Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition
Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Baryshnikov, S. V. [verfasserIn] Charnaya, E. V. [verfasserIn] Shatskaya, Yu. A. [verfasserIn] Milinskiy, A. Yu. [verfasserIn] Samoilovich, M. I. [verfasserIn] Michel, D. [verfasserIn] Tien, C. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2011 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Physics of the solid state - College Park, Md. : Inst., 1997, 53(2011), 6 vom: 10. Juni |
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| Übergeordnetes Werk: |
volume:53 ; year:2011 ; number:6 ; day:10 ; month:06 |
| Links: |
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| DOI / URN: |
10.1134/S1063783411060059 |
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| Katalog-ID: |
SPR019655495 |
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| 245 | 1 | 0 | |a Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
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| 520 | |a Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. | ||
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| 650 | 4 | |a Harmonic Amplitude |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Ferroelectric Phase Transition |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Charnaya, E. V. |e verfasserin |4 aut | |
| 700 | 1 | |a Shatskaya, Yu. A. |e verfasserin |4 aut | |
| 700 | 1 | |a Milinskiy, A. Yu. |e verfasserin |4 aut | |
| 700 | 1 | |a Samoilovich, M. I. |e verfasserin |4 aut | |
| 700 | 1 | |a Michel, D. |e verfasserin |4 aut | |
| 700 | 1 | |a Tien, C. |e verfasserin |4 aut | |
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10.1134/S1063783411060059 doi (DE-627)SPR019655495 (SPR)S1063783411060059-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Baryshnikov, S. V. verfasserin aut Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. Phase Transition Temperature (dpeaa)DE-He213 Opal Matrix (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Harmonic Amplitude (dpeaa)DE-He213 Ferroelectric Phase Transition (dpeaa)DE-He213 Charnaya, E. V. verfasserin aut Shatskaya, Yu. A. verfasserin aut Milinskiy, A. Yu. verfasserin aut Samoilovich, M. I. verfasserin aut Michel, D. verfasserin aut Tien, C. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 53(2011), 6 vom: 10. Juni (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:53 year:2011 number:6 day:10 month:06 https://dx.doi.org/10.1134/S1063783411060059 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_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 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_2056 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 33.60 ASE AR 53 2011 6 10 06 |
| spelling |
10.1134/S1063783411060059 doi (DE-627)SPR019655495 (SPR)S1063783411060059-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Baryshnikov, S. V. verfasserin aut Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. Phase Transition Temperature (dpeaa)DE-He213 Opal Matrix (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Harmonic Amplitude (dpeaa)DE-He213 Ferroelectric Phase Transition (dpeaa)DE-He213 Charnaya, E. V. verfasserin aut Shatskaya, Yu. A. verfasserin aut Milinskiy, A. Yu. verfasserin aut Samoilovich, M. I. verfasserin aut Michel, D. verfasserin aut Tien, C. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 53(2011), 6 vom: 10. Juni (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:53 year:2011 number:6 day:10 month:06 https://dx.doi.org/10.1134/S1063783411060059 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_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 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_2056 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 33.60 ASE AR 53 2011 6 10 06 |
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10.1134/S1063783411060059 doi (DE-627)SPR019655495 (SPR)S1063783411060059-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Baryshnikov, S. V. verfasserin aut Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. Phase Transition Temperature (dpeaa)DE-He213 Opal Matrix (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Harmonic Amplitude (dpeaa)DE-He213 Ferroelectric Phase Transition (dpeaa)DE-He213 Charnaya, E. V. verfasserin aut Shatskaya, Yu. A. verfasserin aut Milinskiy, A. Yu. verfasserin aut Samoilovich, M. I. verfasserin aut Michel, D. verfasserin aut Tien, C. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 53(2011), 6 vom: 10. Juni (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:53 year:2011 number:6 day:10 month:06 https://dx.doi.org/10.1134/S1063783411060059 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_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 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_2056 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 33.60 ASE AR 53 2011 6 10 06 |
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10.1134/S1063783411060059 doi (DE-627)SPR019655495 (SPR)S1063783411060059-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Baryshnikov, S. V. verfasserin aut Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. Phase Transition Temperature (dpeaa)DE-He213 Opal Matrix (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Harmonic Amplitude (dpeaa)DE-He213 Ferroelectric Phase Transition (dpeaa)DE-He213 Charnaya, E. V. verfasserin aut Shatskaya, Yu. A. verfasserin aut Milinskiy, A. Yu. verfasserin aut Samoilovich, M. I. verfasserin aut Michel, D. verfasserin aut Tien, C. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 53(2011), 6 vom: 10. Juni (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:53 year:2011 number:6 day:10 month:06 https://dx.doi.org/10.1134/S1063783411060059 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_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 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_2056 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 33.60 ASE AR 53 2011 6 10 06 |
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10.1134/S1063783411060059 doi (DE-627)SPR019655495 (SPR)S1063783411060059-e DE-627 ger DE-627 rakwb eng 530 ASE 33.60 bkl Baryshnikov, S. V. verfasserin aut Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. Phase Transition Temperature (dpeaa)DE-He213 Opal Matrix (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Harmonic Amplitude (dpeaa)DE-He213 Ferroelectric Phase Transition (dpeaa)DE-He213 Charnaya, E. V. verfasserin aut Shatskaya, Yu. A. verfasserin aut Milinskiy, A. Yu. verfasserin aut Samoilovich, M. I. verfasserin aut Michel, D. verfasserin aut Tien, C. verfasserin aut Enthalten in Physics of the solid state College Park, Md. : Inst., 1997 53(2011), 6 vom: 10. Juni (DE-627)269017275 (DE-600)1473624-X 1090-6460 nnns volume:53 year:2011 number:6 day:10 month:06 https://dx.doi.org/10.1134/S1063783411060059 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_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 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_2056 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 33.60 ASE AR 53 2011 6 10 06 |
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Baryshnikov, S. V. @@aut@@ Charnaya, E. V. @@aut@@ Shatskaya, Yu. A. @@aut@@ Milinskiy, A. Yu. @@aut@@ Samoilovich, M. I. @@aut@@ Michel, D. @@aut@@ Tien, C. @@aut@@ |
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Baryshnikov, S. V. |
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Baryshnikov, S. V. ddc 530 bkl 33.60 misc Phase Transition Temperature misc Opal Matrix misc Opal Matrice misc Harmonic Amplitude misc Ferroelectric Phase Transition Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
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530 ASE 33.60 bkl Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition Phase Transition Temperature (dpeaa)DE-He213 Opal Matrix (dpeaa)DE-He213 Opal Matrice (dpeaa)DE-He213 Harmonic Amplitude (dpeaa)DE-He213 Ferroelectric Phase Transition (dpeaa)DE-He213 |
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ddc 530 bkl 33.60 misc Phase Transition Temperature misc Opal Matrix misc Opal Matrice misc Harmonic Amplitude misc Ferroelectric Phase Transition |
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ddc 530 bkl 33.60 misc Phase Transition Temperature misc Opal Matrix misc Opal Matrice misc Harmonic Amplitude misc Ferroelectric Phase Transition |
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ddc 530 bkl 33.60 misc Phase Transition Temperature misc Opal Matrix misc Opal Matrice misc Harmonic Amplitude misc Ferroelectric Phase Transition |
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Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
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| title_full |
Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
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Baryshnikov, S. V. |
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Physics of the solid state |
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Baryshnikov, S. V. Charnaya, E. V. Shatskaya, Yu. A. Milinskiy, A. Yu. Samoilovich, M. I. Michel, D. Tien, C. |
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Baryshnikov, S. V. |
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verfasserin |
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effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
| title_auth |
Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
| abstract |
Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. |
| abstractGer |
Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. |
| abstract_unstemmed |
Abstract The temperature dependence of the linear permittivity and the third harmonic generation amplitude of nanocomposites representing nanoporous silica matrices (opal matrix and SBA-15) with triglycine sulfate embedded in pores has been studied in the region of the ferroelectric phase transition. A broadening of the phase transition and an increase its temperature in comparison with bulk triglycine sulfate have been revealed. The latter becomes more significant as the pore size decreases. It has been shown that the nonlinear dielectric properties of nanocomposites near the phase transition differ significantly from the properties of bulk triglycine sulfate. |
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Effect of confined geometry on linear and nonlinear dielectric properties of triglycine sulfate near the phase transition |
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https://dx.doi.org/10.1134/S1063783411060059 |
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Charnaya, E. V. Shatskaya, Yu. A. Milinskiy, A. Yu Samoilovich, M. I. Michel, D. Tien, C. |
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Charnaya, E. V. Shatskaya, Yu. A. Milinskiy, A. Yu Samoilovich, M. I. Michel, D. Tien, C. |
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269017275 |
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| doi_str |
10.1134/S1063783411060059 |
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2024-07-04T02:28:09.913Z |
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| score |
7.4020147 |