Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals
Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atom...
Ausführliche Beschreibung
Autor*in: |
Belykh, S. F. [verfasserIn] Tolstogouzov, A. B. [verfasserIn] Lozovan, A. A. [verfasserIn] Aleshin, M. E. [verfasserIn] Elantyev, I. A. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2015 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Journal of surface investigation - Moscow : MAIK Nauka/Interperiodics Publ., 2007, 9(2015), 1 vom: Jan., Seite 172-177 |
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Übergeordnetes Werk: |
volume:9 ; year:2015 ; number:1 ; month:01 ; pages:172-177 |
Links: |
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DOI / URN: |
10.1134/S102745101406024X |
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Katalog-ID: |
SPR021906165 |
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245 | 1 | 0 | |a Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
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520 | |a Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. | ||
650 | 4 | |a atomic ion flux formation |7 (dpeaa)DE-He213 | |
650 | 4 | |a ion-beam sputtering of metals |7 (dpeaa)DE-He213 | |
650 | 4 | |a nonlinear collision cascades |7 (dpeaa)DE-He213 | |
700 | 1 | |a Tolstogouzov, A. B. |e verfasserin |4 aut | |
700 | 1 | |a Lozovan, A. A. |e verfasserin |4 aut | |
700 | 1 | |a Aleshin, M. E. |e verfasserin |4 aut | |
700 | 1 | |a Elantyev, I. A. |e verfasserin |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Journal of surface investigation |d Moscow : MAIK Nauka/Interperiodics Publ., 2007 |g 9(2015), 1 vom: Jan., Seite 172-177 |w (DE-627)546007252 |w (DE-600)2389417-9 |x 1819-7094 |7 nnns |
773 | 1 | 8 | |g volume:9 |g year:2015 |g number:1 |g month:01 |g pages:172-177 |
856 | 4 | 0 | |u https://dx.doi.org/10.1134/S102745101406024X |z lizenzpflichtig |3 Volltext |
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10.1134/S102745101406024X doi (DE-627)SPR021906165 (SPR)S102745101406024X-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Belykh, S. F. verfasserin aut Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. atomic ion flux formation (dpeaa)DE-He213 ion-beam sputtering of metals (dpeaa)DE-He213 nonlinear collision cascades (dpeaa)DE-He213 Tolstogouzov, A. B. verfasserin aut Lozovan, A. A. verfasserin aut Aleshin, M. E. verfasserin aut Elantyev, I. A. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 9(2015), 1 vom: Jan., Seite 172-177 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:9 year:2015 number:1 month:01 pages:172-177 https://dx.doi.org/10.1134/S102745101406024X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 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_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.68 ASE 51.30 ASE AR 9 2015 1 01 172-177 |
spelling |
10.1134/S102745101406024X doi (DE-627)SPR021906165 (SPR)S102745101406024X-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Belykh, S. F. verfasserin aut Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. atomic ion flux formation (dpeaa)DE-He213 ion-beam sputtering of metals (dpeaa)DE-He213 nonlinear collision cascades (dpeaa)DE-He213 Tolstogouzov, A. B. verfasserin aut Lozovan, A. A. verfasserin aut Aleshin, M. E. verfasserin aut Elantyev, I. A. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 9(2015), 1 vom: Jan., Seite 172-177 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:9 year:2015 number:1 month:01 pages:172-177 https://dx.doi.org/10.1134/S102745101406024X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 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_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.68 ASE 51.30 ASE AR 9 2015 1 01 172-177 |
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10.1134/S102745101406024X doi (DE-627)SPR021906165 (SPR)S102745101406024X-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Belykh, S. F. verfasserin aut Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. atomic ion flux formation (dpeaa)DE-He213 ion-beam sputtering of metals (dpeaa)DE-He213 nonlinear collision cascades (dpeaa)DE-He213 Tolstogouzov, A. B. verfasserin aut Lozovan, A. A. verfasserin aut Aleshin, M. E. verfasserin aut Elantyev, I. A. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 9(2015), 1 vom: Jan., Seite 172-177 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:9 year:2015 number:1 month:01 pages:172-177 https://dx.doi.org/10.1134/S102745101406024X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 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_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.68 ASE 51.30 ASE AR 9 2015 1 01 172-177 |
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10.1134/S102745101406024X doi (DE-627)SPR021906165 (SPR)S102745101406024X-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Belykh, S. F. verfasserin aut Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. atomic ion flux formation (dpeaa)DE-He213 ion-beam sputtering of metals (dpeaa)DE-He213 nonlinear collision cascades (dpeaa)DE-He213 Tolstogouzov, A. B. verfasserin aut Lozovan, A. A. verfasserin aut Aleshin, M. E. verfasserin aut Elantyev, I. A. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 9(2015), 1 vom: Jan., Seite 172-177 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:9 year:2015 number:1 month:01 pages:172-177 https://dx.doi.org/10.1134/S102745101406024X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 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_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.68 ASE 51.30 ASE AR 9 2015 1 01 172-177 |
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10.1134/S102745101406024X doi (DE-627)SPR021906165 (SPR)S102745101406024X-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Belykh, S. F. verfasserin aut Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals 2015 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. atomic ion flux formation (dpeaa)DE-He213 ion-beam sputtering of metals (dpeaa)DE-He213 nonlinear collision cascades (dpeaa)DE-He213 Tolstogouzov, A. B. verfasserin aut Lozovan, A. A. verfasserin aut Aleshin, M. E. verfasserin aut Elantyev, I. A. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 9(2015), 1 vom: Jan., Seite 172-177 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:9 year:2015 number:1 month:01 pages:172-177 https://dx.doi.org/10.1134/S102745101406024X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 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_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 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_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 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_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.68 ASE 51.30 ASE AR 9 2015 1 01 172-177 |
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Enthalten in Journal of surface investigation 9(2015), 1 vom: Jan., Seite 172-177 volume:9 year:2015 number:1 month:01 pages:172-177 |
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Belykh, S. F. @@aut@@ Tolstogouzov, A. B. @@aut@@ Lozovan, A. A. @@aut@@ Aleshin, M. E. @@aut@@ Elantyev, I. A. @@aut@@ |
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author |
Belykh, S. F. |
spellingShingle |
Belykh, S. F. ddc 530 bkl 33.68 bkl 51.30 misc atomic ion flux formation misc ion-beam sputtering of metals misc nonlinear collision cascades Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
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topic_title |
530 540 ASE 33.68 bkl 51.30 bkl Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals atomic ion flux formation (dpeaa)DE-He213 ion-beam sputtering of metals (dpeaa)DE-He213 nonlinear collision cascades (dpeaa)DE-He213 |
topic |
ddc 530 bkl 33.68 bkl 51.30 misc atomic ion flux formation misc ion-beam sputtering of metals misc nonlinear collision cascades |
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ddc 530 bkl 33.68 bkl 51.30 misc atomic ion flux formation misc ion-beam sputtering of metals misc nonlinear collision cascades |
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Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
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title_full |
Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
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Belykh, S. F. |
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Journal of surface investigation |
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Journal of surface investigation |
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Belykh, S. F. Tolstogouzov, A. B. Lozovan, A. A. Aleshin, M. E. Elantyev, I. A. |
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9 |
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530 540 ASE 33.68 bkl 51.30 bkl |
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Elektronische Aufsätze |
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Belykh, S. F. |
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10.1134/S102745101406024X |
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530 540 |
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verfasserin |
title_sort |
analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
title_auth |
Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
abstract |
Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. |
abstractGer |
Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. |
abstract_unstemmed |
Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. The conditions leading to the formation of an atomic ion flux are analyzed for the case where metals are sputtered in the nonlinear collision-cascade mode. |
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title_short |
Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals |
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https://dx.doi.org/10.1134/S102745101406024X |
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Tolstogouzov, A. B. Lozovan, A. A. Aleshin, M. E. Elantyev, I. A. |
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Tolstogouzov, A. B. Lozovan, A. A. Aleshin, M. E. Elantyev, I. A. |
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546007252 |
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doi_str |
10.1134/S102745101406024X |
up_date |
2024-07-04T00:57:48.868Z |
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F.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Analysis of the conditions underlying the formation of emitted atomic ion fluxes in the nonlinear collision-cascade mode of the sputtering of metals</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The ion-beam sputtering of metals carried out in the nonlinear collision-cascade mode, where the excitation level (average energy per atom) in the thermal-peak volume exceeds the critical ambient temperature, initiates quasi-thermal atom and atomic ion emissions. The energy spectrum of atomic particles is substantially shifted toward the low-energy region and does not correspond to a Maxwellian distribution. Correct description of quasi-thermal ion emission requires first of all knowledge of the conditions under which a sputtered particle flux is formed. 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