ENTRY A0169 20210121 A096A016900000001 SUBENT A0169001 20210121 A096A016900100001 BIB 12 41 A016900100002 TITLE Production of chromium-48 for applications in life A016900100003 sciences A016900100004 AUTHOR (R.Weinreich,H.J.Probst,S.M.Qaim) A016900100005 REFERENCE (J,ARI,31,223,1980) A016900100006 INSTITUTE (2GERJUL) A016900100007 FACILITY (ISOCY,2GERJUL) A016900100008 (CYCLO,2GERJUL) Compact cyclotron 'CV28'. A016900100009 METHOD (STTA,ACTIV,EXTB,BCINT,GSPEC) A016900100010 ADD-RES (TTY-C) And chemical processing. A016900100011 DETECTOR (GELI) 80 cm 3 Ge(Li) detector in conjunction A016900100012 with a 4K analyzer A016900100013 REL-REF (R,,C.F.Williamson+,R,CEA-R-3042,1966) This is A016900100014 stopping power tables. A016900100015 (M,B0174001,H.J.Probst+,J,ARI,27,431,1976) Details on A016900100016 the estimation of individual errors have been describedA016900100017 COMMENT /By authors/ Beam currents were determined by two A016900100018 methods: A016900100019 1) using a Faraday cup and comparison of activities: A016900100020 in this method a thin foil of the material for which A016900100021 excitation function were to be measured was placed in A016900100022 front of the thick stack. Additionally another foil of A016900100023 the same material and thickness as that in front of A016900100024 the stack was irradiated independently (without stack) A016900100025 and the total charge was collected in a Faraday cup. A016900100026 The average beam current incident on the stack was A016900100027 then obtained from a comparison of the various A016900100028 activities produced in the independently irradiated A016900100029 foil with those in the front foil of the stack after A016900100030 applying the relevant corrections such as for foil A016900100031 thickness, irradiation times, etc. A016900100032 2) via a monitor reaction: for the determination of A016900100033 beam currents via monitor reactions, several aluminium A016900100034 foils were placed at different positions in each stack.A016900100035 From the 24Na activity produced in each monitor foil A016900100036 the beam current was calculated. A016900100037 STATUS (APRVD) By S.M.Qaim, 1984/03/16. A016900100038 HISTORY (19821128C) By Cajad. A016900100039 (19850305A) Corrections according to remarks from A016900100040 Prof. S.M.Qaim, 1984/03/16. A016900100041 (20090921A) BIB section was upgraded A016900100042 (20210121A) SD: Corrections in all Subents. A016900100043 ENDBIB 41 0 A016900100044 NOCOMMON 0 0 A016900100045 ENDSUBENT 44 0 A016900199999 SUBENT A0169002 20210121 A096A016900200001 BIB 9 27 A016900200002 REACTION (23-V-51(D,2N)24-CR-51,,SIG) A016900200003 DECAY-DATA (24-CR-51,27.72D,DG,320.,0.102) A016900200004 MONITOR (13-AL-27(D,X)11-NA-24,,SIG) A016900200005 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900200006 SAMPLE Two stacks were irradiated. The first one consisted of A016900200007 39 foils and the second one of 19 foils. A016900200008 The thickness of the vanadium foils varied between A016900200009 25 and 115 um. The purity of vanadium was better A016900200010 than 99.8%. A016900200011 COMMENT By authors. Since 51-V occurs in natural vanadium A016900200012 with an abundance of 99.75%, the 51-Cr should almost A016900200013 exclusively be formed in interactions of deuteron with A016900200014 51-V. A016900200015 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900200016 were obtained by summing up in quadrature all the A016900200017 individual errors such as: A016900200018 * statistical errors, A016900200019 * errors in the analysis of the gamma-ray peaks, A016900200020 * errors in beam current measurements, A016900200021 * uncertainty in the efficiency of the detector. A016900200022 This is typical cross section uncertainty A016900200023 in general, the error in the rising part of excitation A016900200024 curves amounted to 12% and at the peaks to 6-8%. A016900200025 STATUS (CURVE) Fig.1 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900200026 (DEP,A0169014) Monitor reaction A016900200027 HISTORY (20210121A) SD: SF3=2N+3P -> X in MONITOR code. A016900200028 BIB updated. A016900200029 ENDBIB 27 0 A016900200030 COMMON 1 3 A016900200031 EN-ERR-DIG A016900200032 MEV A016900200033 0.6 A016900200034 ENDCOMMON 3 0 A016900200035 DATA 3 54 A016900200036 EN DATA DATA-ERR A016900200037 MEV MB MB A016900200038 5.6 2.09E+01 A016900200039 8.2 1.83E+02 2.00E+01 A016900200040 10.6 4.49E+02 A016900200041 13.9 6.46E+02 A016900200042 17.2 6.78E+02 8.60E+01 A016900200043 19.0 6.28E+02 A016900200044 19.6 6.18E+02 A016900200045 20.3 5.36E+02 A016900200046 21.3 5.27E+02 A016900200047 22.1 4.90E+02 A016900200048 23.5 4.40E+02 5.90E+01 A016900200049 25.1 3.67E+02 A016900200050 26.1 3.06E+02 A016900200051 27.7 2.87E+02 A016900200052 29.9 2.28E+02 A016900200053 29.9 1.99E+02 A016900200054 31.8 1.81E+02 2.30E+01 A016900200055 33.0 1.56E+02 A016900200056 33.6 1.55E+02 A016900200057 35.3 1.40E+02 A016900200058 35.8 1.16E+02 A016900200059 37.9 1.23E+02 A016900200060 38.6 1.01E+02 A016900200061 39.2 1.12E+02 A016900200062 40.9 9.67E+01 1.20E+01 A016900200063 42.6 9.30E+01 A016900200064 42.9 9.30E+01 A016900200065 44.6 8.60E+01 A016900200066 45.5 8.00E+01 A016900200067 46.1 8.00E+01 A016900200068 47.8 7.50E+01 9.00E+00 A016900200069 47.9 6.66E+01 A016900200070 49.5 7.20E+01 A016900200071 50.6 6.80E+01 A016900200072 50.8 5.90E+01 A016900200073 52.3 6.50E+01 A016900200074 53.2 5.40E+01 A016900200075 54.4 5.60E+01 7.00E+00 A016900200076 57.2 5.20E+01 A016900200077 59.6 4.50E+01 A016900200078 62.1 4.60E+01 A016900200079 64.6 4.20E+01 5.00E+00 A016900200080 66.9 3.80E+01 A016900200081 69.0 3.50E+01 A016900200082 71.3 3.40E+01 A016900200083 73.2 3.23E+01 3.80E+00 A016900200084 75.2 3.00E+01 A016900200085 78.3 2.60E+01 A016900200086 81.4 2.64E+01 3.30E+00 A016900200087 83.3 2.35E+01 A016900200088 85.0 2.24E+01 A016900200089 87.0 2.09E+01 A016900200090 88.9 2.20E+01 A016900200091 90.5 2.01E+01 2.60E+00 A016900200092 ENDDATA 56 0 A016900200093 ENDSUBENT 92 0 A016900299999 SUBENT A0169003 20210121 A096A016900300001 BIB 9 28 A016900300002 REACTION (23-V-51(D,4N)24-CR-49,,SIG) A016900300003 DECAY-DATA (24-CR-49,41.9MIN,DG,90.6,0.59, A016900300004 DG,152.9,0.295) A016900300005 MONITOR (13-AL-27(D,X)11-NA-24,,SIG) A016900300006 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900300007 SAMPLE Two stacks were irradiated. The first one consisted of A016900300008 39 foils and the second one of 19 foils. A016900300009 The thickness of the vanadium foils varied between A016900300010 25 and 115 um. The purity of vanadium was better A016900300011 than 99.8%. A016900300012 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900300013 were obtained by summing up in quadrature all the A016900300014 individual errors such as: A016900300015 * statistical errors, A016900300016 * errors in the analysis of the gamma-ray peaks, A016900300017 * errors in beam current measurements, A016900300018 * uncertainty in the efficiency of the detector. A016900300019 This is typical cross section uncertainty A016900300020 in general, the error in the rising part of excitation A016900300021 curves amounted to 12% and at the peaks to 6-8%. A016900300022 COMMENT *By author*.Since 51-V occurs in natural A016900300023 vanadium with an abundance of 99.75%, A016900300024 the 49-Cr should almost exclusively be A016900300025 formed in interactions of deuterons with 51-V. A016900300026 STATUS (CURVE) Fig.1 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900300027 (DEP,A0169014) Monitor reaction A016900300028 HISTORY (20210121A) SD: SF3=2N+3P -> X in MONITOR code. A016900300029 BIB updated. A016900300030 ENDBIB 28 0 A016900300031 COMMON 2 3 A016900300032 MONIT-ERR EN-ERR-DIG A016900300033 PER-CENT MEV A016900300034 3. 0.6 A016900300035 ENDCOMMON 3 0 A016900300036 DATA 3 31 A016900300037 EN DATA DATA-ERR A016900300038 MEV MB MB A016900300039 31.6 4.38E-01 5.60E-02 A016900300040 33.6 1.34E+00 A016900300041 35.3 3.08E+00 A016900300042 37.4 5.87E+00 A016900300043 39.3 9.29E+00 A016900300044 41.1 1.25E+01 1.60E+00 A016900300045 42.9 1.59E+01 A016900300046 44.4 1.83E+01 A016900300047 45.9 1.98E+01 A016900300048 47.5 2.05E+01 2.60E+00 A016900300049 49.1 2.14E+01 A016900300050 50.4 2.08E+01 A016900300051 51.7 1.90E+01 A016900300052 54.6 1.83E+01 2.30E+00 A016900300053 57.0 1.66E+01 A016900300054 59.7 1.55E+01 A016900300055 61.8 1.40E+01 A016900300056 64.2 1.40E+01 1.80E+00 A016900300057 66.6 1.27E+01 A016900300058 68.8 1.21E+01 A016900300059 71.1 1.28E+01 A016900300060 73.0 1.20E+01 1.50E+00 A016900300061 75.4 1.20E+01 A016900300062 77.4 1.16E+01 A016900300063 79.4 1.05E+01 A016900300064 81.6 1.07E+01 1.30E+00 A016900300065 83.3 1.00E+01 A016900300066 85.3 1.04E+01 A016900300067 87.1 1.01E+01 A016900300068 88.8 8.94E+00 A016900300069 90.6 9.05E+00 1.10E+00 A016900300070 ENDDATA 33 0 A016900300071 ENDSUBENT 70 0 A016900399999 SUBENT A0169004 20210121 A096A016900400001 BIB 9 28 A016900400002 REACTION (23-V-51(D,5N)24-CR-48,,SIG) A016900400003 DECAY-DATA (24-CR-48,21.56HR,DG,112.3,0.96, A016900400004 DG,308.2,0.995) A016900400005 MONITOR (13-AL-27(D,X)11-NA-24,,SIG) A016900400006 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900400007 SAMPLE Two stacks were irradiated. The first one consisted of A016900400008 39 foils and the second one of 19 foils. A016900400009 The thickness of the vanadium foils varied between A016900400010 25 and 115 um. The purity of vanadium was better A016900400011 than 99.8%. A016900400012 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900400013 were obtained by summing up in quadrature all the A016900400014 individual errors such as: A016900400015 * statistical errors, A016900400016 * errors in the analysis of the gamma-ray peaks, A016900400017 * errors in beam current measurements, A016900400018 * uncertainty in the efficiency of the detector. A016900400019 This is typical cross section uncertainty A016900400020 in general, the error in the rising part of excitation A016900400021 curves amounted to 12% and at the peaks to 6-8%. A016900400022 COMMENT *By author*.Since 51-V occurs in natural A016900400023 vanadium with an abundance of 99.75 %, A016900400024 the 48-Cr should almost exclusively be formed in A016900400025 interactions of deuterons with 51-V. A016900400026 STATUS (CURVE) Fig.1 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900400027 (DEP,A0169014) Monitor reaction A016900400028 HISTORY (20210121A) SD: SF3=2N+3P -> X in MONITOR code. A016900400029 BIB updated. A016900400030 ENDBIB 28 0 A016900400031 COMMON 2 3 A016900400032 MONIT-ERR EN-ERR-DIG A016900400033 PER-CENT MEV A016900400034 3. 0.6 A016900400035 ENDCOMMON 3 0 A016900400036 DATA 3 21 A016900400037 EN DATA DATA-ERR A016900400038 MEV MB MB A016900400039 49.2 9.20E-02 1.50E-02 A016900400040 50.2 1.45E-01 A016900400041 51.8 1.75E-01 A016900400042 54.4 3.36E-01 3.10E-02 A016900400043 56.9 5.13E-01 A016900400044 59.7 6.14E-01 A016900400045 61.8 7.68E-01 A016900400046 64.5 8.80E-01 1.10E-01 A016900400047 67.6 1.02E+00 A016900400048 68.8 9.00E-01 A016900400049 71.0 9.40E-01 A016900400050 72.5 1.03E+00 1.30E-01 A016900400051 75.1 9.10E-01 A016900400052 77.4 8.80E-01 A016900400053 79.3 8.10E-01 A016900400054 81.4 8.00E-01 1.00E-01 A016900400055 83.4 7.80E-01 A016900400056 85.0 7.37E-01 A016900400057 86.9 6.91E-01 A016900400058 88.7 7.30E-01 A016900400059 90.5 7.20E-01 8.00E-02 A016900400060 ENDDATA 23 0 A016900400061 ENDSUBENT 60 0 A016900499999 SUBENT A0169005 20210121 A096A016900500001 BIB 8 25 A016900500002 REACTION (22-TI-0(A,X)24-CR-51,,SIG) A016900500003 DECAY-DATA (24-CR-51,27.72D,DG,320.,0.102) A016900500004 MONITOR (13-AL-27(A,X)11-NA-24,,SIG) A016900500005 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900500006 SAMPLE Titanium of natural isotopic composition, A016900500007 purity is better than 99.6%. A016900500008 The titanium foils used were 10, 35 and 125 um thick A016900500009 and arranged such that the energy interval between A016900500010 two successive points on the excitation curve A016900500011 varied between 1.8 And 5 MeV. The thickness of each A016900500012 foil was determined independently. A016900500013 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900500014 were obtained by summing up in quadrature all the A016900500015 individual errors such as: A016900500016 * statistical errors, A016900500017 * errors in the analysis of the gamma-ray peaks, A016900500018 * errors in beam current measurements, A016900500019 * uncertainty in the efficiency of the detector. A016900500020 This is typical cross section uncertainty A016900500021 in general, the error in the rising part of excitation A016900500022 curves amounted to 12% and at the peaks to 6-8%. A016900500023 STATUS (CURVE) Fig.2 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900500024 (DEP,A0169014) Monitor reaction A016900500025 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016900500026 SF3=3N+4P -> X in MONITOR code. BIB updated. A016900500027 ENDBIB 25 0 A016900500028 COMMON 1 3 A016900500029 EN-ERR-DIG A016900500030 MEV A016900500031 0.6 A016900500032 ENDCOMMON 3 0 A016900500033 DATA 3 48 A016900500034 EN DATA DATA-ERR A016900500035 MEV MB MB A016900500036 9.0 6.89E+00 3.10E+00 A016900500037 10.4 6.83E+01 A016900500038 11.7 2.28E+02 A016900500039 12.3 3.62E+02 A016900500040 14.0 4.94E+02 A016900500041 14.3 5.25E+02 A016900500042 15.0 5.85E+02 9.00E+01 A016900500043 17.0 5.69E+02 A016900500044 18.6 4.02E+02 A016900500045 20.9 2.44E+02 A016900500046 22.1 1.67E+02 2.50E+01 A016900500047 24.8 1.17E+02 A016900500048 26.3 1.03E+02 A016900500049 26.3 9.22E+01 A016900500050 27.4 7.86E+01 A016900500051 27.5 7.01E+01 A016900500052 34.1 5.50E+01 A016900500053 40.7 4.72E+01 7.30E+00 A016900500054 46.8 3.39E+01 A016900500055 51.8 2.26E+01 A016900500056 57.1 1.51E+01 A016900500057 61.1 9.37E+00 2.30E+00 A016900500058 65.3 8.26E+00 A016900500059 69.0 7.51E+00 1.60E+00 A016900500060 73.4 5.27E+00 A016900500061 76.6 4.31E+00 A016900500062 79.9 3.47E+00 A016900500063 83.8 2.41E+00 A016900500064 86.5 3.04E+00 A016900500065 89.5 2.88E+00 1.14E+00 A016900500066 92.4 2.85E+00 A016900500067 97.5 2.66E+00 A016900500068 102.0 1.94E+00 A016900500069 106.2 1.65E+00 A016900500070 110.0 1.92E+00 A016900500071 114.1 1.52E+00 A016900500072 118.1 1.03E+00 A016900500073 123.0 6.50E-01 4.20E-01 A016900500074 127.9 7.40E-01 A016900500075 133.7 1.08E+00 A016900500076 139.2 6.20E-01 A016900500077 144.3 1.02E+00 A016900500078 148.6 4.70E-01 A016900500079 153.8 4.00E-01 2.30E-01 A016900500080 158.5 5.10E-01 A016900500081 163.1 4.80E-01 A016900500082 167.2 6.30E-01 2.40E-01 A016900500083 171.5 2.40E-01 1.40E-01 A016900500084 ENDDATA 50 0 A016900500085 ENDSUBENT 84 0 A016900599999 SUBENT A0169006 20210121 A096A016900600001 BIB 8 26 A016900600002 REACTION (22-TI-0(A,X)24-CR-48,,SIG) A016900600003 DECAY-DATA (24-CR-48,21.56HR,DG,112.3,0.96, A016900600004 DG,308.2,0.995) A016900600005 MONITOR (13-AL-27(A,X)11-NA-24,,SIG) A016900600006 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900600007 SAMPLE Titanium of natural isotopic composition, A016900600008 purity is better than 99.6%. A016900600009 The titanium foils used were 10,35 and A016900600010 125 um thick and arranged such that the energy A016900600011 interval between two successive points on the A016900600012 excitation curve varied between 1.8 And 5 MeV A016900600013 The thickness of each foil was determined A016900600014 independently. A016900600015 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900600016 were obtained by summing up in quadrature all the A016900600017 individual errors such as: A016900600018 * statistical errors, A016900600019 * errors in the analysis of the gamma-ray peaks, A016900600020 * errors in beam current measurements, A016900600021 * uncertainty in the efficiency of the detector. A016900600022 This is typical cross section uncertainty A016900600023 in general, the error in the rising part of excitation A016900600024 curves amounted to 12% and at the peaks to 6-8%. A016900600025 STATUS (CURVE) Fig.2 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900600026 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016900600027 SF3=3N+4P -> X in MONITOR code. BIB updated. A016900600028 ENDBIB 26 0 A016900600029 COMMON 1 3 A016900600030 EN-ERR-DIG A016900600031 MEV A016900600032 0.6 A016900600033 ENDCOMMON 3 0 A016900600034 DATA 3 37 A016900600035 EN DATA DATA-ERR A016900600036 MEV MB MB A016900600037 19.0 2.30E-01 4.00E-02 A016900600038 21.2 8.80E-01 A016900600039 22.7 1.36E+00 A016900600040 24.8 1.77E+00 A016900600041 26.9 2.14E+00 A016900600042 31.9 2.19E+00 A016900600043 40.3 2.06E+00 A016900600044 46.7 1.72E+00 2.60E-01 A016900600045 52.0 1.82E+00 A016900600046 57.3 2.30E+00 A016900600047 61.0 2.77E+00 A016900600048 65.1 3.02E+00 4.10E-01 A016900600049 68.9 2.88E+00 A016900600050 73.1 2.47E+00 A016900600051 76.4 2.04E+00 A016900600052 80.0 1.76E+00 3.00E-01 A016900600053 84.0 1.58E+00 A016900600054 86.9 1.35E+00 A016900600055 90.0 1.21E+00 A016900600056 92.7 1.14E+00 1.80E-01 A016900600057 97.7 1.06E+00 A016900600058 101.9 9.60E-01 A016900600059 105.8 7.60E-01 A016900600060 110.1 7.40E-01 A016900600061 114.4 6.80E-01 A016900600062 118.1 6.00E-01 9.00E-02 A016900600063 122.8 4.80E-01 A016900600064 128.3 4.20E-01 A016900600065 133.3 4.00E-01 A016900600066 138.8 3.60E-01 A016900600067 143.8 3.00E-01 A016900600068 148.6 2.80E-01 A016900600069 153.5 2.30E-01 3.00E-02 A016900600070 158.3 2.20E-01 A016900600071 163.1 2.20E-01 A016900600072 167.7 2.00E-01 A016900600073 172.4 1.80E-01 4.00E-02 A016900600074 ENDDATA 39 0 A016900600075 ENDSUBENT 74 0 A016900699999 SUBENT A0169007 20210121 A096A016900700001 BIB 8 25 A016900700002 REACTION (22-TI-0(HE3,X)24-CR-48,,SIG) A016900700003 DECAY-DATA (24-CR-48,21.56HR,DG,112.3,0.96, A016900700004 DG,308.2,0.995) A016900700005 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016900700006 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900700007 SAMPLE Titanium of natural isotopic composition, A016900700008 purity is better than 99.6 %. The titanium foils A016900700009 used were 10, 35 and 125 um thick and arranged such A016900700010 that the energy interval between two successive A016900700011 points on the excitation curve varied between A016900700012 1.8 And 5 MeV. The thickness of each foil was A016900700013 determined independently. A016900700014 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900700015 were obtained by summing up in quadrature all the A016900700016 individual errors such as: A016900700017 * statistical errors, A016900700018 * errors in the analysis of the gamma-ray peaks, A016900700019 * errors in beam current measurements, A016900700020 * uncertainty in the efficiency of the detector. A016900700021 This is typical cross section uncertainty A016900700022 in general, the error in the rising part of excitation A016900700023 curves amounted to 12% and at the peaks to 6-8%. A016900700024 STATUS (CURVE) Fig.3 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900700025 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016900700026 SF3=2N+4P -> X in MONITOR code. BIB updated. A016900700027 ENDBIB 25 0 A016900700028 COMMON 1 3 A016900700029 EN-ERR-DIG A016900700030 MEV A016900700031 1.1 A016900700032 ENDCOMMON 3 0 A016900700033 DATA 3 55 A016900700034 EN DATA DATA-ERR A016900700035 MEV MB MB A016900700036 9.4 6.00E-02 1.90E-02 A016900700037 10.4 4.40E-01 A016900700038 11.7 1.20E+00 A016900700039 12.6 1.87E+00 A016900700040 13.7 2.26E+00 A016900700041 15.0 2.65E+00 A016900700042 17.0 2.90E+00 1.70E-01 A016900700043 18.6 2.97E+00 A016900700044 20.5 2.98E+00 A016900700045 21.8 3.28E+00 A016900700046 21.9 3.47E+00 A016900700047 22.9 3.78E+00 A016900700048 24.0 4.19E+00 A016900700049 24.9 4.69E+00 A016900700050 25.8 5.27E+00 A016900700051 26.7 5.42E+00 A016900700052 28.5 5.98E+00 A016900700053 28.5 6.82E+00 A016900700054 29.7 6.68E+00 A016900700055 29.9 7.58E+00 A016900700056 32.2 8.05E+00 A016900700057 32.9 7.27E+00 A016900700058 33.9 8.14E+00 A016900700059 35.1 7.36E+00 A016900700060 35.9 8.27E+00 A016900700061 36.8 6.99E+00 A016900700062 39.4 5.64E+00 A016900700063 42.6 4.65E+00 A016900700064 45.2 3.74E+00 A016900700065 48.3 2.99E+00 A016900700066 51.7 2.39E+00 A016900700067 55.3 1.94E+00 A016900700068 59.0 1.70E+00 A016900700069 61.0 1.62E+00 A016900700070 65.8 1.26E+00 A016900700071 70.2 1.08E+00 A016900700072 74.7 9.30E-01 A016900700073 76.9 8.50E-01 6.00E-02 A016900700074 79.9 7.30E-01 A016900700075 82.9 6.30E-01 A016900700076 86.2 6.00E-01 A016900700077 89.2 5.50E-01 A016900700078 92.4 5.10E-01 A016900700079 95.5 4.60E-01 A016900700080 98.1 4.10E-01 A016900700081 100.5 4.10E-01 A016900700082 103.6 3.60E-01 A016900700083 105.9 3.50E-01 A016900700084 108.5 3.00E-01 5.00E-02 A016900700085 111.5 2.90E-01 A016900700086 116.2 2.60E-01 A016900700087 121.0 2.30E-01 A016900700088 125.6 2.10E-01 A016900700089 130.4 1.90E-01 4.00E-02 A016900700090 134.7 1.80E-01 A016900700091 ENDDATA 57 0 A016900700092 ENDSUBENT 91 0 A016900799999 SUBENT A0169008 20210121 A096A016900800001 BIB 8 24 A016900800002 REACTION (22-TI-0(HE3,X)24-CR-51,,SIG) A016900800003 DECAY-DATA (24-CR-51,27.72D,DG,320.,0.102) A016900800004 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016900800005 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900800006 SAMPLE Titanium of natural isotopic composition, A016900800007 purity is better than 99.6%. The titanium foils used A016900800008 were 10, 35 and 125 um thick and arranged such A016900800009 that the energy interval between two successive A016900800010 points on the excitation curve varied between 1.8 A016900800011 and 5 MeV. The thickness of each foil was A016900800012 determined independently. A016900800013 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900800014 were obtained by summing up in quadrature all the A016900800015 individual errors such as: A016900800016 * statistical errors, A016900800017 * errors in the analysis of the gamma-ray peaks, A016900800018 * errors in beam current measurements, A016900800019 * uncertainty in the efficiency of the detector. A016900800020 This is typical cross section uncertainty A016900800021 in general, the error in the rising part of excitation A016900800022 curves amounted to 12% and at the peaks to 6-8%. A016900800023 STATUS (CURVE) Fig.3 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900800024 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016900800025 SF3=2N+4P -> X in MONITOR code. BIB updated. A016900800026 ENDBIB 24 0 A016900800027 COMMON 1 3 A016900800028 EN-ERR-DIG A016900800029 MEV A016900800030 1.1 A016900800031 ENDCOMMON 3 0 A016900800032 DATA 3 25 A016900800033 EN DATA DATA-ERR A016900800034 MEV MB MB A016900800035 9.7 2.90E-01 A016900800036 10.6 1.63E+00 5.90E-01 A016900800037 11.3 6.52E+00 A016900800038 12.4 1.13E+01 A016900800039 13.6 1.63E+01 A016900800040 14.7 2.12E+01 A016900800041 18.1 2.28E+01 2.35E+00 A016900800042 19.4 1.89E+01 A016900800043 23.1 1.34E+01 A016900800044 25.4 1.13E+01 1.52E+00 A016900800045 26.6 6.85E+00 A016900800046 27.9 4.07E+00 A016900800047 30.4 4.05E+00 A016900800048 33.5 2.89E+00 A016900800049 34.4 3.18E+00 7.50E-01 A016900800050 39.3 2.03E+00 A016900800051 45.3 1.39E+00 A016900800052 52.1 1.33E+00 3.80E-01 A016900800053 70.4 4.70E-01 A016900800054 79.9 4.50E-01 2.20E-01 A016900800055 89.1 4.30E-01 A016900800056 100.5 2.70E-01 A016900800057 111.1 3.60E-01 7.00E-02 A016900800058 126.0 2.20E-01 A016900800059 135.4 1.93E-01 7.40E-02 A016900800060 ENDDATA 27 0 A016900800061 ENDSUBENT 60 0 A016900899999 SUBENT A0169009 20210121 A096A016900900001 BIB 9 26 A016900900002 REACTION (22-TI-0(HE3,X)23-V-48,,SIG) A016900900003 DECAY-DATA (23-V-48,16.21D,DG,983.5,1., A016900900004 DG,1311.9,0.98) A016900900005 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016900900006 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016900900007 SAMPLE Titanium of natural isotopic composition. Purity is A016900900008 better than 99.6%. The titanium foils used were A016900900009 10, 35 and 125 um thick and arranged such that energy A016900900010 interval between two successive points on the A016900900011 excitation curve varied between 1.8 And 5. MeV. The A016900900012 thickness of each foil was determined independently. A016900900013 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016900900014 were obtained by summing up in quadrature all the A016900900015 individual errors such as: A016900900016 * statistical errors, A016900900017 * errors in the analysis of the gamma-ray peaks, A016900900018 * errors in beam current measurements, A016900900019 * uncertainty in the efficiency of the detector. A016900900020 This is typical cross section uncertainty A016900900021 in general, the error in the rising part of excitation A016900900022 curves amounted to 12% and at the peaks to 6-8%. A016900900023 FLAG (1.) CV-28 (low energy, relatively thin stack) A016900900024 (2.) Isochronous cyclotron (high energy, thick stack). A016900900025 STATUS (CURVE) Fig.4 from Int.J.Appl.Rad.Isot.,31(1980)223 A016900900026 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016900900027 SF3=2N+4P -> X in MONITOR code. BIB updated. A016900900028 ENDBIB 26 0 A016900900029 COMMON 1 3 A016900900030 EN-ERR-DIG A016900900031 MEV A016900900032 0.7 A016900900033 ENDCOMMON 3 0 A016900900034 DATA 4 46 A016900900035 EN DATA DATA-ERR FLAG A016900900036 MEV MB MB NO-DIM A016900900037 7.8 1.67E+00 1. A016900900038 8.9 1.21E+00 1. A016900900039 9.2 4.76E+00 1. A016900900040 10.0 1.55E+01 1. A016900900041 11.1 2.93E+01 1. A016900900042 11.9 3.86E+01 1. A016900900043 12.1 5.39E+01 1. A016900900044 15.6 5.96E+01 1. A016900900045 17.0 6.35E+01 1. A016900900046 18.7 7.68E+01 1. A016900900047 19.9 1.02E+02 1. A016900900048 21.6 1.48E+02 1. A016900900049 22.5 2.03E+02 1. A016900900050 24.7 2.96E+02 1. A016900900051 26.2 3.44E+02 1. A016900900052 28.6 3.90E+02 1. A016900900053 30.2 4.03E+02 1. A016900900054 32.4 4.01E+02 1. A016900900055 34.3 3.79E+02 1. A016900900056 37.9 2.89E+02 2. A016900900057 41.2 2.57E+02 2. A016900900058 43.6 2.20E+02 2. A016900900059 45.6 1.97E+02 2. A016900900060 50.2 1.72E+02 2. A016900900061 53.5 1.53E+02 1.60E+01 2. A016900900062 56.7 1.40E+02 2. A016900900063 58.9 1.31E+02 2. A016900900064 63.8 1.13E+02 2. A016900900065 69.0 1.03E+02 2. A016900900066 73.5 9.32E+01 2. A016900900067 75.5 8.88E+01 2. A016900900068 78.5 8.17E+01 2. A016900900069 81.7 7.77E+01 6.00E+00 2. A016900900070 85.0 7.35E+01 2. A016900900071 87.4 7.07E+01 2. A016900900072 93.5 6.18E+01 2. A016900900073 96.1 5.83E+01 2. A016900900074 99.1 5.26E+01 2. A016900900075 104.7 4.87E+01 2. A016900900076 107.3 4.80E+01 2. A016900900077 110.2 4.43E+01 2. A016900900078 115.3 4.12E+01 2. A016900900079 119.8 4.00E+01 2. A016900900080 124.8 3.52E+01 2. A016900900081 128.8 3.37E+01 2.00E+00 2. A016900900082 133.3 3.16E+01 2. A016900900083 ENDDATA 48 0 A016900900084 ENDSUBENT 83 0 A016900999999 SUBENT A0169010 20210121 A096A016901000001 BIB 8 24 A016901000002 REACTION (22-TI-0(HE3,X)21-SC-46,,SIG) A016901000003 DECAY-DATA (21-SC-46-G,83.85D,DG,889.3,1., A016901000004 DG,1120.5,1.) A016901000005 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016901000006 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016901000007 SAMPLE Titanium of natural isotopic composition. Purity is A016901000008 better than 99.6%. The titanium foils used were A016901000009 10, 35 and 125 um thick and arranged such that the A016901000010 energy interval between 1.8 And 5. MeV. The thickness A016901000011 of each foil was determined independently. A016901000012 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016901000013 were obtained by summing up in quadrature all the A016901000014 individual errors such as: A016901000015 * statistical errors, A016901000016 * errors in the analysis of the gamma-ray peaks, A016901000017 * errors in beam current measurements, A016901000018 * uncertainty in the efficiency of the detector. A016901000019 This is typical cross section uncertainty A016901000020 in general, the error in the rising part of excitation A016901000021 curves amounted to 12% and at the peaks to 6-8%. A016901000022 STATUS (CURVE) Fig.4 from Int.J.Appl.Rad.Isot.,31(1980)223 A016901000023 HISTORY (20210121A) SD: SF4=Sc-46g -> Dc-46; SF5=IND/M+ -> M+ A016901000024 in REACTION code. SF3=2N+4P -> X in MONITOR code. A016901000025 BIB updated. A016901000026 ENDBIB 24 0 A016901000027 COMMON 1 3 A016901000028 EN-ERR-DIG A016901000029 MEV A016901000030 0.7 A016901000031 ENDCOMMON 3 0 A016901000032 DATA 3 40 A016901000033 EN DATA DATA-ERR A016901000034 MEV MB MB A016901000035 3.8 1.31E+00 A016901000036 7.8 1.95E+00 A016901000037 10.4 3.16E+00 A016901000038 13.6 5.60E+00 1.10E+00 A016901000039 16.4 1.28E+01 A016901000040 17.0 1.90E+01 A016901000041 20.0 2.75E+01 A016901000042 23.7 3.30E+01 A016901000043 24.8 3.65E+01 A016901000044 26.6 3.55E+01 A016901000045 28.8 3.37E+01 A016901000046 32.0 3.21E+01 A016901000047 35.2 2.80E+01 A016901000048 38.8 2.71E+01 A016901000049 41.0 2.86E+01 A016901000050 44.2 2.81E+01 A016901000051 46.4 3.21E+01 A016901000052 50.8 3.37E+01 A016901000053 53.7 4.15E+01 4.10E+00 A016901000054 57.6 4.59E+01 A016901000055 60.0 5.24E+01 A016901000056 64.4 6.00E+01 A016901000057 69.1 6.09E+01 A016901000058 73.9 6.07E+01 A016901000059 75.5 6.33E+01 A016901000060 79.2 6.08E+01 A016901000061 82.6 6.26E+01 6.20E+00 A016901000062 85.1 6.31E+01 A016901000063 88.2 6.37E+01 A016901000064 96.5 6.41E+01 A016901000065 99.7 6.37E+01 A016901000066 101.9 6.43E+01 A016901000067 104.9 6.40E+01 A016901000068 107.1 6.24E+01 A016901000069 109.4 6.69E+01 A016901000070 116.8 6.65E+01 A016901000071 119.8 6.22E+01 A016901000072 124.6 6.12E+01 A016901000073 128.8 6.49E+01 A016901000074 133.8 6.24E+01 6.20E+00 A016901000075 ENDDATA 42 0 A016901000076 ENDSUBENT 75 0 A016901099999 SUBENT A0169011 20210121 A096A016901100001 BIB 8 23 A016901100002 REACTION (22-TI-0(HE3,X)21-SC-44-M,,SIG) A016901100003 DECAY-DATA (21-SC-44-M,2.44D,DG,271.4,0.86) A016901100004 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016901100005 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016901100006 SAMPLE Titanium of natural isotopic composition, A016901100007 purity is better than 99.6%. The titanium foils used A016901100008 were 10, 35 and 125 um thick and arranged such that theA016901100009 energy interval between two successive points on the A016901100010 excitation curve varied between 1.8 and 50 MeV. The A016901100011 thickness of each foil was determined independently. A016901100012 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016901100013 were obtained by summing up in quadrature all the A016901100014 individual errors such as: A016901100015 * statistical errors, A016901100016 * errors in the analysis of the gamma-ray peaks, A016901100017 * errors in beam current measurements, A016901100018 * uncertainty in the efficiency of the detector. A016901100019 This is typical cross section uncertainty A016901100020 in general, the error in the rising part of excitation A016901100021 curves amounted to 12% and at the peaks to 6-8%. A016901100022 STATUS (CURVE) Fig.4 from Int.J.Appl.Rad.Isot.,31(1980)223 A016901100023 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016901100024 SF3=2N+4P -> X in MONITOR code. BIB updated. A016901100025 ENDBIB 23 0 A016901100026 COMMON 1 3 A016901100027 EN-ERR-DIG A016901100028 MEV A016901100029 0.7 A016901100030 ENDCOMMON 3 0 A016901100031 DATA 3 37 A016901100032 EN DATA DATA-ERR A016901100033 MEV MB MB A016901100034 4.9 2.10E-01 A016901100035 9.0 2.70E-01 A016901100036 11.7 5.60E-01 A016901100037 14.6 9.30E-01 9.00E-02 A016901100038 19.3 2.80E+00 A016901100039 21.5 3.74E+00 A016901100040 23.7 4.74E+00 A016901100041 25.5 5.67E+00 A016901100042 27.2 6.68E+00 A016901100043 32.4 8.76E+00 A016901100044 35.3 1.09E+01 A016901100045 38.8 1.72E+01 A016901100046 41.2 2.84E+01 A016901100047 44.1 3.78E+01 A016901100048 46.7 4.71E+01 A016901100049 50.1 5.66E+01 A016901100050 54.0 5.96E+01 5.50E+00 A016901100051 55.5 5.45E+01 A016901100052 60.1 5.62E+01 A016901100053 65.0 5.28E+01 A016901100054 69.1 4.85E+01 A016901100055 73.6 4.65E+01 A016901100056 75.1 4.71E+01 A016901100057 82.0 4.46E+01 A016901100058 84.9 4.77E+01 A016901100059 87.5 4.91E+01 A016901100060 91.0 4.66E+01 A016901100061 93.7 4.76E+01 A016901100062 96.6 4.87E+01 A016901100063 99.6 4.77E+01 A016901100064 102.0 4.91E+01 A016901100065 109.9 4.84E+01 A016901100066 114.7 4.84E+01 A016901100067 119.3 4.64E+01 A016901100068 123.8 4.64E+01 A016901100069 128.8 4.47E+01 A016901100070 133.4 4.47E+01 A016901100071 ENDDATA 39 0 A016901100072 ENDSUBENT 71 0 A016901199999 SUBENT A0169012 20210121 A096A016901200001 BIB 10 36 A016901200002 REACTION (22-TI-0(HE3,X)21-SC-47,(CUM),SIG) A016901200003 COMMENT Compiler could not exclude the production A016901200004 of 47-Sc via 47-Ca and 47-K. A016901200005 *By author*. The data have been measured using A016901200006 both the high-energy machine (thick stack) A016901200007 and the low-energy machine (relatively thin stack). A016901200008 The discrepancies have been observed for energy A016901200009 overlap region in the case of different stacks. A016901200010 For thick stack secondary neutrons contribute A016901200011 to the formation of scandium via (n,p) and (n,n'p) A016901200012 reactions. A016901200013 DECAY-DATA (21-SC-47,3.39D,DG,159.4,0.69) A016901200014 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016901200015 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016901200016 SAMPLE Titanium of natural isotopic composition, A016901200017 purity is better than 99.6%. The titanium foils were A016901200018 used were 10, 35 and 125 um thick and arranged such A016901200019 that the energy interval between two successive A016901200020 points on the excitation curve varied between 1.8 A016901200021 and 5 MeV. The thickness of each foil was A016901200022 determined independently. A016901200023 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016901200024 were obtained by summing up in quadrature all the A016901200025 individual errors such as: A016901200026 * statistical errors, A016901200027 * errors in the analysis of the gamma-ray peaks, A016901200028 * errors in beam current measurements, A016901200029 * uncertainty in the efficiency of the detector. A016901200030 This is typical cross section uncertainty A016901200031 in general, the error in the rising part of excitation A016901200032 curves amounted to 12% and at the peaks to 6-8%. A016901200033 FLAG (1.) CV-28 (low energy, relatively thin stack) A016901200034 (2.) Isochronous cyclotron (high-energy, thick stack). A016901200035 STATUS (CURVE) Fig.4 from Int.J.Appl.Rad.Isot.,31(1980)223 A016901200036 HISTORY (20210121A) SD: SF3=2N+4P -> X in MONITOR code. A016901200037 BIB updated. A016901200038 ENDBIB 36 0 A016901200039 COMMON 1 3 A016901200040 EN-ERR-DIG A016901200041 MEV A016901200042 0.7 A016901200043 ENDCOMMON 3 0 A016901200044 DATA 4 54 A016901200045 EN DATA DATA-ERR FLAG A016901200046 MEV MB MB NO-DIM A016901200047 4.0 1.28E+00 2. A016901200048 8.8 1.38E+00 2. A016901200049 11.4 1.43E+00 2. A016901200050 14.2 1.58E+00 1.20E-01 2. A016901200051 16.2 3.20E-01 1. A016901200052 17.1 1.81E+00 2. A016901200053 17.9 3.10E-01 1. A016901200054 19.2 2.06E+00 2. A016901200055 19.2 4.80E-01 1. A016901200056 21.0 8.70E-01 1. A016901200057 21.6 2.30E+00 2. A016901200058 21.8 1.14E+00 1. A016901200059 23.6 1.01E+00 1. A016901200060 23.7 2.68E+00 2. A016901200061 25.3 3.08E+00 2. A016901200062 25.4 1.40E+00 1. A016901200063 27.4 1.85E+00 1. A016901200064 27.4 3.40E+00 2. A016901200065 29.3 3.97E+00 2. A016901200066 29.4 2.35E+00 1. A016901200067 31.2 2.67E+00 1. A016901200068 31.8 5.10E+00 3.90E-01 2. A016901200069 33.4 3.62E+00 1. A016901200070 34.8 4.17E+00 1. A016901200071 35.3 6.74E+00 2. A016901200072 38.8 8.64E+00 2. A016901200073 41.4 1.08E+01 2. A016901200074 44.3 1.30E+01 2. A016901200075 46.7 1.52E+01 2. A016901200076 51.7 1.84E+01 2. A016901200077 53.7 1.97E+01 1.60E+00 2. A016901200078 57.4 2.05E+01 2. A016901200079 59.9 2.13E+01 2. A016901200080 64.6 2.20E+01 2. A016901200081 69.3 2.32E+01 2. A016901200082 73.6 2.37E+01 2. A016901200083 75.6 2.36E+01 2. A016901200084 78.9 2.43E+01 2. A016901200085 81.8 2.49E+01 1.80E+00 2. A016901200086 85.3 2.48E+01 2. A016901200087 87.9 2.53E+01 2. A016901200088 90.7 2.55E+01 2. A016901200089 94.2 2.60E+01 2. A016901200090 96.9 2.63E+01 2. A016901200091 99.5 2.67E+01 2. A016901200092 102.8 2.67E+01 2. A016901200093 104.7 2.68E+01 2. A016901200094 107.4 2.78E+01 2. A016901200095 110.1 2.78E+01 2. A016901200096 113.3 2.68E+01 2. A016901200097 120.3 2.86E+01 2. A016901200098 124.6 2.82E+01 2.30E+00 2. A016901200099 129.6 2.90E+01 2. A016901200100 133.8 2.96E+01 2. A016901200101 ENDDATA 56 0 A016901200102 ENDSUBENT 101 0 A016901299999 SUBENT A0169013 20210121 A096A016901300001 BIB 10 34 A016901300002 REACTION (22-TI-0(HE3,X)21-SC-48,,SIG) A016901300003 DECAY-DATA (21-SC-48,43.8HR,DG,1037.4,0.975) A016901300004 MONITOR (13-AL-27(HE3,X)11-NA-24,,SIG) A016901300005 DECAY-MON (11-NA-24,15.HR,DG,1368.6,1.) A016901300006 SAMPLE Titanium of natural isotopic composition, A016901300007 purity is better than 99.6%. The titanium foils used A016901300008 were 10,35 and 125 um thick and arranged such that the A016901300009 energy interval between two successive points on the A016901300010 excitation curve varied between 1.8 and 5 MeV. A016901300011 The thickness of each foil was determined A016901300012 independently. A016901300013 ERR-ANALYS (DATA-ERR) The total errors in the cross section data A016901300014 were obtained by summing up in quadrature all the A016901300015 individual errors such as: A016901300016 * statistical errors, A016901300017 * errors in the analysis of the gamma-ray peaks, A016901300018 * errors in beam current measurements, A016901300019 * uncertainty in the efficiency of the detector. A016901300020 This is typical cross section uncertainty A016901300021 in general, the error in the rising part of excitation A016901300022 curves amounted to 12% and at the peaks to 6-8%. A016901300023 COMMENT *By author*. The data have been measured using A016901300024 both the high-energy machine(thick stack) A016901300025 and the low-energy machine(relatively thin stack). A016901300026 The discrepancies have been observed for energy A016901300027 overlap region in the case of different stacks. A016901300028 For thick stack secondary neutrons contribute to A016901300029 the formation of scandium via (n,p) and (n,n'p) A016901300030 reactions. A016901300031 FLAG (1.) CV-28 (low energy, relatively thin stack) A016901300032 (2.) Isochronous cyclotron (high-energy, thick stack). A016901300033 STATUS (CURVE) Fig.4 from Int.J.Appl.Rad.Isot.,31(1980)223 A016901300034 HISTORY (20210121A) SD: SF5=IND deleted from REACTION code. A016901300035 SF3=2N+4P -> X in MONITOR code. BIB updated. A016901300036 ENDBIB 34 0 A016901300037 COMMON 1 3 A016901300038 EN-ERR-DIG A016901300039 MEV A016901300040 1.0 A016901300041 ENDCOMMON 3 0 A016901300042 DATA 4 52 A016901300043 EN DATA DATA-ERR FLAG A016901300044 MEV MB MB NO-DIM A016901300045 4.6 3.60E-01 2. A016901300046 9.1 4.40E-01 5.00E-02 2. A016901300047 12.1 4.30E-01 2. A016901300048 14.6 5.00E-01 2. A016901300049 16.6 5.30E-01 2. A016901300050 18.2 1.20E-01 1. A016901300051 19.0 5.70E-01 2. A016901300052 19.6 1.90E-01 1. A016901300053 20.9 2.00E-01 1. A016901300054 21.5 6.70E-01 2. A016901300055 22.6 5.00E-01 1. A016901300056 23.8 9.00E-01 2. A016901300057 25.8 1.07E+00 2. A016901300058 26.0 6.60E-01 1. A016901300059 27.7 9.10E-01 1. A016901300060 27.8 1.23E+00 2. A016901300061 29.4 1.40E+00 2. A016901300062 29.7 8.00E-01 1. A016901300063 30.9 1.12E+00 1. A016901300064 33.0 1.42E+00 1. A016901300065 33.8 1.80E+00 1.80E-01 2. A016901300066 34.7 1.58E+00 1. A016901300067 36.0 2.22E+00 2. A016901300068 38.6 2.59E+00 2. A016901300069 41.8 2.69E+00 2. A016901300070 44.4 2.83E+00 2. A016901300071 46.9 2.97E+00 2. A016901300072 50.6 3.05E+00 2. A016901300073 53.9 3.13E+00 3.00E-01 2. A016901300074 57.8 2.87E+00 2. A016901300075 60.3 3.23E+00 2. A016901300076 64.5 3.37E+00 2. A016901300077 69.6 3.49E+00 2. A016901300078 73.3 3.58E+00 2. A016901300079 75.8 3.76E+00 2. A016901300080 79.4 3.65E+00 2. A016901300081 82.1 3.77E+00 3.60E-01 2. A016901300082 85.3 3.73E+00 2. A016901300083 88.8 3.83E+00 2. A016901300084 91.3 3.74E+00 2. A016901300085 94.0 3.90E+00 2. A016901300086 97.2 3.76E+00 2. A016901300087 99.4 4.17E+00 2. A016901300088 102.2 4.04E+00 2. A016901300089 105.0 3.97E+00 2. A016901300090 107.6 3.89E+00 2. A016901300091 110.0 3.96E+00 2. A016901300092 115.0 3.92E+00 2. A016901300093 120.3 4.15E+00 2. A016901300094 124.8 4.07E+00 2. A016901300095 129.3 4.13E+00 3.90E-01 2. A016901300096 133.8 4.12E+00 2. A016901300097 ENDDATA 54 0 A016901300098 ENDSUBENT 97 0 A016901399999 SUBENT A0169014 20210121 A096A016901400001 BIB 7 18 A016901400002 REACTION (13-AL-27(D,X)11-NA-24,,SIG) A016901400003 DECAY-DATA (11-NA-24,15.HR,DG,1368.6,1.) A016901400004 SAMPLE A stack consisting of 54 aluminium foils (purity is A016901400005 better than 99.99%) of thicknesses varying between A016901400006 100 and 500 um was irradiated with deuterons. A016901400007 REL-REF (A,P0124001,P.A.Lenk+,J,PR,116,1229,1959) A016901400008 (A,B0142004,U.Martens+,J,ZP,233,170,1970) A016901400009 ERR-ANALYS (DATA-ERR,,3.) The total errors in the cross section A016901400010 data were obtained by summing up in quadrature all the A016901400011 individual errors such as: A016901400012 * statistical errors, A016901400013 * errors in the analysis of the gamma-ray peaks, A016901400014 * errors in beam current measurements, A016901400015 * uncertainty in the efficiency of the detector. A016901400016 STATUS (TABLE) Tbl. from APPENDIX of A016901400017 Int.J.Appl.Rad.Isot.,31(1980)223 A016901400018 HISTORY (20210121A) SD: SF3=2N+3P -> X in REACTION code. A016901400019 COMMENT -> SAMPLE. STATUS added. A016901400020 ENDBIB 18 0 A016901400021 NOCOMMON 0 0 A016901400022 DATA 2 30 A016901400023 EN DATA A016901400024 MEV MB A016901400025 40.3 2.84E+01 A016901400026 42.6 2.65E+01 A016901400027 44.8 2.51E+01 A016901400028 47.0 2.32E+01 A016901400029 49.0 2.27E+01 A016901400030 51.0 2.28E+01 A016901400031 53.0 2.18E+01 A016901400032 55.0 2.16E+01 A016901400033 56.9 2.17E+01 A016901400034 58.9 2.13E+01 A016901400035 60.8 2.18E+01 A016901400036 62.6 2.18E+01 A016901400037 64.4 2.18E+01 A016901400038 66.1 2.17E+01 A016901400039 67.8 2.17E+01 A016901400040 69.5 2.17E+01 A016901400041 71.1 2.19E+01 A016901400042 72.8 2.18E+01 A016901400043 74.4 2.21E+01 A016901400044 76.0 2.17E+01 A016901400045 77.6 2.19E+01 A016901400046 79.2 2.18E+01 A016901400047 80.8 2.13E+01 A016901400048 82.3 2.17E+01 A016901400049 83.2 2.17E+01 A016901400050 83.9 2.14E+01 A016901400051 84.8 2.17E+01 A016901400052 85.1 2.13E+01 A016901400053 87.0 2.14E+01 A016901400054 88.5 2.17E+01 A016901400055 ENDDATA 32 0 A016901400056 ENDSUBENT 55 0 A016901499999 ENDENTRY 14 0 A016999999999