3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal
Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-anti...
Ausführliche Beschreibung
Autor*in: |
Novik, V. K. [verfasserIn] |
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Artikel |
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Sprache: |
Englisch |
Erschienen: |
2013 |
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Anmerkung: |
© Pleiades Publishing, Ltd. 2013 |
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Übergeordnetes Werk: |
Enthalten in: Physics of the solid state - Springer US, 1993, 55(2013), 8 vom: Aug., Seite 1668-1675 |
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Übergeordnetes Werk: |
volume:55 ; year:2013 ; number:8 ; month:08 ; pages:1668-1675 |
Links: |
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DOI / URN: |
10.1134/S1063783413080222 |
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OLC204073273X |
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520 | |a Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. | ||
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10.1134/S1063783413080222 doi (DE-627)OLC204073273X (DE-He213)S1063783413080222-p DE-627 ger DE-627 rakwb eng 530 VZ Novik, V. K. verfasserin aut 3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. Domain Wall Tetragonal Phase Ferroelectric Phase Paraelectric Phase Ferroelectric Phase Transition Lotonov, A. M. aut Gavrilova, N. D. aut Enthalten in Physics of the solid state Springer US, 1993 55(2013), 8 vom: Aug., Seite 1668-1675 (DE-627)16567332X (DE-600)1159011-7 (DE-576)038490706 1063-7834 nnns volume:55 year:2013 number:8 month:08 pages:1668-1675 https://doi.org/10.1134/S1063783413080222 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 55 2013 8 08 1668-1675 |
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10.1134/S1063783413080222 doi (DE-627)OLC204073273X (DE-He213)S1063783413080222-p DE-627 ger DE-627 rakwb eng 530 VZ Novik, V. K. verfasserin aut 3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. Domain Wall Tetragonal Phase Ferroelectric Phase Paraelectric Phase Ferroelectric Phase Transition Lotonov, A. M. aut Gavrilova, N. D. aut Enthalten in Physics of the solid state Springer US, 1993 55(2013), 8 vom: Aug., Seite 1668-1675 (DE-627)16567332X (DE-600)1159011-7 (DE-576)038490706 1063-7834 nnns volume:55 year:2013 number:8 month:08 pages:1668-1675 https://doi.org/10.1134/S1063783413080222 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 55 2013 8 08 1668-1675 |
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10.1134/S1063783413080222 doi (DE-627)OLC204073273X (DE-He213)S1063783413080222-p DE-627 ger DE-627 rakwb eng 530 VZ Novik, V. K. verfasserin aut 3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. Domain Wall Tetragonal Phase Ferroelectric Phase Paraelectric Phase Ferroelectric Phase Transition Lotonov, A. M. aut Gavrilova, N. D. aut Enthalten in Physics of the solid state Springer US, 1993 55(2013), 8 vom: Aug., Seite 1668-1675 (DE-627)16567332X (DE-600)1159011-7 (DE-576)038490706 1063-7834 nnns volume:55 year:2013 number:8 month:08 pages:1668-1675 https://doi.org/10.1134/S1063783413080222 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 55 2013 8 08 1668-1675 |
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10.1134/S1063783413080222 doi (DE-627)OLC204073273X (DE-He213)S1063783413080222-p DE-627 ger DE-627 rakwb eng 530 VZ Novik, V. K. verfasserin aut 3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. Domain Wall Tetragonal Phase Ferroelectric Phase Paraelectric Phase Ferroelectric Phase Transition Lotonov, A. M. aut Gavrilova, N. D. aut Enthalten in Physics of the solid state Springer US, 1993 55(2013), 8 vom: Aug., Seite 1668-1675 (DE-627)16567332X (DE-600)1159011-7 (DE-576)038490706 1063-7834 nnns volume:55 year:2013 number:8 month:08 pages:1668-1675 https://doi.org/10.1134/S1063783413080222 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 55 2013 8 08 1668-1675 |
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10.1134/S1063783413080222 doi (DE-627)OLC204073273X (DE-He213)S1063783413080222-p DE-627 ger DE-627 rakwb eng 530 VZ Novik, V. K. verfasserin aut 3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2013 Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. Domain Wall Tetragonal Phase Ferroelectric Phase Paraelectric Phase Ferroelectric Phase Transition Lotonov, A. M. aut Gavrilova, N. D. aut Enthalten in Physics of the solid state Springer US, 1993 55(2013), 8 vom: Aug., Seite 1668-1675 (DE-627)16567332X (DE-600)1159011-7 (DE-576)038490706 1063-7834 nnns volume:55 year:2013 number:8 month:08 pages:1668-1675 https://doi.org/10.1134/S1063783413080222 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 55 2013 8 08 1668-1675 |
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3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal |
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Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. © Pleiades Publishing, Ltd. 2013 |
abstractGer |
Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. © Pleiades Publishing, Ltd. 2013 |
abstract_unstemmed |
Abstract The 3D dependences ɛ′(log f, T) and tanδ(logf, T) of a perfect $ BaTiO_{3} $ single crystal grown by the Remeika method have been studied in the ranges f = 1–2 × $ 10^{7} $ Hz and T = −80–130°C. These dependences characterize a transition from the paraelectric phase (121.5°C) as a near-antiferroelectric transition followed by the transition to the tetragonal phase at ∼79.5°C. According to a number of signs, the range 121.5–79.5°C corresponds to a metastable phase typical of first-order phase transitions. The unexpected result of this work has been discussed with invoking the hypothesis on the $ BaTiO_{3} $ structure in the paraelectric phase, according to which it consists of three antiferroelectric states oriented along the crystallographic axes. Using the dielectric properties of $ BaTiO_{3} $ as an example, the method of direct correct determination of the temperatures of the structural transformations from the anomaly of tanδ(logf, T) has also been demonstrated. © Pleiades Publishing, Ltd. 2013 |
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title_short |
3D dependence of the dielectric dispersion in a $ BaTiO_{3} $ single crystal |
url |
https://doi.org/10.1134/S1063783413080222 |
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Lotonov, A. M. Gavrilova, N. D. |
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Lotonov, A. M. Gavrilova, N. D. |
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10.1134/S1063783413080222 |
up_date |
2024-07-04T03:01:00.850Z |
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