ENTRY D4114 20190822 D121D411400000001 SUBENT D4114001 20190822 D121D411400100001 BIB 12 49 D411400100002 TITLE Excitation functions of proton induced nuclear D411400100003 reactions on natRb from 30 to 70 MeV. Implication for D411400100004 the production of 82Sr and other medically important D411400100005 Rb and Sr radioisotopes D411400100006 AUTHOR (T.Ido, A.Hermanne, F.Ditroi, Z.Szucs, I.Mahunka, D411400100007 F.Tarkanyi) D411400100008 INSTITUTE (2JPNTOH,2BLGVUB,3HUNDEB) D411400100009 REFERENCE (J,NIM/B,194,369,2002) D411400100010 (J,NSTS,2,1310,2002) Preliminary data given D411400100011 FACILITY (CYCLO,2JPNTOH) AVF cyclotron D411400100012 (CYCLO,2BLGVUB) CGR 560 cyclotron D411400100013 SAMPLE Samples were RbCl powder (99.4%) from Aldrich Chem. Co.D411400100014 Al 25.0 micron and Cu 10.0 micron foils for D411400100015 beam monitoring. D411400100016 Targets were dried under vacuum and the irradiation D411400100017 was done in He gas atmosphere at 40, 50 and 70 MeV D411400100018 with 20 to 100 nA beam for 30 min. D411400100019 METHOD (ACTIV,EXTB,STTA,GSPEC) D411400100020 Stacked target technique was used. D411400100021 Cu and Al foils were used for beam monitoring beside D411400100022 Faraday-cup measurement. D411400100023 The effect of secondary neutron was checked and no D411400100024 measurable contribution was found. D411400100025 REL-REF (R,,E.Browne+,B,BROWNE,,,1986) D411400100026 Decay data given D411400100027 DETECTOR (HPGE) High purity Ge gamma detector D411400100028 MONITOR Several monitor foils and target foils were placed in D411400100029 the same stack. D411400100030 This way the whole excitation function of the monitor D411400100031 reaction was remeasured and compared with the D411400100032 recommended values. D411400100033 It made possible simultaneous determination of the D411400100034 bombarding energy and beam intensity. D411400100035 Also in to check the energy degradation along the D411400100036 stack. D411400100037 (29-CU-0(P,X)30-ZN-62,,SIG) D411400100038 (29-CU-0(P,X)27-CO-58,,SIG) D411400100039 (13-AL-27(P,X)11-NA-24,,SIG) D411400100040 MONIT-REF (,F.Tarkanyi+,R,IAEA-TECDOC-1211,2001) chapter 4. D411400100041 HISTORY (20030327C) TS D411400100042 (20040120) Finalized at NDS D411400100043 (20070307A) KB Reference was completed. D411400100044 (20130625U) On. REFERENCE: 2001TSUKUB deleted D411400100045 (20160513U) VS Decay data corrected in 006. D411400100046 (20161103A) ST. 010-011 added. D411400100047 (20190822A) SD: REACTION code updated according to new D411400100048 EXFOR rules in Subent 008, 009. D411400100049 Small corrections in all Subents. METHOD and SAMPLE D411400100050 updated. D411400100051 ENDBIB 49 0 D411400100052 NOCOMMON 0 0 D411400100053 ENDSUBENT 52 0 D411400199999 SUBENT D4114002 20190822 D121D411400200001 BIB 7 23 D411400200002 REACTION 1(37-RB-0(P,X)38-SR-82,,SIG) D411400200003 2(37-RB-0(P,X)38-SR-83,,SIG) D411400200004 DECAY-DATA1(37-RB-82-G,1.273MIN,DG,776.5,0.134) D411400200005 2(38-SR-83-G,1.35D,DG,381.6,0.119, D411400200006 DG,762.7,0.30) D411400200007 RAD-DET 1(37-RB-82,DG) Daughter of 82Sr D411400200008 SAMPLE RbCl powder 100 mg/cm2 was pressed into high purity Al D411400200009 backing and covered with 25 micron Al window. D411400200010 Al 25.0 micron and Cu 10.0 micron foils for D411400200011 beam monitoring. D411400200012 ERR-ANALYS (EN-ERR) The energy attenuation was calculated by D411400200013 using the method of Williamson. D411400200014 (ERR-T)Total error of the data are around 12%. D411400200015 Main contributing error components are: D411400200016 (ERR-1) uncertainty in beam intensity 7% D411400200017 (ERR-2) uncertainty in detector efficiency 5% D411400200018 (ERR-3,0.1,10.) uncertainty in peak area 0.1-10% D411400200019 (ERR-4) uncertainty in number of target nuclei 3% D411400200020 (ERR-5) uncertainty in nuclear data 3% D411400200021 STATUS (TABLE) Table 4 from Nucl.Instr.Meth.,B194(2002)369 D411400200022 (APRVD) Approved by F. Tarkanyi. D411400200023 HISTORY (20190822U) SD: SAMPLE added.ERR-ANALYS, STATUS updatedD411400200024 On.DECAY-DATA:RB-82->RB-82-G. RAD-DET addedD411400200025 ENDBIB 23 0 D411400200026 COMMON 4 3 D411400200027 ERR-1 ERR-2 ERR-4 ERR-5 D411400200028 PER-CENT PER-CENT PER-CENT PER-CENT D411400200029 7. 5. 3. 3. D411400200030 ENDCOMMON 3 0 D411400200031 DATA 6 25 D411400200032 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2D411400200033 MEV MEV MB MB MB MB D411400200034 33.7 1.7 0.34 0.05 D411400200035 34.1 0.5 1.06 0.26 D411400200036 35.2 1.6 3.25 0.49 D411400200037 35.8 1.6 4.37 0.72 274.5 30.8D411400200038 37.2 1.4 8.98 1.08 255.5 28.7D411400200039 39.4 1.2 16.1 2.1 D411400200040 39.5 1.2 25.9 3.2 242.4 22.7D411400200041 40.9 1.1 46.0 6.2 203.7 22.9D411400200042 41.2 1.1 54.9 7.1 D411400200043 43. 0.9 68.0 8.0 169.4 19.0D411400200044 44.3 0.8 79.7 9.2 140.2 15.8D411400200045 44.5 0.8 75.1 9.8 D411400200046 46.2 0.6 90.3 10.4 117.0 13.2D411400200047 46.5 2.3 84.3 9.7 103.8 11.7D411400200048 46.8 0.6 96.6 12.6 D411400200049 47.6 0.5 99.0 11.4 106.6 11.6D411400200050 49.3 0.4 98.0 11.3 97.5 10.4D411400200051 49.7 2.1 90.7 10.4 84.4 9.6D411400200052 52.8 1.8 96.6 9.9 76.5 8.7D411400200053 55.8 1.5 81.8 9.4 80.4 9.1D411400200054 58.4 1.3 60.6 7.0 75.0 8.5D411400200055 61.5 1.0 55.0 7.2 80.1 9.1D411400200056 64.2 0.8 48.8 5.7 76.6 8.7D411400200057 66.8 0.6 43.0 5.1 73.3 8.3D411400200058 69.3 0.4 41.2 4.8 71.5 8.1D411400200059 ENDDATA 27 0 D411400200060 ENDSUBENT 59 0 D411400299999 SUBENT D4114003 20190822 D121D411400300001 BIB 6 20 D411400300002 REACTION 1(37-RB-0(P,X)38-SR-85-G,M+,SIG) D411400300003 2(37-RB-0(P,X)38-SR-87-M,,SIG) D411400300004 DECAY-DATA1(38-SR-85-G,64.84D,DG,514.0,0.9927) D411400300005 2(38-SR-87-M,2.8HR,DG,388.4,0.823) D411400300006 SAMPLE RbCl powder 100 mg/cm2 was pressed into high purity Al D411400300007 backing and covered with 25 micron Al window. D411400300008 Al 25.0 micron and Cu 10.0 micron foils for D411400300009 beam monitoring. D411400300010 ERR-ANALYS (EN-ERR) The energy attenuation was calculated by D411400300011 using the method of Williamson. D411400300012 (ERR-T)Total error of the data are around 12%. D411400300013 Main contributing error components are: D411400300014 (ERR-1) uncertainty in beam intensity 7% D411400300015 (ERR-2) uncertainty in detector efficiency 5% D411400300016 (ERR-3,0.1,10.) uncertainty in peak area 0.1-10% D411400300017 (ERR-4) uncertainty in number of target nuclei 3% D411400300018 (ERR-5) uncertainty in nuclear data 3% D411400300019 STATUS (TABLE) Table 4 from Nucl.Instr.Meth.,B194(2002)369 D411400300020 Approved by F. Tarkanyi. D411400300021 HISTORY (20190822U) SD: SAMPLE added.ERR-ANALYS, STATUS updatedD411400300022 ENDBIB 20 0 D411400300023 COMMON 4 3 D411400300024 ERR-1 ERR-2 ERR-4 ERR-5 D411400300025 PER-CENT PER-CENT PER-CENT PER-CENT D411400300026 7. 5. 3. 3. D411400300027 ENDCOMMON 3 0 D411400300028 DATA 6 18 D411400300029 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2D411400300030 MEV MEV MB MB MB MB D411400300031 35.8 1.6 164.7 18.5 8.70 2.40D411400300032 37.2 1.4 147.9 16.6 11.4 2.6D411400300033 39.5 1.2 135.6 12.5 6.56 1.54D411400300034 40.9 1.1 111.1 12.5 12.8 3.0D411400300035 43.0 0.9 97.5 11.0 14.2 3.4D411400300036 44.3 0.8 87.6 10.0 10.3 2.4D411400300037 46.2 0.6 73.9 8.4 9.28 2.28D411400300038 46.5 2.3 70.3 8.0 9.97 2.60D411400300039 47.6 0.5 77.2 8.8 9.35 2.29D411400300040 49.3 0.4 47.4 5.5 7.94 2.06D411400300041 49.7 2.1 63.6 7.2 9.87 2.66D411400300042 52.8 1.8 54.9 6.3 8.76 2.42D411400300043 55.8 1.5 54.3 6.2 10.0 2.7D411400300044 58.4 1.3 47.4 5.4 10.9 3.2D411400300045 61.5 1.0 46.3 5.3 11.0 2.9D411400300046 64.2 0.8 44.3 5.1 11.1 3.0D411400300047 66.8 0.6 41.1 4.7 10.2 2.8D411400300048 69.3 0.4 48.3 5.5 10.3 2.7D411400300049 ENDDATA 20 0 D411400300050 ENDSUBENT 49 0 D411400399999 SUBENT D4114004 20190822 D121D411400400001 BIB 6 25 D411400400002 REACTION 1(37-RB-0(P,X)37-RB-81-G,M+,SIG) D411400400003 2(37-RB-0(P,X)37-RB-82-M,,SIG) D411400400004 DECAY-DATA1(37-RB-81-G,4.58HR,DG,190.4,0.643, D411400400005 DG,446.3,0.233) D411400400006 2(37-RB-82-M,6.47HR,DG,554.4,0.625, D411400400007 DG,619.1,0.38, D411400400008 DG,698.4,0.264) D411400400009 SAMPLE RbCl powder 100 mg/cm2 was pressed into high purity Al D411400400010 backing and covered with 25 micron Al window. D411400400011 Al 25.0 micron and Cu 10.0 micron foils for D411400400012 beam monitoring. D411400400013 ERR-ANALYS (EN-ERR) The energy attenuation was calculated by D411400400014 using the method of Williamson. D411400400015 (ERR-T)Total error of the data are around 12%. D411400400016 Main contributing error components are: D411400400017 (ERR-1) uncertainty in beam intensity 7% D411400400018 (ERR-2) uncertainty in detector efficiency 5% D411400400019 (ERR-3,0.1,10.) uncertainty in peak area 0.1-10% D411400400020 (ERR-4) uncertainty in number of target nuclei 3% D411400400021 (ERR-5) uncertainty in nuclear data 3% D411400400022 STATUS (TABLE) Table 4 from Nucl.Instr.Meth.,B194(2002)369 D411400400023 In the DATA section corrected data are given (it is D411400400024 mistake in publication). D411400400025 (APRVD) Approved by F. Tarkanyi. D411400400026 HISTORY (20190822U) SD: SAMPLE added.ERR-ANALYS, STATUS updatedD411400400027 ENDBIB 25 0 D411400400028 COMMON 4 3 D411400400029 ERR-1 ERR-2 ERR-4 ERR-5 D411400400030 PER-CENT PER-CENT PER-CENT PER-CENT D411400400031 7. 5. 3. 3. D411400400032 ENDCOMMON 3 0 D411400400033 DATA 6 18 D411400400034 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2D411400400035 MEV MEV MB MB MB MB D411400400036 35.8 1.6 2.84 0.26D411400400037 37.2 1.4 3.28 0.37D411400400038 39.5 1.2 22.4 4.6D411400400039 40.9 1.1 21.7 2.5D411400400040 43.0 0.9 58.1 8.4D411400400041 44.3 0.8 1.20 0.20 55.8 6.3D411400400042 46.2 0.6 1.43 0.21 91.0 12.9D411400400043 46.5 2.3 2.17 0.31 91.3 11.1D411400400044 47.6 0.5 2.91 0.38 85.6 9.6D411400400045 49.3 0.4 5.22 0.61 121.4 16.1D411400400046 49.7 2.1 7.15 0.83 120.5 20.2D411400400047 52.8 1.8 21.2 2.4 117.2 14.0D411400400048 55.8 1.5 53.3 8.3 129.2 15.3D411400400049 58.4 1.3 73.2 9.8 112.8 13.4D411400400050 61.5 1.0 108.4 13.5 111.8 13.3D411400400051 64.2 0.8 125.5 15.3 102.4 12.3D411400400052 66.8 0.6 126.6 15.4 99.4 12.1D411400400053 69.3 0.4 135.2 17.5 99.2 12.8D411400400054 ENDDATA 20 0 D411400400055 ENDSUBENT 54 0 D411400499999 SUBENT D4114005 20190822 D121D411400500001 BIB 6 22 D411400500002 REACTION 1(37-RB-0(P,X)37-RB-83,,SIG) D411400500003 2(37-RB-0(P,X)37-RB-84,,SIG) D411400500004 DECAY-DATA1(37-RB-83,86.2D,DG,520.2,0.46) D411400500005 DG,529.7,0.302 D411400500006 DG,552.7,0.163) D411400500007 2(37-RB-84-G,32.87D,DG,881.7,0.679) D411400500008 SAMPLE RbCl powder 100 mg/cm2 was pressed into high purity Al D411400500009 backing and covered with 25 micron Al window. D411400500010 Al 25.0 micron and Cu 10.0 micron foils for D411400500011 beam monitoring. D411400500012 ERR-ANALYS (EN-ERR) The energy attenuation was calculated by D411400500013 using the method of Williamson. D411400500014 (ERR-T)Total error of the data are around 12%. D411400500015 Main contributing error components are: D411400500016 (ERR-1) uncertainty in beam intensity 7% D411400500017 (ERR-2) uncertainty in detector efficiency 5% D411400500018 (ERR-3,0.1,10.) uncertainty in peak area 0.1-10% D411400500019 (ERR-4) uncertainty in number of target nuclei 3% D411400500020 (ERR-5) uncertainty in nuclear data 3% D411400500021 STATUS (TABLE) Table 4 from Nucl.Instr.Meth.,B194(2002)369 D411400500022 (APRVD) Approved by F. Tarkanyi. D411400500023 HISTORY (20190822U) SD: SAMPLE added.ERR-ANALYS, STATUS updatedD411400500024 ENDBIB 22 0 D411400500025 COMMON 4 3 D411400500026 ERR-1 ERR-2 ERR-4 ERR-5 D411400500027 PER-CENT PER-CENT PER-CENT PER-CENT D411400500028 7. 5. 3. 3. D411400500029 ENDCOMMON 3 0 D411400500030 DATA 6 18 D411400500031 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2D411400500032 MEV MEV MB MB MB MB D411400500033 35.8 1.6 458.5 51.5 129.6 14.6D411400500034 37.2 1.4 452.4 50.8 126.3 14.2D411400500035 39.5 1.2 454.7 42.6 136.0 12.8D411400500036 40.9 1.1 407.7 45.9 134.1 15.1D411400500037 43.0 0.9 368.2 41.6 141.5 16.0D411400500038 44.3 0.8 317.8 35.9 140.3 15.8D411400500039 46.2 0.6 279.2 31.6 138.4 15.6D411400500040 46.5 2.3 272.6 30.8 137.9 15.5D411400500041 47.6 0.5 270.5 30.5 153.0 17.2D411400500042 49.3 0.4 247.1 28.1 148.4 16.7D411400500043 49.7 2.1 244.8 28.7 142.7 16.1D411400500044 52.8 1.8 235.1 26.6 145.9 16.4D411400500045 55.8 1.5 240.8 27.2 154.0 17.4D411400500046 58.4 1.3 229.5 25.9 139.3 15.7D411400500047 61.5 1.0 250.7 28.3 143.8 16.2D411400500048 64.2 0.8 251.1 28.4 146.6 16.5D411400500049 66.8 0.6 240.9 27.2 137.8 15.5D411400500050 69.3 0.4 248.6 28.1 142.4 13.0D411400500051 ENDDATA 20 0 D411400500052 ENDSUBENT 51 0 D411400599999 SUBENT D4114006 20190822 D121D411400600001 BIB 6 17 D411400600002 REACTION (37-RB-0(P,X)37-RB-86,,SIG) D411400600003 DECAY-DATA (37-RB-86-G,18.66D,DG,1076.7,0.088) D411400600004 SAMPLE RbCl powder 100 mg/cm2 was pressed into high purity Al D411400600005 backing and covered with 25 micron Al window. D411400600006 Al 25.0 micron and Cu 10.0 micron foils for D411400600007 beam monitoring. D411400600008 ERR-ANALYS (ERR-T)Total error of the data are around 12%. D411400600009 Main contributing error components are: D411400600010 (ERR-1) uncertainty in beam intensity 7% D411400600011 (ERR-2) uncertainty in detector efficiency 5% D411400600012 (ERR-3,0.1,10.) uncertainty in peak area 0.1-10% D411400600013 (ERR-4) uncertainty in number of target nuclei 3% D411400600014 (ERR-5) uncertainty in nuclear data 3% D411400600015 STATUS (TABLE) Table 4 from Nucl.Instr.Meth.,B194(2002)369 D411400600016 (APRVD) Approved by F. Tarkanyi. D411400600017 HISTORY (20160513U) VS Decay data corrected. D411400600018 (20190822U) SD: SAMPLE added.ERR-ANALYS, STATUS updatedD411400600019 ENDBIB 17 0 D411400600020 COMMON 4 3 D411400600021 ERR-1 ERR-2 ERR-4 ERR-5 D411400600022 PER-CENT PER-CENT PER-CENT PER-CENT D411400600023 7. 5. 3. 3. D411400600024 ENDCOMMON 3 0 D411400600025 DATA 4 18 D411400600026 EN EN-ERR DATA ERR-T D411400600027 MEV MEV MB MB D411400600028 35.8 1.6 42.7 2.40 D411400600029 37.2 1.4 40.7 2.6 D411400600030 39.5 1.2 41.6 1.54 D411400600031 40.9 1.1 41.3 3.0 D411400600032 43.0 0.9 41.1 3.4 D411400600033 44.3 0.8 40.7 2.4 D411400600034 46.2 0.6 37.1 2.28 D411400600035 46.5 2.3 35.5 2.60 D411400600036 47.6 0.5 42.0 2.29 D411400600037 49.3 0.4 37.9 2.06 D411400600038 49.7 2.1 34.0 2.66 D411400600039 52.8 1.8 32.9 2.42 D411400600040 55.8 1.5 35.8 2.7 D411400600041 58.4 1.3 33.1 3.2 D411400600042 61.5 1.0 36.5 2.9 D411400600043 64.2 0.8 35.6 3.0 D411400600044 66.8 0.6 33.4 2.8 D411400600045 69.3 0.4 34.9 2.7 D411400600046 ENDDATA 20 0 D411400600047 ENDSUBENT 46 0 D411400699999 SUBENT D4114007 20190822 D121D411400700001 BIB 6 16 D411400700002 REACTION (29-CU-0(P,X)27-CO-58-G,M+,SIG) D411400700003 DECAY-DATA (27-CO-58-G,70.916D,DG,810.791,0.995) D411400700004 SAMPLE RbCl powder 100 mg/cm2 was pressed into high purity Al D411400700005 backing and covered with 25 micron Al window. D411400700006 Al 25.0 micron and Cu 10.0 micron foils for D411400700007 beam monitoring. D411400700008 ERR-ANALYS (ERR-T)Total error of the data are around 12%. D411400700009 Main contributing error components are: D411400700010 (ERR-1) uncertainty in beam intensity 7% D411400700011 (ERR-2) uncertainty in detector efficiency 5% D411400700012 (ERR-3,0.1,10.) uncertainty in peak area 0.1-10% D411400700013 (ERR-4) uncertainty in number of target nuclei 3% D411400700014 (ERR-5) uncertainty in nuclear data 3% D411400700015 STATUS (TABLE) Table 4 from Nucl.Instr.Meth.,B194(2002)369 D411400700016 (APRVD) Approved by F. Tarkanyi. D411400700017 HISTORY (20190822U) SD: SAMPLE added.ERR-ANALYS, STATUS updatedD411400700018 ENDBIB 16 0 D411400700019 COMMON 4 3 D411400700020 ERR-1 ERR-2 ERR-4 ERR-5 D411400700021 PER-CENT PER-CENT PER-CENT PER-CENT D411400700022 7. 5. 3. 3. D411400700023 ENDCOMMON 3 0 D411400700024 DATA 4 29 D411400700025 EN EN-ERR DATA ERR-T D411400700026 MEV MEV MB MB D411400700027 28.9 3.8 7.0 1.6 D411400700028 34.5 3.3 39.9 5.5 D411400700029 35.8 1.5 41.9 5.5 D411400700030 37.2 1.4 44.5 5.8 D411400700031 39.4 2.9 51.7 7.0 D411400700032 39.5 1.2 49.2 6.5 D411400700033 40.9 1.1 49.0 6.4 D411400700034 43.0 0.9 47.3 6.2 D411400700035 44.2 2.5 46.7 6.3 D411400700036 44.3 0.8 40.1 5.3 D411400700037 46.2 0.6 41.9 5.5 D411400700038 47.1 2.3 36.6 4.6 D411400700039 48.4 2.1 35.5 4.9 D411400700040 49.7 0.3 33.0 4.4 D411400700041 49.9 0.3 32.2 4.2 D411400700042 50.2 2.0 33.3 4.0 D411400700043 52.4 1.8 28.9 4.0 D411400700044 53.3 1.7 27.7 3.5 D411400700045 56.1 1.4 28.3 3.8 D411400700046 56.3 1.5 27.3 3.4 D411400700047 59.2 1.2 27.4 3.4 D411400700048 59.6 1.1 30.4 4.1 D411400700049 62.0 1.0 28.1 3.5 D411400700050 63.1 0.8 27.0 3.7 D411400700051 64.7 0.7 32.3 4. D411400700052 66.5 0.5 34.9 4.6 D411400700053 67.2 0.5 33.7 4.1 D411400700054 69.2 0.3 37.8 4.9 D411400700055 69.8 0.3 38.7 4.7 D411400700056 ENDDATA 31 0 D411400700057 ENDSUBENT 56 0 D411400799999 SUBENT D4114008 20190822 D121D411400800001 BIB 6 15 D411400800002 REACTION 1(37-RB-0(P,X)38-SR-82,,TTY,,PHY,DERIV) D411400800003 2(37-RB-0(P,X)38-SR-85-G,M+,TTY,,PHY,DERIV) D411400800004 DECAY-DATA1(37-RB-82-G,1.273MIN,DG,776.5,0.134) D411400800005 2(38-SR-85-G,64.84D,DG,514.0,0.9927) D411400800006 RAD-DET 1(37-RB-82-G,DG) D411400800007 ANALYSIS (INTEF) Derived from measured excitation function D411400800008 With the help of the already existing data(see REL-REF)D411400800009 at the lower energy end, the integral yield of 83Sr D411400800010 over the required energy range can be calculated and D411400800011 the impurity level for the most disturbing D411400800012 radioisotope (85Sr) can be estimated. D411400800013 STATUS (TABLE) Table 6 from Nucl.Instr.Meth.,B194(2002)369 D411400800014 (APRVD) Approved by F. Tarkanyi. D411400800015 HISTORY (20190822A) SD: SF8=DT -> PHY; SF9=DERIV in both D411400800016 REACTION codes. ANALYSIS added. STATUS updated. D411400800017 ENDBIB 15 0 D411400800018 NOCOMMON 0 0 D411400800019 DATA 3 5 D411400800020 EN DATA 1DATA 2 D411400800021 MEV GBQ/COUL GBQ/COUL D411400800022 40. 0.08 2.18 D411400800023 50. 1.40 2.63 D411400800024 55. 2.30 2.80 D411400800025 60. 3.03 2.95 D411400800026 70. 4.06 3.25 D411400800027 ENDDATA 7 0 D411400800028 ENDSUBENT 27 0 D411400899999 SUBENT D4114009 20190822 D121D411400900001 BIB 7 22 D411400900002 REACTION 1(37-RB-85(P,3N)38-SR-83,,TTY,,PHY,DERIV) D411400900003 2(37-RB-85(P,N)38-SR-85-G,M+,TTY,,PHY,DERIV) D411400900004 DECAY-DATA1(37-RB-83,86.2D,DG,520.5,0.46) D411400900005 2(38-SR-85-G,64.84D,DG,514.0,0.9927) D411400900006 ANALYSIS (INTEF) Derived from measured excitation function D411400900007 With the help of the already existing data(see REL-REF)D411400900008 at the lower energy end, the integral yield of 83Sr D411400900009 over the required energy range can be calculated and D411400900010 the impurity level for the most disturbing D411400900011 radioisotope (85Sr) can be estimated. D411400900012 COMMENT From the text. The integral yields for enriched targetsD411400900013 were calculated for estimation of production yields of D411400900014 82Sr, 83Sr and 85Sr. D411400900015 REL-REF (R,B0111002,T.Horiguchi+,J,ARI,31,141,1980) D411400900016 (R,C0780003,Lagunas-Solar,J,NIM/B,69,452,1992). D411400900017 (R,E1867010,K.Sakamoto+,J,ARI,36,481,1985) D411400900018 STATUS (TABLE) Table 7 from Nucl.Instr.Meth.,B194(2002)369 D411400900019 (APRVD) Approved by F. Tarkanyi. D411400900020 (DEP,D4114002) excitation function D411400900021 HISTORY (20190822A) SD: SF8=DT -> PHY; SF9=DERIV in both D411400900022 REACTION codes. ANALYSIS, COMMENT, REL-REF added. D411400900023 STATUS updated. D411400900024 ENDBIB 22 0 D411400900025 NOCOMMON 0 0 D411400900026 DATA 3 5 D411400900027 EN DATA 1DATA 2 D411400900028 MEV GBQ/COUL GBQ/COUL D411400900029 30. 13.0 0.954 D411400900030 35. 62.4 1.03 D411400900031 40. 115. 1.10 D411400900032 45. 151. 1.19 D411400900033 50. 175. 1.28 D411400900034 ENDDATA 7 0 D411400900035 ENDSUBENT 34 0 D411400999999 SUBENT D4114010 20161103 D121D411401000001 BIB 4 15 D411401000002 REACTION 1(37-RB-0(P,X)37-RB-81-G,M+,TTY,,PHY) D411401000003 2(37-RB-0(P,X)37-RB-82-M,,TTY,,PHY) D411401000004 3(37-RB-0(P,X)37-RB-83,,TTY,,PHY) D411401000005 4(37-RB-0(P,X)37-RB-84-G,M+,TTY,,PHY) D411401000006 DECAY-DATA1(37-RB-81-G,4.58HR,DG,190.4,0.643, D411401000007 DG,446.3,0.233) D411401000008 2(37-RB-82-M,6.47HR,DG,554.4,0.625, D411401000009 DG,619.1,0.38, D411401000010 DG,698.4,0.264) D411401000011 3(37-RB-83,86.2D,DG,520.2,0.46) D411401000012 DG,529.7,0.302 D411401000013 DG,552.7,0.163) D411401000014 4(37-RB-84-G,32.87D,DG,881.7,0.679) D411401000015 STATUS (TABLE) Numerical data were taken from author F.Ditroi D411401000016 HISTORY (20161103C) ST D411401000017 ENDBIB 15 0 D411401000018 NOCOMMON 0 0 D411401000019 DATA 5 10 D411401000020 EN DATA 1DATA 2DATA 3DATA 4 D411401000021 MEV GBQ/COUL GBQ/COUL GBQ/COUL GBQ/COUL D411401000022 69.6 440.1 532.9 6.3 7.7 D411401000023 66.5 325.1 469.1 5.8 6.9 D411401000024 62.8 203.9 397.8 5.3 6.0 D411401000025 59.6 114.6 330.0 4.7 5.3 D411401000026 56.0 50.6 255.4 4.2 4.5 D411401000027 52.4 15.8 176.1 3.7 3.7 D411401000028 48.4 3.4 99.4 3.2 2.9 D411401000029 43.9 0.6 39.7 2.6 2.1 D411401000030 39.4 7.7 1.8 1.4 D411401000031 34.3 0.7 0.9 0.7 D411401000032 ENDDATA 12 0 D411401000033 ENDSUBENT 32 0 D411401099999 SUBENT D4114011 20161103 D121D411401100001 BIB 5 12 D411401100002 REACTION 1(37-RB-0(P,X)37-RB-86-G,M+,TTY,,PHY) D411401100003 2(37-RB-0(P,X)38-SR-82,,TTY,,PHY) D411401100004 3(37-RB-0(P,X)38-SR-83-G,M+,TTY,,PHY) D411401100005 4(37-RB-0(P,X)38-SR-85-G,M+,TTY,,PHY) D411401100006 DECAY-DATA1(37-RB-86-G,18.66D,DG,1076.7,0.088) D411401100007 2(37-RB-82-G,1.273MIN,DG,776.5,0.134) D411401100008 3(38-SR-83-G,1.35D,DG,381.6,0.119, D411401100009 DG,762.7,0.30) D411401100010 4(38-SR-85-G,64.84D,DG,514.0,0.9927) D411401100011 RAD-DET (37-RB-82-G,DG) D411401100012 STATUS (TABLE) Numerical data were taken from author F.Ditroi D411401100013 HISTORY (20161103C) ST D411401100014 ENDBIB 12 0 D411401100015 NOCOMMON 0 0 D411401100016 DATA 5 10 D411401100017 EN DATA 1DATA 2DATA 3DATA 4 D411401100018 MEV GBQ/COUL GBQ/COUL GBQ/COUL GBQ/COUL D411401100019 69.6 3.4 3.9 170.2 2.2 D411401100020 66.5 3.1 3.6 160.2 2.0 D411401100021 62.8 2.7 3.2 148.3 1.9 D411401100022 59.6 2.4 2.9 137.1 1.7 D411401100023 56.0 2.1 2.4 126.1 1.6 D411401100024 52.4 1.8 1.8 115.1 1.5 D411401100025 48.4 1.4 1.2 103.3 1.3 D411401100026 43.9 1.1 0.6 87.7 1.1 D411401100027 39.4 0.7 0.13 65.1 0.8 D411401100028 34.3 0.3 0.001 33.6 0.5 D411401100029 ENDDATA 12 0 D411401100030 ENDSUBENT 29 0 D411401199999 ENDENTRY 11 0 D411499999999