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