Multiple hydrogen trapping by vacancies: Its impact on defect dynamics and hydrogen retention in tungsten
|
|
- Ross Nash
- 6 years ago
- Views:
Transcription
1 2014 Joint ICTP-IAEA Conference on Models and Data for Plasma-Material Interaction in Fusion Devices, 3 7 November 2014, International Centre for Theoretical Physics (ICTP), Trieste, Italy. Multiple hydrogen trapping by vacancies: Its impact on defect dynamics and hydrogen retention in tungsten D. Kato a,b, H. Iwakiri c, Y. Watanabe d, K. Morishita e, T. Muroga a,b, N. Fernandez f, A. Allouche f, and Y. Ferro f a National Institute for Fusion Science (NIFS), Toki, Gifu , Japan b The Graduate University for Advanced Studies (SOKENDAI), Toki, Gifu , Japan c University of the Ryukyus, Okinawa , Japan d Japan Atomic Energy Agency (JAEA), Rokkasho, Aomori , Japan e Institute of Advanced Energy, Kyoto University, Ui, Kyoto , Japan f Aix-Marseille University, CNRS, PIIM UMR 7345, Marseille, France 2014/11/05 ICTP-IAEA@Trieste 1
2 Acknowledgments This work has been performed in the period of IAEA-CRP Data for Surface Composition Dynamics Relevant to Erosion Processes ( ), and MEXT Grand-in-Aid Scientific Research in Priority Areas Tritium for Fusion ( ) (Chair: Tetsuo Tanabe). DK is grateful to supports by KAKENHI ( ), Joint Usage/Research Program on Zero-Emission Energy Research (Institute of Advanced Energy, Kyoto University, ZE26A-8), and NIFS/NINS under the proect of Formation of International Scientific Base and Network. 2014/11/05 2
3 contents Introduction: Super-saturation of H in W under high-flux divertor plasma irradiation Di-vacancies formation in W under hydrogen rich condition [D. Kato et al., J. Nucl. Mater. 417 (2011) 1115] C impurity diffusion interacting with ambient H in W [D. Kato et al., Plasma and Fusion Research: Regular Article, Vol. 6 (2011) ] Summary 2014/11/05 ICTP-IAEA@Trieste 3
4 D/T retention in W Fusion power output ~3GW DT fusion reaction ~ a few % FBR~0.1 1 dpa 100 D T microstructure codeposit n ~10 21 n/s blanket ~10 21 T/s TBR > 1 diffusion limit wall saturation (ITER divertor incident particles) ~10 24 T/s No experimental knowledge He /m 2 fluence /m 2 T invetory increase (Wall pumping) thermal diffusion deep and trapped inside (square root of incident fluence) codeposition with sputtered particles (low T, linearly increase with fluence) microstructure develop (T dependence?, fluence dependence?) Reemission character Optimal operation temperature window 2014/11/05 ICTP-IAEA@Trieste 4
5 ITER divertor ITER first-wall D trap concentration in damaged W Surrogate ion experiments Radiation effects depend on character of defects. Scaling with dpa has large uncertainty. PKA energy dependence 300 kev H 12 MeV Si DEMO:10 dpa Power plant:100 dpa Whyte, ITPA (2008) Ueda (Osaka Univ.) 2014/11/05 ICTP-IAEA@Trieste 5
6 Super-saturation of H concentration by high-flux plasma irradiation Fractional concentration of H at the surface is estimated in steady state of incident flux ϕ in = /m 2 /s. in f in 2 k r C s C s f in k r Anderl s data (Fus. Tech. v.21, 745, 1992) for recombination coefficients k r, 1 kev D + ion, Frauenfelder s diffusivity is used. Reflection coefficient (TRIM.SP) 0.76~0.98@10 ev (f=1e-1~1e-2); t Hoen et al. PRL 111, 2013, f = 1e-5~1e-7@5 ev. H solubility in W under high H pressure calculated by Sugimoto&Fukai (Acta Metall. Mater. v.40, 2327, 1992) 2014/11/05 ICTP-IAEA@Trieste 6
7 Super-saturated D and blistering (D/C mixed irradiation) Temperature dependence of D/W fraction on surfaces Peng, Ueda, JNM 2013 D/C mixed irradiation increase D concentration 10-4 Zakharov Blistering on W surfaces by D/C mixed irradiation. (No blistering observed with D only) 10-6 Frauenfelder 2014/11/05 ICTP-IAEA@Trieste 7
8 New vacancy creation under super-saturated hydrogen condition Wright, 18 th PSI (May, 2008) Implanted D super-saturates The implantation zone. W atom is displaced and a vacancy is formed. Vacancy clustering and void/blister formation What experimental factors influence strength and formation of stress fields? Plasma flux density sets rate of implantation (source) Hydrogenic solubility sets saturation limit (boundary condition) Diffusion/surface recombination rate-limiting process removes D from implantation zone (sink) /11/05 ICTP-IAEA@Trieste
9 Super abundant vacancy creation in the form of VH complex Statistical thermodynamics model proposed by Fukai extended to evaluate concentration of each complex. x xi xt N N exp f kt, f VH x N W x f ( T ) e (VH i f i t f f ( T ) e (H) f f i H l ) 6 N W, x, 3 l h l 2 3 (H) x x V0 V exp 0 x f V kt 06 f : formation free energies h l 2 (VH ) ktln 1 exp ktln 1 exp h (H) l h kt 1,6,3,4,12,6,1 (VH ) l kt Collaboration with Y.Ferro, N.Fernandez f 0 f 0 f f ( T 0) 0 f V 3.25 ev 2014/11/05 ICTP-IAEA@Trieste 9
10 2014/11/05 10
11 contents Introduction: Super-saturation of H in W under high-flux divertor plasma irradiation Di-vacancies formation in W under hydrogen rich condition [D. Kato et al., J. Nucl. Mater. 417 (2011) 1115] C impurity diffusion interacting with ambient H in W [D. Kato et al., Plasma and Fusion Research: Regular Article, Vol. 6 (2011) ] Summary 2014/11/05 ICTP-IAEA@Trieste 11
12 In order to investigate influence of ambient hydrogen atoms on coalescence of vacancy clusters, di-vacancy formation associated with hydrogen trapping is studied from first-principles. 2 nd nearest-neighbor (2NN) V 1 st nearest-neighbor (1NN) 3 rd nearest-neighbor (3NN) 2014/11/05 ICTP-IAEA@Trieste 12
13 Equilibrium states of V 2 H complex Relaxation of ionic configuration and cell shape for constant volumes Blue: W Red: H Energy-volume curve Fitting to Birch-Murnaghan s equation of states Equilibrium total-energy, volume, bulk modulus y x z Image of equilibrium configuration of V 2 H cluster in bcc tungsten crystal GGA-PBE DFT calculation using VASP code. A reference bcc super-cell containing 128 tungsten atoms (periodic boundary condition) shifted k-point grid of the Monkhorst-Pack scheme. Plane wave cut-off energy of 300 ev. Numerical convergence < 10 mev. Configuration (ion and cell-shape) relaxation using conugate gradient method (force per atom < 20 mev/å). 2014/11/05 ICTP-IAEA@Trieste 13
14 Surface-energy correction of vacancy formation energy in W 1NN Surface of electronic void 2NN 3NN Di-vacancies S Numerical data for ellium model [S. Kurth, J. P. Perdew, P. Blaha, Int. J. Quantum Chem. 75 (1999) 889.] are adopted; ev/å 2 for Wigner- Seitz radius r s =1.62 corresponding to an electron density of bulk W. w/o surface-energy correction e f(3nn) 2 e f(v) < e f(1nn) < e f(2nn) Ω f(1nn) > Ω f(3nn) 2 Ω f(v) > Ω f(2nn) Surface-energy correction Δe f = S ε PBE-ellium (= ev/å 2 ) S 1NN S 2NN < S 3NN 2 S V Δe f(1nn) Δe f(2nn) < Δe f(3nn) 2 Δe f(v) TABLE: Vacancy formation energy (e f ), formation volume (Ω f ), and binding energy (e b ). V: mono-vacancy, V 2 (1NN): the first nearrestneighbor di-vacancy, V 2 (2NN): the second one, V 2 (3NN): the third one. Bold represents present results (numbers in parentheses are the results w/o correction). V V 2 (1NN) V 2 (2NN) V 2 (3NN) e f (ev) Ω f (Å 3 ) e b (ev) 3.68 (3.17) a 3.56 b 3.6 c 12.4 c 3.95 e (6.50) 6.71 b 7.06 c 7.32 e 7.63 (6.81) 6.93 b 6.42 c 7.36 e 7.48 (6.47) 7.32 c c c c (-0.16) b c +0.7 d e g h (-0.47) b c e g h (-0.13) c a)landolt-börnstein data-book, b)dft-gga (PLATO), c)johnson s model potential, d)experimental (FIM), e)modified embedded atom model, f)kittle s text, g)tight-binding 2014/11/05 Δe b(1nn) Δe b(2nn) ICTP-IAEA@Trieste > Δe b(3nn) 0 methods, h)def-gga(pbe) by Ventelon et al. 14
15 Hydrogen trapping effect on di-vacancy formation in W V 2 H complex binds with H stronger than VH A nucleus of larger vacancy clusters 1NN 2V apparent binding energy ~0.7 ev 2NN DFT potential energy surface of H Binding energy of single hydrogen atom to V ev for 1NN at an octahedral site. 2.1 ev for 2NN at the center of a line connecting two vacancies. (Binding energy to V is 1.4 ev) 2014/11/05 Hydrogen effect in formation energies of V 2 and V 2 H in tungsten for 1NN and 2NN configurations. Other DFT results (triangles, L.Ventelon 2012) using AM05 functional optimized to vacancy calculations are also plotted for comparison. Dotted line indicates an experimental value obtained by field ion microscopy (FIM, J.Y.Park 1983). ICTP-IAEA@Trieste 15
16 Multiple-hydrogen trapping of V 2 is not studied in present work. Theoretical studies on the multiple trapping by V 2 have been reported for C atoms in a bcc Fe [C.J. Först et al., Phys. Rev. Lett. 96 (2006) ]; lower formation energies were obtained for V 2 trapping more C atoms. This suggests that the multiple-hydrogen trapping may also assist the V 2 formation more efficiently. C.J. Först et al., Phys. Rev. Lett. 96 (2006) /11/05 ICTP-IAEA@Trieste 16
17 contents Introduction: Super-saturation of H in W under high-flux divertor plasma irradiation Di-vacancies formation in W under hydrogen rich condition [D. Kato et al., J. Nucl. Mater. 417 (2011) 1115] C impurity diffusion interacting with ambient H in W [D. Kato et al., Plasma and Fusion Research: Regular Article, Vol. 6 (2011) ] Summary 2014/11/05 ICTP-IAEA@Trieste 17
18 SIMS yield C impurity level in SC-W surface increases significantly after D ion implantation. C impurity plays a primary role to explain D retention characteristics. Depth (nm) Depth profile indicates the impurity atoms diffuse into W as deep as D. Impurity levels are apparently increased into 90 nm deep (much longer than intrinsic diffusion lengths of the impurity atoms). Ion energy: 1.5 kev D 3 + (500 ev /D) Flux: 5-6x10 19 /m 2 s Poon et al., JNM (2003) 2014/11/05 ICTP-IAEA@Trieste 18
19 Strong repulsion with dissolved C atom W C H E B ( C-H) EF(C) EF(H) EF(C H) 2014/11/05 ICTP-IAEA@Trieste 19
20 Activation enthalpy, entropy of vibration, and hopping frequency. o-c: an isolated interstitial C, o- C/t-H: an interstitial C-H pair. ΔE (ev) ΔS vib /k B ν (THz) o-c o-c/t-h Jumping rate [/s]: Γ exp S k exp E k T, vib (D. Kato et al., PFR: Regular Article, 2011) B B 2014/11/05 ICTP-IAEA@Trieste 20
21 x Γ x Γ Γ H 0, 2 3 2, W * Γ a D x D D Theoretical evaluation of ambient hydrogen effect /11/05 ICTP-IAEA@Trieste
22 Hydrogen effect on diffusion length of C Diffusion length ratio, L * /L 0 = (D * /D 0 ) 1/2, of an interstitial C in W crystal. L 0 is the diffusion length of an isolated C, L * with 5 at% ambient H concentration. 2014/11/05 ICTP-IAEA@Trieste (D. Kato et al., PFR, 2011) 22
23 Volume diffusion coefficients of C in W single-crystal Interstitial diffusion coefficients of C in the bulk W crystal. Two experimental values of volume diffusion coefficients, which were measured with single-crystal W samples, are also plotted for comparison. 2014/11/05 ICTP-IAEA@Trieste (D. Kato et al., PFR, 2011) 23
24 Summary Super-saturated H is anticipated in W under high-flux divertor plasma irradiation, and gives influence on defect dynamics and concurrently H/D/T retention. Multiscale modeling of the super-saturated H effects is important for a better characterization of defects in divertor of ITER and DEMO. Remarkable effects of H on di-vacancy formation and C impurity diffusion in W are predicted from first-principles based on DFT calculations. Di-vacancy formation is facilitated by trapping H. Calculated formation energy of V 2 H complex coincides to an experimental measurement. Interstitial diffusion of dissolved C in W is enhanced by repulsive interaction with ambient H. Diffusion length increases almost 10 times at low temperatures assuming 5 at% H in W. 2014/11/05 ICTP-IAEA@Trieste 24
Comparison of deuterium retention for ion-irradiated and neutronirradiated
13th International Workshop on Plasma-Facing Materials and Components for Fusion Applications / 1st International Conference on Fusion Energy Materials Science Comparison of deuterium retention for ion-irradiated
More informationImplantation Energy Dependence on Deuterium Retention Behaviors for the Carbon Implanted Tungsten
J. Plasma Fusion Res. SERIES, Vol. 10 (2013) Implantation Energy Dependence on Deuterium Retention Behaviors for the Carbon Implanted Tungsten Yasuhisa Oya 1) *, Makoto Kobayashi 1), Naoaki Yoshida 2),
More informationUnique phenomena of tungsten associated with fusion reactor: uncertainties of stable hydrogen configuration tapped in tungsten vacancy
Unique phenomena of tungsten associated with fusion reactor: uncertainties of stable hydrogen configuration tapped in tungsten vacancy Kyushu University Kazuhito Ohsawa Technical Meeting of the International
More informationMultiscale modelling of D trapping in W
CMS Multiscale modelling of D trapping in W Kalle Heinola, Tommy Ahlgren and Kai Nordlund Department of Physics and Helsinki Institute of Physics University of Helsinki, Finland Contents Background Plasma-wall
More informationH trapping and migra6on in tungsten: a DFT inves6ga6on that includes temperature dependency
H trapping and migra6on in tungsten: a DFT inves6ga6on that includes temperature dependency Yves Ferro, Nicolas Fernandez Physique des Interac2ons Ioniques et Moléculaires (PIIM) Aix- Marseille Université
More informationSCIENCE CHINA Physics, Mechanics & Astronomy
SCIENCE CHINA Physics, Mechanics & Astronomy Article April 2012 Vol.55 No.4: 614 618 doi: 10.1007/s11433-012-4679-8 Stability and diffusion properties of self-interstitial atoms in tungsten: a first-principles
More informationJ. Boisse 1,2, A. De Backer 1,3, C. Domain 4,5, C.S. Becquart 1,4
MODELLING SELF TRAPPING AND TRAP MUTATION IN TUNGSTEN USING DFT AND MOLECULAR DYNAMICS WITH AN EMPIRICAL POTENTIAL BASED ON DFT J. Boisse 1,2, A. De Backer 1,3, C. Domain 4,5, C.S. Becquart 1,4 1 Unité
More informationStudies on bi-directional hydrogen isotopes permeation through the first wall of a magnetic fusion power reactor
Studies on bi-directional hydrogen isotopes permeation through the first wall of a magnetic fusion power reactor IAEA-CRP Plasma-Wall Interaction with Reduced Activation Steel Surfaces in Fusion Devices
More informationMolecular Dynamics Study of Plasma Surface Interactions for Mixed Materials
J. Plasma Fusion Res. SERIES, Vol. 9 () Molecular Dynamics Study of Plasma Surface Interactions for Mixed Materials Kaoru OHYA, Naohide MOHARA, Kensuke INAI, Atsushi ITO, Hiroaki NAKAMURA, Yoshio UEDA
More informationBridging model and real systems with laboratory experiments: dynamic retention of deuterium in tungsten
dynamic retention of deuterium in tungsten PIIM laboratory Aix-Marseille Université - CNRS Marseille, France Régis Bisson summary of common laboratory experiments same parameters, similar retention but
More informationPerformance of MAX phase Ti 3 SiC 2 under the irradiation of He/H :
Performance of MAX phase Ti 3 SiC 2 under the irradiation of He/H : Elaboration from DFT Yuexia Wang Institute of Modern Physics Fudan University Hefei-2016 Materials Issues Neutron flux (14MeV, 0.5-0.8
More informationAvailable online at ScienceDirect. Physics Procedia 71 (2015 ) 30 34
Available online at www.sciencedirect.com ScienceDirect Physics Procedia 71 (2015 ) 30 34 18th Conference on Plasma-Surface Interactions, PSI 2015, 5-6 February 2015, Moscow, Russian Federation and the
More informationJoint ICTP-IAEA Workshop on Fusion Plasma Modelling using Atomic and Molecular Data January 2012
2327-3 Joint ICTP-IAEA Workshop on Fusion Plasma Modelling using Atomic and Molecular Data 23-27 January 2012 Qunatum Methods for Plasma-Facing Materials Alain ALLOUCHE Univ.de Provence, Lab.de la Phys.
More informationJoint ICTP-IAEA Workshop on Physics of Radiation Effect and its Simulation for Non-Metallic Condensed Matter.
2359-3 Joint ICTP-IAEA Workshop on Physics of Radiation Effect and its Simulation for Non-Metallic Condensed Matter 13-24 August 2012 Electrically active defects in semiconductors induced by radiation
More informationModelling diffusion processes of deuterium in tungsten
Modelling diffusion processes of deuterium in tungsten H. Wierenga June 17, 2013 Supervisors: Dr. P.A. Zeijlmans van Emmichoven M.H.J. t Hoen MSc Utrecht University Physics Princetonplein 5 3584 CC Utrecht
More informationHelium effects on Tungsten surface morphology and Deuterium retention
1 Helium effects on Tungsten surface morphology and Deuterium retention Y. Ueda, H.Y. Peng, H. T. Lee (Osaka University) N. Ohno, S. Kajita (Nagoya University) N. Yoshida (Kyushu University) R. Doerner
More informationComparisons of DFT-MD, TB- MD and classical MD calculations of radiation damage and plasmawallinteractions
CMS Comparisons of DFT-MD, TB- MD and classical MD calculations of radiation damage and plasmawallinteractions Kai Nordlund Department of Physics and Helsinki Institute of Physics University of Helsinki,
More informationIn-vessel Tritium Inventory in ITER Evaluated by Deuterium Retention of Carbon Dust
FT/P1-19 In-vessel Tritium Inventory in ITER Evaluated by Deuterium Retention of Carbon Dust T. Hino 1), H. Yoshida 1), M. Akiba 2), S. Suzuki 2), Y. Hirohata 1) and Y. Yamauchi 1) 1) Laboratory of Plasma
More informationComparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices
Comparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices G.M. Wright 1, D. Brunner 1, M.J. Baldwin 2, K. Bystrov 3, R. Doerner 2, B. LaBombard 1, B. Lipschultz 1, G. de Temmerman 3,
More informationMolecular Dynamics Simulation of Chemical Sputtering of Hydrogen Atom on Layer Structured Graphite
1 TH/7-1 Molecular Dynamics Simulation of Chemical Sputtering of Hydrogen Atom on Layer Structured Graphite A. Ito 1,2), Y. Wang 1), S. Irle 1), K. Morokuma 3), and H. Nakamura 2) 1) Nagoya University,
More informationMolecular Dynamics Simulations of Fusion Materials: Challenges and Opportunities (Recent Developments)
Molecular Dynamics Simulations of Fusion Materials: Challenges and Opportunities (Recent Developments) Fei Gao gaofeium@umich.edu Limitations of MD Time scales Length scales (PBC help a lot) Accuracy of
More informationDesign window analysis of LHD-type Heliotron DEMO reactors
Design window analysis of LHD-type Heliotron DEMO reactors Fusion System Research Division, Department of Helical Plasma Research, National Institute for Fusion Science Takuya GOTO, Junichi MIYAZAWA, Teruya
More informationTime accelerated Atomic Kinetic Monte Carlo for radiation damage modelling
PERFORM 60 FP7 Project Time accelerated Atomic Kinetic Monte Carlo for radiation damage modelling C. Domain, C.S. Becquart, R. Ngayam-Happy EDF R&D Dpt Matériaux & Mécanique des Composants Les Renardieres,
More informationComputer-Simulation Studies of Plasma- Surface Interactions
Computer-Simulation Studies of Plasma- Surface Interactions T. Ono ) Collabrators: T. Kawamura 2), T. Muramoto ), S.T. Nakagawa ), T. Kenmotsu 3) ) Okayama Univ. of Science, - Ridai-cho, Okayama 700-0005,
More informationApplications of First-Principles Method in Studying Fusion Materials
Joint ICTP/CAS/IAEA School & Workshop on Plasma-Materials Interaction in Fusion Devices, July 18-22, 2016, Hefei Applications of First-Principles Method in Studying Fusion Materials by Guang-Hong LU (
More informationExperience with Moving from Dpa to Changes in Materials Properties
Experience with Moving from Dpa to Changes in Materials Properties Meimei Li, Argonne National Laboratory N. V. Mokhov, Fermilab 46 th ICFA Advanced Beam Dynamics Workshop Sept. 27 Oct. 1, 2010 Morschach,
More informationMolecular dynamics simulations of the clustering and dislocation loop punching behaviors of noble gas atoms in tungsten
Molecular dynamics simulations of the clustering and dislocation loop punching behaviors of noble gas atoms in tungsten J.Z.Fang, F.Zhou, H.Q.Deng, X.L.Gan, S.F.Xiao, W.Y.Hu Hunan University Contents I,
More informationFundamental science and synergy of multi-species surface interactions in high-plasma--flux environments
Fundamental science and synergy of multi-species surface interactions in high-plasma--flux environments Our thanks to John Hogan Managed by UT-Battelle for the Department of Energy ReNew PMI, UCLA, March
More informationPISCES W fuzz experiments: A summary of work up to now.
FNST/PFC/MASCO meeting, UCLA Aug. 2-6, 2010 W fuzz experiments: A summary of work up to now. M.J. Baldwin, R.P. Doerner, D. Nishijima University of California, San Diego, USA Why do we care about fuzz?
More informationComparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices!
Comparison of tungsten fuzz growth in Alcator C-Mod and linear plasma devices G.M. Wright 1, D. Brunner 1, M.J. Baldwin 2, K. Bystrov 3, R. Doerner 2, B. LaBombard 1, B. Lipschultz 1, G. de Temmerman 3,
More informationNeutron Testing: What are the Options for MFE?
Neutron Testing: What are the Options for MFE? L. El-Guebaly Fusion Technology Institute University of Wisconsin - Madison http://fti.neep.wisc.edu/uwneutronicscenterofexcellence Contributors: M. Sawan
More informationFirst Principles Calculation of Defect and Magnetic Structures in FeCo
Materials Transactions, Vol. 47, No. 11 (26) pp. 2646 to 26 Special Issue on Advances in Computational Materials Science and Engineering IV #26 The Japan Institute of Metals First Principles Calculation
More informationModelling of radiation damage in tungsten including He production
Modelling of radiation damage in tungsten including He production C.S. Becquart 1, C. Domain 2 A. De Backer 1 M.F. Barthe 3 M. Hou 4, C. Ortiz 5 1 Unité Matériaux Et Techniques, UMET, UMR 8207, Villeneuve
More information31704 Dynamic Monte Carlo modeling of hydrogen isotope. reactive-diffusive transport in porous graphite
31704 Dynamic Monte Carlo modeling of hydrogen isotope reactive-diffusive transport in porous graphite * R. Schneider a, A. Rai a, A. Mutzke a, M. Warrier b,e. Salonen c, K. Nordlund d a Max-Planck-Institut
More informationParticle Pinch Model of Passing/Trapped High-Z Impurity with Centrifugal Force Effect )
Particle Pinch Model of Passing/Trapped High-Z Impurity with Centrifugal Force Effect ) Yusuke SHIMIZU, Takaaki FUJITA, Atsushi OKAMOTO, Hideki ARIMOTO, Nobuhiko HAYASHI 1), Kazuo HOSHINO 2), Tomohide
More informationChemical Erosion and Critical Issues for ITER
Chemical Erosion and Critical Issues for ITER J. Roth Max-Planck-Institut für Plasmaphysik, Garching Chemical Erosion Studies Erosion yields: Dependence on temperature, energy and flux Emitted hydrocarbons
More informationAtomic and Molecular Data Activities for Fusion Research in JAEA. T. Nakano Japan Atomic Energy Agency
"Technical Aspects of Atomic and Molecular Data Processing and Exchange" (20th Meeting of the Atomic and Molecular Data Centres and ALADDIN Network), 7-9 September 2009, IAEA HQ, Vienna, Austria Atomic
More informationSputtering Yield of Noble Gas Irradiation onto Tungsten Surface
J. Adv. Simulat. Sci. Eng. Vol. 3, No. 2, 165 172. c 2016 Japan Society for Simulation Technology Sputtering Yield of Noble Gas Irradiation onto Tungsten Surface Hiroaki Nakamura 1,2,*, Seiki Saito 3,
More informationDefects in TiO 2 Crystals
, March 13-15, 2013, Hong Kong Defects in TiO 2 Crystals Richard Rivera, Arvids Stashans 1 Abstract-TiO 2 crystals, anatase and rutile, have been studied using Density Functional Theory (DFT) and the Generalized
More informationAtomistic simulations on the mobility of di- and tri-interstitials in Si
Atomistic simulations on the mobility of di- and tri-interstitials in Si related publications (since 2001): Posselt, M., Gao, F., Zwicker, D., Atomistic study of the migration of di- and tri-interstitials
More informationModelling of JT-60U Detached Divertor Plasma using SONIC code
J. Plasma Fusion Res. SERIES, Vol. 9 (2010) Modelling of JT-60U Detached Divertor Plasma using SONIC code Kazuo HOSHINO, Katsuhiro SHIMIZU, Tomonori TAKIZUKA, Nobuyuki ASAKURA and Tomohide NAKANO Japan
More information1 EX/P4-8. Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device
1 EX/P4-8 Hydrogen Concentration of Co-deposited Carbon Films Produced in the Vicinity of Local Island Divertor in Large Helical Device T. Hino 1,2), T. Hirata 1), N. Ashikawa 2), S. Masuzaki 2), Y. Yamauchi
More informationApplication of atomic data to quantitative analysis of tungsten spectra on EAST tokamak
Technical Meeting on Uncertainty Assessment and Benchmark Experiments for Atomic and Molecular Data for Fusion Applications, 19-21 December 2016, Vienna, Austria Application of atomic data to quantitative
More informationTHE DEPTHS OF HYDROGEN AND HELIUM BUBBLES IN TUNGSTEN: A COMPARISON
THE DEPTHS OF HYDROGEN AND HELIUM BUBBLES IN TUNGSTEN: A COMPARISON K. O. E. HENRIKSSON,* K. NORDLUND, A. KRASHENINNIKOV, and J. KEINONEN University of Helsinki, Accelerator Laboratory, P.O. Box 43, FI-00014
More informationEROSION AND DEPOSITION MECHANISMS IN FUSION PLASMAS. A. Kirschner
EROSION AND DEPOSITION MECHANISMS IN FUSION PLASMAS A. Kirschner Institut für Energieforschung (Plasmaphysik), Forschungszentrum Jülich GmbH, Association EURATOM-FZJ, Trilateral Euregio Cluster, 52425
More informationSnO 2 Physical and Chemical Properties due to the Impurity Doping
, March 13-15, 2013, Hong Kong SnO 2 Physical and Chemical Properties due to the Impurity Doping Richard Rivera, Freddy Marcillo, Washington Chamba, Patricio Puchaicela, Arvids Stashans Abstract First-principles
More informationNon-empirical prediction of impurity segregation in α-fe from first principles. Abstract
APS/123-QED Non-empirical prediction of impurity segregation in α-fe from first principles T. Tsuru, 1, C. Suzuki, 1 Y. Kaji, 1 and T. Tsukada 1 1 Nuclear Science and Engineering Directorate, Japan Atomic
More informationElectrically active defects in semiconductors induced by radiation
Electrically active defects in semiconductors induced by radiation Ivana Capan Rudjer Boskovic Institute, Croatia http://www.irb.hr/users/capan Outline Radiation damage Capacitance transient techniques
More informationModule 16. Diffusion in solids II. Lecture 16. Diffusion in solids II
Module 16 Diffusion in solids II Lecture 16 Diffusion in solids II 1 NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering Keywords: Micro mechanisms of diffusion,
More informationQuantum chemical calculations and MD simulations for Be
start Quantum chemical calculations and MD simulations for Be Institute of Ion Physics University of Innsbruck Michael Probst Michael Stefan Alexander Ivan Andreas Györoek Huber Kaiser Sukuba Mauracher
More informationProgress Report on Chamber Dynamics and Clearing
Progress Report on Chamber Dynamics and Clearing Farrokh Najmabadi, Rene Raffray, Mark S. Tillack, John Pulsifer, Zoran Dragovlovic (UCSD) Ahmed Hassanein (ANL) Laser-IFE Program Workshop May31-June 1,
More informationKinetics. Rate of change in response to thermodynamic forces
Kinetics Rate of change in response to thermodynamic forces Deviation from local equilibrium continuous change T heat flow temperature changes µ atom flow composition changes Deviation from global equilibrium
More informationDepth profiles of helium and hydrogen in tungsten nano-tendril surface morphology using Elastic Recoil Detection
PSFC/JA-12-82 Depth profiles of helium and hydrogen in tungsten nano-tendril surface morphology using Elastic Recoil Detection K.B. Woller, D.G. Whyte, G.M. Wright, R.P. Doerner*, G. de Temmerman** * Center
More informationSimulation of cascades in tungsten-helium N. Juslin a ; V. Jansson a ; K. Nordlund a a
This article was downloaded by: [Nordlund, K.] On: 15 July 2010 Access details: Access Details: [subscription number 924307958] Publisher Taylor & Francis Informa Ltd Registered in England and Wales Registered
More informationExtrinsic Point Defects: Impurities
Extrinsic Point Defects: Impurities Substitutional and interstitial impurities Sol solutions, solubility limit Entropy of ing, eal solution model Enthalpy of ing, quasi-chemical model Ideal and regular
More informationDynamic Monte-Carlo modeling of hydrogen isotope reactive diffusive transport in porous graphite
Journal of Nuclear Materials 367 37 (27) 238 242 www.elsevier.com/locate/jnucmat Dynamic Monte-Carlo modeling of hydrogen isotope reactive diffusive transport in porous graphite R. Schneider a, *, A. Rai
More informationTrapping of He Clusters by Inert Gas Impurities in Tungsten: First-Principles Predictions and Experimental Validation
CCFE-PR(14)07 Duc Nguyen-Manh, S.L. Dudarev Trapping of He Clusters by Inert Gas Impurities in Tungsten: First-Principles Predictions and Experimental Validation Enquiries about copyright and reproduction
More informationMultiscale modelling of sheath physics in edge transport codes
EUROFUSION WPPFC-CP(6) 6599 N Mellet et al. Multiscale modelling of sheath physics in edge transport codes Preprint of Paper to be submitted for publication in Proceedings of 26th IAEA Fusion Energy Conference
More informationMultiscale study on hydrogen mobility in metallic fusion divertor material
UNIVERSITY OF HELSINKI REPORT SERIES IN PHYSICS HU-P-D172 Multiscale study on hydrogen mobility in metallic fusion divertor material Kalle Heinola Division of Materials Physics Department of Physics Faculty
More informationChange of Majority-Carrier Concentration in p-type Silicon by 10 MeV Proton Irradiation. Abstract
Change of Majority-Carrier Concentration in p-type Silicon by 10 MeV Proton Irradiation H. Iwata, S. Kagamihara, H. Matsuura, S. Kawakita 1), T. Oshima ), T. Kamiya ) Osaka Electro-Communication University,
More informationPlasma and Fusion Research: Regular Articles Volume 10, (2015)
Possibility of Quasi-Steady-State Operation of Low-Temperature LHD-Type Deuterium-Deuterium (DD) Reactor Using Impurity Hole Phenomena DD Reactor Controlled by Solid Boron Pellets ) Tsuguhiro WATANABE
More informationSupporting Information Tuning Local Electronic Structure of Single Layer MoS2 through Defect Engineering
Supporting Information Tuning Local Electronic Structure of Single Layer MoS2 through Defect Engineering Yan Chen, 1,2,,$, * Shengxi Huang, 3,6, Xiang Ji, 2 Kiran Adepalli, 2 Kedi Yin, 8 Xi Ling, 3,9 Xinwei
More informationSurface Physics Surface Diffusion. Assistant: Dr. Enrico Gnecco NCCR Nanoscale Science
Surface Physics 008 8. Surface Diffusion Assistant: Dr. Enrico Gnecco NCCR Nanoscale Science Random-Walk Motion Thermal motion of an adatom on an ideal crystal surface: - Thermal excitation the adatom
More informationInvestigations of the effects of 7 TeV proton beams on LHC collimator materials and other materials to be used in the LHC
Russian Research Center Kurchatov Institute Investigations of the effects of 7 ev proton beams on LHC collimator materials and other materials to be used in the LHC A.I.Ryazanov Aims of Investigations:
More informationPhysics and Engineering Studies of the Advanced Divertor for a Fusion Reactor
1 FIP/3-4Ra Physics and Engineering Studies of the Advanced Divertor for a Fusion Reactor N. Asakura 1, K. Hoshino 1, H. Utoh 1, K. Shinya 2, K. Shimizu 3, S. Tokunaga 1, Y.Someya 1, K. Tobita 1, N. Ohno
More informationThe Spherical Tokamak as a Compact Fusion Reactor Concept
The Spherical Tokamak as a Compact Fusion Reactor Concept R. Kaita Princeton Plasma Physics Laboratory ENN Symposium on Compact Fusion Technologies April 19 20, 2018 *This work supported by US DOE Contract
More informationINTERNATIONAL BULLETIN ON ATOMIC AND MOLECULAR FOR FUSION
INTERNATIONAL BULLETIN ON ATOMIC AND MOLECULAR DATA FOR FUSION Number 69 January 2013 Contributors: J. J. Curry, J. Fuhr, A. Kramida, L. I. Podobedova, Yu. Ralchenko, J. Reader, E. B. Saloman, J. E. Sansonetti
More informationRadiation Damage Modeling of Fused Silica in Fusion Systems
1 Radiation Damage Modeling of Fused Silica in Fusion Systems F. Mota 1), M.J. Caturla 2), J.M. Perlado 1), A. Ibarra 3), M. León 3), J.Mollá 3) 1) Instituto de Fusion Nuclear (DENIM) / ETSII / Universidad
More informationThe New Sorgentina Fusion Source Project
The New Sorgentina Fusion Source Project P. Agostini, P. Console Camprini, D. Bernardi, M. Pillon, M. Frisoni, M. Angelone, A. Pietropaolo, P. Batistoni, A. Pizzuto ENEA Agenzia Nazionale per le Nuove
More informationAb initio calculations of proton migration properties in Gd-doped BaCeO 3
Ab initio calculations of proton migration properties in Gd-doped BaCeO 3 Jessica Hermet 1,2, François Bottin 1, Grégory Geneste 1, Guilhem Dezanneau 2 1 CEA, DAM, DIF, F-91297 Arpajon, France 2 Laboratoire
More informationNoninductive Formation of Spherical Tokamak at 7 Times the Plasma Cutoff Density by Electron Bernstein Wave Heating and Current Drive on LATE
1 EX/P6-18 Noninductive Formation of Spherical Tokamak at 7 Times the Plasma Cutoff Density by Electron Bernstein Wave Heating and Current Drive on LATE M. Uchida, T. Maekawa, H. Tanaka, F. Watanabe, Y.
More informationITER Divertor Plasma Modelling with Consistent Core-Edge Parameters
CT/P-7 ITER Divertor Plasma Modelling with Consistent Core-Edge Parameters A. S. Kukushkin ), H. D. Pacher ), G. W. Pacher 3), G. Janeschitz ), D. Coster 5), A. Loarte 6), D. Reiter 7) ) ITER IT, Boltzmannstr.,
More informationIntroduction into Positron Annihilation
Introduction into Positron Annihilation Introduction (How to get positrons? What is special about positron annihilation?) The methods of positron annihilation (positron lifetime, Doppler broadening, ACAR...)
More informationM. Rutigliano a, D. Santoro a, and M. Balat-Pichelin b
M. Rutigliano a, D. Santoro a, and M. Balat-Pichelin b a CNR IMIP, Istituto di Metodologie Inorganiche e dei Plasmi, Via G. Amendola 122/D, 70126 Bari, Italy b Laboratoire Procédés, Matériaux et Energie
More informationThe peculiarities of formation of implanted atom concentration beyond the ion range. V.I. Sugakov Institute for Nuclear Research, Kyiv, Ukraine
The peculiarities of formation of implanted atom concentration beyond the ion range V.I. Sugakov Institute for Nuclear Research, Kyiv, Ukraine Range He in Si, 10 kev Defects E z p (10 100) kev (0.01 0.1)
More informationAtomistic Front-End Process Modeling
Atomistic Front-End Process Modeling A Powerful Tool for Deep-Submicron Device Fabrication SISPAD 2001, Athens Martin Jaraiz University of Valladolid, Spain Thanks to: P. Castrillo (U. Valladolid) R. Pinacho
More informationStrong Facet-Induced and Light-Controlled Room-Temperature. Ferromagnetism in Semiconducting β-fesi 2 Nanocubes
Supporting Information for Manuscript Strong Facet-Induced and Light-Controlled Room-Temperature Ferromagnetism in Semiconducting β-fesi 2 Nanocubes Zhiqiang He, Shijie Xiong, Shuyi Wu, Xiaobin Zhu, Ming
More informationExperiment Section Fig. S1 Fig. S2
Electronic Supplementary Material (ESI) for ChemComm. This journal is The Royal Society of Chemistry 2018 Supplementary Materials Experiment Section The STM experiments were carried out in an ultrahigh
More informationENERGY LANDSCAPE OF POINT DEFECTS IN BCC METALS
ENERGY LANDSCAPE OF POINT DEFECTS IN BCC METALS M.-C. Marinica, R. Alexander, L. Ventelon, L. Proville, F. Willaime CEA, DEN, Service de Recherches de Métallurgie Physique Saclay, France Elementary defects
More informationSupplementary Information
Supplementary Information Supplementary Figure 1: Electronic Kohn-Sham potential profile of a charged monolayer MoTe 2 calculated using PBE-DFT. Plotted is the averaged electronic Kohn- Sham potential
More informationMolybdenum compound MoP as an efficient. electrocatalyst for hydrogen evolution reaction
Electronic Supplementary Material (ESI) for Energy & Environmental Science. This journal is The Royal Society of Chemistry 2014 Molybdenum compound MoP as an efficient electrocatalyst for hydrogen evolution
More informationFirst-principles study of temperature-dependent diffusion coefficients: Hydrogen, deuterium, and tritium in α-ti. Abstract
First-principles study of temperature-dependent diffusion coefficients: Hydrogen, deuterium, and tritium in α-ti Yong Lu 1 and Ping Zhang 1,2, 1 LCP, Institute of Applied Physics and Computational Mathematics,
More informationJoint ICTP-IAEA Workshop on Physics of Radiation Effect and its Simulation for Non-Metallic Condensed Matter.
2359-23 Joint ICTP-IAEA Workshop on Physics of Radiation Effect and its Simulation for Non-Metallic Condensed Matter 13-24 August 2012 Overview of non-metallic materials for fusion applications S. M. González
More informationThomas Schwarz-Selinger Max-Planck-Institut für Plasmaphysik, Garching, Germany
Deuterium retention and isotope exchange studies in self-ion damaged tungsten exposed to neutral atoms Project: Hydrogen retention in self-damaged and Heirradiated tungsten and alloys for PFC Sabina Markelj,
More informationHydrogenic retention of high-z refractory metals exposed to ITER divertor relevant plasma conditions
1 Hydrogenic retention of high-z refractory metals exposed to ITER divertor relevant plasma conditions G.M. Wright 1), E. Alves 2), L.C. Alves 2), N.P. Barradas 2), M. Mayer 3), G.J. van Rooij 1), R.S.
More informationA Project for High Fluence 14 MeV Neutron Source
A Project for High Fluence 14 MeV Neutron Source Mario Pillon 1, Maurizio Angelone 1, Aldo Pizzuto 1, Antonino Pietropaolo 1 1 Associazione ENEA-EURATOM Sulla Fusione, ENEA C.R. Frascati, via E. Fermi,
More informationHydrogen isotope accumulation in helium implantation zone in tungsten
Home Search Collections Journals About Contact us My IOPscience Hydrogen isotope accumulation in helium implantation zone in tungsten This content has been downloaded from IOPscience. Please scroll down
More informationVibrationally resolved ion-molecule collisions
Vibrationally resolved ion-molecule collisions CRP: Atomic and Molecular Data for State-Resolved Modelling of Hydrogen and Helium and Their Isotopes in Fusion plasma Predrag Krstic Physics Division, Oak
More informationOn Dust Particle Dynamics in Tokamak Edge Plasma
On Dust Particle Dynamics in Tokamak Edge Plasma Sergei Krasheninnikov University of California, San Diego, USA With contributions from Y. Tomita 1, R. D. Smirnov, and R. K. Janev 1 1 National Institute
More informationChemical Sputtering of Carbon Materials due to Combined Bombardment by Ions and Atomic Hydrogen
Chemical Sputtering of Carbon Materials due to Combined Bombardment by Ions and Atomic Hydrogen W. Jacob, C. Hopf, and M. Schlüter Max-Planck-Institut für Plasmaphysik, EURATOM Association, Boltzmannstr.
More informationDefects and diffusion in metal oxides: Challenges for first-principles modelling
Defects and diffusion in metal oxides: Challenges for first-principles modelling Karsten Albe, FG Materialmodellierung, TU Darmstadt Johan Pohl, Peter Agoston, Paul Erhart, Manuel Diehm FUNDING: ICTP Workshop
More informationIn situ TEM studies of helium bubble/platelet evolution in Si based materials
In situ TEM studies of helium bubble/platelet evolution in Si based materials M. Vallet 1, M.F. Beaufort 1, J.F. Barbot 1, E. Oliviero 2 and S.E. Donnelly 3 1 Institut Pprime, CNRS-Université de Poitiers,
More informationIn-Vessel Tritium Inventory in Fusion DEMO Plant at JAERI
Japan-US Workshop on Fusion Power Plants and Related Advanced Technologies with participation of EU January 11-13, 2005 at Tokyo, JAPAN In-Vessel Tritium Inventory in Fusion DEMO Plant at JAERI Hirofumi
More informationKinetic lattice Monte Carlo simulations of diffusion processes in Si and SiGe alloys
Kinetic lattice Monte Carlo simulations of diffusion processes in Si and SiGe alloys, Scott Dunham Department of Electrical Engineering Multiscale Modeling Hierarchy Configuration energies and transition
More informationMission Elements of the FNSP and FNSF
Mission Elements of the FNSP and FNSF by R.D. Stambaugh PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION Presented at FNST Workshop August 3, 2010 In Addition to What Will Be Learned
More informationSTUDY OF SEMICONDUCTOR DEVICES EXPOSED TO SPATIAL RADIATION
STUDY OF SEMICONDUCTOR DEVICES EXPOSED TO SPATIAL RADIATION G. DOMINGO YAGÜEZ 1, D. N. VILLARRAZA 1, M. A. CAPPELLETTI 1 y E. L. PELTZER y BLANCÁ 1,2 1 Grupo de Estudio de Materiales y Dispositivos Electrónicos
More informationModeling of charge collection efficiency degradation in semiconductor devices induced by MeV ion beam irradiation
Modeling of charge collection efficiency degradation in semiconductor devices induced by MeV ion beam irradiation Ettore Vittone Physics Department University of Torino - Italy 1 IAEA Coordinate Research
More informationProvisional scenario of radioactive waste management for DEMO
US-Japan Workshop on Fusion power plants and Related advanced technologies 13-14 March 2014 UCSD, USA Provisional scenario of radioactive waste management for DEMO Youji Someya Japan Atomic Energy Agency,
More informationATOMISTIC MODELING OF BORON ACTIVATION AND DIFFUSION IN STRAINED SIGE
ATOMISTIC MODELING OF BORON ACTIVATION AND DIFFUSION IN STRAINED SIGE Scott T. Dunham,, Jakyoung Song, and Chihak Ahn Dept. of Electrical Engineering, Dept. of Physics University of Washington, Box 35500,
More informationSupporting Online Material (1)
Supporting Online Material The density functional theory (DFT) calculations were carried out using the dacapo code (http://www.fysik.dtu.dk/campos), and the RPBE (1) generalized gradient correction (GGA)
More information