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Association Euroatom – IPP.CR Nuclear Physics Institute Řež_________________________________________________________________________________________________
NPI Experimental Activities 2003-5 on IFMIF Neutronics
IEA International Workshop on Fusion Neutronics (23rd Symposium on Fusion Technology - SOFT)
September 21, 2004, Venice
P. Bém, V.Burjan, M.Götz, M.Honusek, V.Kroha, J.Novák E.Šimečková Nuclear Physics Institute Řež, CR
U. Fischer, U.v. Möllendorff, S.P. Simakov, FZ Karlsruhe B. Esposito, ENEA Frascati R.A. Forrest, UKAEA Culham J. Kopecky, JUKO Research
221.09.2004, Venice IEA IACP
NG2 target stationnegative ions, H(-) 18-37 MeV (20 μA), D(-) 11-18 MeV (10 μA)
NG1 target stationpositive ionsprotons 18-24 MeV deuterons 11-17 MeV3,4He-ions 20-40 MeV
U-120Mvariable-energy cyclotron K=40 two-mode of acceleration
NPI cyclotron-based Fast Neutron Facility
321.09.2004, Venice IEA IACP
neutron transport benchmark tests (IFMIF-like spectrum)
NG1 target station: source reaction 3He+D2O
0 5 10 15 20 25 30 35
107
108
109
[d(32MeV) + Li] x 0,015
[d(40MeV) + Li] x 0,015
3He (40MeV) + D2O
Spec
tral
Neu
tron
Yie
ld [
n/sr
/Mev
/C
]
Neutron Energy [MeV]
E(3He) 40 MeV
Ēn 14.1 MeV En ≤ 33.0 MeV FWHM 15o
well simulate d-Li source spectrum
421.09.2004, Venice IEA IACP
Ep 37 MeV
Ēn 13.9 MeV En ≤ 33.0 MeVFWHM 40o
Yn 4.4 x 1010 n/sr/s/μA Φn ≤ 3 x1011 n/cm2/s (5mm distance from the target)
0 10 20 30 40107
108
109
1010
D2O (p,xn)
0o
20o
40o
Sp
ectr
al N
eutr
on Y
ield
[ n
/sr/
MeV
/C
]
Neutron Energy [MeV]
0o
37 MeV
24 MeV
NG2 target station: source reaction p+D2O
activation benchmark tests (IFMIF-relevant energies)
521.09.2004, Venice IEA IACP
Ed 17 MeV
Ēn 8.3 MeV En ≤ 20 MeVFWHM 22 o
Yn 3.1 x 1010 n/sr/s/μA Φn ≤ 2 x1011 n/cm2/s (5mm distance from the target)
NG2 target station: source reaction d+D2O
0 10 20 30 40107
108
109
1010
10 deg 20 deg 40 deg
Sp
ectr
al N
eutr
on Y
ield
[ n
/sr/
MeV
/C ]
Neutron Energy [MeV]
Ed = 17.1 MeVD
2O (d,xn)
0 deg
activation benchmark tests (fusion-relevant energies)
621.09.2004, Venice IEA IACP
1 - U-120M cyclotron, 2 - beam guide and vacuum system, 3 - beam-diagnostic hardware 4 - quadrupole lenses 5 - beam-guide support 6 - target chamber of cooled heavy- water flow 7 - holder for irradiated samples
NG2 station: heavy-water target
■ negative-ion mode of acceleration (37 MeV protons, 18 MeV deuterons) ■ up to 20 μA, stable long-term operation at ≤ 5% fluctuation ■ flowing heavy-water target (beam-power dissipation up to kW) ■ collimator free beam-guide (no false neutron source) ► suitable for neutron activation experiments
721.09.2004, Venice IEA IACP
Neutron transport benchmark on iron IFMIF-like spectrum (TW3-TTMN-002, D6)
■ iron (the main constituent of the IMIF high-flux test module) ■ INPE/FZK evaluation- and LANL-150 iron data libraries■ 20 cm thick iron slab (0 and 20o)■ scintillation detector + pulse height technique ■ computational analysis at FZK (MCNP code and detailed three-dimensional geometry model of experiment0 5 10 15 20 25 30 35
10-3
10-2
10-1
Fe cylindrical slab (20 cm) irradiated with
D2O(3He,xn) source spectrum (40 MeV 3He)
= 20o
Experiment NPI Rez MCNP FZK/INPE-50 MCNP LANL-150
Spec
tral
Neu
tron
Yie
ld,
10
8 n/s
r/M
eV/
C
Neutron Energy, MeV
► good agreement observed for INPE/FZK evaluation► LANL-150 data overestimates calculations by up to 50% above 15 MeV
821.09.2004, Venice IEA IACP
Neutron transport benchmark on iron IFMIF-like spectrum (TW3-TTMN-002, D6b)
■ to account for the inelastic- scattering of neutrons ■ upgraded scintillator-detector hardware and double-conical neutron collimator assembly utilized ■ neutrons reliably determined above 0.7 MeV (twofold extending of energy range compared to previous data)
1 10105
106
107
108
109
Spec
tral
Neu
tron
Yie
ld [
n/sr
/MeV
/C
]
Neutron Energy [MeV]
Fe-disk d80shielded detector
Fe-disk
D2O( 3He,xn) source
Fe-disk d40collimated neutron beam
► computational analysis is under way at FZK
921.09.2004, Venice IEA IACP
0 5 10 15 20 25 30 3510-4
10-3
10-2
10-1
100
Neutron Energy, MeV
MCNPX
Bem et al. (2003)
Ed = 17 MeV, = 0o
McDeLicious
Spec
tral
Yie
ld,
10
10 n
/sr/
MeV
/C
Experimental verification of D-Li neutron yield at 17 MeV (TW3-TTMI-003/D6)
■ Li(d,xn) reaction, thick target energy spectra at 17.1 and 16.3 MeV (five angles)
■ computational analysisMCDeLi (semi-empirical d-Li model) MCDeLicious (evaluated d+6,7Li cross-section data) MCNPX (ISABEL (intra-nuclear cascade model)
► MCDeLicious predicts thick-target yield spectra + angle-dependent yield observables► all models fail to reproduce the structure of higher energy tail of spectra ► further revision of the d+ 6,7Li cross-section database needed
1021.09.2004, Venice IEA IACP
1 100,01
0,1
1
10
100
DD
CS
[mb/
sr/M
eV]
Neutron Energy [MeV]
= 15°
7Li(d,xn), Ed=17.1 MeV
Td=1.4 MeV
MCDeLicious,E
d=16.5 MeV
Experimental verification of D-Li neutron yield at 17 MeV (TW3-TTMI-003/D6)
■ 7Li(d,n) reaction at 17.1 MeV (eight angles) first time data on double-differential cross-section (DDCS)
MCDeLicious code ■ described well the deuteron break-up and compound nucleus excitation processes (low energy region) ■ fails to reproduce the structure corresponding the excitation of *Be
► present and recently published Tohoku University data on DDCS will be used at FZK to updating the d+ 6,7Li database
1121.09.2004, Venice IEA IACP
Activation experiment on CuCrZr at energies below 20 MeV (Underlying Technology 2003)
Na
24
Cr5
1
Mn
56
Co
61
Co
62
m
Ni6
5
Cu
64
Zr8
9
Zr9
5
0,1
1
Ca
lc.
/ E
xpt.
4
NPI d-BeTUD d-T
■ samples activated in the d+Be neutron source (consistency with previous investigations at FZK) ■ 9 activation products determined
■ C/E analysis by the Fispact code (with EAF 2003 data library)
► results agree with activation data from TUD (d+T neutron source)► indicate the need for investigation of discrepancies in the activation cross-section data ► further analysis in terms of upgraded EAF (improved model TALYS) is under way (R. A. Forrest)
1221.09.2004, Venice IEA IACP
Activation experiment on Eurofer-97IFMIF-like spectrum (TW3-TTMN-002, D6a)
■ the first activation experiment for Eu-97 steel in a white neutron field extending to 32 MeV ■ motivation: validation of IEAF-2001 cross-section data a continuation of activation experiments on SS-316 and F82H steels and vanadium alloys in FZ Karlsruhe ■ two independent runs (source-to-sample distance of 1.7 and 47.1 mm) ■ activated samples investigated by HPGe at 11 cooling times (from 0.5 to 102 days) ■ specific activities (Asp) at the end of irradiation in Bq/kg of Eurofer-97 determined
37 MeV protons
D2O Target(Ř30×26 mm2)
Activation Foils
1.7 mm 47 mm
► Resulting 22 activation products present the first integral benchmark data for the Eurofer steel at IFMIF-relevant neutron energies
1321.09.2004, Venice IEA IACP
10 1001E8
1E9
1E10
1E11p(37MeV) + D2O
Neu
tron
Flu
x [n
/µC
.cm
2 ]
x [mm]
27Al(n,)
24Na
d 20d 10 d 0
FZK[d(40MeV) +Li]5x5
Activation experiment on Eurofer-97Study of p-D2O neutron source spectrum
0 5 10 15 20 25 30 3510-3
10-2
10-1
100
p + D2O, E
p = 36 MeV
Rez Experiment
Neutron Energy, MeV
MCNPX/LA-150
= 0o
MCNPX/Model
Spec
tral
Neu
tron
Yie
ld,
1010
n/s
r/M
eV/
C
■ source spectra are measured at large distance (point-like geometry, PLG) ■ due to space and energy integration over target and foil dimensions the set-up can not be considered as the PLG (neutron flux dependence on distance does not follow 1/r2 law) ►correct calculations needed
■ due to identified discrepancy in LA-150h, MCNPX failed to represent the p+D2O source spectra
►spectral flux constructed by combining the measured and calculated (MCNPX) data and normalized by the 24Na activity (Al monitoring foils).
1421.09.2004, Venice IEA IACP
Comprehensive analysis performed at FZK by S.P.Simakov,
[Workshop on Activation Data, Prague, June 2004, CD]
Activation experiment on Eurofer-97the activation analysis
Na
24Sc
46
Sc 4
7Sc
48
V 4
8C
r 48
Cr
51M
n 52
Mn
54M
n 56
Fe 5
2Fe
59
Co
56C
o 57
Co
58C
o 60
Ni 5
7H
f 18
0mT
a 17
7T
a 18
0T
a 18
2T
a 18
3T
a 18
4W
18710-3
10-2
10-1
100
101
Distance from the D2O Target 47mm
C/E
Distance from the D2O Target 1.7mm
■ the activities in the Eu-97 steel predicted by the ALARA code with IEAF-2001 fail
■ the C/E ratios calculated for samples irradiated at 1.7 and 47.1 mm distance reasonably agree each other (proving experimental consistency)
► reasonable agreement found for half of the detected radio-nuclides ► large discrepancies for the others necessitate updating of the relevant IEAF-2001 cross sections (usually rely on theoretical model considerations not yet backed by cross section measurement for En above 15 MeV)
1521.09.2004, Venice IEA IACP
Current and next program
IFMIF white spectrum: Activation experiment on Tungsten (TW4-TTMN-002, D6, 2004) on Tantalum (TW5-TTMN-002, D6, 2005)
► continuing program of first time activation at IFMIF relevant energies► currently, W samples were irradiated, 15 activation products are investigated by two HPGe detectors► pre- and post- C/E analysis with the ALARA inventory code has been and will be done at FZK► neutron spectrum at the sample position will be determined by MCNP model calculations combined with experimental data from multi-foil activation-, scintillation- and proton-recoil spectrometry technique (1) to calibrate absolutely the spectral flux at sample position and (2) to renormalize previous activation experiments on Eu-97
1621.09.2004, Venice IEA IACP
Current and next program
Activation cross-section measurement (Underlying Technology 2005)
► development and testing the p(20-37 MeV) + Li (thin target) monoenergetic neutron source on the NG2 target station (high-current proton beam)► neutron spectrum from p+Li source at the sample position will be determined by MCNP model calculations combined with experimental data from multi-foil activation-, scintillation- and PRT technique ► to extend the EASY database above 20 MeV neutron energy for selected nuclides