ENTRY A0497 20240926 A119A0497000 1 SUBENT A0497001 20240926 A119A0497001 1 BIB 13 50 A0497001 2 TITLE Production of Fe-52 via proton-induced reactions A0497001 3 on manganese and nickel A0497001 4 AUTHOR (G.F.Steyn,S.J.Mills,F.M.Nortier,B.R.S.Simpson, A0497001 5 B.R.Meyer) A0497001 6 INSTITUTE (3SAFNAC) A0497001 7 REFERENCE (J,ARI,41,315,1990) A0497001 8 DETECTOR (GE-IN) A0497001 9 FACILITY (ISOCY,3SAFNAC) Separated-sector Cyclotron Facility A0497001 10 ANALYSIS Cross-sections and radionuclide yields were calculated A0497001 11 from the measured emission rates of the characteristic A0497001 12 gamma-rays of the relevant activation products, making A0497001 13 use of the decay data tables of Reus et al. (1983). A0497001 14 METHOD (STTA,EXTB,ACTIV) A0497001 15 For irradiation, the foil stacks were mounted either A0497001 16 in one of the standard Faraday cups used for beam A0497001 17 diagnostic purposes in the NAC external beam lines, A0497001 18 or in a simple, more easily accessible stack holder A0497001 19 at the end of one of the beam lines. A0497001 20 CORRECTION All yields were corrected for decay losses during and A0497001 21 after bombardment, and are therefore reported as A0497001 22 (instantaneous) 'production rates', rather A0497001 23 than 'yields'. A0497001 24 Corrections for the decrease in beam current due to A0497001 25 nonelastic nuclear interactions as the beam traversed A0497001 26 the stacks were taken from the tabulation of A0497001 27 Janni (1982) while the energy degradation in the stacksA0497001 28 was computed by means of the stopping power expressionsA0497001 29 of Anderson and Ziegler (1977). A0497001 30 REL-REF (R,,J.F.Janni,J,AND,27,147,1982) see CORRECTION A0497001 31 (R,,H.H.Anderson+,B,ANDERSEN,3,1,1977) see CORRECTION A0497001 32 (R,,U.Reus+,J,AND,29,193,1983) see METHOD A0497001 33 ERR-ANALYS (ERR-T) Total uncertainty includes partial A0497001 34 uncertainties described in Subents 002-009. A0497001 35 COMMENT /By authors/ The total uncertainties in the cross- A0497001 36 sections and production rates were obtained by A0497001 37 summing all the contributing uncertainties in A0497001 38 quadrature and were expressed with a 1 standard A0497001 39 deviation (1 sigma) criterion. A0497001 40 HISTORY (19910912C) A0497001 41 (20140829A) SD: Updated to new date format, lower case.A0497001 42 Corrections according to last EXFOR rules and Dict. A0497001 43 BIB was updated in all Subents. A0497001 44 (20170203A) SD: Correction in Subent 002. Page of the A0497001 45 ref.J,AND,29,194... in REL-REF corrected (p.193). A0497001 46 (20180527A) SD: REACTION code was updated according to A0497001 47 MEMO CP-D/933rev. in Subents 003-004. A0497001 48 (20190626A) SD: Corrections in Subents 006,007. A0497001 49 (20210628A) SD: Corrections in Subents 005,006. A0497001 50 (20231227A) SD: Corrections in all Subents. A0497001 51 (20240926A) SD: Correction in Subent 008. A0497001 52 ENDBIB 50 0 A0497001 53 COMMON 1 3 A0497001 54 EN-ERR A0497001 55 MEV A0497001 56 1. A0497001 57 ENDCOMMON 3 0 A0497001 58 ENDSUBENT 57 0 A049700199999 SUBENT A0497002 20231227 A105A0497 2 1 BIB 8 29 A0497 2 2 REACTION (13-AL-27(P,X)11-NA-22,,SIG) A0497 2 3 REL-REF (A,,J.Tobailem+,R,CEA-N-1466(3),1975) A0497 2 4 (A,D0505023,A.Grutter+,J,NP/A,383,98,1982) A0497 2 5 (A,O0501003,H.R.Heydegger+,J,PR/C,14,1506,1976) A0497 2 6 SAMPLE Each of the target foils was followed by a 250 mu-m A0497 2 7 high-purity Al catcher foil (99.999%). A0497 2 8 These foils also served as monitor foils for the A0497 2 9 accurate measurement of the incident proton flux. A0497 2 10 Additional beam degradation within the stacks, if A0497 2 11 required, was accomplished by means of suitable Al A0497 2 12 foils and/or Cu foils or discs. All the foils and discsA0497 2 13 had a diameter of 19 mm and their individual A0497 2 14 thicknesses were determined by weighing. A0497 2 15 METHOD (BCINT) The monitor reaction cross-sections were based A0497 2 16 on accurate Faraday-cup measurements. A0497 2 17 ERR-ANALYS (ERR-S,,4.2) The error due to counting statistics and A0497 2 18 photopeak integration as well as uncertainties in A0497 2 19 beam-loss corrections A0497 2 20 (ERR-1) The uncertainty in beam-loss corrections. A0497 2 21 (ERR-2) The uncertainty in detector efficiency. A0497 2 22 (ERR-3) The uncertainty in country geometry. A0497 2 23 (ERR-4) The uncertainty in decay corrections. A0497 2 24 (ERR-5) The uncertainty in the foil thickness. A0497 2 25 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.2 A0497 2 26 COMMENT /By authors/ The measured excitation function for A0497 2 27 the production of Na-22 in the bombardment of natural A0497 2 28 Al with protons used as monitor reaction in this work. A0497 2 29 HISTORY (20170203A) SD: METHOD was added. A0497 2 30 (20231227U) SD: STATUS updated. A0497 2 31 ENDBIB 29 0 A0497 2 32 COMMON 5 3 A0497 2 33 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 A0497 2 34 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A0497 2 35 3. 5. 1. 1. 1. A0497 2 36 ENDCOMMON 3 0 A0497 2 37 DATA 3 57 A0497 2 38 EN DATA ERR-T A0497 2 39 MEV MB MB A0497 2 40 199.6 14.96 0.92 A0497 2 41 193.3 15.22 0.93 A0497 2 42 187.5 15.75 0.97 A0497 2 43 181.0 16.05 1.00 A0497 2 44 174.3 16.34 1.03 A0497 2 45 169.1 16.67 1.07 A0497 2 46 163.2 16.90 1.09 A0497 2 47 157.2 16.85 1.10 A0497 2 48 151.8 17.03 1.13 A0497 2 49 146.0 17.30 1.16 A0497 2 50 141.3 17.19 1.17 A0497 2 51 136.4 17.72 1.23 A0497 2 52 131.4 17.71 1.25 A0497 2 53 126.3 17.97 1.28 A0497 2 54 121.5 18.15 1.32 A0497 2 55 119.4 18.08 1.13 A0497 2 56 113.7 18.77 1.17 A0497 2 57 107.0 19.07 1.19 A0497 2 58 101.4 19.66 1.23 A0497 2 59 95.6 19.81 1.25 A0497 2 60 93.2 19.79 1.20 A0497 2 61 91.0 19.87 1.21 A0497 2 62 88.8 20.00 1.22 A0497 2 63 86.6 19.87 1.21 A0497 2 64 84.4 20.71 1.26 A0497 2 65 82.1 20.00 1.22 A0497 2 66 79.7 20.19 1.24 A0497 2 67 77.3 20.30 1.25 A0497 2 68 74.8 20.33 1.25 A0497 2 69 72.3 21.69 1.34 A0497 2 70 69.7 21.92 1.36 A0497 2 71 67.0 22.69 1.41 A0497 2 72 65.7 23.04 1.39 A0497 2 73 64.1 23.80 1.44 A0497 2 74 62.4 24.91 1.51 A0497 2 75 60.7 25.93 1.57 A0497 2 76 59.0 26.95 1.63 A0497 2 77 57.2 28.25 1.71 A0497 2 78 55.4 30.55 1.85 A0497 2 79 53.5 33.05 2.00 A0497 2 80 51.5 35.13 2.13 A0497 2 81 49.6 38.34 2.32 A0497 2 82 47.5 40.74 2.47 A0497 2 83 45.4 43.05 2.61 A0497 2 84 43.2 43.46 2.64 A0497 2 85 40.9 41.37 2.52 A0497 2 86 39.2 36.57 2.21 A0497 2 87 38.0 32.70 1.98 A0497 2 88 36.7 27.72 1.68 A0497 2 89 35.4 21.96 1.34 A0497 2 90 34.1 15.96 0.98 A0497 2 91 32.8 9.874 0.612 A0497 2 92 31.4 5.262 0.336 A0497 2 93 29.9 2.094 0.145 A0497 2 94 28.4 0.671 0.060 A0497 2 95 26.8 0.181 0.028 A0497 2 96 25.2 0.035 0.015 A0497 2 97 ENDDATA 59 0 A0497 2 98 ENDSUBENT 97 0 A0497 299999 SUBENT A0497003 20231227 A105A0497 3 1 BIB 7 21 A0497 3 2 REACTION 1(25-MN-55(P,4N)26-FE-52-G,,SIG) A0497 3 3 2(25-MN-55(P,4N)26-FE-52-G,,TTY/DEN,,PHY) A0497 3 4 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497 3 5 METHOD The incident beam currents were determined from the A0497 3 6 22Na activity produced in the Al monitor foils in A0497 3 7 the stacks. A0497 3 8 SAMPLE The alloy of Mn/Ni(Mn-88%,Ni-12%) was used. A0497 3 9 ERR-ANALYS (ERR-S,,4.2).The error due to counting statistics and A0497 3 10 photopeak integration as well as uncertainties in A0497 3 11 beam-loss corrections A0497 3 12 (ERR-1) The uncertainty in beam-loss corrections. A0497 3 13 (ERR-2) The uncertainty in detector efficiency. A0497 3 14 (ERR-3) The uncertainty in country geometry. A0497 3 15 (ERR-4) The uncertainty in decay corrections. A0497 3 16 (ERR-5) The uncertainty in the foil thickness. A0497 3 17 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.3 A0497 3 18 (DEP,A0497002) - MONITOR data A0497 3 19 HISTORY (20180527A) SD: SF6=TTY -> TTY/DEN; SF8=TM -> PHY in A0497 3 20 REACTION code (2). Value at Ep=174. MeV corrected. A0497 3 21 (20231227A) SD: SF4=Fe-52 -> Fe-52g in REACTION code. A0497 3 22 STATUS updated. A0497 3 23 ENDBIB 21 0 A0497 3 24 COMMON 5 3 A0497 3 25 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 A0497 3 26 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A0497 3 27 6. 5. 1. 1. 1. A0497 3 28 ENDCOMMON 3 0 A0497 3 29 DATA 5 46 A0497 3 30 EN DATA 1ERR-T 1DATA 2ERR-T 2 A0497 3 31 MEV MB MB CI/AHR/MEV CI/AHR/MEV A0497 3 32 199.9 0.193 0.025 9.58 1.22 A0497 3 33 193.6 0.184 0.021 8.98 1.04 A0497 3 34 187.2 0.208 0.028 9.95 1.32 A0497 3 35 180.7 0.189 0.022 8.81 1.03 A0497 3 36 174.0 0.227 0.031 10.35 1.40 A0497 3 37 168.8 0.205 0.023 9.13 1.04 A0497 3 38 163.5 0.214 0.025 9.38 1.11 A0497 3 39 158.1 0.231 0.027 9.86 1.14 A0497 3 40 152.5 0.245 0.027 10.22 1.14 A0497 3 41 146.8 0.243 0.027 9.87 1.08 A0497 3 42 142.1 0.279 0.031 11.09 1.23 A0497 3 43 137.2 0.269 0.029 10.47 1.12 A0497 3 44 132.2 0.282 0.031 10.69 1.19 A0497 3 45 127.1 0.270 0.031 9.95 1.14 A0497 3 46 121.9 0.323 0.036 11.58 1.27 A0497 3 47 119.8 0.263 0.028 9.31 0.99 A0497 3 48 116.5 0.312 0.034 10.84 1.18 A0497 3 49 113.4 0.308 0.030 10.47 1.01 A0497 3 50 110.9 0.350 0.038 11.72 1.28 A0497 3 51 106.6 0.369 0.036 12.02 1.17 A0497 3 52 101.0 0.384 0.036 12.04 1.12 A0497 3 53 97.7 0.386 0.036 11.81 1.11 A0497 3 54 95.2 0.421 0.039 12.62 1.17 A0497 3 55 93.6 0.423 0.040 12.56 1.19 A0497 3 56 91.5 0.431 0.040 12.56 1.15 A0497 3 57 89.3 0.428 0.041 12.27 1.18 A0497 3 58 87.1 0.441 0.040 12.42 1.14 A0497 3 59 84.8 0.442 0.042 12.21 1.15 A0497 3 60 82.5 0.476 0.048 12.87 1.29 A0497 3 61 80.2 0.531 0.050 14.05 1.32 A0497 3 62 77.8 0.549 0.051 14.21 1.32 A0497 3 63 75.3 0.584 0.054 14.77 1.36 A0497 3 64 72.8 0.647 0.060 15.94 1.47 A0497 3 65 70.3 0.720 0.065 17.26 1.55 A0497 3 66 67.6 0.762 0.068 17.75 1.60 A0497 3 67 64.7 0.897 0.083 20.21 1.87 A0497 3 68 62.7 0.937 0.087 20.63 1.92 A0497 3 69 60.7 1.06 0.097 22.73 2.08 A0497 3 70 58.6 1.12 0.106 23.51 2.21 A0497 3 71 56.4 1.25 0.114 25.47 2.32 A0497 3 72 54.2 1.29 0.116 25.40 2.29 A0497 3 73 52.0 1.12 0.105 21.33 2.00 A0497 3 74 49.6 0.971 0.096 18.01 1.78 A0497 3 75 47.2 0.688 0.073 12.28 1.31 A0497 3 76 44.6 0.496 0.063 8.49 1.08 A0497 3 77 42.0 0.141 0.033 2.31 0.54 A0497 3 78 ENDDATA 48 0 A0497 3 79 ENDSUBENT 78 0 A0497 399999 SUBENT A0497004 20231227 A105A0497 4 1 BIB 8 22 A0497 4 2 REACTION 1(28-NI-0(P,X)26-FE-52-G,,SIG) A0497 4 3 2(28-NI-0(P,X)26-FE-52-G,,TTY/DEN,,PHY) A0497 4 4 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497 4 5 METHOD The incident beam currents were determined from the A0497 4 6 22Na activity produced in the Al monitor foils in A0497 4 7 the stacks. A0497 4 8 SAMPLE The high purity (99.98%) nickel foil. A0497 4 9 REL-REF (A,,S.Tanaka+,J,JIN,34,2419,1972) A0497 4 10 ERR-ANALYS (ERR-S,,4.2).The error due to counting statistics and A0497 4 11 photopeak integration as well as uncertainties in A0497 4 12 beam-loss corrections A0497 4 13 (ERR-1).The uncertainty in beam-loss corrections. A0497 4 14 (ERR-2).The uncertainty in detector efficiency. A0497 4 15 (ERR-3).The uncertainty in country geometry. A0497 4 16 (ERR-4).The uncertainty in decay corrections. A0497 4 17 (ERR-5).The uncertainty in the foil thickness. A0497 4 18 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.4 A0497 4 19 (DEP,A0497002) - MONITOR data A0497 4 20 HISTORY (20180527A) SD: SF1=Ni-50->Ni-0 in both REACTION codes.A0497 4 21 SF6=TTY -> TTY/DEN; SF8=TM -> PHY in REACTION code (2)A0497 4 22 (20231227A) SD: SF4=Fe-52 -> Fe-52g in REACTION code. A0497 4 23 STATUS updated. A0497 4 24 ENDBIB 22 0 A0497 4 25 COMMON 5 3 A0497 4 26 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 A0497 4 27 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A0497 4 28 6. 5. 1. 1. 1. A0497 4 29 ENDCOMMON 3 0 A0497 4 30 DATA 5 45 A0497 4 31 EN DATA 1ERR-T 1DATA 2ERR-T 2 A0497 4 32 MEV MB MB CI/AHR/MEV CI/AHR/MEV A0497 4 33 199.4 2.22 0.18 100.3 8.33 A0497 4 34 193.2 2.16 0.18 95.81 8.01 A0497 4 35 186.8 2.26 0.19 98.23 8.20 A0497 4 36 180.2 2.30 0.19 97.76 8.25 A0497 4 37 173.5 2.27 0.19 94.03 8.03 A0497 4 38 168.3 2.44 0.22 98.90 8.78 A0497 4 39 163.0 2.35 0.20 93.37 8.09 A0497 4 40 157.5 2.33 0.20 90.73 7.94 A0497 4 41 152.0 2.29 0.20 87.04 7.58 A0497 4 42 146.3 2.31 0.21 85.55 7.60 A0497 4 43 141.5 2.34 0.21 84.82 7.53 A0497 4 44 136.6 2.36 0.22 83.28 7.80 A0497 4 45 131.7 2.29 0.21 79.01 7.18 A0497 4 46 126.5 2.25 0.21 75.40 7.15 A0497 4 47 121.3 2.22 0.21 72.20 6.76 A0497 4 48 119.2 2.20 0.19 71.52 6.32 A0497 4 49 112.7 2.15 0.18 66.55 5.60 A0497 4 50 106.0 2.14 0.19 63.19 5.67 A0497 4 51 99.1 2.10 0.20 59.33 5.57 A0497 4 52 97.0 2.08 0.20 57.69 5.43 A0497 4 53 95.0 2.10 0.20 57.40 5.43 A0497 4 54 92.8 2.04 0.20 54.80 5.26 A0497 4 55 90.7 2.12 0.21 56.00 5.27 A0497 4 56 88.5 2.00 0.19 51.91 5.06 A0497 4 57 86.3 2.00 0.19 51.02 4.97 A0497 4 58 84.0 1.96 0.20 48.99 4.88 A0497 4 59 81.7 2.04 0.21 50.04 5.20 A0497 4 60 79.4 2.05 0.21 49.22 5.14 A0497 4 61 76.9 2.26 0.22 53.10 5.21 A0497 4 62 74.5 2.32 0.23 53.13 5.23 A0497 4 63 71.9 2.35 0.23 52.41 5.21 A0497 4 64 69.3 2.66 0.26 57.77 5.57 A0497 4 65 66.6 2.79 0.27 58.86 5.69 A0497 4 66 65.3 2.79 0.25 57.95 5.19 A0497 4 67 63.7 2.75 0.23 55.92 4.71 A0497 4 68 62.0 2.70 0.23 53.80 4.55 A0497 4 69 60.3 2.58 0.22 50.50 4.24 A0497 4 70 58.5 2.46 0.21 47.08 4.07 A0497 4 71 56.7 2.01 0.18 37.43 3.32 A0497 4 72 54.9 1.56 0.14 28.35 2.56 A0497 4 73 53.0 1.20 0.12 21.25 2.14 A0497 4 74 51.1 0.691 0.058 11.91 1.01 A0497 4 75 49.1 0.409 0.071 6.89 1.19 A0497 4 76 47.0 0.203 0.067 3.31 1.10 A0497 4 77 44.9 0.070 0.026 1.15 0.42 A0497 4 78 ENDDATA 47 0 A0497 4 79 ENDSUBENT 78 0 A0497 499999 SUBENT A0497005 20231227 A105A0497 5 1 BIB 7 19 A0497 5 2 REACTION (25-MN-55(P,4N)26-FE-52-G,,TTY,,PHY) A0497 5 3 SAMPLE The stacks of pressed tablets of MnCl(2). A0497 5 4 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497 5 5 METHOD The incident beam currents were determined from the A0497 5 6 22Na activity produced in the Al monitor foils in A0497 5 7 the stacks. A0497 5 8 ERR-ANALYS (ERR-S,,4.2).The error due to counting statistics and A0497 5 9 photopeak integration as well as uncertainties in A0497 5 10 beam-loss corrections A0497 5 11 (ERR-1) The uncertainty in beam-loss corrections. A0497 5 12 (ERR-2) The uncertainty in detector efficiency. A0497 5 13 (ERR-3) The uncertainty in country geometry. A0497 5 14 (ERR-4) The uncertainty in decay corrections. A0497 5 15 (ERR-5) The uncertainty in the foil thickness. A0497 5 16 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.5 A0497 5 17 (DEP,A0497002) - MONITOR data A0497 5 18 HISTORY (20210628A) SD: SF3=X -> 4N in REACTION code. A0497 5 19 (20231227A) SD: SF4=Fe-52 -> Fe-52g in REACTION code. A0497 5 20 STATUS updated. A0497 5 21 ENDBIB 19 0 A0497 5 22 COMMON 5 3 A0497 5 23 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 A0497 5 24 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A0497 5 25 6. 5. 1. 1. 1. A0497 5 26 ENDCOMMON 3 0 A0497 5 27 DATA 4 10 A0497 5 28 EN-MAX EN-MIN DATA ERR-T A0497 5 29 MEV MEV MUCI/MUAHR MUCI/MUAHR A0497 5 30 99.23 94.30 56.77 4.61 A0497 5 31 94.30 89.16 64.41 5.22 A0497 5 32 89.16 83.79 70.71 5.72 A0497 5 33 83.79 78.20 78.31 6.33 A0497 5 34 78.20 72.36 89.20 7.20 A0497 5 35 72.36 66.09 110.43 8.92 A0497 5 36 66.09 59.28 157.36 12.81 A0497 5 37 59.28 51.89 173.75 14.30 A0497 5 38 51.89 43.53 87.03 7.26 A0497 5 39 43.53 33.63 2.76 0.31 A0497 5 40 ENDDATA 12 0 A0497 5 41 ENDSUBENT 40 0 A0497 599999 SUBENT A0497006 20231227 A105A0497 6 1 BIB 7 22 A0497 6 2 REACTION (25-MN-55(P,N)26-FE-55,,TTY,,PHY) A0497 6 3 SAMPLE The stacks of pressed tables of MnCl(2). A0497 6 4 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497 6 5 METHOD The incident beam currents were determined from the A0497 6 6 22Na activity produced in the Al monitor foils in A0497 6 7 the stacks. A0497 6 8 ERR-ANALYS (ERR-S) experimental uncertainty of 2% due to imperfectA0497 6 9 matching of the photomultiplier tubes A0497 6 10 (ERR-3,,2.5).The uncertainty in the beam-loss A0497 6 11 corrections. A0497 6 12 (ERR-4) The uncertainty in beam current integration. A0497 6 13 (ERR-5) The uncertainty in the thickness variations. A0497 6 14 (ERR-6) The uncertainties in the chemical separation A0497 6 15 losses and A0497 6 16 * the subtraction of the indirectly-produced 55Fe A0497 6 17 (via 55Co) from the measured 55Fe contents. A0497 6 18 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.5 A0497 6 19 (DEP,A0497002) - MONITOR data A0497 6 20 HISTORY (20190626A) SD: One of ERR-S -> ERR-T according to A0497 6 21 presentation in the article. A0497 6 22 (20210628A) SD: SF3=X -> N in REACTION code. A0497 6 23 (20231227U) SD: STATUS updated. A0497 6 24 ENDBIB 22 0 A0497 6 25 COMMON 4 3 A0497 6 26 ERR-S ERR-4 ERR-5 ERR-6 A0497 6 27 PER-CENT PER-CENT PER-CENT PER-CENT A0497 6 28 2. 6. 1. 3. A0497 6 29 ENDCOMMON 3 0 A0497 6 30 DATA 4 12 A0497 6 31 EN-MAX EN-MIN DATA ERR-T A0497 6 32 MEV MEV MUCI/MUAHR MUCI/MUAHR A0497 6 33 99.23 94.30 0.274 0.024 A0497 6 34 94.30 89.16 0.288 0.025 A0497 6 35 89.16 83.79 0.301 0.022 A0497 6 36 83.79 78.20 0.351 0.025 A0497 6 37 78.20 72.36 0.370 0.027 A0497 6 38 72.36 66.09 0.397 0.029 A0497 6 39 66.09 59.28 0.482 0.042 A0497 6 40 59.28 51.89 0.553 0.049 A0497 6 41 51.89 43.55 0.668 0.049 A0497 6 42 43.55 33.63 0.867 0.065 A0497 6 43 33.63 20.65 3.01 0.23 A0497 6 44 20.65 0. 5.87 0.44 A0497 6 45 ENDDATA 14 0 A0497 6 46 ENDSUBENT 45 0 A0497 699999 SUBENT A0497007 20231227 A105A0497 7 1 BIB 7 20 A0497 7 2 REACTION (28-NI-0(P,X)26-FE-52-G,,TTY,,PHY) A0497 7 3 SAMPLE The stacks of Ni powder(99.5%) was used. A0497 7 4 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497 7 5 METHOD The incident beam currents were determined from the A0497 7 6 22Na activity produced in the Al monitor foils in A0497 7 7 the stacks. A0497 7 8 ERR-ANALYS (ERR-S,,4.2) The error due to counting statistics and A0497 7 9 photopeak integration as well as uncertainties in A0497 7 10 beam-loss corrections A0497 7 11 (ERR-1) The uncertainty in beam-loss corrections. A0497 7 12 (ERR-2) The uncertainty in detector efficiency. A0497 7 13 (ERR-3) The uncertainty in country geometry. A0497 7 14 (ERR-4) The uncertainty in decay corrections. A0497 7 15 (ERR-5) The uncertainty in the foil thickness. A0497 7 16 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.6 A0497 7 17 (DEP,A0497002) - MONITOR data A0497 7 18 HISTORY (20190626A) SD: ERR-S -> ERR-T in the DATA section A0497 7 19 according to presentation in the article. A0497 7 20 (20231227A) SD: SF4=Fe-52 -> Fe-52g in REACTION code. A0497 7 21 STATUS updated. A0497 7 22 ENDBIB 20 0 A0497 7 23 COMMON 5 3 A0497 7 24 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 A0497 7 25 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A0497 7 26 6. 5. 1. 1. 1. A0497 7 27 ENDCOMMON 3 0 A0497 7 28 DATA 4 12 A0497 7 29 EN-MAX EN-MIN DATA ERR-T A0497 7 30 MEV MEV MUCI/MUAHR MUCI/MUAHR A0497 7 31 99.81 96.09 215.60 18.37 A0497 7 32 96.09 92.27 206.20 17.35 A0497 7 33 92.27 88.33 206.20 18.37 A0497 7 34 88.33 84.25 213.11 19.41 A0497 7 35 84.25 80.02 207.30 18.24 A0497 7 36 80.02 75.62 215.73 18.57 A0497 7 37 75.62 71.02 239.03 20.70 A0497 7 38 71.02 66.19 265.40 22.88 A0497 7 39 66.19 61.07 292.82 25.21 A0497 7 40 61.07 55.61 267.43 23.43 A0497 7 41 55.61 49.72 119.48 12.64 A0497 7 42 49.72 43.28 27.94 6.76 A0497 7 43 ENDDATA 14 0 A0497 7 44 ENDSUBENT 43 0 A0497 799999 SUBENT A0497008 20240926 A119A0497008 1 BIB 9 31 A0497008 2 REACTION 1(28-NI-0(P,X)27-CO-55,,TTY,,PHY/MSC) A0497008 3 Ni(p,x)55Co -> 55Fe part of 55Fe production A0497008 4 2(28-NI-0(P,X)26-FE-55,,TTY,,PHY) A0497008 5 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497008 6 METHOD The incident beam currents were determined from the A0497008 7 22Na activity produced in the Al monitor foils in A0497008 8 the stacks. A0497008 9 SAMPLE The stacks of Ni powder(99.5%) was used. A0497008 10 MISC-COL Ni(p,x)55Co -> 55Fe part of 55Fe production A0497008 11 ERR-ANALYS (ERR-S) The total uncertainty in the liquid- A0497008 12 scintillation data. A0497008 13 (ERR-1,,2.5) The uncertainty in the beam-loss A0497008 14 corrections. A0497008 15 (ERR-2) The uncertainty in beam current integration. A0497008 16 (ERR-3) The uncertainty in the thickness variations. A0497008 17 (ERR-4) The uncertainties in the chemical separation A0497008 18 losses and A0497008 19 * the subtraction of the indirectly-produced 55Fe A0497008 20 (via 55Co) from the measured 55Fe contents. A0497008 21 COMMENT From Dr. G.F.Steyn (2014-09-02): The Ni(p,x)55Co yield A0497008 22 used for the correction (REATION (1)) is from the A0497008 23 measurement on the same set of Ni targets, but it is A0497008 24 unpublished and no longer available. A0497008 25 From Dr. N.Otsuka (24.09.2024): It actually gives A0497008 26 Ni(p,x)55Co decay contribution used for subtraction of A0497008 27 the decay contribution to obtain the 008.2 dataset. A0497008 28 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.6 A0497008 29 (DEP,A0497002) - MONITOR data A0497008 30 HISTORY (20231227A) SD: SF5=IND in REACTION code (2) deleted. A0497008 31 STATUS updated. A0497008 32 (20240926A) SD: SF4=Fe-55 -> Co-55 in REACTION (1). A0497008 33 ENDBIB 31 0 A0497008 34 COMMON 4 3 A0497008 35 ERR-S ERR-2 ERR-3 ERR-4 A0497008 36 PER-CENT PER-CENT PER-CENT PER-CENT A0497008 37 3. 6. 1. 3. A0497008 38 ENDCOMMON 3 0 A0497008 39 DATA 6 14 A0497008 40 EN-MAX EN-MIN DATA 2ERR-T 2DATA 1ERR-T 1A0497008 41 MEV MEV MUCI/MUAHR MUCI/MUAHR MUCI/MUAHR MUCI/MUAHR A0497008 42 99.81 96.09 2.470 0.197 0.867 0.076A0497008 43 96.09 92.27 2.636 0.210 0.918 0.080A0497008 44 92.27 88.33 2.731 0.198 0.891 0.078A0497008 45 88.33 84.25 2.677 0.215 0.959 0.084A0497008 46 84.25 80.02 2.815 0.226 0.982 0.086A0497008 47 80.02 75.62 2.852 0.231 0.997 0.088A0497008 48 75.62 71.02 2.981 0.242 1.062 0.092A0497008 49 71.02 66.19 3.238 0.263 1.122 0.095A0497008 50 66.19 61.07 3.457 0.285 1.230 0.108A0497008 51 61.07 55.61 3.665 0.305 1.357 0.118A0497008 52 55.61 49.72 3.972 0.322 1.230 0.109A0497008 53 49.72 43.28 3.327 0.269 0.889 0.081A0497008 54 43.28 36.02 1.459 0.119 0.348 0.038A0497008 55 36.02 27.41 0.300 0.047 0.196 0.039A0497008 56 ENDDATA 16 0 A0497008 57 ENDSUBENT 56 0 A049700899999 SUBENT A0497009 20231227 A105A0497 9 1 BIB 7 21 A0497 9 2 REACTION (28-NI-0(P,X)26-FE-59,,TTY,,PHY) A0497 9 3 SAMPLE The stacks of Ni powder(99.5%) was used. A0497 9 4 MONITOR (13-AL-27(P,X)11-NA-22,,SIG) A0497 9 5 METHOD The incident beam currents were determined from the A0497 9 6 22Na activity produced in the Al monitor foils in A0497 9 7 the stacks. A0497 9 8 ERR-ANALYS (ERR-S) The total uncertainty in the liquid- A0497 9 9 scintillation data. A0497 9 10 (ERR-1) An uncertainty in the correction for the effectA0497 9 11 of the Fe-59 gamma-activity. A0497 9 12 (ERR-2,,2.5) The uncertainty in the beam-loss A0497 9 13 corrections. A0497 9 14 (ERR-3) The uncertainty in beam current integration. A0497 9 15 (ERR-4) The uncertainty in the thickness variations. A0497 9 16 (ERR-5) The uncertainties in the chemical separation A0497 9 17 losses and A0497 9 18 * the subtraction of the indirectly-produced 55Fe A0497 9 19 (via 55Co) from the measured 55Fe contents. A0497 9 20 STATUS (TABLE,,G.F.Steyn+,J,ARI,41,315,1990) Tbl.6 A0497 9 21 (DEP,A0497002) - MONITOR data A0497 9 22 HISTORY (20231227U) SD: STATUS updated. A0497 9 23 ENDBIB 21 0 A0497 9 24 COMMON 5 3 A0497 9 25 ERR-S ERR-1 ERR-3 ERR-4 ERR-5 A0497 9 26 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT A0497 9 27 3. 2. 6. 1. 3. A0497 9 28 ENDCOMMON 3 0 A0497 9 29 DATA 4 15 A0497 9 30 EN-MAX EN-MIN DATA ERR-T A0497 9 31 MEV MEV MUCI/MUAHR MUCI/MUAHR A0497 9 32 99.81 96.09 115.60E-3 10.42E-3 A0497 9 33 96.09 92.27 124.20E-3 11.22E-3 A0497 9 34 92.27 88.33 120.60E-3 10.88E-3 A0497 9 35 88.33 84.25 118.55E-3 10.51E-3 A0497 9 36 84.25 80.02 110.72E-3 10.17E-3 A0497 9 37 80.02 75.62 111.60E-3 10.12E-3 A0497 9 38 75.62 71.02 110.92E-3 9.26E-3 A0497 9 39 71.02 66.19 99.91E-3 9.16E-3 A0497 9 40 66.19 61.07 99.31E-3 9.12E-3 A0497 9 41 61.07 55.61 82.62E-3 7.91E-3 A0497 9 42 55.61 49.72 77.69E-3 7.38E-3 A0497 9 43 49.72 43.28 72.06E-3 7.03E-3 A0497 9 44 43.28 36.02 58.53E-3 6.02E-3 A0497 9 45 36.02 27.41 23.39E-3 3.02E-3 A0497 9 46 27.41 15.89 8.81E-3 1.92E-3 A0497 9 47 ENDDATA 17 0 A0497 9 48 ENDSUBENT 47 0 A0497 999999 ENDENTRY 9 0 A049799999999