Relevant bibliographies by topics / Ferroelectric-loop

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  1. Journal articles

Academic literature on the topic 'Ferroelectric-loop'

Author: Grafiati
Published: 6 September 2023

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Journal articles on the topic "Ferroelectric-loop"

1

Nishimura, Kiyoshi, Takaaki Fuchikami, and Kazuhiro Hoshiba. "A ferroelectric hysteresis loop model." Electronics and Communications in Japan (Part II: Electronics) 80, no. 10 (1997): 1–8. http://dx.doi.org/10.1002/(sici)1520-6432(199710)80:10<1::aid-ecjb1>3.0.co;2-c.

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2

Kim, Bora, Daehee Seol, Shinbuhm Lee, Ho Nyung Lee, and Yunseok Kim. "Ferroelectric-like hysteresis loop originated from non-ferroelectric effects." Applied Physics Letters 109, no. 10 (2016): 102901. http://dx.doi.org/10.1063/1.4962387.

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3

Unruan, Muangjai, R. Wongmaneerung, Yongyut Laosiritaworn, Supon Ananta, and Rattikorn Yimnirun. "Changes in Ferroelectric Properties of 0.7PMN–0.3PT Ceramic with Compressive Stress." Advanced Materials Research 55-57 (August 2008): 277–80. http://dx.doi.org/10.4028/www.scientific.net/amr.55-57.277.

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In this work, effects of compressive stress on the ferroelectric properties of 0.7PMN–0.3PT ceramics were investigated. The ceramics with the formula (0.7)Pb(Mg1/3Nb2/3)O3-(0.3)PbTiO were prepared by a conventional mixed-oxide method. The ferroelectric properties under compressive stress were observed at stress up to 80 MPa using a compressometer in conjunction with a modified Sawyer-Tower circuit. The results showed that applied stress had a significant influence on the ferroelectric properties of 0.7PMN–0.3PT ceramics. Ferroelectric characteristics, i.e. the area of the ferroelectric hysteresis (P-E) loop, the saturation polarization (Psat), the remanent polarization (Pr) and loop squareness (Rsq), decreased with increasing compressive stress, while the coercive field (Ec) remained relatively constant. Stress-induced domain wall motion suppression and non-180oC ferroelectric domain switching processes are responsible for the changes observed.
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4

Kumar, Neeraj, and Rabinder Nath. "Ferroelectric and Electrical Properties of Potassium Nitrate Thin Composite Layers." Advanced Materials Research 403-408 (November 2011): 607–17. http://dx.doi.org/10.4028/www.scientific.net/amr.403-408.607.

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The ferroelectric and electrical properties of potassium nitrate (KNO3): polyvinylidene fluoride (PVDF) composite layers prepared by melt press method have been studied. The stability of ferroelectric phase (phase –III) of potassium nitrate (KNO3) in the composite layers at room temperature have been analyzed. The temperature dependence of ferroelectric hysteresis loop (P-E) characteristics have been investigated in the composite layers. The electrical conductivity (σ) and dielectric behaviour of composite layers have been characterized. The conductivity and dielectric variation with temperature during heating and cooling modes has been found to provide the knowledge of phase transition in the composite. The capacitance –-voltage (C-V) and conductance - voltage (G-V) characteristics clearly show the ferroelectric butterfly loop, which is attributed to the features of ferroelectricity in the composite layers at room temperature. The coexistence of ferroelectric phase (phase III) with paraelectric phase (phase II) has also been observed at room temperature in the composite layers during dielectric and conductivity measurements.
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5

Pintilie, L., and M. Alexe. "Ferroelectric-like hysteresis loop in nonferroelectric systems." Applied Physics Letters 87, no. 11 (2005): 112903. http://dx.doi.org/10.1063/1.2045543.

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6

Itskovsky, M. A. "Pyroelectric hysteresis loop at ferroelectric phase transition." Journal of Applied Physics 85, no. 8 (1999): 4256–58. http://dx.doi.org/10.1063/1.370339.

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7

Cui, Lian, Haiying Cui, and Yuchun Li. "Dynamic hysteresis loop in a ferroelectric heterostructure." Chinese Journal of Physics 56, no. 1 (2018): 185–92. http://dx.doi.org/10.1016/j.cjph.2017.12.009.

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8

Nishimura, Kiyoshi. "Ferroelectric hysteresis loop model of imprint properties." Electronics and Communications in Japan (Part II: Electronics) 82, no. 10 (1999): 27–34. http://dx.doi.org/10.1002/(sici)1520-6432(199910)82:10<27::aid-ecjb4>3.0.co;2-j.

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9

Kour, P., and S. K. Sinha. "Studies of Sr2+ ion substitution on ferroelectric and piezoelectric properties of PZT nanocrystalline." Cerâmica 59, no. 349 (2013): 34–38. http://dx.doi.org/10.1590/s0366-69132013000100004.

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Strontium substituted lead zirconate titanate nanocrystalline material with chemical formula Pb0.95Sr0.05 (Zr0.52Ti0.48) O3 have been synthesized by alkoxide based sol gel method. The product was characterized by differential thermal analysis, thermogravimetric analysis, powder X-ray diffraction and scanning electron microscopy. The ferroelectric hysteresis loop measurement was carried out at room temperature using ferroelectric loop tracer over a field range of 20 kV/cm. The remanent polarization Pr, saturation polarization Pmax and coercive field Ec were 12.97 µC/cm², 30.52 µC/cm² and 6.5 kV/cm respectively. The piezoelectric coefficient d33 was measured with the variation of polling field.
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10

KASHYAP, RAMAN, TANUJ DHAWAN, PRIKSHIT GAUTAM, O. P. THAKUR, N. C. MEHRA, and R. P. TANDON. "EFFECT OF PROCESSING CONDITIONS ON ELECTRICAL PROPERTIES OF CaCu3Ti4O12 CERAMICS." Modern Physics Letters B 24, no. 12 (2010): 1267–73. http://dx.doi.org/10.1142/s021798491002327x.

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CaCu 3 Ti 4 O 12 ( CCTO ) ceramics were prepared by the solid-state reaction route. Effect of sintering time was studied on the polarization (P) versus electric field (E) behavior. Unlike conventional ferroelectric hysteresis loop, PE hysteresis behavior in CCTO ceramics was observed to exhibit ferroelectric-like loop where polarization does not saturate but gives a maximum value. Remnant polarization and maximum polarization was observed to increase with sintering time. Current (I)–voltage (V) characteristics shows a nonlinear behavior making them useful for varistor applications. Coefficient of non-linearity (α) is also found to depend on sintering duration.
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