ENTRY B0084 20160824 B025B008400000001 SUBENT B0084001 20160824 B025B008400100001 BIB 7 13 B008400100002 TITLE Excitation functions and yields of (d,a) reaction on B008400100003 natural molybdenum up to the deuteron energy of 13 MeVB008400100004 AUTHOR (Z.Randa, K.Svoboda) B008400100005 INSTITUTE (3CZRCZR) Inst. of Mineral Raw Materials, Kutna Hora B008400100006 (3CZRUJV) B008400100007 REFERENCE (J,ARI,28,555,1977) B008400100008 REL-REF (M,,Z.Randa+,J,IP,11,386,1975) Experimental details B008400100009 FACILITY (CYCLO,3CZRUJV) U-120 cyclotron B008400100010 HISTORY (19781031C) Lapf B008400100011 (19940707A) Some corrections included by CAJaD B008400100012 (19970923A) Reaction lines are corrected. B008400100013 (20011010U) Last checking has been done. B008400100014 (20160824A) On. 006-008 moved to D0822. 009-012 added. B008400100015 ENDBIB 13 0 B008400100016 NOCOMMON 0 0 B008400100017 ENDSUBENT 16 0 B008400199999 SUBENT B0084002 20160824 B025B008400200001 BIB 11 27 B008400200002 REACTION 1(42-MO-92(D,A)41-NB-90,,SIG) Stack 1 B008400200003 2(42-MO-92(D,A)41-NB-90,,SIG) Stack 2 B008400200004 SAMPLE 1Mo foils (17.82 mg/cm2 thick, >99% purity) and Al B008400200005 foils (3.02 mg/cm2 thick). B008400200006 2Mo foils (20.37 mg/cm2 thick) B008400200007 DECAY-DATA (41-NB-90-G,0.6083D,DG,139.7,0.75, B008400200008 DG,1128.,0.97, B008400200009 DG,2187.,0.14, B008400200010 DG,2319.,0.82) B008400200011 MONITOR 1(13-AL-27(D,X)11-NA-24,,SIG) B008400200012 MONIT-REF 1(B0099004,H.F.Roehm+,J,JIN,31,3345,1969) B008400200013 DETECTOR (GELI) Resolution 2.6 KeV (FWHM) At 1332.5 KeV B008400200014 METHOD (STTA) Energy loss was calculated by range and B008400200015 mass stopping power table by Williamson (1962). B008400200016 (BCINT) Faraday cup used in parallel with calorimetric B008400200017 determination and by means of monitor reaction B008400200018 1(ACTIV) 17.78 hr irradiation, E0=13.5 MeV, 3.4 uA B008400200019 (REC,MOSEP) B008400200020 2(ACTIV) 5.0 min irradiation, E0=12.0 MeV, 5.3 uA B008400200021 REL-REF (R,,C.Williamson+,R,CEA-2189,1962) B008400200022 Range and mass stopping power table given B008400200023 ERR-ANALYS Relative accuracy of cross section determination B008400200024 better than 10% except at highest and low energies B008400200025 where errors can amount to as much as 40%. B008400200026 STATUS (TABLE) Table 2 of Appl.Radiat.Isotopes 28(1977)555 B008400200027 HISTORY (20160824A) On. Thick target yields moved to 009; B008400200028 REACTION(SF4-SF5): -G,M+ deleted. B008400200029 ENDBIB 27 0 B008400200030 NOCOMMON 0 0 B008400200031 DATA 3 17 B008400200032 EN DATA 1DATA 2 B008400200033 MEV MB MB B008400200034 12.7 22.6 B008400200035 11.9 16.0 B008400200036 11.3 6.9 B008400200037 11.2 13.4 B008400200038 10.6 9.8 B008400200039 10.2 10.9 B008400200040 9.85 5.3 B008400200041 9.3 7.2 B008400200042 9.0 6.5 B008400200043 8.4 4.7 B008400200044 8.2 3.8 B008400200045 7.4 3.1 B008400200046 7.3 2.26 B008400200047 6.4 0.91 B008400200048 6.3 0.69 B008400200049 4.9 0.10 B008400200050 3.4 0.017 B008400200051 ENDDATA 19 0 B008400200052 ENDSUBENT 51 0 B008400299999 SUBENT B0084003 20160824 B025B008400300001 BIB 13 32 B008400300002 REACTION 1(42-MO-94(D,A)41-NB-92-M,,SIG) Stack 1 B008400300003 2(42-MO-94(D,A)41-NB-92-M,,SIG) Stack 2 B008400300004 SAMPLE 1Mo foils (17.82 mg/cm2 thick, >99% purity) and Al B008400300005 foils (3.02 mg/cm2 thick). B008400300006 2Mo foils (20.37 mg/cm2 thick) B008400300007 DECAY-DATA (41-NB-92-M,10.16D,DG,934.5,0.975) B008400300008 MONITOR 1(13-AL-27(D,X)11-NA-24,,SIG) B008400300009 MONIT-REF 1(B0099004,H.F.Roehm+,J,JIN,31,3345,1969) B008400300010 DETECTOR (GELI) Resolution 2.6 KeV (FWHM) At 1332.5 KeV B008400300011 METHOD (STTA) Energy loss was calculated by range and B008400300012 mass stopping power table by Williamson (1962). B008400300013 (BCINT) Faraday cup used in parallel with calorimetric B008400300014 determination and by means of monitor reaction B008400300015 1(ACTIV) 17.78 hr irradiation, E0=13.5 MeV, 3.4 uA B008400300016 (REC,MOSEP) B008400300017 2(ACTIV) 5.0 min irradiation, E0=12.0 MeV, 5.3 uA B008400300018 REL-REF (R,,C.Williamson+,R,CEA-2189,1962) B008400300019 Range and mass stopping power table given B008400300020 CORRECTION Contribution of (n,p) reaction was determined by B008400300021 activity of Mo foils placed beyond the deuteron B008400300022 range. B008400300023 CRITIQUE By KaChaPaG: B008400300024 Above ~7 MeV the 95Mo(d,a+n)92Nb even with larger B008400300025 abundance contributes increasingly. The values given B008400300026 in the DATA section have to be recorrected for the B008400300027 natural target. B008400300028 ERR-ANALYS Relative accuracy of cross section determination B008400300029 better than 10% except at highest and low energies B008400300030 where errors can amount to as much as 40%. B008400300031 STATUS (TABLE) Table 2 of Appl.Radiat.Isotopes 28(1977)555 B008400300032 HISTORY (20160824A) On. Thick target yields moved to 009. B008400300033 REACTION: SF1 changed from 42-MO-0, SF8=FCT deleted. B008400300034 ENDBIB 32 0 B008400300035 NOCOMMON 0 0 B008400300036 DATA 3 16 B008400300037 EN DATA 1DATA 2 B008400300038 MEV MB MB B008400300039 12.7 20.0 B008400300040 11.9 13.2 B008400300041 11.3 12.2 B008400300042 11.2 10.0 B008400300043 10.6 10.5 B008400300044 10.2 7.6 B008400300045 9.85 8.0 B008400300046 9.3 5.4 B008400300047 9.0 5.4 B008400300048 8.4 4.0 B008400300049 8.2 4.4 B008400300050 7.4 2.4 B008400300051 7.3 1.98 B008400300052 6.4 1.10 B008400300053 6.3 1.42 B008400300054 4.9 0.066 B008400300055 ENDDATA 18 0 B008400300056 ENDSUBENT 55 0 B008400399999 SUBENT B0084004 20160824 B025B008400400001 BIB 13 34 B008400400002 REACTION G(42-MO-97(D,A)41-NB-95-G,M-,SIG) B008400400003 M(42-MO-97(D,A)41-NB-95-M,,SIG) B008400400004 SAMPLE Mo foils (17.82 mg/cm2 thick, >99% purity) and Al B008400400005 foils (3.02 mg/cm2 thick). B008400400006 DECAY-DATAG(41-NB-95-G,35.0D,DG,765.8,1.00) B008400400007 M(41-NB-95-M,3.75D,DG,235.7,0.247) B008400400008 MONITOR (13-AL-27(D,X)11-NA-24,,SIG) B008400400009 MONIT-REF (B0099004,H.F.Roehm+,J,JIN,31,3345,1969) B008400400010 DETECTOR (GELI) Resolution 2.6 KeV (FWHM) At 1332.5 KeV B008400400011 METHOD (STTA) Energy loss was calculated by range and B008400400012 mass stopping power table by Williamson (1962). B008400400013 (BCINT) Faraday cup used in parallel with calorimetric B008400400014 determination and by means of monitor reaction B008400400015 (ACTIV) 17.78 hr irradiation, E0=13.5 MeV, 3.4 uA B008400400016 (REC,MOSEP) B008400400017 REL-REF (R,,C.Williamson+,R,CEA-2189,1962) B008400400018 Range and mass stopping power table given B008400400019 CORRECTION Contribution of (n,p) reaction was determined by B008400400020 activity of Mo foils placed beyond the deuteron B008400400021 range. B008400400022 Contribution of 95mNb production subtracted from the B008400400023 95gNb production cross section (amounts to ~20% of B008400400024 the primarily produced 95gNb). B008400400025 CRITIQUE By KaChaPaG: B008400400026 Above ~7 MeV the 98Mo(d,a+n)95Nb even with larger B008400400027 abundance contributes increasingly. The values given B008400400028 in the DATA section have to be recorrected for the B008400400029 natural target. B008400400030 ERR-ANALYS Relative accuracy of cross section determination B008400400031 better than 10% except at highest and low energies B008400400032 where errors can amount to as much as 40%. B008400400033 STATUS (TABLE) Table 2 of Appl.Radiat.Isotopes 28(1977)555 B008400400034 HISTORY (20160824A) On. Thick target yields moved to 009. B008400400035 REACTION: SF1 changed from 42-MO-0, SF8=FCT deleted. B008400400036 ENDBIB 34 0 B008400400037 NOCOMMON 0 0 B008400400038 DATA 3 9 B008400400039 EN DATA GDATA M B008400400040 MEV MB MB B008400400041 12.7 14.3 3.7 B008400400042 11.9 9.8 2.3 B008400400043 11.2 8.2 2.0 B008400400044 10.2 5.8 1.62 B008400400045 9.3 4.2 1.39 B008400400046 8.4 3.8 1.08 B008400400047 7.4 1.94 0.80 B008400400048 6.4 0.53 0.38 B008400400049 3.4 0.025 0.043 B008400400050 ENDDATA 11 0 B008400400051 ENDSUBENT 50 0 B008400499999 SUBENT B0084005 20160824 B025B008400500001 BIB 11 27 B008400500002 REACTION 1(42-MO-98(D,A)41-NB-96,,SIG) Stack 1 B008400500003 2(42-MO-98(D,A)41-NB-96,,SIG) Stack 2 B008400500004 SAMPLE 1Mo foils (17.82 mg/cm2 thick, >99% purity) and Al B008400500005 foils (3.02 mg/cm2 thick). B008400500006 2Mo foils (20.37 mg/cm2 thick) B008400500007 DECAY-DATA (41-NB-96,0.973D,DG,460.0,0.28, B008400500008 DG,569.1,0.59, B008400500009 DG,777.8,0.97, B008400500010 DG,1090.5,0.49, B008400500011 DG,1198.,0.21) B008400500012 MONITOR 1(13-AL-27(D,X)11-NA-24,,SIG) B008400500013 MONIT-REF 1(B0099004,H.F.Roehm+,J,JIN,31,3345,1969) B008400500014 DETECTOR (GELI) Resolution 2.6 KeV (FWHM) At 1332.5 KeV B008400500015 METHOD (STTA) Energy loss was calculated by range and B008400500016 mass stopping power table by Williamson (1962). B008400500017 (BCINT) Faraday cup used in parallel with calorimetric B008400500018 determination and by means of monitor reaction B008400500019 1(ACTIV) 17.78 hr irradiation, E0=13.5 MeV, 3.4 uA B008400500020 (REC,MOSEP) B008400500021 2(ACTIV) 5.0 min irradiation, E0=12.0 MeV, 5.3 uA B008400500022 REL-REF (R,,C.Williamson+,R,CEA-2189,1962) B008400500023 Range and mass stopping power table given B008400500024 ERR-ANALYS Relative accuracy of cross section determination B008400500025 better than 10% except at highest and low energies B008400500026 where errors can amount to as much as 40%. B008400500027 STATUS (TABLE) Table 2 of Appl.Radiat.Isotopes 28(1977)555 B008400500028 HISTORY (20160824A) On. Thick target yields moved to 009. B008400500029 ENDBIB 27 0 B008400500030 NOCOMMON 0 0 B008400500031 DATA 3 17 B008400500032 EN DATA 1DATA 2 B008400500033 MEV MB MB B008400500034 12.7 9.2 B008400500035 11.9 6.1 B008400500036 11.3 6.3 B008400500037 11.2 5.4 B008400500038 10.6 6.2 B008400500039 10.2 5.0 B008400500040 9.85 5.4 B008400500041 9.3 4.2 B008400500042 9.0 3.85 B008400500043 8.4 3.7 B008400500044 8.2 3.78 B008400500045 7.4 2.8 B008400500046 7.3 2.9 B008400500047 6.4 1.05 B008400500048 6.3 1.63 B008400500049 4.9 0.45 B008400500050 3.4 0.013 B008400500051 ENDDATA 19 0 B008400500052 ENDSUBENT 51 0 B008400599999 NOSUBENT B0084006 20160824 B025B008400600001 NOSUBENT B0084007 20160824 B025B008400700001 NOSUBENT B0084008 20160824 B025B008400800001 SUBENT B0084009 20160824 B025B008400900001 BIB 5 10 B008400900002 REACTION 1(42-MO-0(D,X)41-NB-90,,TTY,,PHY,DERIV) B008400900003 2(42-MO-0(D,X)41-NB-90,,TTY,,SAT,DERIV) B008400900004 ANALYSIS Integration of excitation function B008400900005 COMMENT By NDS (2016-08-24): B008400900006 Because R/Y=ln(2)/T in Eqs.(2-3) and R is introduced B008400900007 as the "saturation product rate", the Y ("thick B008400900008 target yield") was coded as the physical yield. B008400900009 (DEP,B0084002) Excitation function given B008400900010 STATUS (TABLE) Table 4 of Appl.Radiat.Isotopes 28(1977)555 B008400900011 HISTORY (20160824C) On. Moved from 002. Saturation yield added.B008400900012 ENDBIB 10 0 B008400900013 NOCOMMON 0 0 B008400900014 DATA 3 2 B008400900015 EN DATA 1DATA 2 B008400900016 MEV MUCI/MUAHR MUCI/MUA B008400900017 13.0 21.4 451. B008400900018 11.7 6.0 126. B008400900019 ENDDATA 4 0 B008400900020 ENDSUBENT 19 0 B008400999999 SUBENT B0084010 20160824 B025B008401000001 BIB 5 10 B008401000002 REACTION 1(42-MO-0(D,X)41-NB-92-M,,TTY,,PHY,DERIV) B008401000003 2(42-MO-0(D,X)41-NB-92-M,,TTY,,SAT,DERIV) B008401000004 ANALYSIS Integration of excitation function B008401000005 COMMENT By NDS (2016-08-24): B008401000006 Because R/Y=ln(2)/T in Eqs.(2-3) and R is introduced B008401000007 as the "saturation product rate", the Y ("thick B008401000008 target yield") was coded as the physical yield. B008401000009 STATUS (TABLE) Table 4 of Appl.Radiat.Isotopes 28(1977)555 B008401000010 (DEP,B0084003) Excitation function given B008401000011 HISTORY (20160824C) On. Moved from 003. Saturation yield added.B008401000012 ENDBIB 10 0 B008401000013 NOCOMMON 0 0 B008401000014 DATA 3 2 B008401000015 EN DATA 1DATA 2 B008401000016 MEV MUCI/MUAHR MUCI/MUA B008401000017 13.0 0.408 144. B008401000018 11.7 0.25 83. B008401000019 ENDDATA 4 0 B008401000020 ENDSUBENT 19 0 B008401099999 SUBENT B0084011 20160824 B025B008401100001 BIB 5 12 B008401100002 REACTION 1(42-MO-0(D,X)41-NB-95-G,M-,TTY,,PHY,DERIV) B008401100003 2(42-MO-0(D,X)41-NB-95-M,,TTY,,PHY,DERIV) B008401100004 3(42-MO-0(D,X)41-NB-95-G,M-,TTY,,SAT,DERIV) B008401100005 4(42-MO-0(D,X)41-NB-95-M,,TTY,,SAT,DERIV) B008401100006 ANALYSIS Integration of excitation function B008401100007 COMMENT By NDS (2016-08-24): B008401100008 Because R/Y=ln(2)/T in Eqs.(2-3) and R is introduced B008401100009 as the "saturation product rate", the Y ("thick B008401100010 target yield") was coded as the physical yield. B008401100011 STATUS (TABLE) Table 4 of Appl.Radiat.Isotopes 28(1977)555 B008401100012 (DEP,B0084004) Excitation function given B008401100013 HISTORY (20160824C) On. Moved from 004. Saturation yield added.B008401100014 ENDBIB 12 0 B008401100015 NOCOMMON 0 0 B008401100016 DATA 5 1 B008401100017 EN DATA 1DATA 2DATA 3DATA 4 B008401100018 MEV MUCI/MUAHR MUCI/MUAHR MUCI/MUA MUCI/MUA B008401100019 13. 0.089 0.245 108. 31.8 B008401100020 ENDDATA 3 0 B008401100021 ENDSUBENT 20 0 B008401199999 SUBENT B0084012 20160824 B025B008401200001 BIB 5 10 B008401200002 REACTION 1(42-MO-0(D,X)41-NB-96,,TTY,,PHY,DERIV) B008401200003 2(42-MO-0(D,X)41-NB-96,,TTY,,SAT,DERIV) B008401200004 ANALYSIS Integration of excitation function B008401200005 COMMENT By NDS (2016-08-24): B008401200006 Because R/Y=ln(2)/T in Eqs.(2-3) and R is introduced B008401200007 as the "saturation product rate", the Y ("thick B008401200008 target yield") was coded as the physical yield. B008401200009 STATUS (TABLE) Table 4 of Appl.Radiat.Isotopes 28(1977)555 B008401200010 (DEP,B0084005) Excitation function given B008401200011 HISTORY (20160824C) On. Moved from 005. Saturation yield added.B008401200012 ENDBIB 10 0 B008401200013 NOCOMMON 0 0 B008401200014 DATA 3 2 B008401200015 EN DATA 1DATA 2 B008401200016 MEV MUCI/MUAHR MUCI/MUA B008401200017 13.0 8.33 281. B008401200018 11.7 4.5 151. B008401200019 ENDDATA 4 0 B008401200020 ENDSUBENT 19 0 B008401299999 ENDENTRY 12 0 B008499999999