Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes

Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube.

Gespeichert in:

Autor*in:	Aleksandrov, V. A. [verfasserIn] Filippov, G. M. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2014

Schlagwörter:	Surface Investigation Neutron Technique Point Charge Polarization Force Image Charge

Übergeordnetes Werk:	Enthalten in: Journal of surface investigation - Moscow : MAIK Nauka/Interperiodics Publ., 2007, 8(2014), 4 vom: Juli, Seite 832-836
Übergeordnetes Werk:	volume:8 ; year:2014 ; number:4 ; month:07 ; pages:832-836

Links:	Volltext

DOI / URN:	10.1134/S1027451014020281

Katalog-ID:	SPR021904928

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allfields	10.1134/S1027451014020281 doi (DE-627)SPR021904928 (SPR)S1027451014020281-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Aleksandrov, V. A. verfasserin aut Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube. Surface Investigation (dpeaa)DE-He213 Neutron Technique (dpeaa)DE-He213 Point Charge (dpeaa)DE-He213 Polarization Force (dpeaa)DE-He213 Image Charge (dpeaa)DE-He213 Filippov, G. M. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 8(2014), 4 vom: Juli, Seite 832-836 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:8 year:2014 number:4 month:07 pages:832-836 https://dx.doi.org/10.1134/S1027451014020281 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 8 2014 4 07 832-836
spelling	10.1134/S1027451014020281 doi (DE-627)SPR021904928 (SPR)S1027451014020281-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Aleksandrov, V. A. verfasserin aut Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube. Surface Investigation (dpeaa)DE-He213 Neutron Technique (dpeaa)DE-He213 Point Charge (dpeaa)DE-He213 Polarization Force (dpeaa)DE-He213 Image Charge (dpeaa)DE-He213 Filippov, G. M. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 8(2014), 4 vom: Juli, Seite 832-836 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:8 year:2014 number:4 month:07 pages:832-836 https://dx.doi.org/10.1134/S1027451014020281 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 8 2014 4 07 832-836
allfields_unstemmed	10.1134/S1027451014020281 doi (DE-627)SPR021904928 (SPR)S1027451014020281-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Aleksandrov, V. A. verfasserin aut Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube. Surface Investigation (dpeaa)DE-He213 Neutron Technique (dpeaa)DE-He213 Point Charge (dpeaa)DE-He213 Polarization Force (dpeaa)DE-He213 Image Charge (dpeaa)DE-He213 Filippov, G. M. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 8(2014), 4 vom: Juli, Seite 832-836 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:8 year:2014 number:4 month:07 pages:832-836 https://dx.doi.org/10.1134/S1027451014020281 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 8 2014 4 07 832-836
allfieldsGer	10.1134/S1027451014020281 doi (DE-627)SPR021904928 (SPR)S1027451014020281-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Aleksandrov, V. A. verfasserin aut Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube. Surface Investigation (dpeaa)DE-He213 Neutron Technique (dpeaa)DE-He213 Point Charge (dpeaa)DE-He213 Polarization Force (dpeaa)DE-He213 Image Charge (dpeaa)DE-He213 Filippov, G. M. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 8(2014), 4 vom: Juli, Seite 832-836 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:8 year:2014 number:4 month:07 pages:832-836 https://dx.doi.org/10.1134/S1027451014020281 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 8 2014 4 07 832-836
allfieldsSound	10.1134/S1027451014020281 doi (DE-627)SPR021904928 (SPR)S1027451014020281-e DE-627 ger DE-627 rakwb eng 530 540 ASE 33.68 bkl 51.30 bkl Aleksandrov, V. A. verfasserin aut Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube. Surface Investigation (dpeaa)DE-He213 Neutron Technique (dpeaa)DE-He213 Point Charge (dpeaa)DE-He213 Polarization Force (dpeaa)DE-He213 Image Charge (dpeaa)DE-He213 Filippov, G. M. verfasserin aut Enthalten in Journal of surface investigation Moscow : MAIK Nauka/Interperiodics Publ., 2007 8(2014), 4 vom: Juli, Seite 832-836 (DE-627)546007252 (DE-600)2389417-9 1819-7094 nnns volume:8 year:2014 number:4 month:07 pages:832-836 https://dx.doi.org/10.1134/S1027451014020281 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 8 2014 4 07 832-836
language	English
source	Enthalten in Journal of surface investigation 8(2014), 4 vom: Juli, Seite 832-836 volume:8 year:2014 number:4 month:07 pages:832-836
sourceStr	Enthalten in Journal of surface investigation 8(2014), 4 vom: Juli, Seite 832-836 volume:8 year:2014 number:4 month:07 pages:832-836
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Surface Investigation Neutron Technique Point Charge Polarization Force Image Charge
dewey-raw	530
isfreeaccess_bool	false
container_title	Journal of surface investigation
authorswithroles_txt_mv	Aleksandrov, V. A. @@aut@@ Filippov, G. M. @@aut@@
publishDateDaySort_date	2014-07-01T00:00:00Z
hierarchy_top_id	546007252
dewey-sort	3530
id	SPR021904928
language_de	englisch
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author	Aleksandrov, V. A.
spellingShingle	Aleksandrov, V. A. ddc 530 bkl 33.68 bkl 51.30 misc Surface Investigation misc Neutron Technique misc Point Charge misc Polarization Force misc Image Charge Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes
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topic_title	530 540 ASE 33.68 bkl 51.30 bkl Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes Surface Investigation (dpeaa)DE-He213 Neutron Technique (dpeaa)DE-He213 Point Charge (dpeaa)DE-He213 Polarization Force (dpeaa)DE-He213 Image Charge (dpeaa)DE-He213
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title	Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes
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title_full	Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes
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author_browse	Aleksandrov, V. A. Filippov, G. M.
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title_sort	model estimation of the polarization forces generated by a moving point charge in carbon nanotubes
title_auth	Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes
abstract	Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube.
abstractGer	Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube.
abstract_unstemmed	Abstract Two models of polarization forces generated inside a carbon nanotube by a moving point charge are considered. In the first model, carbon atoms are replaced by equivalent spherical dielectrics; in the second model, the carbon nanotube is replaced by a homogeneous hollow dielectric tube.
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title_short	Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes
url	https://dx.doi.org/10.1134/S1027451014020281
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Model estimation of the polarization forces generated by a moving point charge in carbon nanotubes

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