ENTRY 20004 20181026 22732000400000001 SUBENT 20004001 20181026 22732000400100001 BIB 11 61 2000400100002 INSTITUTE (2UK HAR) 2000400100003 REFERENCE (J,NP,24,274,1961) 2000400100004 AUTHOR (D.L.Allan) 2000400100005 TITLE An experimental test of the statistical theory of 2000400100006 nuclear reactions 2000400100007 INC-SOURCE (D-T) Deuteron-tritium reaction. 2000400100008 SAMPLE Most of the targets were isotropically pure (> 90 %) 2000400100009 and they were deposited upon the 0.01 cm gold strips as2000400100010 the element, oxide or carbonate (halogen targets were 2000400100011 prepared from silver or tin halides). Some of the 2000400100012 deposits were electroplated and others were laid down 2000400100013 as compacted powders to form layers of thickness 2000400100014 varying from 6 to 40 mg/cm2. 2000400100015 0.2 to 0.5 mg/cm2 of polystyrene binder was added to 2000400100016 some of the powder targets to obtain a mechanically 2000400100017 stable deposit. 2000400100018 A Pb3O4 target was exposed simultaneously with the 2000400100019 oxide and carbonate targets in order to measure the 2000400100020 contribution of protons from the 0-16(n,p)N-16 2000400100021 reaction (Q = -9.6 MeV). 2000400100022 METHOD (STTA) Direct detection of protons. 2000400100023 .The apparatus is rotating round its axis of symmetry 2000400100024 once every two minutes in order to eliminate 2000400100025 background anisotropy. 2000400100026 DETECTOR (TRD) Photographic plate track detector, 2000400100027 2.5 cm * 2.5 cm, 300 mum thick Ilford C2 photographic 2000400100028 plate cemented in the centre of a 8 cm diam. 2000400100029 aluminium disc. 2000400100030 .It was surrounded by a 2.54 cm wide 0.05 cm thick gold2000400100031 anular band with six 2.0 cm * 1.2 cm rectangular 2000400100032 windows through which charged particles from six 2000400100033 different targets could reach the plate. 2000400100034 .Plate and target placed in a cylindrical drum lined 2000400100035 with 0.05 cm gold. 2000400100036 .The whole assembly placed in aluminium alloy vacuum 2000400100037 chamber. 2000400100038 .Plate screened from direct neutrons by 15 cm long 2000400100039 1.3 cm diameter copper rod with axis perpendicular on 2000400100040 the plate. 2000400100041 .The neutron source is on the axis of this rod at 2000400100042 7.6 cm from the end and the anular band is seen under 2000400100043 a half angle of 8.5 degrees. 2000400100044 .The rod is at right angle to the deuteron beam. 2000400100045 COMMENT Measurements are in favour of Fermi-gas model for 2000400100046 these nuclides especially with respect to the 2000400100047 theoretically calculated cross sections as compared 2000400100048 with the measured ones, the shape of the proton 2000400100049 spectra fitted to both theories in the region 2000400100050 which was free from (n,n+p) contamination. 2000400100051 CORRECTION (n,np) contribution is subtracted to obtain 2000400100052 (n,p) cross section 2000400100053 HISTORY (19700823C) 2000400100054 (19700826T) From NEUDADA 2000400100055 (20181026A) SD:Updated to new date formats,lower case. 2000400100056 REACTION code corrected in several Subents. Angle was 2000400100057 added to several Subents. BIB updated. 2000400100058 Several Subents were merged (002+003; 004+005; 006+007;2000400100059 009+010; 011+012; 016+017; 021+22; 026+027; 031+032; 2000400100060 033+034; 038+039; 040+041; 043+044; 045+046; 047+048; 2000400100061 052+053; 054+055; 057+058; 059+060; 064+065; 069+070; 2000400100062 071+072; 076+077; 081+082; 086+087; 091+092; 095+096). 2000400100063 ENDBIB 61 0 2000400100064 COMMON 1 3 2000400100065 EN 2000400100066 MEV 2000400100067 14. 2000400100068 ENDCOMMON 3 0 2000400100069 ENDSUBENT 68 0 2000400199999 SUBENT 20004002 20181026 22732000400200001 BIB 8 30 2000400200002 REACTION 1(11-NA-23(N,P)10-NE-23,,DA,,4PI) 2000400200003 2(11-NA-23(N,P)10-NE-23,,DA,,4PI) 2000400200004 ANALYSIS Histograms as a function of angle from 0 to 2000400200005 360 degr. in 2 degr. steps give six peaks with a 2000400200006 small uniform background to be subtracted. 2000400200007 .Histograms as a function of energy from 2 or 3 MeV to 2000400200008 12 MeV in steps of 0.5 MeV or each target peak. 2000400200009 (4PI1A) 4*Pi*differential cross section assuming that 2000400200010 the direct cross section is negligible at this angle 2000400200011 and that the compound cross section is isotropic. 2000400200012 1 Plots of ln(ro(E)) against E with ro based 2000400200013 on constant nuclear temperature model in order 2000400200014 to separate sigma(n,p) from sigma(n,n p). 2000400200015 2 Plots of ln(ro(U)) against (square root(U)) based on 2000400200016 the Fermi gas model in order to separate sigma(n,p) 2000400200017 from sigma(n,n p). 2000400200018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000400200019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000400200020 CORRECTION .Corrected for background and 2000400200021 isotopic composition of the enriched targets. 2000400200022 .The extrapolation of the proton spectrum below the 2000400200023 bias energy (3 MeV) amounts to a fairly constant 40% 2000400200024 for each nuclide. 2000400200025 ERR-ANALYS (DATA-ERR) Error given includes: 2000400200026 .statistical error from track counting, 2000400200027 .errors due to proton spectrum extrapolation. 2000400200028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000400200029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000400200030 added to REACTION code. REACTION (2) was added. Data 2000400200031 from Subent 003 were added. MONIT-REF, ANG added. 2000400200032 ENDBIB 30 0 2000400200033 NOCOMMON 0 0 2000400200034 DATA 4 1 2000400200035 ANG DATA 1DATA-ERR 1DATA 2 2000400200036 ADEG B B B 2000400200037 120. 0.057 0.020 0.050 2000400200038 ENDDATA 3 0 2000400200039 ENDSUBENT 38 0 2000400299999 NOSUBENT 20004003 20181026 22732000400300001 SUBENT 20004004 20181026 22732000400400001 BIB 8 30 2000400400002 REACTION 1(12-MG-24(N,P)11-NA-24,,DA,,4PI) 2000400400003 2(12-MG-24(N,P)11-NA-24,,DA,,4PI) 2000400400004 ANALYSIS Histograms as a function of angle from 0 to 2000400400005 360 degrees in 2 degree steps give six peaks with a 2000400400006 small uniform background to be subtracted. 2000400400007 .Histograms as a function of energy from 2 or 3 MeV to 2000400400008 12 MeV in steps of 0.5 MeV or each target peak. 2000400400009 (4PI1A) 4*Pi*differential cross section assuming that 2000400400010 the direct cross section is negligible at this angle 2000400400011 and that the compound cross section is isotropic. 2000400400012 1 Plots of ln(ro(E)) against E with ro based 2000400400013 on constant nuclear temperature model in order 2000400400014 to separate.Sigma(n,p) from sigma(n,n p). 2000400400015 2 Plots of ln(ro(U)) against (square root(U)) 2000400400016 based on the Fermi gas model in order to separate 2000400400017 sigma(n,p) from sigma(n,n p). 2000400400018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000400400019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000400400020 CORRECTION .Corrected for background and 2000400400021 .isotopic composition of the enriched targets. 2000400400022 .The extrapolation of the proton spectrum below the 2000400400023 bias energy (3 MeV) amounts to a fairly constant 40% 2000400400024 for each nuclide. 2000400400025 ERR-ANALYS (DATA-ERR) Error given includes: 2000400400026 .statistical error from track counting, 2000400400027 .errors due to proton spectrum extrapolation. 2000400400028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000400400029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000400400030 added to REACTION code. REACTION (2) was added. Data 2000400400031 from Subent 005 were added. MONIT-REF, ANG added. 2000400400032 ENDBIB 30 0 2000400400033 NOCOMMON 0 0 2000400400034 DATA 4 1 2000400400035 ANG DATA 1DATA-ERR 1DATA 2 2000400400036 ADEG B B B 2000400400037 120. 0.118 0.016 0.110 2000400400038 ENDDATA 3 0 2000400400039 ENDSUBENT 38 0 2000400499999 NOSUBENT 20004005 20181026 22732000400500001 SUBENT 20004006 20181026 22732000400600001 BIB 8 30 2000400600002 REACTION 1(12-MG-25(N,P)11-NA-25,,DA,,4PI) 2000400600003 2(12-MG-25(N,P)11-NA-25,,DA,,4PI) 2000400600004 ANALYSIS Histograms as a function of angle from 0 to 2000400600005 360 degrees in 2 degree steps give six peaks with a 2000400600006 small uniform background to be subtracted. 2000400600007 .Histograms as a function of energy from 2 or 3 MeV to 2000400600008 12 MeV in steps of 0.5 MeV or each target peak. 2000400600009 (4PI1A) 4*Pi*differential cross section assuming that 2000400600010 the direct cross section is negligible at this angle 2000400600011 and that the compound cross section is isotropic. 2000400600012 1 Plots of ln(ro(E)) against E with ro based 2000400600013 on constant nuclear temperature model in order 2000400600014 to separate sigma(n,p) from sigma(n,n p). 2000400600015 2 Plots of ln(ro(U)) against (square root(U)) 2000400600016 based on the fermi gas model in order to separate 2000400600017 sigma(n,p) from sigma(n,n p). 2000400600018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000400600019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000400600020 CORRECTION .Corrected for background and 2000400600021 .isotopic composition of the enriched targets. 2000400600022 .The extrapolation of the proton spectrum below the 2000400600023 bias energy (3 MeV) amounts to a fairly constant 40% 2000400600024 for each nuclide. 2000400600025 ERR-ANALYS (DATA-ERR) Error given includes: 2000400600026 .statistical error from track counting, 2000400600027 .errors due to proton spectrum extrapolation. 2000400600028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000400600029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000400600030 added to REACTION code. REACTION (2) was added. Data 2000400600031 from Subent 007 were added. MONIT-REF, ANG added. 2000400600032 ENDBIB 30 0 2000400600033 NOCOMMON 0 0 2000400600034 DATA 4 1 2000400600035 ANG DATA 1DATA-ERR 1DATA 2 2000400600036 ADEG B B B 2000400600037 120. 0.067 0.010 0.063 2000400600038 ENDDATA 3 0 2000400600039 ENDSUBENT 38 0 2000400699999 NOSUBENT 20004007 20181026 22732000400700001 SUBENT 20004008 20181026 22732000400800001 BIB 6 11 2000400800002 REACTION (12-MG-25(0,0),,TEM) 2000400800003 For (n,p) reaction at 120 degrees (compound part). 2000400800004 ANALYSIS From plots of proton spectra assuming the 2000400800005 constant nuclear temperature statistical model. 2000400800006 COMMENT The value of the nuclear temperature of the residual 2000400800007 nucleus formed in a (n,n+p) reaction varied between 2000400800008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000400800009 temperature is given. 2000400800010 ERR-ANALYS (ERR-S) Statistical errors 2000400800011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000400800012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000400800013 ENDBIB 11 0 2000400800014 NOCOMMON 0 0 2000400800015 DATA 2 1 2000400800016 DATA ERR-S 2000400800017 MEV MEV 2000400800018 1.5 0.2 2000400800019 ENDDATA 3 0 2000400800020 ENDSUBENT 19 0 2000400899999 SUBENT 20004009 20181026 22732000400900001 BIB 8 30 2000400900002 REACTION 1(12-MG-26(N,P)11-NA-26,,DA,,4PI) 2000400900003 2(12-MG-26(N,P)11-NA-26,,DA,,4PI) 2000400900004 ANALYSIS Histograms as a function of angle from 0 to 2000400900005 360 degrees in 2 degree steps give six peaks with a 2000400900006 small uniform background to be subtracted. 2000400900007 .Histograms as a function of energy from 2 or 3 MeV to 2000400900008 12 MeV in steps of 0.5 MeV or each target peak. 2000400900009 (4PI1A) 4*Pi*differential cross section assuming that 2000400900010 the direct cross section is negligible at this angle 2000400900011 and that the compound cross section is isotropic. 2000400900012 1 Plots of ln(ro(E)) against E with ro based 2000400900013 on constant nuclear temperature model in order 2000400900014 to separate sigma(n,p) from sigma(n,n p). 2000400900015 2 Plots of ln(ro(U)) against (square root(U)) 2000400900016 based on the fermi gas model in order to separate 2000400900017 sigma(n,p) from sigma(n,n p). 2000400900018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000400900019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000400900020 CORRECTION .Corrected for background and 2000400900021 .isotopic composition of the enriched targets. 2000400900022 .The extrapolation of the proton spectrum below the 2000400900023 bias energy (3 MeV) amounts to a fairly constant 40% 2000400900024 for each nuclide. 2000400900025 ERR-ANALYS (DATA-ERR) Error given includes: 2000400900026 .statistical error from track counting, 2000400900027 .errors due to proton spectrum extrapolation. 2000400900028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000400900029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000400900030 added to REACTION code. REACTION (2) was added. Data 2000400900031 from Subent 010 were added. MONIT-REF, ANG added. 2000400900032 ENDBIB 30 0 2000400900033 NOCOMMON 0 0 2000400900034 DATA 4 1 2000400900035 ANG DATA 1DATA-ERR 1DATA 2 2000400900036 ADEG B B B 2000400900037 120. 0.027 0.007 0.027 2000400900038 ENDDATA 3 0 2000400900039 ENDSUBENT 38 0 2000400999999 NOSUBENT 20004010 20181026 22732000401000001 SUBENT 20004011 20181026 22732000401100001 BIB 8 30 2000401100002 REACTION 1(13-AL-27(N,P)12-MG-27,,DA,,4PI) 2000401100003 2(13-AL-27(N,P)12-MG-27,,DA,,4PI) 2000401100004 ANALYSIS Histograms as a function of angle from 0 to 2000401100005 360 degrees in 2 degree steps give six peaks with a 2000401100006 small uniform background to be subtracted. 2000401100007 .Histograms as a function of energy from 2 or 3 MeV to 2000401100008 12 MeV in steps of 0.5 MeV or each target peak. 2000401100009 (4PI1A) 4*Pi*differential cross section assuming that 2000401100010 the direct cross section is negligible at this angle 2000401100011 and that the compound cross section is isotropic. 2000401100012 1 Plots of ln(ro(e)) against E with ro based 2000401100013 on constant nuclear temperature model in order 2000401100014 to separate sigma(n,p) from sigma(n,n p). 2000401100015 2 Plots of ln(ro(U)) against (square root(U)) 2000401100016 based on the fermi gas model in order to separate 2000401100017 sigma(n,p) from sigma(n,n p). 2000401100018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000401100019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000401100020 CORRECTION .Corrected for background and 2000401100021 .isotopic composition of the enriched targets. 2000401100022 .The extrapolation of the proton spectrum below the 2000401100023 bias energy (3 MeV) amounts to a fairly constant 40% 2000401100024 for each nuclide. 2000401100025 ERR-ANALYS (DATA-ERR) Error given includes: 2000401100026 .statistical error from track counting, 2000401100027 .errors due to proton spectrum extrapolation. 2000401100028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000401100029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000401100030 added to REACTION code. REACTION (2) was added. Data 2000401100031 from Subent 012 were added. MONIT-REF, ANG added. 2000401100032 ENDBIB 30 0 2000401100033 NOCOMMON 0 0 2000401100034 DATA 4 1 2000401100035 ANG DATA 1DATA-ERR 1DATA 2 2000401100036 ADEG B B B 2000401100037 120. 0.087 0.011 0.076 2000401100038 ENDDATA 3 0 2000401100039 ENDSUBENT 38 0 2000401199999 NOSUBENT 20004012 20181026 22732000401200001 SUBENT 20004013 20181026 22732000401300001 BIB 8 26 2000401300002 REACTION (13-AL-27(N,N+P)12-MG-26,,DA,,4PI) 2000401300003 ANALYSIS Histograms as a function of angle from 0 to 2000401300004 360 degrees in 2 degree steps give six peaks with a 2000401300005 small uniform background to be subtracted. 2000401300006 .Histograms as a function of energy from 2 or 3 MeV to 2000401300007 12 MeV in steps of 0.5 MeV or each target peak. 2000401300008 (4PI1A) 4*Pi*differential cross section assuming that 2000401300009 the direct cross section is negligible at this angle 2000401300010 and that the compound cross section is isotropic. 2000401300011 Subtraction of sigma(n,p) cross section 2000401300012 determined by statistical plot method from the total 2000401300013 proton emission cross section. 2000401300014 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000401300015 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000401300016 CORRECTION .Corrected for background and 2000401300017 .isotopic composition of the enriched targets. 2000401300018 .The extrapolation of the proton spectrum below the 2000401300019 bias energy (3 MeV) amounts to a fairly constant 40% 2000401300020 for each nuclide. 2000401300021 ERR-ANALYS (DATA-ERR) Error given includes: 2000401300022 .statistical error from track counting, 2000401300023 .errors due to proton spectrum extrapolation. 2000401300024 .Errors are estimated equal to those of sigma(n,p). 2000401300025 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000401300026 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000401300027 added to REACTION code. MONIT-REF, ANG added. 2000401300028 ENDBIB 26 0 2000401300029 NOCOMMON 0 0 2000401300030 DATA 3 1 2000401300031 ANG DATA DATA-ERR 2000401300032 ADEG B B 2000401300033 120. 0.053 0.011 2000401300034 ENDDATA 3 0 2000401300035 ENDSUBENT 34 0 2000401399999 SUBENT 20004014 20181026 22732000401400001 BIB 4 7 2000401400002 REACTION ((13-AL-27(N,N+P)12-MG-26,,DA,,4PI)/ 2000401400003 (13-AL-27(N,P)12-MG-27,,DA,,4PI)) 2000401400004 ERR-ANALYS Not given. 2000401400005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000401400006 (DEP,20004013) Cr. section (n,n+p) 2000401400007 (DEP,20004011) REACTION (2) from Subent 011. 2000401400008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000401400009 ENDBIB 7 0 2000401400010 NOCOMMON 0 0 2000401400011 DATA 2 1 2000401400012 ANG DATA 2000401400013 ADEG NO-DIM 2000401400014 120. 0.7 2000401400015 ENDDATA 3 0 2000401400016 ENDSUBENT 15 0 2000401499999 SUBENT 20004015 20181026 22732000401500001 BIB 6 11 2000401500002 REACTION (13-AL-28(0,0),,TEM) 2000401500003 For (n,p) reaction at 120 degrees (compound part). 2000401500004 ANALYSIS From plots of proton spectra assuming the 2000401500005 constant nuclear temperature statistical model. 2000401500006 COMMENT The value of the nuclear temperature of the residual 2000401500007 nucleus formed in a (n,n p) reaction varied between 2000401500008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000401500009 temperature is given. 2000401500010 STATUS (TABLE) Table 2, Nucl.Phys.,24,P.292. 2000401500011 ERR-ANALYS (ERR-S) Statistical errors in the plot. 2000401500012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000401500013 ENDBIB 11 0 2000401500014 NOCOMMON 0 0 2000401500015 DATA 2 1 2000401500016 DATA ERR-S 2000401500017 MEV MEV 2000401500018 1.5 0.2 2000401500019 ENDDATA 3 0 2000401500020 ENDSUBENT 19 0 2000401599999 SUBENT 20004016 20181026 22732000401600001 BIB 8 30 2000401600002 REACTION 1(14-SI-28(N,P)13-AL-28,,DA,,4PI) 2000401600003 2(14-SI-28(N,P)13-AL-28,,DA,,4PI) 2000401600004 ANALYSIS Histograms as a function of angle from 0 to 2000401600005 360 degrees in 2 degree steps give six peaks with a 2000401600006 small uniform background to be subtracted. 2000401600007 .Histograms as a function of energy from 2 or 3 MeV to 2000401600008 12 MeV in steps of 0.5 MeV or each target peak. 2000401600009 (4PI1A) 4*Pi*differential cross section assuming that 2000401600010 the direct cross section is negligible at this angle 2000401600011 and that the compound cross section is isotropic. 2000401600012 1 Plots of ln(ro(E)) against E with ro based 2000401600013 on constant nuclear temperature model in order 2000401600014 to separate sigma(n,p) from sigma(n,n p). 2000401600015 2 Plots of ln(ro(U)) against (square root(U)) 2000401600016 based on the Fermi gas model in order to separate 2000401600017 sigma(n,p) from sigma(n,n p). 2000401600018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000401600019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000401600020 CORRECTION .Corrected for background and 2000401600021 .isotopic composition of the enriched targets. 2000401600022 .The extrapolation of the proton spectrum below the 2000401600023 bias energy (3 MeV) amounts to a fairly constant 40% 2000401600024 for each nuclide. 2000401600025 ERR-ANALYS (DATA-ERR) Error given includes: 2000401600026 .statistical error from track counting, 2000401600027 .errors due to proton spectrum extrapolation. 2000401600028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000401600029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000401600030 added to REACTION code. REACTION (2) was added. Data 2000401600031 from Subent 017 were added. MONIT-REF, ANG added. 2000401600032 ENDBIB 30 0 2000401600033 NOCOMMON 0 0 2000401600034 DATA 4 1 2000401600035 ANG DATA 1DATA-ERR 1DATA 2 2000401600036 ADEG B B B 2000401600037 120. 0.243 0.022 0.246 2000401600038 ENDDATA 3 0 2000401600039 ENDSUBENT 38 0 2000401699999 NOSUBENT 20004017 20181026 22732000401700001 SUBENT 20004018 20181026 22732000401800001 BIB 8 26 2000401800002 REACTION (14-SI-28(N,N+P)13-AL-27,,DA,,4PI) 2000401800003 ANALYSIS Histograms as a function of angle from 0 to 2000401800004 360 degrees in 2 degree steps give six peaks with a 2000401800005 small uniform background to be subtracted. 2000401800006 .Histograms as a function of energy from 2 or 3 MeV to 2000401800007 12 MeV in steps of 0.5 MeV or each target peak. 2000401800008 (4PI1A) 4*Pi*differential cross section assuming that 2000401800009 the direct cross section is negligible at this angle 2000401800010 and that the compound cross section is isotropic. 2000401800011 Subtraction of sigma(n,p) cross section 2000401800012 determined by statistical plot method from the total 2000401800013 proton emission cross section. 2000401800014 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000401800015 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000401800016 CORRECTION .Corrected for background and 2000401800017 .isotopic composition of the enriched targets. 2000401800018 .The extrapolation of the proton spectrum below the 2000401800019 bias energy (3 MeV) amounts to a fairly constant 40% 2000401800020 for each nuclide. 2000401800021 ERR-ANALYS (DATA-ERR) Error given includes: 2000401800022 .statistical error from track counting, 2000401800023 .errors due to proton spectrum extrapolation. 2000401800024 .Errors are estimated equal to those of sigma(n,p). 2000401800025 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000401800026 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000401800027 added to REACTION code. MONIT-REF, ANG added. 2000401800028 ENDBIB 26 0 2000401800029 NOCOMMON 0 0 2000401800030 DATA 3 1 2000401800031 ANG DATA DATA-ERR 2000401800032 ADEG B B 2000401800033 120. 0.027 0.022 2000401800034 ENDDATA 3 0 2000401800035 ENDSUBENT 34 0 2000401899999 SUBENT 20004019 20181026 22732000401900001 BIB 4 7 2000401900002 REACTION ((14-SI-28(N,N+P)13-AL-27,,DA,,4PI)/ 2000401900003 (14-SI-28(N,P)13-AL-28,,DA,,4PI)) 2000401900004 ERR-ANALYS Not given. 2000401900005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000401900006 (DEP,20004018) Cr. section (n,n+p) 2000401900007 (DEP,20004016) REACTION (2) from Subent 016. 2000401900008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000401900009 ENDBIB 7 0 2000401900010 NOCOMMON 0 0 2000401900011 DATA 2 1 2000401900012 ANG DATA 2000401900013 ADEG NO-DIM 2000401900014 120. 0.11 2000401900015 ENDDATA 3 0 2000401900016 ENDSUBENT 15 0 2000401999999 SUBENT 20004020 20181026 22732000402000001 BIB 6 11 2000402000002 REACTION (14-SI-29(0,0),,TEM) 2000402000003 For (n,p) reaction at 120 degrees (compound part). 2000402000004 ANALYSIS From plots of proton spectra assuming the 2000402000005 constant nuclear temperature statistical model. 2000402000006 COMMENT The value of the nuclear temperature of the residual 2000402000007 nucleus formed in a (n,n p) reaction varied between 2000402000008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000402000009 temperature is given. 2000402000010 ERR-ANALYS (ERR-S) Statistical errors 2000402000011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000402000012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000402000013 ENDBIB 11 0 2000402000014 NOCOMMON 0 0 2000402000015 DATA 2 1 2000402000016 DATA ERR-S 2000402000017 MEV MEV 2000402000018 1.5 0.2 2000402000019 ENDDATA 3 0 2000402000020 ENDSUBENT 19 0 2000402099999 SUBENT 20004021 20181026 22732000402100001 BIB 8 34 2000402100002 REACTION 1(15-P-31(N,P)14-SI-31,,DA,,4PI) 2000402100003 Separation of sigma(n,p) from sigma(n,n'p) based on 2000402100004 nuclear temperature model 2000402100005 2(15-P-31(N,P)14-SI-31,,DA,,4PI) 2000402100006 Separation of sigma(n,p) from sigma(n,n'p) based on 2000402100007 Fermi gas model 2000402100008 ANALYSIS Histograms as a function of angle from 0 to 2000402100009 360 degrees in 2 degree steps give six peaks with a 2000402100010 small uniform background to be subtracted. 2000402100011 .Histograms as a function of energy from 2 or 3 MeV to 2000402100012 12 MeV in steps of 0.5 MeV or each target peak. 2000402100013 (4PI1A) 4*Pi*differential cross section assuming that 2000402100014 the direct cross section is negligible at this angle 2000402100015 and that the compound cross section is isotropic. 2000402100016 1 Plots of ln(ro(E)) against E with ro based on 2000402100017 constant nuclear temperature model in order 2000402100018 to separate sigma(n,p) from sigma(n,n p). 2000402100019 2 Plots of ln(ro(u)) against (square root(u)) 2000402100020 based on the Fermi gas model in order to separate 2000402100021 sigma(n,p) from sigma(n,n p). 2000402100022 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000402100023 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000402100024 CORRECTION .Corrected for background and 2000402100025 .isotopic composition of the enriched targets. 2000402100026 .The extrapolation of the proton spectrum below the 2000402100027 bias energy (3 MeV) amounts to a fairly constant 40% 2000402100028 for each nuclide. 2000402100029 ERR-ANALYS (DATA-ERR) Error given includes: 2000402100030 .statistical error from track counting, 2000402100031 .errors due to proton spectrum extrapolation. 2000402100032 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000402100033 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000402100034 added to REACTION code. REACTION (2) was added. Data 2000402100035 from Subent 022 were added. MONIT-REF, ANG added. 2000402100036 ENDBIB 34 0 2000402100037 NOCOMMON 0 0 2000402100038 DATA 4 1 2000402100039 ANG DATA 1DATA-ERR 1DATA 2 2000402100040 ADEG B B B 2000402100041 120. 0.184 0.014 0.114 2000402100042 ENDDATA 3 0 2000402100043 ENDSUBENT 42 0 2000402199999 NOSUBENT 20004022 20181026 22732000402200001 SUBENT 20004023 20181026 22732000402300001 BIB 8 28 2000402300002 REACTION (15-P-31(N,N+P)14-SI-30,,DA,,4PI) 2000402300003 ANALYSIS Histograms as a function of angle from 0 to 2000402300004 360 degrees in 2 degree steps give six peaks with a 2000402300005 small uniform background to be subtracted. 2000402300006 .Normalization to obtain the absolute differential 2000402300007 cross section at 120 degrees. 2000402300008 .Histograms as a function of energy from 2 or 3 MeV to 2000402300009 12 MeV in steps of 0.5 MeV or each target peak. 2000402300010 (4PI1A) 4*Pi*differential cross section assuming that 2000402300011 the direct cross section is negligible at this angle 2000402300012 and that the compound cross section is isotropic. 2000402300013 Subtraction of sigma(n,p) cross section 2000402300014 determined by statistical plot method from the total 2000402300015 proton emission cross section. 2000402300016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000402300017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000402300018 CORRECTION .Corrected for background and 2000402300019 .isotopic composition of the enriched targets. 2000402300020 .The extrapolation of the proton spectrum below the 2000402300021 bias energy (3 MeV) amounts to a fairly constant 40% 2000402300022 for each nuclide. 2000402300023 ERR-ANALYS (DATA-ERR) Error given includes: 2000402300024 .statistical error from track counting, 2000402300025 .errors due to proton spectrum extrapolation. 2000402300026 .Errors are estimated equal to those of sigma(n,p). 2000402300027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000402300028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000402300029 added to REACTION code. MONIT-REF, ANG added. 2000402300030 ENDBIB 28 0 2000402300031 NOCOMMON 0 0 2000402300032 DATA 3 1 2000402300033 ANG DATA DATA-ERR 2000402300034 ADEG B B 2000402300035 120. 0.163 0.014 2000402300036 ENDDATA 3 0 2000402300037 ENDSUBENT 36 0 2000402399999 SUBENT 20004024 20181026 22732000402400001 BIB 4 7 2000402400002 REACTION ((15-P-31(N,N+P)14-SI-30,,DA,,4PI)/ 2000402400003 (15-P-31(N,P)14-SI-31,,DA,,4PI)) 2000402400004 ERR-ANALYS Not given. 2000402400005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000402400006 (DEP,20004023) Cr. section (n,n+p) 2000402400007 (DEP,20004021) REACTION (2) from Subent 021. 2000402400008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000402400009 ENDBIB 7 0 2000402400010 NOCOMMON 0 0 2000402400011 DATA 2 1 2000402400012 ANG DATA 2000402400013 ADEG NO-DIM 2000402400014 120. 1.43 2000402400015 ENDDATA 3 0 2000402400016 ENDSUBENT 15 0 2000402499999 SUBENT 20004025 20181026 22732000402500001 BIB 6 14 2000402500002 REACTION (15-P-32(0,0),,TEM) 2000402500003 For the (n,p) and (n,n p) reactions at 120 degrees 2000402500004 (compound part). 2000402500005 ANALYSIS From plots of proton spectra assuming the 2000402500006 constant nuclear temperature statistical model. 2000402500007 .The (n,n+p) spectrum dominates so that only one 2000402500008 straight line could be fitted. 2000402500009 COMMENT The value of the nuclear temperature of the residual 2000402500010 nucleus formed in a (n,n+p) reaction varied between 2000402500011 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000402500012 temperature is given. 2000402500013 ERR-ANALYS (ERR-S) Statistical errors 2000402500014 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000402500015 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000402500016 ENDBIB 14 0 2000402500017 NOCOMMON 0 0 2000402500018 DATA 2 1 2000402500019 DATA ERR-S 2000402500020 MEV MEV 2000402500021 1.2 0.1 2000402500022 ENDDATA 3 0 2000402500023 ENDSUBENT 22 0 2000402599999 SUBENT 20004026 20181026 22732000402600001 BIB 8 30 2000402600002 REACTION 1(16-S-32(N,P)15-P-32,,DA,,4PI) 2000402600003 2(16-S-32(N,P)15-P-32,,DA,,4PI) 2000402600004 ANALYSIS Histograms as a function of angle from 0 to 2000402600005 360 degrees in 2 degree steps give six peaks with a 2000402600006 small uniform background to be subtracted. 2000402600007 .Histograms as a function of energy from 2 or 3 MeV to 2000402600008 12 MeV in steps of 0.5 MeV or each target peak. 2000402600009 (4PI1A) 4*Pi*differential cross section assuming that 2000402600010 the direct cross section is negligible at this angle 2000402600011 and that the compound cross section is isotropic. 2000402600012 1 Plots of ln(ro(E)) against E with ro based 2000402600013 on constant nuclear temperature model in order 2000402600014 to separate sigma(n,p) from sigma(n,n+p). 2000402600015 Plots of ln(ro(U)) against (square root(U)) 2000402600016 2 based on the fermi gas model in order to separate 2000402600017 sigma(n,p) from sigma(n,n+p). 2000402600018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000402600019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000402600020 CORRECTION .Corrected for background and 2000402600021 .isotopic composition of the enriched targets. 2000402600022 .The extrapolation of the proton spectrum below the 2000402600023 bias energy (3 MeV) amounts to a fairly constant 40% 2000402600024 for each nuclide. 2000402600025 ERR-ANALYS (DATA-ERR) Error given includes: 2000402600026 .statistical error from track counting, 2000402600027 .errors due to proton spectrum extrapolation. 2000402600028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000402600029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000402600030 added to REACTION code. REACTION (2) was added. Data 2000402600031 from Subent 027 were added. MONIT-REF, ANG added. 2000402600032 ENDBIB 30 0 2000402600033 NOCOMMON 0 0 2000402600034 DATA 4 1 2000402600035 ANG DATA 1DATA-ERR 1DATA 2 2000402600036 ADEG B B B 2000402600037 120. 0.365 0.025 0.289 2000402600038 ENDDATA 3 0 2000402600039 ENDSUBENT 38 0 2000402699999 NOSUBENT 20004027 20181026 22732000402700001 SUBENT 20004028 20181026 22732000402800001 BIB 8 26 2000402800002 REACTION (16-S-32(N,N+P)15-P-31,,DA,,4PI) 2000402800003 ANALYSIS Histograms as a function of angle from 0 to 2000402800004 360 degrees in 2 degree steps give six peaks with a 2000402800005 small uniform background to be subtracted. 2000402800006 .Histograms as a function of energy from 2 or 3 MeV to 2000402800007 12 MeV in steps of 0.5 MeV or each target peak. 2000402800008 (4PI1A) 4*Pi*differential cross section assuming that 2000402800009 the direct cross section is negligible at this angle 2000402800010 and that the compound cross section is isotropic. 2000402800011 Subtraction of sigma(n,p) cross section 2000402800012 determined by statistical plot method from the total 2000402800013 proton emission cross section. 2000402800014 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000402800015 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000402800016 CORRECTION .Corrected for background and 2000402800017 .isotopic composition of the enriched targets. 2000402800018 .The extrapolation of the proton spectrum below the 2000402800019 bias energy (3 MeV) amounts to a fairly constant 40% 2000402800020 for each nuclide. 2000402800021 ERR-ANALYS (DATA-ERR) Error given includes: 2000402800022 .statistical error from track counting, 2000402800023 .errors due to proton spectrum extrapolation. 2000402800024 .Errors are estimated equal to those of sigma(n,p). 2000402800025 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000402800026 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000402800027 added to REACTION code. MONIT-REF, ANG added. 2000402800028 ENDBIB 26 0 2000402800029 NOCOMMON 0 0 2000402800030 DATA 3 1 2000402800031 ANG DATA DATA-ERR 2000402800032 ADEG B B 2000402800033 120. 0.105 0.025 2000402800034 ENDDATA 3 0 2000402800035 ENDSUBENT 34 0 2000402899999 SUBENT 20004029 20181026 22732000402900001 BIB 4 7 2000402900002 REACTION ((16-S-32(N,N+P)15-P-31,,DA,,4PI)/ 2000402900003 (16-S-32(N,P)15-P-32,,DA,,4PI)) 2000402900004 ERR-ANALYS Not given. 2000402900005 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000402900006 (DEP,20004028) Cr. section (n,n+p) 2000402900007 (DEP,20004026) REACTION (2) from Subent 026. 2000402900008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000402900009 ENDBIB 7 0 2000402900010 NOCOMMON 0 0 2000402900011 DATA 2 1 2000402900012 ANG DATA 2000402900013 ADEG NO-DIM 2000402900014 120. 0.26 2000402900015 ENDDATA 3 0 2000402900016 ENDSUBENT 15 0 2000402999999 SUBENT 20004030 20181026 22732000403000001 BIB 6 14 2000403000002 REACTION (16-S-33(0,0),,TEM) 2000403000003 For the (n,p) and (n,n p) reactions at 120 degrees 2000403000004 (compound part). 2000403000005 ANALYSIS From plots of proton spectra assuming the 2000403000006 constant nuclear temperature statistical model. 2000403000007 .The (n,n p) spectrum dominates so that only one 2000403000008 straight line could be fitted. 2000403000009 COMMENT The value of the nuclear temperature of the residual 2000403000010 nucleus formed in a (n,n p) reaction varied between 2000403000011 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000403000012 temperature is given. 2000403000013 ERR-ANALYS (ERR-S) Statistical errors 2000403000014 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000403000015 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000403000016 ENDBIB 14 0 2000403000017 NOCOMMON 0 0 2000403000018 DATA 2 1 2000403000019 DATA ERR-S 2000403000020 MEV MEV 2000403000021 1.2 0.1 2000403000022 ENDDATA 3 0 2000403000023 ENDSUBENT 22 0 2000403099999 SUBENT 20004031 20181026 22732000403100001 BIB 8 30 2000403100002 REACTION 1(17-CL-35(N,P)16-S-35,,DA,,4PI) 2000403100003 2(17-CL-35(N,P)16-S-35,,DA,,4PI) 2000403100004 ANALYSIS Histograms as a function of angle from 0 to 2000403100005 360 degrees in 2 degree steps give six peaks with a 2000403100006 small uniform background to be subtracted. 2000403100007 .Histograms as a function of energy from 2 or 3 MeV to 2000403100008 12 MeV in steps of 0.5 MeV or each target peak. 2000403100009 (4PI1A) 4*Pi*differential cross section assuming that 2000403100010 the direct cross section is negligible at this angle 2000403100011 and that the compound cross section is isotropic. 2000403100012 1 Plots of ln(ro(E)) against E with ro based 2000403100013 on constant nuclear temperature model in order 2000403100014 to separate sigma(n,p) from sigma(n,n p). 2000403100015 2 Plots of ln(ro(U)) against (square root(U)) 2000403100016 based on the Fermi gas model in order to separate 2000403100017 sigma(n,p) from sigma(n,n p). 2000403100018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000403100019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000403100020 CORRECTION .Corrected for background and 2000403100021 .isotopic composition of the enriched targets. 2000403100022 .The extrapolation of the proton spectrum below the 2000403100023 bias energy (3 MeV) amounts to a fairly constant 40% 2000403100024 for each nuclide. 2000403100025 ERR-ANALYS (DATA-ERR) Error given includes: 2000403100026 .statistical error from track counting, 2000403100027 .errors due to proton spectrum extrapolation. 2000403100028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000403100029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000403100030 added to REACTION code. REACTION (2) was added. Data 2000403100031 from Subent 032 were added. MONIT-REF, ANG added. 2000403100032 ENDBIB 30 0 2000403100033 NOCOMMON 0 0 2000403100034 DATA 4 1 2000403100035 ANG DATA 1DATA-ERR 1DATA 2 2000403100036 ADEG B B B 2000403100037 120. 0.125 0.038 0.107 2000403100038 ENDDATA 3 0 2000403100039 ENDSUBENT 38 0 2000403199999 NOSUBENT 20004032 20181026 22732000403200001 SUBENT 20004033 20181026 22732000403300001 BIB 8 30 2000403300002 REACTION 1(20-CA-40(N,P)19-K-40,,DA,,4PI) 2000403300003 2(20-CA-40(N,P)19-K-40,,DA,,4PI) 2000403300004 ANALYSIS Histograms as a function of angle from 0 to 2000403300005 360 degrees in 2 degree steps give six peaks with a 2000403300006 small uniform background to be subtracted. 2000403300007 .Histograms as a function of energy from 2 or 3 MeV to 2000403300008 12 MeV in steps of 0.5 MeV or each target peak. 2000403300009 (4PI1A) 4*Pi*differential cross section assuming that 2000403300010 the direct cross section is negligible at this angle 2000403300011 and that the compound cross section is isotropic. 2000403300012 1 Plots of ln(ro(E)) against E with ro based 2000403300013 on constant nuclear temperature model in order 2000403300014 to separate sigma(n,p) from sigma(n,n p). 2000403300015 2 Plots of ln(ro(U)) against (square root(U)) 2000403300016 based on the Fermi gas model in order to separate 2000403300017 sigma(n,p) from sigma(n,n p). 2000403300018 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000403300019 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000403300020 CORRECTION .Corrected for background and 2000403300021 .isotopic composition of the enriched targets. 2000403300022 .The extrapolation of the proton spectrum below the 2000403300023 bias energy (3 MeV) amounts to a fairly constant 40% 2000403300024 for each nuclide. 2000403300025 ERR-ANALYS (DATA-ERR) Error given includes: 2000403300026 .statistical error from track counting, 2000403300027 .errors due to proton spectrum extrapolation. 2000403300028 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000403300029 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000403300030 added to REACTION code. REACTION (2) was added. Data 2000403300031 from Subent 034 were added. MONIT-REF, ANG added. 2000403300032 ENDBIB 30 0 2000403300033 NOCOMMON 0 0 2000403300034 DATA 4 1 2000403300035 ANG DATA 1DATA-ERR 1DATA 2 2000403300036 ADEG B B B 2000403300037 120. 0.451 0.038 0.298 2000403300038 ENDDATA 3 0 2000403300039 ENDSUBENT 38 0 2000403399999 NOSUBENT 20004034 20181026 22732000403400001 SUBENT 20004035 20181026 22732000403500001 BIB 8 26 2000403500002 REACTION (20-CA-40(N,N+P)19-K-39,,DA,,4PI) 2000403500003 ANALYSIS Histograms as a function of angle from 0 to 2000403500004 360 degrees in 2 degree steps give six peaks with a 2000403500005 small uniform background to be subtracted. 2000403500006 .Normalization to obtain the absolute differential 2000403500007 cross section at 120 degrees. 2000403500008 (4PI1A) 4*Pi*differential cross section assuming that 2000403500009 the direct cross section is negligible at this angle 2000403500010 and that the compound cross section is isotropic. 2000403500011 Subtraction of sigma(n,p) cross section 2000403500012 determined by statistical plot method from the total 2000403500013 proton emission cross section. 2000403500014 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000403500015 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000403500016 CORRECTION .Corrected for background and 2000403500017 .isotopic composition of the enriched targets. 2000403500018 .The extrapolation of the proton spectrum below the 2000403500019 bias energy (3 MeV) amounts to a fairly constant 40% 2000403500020 for each nuclide. 2000403500021 ERR-ANALYS (DATA-ERR) Error given includes: 2000403500022 .statistical error from track counting, 2000403500023 .errors due to proton spectrum extrapolation. 2000403500024 .Errors are estimated equal to those of sigma(n,p). 2000403500025 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000403500026 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000403500027 added to REACTION code. MONIT-REF, ANG added. 2000403500028 ENDBIB 26 0 2000403500029 NOCOMMON 0 0 2000403500030 DATA 3 1 2000403500031 ANG DATA DATA-ERR 2000403500032 ADEG B B 2000403500033 120. 0.205 0.038 2000403500034 ENDDATA 3 0 2000403500035 ENDSUBENT 34 0 2000403599999 SUBENT 20004036 20181026 22732000403600001 BIB 4 7 2000403600002 REACTION ((20-CA-40(N,N+P)19-K-39,,DA,,4PI)/ 2000403600003 (20-CA-40(N,P)19-K-40,,DA,,4PI)) 2000403600004 ERR-ANALYS Not given. 2000403600005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000403600006 (DEP,20004035) Cr. section (n,n+p) 2000403600007 (DEP,20004033) REACTION (2) from Subent 033. 2000403600008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000403600009 ENDBIB 7 0 2000403600010 NOCOMMON 0 0 2000403600011 DATA 2 1 2000403600012 ANG DATA 2000403600013 ADEG NO-DIM 2000403600014 120. 0.69 2000403600015 ENDDATA 3 0 2000403600016 ENDSUBENT 15 0 2000403699999 SUBENT 20004037 20181026 22732000403700001 BIB 6 14 2000403700002 REACTION (20-CA-41(0,0),,TEM) 2000403700003 For the (n,p) and (n,n p) reactions at 120 degrees 2000403700004 (compound part). 2000403700005 ANALYSIS From plots of proton spectra assuming the 2000403700006 constant nuclear temperature statistical model. 2000403700007 .The (n,n p) spectrum dominates so that only one 2000403700008 straight line could be fitted. 2000403700009 COMMENT The value of the nuclear temperature of the residual 2000403700010 nucleus formed in a (n,n p) reaction varied between 2000403700011 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000403700012 temperature is given. 2000403700013 ERR-ANALYS (ERR-S) Statistical errors 2000403700014 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000403700015 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000403700016 ENDBIB 14 0 2000403700017 NOCOMMON 0 0 2000403700018 DATA 2 1 2000403700019 DATA ERR-S 2000403700020 MEV MEV 2000403700021 1.2 0.1 2000403700022 ENDDATA 3 0 2000403700023 ENDSUBENT 22 0 2000403799999 SUBENT 20004038 20181026 22732000403800001 BIB 8 32 2000403800002 REACTION 1(22-TI-46(N,P)21-SC-46,,DA,,4PI) 2000403800003 2(22-TI-46(N,P)21-SC-46,,DA,,4PI) 2000403800004 ANALYSIS Histograms as a function of angle from 0 to 2000403800005 360 degrees in 2 degree steps give six peaks with a 2000403800006 small uniform background to be subtracted. 2000403800007 .Normalization to obtain the absolute differential 2000403800008 cross section at 120 degrees. 2000403800009 .Histograms as a function of energy from 2 or 3 MeV to 2000403800010 12 MeV in steps of 0.5 MeV or each target peak. 2000403800011 (4PI1A) 4*Pi*differential cross section assuming that 2000403800012 the direct cross section is negligible at this angle 2000403800013 and that the compound cross section is isotropic. 2000403800014 1 Plots of ln(ro(E)) against E with ro based 2000403800015 on constant nuclear temperature model in order 2000403800016 to separate sigma(n,p) from sigma(n,n p). 2000403800017 2 Plots of ln(ro(U)) against (square root(U)) 2000403800018 based on the fermi gas model in order to separate 2000403800019 sigma(n,p) from sigma(n,n p). 2000403800020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000403800021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000403800022 CORRECTION .Corrected for background and 2000403800023 .isotopic composition of the enriched targets. 2000403800024 .The extrapolation of the proton spectrum below the 2000403800025 bias energy (3 MeV) amounts to a fairly constant 40% 2000403800026 for each nuclide. 2000403800027 ERR-ANALYS (DATA-ERR) Error given includes: 2000403800028 .statistical error from track counting, 2000403800029 .errors due to proton spectrum extrapolation. 2000403800030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000403800031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000403800032 added to REACTION code. REACTION (2) was added. Data 2000403800033 from Subent 039 were added. MONIT-REF, ANG added. 2000403800034 ENDBIB 32 0 2000403800035 NOCOMMON 0 0 2000403800036 DATA 4 1 2000403800037 ANG DATA 1DATA-ERR 1DATA 2 2000403800038 ADEG B B B 2000403800039 120. 0.203 0.021 0.196 2000403800040 ENDDATA 3 0 2000403800041 ENDSUBENT 40 0 2000403899999 NOSUBENT 20004039 20181026 22732000403900001 SUBENT 20004040 20181026 22732000404000001 BIB 8 32 2000404000002 REACTION 1(22-TI-47(N,P)21-SC-47,,DA,,4PI) 2000404000003 2(22-TI-47(N,P)21-SC-47,,DA,,4PI) 2000404000004 ANALYSIS Histograms as a function of angle from 0 to 2000404000005 360 degrees in 2 degree steps give six peaks with a 2000404000006 small uniform background to be subtracted. 2000404000007 .Normalization to obtain the absolute differential 2000404000008 cross section at 120 degrees. 2000404000009 .Histograms as a function of energy from 2 or 3 MeV to 2000404000010 12 MeV in steps of 0.5 MeV or each target peak. 2000404000011 (4PI1A) 4*Pi*differential cross section assuming that 2000404000012 the direct cross section is negligible at this angle 2000404000013 and that the compound cross section is isotropic. 2000404000014 1 Plots of ln(ro(E)) against E with ro based 2000404000015 on constant nuclear temperature model in order 2000404000016 to separate sigma(n,p) from sigma(n,n p). 2000404000017 2 Plots of ln(ro(U)) against (square root(U)) 2000404000018 based on the fermi gas model in order to separate 2000404000019 sigma(n,p) from sigma(n,n p). 2000404000020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000404000021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000404000022 CORRECTION .Corrected for background and 2000404000023 .isotopic composition of the enriched targets. 2000404000024 .The extrapolation of the proton spectrum below the 2000404000025 bias energy (3 MeV) amounts to a fairly constant 40% 2000404000026 for each nuclide. 2000404000027 ERR-ANALYS (DATA-ERR) Error given includes: 2000404000028 .statistical error from track counting, 2000404000029 .errors due to proton spectrum extrapolation. 2000404000030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000404000031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000404000032 added to REACTION code. REACTION (2) was added. Data 2000404000033 from Subent 041 were added. MONIT-REF, ANG added. 2000404000034 ENDBIB 32 0 2000404000035 NOCOMMON 0 0 2000404000036 DATA 4 1 2000404000037 ANG DATA 1DATA-ERR 1DATA 2 2000404000038 ADEG B B B 2000404000039 120. 0.112 0.015 0.111 2000404000040 ENDDATA 3 0 2000404000041 ENDSUBENT 40 0 2000404099999 NOSUBENT 20004041 20181026 22732000404100001 SUBENT 20004042 20181026 22732000404200001 BIB 6 11 2000404200002 REACTION (22-TI-47(0,0),,TEM) 2000404200003 For (n,p) reaction at 120 degrees (compound part). 2000404200004 ANALYSIS From plots of proton spectra assuming the 2000404200005 constant nuclear temperature statistical model. 2000404200006 COMMENT The value of the nuclear temperature of the residual 2000404200007 nucleus formed in a (n,n p) reaction varied between 2000404200008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000404200009 temperature is given. 2000404200010 ERR-ANALYS (ERR-S) Statistical errors 2000404200011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000404200012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000404200013 ENDBIB 11 0 2000404200014 NOCOMMON 0 0 2000404200015 DATA 2 1 2000404200016 DATA ERR-S 2000404200017 MEV MEV 2000404200018 1.25 0.1 2000404200019 ENDDATA 3 0 2000404200020 ENDSUBENT 19 0 2000404299999 SUBENT 20004043 20181026 22732000404300001 BIB 8 32 2000404300002 REACTION 1(22-TI-48(N,P)21-SC-48,,DA,,4PI) 2000404300003 2(22-TI-48(N,P)21-SC-48,,DA,,4PI) 2000404300004 ANALYSIS Histograms as a function of angle from 0 to 2000404300005 360 degrees in 2 degree steps give six peaks with a 2000404300006 small uniform background to be subtracted. 2000404300007 .Normalization to obtain the absolute differential 2000404300008 cross section at 120 degrees. 2000404300009 .Histograms as a function of energy from 2 or 3 MeV to 2000404300010 12 MeV in steps of 0.5 MeV or each target peak. 2000404300011 (4PI1A) 4*Pi*differential cross section assuming that 2000404300012 the direct cross section is negligible at this angle 2000404300013 and that the compound cross section is isotropic. 2000404300014 1 Plots of ln(ro(E)) against E with ro based 2000404300015 on constant nuclear temperature model in order 2000404300016 to separate sigma(n,p) from sigma(n,n p). 2000404300017 2 Plots of ln(ro(U)) against (square root(U)) 2000404300018 based on the Fermi gas model in order to separate 2000404300019 sigma(n,p) from sigma(n,n p). 2000404300020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000404300021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000404300022 CORRECTION .Corrected for background and 2000404300023 .isotopic composition of the enriched targets. 2000404300024 .The extrapolation of the proton spectrum below the 2000404300025 bias energy (3 MeV) amounts to a fairly constant 40% 2000404300026 for each nuclide. 2000404300027 ERR-ANALYS (DATA-ERR) Error given includes: 2000404300028 .statistical error from track counting, 2000404300029 .errors due to proton spectrum extrapolation. 2000404300030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000404300031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000404300032 added to REACTION code. REACTION (2) was added. Data 2000404300033 from Subent 044 were added. MONIT-REF, ANG added. 2000404300034 ENDBIB 32 0 2000404300035 NOCOMMON 0 0 2000404300036 DATA 4 1 2000404300037 ANG DATA 1DATA-ERR 1DATA 2 2000404300038 ADEG B B B 2000404300039 120. 0.029 0.008 0.029 2000404300040 ENDDATA 3 0 2000404300041 ENDSUBENT 40 0 2000404399999 NOSUBENT 20004044 20181026 22732000404400001 SUBENT 20004045 20181026 22732000404500001 BIB 8 32 2000404500002 REACTION 1(23-V-51(N,P)22-TI-51,,DA,,4PI) 2000404500003 2(23-V-51(N,P)22-TI-51,,DA,,4PI) 2000404500004 ANALYSIS Histograms as a function of angle from 0 to 2000404500005 360 degrees in 2 degree steps give six peaks with a 2000404500006 small uniform background to be subtracted. 2000404500007 .Normalization to obtain the absolute differential 2000404500008 cross section at 120 degrees. 2000404500009 .Histograms as a function of energy from 2 or 3 MeV to 2000404500010 12 MeV in steps of 0.5 MeV or each target peak. 2000404500011 (4PI1A) 4*Pi*differential cross section assuming that 2000404500012 the direct cross section is negligible at this angle 2000404500013 and that the compound cross section is isotropic. 2000404500014 1 Plots of ln(ro(E)) against E with ro based 2000404500015 on constant nuclear temperature model in order 2000404500016 to separate sigma(n,p) from sigma(n,n p). 2000404500017 2 Plots of ln(ro(U)) against (square root(U)) 2000404500018 based on the Fermi gas model in order to separate 2000404500019 sigma(n,p) from sigma(n,n p). 2000404500020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000404500021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000404500022 CORRECTION .Corrected for background and 2000404500023 .isotopic composition of the enriched targets. 2000404500024 .The extrapolation of the proton spectrum below the 2000404500025 bias energy (3 MeV) amounts to a fairly constant 40% 2000404500026 for each nuclide. 2000404500027 ERR-ANALYS (DATA-ERR) Error given includes: 2000404500028 .statistical error from track counting, 2000404500029 .errors due to proton spectrum extrapolation. 2000404500030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000404500031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000404500032 added to REACTION code. REACTION (2) was added. Data 2000404500033 from Subent 046 were added. MONIT-REF, ANG added. 2000404500034 ENDBIB 32 0 2000404500035 NOCOMMON 0 0 2000404500036 DATA 4 1 2000404500037 ANG DATA 1DATA-ERR 1DATA 2 2000404500038 ADEG B B B 2000404500039 120. 0.020 0.007 0.023 2000404500040 ENDDATA 3 0 2000404500041 ENDSUBENT 40 0 2000404599999 NOSUBENT 20004046 20181026 22732000404600001 SUBENT 20004047 20181026 22732000404700001 BIB 8 32 2000404700002 REACTION 1(24-CR-50(N,P)23-V-50,,DA,,4PI) 2000404700003 2(24-CR-50(N,P)23-V-50,,DA,,4PI) 2000404700004 ANALYSIS Histograms as a function of angle from 0 to 2000404700005 360 degrees in 2 degree steps give six peaks with a 2000404700006 small uniform background to be subtracted. 2000404700007 .Normalization to obtain the absolute differential 2000404700008 cross section at 120 degrees. 2000404700009 .Histograms as a function of energy from 2 or 3 MeV to 2000404700010 12 MeV in steps of 0.5 MeV or each target peak. 2000404700011 (4PI1A) 4*Pi*differential cross section assuming that 2000404700012 the direct cross section is negligible at this angle 2000404700013 and that the compound cross section is isotropic. 2000404700014 1 Plots of ln(ro(E)) against E with ro based 2000404700015 on constant nuclear temperature model in order 2000404700016 to separate sigma(n,p) from sigma(n,n p). 2000404700017 2 Plots of ln(ro(U)) against (square root(U)) 2000404700018 based on the Fermi gas model in order to separate 2000404700019 sigma(n,p) from sigma(n,n p). 2000404700020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000404700021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000404700022 CORRECTION .Corrected for background and 2000404700023 .isotopic composition of the enriched targets. 2000404700024 .The extrapolation of the proton spectrum below the 2000404700025 bias energy (3 MeV) amounts to a fairly constant 40% 2000404700026 for each nuclide. 2000404700027 ERR-ANALYS (DATA-ERR) Error given includes: 2000404700028 .statistical error from track counting, 2000404700029 .errors due to proton spectrum extrapolation. 2000404700030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000404700031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000404700032 added to REACTION code. REACTION (2) was added. Data 2000404700033 from Subent 048 were added. MONIT-REF, ANG added. 2000404700034 ENDBIB 32 0 2000404700035 NOCOMMON 0 0 2000404700036 DATA 4 1 2000404700037 ANG DATA 1DATA-ERR 1DATA 2 2000404700038 ADEG B B B 2000404700039 120. 0.265 0.021 0.277 2000404700040 ENDDATA 3 0 2000404700041 ENDSUBENT 40 0 2000404799999 NOSUBENT 20004048 20181026 22732000404800001 SUBENT 20004049 20181026 22732000404900001 BIB 8 28 2000404900002 REACTION (24-CR-50(N,N+P)23-V-49,,DA,,4PI) 2000404900003 ANALYSIS Histograms as a function of angle from 0 to 2000404900004 360 degrees in 2 degree steps give six peaks with a 2000404900005 small uniform background to be subtracted. 2000404900006 .Normalization to obtain the absolute differential 2000404900007 cross section at 120 degrees. 2000404900008 .Histograms as a function of energy from 2 or 3 MeV to 2000404900009 12 MeV in steps of 0.5 MeV or each target peak. 2000404900010 (4PI1A) 4*Pi*differential cross section assuming that 2000404900011 the direct cross section is negligible at this angle 2000404900012 and that the compound cross section is isotropic. 2000404900013 Subtraction of sigma(n,p) cross section 2000404900014 determined by statistical plot method from the total 2000404900015 proton emission cross section. 2000404900016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000404900017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000404900018 CORRECTION .Corrected for background and 2000404900019 .isotopic composition of the enriched targets. 2000404900020 .The extrapolation of the proton spectrum below the 2000404900021 bias energy (3 MeV) amounts to a fairly constant 40% 2000404900022 for each nuclide. 2000404900023 ERR-ANALYS (DATA-ERR) Error given includes: 2000404900024 .statistical error from track counting, 2000404900025 .errors due to proton spectrum extrapolation. 2000404900026 .Errors are estimated equal to those of sigma(n,p). 2000404900027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000404900028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000404900029 added to REACTION code. MONIT-REF, ANG added. 2000404900030 ENDBIB 28 0 2000404900031 NOCOMMON 0 0 2000404900032 DATA 3 1 2000404900033 ANG DATA DATA-ERR 2000404900034 ADEG B B 2000404900035 120. 0.153 0.021 2000404900036 ENDDATA 3 0 2000404900037 ENDSUBENT 36 0 2000404999999 SUBENT 20004050 20181026 22732000405000001 BIB 4 7 2000405000002 REACTION ((24-CR-50(N,N+P)23-V-49,,DA,,4PI)/ 2000405000003 (24-CR-50(N,P)23-V-50,,DA,,4PI)) 2000405000004 ERR-ANALYS Not given. 2000405000005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000405000006 (DEP,20004049) Cr. section (n,n+p) 2000405000007 (DEP,20004047) REACTION (2) from Subent 047. 2000405000008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000405000009 ENDBIB 7 0 2000405000010 NOCOMMON 0 0 2000405000011 DATA 2 1 2000405000012 ANG DATA 2000405000013 ADEG NO-DIM 2000405000014 120. 0.55 2000405000015 ENDDATA 3 0 2000405000016 ENDSUBENT 15 0 2000405099999 SUBENT 20004051 20181026 22732000405100001 BIB 6 11 2000405100002 REACTION (24-CR-51(0,0),,TEM) 2000405100003 For (n,p) reaction at 120 degrees (compound part). 2000405100004 ANALYSIS From plots of proton spectra assuming the 2000405100005 constant nuclear temperature statistical model. 2000405100006 COMMENT The value of the nuclear temperature of the residual 2000405100007 nucleus formed in a (n,n p) reaction varied between 2000405100008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000405100009 temperature is given. 2000405100010 ERR-ANALYS (ERR-S) Statistical errors 2000405100011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000405100012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000405100013 ENDBIB 11 0 2000405100014 NOCOMMON 0 0 2000405100015 DATA 2 1 2000405100016 DATA ERR-S 2000405100017 MEV MEV 2000405100018 1.1 0.1 2000405100019 ENDDATA 3 0 2000405100020 ENDSUBENT 19 0 2000405199999 SUBENT 20004052 20181026 22732000405200001 BIB 8 32 2000405200002 REACTION 1(24-CR-52(N,P)23-V-52,,DA,,4PI) 2000405200003 2(24-CR-52(N,P)23-V-52,,DA,,4PI) 2000405200004 ANALYSIS Histograms as a function of angle from 0 to 2000405200005 360 degrees in 2 degree steps give six peaks with a 2000405200006 small uniform background to be subtracted. 2000405200007 .Normalization to obtain the absolute differential 2000405200008 cross section at 120 degrees. 2000405200009 .Histograms as a function of energy from 2 or 3 MeV to 2000405200010 12 MeV in steps of 0.5 MeV or each target peak. 2000405200011 (4PI1A) 4*Pi*differential cross section assuming that 2000405200012 the direct cross section is negligible at this angle 2000405200013 and that the compound cross section is isotropic. 2000405200014 1 Plots of ln(ro(E)) against E with ro based 2000405200015 on constant nuclear temperature model in order 2000405200016 to separate sigma(n,p) from sigma(n,n p). 2000405200017 2 Plots of ln(ro(U)) against (square root(U)) 2000405200018 based on the Fermi gas model in order to separate 2000405200019 sigma(n,p) from sigma(n,n p). 2000405200020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000405200021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000405200022 CORRECTION .Corrected for background and 2000405200023 .isotopic composition of the enriched targets. 2000405200024 .The extrapolation of the proton spectrum below the 2000405200025 bias energy (3 MeV) amounts to a fairly constant 40% 2000405200026 for each nuclide. 2000405200027 ERR-ANALYS (DATA-ERR) Error given includes: 2000405200028 .statistical error from track counting, 2000405200029 .errors due to proton spectrum extrapolation. 2000405200030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000405200031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000405200032 added to REACTION code. REACTION (2) was added. Data 2000405200033 from Subent 053 were added. MONIT-REF, ANG added. 2000405200034 ENDBIB 32 0 2000405200035 NOCOMMON 0 0 2000405200036 DATA 4 1 2000405200037 ANG DATA 1DATA-ERR 1DATA 2 2000405200038 ADEG B B B 2000405200039 120. 0.074 0.010 0.067 2000405200040 ENDDATA 3 0 2000405200041 ENDSUBENT 40 0 2000405299999 NOSUBENT 20004053 20181026 22732000405300001 SUBENT 20004054 20181026 22732000405400001 BIB 8 32 2000405400002 REACTION 1(24-CR-53(N,P)23-V-53,,DA,,4PI) 2000405400003 2(24-CR-53(N,P)23-V-53,,DA,,4PI) 2000405400004 ANALYSIS Histograms as a function of angle from 0 to 2000405400005 360 degrees in 2 degree steps give six peaks with a 2000405400006 small uniform background to be subtracted. 2000405400007 .Normalization to obtain the absolute differential 2000405400008 cross section at 120 degrees. 2000405400009 .Histograms as a function of energy from 2 or 3 MeV to 2000405400010 12 MeV in steps of 0.5 MeV or each target peak. 2000405400011 (4PI1A) 4*Pi*differential cross section assuming that 2000405400012 the direct cross section is negligible at this angle 2000405400013 and that the compound cross section is isotropic. 2000405400014 1 Plots of ln(ro(E)) against E with ro based 2000405400015 on constant nuclear temperature model in order 2000405400016 to separate sigma(n,p) from sigma(n,n p). 2000405400017 2 Plots of ln(ro(U)) against (square root(U)) 2000405400018 based on the Fermi gas model in order to separate 2000405400019 sigma(n,p) from sigma(n,n p). 2000405400020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000405400021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000405400022 CORRECTION .Corrected for background and 2000405400023 .isotopic composition of the enriched targets. 2000405400024 .The extrapolation of the proton spectrum below the 2000405400025 bias energy (3 MeV) amounts to a fairly constant 40% 2000405400026 for each nuclide. 2000405400027 ERR-ANALYS (DATA-ERR) Error given includes: 2000405400028 .statistical error from track counting, 2000405400029 .errors due to proton spectrum extrapolation. 2000405400030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000405400031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000405400032 added to REACTION code. REACTION (2) was added. Data 2000405400033 from Subent 055 were added. MONIT-REF, ANG added. 2000405400034 ENDBIB 32 0 2000405400035 NOCOMMON 0 0 2000405400036 DATA 4 1 2000405400037 ANG DATA 1DATA-ERR 1DATA 2 2000405400038 ADEG B B B 2000405400039 120. 0.044 0.007 0.048 2000405400040 ENDDATA 3 0 2000405400041 ENDSUBENT 40 0 2000405499999 NOSUBENT 20004055 20181026 22732000405500001 SUBENT 20004056 20181026 22732000405600001 BIB 6 11 2000405600002 REACTION (24-CR-53(0,0),,TEM) 2000405600003 For (n,p) reaction at 120 degrees (compound part). 2000405600004 ANALYSIS From plots of proton spectra assuming the 2000405600005 constant nuclear temperature statistical model. 2000405600006 COMMENT The value of the nuclear temperature of the residual 2000405600007 nucleus formed in a (n,n p) reaction varied between 2000405600008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000405600009 temperature is given. 2000405600010 ERR-ANALYS (ERR-S) Statistical errors 2000405600011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000405600012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000405600013 ENDBIB 11 0 2000405600014 NOCOMMON 0 0 2000405600015 DATA 2 1 2000405600016 DATA ERR-S 2000405600017 MEV MEV 2000405600018 1.1 0.1 2000405600019 ENDDATA 3 0 2000405600020 ENDSUBENT 19 0 2000405699999 SUBENT 20004057 20181026 22732000405700001 BIB 8 32 2000405700002 REACTION 1(25-MN-55(N,P)24-CR-55,,DA,,4PI) 2000405700003 2(25-MN-55(N,P)24-CR-55,,DA,,4PI) 2000405700004 ANALYSIS Histograms as a function of angle from 0 to 2000405700005 360 degrees in 2 degree steps give six peaks with a 2000405700006 small uniform background to be subtracted. 2000405700007 .Normalization to obtain the absolute differential 2000405700008 cross section at 120 degrees. 2000405700009 .Histograms as a function of energy from 2 or 3 MeV to 2000405700010 12 MeV in steps of 0.5 MeV or each target peak. 2000405700011 (4PI1A) 4*Pi*differential cross section assuming that 2000405700012 the direct cross section is negligible at this angle 2000405700013 and that the compound cross section is isotropic. 2000405700014 1 Plots of ln(ro(E)) against E with ro based 2000405700015 on constant nuclear temperature model in order 2000405700016 to separate sigma(n,p) from sigma(n,n p). 2000405700017 2 Plots of ln(ro(U)) against (square root(U)) 2000405700018 based on the Fermi gas model in order to separate 2000405700019 sigma(n,p) from sigma(n,n p). 2000405700020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000405700021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000405700022 CORRECTION .Corrected for background and 2000405700023 .isotopic composition of the enriched targets. 2000405700024 .The extrapolation of the proton spectrum below the 2000405700025 bias energy (3 MeV) amounts to a fairly constant 40% 2000405700026 for each nuclide. 2000405700027 ERR-ANALYS (DATA-ERR) Error given includes: 2000405700028 .statistical error from track counting, 2000405700029 .errors due to proton spectrum extrapolation. 2000405700030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000405700031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000405700032 added to REACTION code. REACTION (2) was added. Data 2000405700033 from Subent 058 were added. MONIT-REF, ANG added. 2000405700034 ENDBIB 32 0 2000405700035 NOCOMMON 0 0 2000405700036 DATA 4 1 2000405700037 ANG DATA 1DATA-ERR 1DATA 2 2000405700038 ADEG B B B 2000405700039 120. 0.043 0.007 0.045 2000405700040 ENDDATA 3 0 2000405700041 ENDSUBENT 40 0 2000405799999 NOSUBENT 20004058 20181026 22732000405800001 SUBENT 20004059 20181026 22732000405900001 BIB 8 32 2000405900002 REACTION 1(26-FE-54(N,P)25-MN-54,,DA,,4PI) 2000405900003 2(26-FE-54(N,P)25-MN-54,,DA,,4PI) 2000405900004 ANALYSIS Histograms as a function of angle from 0 to 2000405900005 360 degrees in 2 degree steps give six peaks with a 2000405900006 small uniform background to be subtracted. 2000405900007 .Normalization to obtain the absolute differential 2000405900008 cross section at 120 degrees. 2000405900009 .Histograms as a function of energy from 2 or 3 MeV to 2000405900010 12 MeV in steps of 0.5 MeV or each target peak. 2000405900011 (4PI1A) 4*Pi*differential cross section assuming that 2000405900012 the direct cross section is negligible at this angle 2000405900013 and that the compound cross section is isotropic. 2000405900014 1 Plots of ln(ro(E)) against E with ro based 2000405900015 on constant nuclear temperature model in order 2000405900016 to separate sigma(n,p) from sigma(n,n p). 2000405900017 2 Plots of ln(ro(U)) against (square root(U)) 2000405900018 based on the Fermi gas model in order to separate 2000405900019 sigma(n,p) from sigma(n,n p). 2000405900020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000405900021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000405900022 CORRECTION .Corrected for background and 2000405900023 .isotopic composition of the enriched targets. 2000405900024 .The extrapolation of the proton spectrum below the 2000405900025 bias energy (3 MeV) amounts to a fairly constant 40% 2000405900026 for each nuclide. 2000405900027 ERR-ANALYS (DATA-ERR) Error given includes: 2000405900028 .statistical error from track counting, 2000405900029 .errors due to proton spectrum extrapolation. 2000405900030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000405900031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000405900032 added to REACTION code. REACTION (2) was added. Data 2000405900033 from Subent 060 were added. MONIT-REF, ANG added. 2000405900034 ENDBIB 32 0 2000405900035 NOCOMMON 0 0 2000405900036 DATA 4 1 2000405900037 ANG DATA 1DATA-ERR 1DATA 2 2000405900038 ADEG B B B 2000405900039 120. 0.382 0.013 0.382 2000405900040 ENDDATA 3 0 2000405900041 ENDSUBENT 40 0 2000405999999 NOSUBENT 20004060 20181026 22732000406000001 SUBENT 20004061 20181026 22732000406100001 BIB 8 28 2000406100002 REACTION (26-FE-54(N,N+P)25-MN-53,,DA,,4PI) 2000406100003 ANALYSIS Histograms as a function of angle from 0 to 2000406100004 360 degrees in 2 degree steps give six peaks with a 2000406100005 small uniform background to be subtracted. 2000406100006 .Normalization to obtain the absolute differential 2000406100007 cross section at 120 degrees. 2000406100008 .Histograms as a function of energy from 2 or 3 MeV to 2000406100009 12 MeV in steps of 0.5 MeV or each target peak. 2000406100010 (4PI1A) 4*Pi*differential cross section assuming that 2000406100011 the direct cross section is negligible at this angle 2000406100012 and that the compound cross section is isotropic. 2000406100013 Subtraction of sigma(n,p) cross section 2000406100014 determined by statistical plot method from the total 2000406100015 proton emission cross section. 2000406100016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000406100017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000406100018 CORRECTION .Corrected for background and 2000406100019 .isotopic composition of the enriched targets. 2000406100020 .The extrapolation of the proton spectrum below the 2000406100021 bias energy (3 MeV) amounts to a fairly constant 40% 2000406100022 for each nuclide. 2000406100023 ERR-ANALYS (DATA-ERR) Error given includes: 2000406100024 .statistical error from track counting, 2000406100025 .errors due to proton spectrum extrapolation. 2000406100026 .Errors are estimated equal to those of sigma(n,p). 2000406100027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000406100028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000406100029 added to REACTION code. MONIT-REF, ANG added. 2000406100030 ENDBIB 28 0 2000406100031 NOCOMMON 0 0 2000406100032 DATA 3 1 2000406100033 ANG DATA DATA-ERR 2000406100034 ADEG B B 2000406100035 120. 0.218 0.013 2000406100036 ENDDATA 3 0 2000406100037 ENDSUBENT 36 0 2000406199999 SUBENT 20004062 20181026 22732000406200001 BIB 4 7 2000406200002 REACTION ((26-FE-54(N,N+P)25-MN-53,,DA,,4PI)/ 2000406200003 (26-FE-54(N,P)25-MN-54,,DA,,4PI)) 2000406200004 ERR-ANALYS Not given. 2000406200005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000406200006 (DEP,20004061) Cr. section (n,n+p) 2000406200007 (DEP,20004059) REACTION (2) from Subent 059. 2000406200008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000406200009 ENDBIB 7 0 2000406200010 NOCOMMON 0 0 2000406200011 DATA 2 1 2000406200012 ANG DATA 2000406200013 ADEG NO-DIM 2000406200014 120. 0.57 2000406200015 ENDDATA 3 0 2000406200016 ENDSUBENT 15 0 2000406299999 SUBENT 20004063 20181026 22732000406300001 BIB 6 11 2000406300002 REACTION (26-FE-55(0,0),,TEM) 2000406300003 For (n,p) reaction at 120 degrees (compound part). 2000406300004 ANALYSIS From plots of proton spectra assuming the 2000406300005 constant nuclear temperature statistical model. 2000406300006 COMMENT The value of the nuclear temperature of the residual 2000406300007 nucleus formed in a (n,n p) reaction varied between 2000406300008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000406300009 temperature is given. 2000406300010 ERR-ANALYS (ERR-S) Statistical errors 2000406300011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000406300012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000406300013 ENDBIB 11 0 2000406300014 NOCOMMON 0 0 2000406300015 DATA 2 1 2000406300016 DATA ERR-S 2000406300017 MEV MEV 2000406300018 1.1 0.1 2000406300019 ENDDATA 3 0 2000406300020 ENDSUBENT 19 0 2000406399999 SUBENT 20004064 20181026 22732000406400001 BIB 8 32 2000406400002 REACTION 1(26-FE-56(N,P)25-MN-56,,DA,,4PI) 2000406400003 2(26-FE-56(N,P)25-MN-56,,DA,,4PI) 2000406400004 ANALYSIS Histograms as a function of angle from 0 to 2000406400005 360 degrees in 2 degree steps give six peaks with a 2000406400006 small uniform background to be subtracted. 2000406400007 .Normalization to obtain the absolute differential 2000406400008 cross section at 120 degrees. 2000406400009 .Histograms as a function of energy from 2 or 3 MeV to 2000406400010 12 MeV in steps of 0.5 MeV or each target peak. 2000406400011 (4PI1A) 4*Pi*differential cross section assuming that 2000406400012 the direct cross section is negligible at this angle 2000406400013 and that the compound cross section is isotropic. 2000406400014 1 Plots of ln(ro(E)) against E with ro based 2000406400015 on constant nuclear temperature model in order 2000406400016 to separate sigma(n,p) from sigma(n,n p). 2000406400017 2 Plots of ln(ro(U)) against (square root(U)) 2000406400018 based on the Fermi gas model in order to separate 2000406400019 sigma(n,p) from sigma(n,n p). 2000406400020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000406400021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000406400022 CORRECTION .Corrected for background and 2000406400023 .isotopic composition of the enriched targets. 2000406400024 .The extrapolation of the proton spectrum below the 2000406400025 bias energy (3 MeV) amounts to a fairly constant 40% 2000406400026 for each nuclide. 2000406400027 ERR-ANALYS (DATA-ERR) Error given includes: 2000406400028 .statistical error from track counting, 2000406400029 .errors due to proton spectrum extrapolation. 2000406400030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000406400031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000406400032 added to REACTION code. REACTION (2) was added. Data 2000406400033 from Subent 065 were added. MONIT-REF, ANG added. 2000406400034 ENDBIB 32 0 2000406400035 NOCOMMON 0 0 2000406400036 DATA 4 1 2000406400037 ANG DATA 1DATA-ERR 1DATA 2 2000406400038 ADEG B B B 2000406400039 120. 0.082 0.007 0.086 2000406400040 ENDDATA 3 0 2000406400041 ENDSUBENT 40 0 2000406499999 NOSUBENT 20004065 20181026 22732000406500001 SUBENT 20004066 20181026 22732000406600001 BIB 8 28 2000406600002 REACTION (26-FE-56(N,N+P)25-MN-55,,DA,,4PI) 2000406600003 ANALYSIS Histograms as a function of angle from 0 to 2000406600004 360 degrees in 2 degree steps give six peaks with a 2000406600005 small uniform background to be subtracted. 2000406600006 .Normalization to obtain the absolute differential 2000406600007 cross section at 120 degrees. 2000406600008 .Histograms as a function of energy from 2 or 3 MeV to 2000406600009 12 MeV in steps of 0.5 MeV or each target peak. 2000406600010 (4PI1A) 4*Pi*differential cross section assuming that 2000406600011 the direct cross section is negligible at this angle 2000406600012 and that the compound cross section is isotropic. 2000406600013 Subtraction of sigma(n,p) cross section 2000406600014 determined by statistical plot method from the total 2000406600015 proton emission cross section. 2000406600016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000406600017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000406600018 CORRECTION .Corrected for background and 2000406600019 .isotopic composition of the enriched targets. 2000406600020 .The extrapolation of the proton spectrum below the 2000406600021 bias energy (3 MeV) amounts to a fairly constant 40% 2000406600022 for each nuclide. 2000406600023 ERR-ANALYS (DATA-ERR) Error given includes: 2000406600024 .statistical error from track counting, 2000406600025 .errors due to proton spectrum extrapolation. 2000406600026 .Errors are estimated equal to those of sigma(n,p). 2000406600027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000406600028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000406600029 added to REACTION code. MONIT-REF, ANG added. 2000406600030 ENDBIB 28 0 2000406600031 NOCOMMON 0 0 2000406600032 DATA 3 1 2000406600033 ANG DATA DATA-ERR 2000406600034 ADEG B B 2000406600035 120. 0.035 0.007 2000406600036 ENDDATA 3 0 2000406600037 ENDSUBENT 36 0 2000406699999 SUBENT 20004067 20181026 22732000406700001 BIB 4 7 2000406700002 REACTION ((26-FE-56(N,N+P)25-MN-55,,DA,,4PI)/ 2000406700003 (26-FE-56(N,P)25-MN-56,,DA,,4PI)) 2000406700004 ERR-ANALYS Not given. 2000406700005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000406700006 (DEP,20004066) Cr. section (n,n+p) 2000406700007 (DEP,20004064) REACTION (2) from Subent 064. 2000406700008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000406700009 ENDBIB 7 0 2000406700010 NOCOMMON 0 0 2000406700011 DATA 2 1 2000406700012 ANG DATA 2000406700013 ADEG NO-DIM 2000406700014 120. 0.41 2000406700015 ENDDATA 3 0 2000406700016 ENDSUBENT 15 0 2000406799999 SUBENT 20004068 20181026 22732000406800001 BIB 6 11 2000406800002 REACTION (26-FE-57(0,0),,TEM) 2000406800003 For (n,p) reaction at 120 degrees (compound part). 2000406800004 ANALYSIS From plots of proton spectra assuming the 2000406800005 constant nuclear temperature statistical model. 2000406800006 COMMENT The value of the nuclear temperature of the residual 2000406800007 nucleus formed in a (n,n p) reaction varied between 2000406800008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000406800009 temperature is given. 2000406800010 ERR-ANALYS (ERR-S) Statistical errors 2000406800011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000406800012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000406800013 ENDBIB 11 0 2000406800014 NOCOMMON 0 0 2000406800015 DATA 2 1 2000406800016 DATA ERR-S 2000406800017 MEV MEV 2000406800018 1.1 0.1 2000406800019 ENDDATA 3 0 2000406800020 ENDSUBENT 19 0 2000406899999 SUBENT 20004069 20181026 22732000406900001 BIB 8 32 2000406900002 REACTION 1(27-CO-59(N,P)26-FE-59,,DA,,4PI) 2000406900003 2(27-CO-59(N,P)26-FE-59,,DA,,4PI) 2000406900004 ANALYSIS Histograms as a function of angle from 0 to 2000406900005 360 degrees in 2 degree steps give six peaks with a 2000406900006 small uniform background to be subtracted. 2000406900007 .Normalization to obtain the absolute differential 2000406900008 cross section at 120 degrees. 2000406900009 .Histograms as a function of energy from 2 or 3 MeV to 2000406900010 12 MeV in steps of 0.5 MeV or each target peak. 2000406900011 (4PI1A) 4*Pi*differential cross section assuming that 2000406900012 the direct cross section is negligible at this angle 2000406900013 and that the compound cross section is isotropic. 2000406900014 1 Plots of ln(ro(E)) against E with ro based 2000406900015 on constant nuclear temperature model in order 2000406900016 to separate sigma(n,p) from sigma(n,n p). 2000406900017 2 Plots of ln(ro(U)) against (square root(U)) 2000406900018 based on the Fermi gas model in order to separate 2000406900019 sigma(n,p) from sigma(n,n p). 2000406900020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000406900021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000406900022 CORRECTION .Corrected for background and 2000406900023 .isotopic composition of the enriched targets. 2000406900024 .The extrapolation of the proton spectrum below the 2000406900025 bias energy (3 MeV) amounts to a fairly constant 40% 2000406900026 for each nuclide. 2000406900027 ERR-ANALYS (DATA-ERR) Error given includes: 2000406900028 .statistical error from track counting, 2000406900029 .errors due to proton spectrum extrapolation. 2000406900030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000406900031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000406900032 added to REACTION code. REACTION (2) was added. Data 2000406900033 from Subent 070 were added. MONIT-REF, ANG added. 2000406900034 ENDBIB 32 0 2000406900035 NOCOMMON 0 0 2000406900036 DATA 4 1 2000406900037 ANG DATA 1DATA-ERR 1DATA 2 2000406900038 ADEG B B B 2000406900039 120. 0.081 0.010 0.061 2000406900040 ENDDATA 3 0 2000406900041 ENDSUBENT 40 0 2000406999999 NOSUBENT 20004070 20181026 22732000407000001 SUBENT 20004071 20181026 22732000407100001 BIB 8 32 2000407100002 REACTION 1(28-NI-58(N,P)27-CO-58,,DA,,4PI) 2000407100003 2(28-NI-58(N,P)27-CO-58,,DA,,4PI) 2000407100004 ANALYSIS Histograms as a function of angle from 0 to 2000407100005 360 degrees in 2 degree steps give six peaks with a 2000407100006 small uniform background to be subtracted. 2000407100007 .Normalization to obtain the absolute differential 2000407100008 cross section at 120 degrees. 2000407100009 .Histograms as a function of energy from 2 or 3 MeV to 2000407100010 12 MeV in steps of 0.5 MeV or each target peak. 2000407100011 (4PI1A) 4*Pi*differential cross section assuming that 2000407100012 the direct cross section is negligible at this angle 2000407100013 and that the compound cross section is isotropic. 2000407100014 1 Plots of ln(ro(E)) against E with ro based 2000407100015 on constant nuclear temperature model in order 2000407100016 to separate sigma(n,p) from sigma(n,n p). 2000407100017 2 Plots of ln(ro(U)) against (square root(U)) 2000407100018 based on the Fermi gas model in order to separate 2000407100019 sigma(n,p) from sigma(n,n p). 2000407100020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000407100021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000407100022 CORRECTION .Corrected for background and 2000407100023 .isotopic composition of the enriched targets. 2000407100024 .The extrapolation of the proton spectrum below the 2000407100025 bias energy (3 MeV) amounts to a fairly constant 40% 2000407100026 for each nuclide. 2000407100027 ERR-ANALYS (DATA-ERR) Error given includes: 2000407100028 .statistical error from track counting, 2000407100029 .errors due to proton spectrum extrapolation. 2000407100030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000407100031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000407100032 added to REACTION code. REACTION (2) was added. Data 2000407100033 from Subent 072 were added. MONIT-REF, ANG added. 2000407100034 ENDBIB 32 0 2000407100035 NOCOMMON 0 0 2000407100036 DATA 4 1 2000407100037 ANG DATA 1DATA-ERR 1DATA 2 2000407100038 ADEG B B B 2000407100039 120. 0.440 0.027 0.430 2000407100040 ENDDATA 3 0 2000407100041 ENDSUBENT 40 0 2000407199999 NOSUBENT 20004072 20181026 22732000407200001 SUBENT 20004073 20181026 22732000407300001 BIB 8 28 2000407300002 REACTION (28-NI-58(N,N+P)27-CO-57,,DA,,4PI) 2000407300003 ANALYSIS Histograms as a function of angle from 0 to 2000407300004 360 degrees in 2 degree steps give six peaks with a 2000407300005 small uniform background to be subtracted. 2000407300006 .Normalization to obtain the absolute differential 2000407300007 cross section at 120 degrees. 2000407300008 .Histograms as a function of energy from 2 or 3 MeV to 2000407300009 12 MeV in steps of 0.5 MeV or each target peak. 2000407300010 (4PI1A) 4*Pi*differential cross section assuming that 2000407300011 the direct cross section is negligible at this angle 2000407300012 and that the compound cross section is isotropic. 2000407300013 Subtraction of sigma(n,p) cross section 2000407300014 determined by statistical plot method from the total 2000407300015 proton emission cross section. 2000407300016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000407300017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000407300018 CORRECTION .Corrected for background and 2000407300019 .isotopic composition of the enriched targets. 2000407300020 .The extrapolation of the proton spectrum below the 2000407300021 bias energy (3 MeV) amounts to a fairly constant 40% 2000407300022 for each nuclide. 2000407300023 ERR-ANALYS (DATA-ERR) Error given includes: 2000407300024 .statistical error from track counting, 2000407300025 .errors due to proton spectrum extrapolation. 2000407300026 .Errors are estimated equal to those of sigma(n,p). 2000407300027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000407300028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000407300029 added to REACTION code. MONIT-REF, ANG added. 2000407300030 ENDBIB 28 0 2000407300031 NOCOMMON 0 0 2000407300032 DATA 3 1 2000407300033 ANG DATA DATA-ERR 2000407300034 ADEG B B 2000407300035 120. 0.343 0.027 2000407300036 ENDDATA 3 0 2000407300037 ENDSUBENT 36 0 2000407399999 SUBENT 20004074 20181026 22732000407400001 BIB 4 7 2000407400002 REACTION ((28-NI-58(N,N+P)27-CO-57,,DA,,4PI)/ 2000407400003 (28-NI-58(N,P)27-CO-58,,DA,,4PI)) 2000407400004 ERR-ANALYS Not given. 2000407400005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000407400006 (DEP,20004073) Cr. section (n,n+p) 2000407400007 (DEP,20004071) REACTION (2) from Subent 071. 2000407400008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000407400009 ENDBIB 7 0 2000407400010 NOCOMMON 0 0 2000407400011 DATA 2 1 2000407400012 ANG DATA 2000407400013 ADEG NO-DIM 2000407400014 120. 0.80 2000407400015 ENDDATA 3 0 2000407400016 ENDSUBENT 15 0 2000407499999 SUBENT 20004075 20181026 22732000407500001 BIB 6 11 2000407500002 REACTION (28-NI-59(0,0),,TEM) 2000407500003 For (n,p) reaction at 120 degrees (compound part). 2000407500004 ANALYSIS From plots of proton spectra assuming the 2000407500005 constant nuclear temperature statistical model. 2000407500006 COMMENT The value of the nuclear temperature of the residual 2000407500007 nucleus formed in a (n,n p) reaction varied between 2000407500008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000407500009 temperature is given. 2000407500010 ERR-ANALYS (ERR-S) Statistical errors 2000407500011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000407500012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000407500013 ENDBIB 11 0 2000407500014 NOCOMMON 0 0 2000407500015 DATA 2 1 2000407500016 DATA ERR-S 2000407500017 MEV MEV 2000407500018 1.1 0.1 2000407500019 ENDDATA 3 0 2000407500020 ENDSUBENT 19 0 2000407599999 SUBENT 20004076 20181026 22732000407600001 BIB 8 32 2000407600002 REACTION 1(28-NI-60(N,P)27-CO-60,,DA,,4PI) 2000407600003 2(28-NI-60(N,P)27-CO-60,,DA,,4PI) 2000407600004 ANALYSIS Histograms as a function of angle from 0 to 2000407600005 360 degrees in 2 degree steps give six peaks with a 2000407600006 small uniform background to be subtracted. 2000407600007 .Normalization to obtain the absolute differential 2000407600008 cross section at 120 degrees. 2000407600009 .Histograms as a function of energy from 2 or 3 MeV to 2000407600010 12 MeV in steps of 0.5 MeV or each target peak. 2000407600011 (4PI1A) 4*Pi*differential cross section assuming that 2000407600012 the direct cross section is negligible at this angle 2000407600013 and that the compound cross section is isotropic. 2000407600014 1 Plots of ln(ro(E)) against E with ro based 2000407600015 on constant nuclear temperature model in order 2000407600016 to separate sigma(n,p) from sigma(n,n p). 2000407600017 2 Plots of ln(ro(U)) against (square root(U)) 2000407600018 based on the Fermi gas model in order to separate 2000407600019 sigma(n,p) from sigma(n,n p). 2000407600020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000407600021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000407600022 CORRECTION .Corrected for background and 2000407600023 .isotopic composition of the enriched targets. 2000407600024 .The extrapolation of the proton spectrum below the 2000407600025 bias energy (3 MeV) amounts to a fairly constant 40% 2000407600026 for each nuclide. 2000407600027 ERR-ANALYS (DATA-ERR) Error given includes: 2000407600028 .statistical error from track counting, 2000407600029 .errors due to proton spectrum extrapolation. 2000407600030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000407600031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000407600032 added to REACTION code. REACTION (2) was added. Data 2000407600033 from Subent 077 were added. MONIT-REF, ANG added. 2000407600034 ENDBIB 32 0 2000407600035 NOCOMMON 0 0 2000407600036 DATA 4 1 2000407600037 ANG DATA 1DATA-ERR 1DATA 2 2000407600038 ADEG B B B 2000407600039 120. 0.124 0.009 0.134 2000407600040 ENDDATA 3 0 2000407600041 ENDSUBENT 40 0 2000407699999 NOSUBENT 20004077 20181026 22732000407700001 SUBENT 20004078 20181026 22732000407800001 BIB 8 28 2000407800002 REACTION (28-NI-60(N,N+P)27-CO-59,,DA,,4PI) 2000407800003 ANALYSIS Histograms as a function of angle from 0 to 2000407800004 360 degrees in 2 degree steps give six peaks with a 2000407800005 small uniform background to be subtracted. 2000407800006 .Normalization to obtain the absolute differential 2000407800007 cross section at 120 degrees. 2000407800008 .Histograms as a function of energy from 2 or 3 MeV to 2000407800009 12 MeV in steps of 0.5 MeV or each target peak. 2000407800010 (4PI1A) 4*Pi*differential cross section assuming that 2000407800011 the direct cross section is negligible at this angle 2000407800012 and that the compound cross section is isotropic. 2000407800013 Subtraction of sigma(n,p) cross section 2000407800014 determined by statistical plot method from the total 2000407800015 proton emission cross section. 2000407800016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000407800017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000407800018 CORRECTION .Corrected for background and 2000407800019 .isotopic composition of the enriched targets. 2000407800020 .The extrapolation of the proton spectrum below the 2000407800021 bias energy (3 MeV) amounts to a fairly constant 40% 2000407800022 for each nuclide. 2000407800023 ERR-ANALYS (DATA-ERR) Error given includes: 2000407800024 .statistical error from track counting, 2000407800025 .errors due to proton spectrum extrapolation. 2000407800026 .Errors are estimated equal to those of sigma(n,p). 2000407800027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000407800028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000407800029 added to REACTION code. MONIT-REF, ANG added. 2000407800030 ENDBIB 28 0 2000407800031 NOCOMMON 0 0 2000407800032 DATA 3 1 2000407800033 ANG DATA DATA-ERR 2000407800034 ADEG B B 2000407800035 120. 0.051 0.009 2000407800036 ENDDATA 3 0 2000407800037 ENDSUBENT 36 0 2000407899999 SUBENT 20004079 20181026 22732000407900001 BIB 4 7 2000407900002 REACTION ((28-NI-60(N,N+P)27-CO-59,,DA,,4PI)/ 2000407900003 (28-NI-60(N,P)27-CO-60,,DA,,4PI)) 2000407900004 ERR-ANALYS Not given. 2000407900005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000407900006 (DEP,20004078) Cr. section (n,n+p) 2000407900007 (DEP,20004076) REACTION (2) from Subent 076. 2000407900008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000407900009 ENDBIB 7 0 2000407900010 NOCOMMON 0 0 2000407900011 DATA 2 1 2000407900012 ANG DATA 2000407900013 ADEG NO-DIM 2000407900014 120. 0.38 2000407900015 ENDDATA 3 0 2000407900016 ENDSUBENT 15 0 2000407999999 SUBENT 20004080 20181026 22732000408000001 BIB 6 11 2000408000002 REACTION (28-NI-61(0,0),,TEM) 2000408000003 For (n,p) reaction at 120 degrees (compound part). 2000408000004 ANALYSIS From plots of proton spectra assuming the 2000408000005 constant nuclear temperature statistical model. 2000408000006 COMMENT The value of the nuclear temperature of the residual 2000408000007 nucleus formed in a (n,n p) reaction varied between 2000408000008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000408000009 temperature is given. 2000408000010 ERR-ANALYS (ERR-S) Statistical errors 2000408000011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000408000012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000408000013 ENDBIB 11 0 2000408000014 NOCOMMON 0 0 2000408000015 DATA 2 1 2000408000016 DATA ERR-S 2000408000017 MEV MEV 2000408000018 1.1 0.1 2000408000019 ENDDATA 3 0 2000408000020 ENDSUBENT 19 0 2000408099999 SUBENT 20004081 20181026 22732000408100001 BIB 8 32 2000408100002 REACTION 1(29-CU-63(N,P)28-NI-63,,DA,,4PI) 2000408100003 2(29-CU-63(N,P)28-NI-63,,DA,,4PI) 2000408100004 ANALYSIS Histograms as a function of angle from 0 to 2000408100005 360 degrees in 2 degree steps give six peaks with a 2000408100006 small uniform background to be subtracted. 2000408100007 .Normalization to obtain the absolute differential 2000408100008 cross section at 120 degrees. 2000408100009 .Histograms as a function of energy from 2 or 3 MeV to 2000408100010 12 MeV in steps of 0.5 MeV or each target peak. 2000408100011 (4PI1A) 4*Pi*differential cross section assuming that 2000408100012 the direct cross section is negligible at this angle 2000408100013 and that the compound cross section is isotropic. 2000408100014 1 Plots of ln(ro(E)) against E with ro based 2000408100015 on constant nuclear temperature model in order 2000408100016 to separate sigma(n,p) from sigma(n,n p). 2000408100017 2 Plots of ln(ro(U)) against (square root(U)) 2000408100018 based on the Fermi gas model in order to separate 2000408100019 sigma(n,p) from sigma(n,n p). 2000408100020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000408100021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000408100022 CORRECTION .Corrected for background and 2000408100023 .isotopic composition of the enriched targets. 2000408100024 .The extrapolation of the proton spectrum below the 2000408100025 bias energy (3 MeV) amounts to a fairly constant 40% 2000408100026 for each nuclide. 2000408100027 ERR-ANALYS (DATA-ERR) Error given includes: 2000408100028 .statistical error from track counting, 2000408100029 .errors due to proton spectrum extrapolation. 2000408100030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000408100031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000408100032 added to REACTION code. REACTION (2) was added. Data 2000408100033 from Subent 082 were added. MONIT-REF, ANG added. 2000408100034 ENDBIB 32 0 2000408100035 NOCOMMON 0 0 2000408100036 DATA 4 1 2000408100037 ANG DATA 1DATA-ERR 1DATA 2 2000408100038 ADEG B B B 2000408100039 120. 0.118 0.009 0.105 2000408100040 ENDDATA 3 0 2000408100041 ENDSUBENT 40 0 2000408199999 NOSUBENT 20004082 20181026 22732000408200001 SUBENT 20004083 20181026 22732000408300001 BIB 8 28 2000408300002 REACTION (29-CU-63(N,N+P)28-NI-62,,DA,,4PI) 2000408300003 ANALYSIS Histograms as a function of angle from 0 to 2000408300004 360 degrees in 2 degree steps give six peaks with a 2000408300005 small uniform background to be subtracted. 2000408300006 .Normalization to obtain the absolute differential 2000408300007 cross section at 120 degrees. 2000408300008 .Histograms as a function of energy from 2 or 3 MeV to 2000408300009 12 MeV in steps of 0.5 MeV or each target peak. 2000408300010 (4PI1A) 4*Pi*differential cross section assuming that 2000408300011 the direct cross section is negligible at this angle 2000408300012 and that the compound cross section is isotropic. 2000408300013 Subtraction of sigma(n,p) cross section 2000408300014 determined by statistical plot method from the total 2000408300015 proton emission cross section. 2000408300016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000408300017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000408300018 CORRECTION .Corrected for background and 2000408300019 .isotopic composition of the enriched targets. 2000408300020 .The extrapolation of the proton spectrum below the 2000408300021 bias energy (3 MeV) amounts to a fairly constant 40% 2000408300022 for each nuclide. 2000408300023 ERR-ANALYS (DATA-ERR) Error given includes: 2000408300024 .statistical error from track counting, 2000408300025 .errors due to proton spectrum extrapolation. 2000408300026 .Errors are estimated equal to those of sigma(n,p). 2000408300027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000408300028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000408300029 added to REACTION code. MONIT-REF, ANG added. 2000408300030 ENDBIB 28 0 2000408300031 NOCOMMON 0 0 2000408300032 DATA 3 1 2000408300033 ANG DATA DATA-ERR 2000408300034 ADEG B B 2000408300035 120. 0.152 0.009 2000408300036 ENDDATA 3 0 2000408300037 ENDSUBENT 36 0 2000408399999 SUBENT 20004084 20181026 22732000408400001 BIB 4 7 2000408400002 REACTION ((29-CU-63(N,N+P)28-NI-62,,DA,,4PI)/ 2000408400003 (29-CU-63(N,P)28-NI-63,,DA,,4PI)) 2000408400004 ERR-ANALYS Not given. 2000408400005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000408400006 (DEP,20004083) Cr. section (n,n+p) 2000408400007 (DEP,20004081) REACTION (2) from Subent 081. 2000408400008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000408400009 ENDBIB 7 0 2000408400010 NOCOMMON 0 0 2000408400011 DATA 2 1 2000408400012 ANG DATA 2000408400013 ADEG NO-DIM 2000408400014 120. 1.45 2000408400015 ENDDATA 3 0 2000408400016 ENDSUBENT 15 0 2000408499999 SUBENT 20004085 20181026 22732000408500001 BIB 6 11 2000408500002 REACTION (29-CU-64(0,0),,TEM) 2000408500003 For (n,p) reaction at 120 degrees (compound part). 2000408500004 ANALYSIS From plots of proton spectra assuming the 2000408500005 constant nuclear temperature statistical model. 2000408500006 COMMENT The value of the nuclear temperature of the residual 2000408500007 nucleus formed in a (n,n p) reaction varied between 2000408500008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000408500009 temperature is given. 2000408500010 ERR-ANALYS (ERR-S) Statistical errors 2000408500011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000408500012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000408500013 ENDBIB 11 0 2000408500014 NOCOMMON 0 0 2000408500015 DATA 2 1 2000408500016 DATA ERR-S 2000408500017 MEV MEV 2000408500018 1.1 0.1 2000408500019 ENDDATA 3 0 2000408500020 ENDSUBENT 19 0 2000408599999 SUBENT 20004086 20181026 22732000408600001 BIB 8 32 2000408600002 REACTION 1(30-ZN-64(N,P)29-CU-64,,DA,,4PI) 2000408600003 2(30-ZN-64(N,P)29-CU-64,,DA,,4PI) 2000408600004 ANALYSIS Histograms as a function of angle from 0 to 2000408600005 360 degrees in 2 degree steps give six peaks with a 2000408600006 small uniform background to be subtracted. 2000408600007 .Normalization to obtain the absolute differential 2000408600008 cross section at 120 degrees. 2000408600009 .Histograms as a function of energy from 2 or 3 MeV to 2000408600010 12 MeV in steps of 0.5 MeV or each target peak. 2000408600011 (4PI1A) 4*Pi*differential cross section assuming that 2000408600012 the direct cross section is negligible at this angle 2000408600013 and that the compound cross section is isotropic. 2000408600014 1 Plots of ln(ro(E)) against E with ro based 2000408600015 on constant nuclear temperature model in order 2000408600016 to separate sigma(n,p) from sigma(n,n p). 2000408600017 2 Plots of ln(ro(U)) against (square root(U)) 2000408600018 based on the Fermi gas model in order to separate 2000408600019 sigma(n,p) from sigma(n,n p). 2000408600020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000408600021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000408600022 CORRECTION .Corrected for background and 2000408600023 .isotopic composition of the enriched targets. 2000408600024 .The extrapolation of the proton spectrum below the 2000408600025 bias energy (3 MeV) amounts to a fairly constant 40% 2000408600026 for each nuclide. 2000408600027 ERR-ANALYS (DATA-ERR) Error given includes: 2000408600028 .statistical error from track counting, 2000408600029 .errors due to proton spectrum extrapolation. 2000408600030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000408600031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000408600032 added to REACTION code. REACTION (2) was added. Data 2000408600033 from Subent 087 were added. MONIT-REF, ANG added. 2000408600034 ENDBIB 32 0 2000408600035 NOCOMMON 0 0 2000408600036 DATA 4 1 2000408600037 ANG DATA 1DATA-ERR 1DATA 2 2000408600038 ADEG B B B 2000408600039 120. 0.179 0.018 0.171 2000408600040 ENDDATA 3 0 2000408600041 ENDSUBENT 40 0 2000408699999 NOSUBENT 20004087 20181026 22732000408700001 SUBENT 20004088 20181026 22732000408800001 BIB 8 28 2000408800002 REACTION (30-ZN-64(N,N+P)29-CU-63,,DA,,4PI) 2000408800003 ANALYSIS Histograms as a function of angle from 0 to 2000408800004 360 degrees in 2 degree steps give six peaks with a 2000408800005 small uniform background to be subtracted. 2000408800006 .Normalization to obtain the absolute differential 2000408800007 cross section at 120 degrees. 2000408800008 .Histograms as a function of energy from 2 or 3 MeV to 2000408800009 12 MeV in steps of 0.5 MeV or each target peak. 2000408800010 (4PI1A) 4*Pi*differential cross section assuming that 2000408800011 the direct cross section is negligible at this angle 2000408800012 and that the compound cross section is isotropic. 2000408800013 Subtraction of sigma(n,p) cross section 2000408800014 determined by statistical plot method from the total 2000408800015 proton emission cross section. 2000408800016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000408800017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000408800018 CORRECTION .Corrected for background and 2000408800019 .isotopic composition of the enriched targets. 2000408800020 .The extrapolation of the proton spectrum below the 2000408800021 bias energy (3 MeV) amounts to a fairly constant 40% 2000408800022 for each nuclide. 2000408800023 ERR-ANALYS (DATA-ERR) Error given includes: 2000408800024 .statistical error from track counting, 2000408800025 .errors due to proton spectrum extrapolation. 2000408800026 .Errors are estimated equal to those of sigma(n,p). 2000408800027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000408800028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000408800029 added to REACTION code. MONIT-REF, ANG added. 2000408800030 ENDBIB 28 0 2000408800031 NOCOMMON 0 0 2000408800032 DATA 3 1 2000408800033 ANG DATA DATA-ERR 2000408800034 ADEG B B 2000408800035 120. 0.281 0.018 2000408800036 ENDDATA 3 0 2000408800037 ENDSUBENT 36 0 2000408899999 SUBENT 20004089 20181026 22732000408900001 BIB 4 7 2000408900002 REACTION ((30-ZN-64(N,N+P)29-CU-63,,DA,,4PI)/ 2000408900003 (30-ZN-64(N,P)29-CU-64,,DA,,4PI)) 2000408900004 ERR-ANALYS Not given. 2000408900005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000408900006 (DEP,20004088) Cr. section (n,n+p) 2000408900007 (DEP,20004086) REACTION (2) from Subent 086. 2000408900008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000408900009 ENDBIB 7 0 2000408900010 NOCOMMON 0 0 2000408900011 DATA 2 1 2000408900012 ANG DATA 2000408900013 ADEG NO-DIM 2000408900014 120. 1.64 2000408900015 ENDDATA 3 0 2000408900016 ENDSUBENT 15 0 2000408999999 SUBENT 20004090 20181026 22732000409000001 BIB 6 11 2000409000002 REACTION (30-ZN-65(0,0),,TEM) 2000409000003 For (n,p) reaction at 120 degrees (compound part). 2000409000004 ANALYSIS From plots of proton spectra assuming the 2000409000005 constant nuclear temperature statistical model. 2000409000006 COMMENT The value of the nuclear temperature of the residual 2000409000007 nucleus formed in a (n,n p) reaction varied between 2000409000008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000409000009 temperature is given. 2000409000010 ERR-ANALYS (ERR-S) Statistical errors 2000409000011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000409000012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000409000013 ENDBIB 11 0 2000409000014 NOCOMMON 0 0 2000409000015 DATA 2 1 2000409000016 DATA ERR-S 2000409000017 MEV MEV 2000409000018 1.1 0.1 2000409000019 ENDDATA 3 0 2000409000020 ENDSUBENT 19 0 2000409099999 SUBENT 20004091 20181026 22732000409100001 BIB 8 32 2000409100002 REACTION 1(30-ZN-66(N,P)29-CU-66,,DA,,4PI) 2000409100003 2(30-ZN-66(N,P)29-CU-66,,DA,,4PI) 2000409100004 ANALYSIS Histograms as a function of angle from 0 to 2000409100005 360 degrees in 2 degree steps give six peaks with a 2000409100006 small uniform background to be subtracted. 2000409100007 .Normalization to obtain the absolute differential 2000409100008 cross section at 120 degrees. 2000409100009 .Histograms as a function of energy from 2 or 3 MeV to 2000409100010 12 MeV in steps of 0.5 MeV or each target peak. 2000409100011 (4PI1A) 4*Pi*differential cross section assuming that 2000409100012 the direct cross section is negligible at this angle 2000409100013 and that the compound cross section is isotropic. 2000409100014 1 Plots of ln(ro(E)) against E with ro based 2000409100015 on constant nuclear temperature model in order 2000409100016 to separate sigma(n,p) from sigma(n,n p). 2000409100017 2 Plots of ln(ro(U)) against (square root(U)) 2000409100018 based on the Fermi gas model in order to separate 2000409100019 sigma(n,p) from sigma(n,n p). 2000409100020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000409100021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000409100022 CORRECTION .Corrected for background and 2000409100023 .isotopic composition of the enriched targets. 2000409100024 .The extrapolation of the proton spectrum below the 2000409100025 bias energy (3 MeV) amounts to a fairly constant 40% 2000409100026 for each nuclide. 2000409100027 ERR-ANALYS (DATA-ERR) Error given includes: 2000409100028 .statistical error from track counting, 2000409100029 .errors due to proton spectrum extrapolation. 2000409100030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000409100031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000409100032 added to REACTION code. REACTION (2) was added. Data 2000409100033 from Subent 092 were added. MONIT-REF, ANG added. 2000409100034 ENDBIB 32 0 2000409100035 NOCOMMON 0 0 2000409100036 DATA 4 1 2000409100037 ANG DATA 1DATA-ERR 1DATA 2 2000409100038 ADEG B B B 2000409100039 120. 0.034 0.004 0.035 2000409100040 ENDDATA 3 0 2000409100041 ENDSUBENT 40 0 2000409199999 NOSUBENT 20004092 20181026 22732000409200001 SUBENT 20004093 20181026 22732000409300001 BIB 8 28 2000409300002 REACTION (30-ZN-66(N,N+P)29-CU-65,,DA,,4PI) 2000409300003 ANALYSIS Histograms as a function of angle from 0 to 2000409300004 360 degrees in 2 degree steps give six peaks with a 2000409300005 small uniform background to be subtracted. 2000409300006 .Normalization to obtain the absolute differential 2000409300007 cross section at 120 degrees. 2000409300008 .Histograms as a function of energy from 2 or 3 MeV to 2000409300009 12 MeV in steps of 0.5 MeV or each target peak. 2000409300010 (4PI1A) 4*Pi*differential cross section assuming that 2000409300011 the direct cross section is negligible at this angle 2000409300012 and that the compound cross section is isotropic. 2000409300013 Subtraction of sigma(n,p) cross section 2000409300014 determined by statistical plot method from the total 2000409300015 proton emission cross section. 2000409300016 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000409300017 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000409300018 CORRECTION .Corrected for background and 2000409300019 .isotopic composition of the enriched targets. 2000409300020 .The extrapolation of the proton spectrum below the 2000409300021 bias energy (3 MeV) amounts to a fairly constant 40% 2000409300022 for each nuclide. 2000409300023 ERR-ANALYS (DATA-ERR) Error given includes: 2000409300024 .statistical error from track counting, 2000409300025 .errors due to proton spectrum extrapolation. 2000409300026 .Errors are estimated equal to those of sigma(n,p). 2000409300027 STATUS (TABLE) Table 4, Nucl.Phys.,24,p.294. 2000409300028 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000409300029 added to REACTION code. MONIT-REF, ANG added. 2000409300030 ENDBIB 28 0 2000409300031 NOCOMMON 0 0 2000409300032 DATA 3 1 2000409300033 ANG DATA DATA-ERR 2000409300034 ADEG B B 2000409300035 120. 0.050 0.004 2000409300036 ENDDATA 3 0 2000409300037 ENDSUBENT 36 0 2000409399999 SUBENT 20004094 20181026 22732000409400001 BIB 4 7 2000409400002 REACTION ((30-ZN-66(N,N+P)29-CU-65,,DA,,4PI)/ 2000409400003 (30-ZN-66(N,P)29-CU-66,,DA,,4PI)) 2000409400004 ERR-ANALYS Not given. 2000409400005 STATUS (TABLE) Table 4, Nucl.Phys.,24,P.294. 2000409400006 (DEP,20004093) Cr. section (n,n+p) 2000409400007 (DEP,20004091) REACTION (2) from Subent 091. 2000409400008 HISTORY (20181026U) SD: STATUS updated. ANG added. 2000409400009 ENDBIB 7 0 2000409400010 NOCOMMON 0 0 2000409400011 DATA 2 1 2000409400012 ANG DATA 2000409400013 ADEG NO-DIM 2000409400014 120. 1.43 2000409400015 ENDDATA 3 0 2000409400016 ENDSUBENT 15 0 2000409499999 SUBENT 20004095 20181026 22732000409500001 BIB 8 32 2000409500002 REACTION 1(30-ZN-67(N,P)29-CU-67,,DA,,4PI) 2000409500003 2(30-ZN-67(N,P)29-CU-67,,DA,,4PI) 2000409500004 ANALYSIS Histograms as a function of angle from 0 to 2000409500005 360 degrees in 2 degree steps give six peaks with a 2000409500006 small uniform background to be subtracted. 2000409500007 .Normalization to obtain the absolute differential 2000409500008 cross section at 120 degrees. 2000409500009 .Histograms as a function of energy from 2 or 3 MeV to 2000409500010 12 MeV in steps of 0.5 MeV or each target peak. 2000409500011 (4PI1A) 4*Pi*differential cross section assuming that 2000409500012 the direct cross section is negligible at this angle 2000409500013 and that the compound cross section is isotropic. 2000409500014 1 Plots of ln(ro(E)) against E with ro based 2000409500015 on constant nuclear temperature model in order 2000409500016 to separate sigma(n,p) from sigma(n,n p). 2000409500017 2 Plots of ln(ro(U)) against (square root(U)) 2000409500018 based on the Fermi gas model in order to separate 2000409500019 sigma(n,p) from sigma(n,n p). 2000409500020 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000409500021 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000409500022 CORRECTION .Corrected for background and 2000409500023 .isotopic composition of the enriched targets. 2000409500024 .The extrapolation of the proton spectrum below the 2000409500025 bias energy (3 MeV) amounts to a fairly constant 40% 2000409500026 for each nuclide. 2000409500027 ERR-ANALYS (DATA-ERR) Error given includes: 2000409500028 .statistical error from track counting, 2000409500029 .errors due to proton spectrum extrapolation. 2000409500030 STATUS (TABLE) Table 1, Nucl.Phys.,24,p.280. 2000409500031 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000409500032 added to REACTION code. REACTION (2) was added. Data 2000409500033 from Subent 096 were added. MONIT-REF, ANG added. 2000409500034 ENDBIB 32 0 2000409500035 NOCOMMON 0 0 2000409500036 DATA 4 1 2000409500037 ANG DATA 1DATA-ERR 1DATA 2 2000409500038 ADEG B B B 2000409500039 120. 0.041 0.007 0.033 2000409500040 ENDDATA 3 0 2000409500041 ENDSUBENT 40 0 2000409599999 NOSUBENT 20004096 20181026 22732000409600001 SUBENT 20004097 20181026 22732000409700001 BIB 6 11 2000409700002 REACTION (30-ZN-67(0,0),,TEM) 2000409700003 For (n,p) reaction at 120 degrees (compound part). 2000409700004 ANALYSIS From plots of proton spectra assuming the 2000409700005 constant nuclear temperature statistical model. 2000409700006 COMMENT The value of the nuclear temperature of the residual 2000409700007 nucleus formed in a (n,n p) reaction varied between 2000409700008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000409700009 temperature is given. 2000409700010 ERR-ANALYS (ERR-S) Statistical errors 2000409700011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000409700012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000409700013 ENDBIB 11 0 2000409700014 NOCOMMON 0 0 2000409700015 DATA 2 1 2000409700016 DATA ERR-S 2000409700017 MEV MEV 2000409700018 1.1 0.1 2000409700019 ENDDATA 3 0 2000409700020 ENDSUBENT 19 0 2000409799999 SUBENT 20004098 20181026 22732000409800001 BIB 6 11 2000409800002 REACTION (30-ZN-68(0,0),,TEM) 2000409800003 For (n,p) reaction at 120 degrees (compound part). 2000409800004 ANALYSIS From plots of proton spectra assuming the 2000409800005 constant nuclear temperature statistical model. 2000409800006 COMMENT The value of the nuclear temperature of the residual 2000409800007 nucleus formed in a (n,n p) reaction varied between 2000409800008 0.3 and 0.4 MeV for all nuclei for which a nuclear 2000409800009 temperature is given. 2000409800010 ERR-ANALYS (ERR-S) Statistical errors 2000409800011 STATUS (TABLE) Table 2, Nucl.Phys.,24,p.292. 2000409800012 HISTORY (20181026U) SD: DATA-ERR -> ERR-S. 2000409800013 ENDBIB 11 0 2000409800014 NOCOMMON 0 0 2000409800015 DATA 2 1 2000409800016 DATA ERR-S 2000409800017 MEV MEV 2000409800018 1.1 0.1 2000409800019 ENDDATA 3 0 2000409800020 ENDSUBENT 19 0 2000409899999 SUBENT 20004099 20181026 22732000409900001 BIB 8 21 2000409900002 REACTION (33-AS-75(N,P)32-GE-75,,DA,,4PI) 2000409900003 ANALYSIS Histograms as a function of angle from 0 to 2000409900004 360 degrees in 2 degree steps give six peaks with a 2000409900005 small uniform background to be subtracted. 2000409900006 .Histograms as a function of energy from 2 or 3 MeV to 2000409900007 12 MeV in steps of 0.5 MeV or each target peak. 2000409900008 (4PI1A) 4*Pi*differential cross section assuming that 2000409900009 the direct cross section is negligible at this angle 2000409900010 and that the compound cross section is isotropic. 2000409900011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000409900012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000409900013 CORRECTION .Corrected for background. 2000409900014 .The extrapolation of the proton spectrum below the 2000409900015 bias energy (3 MeV) amounts to a fairly constant 40% 2000409900016 for each nuclide. 2000409900017 ERR-ANALYS (DATA-ERR) Error given includes: 2000409900018 .statistical error from track counting, 2000409900019 .errors due to proton spectrum extrapolation. 2000409900020 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000409900021 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000409900022 added to REACTION code. MONIT-REF, ANG added. 2000409900023 ENDBIB 21 0 2000409900024 NOCOMMON 0 0 2000409900025 DATA 3 1 2000409900026 ANG DATA DATA-ERR 2000409900027 ADEG B B 2000409900028 120. 0.027 0.005 2000409900029 ENDDATA 3 0 2000409900030 ENDSUBENT 29 0 2000409999999 SUBENT 20004100 20181026 22732000410000001 BIB 7 16 2000410000002 REACTION (34-SE-0(N,P),,DA,,4PI) 2000410000003 ANALYSIS Histograms as a function of angle from 0 to 2000410000004 360 degrees in 2 degree steps give six peaks with a 2000410000005 small uniform background to be subtracted. 2000410000006 .Histograms as a function of energy from 2 or 3 MeV to 2000410000007 12 MeV in steps of 0.5 MeV or each target peak. 2000410000008 (4PI1A) 4*Pi*differential cross section assuming that 2000410000009 the direct cross section is negligible at this angle 2000410000010 and that the compound cross section is isotropic. 2000410000011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410000012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410000013 ERR-ANALYS Only an upper limit could be given because of bad 2000410000014 signal to background ratio. 2000410000015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410000016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410000017 added to REACTION code. MONIT-REF, ANG added. 2000410000018 ENDBIB 16 0 2000410000019 NOCOMMON 0 0 2000410000020 DATA 2 1 2000410000021 ANG DATA-MAX 2000410000022 ADEG B 2000410000023 120. 0.014 2000410000024 ENDDATA 3 0 2000410000025 ENDSUBENT 24 0 2000410099999 SUBENT 20004101 20181026 22732000410100001 BIB 7 16 2000410100002 REACTION (35-BR-0(N,P),,DA,,4PI) 2000410100003 ANALYSIS Histograms as a function of angle from 0 to 2000410100004 360 degrees in 2 degree steps give six peaks with a 2000410100005 small uniform background to be subtracted. 2000410100006 .Histograms as a function of energy from 2 or 3 MeV to 2000410100007 12 MeV in steps of 0.5 MeV or each target peak. 2000410100008 (4PI1A) 4*Pi*differential cross section assuming that 2000410100009 the direct cross section is negligible at this angle 2000410100010 and that the compound cross section is isotropic. 2000410100011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410100012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410100013 ERR-ANALYS Only an upper limit could be given because of bad 2000410100014 signal to background ratio. 2000410100015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410100016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410100017 added to REACTION code. MONIT-REF, ANG added. 2000410100018 ENDBIB 16 0 2000410100019 NOCOMMON 0 0 2000410100020 DATA 2 1 2000410100021 ANG DATA-MAX 2000410100022 ADEG B 2000410100023 120. 0.014 2000410100024 ENDDATA 3 0 2000410100025 ENDSUBENT 24 0 2000410199999 SUBENT 20004102 20181026 22732000410200001 BIB 8 21 2000410200002 REACTION (38-SR-0(N,P),,DA,,4PI) 2000410200003 ANALYSIS Histograms as a function of angle from 0 to 2000410200004 360 degrees in 2 degree steps give six peaks with a 2000410200005 small uniform background to be subtracted. 2000410200006 .Histograms as a function of energy from 2 or 3 MeV to 2000410200007 12 MeV in steps of 0.5 MeV or each target peak. 2000410200008 (4PI1A) 4*Pi*differential cross section assuming that 2000410200009 the direct cross section is negligible at this angle 2000410200010 and that the compound cross section is isotropic. 2000410200011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410200012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410200013 CORRECTION .Corrected for background. 2000410200014 .The extrapolation of the proton spectrum below the 2000410200015 bias energy (3 MeV) amounts to a fairly constant 40% 2000410200016 for each nuclide. 2000410200017 ERR-ANALYS (DATA-ERR) Error given includes: 2000410200018 .statistical error from track counting, 2000410200019 .errors due to proton spectrum extrapolation. 2000410200020 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410200021 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410200022 added to REACTION code. MONIT-REF, ANG added. 2000410200023 ENDBIB 21 0 2000410200024 NOCOMMON 0 0 2000410200025 DATA 3 1 2000410200026 ANG DATA DATA-ERR 2000410200027 ADEG B B 2000410200028 120. 0.022 0.017 2000410200029 ENDDATA 3 0 2000410200030 ENDSUBENT 29 0 2000410299999 SUBENT 20004103 20181026 22732000410300001 BIB 8 21 2000410300002 REACTION (40-ZR-0(N,P),,DA,,4PI) 2000410300003 ANALYSIS Histograms as a function of angle from 0 to 2000410300004 360 degrees in 2 degree steps give six peaks with a 2000410300005 small uniform background to be subtracted. 2000410300006 .Histograms as a function of energy from 2 or 3 MeV to 2000410300007 12 MeV in steps of 0.5 MeV or each target peak. 2000410300008 (4PI1A) 4*Pi*differential cross section assuming that 2000410300009 the direct cross section is negligible at this angle 2000410300010 and that the compound cross section is isotropic. 2000410300011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410300012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410300013 CORRECTION .Corrected for background. 2000410300014 .The extrapolation of the proton spectrum below the 2000410300015 bias energy (3 MeV) amounts to a fairly constant 40% 2000410300016 for each nuclide. 2000410300017 ERR-ANALYS (DATA-ERR) Error given includes: 2000410300018 .statistical error from track counting, 2000410300019 .errors due to proton spectrum extrapolation. 2000410300020 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410300021 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410300022 added to REACTION code. MONIT-REF, ANG added. 2000410300023 ENDBIB 21 0 2000410300024 NOCOMMON 0 0 2000410300025 DATA 3 1 2000410300026 ANG DATA DATA-ERR 2000410300027 ADEG B B 2000410300028 120. 0.062 0.012 2000410300029 ENDDATA 3 0 2000410300030 ENDSUBENT 29 0 2000410399999 SUBENT 20004104 20181026 22732000410400001 BIB 8 21 2000410400002 REACTION (42-MO-0(N,P),,DA,,4PI) 2000410400003 ANALYSIS Histograms as a function of angle from 0 to 2000410400004 360 degrees in 2 degree steps give six peaks with a 2000410400005 small uniform background to be subtracted. 2000410400006 .Histograms as a function of energy from 2 or 3 MeV to 2000410400007 12 MeV in steps of 0.5 MeV or each target peak. 2000410400008 (4PI1A) 4*Pi*differential cross section assuming that 2000410400009 the direct cross section is negligible at this angle 2000410400010 and that the compound cross section is isotropic. 2000410400011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410400012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410400013 CORRECTION .Corrected for background. 2000410400014 .The extrapolation of the proton spectrum below the 2000410400015 bias energy (3 MeV) amounts to a fairly constant 40% 2000410400016 for each nuclide. 2000410400017 ERR-ANALYS (DATA-ERR) Error given includes: 2000410400018 .statistical error from track counting, 2000410400019 .errors due to proton spectrum extrapolation. 2000410400020 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410400021 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410400022 added to REACTION code. MONIT-REF, ANG added. 2000410400023 ENDBIB 21 0 2000410400024 NOCOMMON 0 0 2000410400025 DATA 3 1 2000410400026 ANG DATA DATA-ERR 2000410400027 ADEG B B 2000410400028 120. 0.120 0.020 2000410400029 ENDDATA 3 0 2000410400030 ENDSUBENT 29 0 2000410499999 SUBENT 20004105 20181026 22732000410500001 BIB 7 16 2000410500002 REACTION (47-AG-0(N,P),,DA,,4PI) 2000410500003 ANALYSIS Histograms as a function of angle from 0 to 2000410500004 360 degrees in 2 degree steps give six peaks with a 2000410500005 small uniform background to be subtracted. 2000410500006 .Histograms as a function of energy from 2 or 3 MeV to 2000410500007 12 MeV in steps of 0.5 MeV or each target peak. 2000410500008 (4PI1A) 4*Pi*differential cross section assuming that 2000410500009 the direct cross section is negligible at this angle 2000410500010 and that the compound cross section is isotropic. 2000410500011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410500012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410500013 ERR-ANALYS Only an upper limit could be given because of bad 2000410500014 signal to background ratio. 2000410500015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410500016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410500017 added to REACTION code. MONIT-REF, ANG added. 2000410500018 ENDBIB 16 0 2000410500019 NOCOMMON 0 0 2000410500020 DATA 2 1 2000410500021 ANG DATA-MAX 2000410500022 ADEG B 2000410500023 120. 0.014 2000410500024 ENDDATA 3 0 2000410500025 ENDSUBENT 24 0 2000410599999 SUBENT 20004106 20181026 22732000410600001 BIB 7 16 2000410600002 REACTION (48-CD-0(N,P),,DA,,4PI) 2000410600003 ANALYSIS Histograms as a function of angle from 0 to 2000410600004 360 degrees in 2 degree steps give six peaks with a 2000410600005 small uniform background to be subtracted. 2000410600006 .Histograms as a function of energy from 2 or 3 MeV to 2000410600007 12 MeV in steps of 0.5 MeV or each target peak. 2000410600008 (4PI1A) 4*Pi*differential cross section assuming that 2000410600009 the direct cross section is negligible at this angle 2000410600010 and that the compound cross section is isotropic. 2000410600011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410600012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410600013 ERR-ANALYS Only an upper limit could be given because of bad 2000410600014 signal to background ratio. 2000410600015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410600016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410600017 added to REACTION code. MONIT-REF, ANG added. 2000410600018 ENDBIB 16 0 2000410600019 NOCOMMON 0 0 2000410600020 DATA 2 1 2000410600021 ANG DATA-MAX 2000410600022 ADEG B 2000410600023 120. 0.014 2000410600024 ENDDATA 3 0 2000410600025 ENDSUBENT 24 0 2000410699999 SUBENT 20004107 20181026 22732000410700001 BIB 7 16 2000410700002 REACTION (49-IN-0(N,P),,DA,,4PI) 2000410700003 ANALYSIS Histograms as a function of angle from 0 to 2000410700004 360 degrees in 2 degree steps give six peaks with a 2000410700005 small uniform background to be subtracted. 2000410700006 .Histograms as a function of energy from 2 or 3 MeV to 2000410700007 12 MeV in steps of 0.5 MeV or each target peak. 2000410700008 (4PI1A) 4*Pi*differential cross section assuming that 2000410700009 the direct cross section is negligible at this angle 2000410700010 and that the compound cross section is isotropic. 2000410700011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410700012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410700013 ERR-ANALYS Only an upper limit could be given because of bad 2000410700014 signal to background ratio. 2000410700015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410700016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410700017 added to REACTION code. MONIT-REF, ANG added. 2000410700018 ENDBIB 16 0 2000410700019 NOCOMMON 0 0 2000410700020 DATA 2 1 2000410700021 ANG DATA-MAX 2000410700022 ADEG B 2000410700023 120. 0.014 2000410700024 ENDDATA 3 0 2000410700025 ENDSUBENT 24 0 2000410799999 SUBENT 20004108 20181026 22732000410800001 BIB 7 16 2000410800002 REACTION (50-SN-0(N,P),,DA,,4PI) 2000410800003 ANALYSIS Histograms as a function of angle from 0 to 2000410800004 360 degrees in 2 degree steps give six peaks with a 2000410800005 small uniform background to be subtracted. 2000410800006 .Histograms as a function of energy from 2 or 3 MeV to 2000410800007 12 MeV in steps of 0.5 MeV or each target peak. 2000410800008 (4PI1A) 4*Pi*differential cross section assuming that 2000410800009 the direct cross section is negligible at this angle 2000410800010 and that the compound cross section is isotropic. 2000410800011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410800012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410800013 ERR-ANALYS Only an upper limit could be given because of bad 2000410800014 signal to background ratio. 2000410800015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410800016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410800017 added to REACTION code. MONIT-REF, ANG added. 2000410800018 ENDBIB 16 0 2000410800019 NOCOMMON 0 0 2000410800020 DATA 2 1 2000410800021 ANG DATA-MAX 2000410800022 ADEG B 2000410800023 120. 0.015 2000410800024 ENDDATA 3 0 2000410800025 ENDSUBENT 24 0 2000410899999 SUBENT 20004109 20181026 22732000410900001 BIB 8 21 2000410900002 REACTION (51-SB-0(N,P),,DA,,4PI) 2000410900003 ANALYSIS Histograms as a function of angle from 0 to 2000410900004 360 degrees in 2 degree steps give six peaks with a 2000410900005 small uniform background to be subtracted. 2000410900006 .Histograms as a function of energy from 2 or 3 MeV to 2000410900007 12 MeV in steps of 0.5 MeV or each target peak. 2000410900008 (4PI1A) 4*Pi*differential cross section assuming that 2000410900009 the direct cross section is negligible at this angle 2000410900010 and that the compound cross section is isotropic. 2000410900011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000410900012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000410900013 CORRECTION .Corrected for background. 2000410900014 .The extrapolation of the proton spectrum below the 2000410900015 bias energy (3 MeV) amounts to a fairly constant 40% 2000410900016 for each nuclide. 2000410900017 ERR-ANALYS (DATA-ERR) Error given includes: 2000410900018 .statistical error from track counting, 2000410900019 .errors due to proton spectrum extrapolation. 2000410900020 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000410900021 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000410900022 added to REACTION code. MONIT-REF, ANG added. 2000410900023 ENDBIB 21 0 2000410900024 NOCOMMON 0 0 2000410900025 DATA 3 1 2000410900026 ANG DATA DATA-ERR 2000410900027 ADEG B B 2000410900028 120. 0.011 0.006 2000410900029 ENDDATA 3 0 2000410900030 ENDSUBENT 29 0 2000410999999 SUBENT 20004110 20181026 22732000411000001 BIB 7 16 2000411000002 REACTION (52-TE-0(N,P),,DA,,4PI) 2000411000003 ANALYSIS Histograms as a function of angle from 0 to 2000411000004 360 degrees in 2 degree steps give six peaks with a 2000411000005 small uniform background to be subtracted. 2000411000006 .Histograms as a function of energy from 2 or 3 MeV to 2000411000007 12 MeV in steps of 0.5 MeV or each target peak. 2000411000008 (4PI1A) 4*Pi*differential cross section assuming that 2000411000009 the direct cross section is negligible at this angle 2000411000010 and that the compound cross section is isotropic. 2000411000011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000411000012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000411000013 ERR-ANALYS Only an upper limit could be given because of bad 2000411000014 signal to background ratio. 2000411000015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000411000016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000411000017 added to REACTION code. MONIT-REF, ANG added. 2000411000018 ENDBIB 16 0 2000411000019 NOCOMMON 0 0 2000411000020 DATA 2 1 2000411000021 ANG DATA-MAX 2000411000022 ADEG B 2000411000023 120. 0.005 2000411000024 ENDDATA 3 0 2000411000025 ENDSUBENT 24 0 2000411099999 SUBENT 20004111 20181026 22732000411100001 BIB 7 16 2000411100002 REACTION (53-I-127(N,P)52-TE-127,,DA,,4PI) 2000411100003 ANALYSIS Histograms as a function of angle from 0 to 2000411100004 360 degrees in 2 degree steps give six peaks with a 2000411100005 small uniform background to be subtracted. 2000411100006 .Histograms as a function of energy from 2 or 3 MeV to 2000411100007 12 MeV in steps of 0.5 MeV or each target peak. 2000411100008 (4PI1A) 4*Pi*differential cross section assuming that 2000411100009 the direct cross section is negligible at this angle 2000411100010 and that the compound cross section is isotropic. 2000411100011 MONITOR (26-FE-56(N,X)1-H-1,,DA) at 120 degr. 2000411100012 MONIT-REF (20961001,D.L.Allan,J,NP,10,348,1959) 2000411100013 ERR-ANALYS Only an upper limit could be given because of bad 2000411100014 signal to background ratio. 2000411100015 STATUS (TABLE) Table 3, Nucl.Phys.,24,p.293. 2000411100016 HISTORY (20181026A) SD: SF5=CN deleted; SF6=SIG -> DA; SF8=4PI 2000411100017 added to REACTION code. MONIT-REF, ANG added. 2000411100018 ENDBIB 16 0 2000411100019 NOCOMMON 0 0 2000411100020 DATA 2 1 2000411100021 ANG DATA-MAX 2000411100022 ADEG B 2000411100023 120. 0.005 2000411100024 ENDDATA 3 0 2000411100025 ENDSUBENT 24 0 2000411199999 ENDENTRY 111 0 2000499999999