ENTRY A0934 20130129 A078A093400000001 SUBENT A0934001 20130129 A078A093400100001 BIB 11 40 A093400100002 TITLE Nuclear fission cross sections induced by deuterons of A093400100003 4 GeV. A093400100004 AUTHOR (S.Stoulos, W.Westmeier, R.Hashemi-Nezhad, A093400100005 M.Fragopoulou, A.Lagoyannis, M.Zamani) A093400100006 REFERENCE (J,PR/C,85,024612,2012) A093400100007 INSTITUTE (2GRCARU) A093400100008 (2GERGER) Institute fur Kernchemie, Philipps A093400100009 University, Marburg A093400100010 (3AULASY) A093400100011 (2GRCATH) A093400100012 FACILITY (ACCEL,4ZZZDUB) the Nuclotron accelerator, A093400100013 Joint Institute for Nuclear Research (JINR), Dubna. A093400100014 METHOD (SITA) A093400100015 SAMPLE Th-232, U-238, U-235, Bi-209 and Au-197 targets had a A093400100016 diameter of 1.2 cm. The mass of the radioactive targetsA093400100017 was measured using alpha and gamma spectrometry A093400100018 gamma spectrometry-(mug) A093400100019 Th-232 136+-6, U-238 95+-12, U-235 104+-6 A093400100020 alpha spectrometry(mug)- A093400100021 Th-232 target- Th-232 126+-6, U-238 7+-1, A093400100022 U-238 target- U-238 91+-7 A093400100023 U-235 target- U-238 less than 9, U-235 99+-14, A093400100024 U-234 1.3+-0.2 A093400100025 DETECTOR (TRD) The neutron distribution was studied on the A093400100026 paraffin moderator a long the target by using Solid A093400100027 State Nuclear Track Detectors A093400100028 ERR-ANALYS The uncertainties given for mass of the radioactive A093400100029 targets were estimated taking into account the A093400100030 contributions due to- A093400100031 (ERR-1).The error in the calibration of the source A093400100032 (ERR-2,2.,5.).The error in counting statistics A093400100033 (ERR-3).The error in ray intensity for gamma rays A093400100034 (ERR-4,2.,4.).The error in ray intensity for alpha raysA093400100035 (ERR-5).The error in mass of Th-232 A093400100036 (DATA-ERR).The uncertainty is reported by authors in A093400100037 table. A093400100038 HISTORY (20110315C) SB A093400100039 (20130129A) Correction was made according N.Otsuka A093400100040 remarks A093400100041 STATUS (TABLE).Table 3 of J,PR/C,85,024612,2012 A093400100042 ENDBIB 40 0 A093400100043 COMMON 4 3 A093400100044 EN ERR-1 ERR-3 ERR-5 A093400100045 GEV PER-CENT PER-CENT PER-CENT A093400100046 4. 3.7 1. 4. A093400100047 ENDCOMMON 3 0 A093400100048 ENDSUBENT 47 0 A093400199999 SUBENT A0934002 20130129 A078A093400200001 BIB 3 11 A093400200002 REACTION 1(92-U-235(D,F),,SIG) A093400200003 2((92-U-235(D,F),,SIG)/(90-TH-232(D,F),,SIG)) A093400200004 MONITOR (90-TH-232(D,F),,SIG) A093400200005 ERR-ANALYS (ERR-7).The error in target mass A093400200006 (ERR-8,17.,21.).The error in number of tracks Th-232, A093400200007 include the correction for fissions induced by A093400200008 backscattered neutrons and fissions induced by A093400200009 deuterons in impurities. A093400200010 (ERR-9,11.,17.).The error in number of tracks(target) A093400200011 (ERR-T,27.,30.).Overall uncertainty of cross section A093400200012 (MONIT-ERR).Error in monitor A093400200013 ENDBIB 11 0 A093400200014 COMMON 2 3 A093400200015 ERR-7 MONIT-ERR A093400200016 PER-CENT PER-CENT A093400200017 6. 17. A093400200018 ENDCOMMON 3 0 A093400200019 DATA 4 1 A093400200020 DATA 1DATA-ERR 1DATA 2DATA-ERR 2 A093400200021 MB MB NO-DIM NO-DIM A093400200022 1666. 430. 1.44 0.28 A093400200023 ENDDATA 3 0 A093400200024 ENDSUBENT 23 0 A093400299999 SUBENT A0934003 20130129 A078A093400300001 BIB 3 11 A093400300002 REACTION 1(92-U-238(D,F),,SIG) A093400300003 2((92-U-238(D,F),,SIG)/(90-TH-232(D,F),,SIG)) A093400300004 MONITOR (90-TH-232(D,F),,SIG) A093400300005 ERR-ANALYS (ERR-7).The error in target mass A093400300006 (ERR-8,9.,11.).The error in number of tracks Th-232, A093400300007 include the correction for fissions induced by A093400300008 backscattered neutrons and fissions induced by A093400300009 deuterons in impurities. A093400300010 (ERR-9,14.,21.).The error in number of tracks(target) A093400300011 (ERR-T,24.,29.).Overall uncertainty of cross section A093400300012 (MONIT-ERR).Error in monitor A093400300013 ENDBIB 11 0 A093400300014 COMMON 2 3 A093400300015 ERR-7 MONIT-ERR A093400300016 PER-CENT PER-CENT A093400300017 7. 17. A093400300018 ENDCOMMON 3 0 A093400300019 DATA 4 1 A093400300020 DATA 1DATA-ERR 1DATA 2DATA-ERR 2 A093400300021 MB MB NO-DIM NO-DIM A093400300022 1453. 350. 1.26 0.22 A093400300023 ENDDATA 3 0 A093400300024 ENDSUBENT 23 0 A093400399999 SUBENT A0934004 20130129 A078A093400400001 BIB 3 11 A093400400002 REACTION 1(83-BI-209(D,F),,SIG) A093400400003 2((83-BI-209(D,F),,SIG)/(90-TH-232(D,F),,SIG)) A093400400004 MONITOR (90-TH-232(D,F),,SIG) A093400400005 ERR-ANALYS (ERR-7,9.,12.).The error in target mass A093400400006 (ERR-8,11.,19.).The error in number of tracks Th-232, A093400400007 include the correction for fissions induced by A093400400008 backscattered neutrons and fissions induced by A093400400009 deuterons in impurities. A093400400010 (ERR-9,5.,7.).The error in number of tracks(target) A093400400011 (ERR-T,22.,28.).Overall uncertainty of cross section A093400400012 (MONIT-ERR).Error in monitor A093400400013 ENDBIB 11 0 A093400400014 COMMON 1 3 A093400400015 MONIT-ERR A093400400016 PER-CENT A093400400017 17. A093400400018 ENDCOMMON 3 0 A093400400019 DATA 4 1 A093400400020 DATA 1DATA-ERR 1DATA 2DATA-ERR 2 A093400400021 MB MB NO-DIM NO-DIM A093400400022 206. 46. 0.18 0.03 A093400400023 ENDDATA 3 0 A093400400024 ENDSUBENT 23 0 A093400499999 SUBENT A0934005 20130129 A078A093400500001 BIB 3 11 A093400500002 REACTION 1(79-AU-197(D,F),,SIG) A093400500003 2((79-AU-197(D,F),,SIG)/(90-TH-232(D,F),,SIG)) A093400500004 MONITOR (90-TH-232(D,F),,SIG) A093400500005 ERR-ANALYS (ERR-7,11.,15.).The error in target mass A093400500006 (ERR-8,13.,19.).The error in number of tracks Th-232, A093400500007 include the correction for fissions induced by A093400500008 backscattered neutrons and fissions induced by A093400500009 deuterons in impurities. A093400500010 (ERR-9,5.,7.).The error in number of tracks(target) A093400500011 (ERR-T,24.,29.).Overall uncertainty of cross section A093400500012 (MONIT-ERR).Error in monitor A093400500013 ENDBIB 11 0 A093400500014 COMMON 1 3 A093400500015 MONIT-ERR A093400500016 PER-CENT A093400500017 17. A093400500018 ENDCOMMON 3 0 A093400500019 DATA 4 1 A093400500020 DATA 1DATA-ERR 1DATA 2DATA-ERR 2 A093400500021 MB MB NO-DIM NO-DIM A093400500022 92. 23. 0.08 0.02 A093400500023 ENDDATA 3 0 A093400500024 ENDSUBENT 23 0 A093400599999 SUBENT A0934006 20130129 A078A093400600001 BIB 2 7 A093400600002 REACTION (90-TH-232(D,F),,SIG) A093400600003 ERR-ANALYS (ERR-7,9.,21.).The error in number of tracks Th-232, A093400600004 include the correction for fissions induced by A093400600005 backscattered neutrons and fissions induced by A093400600006 deuterons in impurities. A093400600007 (ERR-T,19.,27.).Overall uncertainty of cross section A093400600008 (ERR-6).The error in beam fluence A093400600009 ENDBIB 7 0 A093400600010 COMMON 1 3 A093400600011 ERR-6 A093400600012 PER-CENT A093400600013 9. A093400600014 ENDCOMMON 3 0 A093400600015 DATA 2 1 A093400600016 DATA DATA-ERR A093400600017 MB MB A093400600018 1153. 198. A093400600019 ENDDATA 3 0 A093400600020 ENDSUBENT 19 0 A093400699999 ENDENTRY 6 0 A093499999999