Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces

Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen ato...
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Autor*in:	D.H. Liu [verfasserIn] S.Y. Dai [verfasserIn] M. Wada [verfasserIn] K.R. Yang [verfasserIn] J.Y. Chen [verfasserIn] D.P. Liu [verfasserIn] N. Cherenda [verfasserIn] D.Z. Wang [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2021

Schlagwörter:	Tungsten Fuzz Porosity Kinetic Monte Carlo

Übergeordnetes Werk:	In: Nuclear Materials and Energy - Elsevier, 2016, 26(2021), Seite 100909-
Übergeordnetes Werk:	volume:26 ; year:2021 ; pages:100909-

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.1016/j.nme.2021.100909

Katalog-ID:	DOAJ07381489X

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520			\|a Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data.
650		4	\|a Tungsten
650		4	\|a Fuzz
650		4	\|a Porosity
650		4	\|a Kinetic Monte Carlo
653		0	\|a Nuclear engineering. Atomic power
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700	0		\|a N. Cherenda \|e verfasserin \|4 aut
700	0		\|a D.Z. Wang \|e verfasserin \|4 aut
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publishDate	2021
allfields	10.1016/j.nme.2021.100909 doi (DE-627)DOAJ07381489X (DE-599)DOAJ6a52d7d855954a7fbeab2c5777e6c5fe DE-627 ger DE-627 rakwb eng TK9001-9401 D.H. Liu verfasserin aut Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data. Tungsten Fuzz Porosity Kinetic Monte Carlo Nuclear engineering. Atomic power S.Y. Dai verfasserin aut M. Wada verfasserin aut K.R. Yang verfasserin aut J.Y. Chen verfasserin aut D.P. Liu verfasserin aut N. Cherenda verfasserin aut D.Z. Wang verfasserin aut In Nuclear Materials and Energy Elsevier, 2016 26(2021), Seite 100909- (DE-627)817363181 (DE-600)2808888-8 23521791 nnns volume:26 year:2021 pages:100909- https://doi.org/10.1016/j.nme.2021.100909 kostenfrei https://doaj.org/article/6a52d7d855954a7fbeab2c5777e6c5fe kostenfrei http://www.sciencedirect.com/science/article/pii/S2352179121000089 kostenfrei https://doaj.org/toc/2352-1791 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 26 2021 100909-
spelling	10.1016/j.nme.2021.100909 doi (DE-627)DOAJ07381489X (DE-599)DOAJ6a52d7d855954a7fbeab2c5777e6c5fe DE-627 ger DE-627 rakwb eng TK9001-9401 D.H. Liu verfasserin aut Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data. Tungsten Fuzz Porosity Kinetic Monte Carlo Nuclear engineering. Atomic power S.Y. Dai verfasserin aut M. Wada verfasserin aut K.R. Yang verfasserin aut J.Y. Chen verfasserin aut D.P. Liu verfasserin aut N. Cherenda verfasserin aut D.Z. Wang verfasserin aut In Nuclear Materials and Energy Elsevier, 2016 26(2021), Seite 100909- (DE-627)817363181 (DE-600)2808888-8 23521791 nnns volume:26 year:2021 pages:100909- https://doi.org/10.1016/j.nme.2021.100909 kostenfrei https://doaj.org/article/6a52d7d855954a7fbeab2c5777e6c5fe kostenfrei http://www.sciencedirect.com/science/article/pii/S2352179121000089 kostenfrei https://doaj.org/toc/2352-1791 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 26 2021 100909-
allfields_unstemmed	10.1016/j.nme.2021.100909 doi (DE-627)DOAJ07381489X (DE-599)DOAJ6a52d7d855954a7fbeab2c5777e6c5fe DE-627 ger DE-627 rakwb eng TK9001-9401 D.H. Liu verfasserin aut Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data. Tungsten Fuzz Porosity Kinetic Monte Carlo Nuclear engineering. Atomic power S.Y. Dai verfasserin aut M. Wada verfasserin aut K.R. Yang verfasserin aut J.Y. Chen verfasserin aut D.P. Liu verfasserin aut N. Cherenda verfasserin aut D.Z. Wang verfasserin aut In Nuclear Materials and Energy Elsevier, 2016 26(2021), Seite 100909- (DE-627)817363181 (DE-600)2808888-8 23521791 nnns volume:26 year:2021 pages:100909- https://doi.org/10.1016/j.nme.2021.100909 kostenfrei https://doaj.org/article/6a52d7d855954a7fbeab2c5777e6c5fe kostenfrei http://www.sciencedirect.com/science/article/pii/S2352179121000089 kostenfrei https://doaj.org/toc/2352-1791 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 26 2021 100909-
allfieldsGer	10.1016/j.nme.2021.100909 doi (DE-627)DOAJ07381489X (DE-599)DOAJ6a52d7d855954a7fbeab2c5777e6c5fe DE-627 ger DE-627 rakwb eng TK9001-9401 D.H. Liu verfasserin aut Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data. Tungsten Fuzz Porosity Kinetic Monte Carlo Nuclear engineering. Atomic power S.Y. Dai verfasserin aut M. Wada verfasserin aut K.R. Yang verfasserin aut J.Y. Chen verfasserin aut D.P. Liu verfasserin aut N. Cherenda verfasserin aut D.Z. Wang verfasserin aut In Nuclear Materials and Energy Elsevier, 2016 26(2021), Seite 100909- (DE-627)817363181 (DE-600)2808888-8 23521791 nnns volume:26 year:2021 pages:100909- https://doi.org/10.1016/j.nme.2021.100909 kostenfrei https://doaj.org/article/6a52d7d855954a7fbeab2c5777e6c5fe kostenfrei http://www.sciencedirect.com/science/article/pii/S2352179121000089 kostenfrei https://doaj.org/toc/2352-1791 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 26 2021 100909-
allfieldsSound	10.1016/j.nme.2021.100909 doi (DE-627)DOAJ07381489X (DE-599)DOAJ6a52d7d855954a7fbeab2c5777e6c5fe DE-627 ger DE-627 rakwb eng TK9001-9401 D.H. Liu verfasserin aut Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces 2021 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data. Tungsten Fuzz Porosity Kinetic Monte Carlo Nuclear engineering. Atomic power S.Y. Dai verfasserin aut M. Wada verfasserin aut K.R. Yang verfasserin aut J.Y. Chen verfasserin aut D.P. Liu verfasserin aut N. Cherenda verfasserin aut D.Z. Wang verfasserin aut In Nuclear Materials and Energy Elsevier, 2016 26(2021), Seite 100909- (DE-627)817363181 (DE-600)2808888-8 23521791 nnns volume:26 year:2021 pages:100909- https://doi.org/10.1016/j.nme.2021.100909 kostenfrei https://doaj.org/article/6a52d7d855954a7fbeab2c5777e6c5fe kostenfrei http://www.sciencedirect.com/science/article/pii/S2352179121000089 kostenfrei https://doaj.org/toc/2352-1791 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2088 GBV_ILN_2106 GBV_ILN_2110 GBV_ILN_2112 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 26 2021 100909-
language	English
source	In Nuclear Materials and Energy 26(2021), Seite 100909- volume:26 year:2021 pages:100909-
sourceStr	In Nuclear Materials and Energy 26(2021), Seite 100909- volume:26 year:2021 pages:100909-
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Tungsten Fuzz Porosity Kinetic Monte Carlo Nuclear engineering. Atomic power
isfreeaccess_bool	true
container_title	Nuclear Materials and Energy
authorswithroles_txt_mv	D.H. Liu @@aut@@ S.Y. Dai @@aut@@ M. Wada @@aut@@ K.R. Yang @@aut@@ J.Y. Chen @@aut@@ D.P. Liu @@aut@@ N. Cherenda @@aut@@ D.Z. Wang @@aut@@
publishDateDaySort_date	2021-01-01T00:00:00Z
hierarchy_top_id	817363181
id	DOAJ07381489X
language_de	englisch
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callnumber-first	T - Technology
author	D.H. Liu
spellingShingle	D.H. Liu misc TK9001-9401 misc Tungsten misc Fuzz misc Porosity misc Kinetic Monte Carlo misc Nuclear engineering. Atomic power Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces
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topic_title	TK9001-9401 Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces Tungsten Fuzz Porosity Kinetic Monte Carlo
topic	misc TK9001-9401 misc Tungsten misc Fuzz misc Porosity misc Kinetic Monte Carlo misc Nuclear engineering. Atomic power
topic_unstemmed	misc TK9001-9401 misc Tungsten misc Fuzz misc Porosity misc Kinetic Monte Carlo misc Nuclear engineering. Atomic power
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title	Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces
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title_full	Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces
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title_sort	modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces
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title_auth	Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces
abstract	Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data.
abstractGer	Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data.
abstract_unstemmed	Modelling of the hydrogen reflection on tungsten smooth and fuzz surfaces under the low-energy hydrogen plasma bombardment has been performed with the three-dimensional kinetic Monte Carlo code SURO-FUZZ. The relative reflection coefficient of hydrogen atoms, i.e. the ratio of reflected hydrogen atoms on the tungsten fuzz surface to that on the tungsten smooth one, is employed to illustrate the change in the hydrogen reflection on the tungsten fuzz and smooth surfaces. The simulated relative reflection coefficient of hydrogen atoms shows a large discrepancy with the measured values obtained in the hydrogen plasma bombardment experiment. The impinging hydrogen particles with a low incident energy result in a small sputtering and large residual nanostructure existing on the tungsten fuzz surface, which lead to a small change in the relative reflection coefficient of hydrogen atoms. The discrepancy between simulations and experiments motivates us to take the impacts of the annealing effect into account in SURO-FUZZ code. Implementation of annealing effect into SURO-FUZZ has been benchmarked against the experimental data. The simulated temporal evolution of the hydrogen reflection coefficient is in reasonable agreement with the experimental data.
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title_short	Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces
url	https://doi.org/10.1016/j.nme.2021.100909 https://doaj.org/article/6a52d7d855954a7fbeab2c5777e6c5fe http://www.sciencedirect.com/science/article/pii/S2352179121000089 https://doaj.org/toc/2352-1791
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up_date	2024-07-03T19:45:47.529Z
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Modelling of hydrogen atoms reflection from an annealed tungsten fuzzy surfaces

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