600014 NOCOMMON 0 0 1117401600015 DATA 4 1 1117401600016 EN EN-RSL DATA-MIN DATA-ERR 1117401600017 MEV MEV NO-DIM NO-DIM 1117401600018 9.5E+01 2.6E+01 0.45 0.015 1117401600019 ENDDATA 3 0 1117401600020 ENDSUBENT 19 0 1117401699999 SUBENT 11174017 20220315 14981117401700001 BIB 5 11 1117401700002 REACTION ((13-AL-27(N,INL)13-AL-27,,SIG)/(13-AL-27(N,TOT),,SIG))1117401700003 METHOD The inelastic cross-section measurements are subject 1117401700004 to greater sources of error. The "poor geometry" 1117401700005 detector count inelastically scattered neutrons or 1117401700006 neutrons ejected from nuclei if their energies are 1117401700007 above the threshold for bismuth fission. The 1117401700008 inelastic cross sections obtained, therefore, 1117401700009 represent a lower limit to the true values. 1117401700010 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1117401700011 STATUS (TABLE) Table II, page 611. 1117401700012 HISTORY (20220315A) BP 1117401700013 ENDBIB 11 0 1117401700014 NOCOMMON 0 0 1117401700015 DATA 4 1 1117401700016 EN EN-RSL DATA-MIN DATA-ERR 1117401700017 MEV MEV NO-DIM NO-DIM 1117401700018 9.5E+01 2.6E+01 0.42 0.015 1117401700019 ENDDATA 3 0 1117401700020 ENDSUBENT 19 0 1117401799999 SUBENT 11174018 20220315 14981117401800001 BIB 5 11 1117401800002 REACTION ((29-CU-0(N,INL)29-CU-0,,SIG)/(29-CU-0(N,TOT),,SIG)) 1117401800003 METHOD The inelastic cross-section measurements are subject 1117401800004 to greater sources of error. The "poor geometry" 1117401800005 detector count inelastically scattered neutrons or 1117401800006 neutrons ejected from nuclei if their energies are 1117401800007 above the threshold for bismuth fission. The 1117401800008 inelastic cross sections obtained, therefore, 1117401800009 represent a lower limit to the true values. 1117401800010 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1117401800011 STATUS (TABLE) Table II, page 611. 1117401800012 HISTORY (20220315A) BP 1117401800013 ENDBIB 11 0 1117401800014 NOCOMMON 0 0 1117401800015 DATA 4 1 1117401800016 EN EN-RSL DATA-MIN DATA-ERR 1117401800017 MEV MEV NO-DIM NO-DIM 1117401800018 9.5E+01 2.6E+01 0.39 0.005 1117401800019 ENDDATA 3 0 1117401800020 ENDSUBENT 19 0 1117401899999 SUBENT 11174019 20220315 14981117401900001 BIB 5 11 1117401900002 REACTION ((82-PB-0(N,INL)82-PB-0,,SIG)/(82-PB-0(N,TOT),,SIG)) 1117401900003 METHOD The inelastic cross-section measurements are subject 1117401900004 to greater sources of error. The "poor geometry" 1117401900005 detector count inelastically scattered neutrons or 1117401900006 neutrons ejected from nuclei if their energies are 1117401900007 above the threshold for bismuth fission. The 1117401900008 inelastic cross sections obtained, therefore, 1117401900009 represent a lower limit to the true values. 1117401900010 ERR-ANALYS (DATA-ERR) No details on sources of uncertainties. 1117401900011 STATUS (TABLE) Table II, page 611. 1117401900012 HISTORY (20220315A) BP 1117401900013 ENDBIB 11 0 1117401900014 NOCOMMON 0 0 1117401900015 DATA 4 1 1117401900016 EN EN-RSL DATA-MIN DATA-ERR 1117401900017 MEV MEV NO-DIM NO-DIM 1117401900018 9.5E+01 2.6E+01 0.39 0.01 1117401900019 ENDDATA 3 0 1117401900020 ENDSUBENT 19 0 1117401999999 ENDENTRY 19 0 1117499999999