A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite
Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imagi...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Voilov, D. N. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2009 |
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| Schlagwörter: |
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| Anmerkung: |
© Pleiades Publishing, Ltd. 2009 |
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| Übergeordnetes Werk: |
Enthalten in: Nanotechnologies in Russia - [Moskau] : Pleiades Publishing, 2008, 4(2009), 5-6 vom: Juni, Seite 290-295 |
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| Übergeordnetes Werk: |
volume:4 ; year:2009 ; number:5-6 ; month:06 ; pages:290-295 |
| Links: |
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| DOI / URN: |
10.1134/S199507800905005X |
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| Katalog-ID: |
SPR025214683 |
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| 100 | 1 | |a Voilov, D. N. |e verfasserin |4 aut | |
| 245 | 1 | 2 | |a A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite |
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| 520 | |a Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. | ||
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| 650 | 4 | |a Kinetic Unit |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Zeolite Matrix |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Novikov, G. F. |4 aut | |
| 700 | 1 | |a Meteleva-Fisher, Yu. V. |4 aut | |
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10.1134/S199507800905005X doi (DE-627)SPR025214683 (SPR)S199507800905005X-e DE-627 ger DE-627 rakwb eng Voilov, D. N. verfasserin aut A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2009 Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. Relaxation Transition (dpeaa)DE-He213 Dielectric Spectrum (dpeaa)DE-He213 Dielectric Relaxation Time (dpeaa)DE-He213 Kinetic Unit (dpeaa)DE-He213 Zeolite Matrix (dpeaa)DE-He213 Novikov, G. F. aut Meteleva-Fisher, Yu. V. aut Enthalten in Nanotechnologies in Russia [Moskau] : Pleiades Publishing, 2008 4(2009), 5-6 vom: Juni, Seite 290-295 (DE-627)565518887 (DE-600)2424432-6 1995-0799 nnns volume:4 year:2009 number:5-6 month:06 pages:290-295 https://dx.doi.org/10.1134/S199507800905005X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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 AR 4 2009 5-6 06 290-295 |
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10.1134/S199507800905005X doi (DE-627)SPR025214683 (SPR)S199507800905005X-e DE-627 ger DE-627 rakwb eng Voilov, D. N. verfasserin aut A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2009 Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. Relaxation Transition (dpeaa)DE-He213 Dielectric Spectrum (dpeaa)DE-He213 Dielectric Relaxation Time (dpeaa)DE-He213 Kinetic Unit (dpeaa)DE-He213 Zeolite Matrix (dpeaa)DE-He213 Novikov, G. F. aut Meteleva-Fisher, Yu. V. aut Enthalten in Nanotechnologies in Russia [Moskau] : Pleiades Publishing, 2008 4(2009), 5-6 vom: Juni, Seite 290-295 (DE-627)565518887 (DE-600)2424432-6 1995-0799 nnns volume:4 year:2009 number:5-6 month:06 pages:290-295 https://dx.doi.org/10.1134/S199507800905005X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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 AR 4 2009 5-6 06 290-295 |
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10.1134/S199507800905005X doi (DE-627)SPR025214683 (SPR)S199507800905005X-e DE-627 ger DE-627 rakwb eng Voilov, D. N. verfasserin aut A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2009 Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. Relaxation Transition (dpeaa)DE-He213 Dielectric Spectrum (dpeaa)DE-He213 Dielectric Relaxation Time (dpeaa)DE-He213 Kinetic Unit (dpeaa)DE-He213 Zeolite Matrix (dpeaa)DE-He213 Novikov, G. F. aut Meteleva-Fisher, Yu. V. aut Enthalten in Nanotechnologies in Russia [Moskau] : Pleiades Publishing, 2008 4(2009), 5-6 vom: Juni, Seite 290-295 (DE-627)565518887 (DE-600)2424432-6 1995-0799 nnns volume:4 year:2009 number:5-6 month:06 pages:290-295 https://dx.doi.org/10.1134/S199507800905005X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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 AR 4 2009 5-6 06 290-295 |
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10.1134/S199507800905005X doi (DE-627)SPR025214683 (SPR)S199507800905005X-e DE-627 ger DE-627 rakwb eng Voilov, D. N. verfasserin aut A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2009 Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. Relaxation Transition (dpeaa)DE-He213 Dielectric Spectrum (dpeaa)DE-He213 Dielectric Relaxation Time (dpeaa)DE-He213 Kinetic Unit (dpeaa)DE-He213 Zeolite Matrix (dpeaa)DE-He213 Novikov, G. F. aut Meteleva-Fisher, Yu. V. aut Enthalten in Nanotechnologies in Russia [Moskau] : Pleiades Publishing, 2008 4(2009), 5-6 vom: Juni, Seite 290-295 (DE-627)565518887 (DE-600)2424432-6 1995-0799 nnns volume:4 year:2009 number:5-6 month:06 pages:290-295 https://dx.doi.org/10.1134/S199507800905005X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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 AR 4 2009 5-6 06 290-295 |
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10.1134/S199507800905005X doi (DE-627)SPR025214683 (SPR)S199507800905005X-e DE-627 ger DE-627 rakwb eng Voilov, D. N. verfasserin aut A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2009 Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. Relaxation Transition (dpeaa)DE-He213 Dielectric Spectrum (dpeaa)DE-He213 Dielectric Relaxation Time (dpeaa)DE-He213 Kinetic Unit (dpeaa)DE-He213 Zeolite Matrix (dpeaa)DE-He213 Novikov, G. F. aut Meteleva-Fisher, Yu. V. aut Enthalten in Nanotechnologies in Russia [Moskau] : Pleiades Publishing, 2008 4(2009), 5-6 vom: Juni, Seite 290-295 (DE-627)565518887 (DE-600)2424432-6 1995-0799 nnns volume:4 year:2009 number:5-6 month:06 pages:290-295 https://dx.doi.org/10.1134/S199507800905005X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER 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_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 AR 4 2009 5-6 06 290-295 |
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Enthalten in Nanotechnologies in Russia 4(2009), 5-6 vom: Juni, Seite 290-295 volume:4 year:2009 number:5-6 month:06 pages:290-295 |
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Enthalten in Nanotechnologies in Russia 4(2009), 5-6 vom: Juni, Seite 290-295 volume:4 year:2009 number:5-6 month:06 pages:290-295 |
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Voilov, D. N. @@aut@@ Novikov, G. F. @@aut@@ Meteleva-Fisher, Yu. V. @@aut@@ |
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2009-06-01T00:00:00Z |
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Voilov, D. N. |
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Voilov, D. N. misc Relaxation Transition misc Dielectric Spectrum misc Dielectric Relaxation Time misc Kinetic Unit misc Zeolite Matrix A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite |
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A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite Relaxation Transition (dpeaa)DE-He213 Dielectric Spectrum (dpeaa)DE-He213 Dielectric Relaxation Time (dpeaa)DE-He213 Kinetic Unit (dpeaa)DE-He213 Zeolite Matrix (dpeaa)DE-He213 |
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misc Relaxation Transition misc Dielectric Spectrum misc Dielectric Relaxation Time misc Kinetic Unit misc Zeolite Matrix |
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misc Relaxation Transition misc Dielectric Spectrum misc Dielectric Relaxation Time misc Kinetic Unit misc Zeolite Matrix |
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A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite |
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A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite |
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Voilov, D. N. |
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Nanotechnologies in Russia |
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Voilov, D. N. Novikov, G. F. Meteleva-Fisher, Yu. V. |
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Voilov, D. N. |
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10.1134/S199507800905005X |
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broadband dielectric spectroscopy study of the relaxation properties of h-beta-zns zeolite-semiconductor nanocomposite |
| title_auth |
A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite |
| abstract |
Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. © Pleiades Publishing, Ltd. 2009 |
| abstractGer |
Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. © Pleiades Publishing, Ltd. 2009 |
| abstract_unstemmed |
Abstract Broadband dielectric spectroscopy was used to determine the dependences of the complex permittivity for H-Beta zeolite and H-Beta-ZnS composite in a frequency range of $ 10^{−1} $−$ 10^{5} $ Hz and a temperature range from −160 to +300°C. A difference in the dispersion of the real and imaginary parts of the permittivity of H-Beta-ZnS nanocomposite in comparison with initial zeolite was detected. Approximating the dielectric spectrum by the Havriliak-Negami functions made it possible to obtain the distribution of dielectric relaxation times, which contained several maxima corresponding to the relaxation transitions in both nanocomposite and initial zeolite. A new relaxation transition was observed in the nanocomposite in a temperature range of 170–230°C. The temperature dependence of the relaxation time of this transition was linearized in the Arrhenius coordinates with an activation energy of ∼2.0 eV. © Pleiades Publishing, Ltd. 2009 |
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A broadband dielectric spectroscopy study of the relaxation properties of H-Beta-ZnS zeolite-semiconductor nanocomposite |
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https://dx.doi.org/10.1134/S199507800905005X |
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Novikov, G. F. Meteleva-Fisher, Yu. V. |
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10.1134/S199507800905005X |
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2024-07-03T14:36:17.941Z |
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