Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics
Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Fujii, Ichiro [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2016 |
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| Systematik: |
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| Anmerkung: |
© The Materials Research Society 2015 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of materials research - Springer International Publishing, 1986, 31(2016), 1 vom: 01. Jan., Seite 28-35 |
|---|---|
| Übergeordnetes Werk: |
volume:31 ; year:2016 ; number:1 ; day:01 ; month:01 ; pages:28-35 |
| Links: |
|---|
| DOI / URN: |
10.1557/jmr.2015.315 |
|---|
| Katalog-ID: |
OLC2123224065 |
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| 245 | 1 | 0 | |a Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics |
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| 520 | |a Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. | ||
| 700 | 1 | |a Ito, Yutaka |4 aut | |
| 700 | 1 | |a Suzuki, Teppei |4 aut | |
| 700 | 1 | |a Wada, Takahiro |4 aut | |
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10.1557/jmr.2015.315 doi (DE-627)OLC2123224065 (DE-He213)jmr.2015.315-p DE-627 ger DE-627 rakwb eng 670 VZ VA 5350 VZ rvk Fujii, Ichiro verfasserin aut Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Materials Research Society 2015 Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. Ito, Yutaka aut Suzuki, Teppei aut Wada, Takahiro aut Enthalten in Journal of materials research Springer International Publishing, 1986 31(2016), 1 vom: 01. Jan., Seite 28-35 (DE-627)129206288 (DE-600)54876-5 (DE-576)01445744X 0884-2914 nnns volume:31 year:2016 number:1 day:01 month:01 pages:28-35 https://doi.org/10.1557/jmr.2015.315 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_21 GBV_ILN_24 GBV_ILN_70 GBV_ILN_2005 GBV_ILN_2020 GBV_ILN_4126 GBV_ILN_4319 GBV_ILN_4323 VA 5350 AR 31 2016 1 01 01 28-35 |
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10.1557/jmr.2015.315 doi (DE-627)OLC2123224065 (DE-He213)jmr.2015.315-p DE-627 ger DE-627 rakwb eng 670 VZ VA 5350 VZ rvk Fujii, Ichiro verfasserin aut Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Materials Research Society 2015 Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. Ito, Yutaka aut Suzuki, Teppei aut Wada, Takahiro aut Enthalten in Journal of materials research Springer International Publishing, 1986 31(2016), 1 vom: 01. Jan., Seite 28-35 (DE-627)129206288 (DE-600)54876-5 (DE-576)01445744X 0884-2914 nnns volume:31 year:2016 number:1 day:01 month:01 pages:28-35 https://doi.org/10.1557/jmr.2015.315 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_21 GBV_ILN_24 GBV_ILN_70 GBV_ILN_2005 GBV_ILN_2020 GBV_ILN_4126 GBV_ILN_4319 GBV_ILN_4323 VA 5350 AR 31 2016 1 01 01 28-35 |
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10.1557/jmr.2015.315 doi (DE-627)OLC2123224065 (DE-He213)jmr.2015.315-p DE-627 ger DE-627 rakwb eng 670 VZ VA 5350 VZ rvk Fujii, Ichiro verfasserin aut Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Materials Research Society 2015 Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. Ito, Yutaka aut Suzuki, Teppei aut Wada, Takahiro aut Enthalten in Journal of materials research Springer International Publishing, 1986 31(2016), 1 vom: 01. Jan., Seite 28-35 (DE-627)129206288 (DE-600)54876-5 (DE-576)01445744X 0884-2914 nnns volume:31 year:2016 number:1 day:01 month:01 pages:28-35 https://doi.org/10.1557/jmr.2015.315 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_21 GBV_ILN_24 GBV_ILN_70 GBV_ILN_2005 GBV_ILN_2020 GBV_ILN_4126 GBV_ILN_4319 GBV_ILN_4323 VA 5350 AR 31 2016 1 01 01 28-35 |
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10.1557/jmr.2015.315 doi (DE-627)OLC2123224065 (DE-He213)jmr.2015.315-p DE-627 ger DE-627 rakwb eng 670 VZ VA 5350 VZ rvk Fujii, Ichiro verfasserin aut Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Materials Research Society 2015 Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. Ito, Yutaka aut Suzuki, Teppei aut Wada, Takahiro aut Enthalten in Journal of materials research Springer International Publishing, 1986 31(2016), 1 vom: 01. Jan., Seite 28-35 (DE-627)129206288 (DE-600)54876-5 (DE-576)01445744X 0884-2914 nnns volume:31 year:2016 number:1 day:01 month:01 pages:28-35 https://doi.org/10.1557/jmr.2015.315 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_21 GBV_ILN_24 GBV_ILN_70 GBV_ILN_2005 GBV_ILN_2020 GBV_ILN_4126 GBV_ILN_4319 GBV_ILN_4323 VA 5350 AR 31 2016 1 01 01 28-35 |
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10.1557/jmr.2015.315 doi (DE-627)OLC2123224065 (DE-He213)jmr.2015.315-p DE-627 ger DE-627 rakwb eng 670 VZ VA 5350 VZ rvk Fujii, Ichiro verfasserin aut Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © The Materials Research Society 2015 Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. Ito, Yutaka aut Suzuki, Teppei aut Wada, Takahiro aut Enthalten in Journal of materials research Springer International Publishing, 1986 31(2016), 1 vom: 01. Jan., Seite 28-35 (DE-627)129206288 (DE-600)54876-5 (DE-576)01445744X 0884-2914 nnns volume:31 year:2016 number:1 day:01 month:01 pages:28-35 https://doi.org/10.1557/jmr.2015.315 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC GBV_ILN_21 GBV_ILN_24 GBV_ILN_70 GBV_ILN_2005 GBV_ILN_2020 GBV_ILN_4126 GBV_ILN_4319 GBV_ILN_4323 VA 5350 AR 31 2016 1 01 01 28-35 |
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Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics |
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(DE-627)OLC2123224065 (DE-He213)jmr.2015.315-p |
| title_full |
Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics |
| author_sort |
Fujii, Ichiro |
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Journal of materials research |
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Journal of materials research |
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eng |
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600 - Technology |
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marc |
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2016 |
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txt |
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28 |
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Fujii, Ichiro Ito, Yutaka Suzuki, Teppei Wada, Takahiro |
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31 |
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670 VZ VA 5350 VZ rvk |
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Fujii, Ichiro |
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10.1557/jmr.2015.315 |
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670 |
| title_sort |
ferroelectric and piezoelectric properties of ($ bi_{1/2} $$ na_{1/2} $)$ tio_{3} $–$ bifeo_{3} $ ceramics |
| title_auth |
Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics |
| abstract |
Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. © The Materials Research Society 2015 |
| abstractGer |
Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. © The Materials Research Society 2015 |
| abstract_unstemmed |
Abstract (1 − x) ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–x $ BiFeO_{3} $ (x = 0–0.9) ceramics were prepared and the ferroelectric and piezoelectric properties along with the crystal structure were investigated. The crystal system of the ceramics was rhombohedral with the R 3 c symmetry throughout the compositions. The rhombohedral distortion (90° − α), where α was the rhombohedral angle based on a pseudocubic perovskite cell, was minimized at x = 0.1, while the lattice constant increased linearly with x. Saturated ferroelectric polarization-electric field hysteresis loops were observed at x = 0–0.6. The coercive field was reduced at x = 0.05–0.2 and the high remanent polarization of 30–35 µC/$ cm^{2} $ was obtained at x = 0–0.4. The piezoelectric constants d33 and d33* (which was calculated from a unipolar strain–electric field curve) were maximized to 93 pC/N at x = 0.1 and 183 pm/V at x = 0.05, respectively. These results suggested that the increase in the piezoelectric properties was associated with the reduction in the rhombohedral distortion, which could be useful in development of high performance lead-free piezoelectric materials. © The Materials Research Society 2015 |
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| title_short |
Ferroelectric and piezoelectric properties of ($ Bi_{1/2} $$ Na_{1/2} $)$ TiO_{3} $–$ BiFeO_{3} $ ceramics |
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https://doi.org/10.1557/jmr.2015.315 |
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Ito, Yutaka Suzuki, Teppei Wada, Takahiro |
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Ito, Yutaka Suzuki, Teppei Wada, Takahiro |
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| up_date |
2024-07-03T17:03:34.311Z |
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