ENTRY O1426 20221223 O092O1426 0 1 SUBENT O1426001 20221223 O092O1426 1 1 BIB 11 35 O1426 1 2 TITLE Systematic investigation of 1.2-GeV proton-induced O1426 1 3 spallation reactions on targets between Al and U. O1426 1 4 AUTHOR (C.-M.Herbach, D.Hilscher, U.Jahnke, V.G.Tishchenko, O1426 1 5 J.Galin, A.Letourneau, A.Peghaire, D.Filges, O1426 1 6 F.Goldenbaum, L.Pienkowski, W.U.Schroeder, J.Toke) O1426 1 7 REFERENCE (J,NIM/A,562,729,2006) O1426 1 8 REL-REF (I,O1305001,C.-M.Herbach+,J,NP/A,765,426,2006) More O1426 1 9 details of experiment. O1426 1 10 INSTITUTE (2GERBER,2FR GAN,2GERJUL,3POLWWA,1USAROC) O1426 1 11 DETECTOR (SPEC) The experiments utilised the 4pi-detector NESSIO1426 1 12 (Neutron Scintillator tank and Silicon ball) for an O1426 1 13 efficient and simultaneous detection of neutrons and O1426 1 14 charged particles. In addition to the Berlin Neutron O1426 1 15 Ball (BNB), and the Berlin Silicon Ball (BSiB), the O1426 1 16 setup has been equipped with six threefold delta-E-E O1426 1 17 telescopes. Each telescope consists of a stack of O1426 1 18 three delta-E Si detectors with thicknesses of 25-27 O1426 1 19 mum, 80-90 mum and approximately 1000 mum, backed by a O1426 1 20 7-cm thick CsI(Tl) crystal of 4 cm in diameter. O1426 1 21 FACILITY (SYNCH,2GERGSI) The Cooler Synchrotron Facility COSY. O1426 1 22 METHOD (EXTB) O1426 1 23 (TOF) Particle identification with BSiB detectors wasO1426 1 24 obtained by means of energy and time-of-flight O1426 1 25 measurements; O1426 1 26 (EDE) For the Si/CsI(Tl) telescopes. O1426 1 27 ADD-RES (COMP) Results of simulation calculations with the O1426 1 28 intra-nuclear cascade code INCL2.0 coupled to the O1426 1 29 statistical model GEMINI. O1426 1 30 CORRECTION The cross sections are corrected for the counting O1426 1 31 losses. O1426 1 32 HISTORY (20081125C) SB O1426 1 33 (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O1426 1 34 SF8=RAW added in REACTION code in Subents 2-11 O1426 1 35 according MEMO CP-C/406. O1426 1 36 (20221223A) SD: Correction in several Subents. O1426 1 37 ENDBIB 35 0 O1426 1 38 COMMON 1 3 O1426 1 39 EN O1426 1 40 MEV O1426 1 41 1200. O1426 1 42 ENDCOMMON 3 0 O1426 1 43 ENDSUBENT 42 0 O1426 199999 SUBENT O1426002 20140205 O052O142600200001 BIB 6 27 O142600200002 REACTION (13-AL-27(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600200003 see CORRECTION O142600200004 CORRECTION Not corrected for the neutron energy dependent O142600200005 efficiency. O142600200006 The following corrections have been applied to the O142600200007 measured distributions- O142600200008 -the portion of background from reaction outside the O142600200009 target 1-2%,or He4. O142600200010 -events rejected by the double reactions inspection O142600200011 2-4% are accounted for, continuously monitored duringO142600200012 the runs, O142600200013 -An off-line threshold was introduced into the O142600200014 measured BNB-light spectrum at 10 MeV to cut events O142600200015 from electrons observed at M(n) less than 3. The O142600200016 extrapolation to zero energy was estimated assuming O142600200017 similar spectra shapes as measured for M(n)=3-5, O142600200018 -A small portion of elastically scattered beam protonsO142600200019 may enter the BNB scintillator thus simulating real O142600200020 events. This background of about 1-3% contributes to O142600200021 the peak observed in the BNB-light spectrum which is O142600200022 well pronounced for M(n) less or equal 5 at energies O142600200023 of about 50 MeV. O142600200024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600200025 STATUS (CURVE).By CAJAD. Digitized from fig.2 of NIM/A,562,729O142600200026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600200027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600200028 SF8=RAW added in REACTION code O142600200029 ENDBIB 27 0 O142600200030 COMMON 1 3 O142600200031 ERR-DIG O142600200032 MB O142600200033 1.1 O142600200034 ENDCOMMON 3 0 O142600200035 DATA 2 8 O142600200036 PART-OUT DATA O142600200037 NO-DIM MB O142600200038 0. 72.6 O142600200039 1. 109.1 O142600200040 2. 98.6 O142600200041 3. 71.8 O142600200042 4. 47.3 O142600200043 5. 29.8 O142600200044 6. 14.6 O142600200045 7. 8.7 O142600200046 ENDDATA 10 0 O142600200047 ENDSUBENT 46 0 O142600299999 SUBENT O1426003 20140205 O052O142600300001 BIB 6 27 O142600300002 REACTION (26-FE-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600300003 see CORRECTION O142600300004 CORRECTION Not corrected for the neutron energy dependent O142600300005 efficiency. O142600300006 The following corrections have been applied to the O142600300007 measured distributions- O142600300008 -the portion of background from reaction outside the O142600300009 target 1-2%,or He4. O142600300010 -events rejected by the double reactions inspection O142600300011 2-4% are accounted for, continuously monitored duringO142600300012 the runs, O142600300013 -An off-line threshold was introduced into the O142600300014 measured BNB-light spectrum at 10 MeV to cut events O142600300015 from electrons observed at M(n) less than 3. The O142600300016 extrapolation to zero energy was estimated assuming O142600300017 similar spectra shapes as measured for M(n)=3-5, O142600300018 -A small portion of elastically scattered beam protonsO142600300019 may enter the BNB scintillator thus simulating real O142600300020 events. This background of about 1-3% contributes to O142600300021 the peak observed in the BNB-light spectrum which is O142600300022 well pronounced for M(n) less or equal 5 at energies O142600300023 of about 50 MeV. O142600300024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600300025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142600300026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600300027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600300028 SF8=RAW added in REACTION code O142600300029 ENDBIB 27 0 O142600300030 COMMON 1 3 O142600300031 ERR-DIG O142600300032 MB O142600300033 1.1 O142600300034 ENDCOMMON 3 0 O142600300035 DATA 2 11 O142600300036 PART-OUT DATA O142600300037 NO-DIM MB O142600300038 0. 66.9 O142600300039 1. 99.3 O142600300040 2. 120.2 O142600300041 3. 122.7 O142600300042 4. 109.2 O142600300043 5. 87.2 O142600300044 6. 61.4 O142600300045 7. 37.8 O142600300046 8. 22.7 O142600300047 9. 15.2 O142600300048 10. 7.9 O142600300049 ENDDATA 13 0 O142600300050 ENDSUBENT 49 0 O142600399999 SUBENT O1426004 20140205 O052O142600400001 BIB 6 27 O142600400002 REACTION (28-NI-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600400003 see CORRECTION O142600400004 CORRECTION Not corrected for the neutron energy dependent O142600400005 efficiency. O142600400006 The following corrections have been applied to the O142600400007 measured distributions- O142600400008 -the portion of background from reaction outside the O142600400009 target 1-2%,or He4. O142600400010 -events rejected by the double reactions inspection O142600400011 2-4% are accounted for, continuously monitored duringO142600400012 the runs, O142600400013 -An off-line threshold was introduced into the O142600400014 measured BNB-light spectrum at 10 MeV to cut events O142600400015 from electrons observed at M(n) less than 3. The O142600400016 extrapolation to zero energy was estimated assuming O142600400017 similar spectra shapes as measured for M(n)=3-5, O142600400018 -A small portion of elastically scattered beam protonsO142600400019 may enter the BNB scintillator thus simulating real O142600400020 events. This background of about 1-3% contributes to O142600400021 the peak observed in the BNB-light spectrum which is O142600400022 well pronounced for M(n) less or equal 5 at energies O142600400023 of about 50 MeV. O142600400024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600400025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142600400026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600400027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600400028 SF8=RAW added in REACTION code O142600400029 ENDBIB 27 0 O142600400030 COMMON 1 3 O142600400031 ERR-DIG O142600400032 MB O142600400033 1.1 O142600400034 ENDCOMMON 3 0 O142600400035 DATA 2 11 O142600400036 PART-OUT DATA O142600400037 NO-DIM MB O142600400038 0. 83. O142600400039 1. 114.9 O142600400040 2. 125.5 O142600400041 3. 122.3 O142600400042 4. 103.1 O142600400043 5. 80.9 O142600400044 6. 53.4 O142600400045 7. 31.9 O142600400046 8. 18.8 O142600400047 9. 8. O142600400048 10. 4.1 O142600400049 ENDDATA 13 0 O142600400050 ENDSUBENT 49 0 O142600499999 SUBENT O1426005 20140205 O052O142600500001 BIB 6 27 O142600500002 REACTION (29-CU-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600500003 see CORRECTION O142600500004 CORRECTION Not corrected for the neutron energy dependent O142600500005 efficiency. O142600500006 The following corrections have been applied to the O142600500007 measured distributions- O142600500008 -the portion of background from reaction outside the O142600500009 target 1-2%,or He4. O142600500010 -events rejected by the double reactions inspection O142600500011 2-4% are accounted for, continuously monitored duringO142600500012 the runs, O142600500013 -An off-line threshold was introduced into the O142600500014 measured BNB-light spectrum at 10 MeV to cut events O142600500015 from electrons observed at M(n) less than 3. The O142600500016 extrapolation to zero energy was estimated assuming O142600500017 similar spectra shapes as measured for M(n)=3-5, O142600500018 -A small portion of elastically scattered beam protonsO142600500019 may enter the BNB scintillator thus simulating real O142600500020 events. This background of about 1-3% contributes to O142600500021 the peak observed in the BNB-light spectrum which is O142600500022 well pronounced for M(n) less or equal 5 at energies O142600500023 of about 50 MeV. O142600500024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600500025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142600500026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600500027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600500028 SF8=RAW added in REACTION code O142600500029 ENDBIB 27 0 O142600500030 COMMON 1 3 O142600500031 ERR-DIG O142600500032 MB O142600500033 1.1 O142600500034 ENDCOMMON 3 0 O142600500035 DATA 2 12 O142600500036 PART-OUT DATA O142600500037 NO-DIM MB O142600500038 0. 54.7 O142600500039 1. 85.6 O142600500040 2. 105.7 O142600500041 3. 118.9 O142600500042 4. 119.8 O142600500043 5. 105.3 O142600500044 6. 85.4 O142600500045 7. 57.8 O142600500046 8. 37.1 O142600500047 9. 20.3 O142600500048 10. 11.2 O142600500049 11. 6. O142600500050 ENDDATA 14 0 O142600500051 ENDSUBENT 50 0 O142600599999 SUBENT O1426006 20140205 O052O142600600001 BIB 6 27 O142600600002 REACTION (40-ZR-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600600003 see CORRECTION O142600600004 CORRECTION Not corrected for the neutron energy dependent O142600600005 efficiency. O142600600006 The following corrections have been applied to the O142600600007 measured distributions- O142600600008 -the portion of background from reaction outside the O142600600009 target 1-2%,or He4. O142600600010 -events rejected by the double reactions inspection O142600600011 2-4% are accounted for, continuously monitored duringO142600600012 the runs, O142600600013 -An off-line threshold was introduced into the O142600600014 measured BNB-light spectrum at 10 MeV to cut events O142600600015 from electrons observed at M(n) less than 3. The O142600600016 extrapolation to zero energy was estimated assuming O142600600017 similar spectra shapes as measured for M(n)=3-5, O142600600018 -A small portion of elastically scattered beam protonsO142600600019 may enter the BNB scintillator thus simulating real O142600600020 events. This background of about 1-3% contributes to O142600600021 the peak observed in the BNB-light spectrum which is O142600600022 well pronounced for M(n) less or equal 5 at energies O142600600023 of about 50 MeV.Digitized from fig.2 of NIM/A,562,729 O142600600024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600600025 STATUS (CURVE).By CAJAD. O142600600026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600600027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600600028 SF8=RAW added in REACTION code O142600600029 ENDBIB 27 0 O142600600030 COMMON 1 3 O142600600031 ERR-DIG O142600600032 MB O142600600033 1.1 O142600600034 ENDCOMMON 3 0 O142600600035 DATA 2 15 O142600600036 PART-OUT DATA O142600600037 NO-DIM MB O142600600038 0. 58.2 O142600600039 1. 73. O142600600040 2. 86.9 O142600600041 3. 102.5 O142600600042 4. 110.4 O142600600043 5. 115.2 O142600600044 6. 116.9 O142600600045 7. 107.2 O142600600046 8. 92.9 O142600600047 9. 72.6 O142600600048 10. 53.7 O142600600049 11. 37.1 O142600600050 12. 25.1 O142600600051 13. 16.9 O142600600052 14. 8. O142600600053 ENDDATA 17 0 O142600600054 ENDSUBENT 53 0 O142600699999 SUBENT O1426007 20140205 O052O142600700001 BIB 6 27 O142600700002 REACTION (47-AG-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600700003 see CORRECTION O142600700004 CORRECTION Not corrected for the neutron energy dependent O142600700005 efficiency. O142600700006 The following corrections have been applied to the O142600700007 measured distributions- O142600700008 -the portion of background from reaction outside the O142600700009 target 1-2%,or He4. O142600700010 -events rejected by the double reactions inspection O142600700011 2-4% are accounted for, continuously monitored duringO142600700012 the runs, O142600700013 -An off-line threshold was introduced into the O142600700014 measured BNB-light spectrum at 10 MeV to cut events O142600700015 from electrons observed at M(n) less than 3. The O142600700016 extrapolation to zero energy was estimated assuming O142600700017 similar spectra shapes as measured for M(n)=3-5, O142600700018 -A small portion of elastically scattered beam protonsO142600700019 may enter the BNB scintillator thus simulating real O142600700020 events. This background of about 1-3% contributes to O142600700021 the peak observed in the BNB-light spectrum which is O142600700022 well pronounced for M(n) less or equal 5 at energies O142600700023 of about 50 MeV. O142600700024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600700025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142600700026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600700027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600700028 SF8=RAW added in REACTION code O142600700029 ENDBIB 27 0 O142600700030 COMMON 1 3 O142600700031 ERR-DIG O142600700032 MB O142600700033 1.1 O142600700034 ENDCOMMON 3 0 O142600700035 DATA 2 17 O142600700036 PART-OUT DATA O142600700037 NO-DIM MB O142600700038 0. 47.2 O142600700039 1. 65. O142600700040 2. 73.5 O142600700041 3. 83.6 O142600700042 4. 96.7 O142600700043 5. 107.6 O142600700044 6. 118.4 O142600700045 7. 121.5 O142600700046 8. 113.8 O142600700047 9. 99.8 O142600700048 10. 79.7 O142600700049 11. 57.3 O142600700050 12. 40.2 O142600700051 13. 24.8 O142600700052 14. 13.2 O142600700053 15. 7.7 O142600700054 16. 3.9 O142600700055 ENDDATA 19 0 O142600700056 ENDSUBENT 55 0 O142600799999 SUBENT O1426008 20140205 O052O142600800001 BIB 6 27 O142600800002 REACTION (67-HO-165(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600800003 see CORRECTION O142600800004 CORRECTION Not corrected for the neutron energy dependent O142600800005 efficiency. O142600800006 The following corrections have been applied to the O142600800007 measured distributions- O142600800008 -the portion of background from reaction outside the O142600800009 target 1-2%,or He4. O142600800010 -events rejected by the double reactions inspection O142600800011 2-4% are accounted for, continuously monitored duringO142600800012 the runs, O142600800013 -An off-line threshold was introduced into the O142600800014 measured BNB-light spectrum at 10 MeV to cut events O142600800015 from electrons observed at M(n) less than 3. The O142600800016 extrapolation to zero energy was estimated assuming O142600800017 similar spectra shapes as measured for M(n)=3-5, O142600800018 -A small portion of elastically scattered beam protonsO142600800019 may enter the BNB scintillator thus simulating real O142600800020 events. This background of about 1-3% contributes to O142600800021 the peak observed in the BNB-light spectrum which is O142600800022 well pronounced for M(n) less or equal 5 at energies O142600800023 of about 50 MeV. O142600800024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600800025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142600800026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600800027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600800028 SF8=RAW added in REACTION code O142600800029 ENDBIB 27 0 O142600800030 COMMON 1 3 O142600800031 ERR-DIG O142600800032 MB O142600800033 1.1 O142600800034 ENDCOMMON 3 0 O142600800035 DATA 2 25 O142600800036 PART-OUT DATA O142600800037 NO-DIM MB O142600800038 0. 52.4 O142600800039 1. 57.8 O142600800040 2. 58.5 O142600800041 3. 58.4 O142600800042 4. 59.9 O142600800043 5. 59.8 O142600800044 6. 63.7 O142600800045 7. 63.5 O142600800046 8. 72.8 O142600800047 9. 76.6 O142600800048 10. 86.7 O142600800049 11. 95.2 O142600800050 12. 102.9 O142600800051 13. 109.9 O142600800052 14. 108.2 O142600800053 15. 101.1 O142600800054 16. 90.7 O142600800055 17. 74.2 O142600800056 18. 56.8 O142600800057 19. 41. O142600800058 20. 26.8 O142600800059 21. 16.5 O142600800060 22. 7.8 O142600800061 23. 3. O142600800062 24. 1.3 O142600800063 ENDDATA 27 0 O142600800064 ENDSUBENT 63 0 O142600899999 SUBENT O1426009 20140205 O052O142600900001 BIB 6 27 O142600900002 REACTION (74-W-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142600900003 see CORRECTION O142600900004 CORRECTION Not corrected for the neutron energy dependent O142600900005 efficiency. O142600900006 The following corrections have been applied to the O142600900007 measured distributions- O142600900008 -the portion of background from reaction outside the O142600900009 target 1-2%,or He4. O142600900010 -events rejected by the double reactions inspection O142600900011 2-4% are accounted for, continuously monitored duringO142600900012 the runs, O142600900013 -An off-line threshold was introduced into the O142600900014 measured BNB-light spectrum at 10 MeV to cut events O142600900015 from electrons observed at M(n) less than 3. The O142600900016 extrapolation to zero energy was estimated assuming O142600900017 similar spectra shapes as measured for M(n)=3-5, O142600900018 -A small portion of elastically scattered beam protonsO142600900019 may enter the BNB scintillator thus simulating real O142600900020 events. This background of about 1-3% contributes to O142600900021 the peak observed in the BNB-light spectrum which is O142600900022 well pronounced for M(n) less or equal 5 at energies O142600900023 of about 50 MeV. O142600900024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142600900025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142600900026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142600900027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142600900028 SF8=RAW added in REACTION code O142600900029 ENDBIB 27 0 O142600900030 COMMON 1 3 O142600900031 ERR-DIG O142600900032 MB O142600900033 1.1 O142600900034 ENDCOMMON 3 0 O142600900035 DATA 2 26 O142600900036 PART-OUT DATA O142600900037 NO-DIM MB O142600900038 0. 53.9 O142600900039 1. 58. O142600900040 2. 57.2 O142600900041 3. 55. O142600900042 4. 56.7 O142600900043 5. 58.3 O142600900044 6. 60. O142600900045 7. 62.5 O142600900046 8. 68.9 O142600900047 9. 74.6 O142600900048 10. 83.4 O142600900049 11. 93.8 O142600900050 12. 99.4 O142600900051 13. 102.7 O142600900052 14. 109.1 O142600900053 15. 112.4 O142600900054 15. 108.6 O142600900055 17. 95.3 O142600900056 18. 85.1 O142600900057 19. 71. O142600900058 20. 52.9 O142600900059 21. 39.6 O142600900060 22. 27.8 O142600900061 23. 18.4 O142600900062 24. 9.8 O142600900063 25. 6.8 O142600900064 ENDDATA 28 0 O142600900065 ENDSUBENT 64 0 O142600999999 SUBENT O1426010 20140205 O052O142601000001 BIB 6 27 O142601000002 REACTION (82-PB-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142601000003 see CORRECTION O142601000004 CORRECTION Not corrected for the neutron energy dependent O142601000005 efficiency. O142601000006 The following corrections have been applied to the O142601000007 measured distributions- O142601000008 -the portion of background from reaction outside the O142601000009 target 1-2%,or He4. O142601000010 -events rejected by the double reactions inspection O142601000011 2-4% are accounted for, continuously monitored duringO142601000012 the runs, O142601000013 -An off-line threshold was introduced into the O142601000014 measured BNB-light spectrum at 10 MeV to cut events O142601000015 from electrons observed at M(n) less than 3. The O142601000016 extrapolation to zero energy was estimated assuming O142601000017 similar spectra shapes as measured for M(n)=3-5, O142601000018 -A small portion of elastically scattered beam protonsO142601000019 may enter the BNB scintillator thus simulating real O142601000020 events. This background of about 1-3% contributes to O142601000021 the peak observed in the BNB-light spectrum which is O142601000022 well pronounced for M(n) less or equal 5 at energies O142601000023 of about 50 MeV. O142601000024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142601000025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142601000026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142601000027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142601000028 SF8=RAW added in REACTION code O142601000029 ENDBIB 27 0 O142601000030 COMMON 1 3 O142601000031 ERR-DIG O142601000032 MB O142601000033 1.1 O142601000034 ENDCOMMON 3 0 O142601000035 DATA 2 29 O142601000036 PART-OUT DATA O142601000037 NO-DIM MB O142601000038 0. 58.5 O142601000039 1. 63.1 O142601000040 2. 59.2 O142601000041 3. 56.9 O142601000042 4. 54.6 O142601000043 5. 57.7 O142601000044 6. 58.5 O142601000045 7. 60. O142601000046 8. 63.1 O142601000047 9. 70. O142601000048 10. 73.1 O142601000049 11. 82.3 O142601000050 12. 89.2 O142601000051 13. 95.4 O142601000052 14. 100.8 O142601000053 15. 103.1 O142601000054 16. 104.6 O142601000055 17. 103.1 O142601000056 18. 98.5 O142601000057 19. 91.5 O142601000058 20. 79.2 O142601000059 21. 66.2 O142601000060 22. 53.1 O142601000061 23. 39.2 O142601000062 24. 27.7 O142601000063 25. 16.9 O142601000064 26. 9.2 O142601000065 27. 6.2 O142601000066 28. 3.8 O142601000067 ENDDATA 31 0 O142601000068 ENDSUBENT 67 0 O142601099999 SUBENT O1426011 20140205 O052O142601100001 BIB 6 27 O142601100002 REACTION (92-U-0(P,X)0-NN-1,NUM,SIG,,RAW) fig 2 O142601100003 see CORRECTION O142601100004 CORRECTION Not corrected for the neutron energy dependent O142601100005 efficiency. O142601100006 The following corrections have been applied to the O142601100007 measured distributions- O142601100008 -the portion of background from reaction outside the O142601100009 target 1-2%,or He4. O142601100010 -events rejected by the double reactions inspection O142601100011 2-4% are accounted for, continuously monitored duringO142601100012 the runs, O142601100013 -An off-line threshold was introduced into the O142601100014 measured BNB-light spectrum at 10 MeV to cut events O142601100015 from electrons observed at M(n) less than 3. The O142601100016 extrapolation to zero energy was estimated assuming O142601100017 similar spectra shapes as measured for M(n)=3-5, O142601100018 -A small portion of elastically scattered beam protonsO142601100019 may enter the BNB scintillator thus simulating real O142601100020 events. This background of about 1-3% contributes to O142601100021 the peak observed in the BNB-light spectrum which is O142601100022 well pronounced for M(n) less or equal 5 at energies O142601100023 of about 50 MeV. O142601100024 SAMPLE A thin targets, thickness 0.1-1 g/cm**2 were used. O142601100025 STATUS (CURVE).By CAJAD.Digitized from fig.2 of NIM/A,562,729 O142601100026 ERR-ANALYS (ERR-DIG).Digitizing error of data. O142601100027 HISTORY (20140205A) SD: SF4=NPART -> 0-NN-1; SF7=N deleted and O142601100028 SF8=RAW added in REACTION code O142601100029 ENDBIB 27 0 O142601100030 COMMON 1 3 O142601100031 ERR-DIG O142601100032 MB O142601100033 1.1 O142601100034 ENDCOMMON 3 0 O142601100035 DATA 2 34 O142601100036 PART-OUT DATA O142601100037 NO-DIM MB O142601100038 0. 56.7 O142601100039 1. 53.6 O142601100040 2. 43.3 O142601100041 3. 38.5 O142601100042 4. 38.4 O142601100043 5. 36. O142601100044 6. 41.3 O142601100045 7. 42.7 O142601100046 8. 46.5 O142601100047 9. 51.1 O142601100048 10. 54.9 O142601100049 11. 61.8 O142601100050 12. 65.5 O142601100051 13. 70.9 O142601100052 14. 80.9 O142601100053 15. 84.7 O142601100054 16. 93.9 O142601100055 17. 100.8 O142601100056 18. 106.9 O142601100057 19. 106.8 O142601100058 20. 107.4 O142601100059 21. 105.8 O142601100060 22. 95.6 O142601100061 23. 84.6 O142601100062 24. 70.4 O142601100063 25. 56.3 O142601100064 26. 44.5 O142601100065 27. 32. O142601100066 28. 21.7 O142601100067 29. 13.8 O142601100068 30. 7.5 O142601100069 31. 4.3 O142601100070 32. 1. O142601100071 33. 0.04 O142601100072 ENDDATA 36 0 O142601100073 ENDSUBENT 72 0 O142601199999 SUBENT O1426012 20221223 O092O1426 12 1 BIB 7 11 O1426 12 2 REACTION (13-AL-27(P,X)0-NN-1,,PY) O1426 12 3 ASSUMED (ASSUM,13-AL-27(P,NON),,SIG) O1426 12 4 CORRECTION Corrections for detector efficiency and other O1426 12 5 corrections. O1426 12 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 12 7 from the literature to derive the neutron product yieldO1426 12 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 12 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 12 10 (DEP,O1426002) O1426 12 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 12 12 to ASSUM (see COMMENT). O1426 12 13 ENDBIB 11 0 O1426 12 14 NOCOMMON 0 0 O1426 12 15 DATA 4 1 O1426 12 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 12 17 PRD/REAC PRD/REAC MB MB O1426 12 18 2.95 0.20 456. 20. O1426 12 19 ENDDATA 3 0 O1426 12 20 ENDSUBENT 19 0 O1426 1299999 SUBENT O1426013 20221223 O092O1426 13 1 BIB 7 11 O1426 13 2 REACTION (26-FE-0(P,X)0-NN-1,,PY) O1426 13 3 ASSUMED (ASSUM,26-FE-0(P,NON),,SIG) O1426 13 4 CORRECTION Corrections for detector efficiency and other O1426 13 5 corrections. O1426 13 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 13 7 from the literature to derive the neutron product yieldO1426 13 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 13 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 13 10 (DEP,O1426003) O1426 13 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 13 12 to ASSUM (see COMMENT). O1426 13 13 ENDBIB 11 0 O1426 13 14 NOCOMMON 0 0 O1426 13 15 DATA 4 1 O1426 13 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 13 17 PRD/REAC PRD/REAC MB MB O1426 13 18 4.50 0.25 746. 30. O1426 13 19 ENDDATA 3 0 O1426 13 20 ENDSUBENT 19 0 O1426 1399999 SUBENT O1426014 20221223 O092O1426 14 1 BIB 7 11 O1426 14 2 REACTION (28-NI-0(P,X)0-NN-1,,PY) O1426 14 3 ASSUMED (ASSUM,28-NI-0(P,NON),,SIG) O1426 14 4 CORRECTION Corrections for detector efficiency and other O1426 14 5 corrections. O1426 14 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 14 7 from the literature to derive the neutron product yieldO1426 14 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 14 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 14 10 (DEP,O1426004) O1426 14 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 14 12 to ASSUM (see COMMENT). O1426 14 13 ENDBIB 11 0 O1426 14 14 NOCOMMON 0 0 O1426 14 15 DATA 4 1 O1426 14 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 14 17 PRD/REAC PRD/REAC MB MB O1426 14 18 4.13 0.25 764. 30. O1426 14 19 ENDDATA 3 0 O1426 14 20 ENDSUBENT 19 0 O1426 1499999 SUBENT O1426015 20221223 O092O1426 15 1 BIB 7 11 O1426 15 2 REACTION (29-CU-0(P,X)0-NN-1,,PY) O1426 15 3 ASSUMED (ASSUM,29-CU-0(P,NON),,SIG) O1426 15 4 CORRECTION Corrections for detector efficiency and other O1426 15 5 corrections. O1426 15 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 15 7 from the literature to derive the neutron product yieldO1426 15 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 15 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 15 10 (DEP,O1426005) O1426 15 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 15 12 to ASSUM (see COMMENT). O1426 15 13 ENDBIB 11 0 O1426 15 14 NOCOMMON 0 0 O1426 15 15 DATA 4 1 O1426 15 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 15 17 PRD/REAC PRD/REAC MB MB O1426 15 18 5.28 0.30 813. 30. O1426 15 19 ENDDATA 3 0 O1426 15 20 ENDSUBENT 19 0 O1426 1599999 SUBENT O1426016 20221223 O092O1426 16 1 BIB 7 11 O1426 16 2 REACTION (40-ZR-0(P,X)0-NN-1,,PY) O1426 16 3 ASSUMED (ASSUM,40-ZR-0(P,NON),,SIG) O1426 16 4 CORRECTION Corrections for detector efficiency and other O1426 16 5 corrections. O1426 16 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 16 7 from the literature to derive the neutron product yieldO1426 16 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 16 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 16 10 (DEP,O1426006) O1426 16 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 16 12 to ASSUM (see COMMENT). O1426 16 13 ENDBIB 11 0 O1426 16 14 NOCOMMON 0 0 O1426 16 15 DATA 4 1 O1426 16 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 16 17 PRD/REAC PRD/REAC MB MB O1426 16 18 7.34 0.35 1066. 40. O1426 16 19 ENDDATA 3 0 O1426 16 20 ENDSUBENT 19 0 O1426 1699999 SUBENT O1426017 20221223 O092O1426 17 1 BIB 7 10 O1426 17 2 REACTION (41-NB-93(P,X)0-NN-1,,PY) O1426 17 3 ASSUMED (ASSUM,41-NB-93(P,NON),,SIG) O1426 17 4 CORRECTION Corrections for detector efficiency and other O1426 17 5 corrections. O1426 17 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 17 7 from the literature to derive the neutron product yieldO1426 17 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 17 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 17 10 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 17 11 to ASSUM (see COMMENT). O1426 17 12 ENDBIB 10 0 O1426 17 13 NOCOMMON 0 0 O1426 17 14 DATA 4 1 O1426 17 15 DATA DATA-ERR ASSUM ASSUM-ERR O1426 17 16 PRD/REAC PRD/REAC MB MB O1426 17 17 7.24 0.35 1063. 40. O1426 17 18 ENDDATA 3 0 O1426 17 19 ENDSUBENT 18 0 O1426 1799999 SUBENT O1426018 20221223 O092O1426 18 1 BIB 7 11 O1426 18 2 REACTION (47-AG-0(P,X)0-NN-1,,PY) O1426 18 3 ASSUMED (ASSUM,47-AG-0(P,NON),,SIG) O1426 18 4 CORRECTION Corrections for detector efficiency and other O1426 18 5 corrections. O1426 18 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 18 7 from the literature to derive the neutron product yieldO1426 18 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 18 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 18 10 (DEP,O1426007) O1426 18 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 18 12 to ASSUM (see COMMENT). O1426 18 13 ENDBIB 11 0 O1426 18 14 NOCOMMON 0 0 O1426 18 15 DATA 4 1 O1426 18 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 18 17 PRD/REAC PRD/REAC MB MB O1426 18 18 8.46 0.35 1155. 40. O1426 18 19 ENDDATA 3 0 O1426 18 20 ENDSUBENT 19 0 O1426 1899999 SUBENT O1426019 20221223 O092O1426 19 1 BIB 7 11 O1426 19 2 REACTION (67-HO-165(P,X)0-NN-1,,PY) O1426 19 3 ASSUMED (ASSUM,67-HO-165(P,NON),,SIG) O1426 19 4 CORRECTION Corrections for detector efficiency and other O1426 19 5 corrections. O1426 19 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 19 7 from the literature to derive the neutron product yieldO1426 19 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 19 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 19 10 (DEP,O1426008) O1426 19 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 19 12 to ASSUM (see COMMENT). O1426 19 13 ENDBIB 11 0 O1426 19 14 NOCOMMON 0 0 O1426 19 15 DATA 4 1 O1426 19 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 19 17 PRD/REAC PRD/REAC MB MB O1426 19 18 13.35 0.55 1512. 50. O1426 19 19 ENDDATA 3 0 O1426 19 20 ENDSUBENT 19 0 O1426 1999999 SUBENT O1426020 20221223 O092O1426 20 1 BIB 7 11 O1426 20 2 REACTION (74-W-0(P,X)0-NN-1,,PY) O1426 20 3 ASSUMED (ASSUM,74-W-0(P,NON),,SIG) O1426 20 4 CORRECTION Corrections for detector efficiency and other O1426 20 5 corrections. O1426 20 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 20 7 from the literature to derive the neutron product yieldO1426 20 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 20 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 20 10 (DEP,O1426009) O1426 20 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 20 12 to ASSUM (see COMMENT). O1426 20 13 ENDBIB 11 0 O1426 20 14 NOCOMMON 0 0 O1426 20 15 DATA 4 1 O1426 20 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 20 17 PRD/REAC PRD/REAC MB MB O1426 20 18 14.62 0.60 1666. 55. O1426 20 19 ENDDATA 3 0 O1426 20 20 ENDSUBENT 19 0 O1426 2099999 SUBENT O1426021 20221223 O092O1426 21 1 BIB 7 11 O1426 21 2 REACTION (82-PB-0(P,X)0-NN-1,,PY) O1426 21 3 ASSUMED (ASSUM,82-PB-0(P,NON),,SIG) O1426 21 4 CORRECTION Corrections for detector efficiency and other O1426 21 5 corrections. O1426 21 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 21 7 from the literature to derive the neutron product yieldO1426 21 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 21 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 21 10 (DEP,O1426010) O1426 21 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 21 12 to ASSUM (see COMMENT). O1426 21 13 ENDBIB 11 0 O1426 21 14 NOCOMMON 0 0 O1426 21 15 DATA 4 1 O1426 21 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 21 17 PRD/REAC PRD/REAC MB MB O1426 21 18 16.03 0.65 1775. 60. O1426 21 19 ENDDATA 3 0 O1426 21 20 ENDSUBENT 19 0 O1426 2199999 SUBENT O1426022 20221223 O092O1426 22 1 BIB 7 11 O1426 22 2 REACTION (92-U-0(P,X)0-NN-1,,PY) O1426 22 3 ASSUMED (ASSUM,92-U-0(P,NON),,SIG) O1426 22 4 CORRECTION Corrections for detector efficiency and other O1426 22 5 corrections. O1426 22 6 COMMENT From A.Konobeev (2022-05-31): Cr.sect. data were taken O1426 22 7 from the literature to derive the neutron product yieldO1426 22 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O1426 22 9 STATUS (TABLE) Table 1 from Nucl.Instr.Meth.,A562(2006)729 O1426 22 10 (DEP,O1426011) O1426 22 11 HISTORY (20221223A) SD: Reaction (1) deleted. Data were move O1426 22 12 to ASSUM (see COMMENT). O1426 22 13 ENDBIB 11 0 O1426 22 14 NOCOMMON 0 0 O1426 22 15 DATA 4 1 O1426 22 16 DATA DATA-ERR ASSUM ASSUM-ERR O1426 22 17 PRD/REAC PRD/REAC MB MB O1426 22 18 20.84 0.80 2021. 65. O1426 22 19 ENDDATA 3 0 O1426 22 20 ENDSUBENT 19 0 O1426 2299999 ENDENTRY 22 0 O142699999999