Anomalous polarization switching and permanent retention in a ferroelectric ionic conductor

2020 ◽  
Vol 7 (1) ◽  
pp. 263-274 ◽  
Author(s):  
Shuang Zhou ◽  
Lu You ◽  
Apoorva Chaturvedi ◽  
Samuel A. Morris ◽  
Jason S. Herrin ◽  
...  

Ionic conduction in a ferroelectric leads to anomalous polarization switching kinetics but prevents retention failure.

2017 ◽  
Vol 255 (3) ◽  
pp. 1700371 ◽  
Author(s):  
Lian Cui ◽  
Fenghui Cao ◽  
Haiying Cui ◽  
Yuchun Li ◽  
Rui Yang

2007 ◽  
Vol 91 (4) ◽  
pp. 042909 ◽  
Author(s):  
C. A. Nguyen ◽  
P. S. Lee ◽  
N. Ng ◽  
H. Su ◽  
S. G. Mhaisalkar ◽  
...  

2016 ◽  
Vol 49 (15) ◽  
pp. 155304
Author(s):  
Huifen Guo ◽  
Gang Cheng ◽  
Yongliang Yong ◽  
Liben Li

1983 ◽  
Vol 32 (9) ◽  
pp. 1177
Author(s):  
CHEN LI-QUAN ◽  
WANG LIAN-ZHONG ◽  
CHE GUANG-CAN ◽  
WANG GANG

2019 ◽  
Vol 1 (3) ◽  
pp. 275-287 ◽  
Author(s):  
Anastasia Chouprik ◽  
Maxim Spiridonov ◽  
Sergei Zarubin ◽  
Roman Kirtaev ◽  
Vitalii Mikheev ◽  
...  

2020 ◽  
Author(s):  
Katsuhiro Ueno ◽  
Naoyuki Hatada ◽  
Tetsuya Uda

<p>To lower operating temperatures of solid oxide fuel cells (SOFCs), the development of ion-conducting oxides with high conductivity and durability is desired. In this work, we investigated Zr-substituted “Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub>” as an ionic conductor at intermediate temperatures and found that the Zr substitution for Y dramatically improves the phase stability in humidified atmospheres at 300-800 °C. The total electrical conductivity of 20 mol% Zr-substituted Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub> is about 1 mS/cm at 700 °C in dry H­<sub>2</sub> and O<sub>2</sub> atmospheres and the contribution of electronic conduction (both hole and electron) is relatively small compared with Y-doped BaZrO<sub>3</sub> (BZY) and Gd-doped CeO­­<sub>2</sub> (GDC) which are typical intermediate-temperature ionic conductors. Besides, in the Zr-substituted “Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub>” samples, we observed that BaO-rich amorphous phase coexists with the main phase whose composition is estimated to be Ba:(Y+Zr) ~ 2:3. Therefore, the main conducting phase might be Ba-deficient Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub>. The mechanism of the ionic conduction and the improvement of chemical stability has not been revealed yet due to the lack of crystallographic information about the Ba-deficient phase. While we are now working on further investigation, we promptly report the characteristic of the new compound.</p>


2020 ◽  
Author(s):  
Katsuhiro Ueno ◽  
Naoyuki Hatada ◽  
Tetsuya Uda

<p>To lower operating temperatures of solid oxide fuel cells (SOFCs), the development of ion-conducting oxides with high conductivity and durability is desired. In this work, we investigated Zr-substituted “Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub>” as an ionic conductor at intermediate temperatures and found that the Zr substitution for Y dramatically improves the phase stability in humidified atmospheres at 300-800 °C. The total electrical conductivity of 20 mol% Zr-substituted Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub> is about 1 mS/cm at 700 °C in dry H­<sub>2</sub> and O<sub>2</sub> atmospheres and the contribution of electronic conduction (both hole and electron) is relatively small compared with Y-doped BaZrO<sub>3</sub> (BZY) and Gd-doped CeO­­<sub>2</sub> (GDC) which are typical intermediate-temperature ionic conductors. Besides, in the Zr-substituted “Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub>” samples, we observed that BaO-rich amorphous phase coexists with the main phase whose composition is estimated to be Ba:(Y+Zr) ~ 2:3. Therefore, the main conducting phase might be Ba-deficient Ba<sub>3</sub>Y<sub>4</sub>O<sub>9</sub>. The mechanism of the ionic conduction and the improvement of chemical stability has not been revealed yet due to the lack of crystallographic information about the Ba-deficient phase. While we are now working on further investigation, we promptly report the characteristic of the new compound.</p>


Author(s):  
J. Y. Koo ◽  
M. P. Anderson

Tetragonal Zr02 has been used as a toughening phase in a large number of ceramic materials. In this system, complex diffraction phenomena have been observed and an understanding of the origin of the diffraction effects provides important information on the nature of transformation toughening, ionic conduction, and phase destabilization. This paper describes the results of an electron diffraction study of Y203-stabilized, tetragonal Zr02 polycrystals (Y-TZP).Thin foils from the bulk Y-TZP sample were prepared by careful grinding and cryo ion-milling. They were carbon coated and examined in a Philips 400T/FEG microscope. Fig. 1 shows a typical bright field image of the 100% tetragonal(t) Zr02. The tetragonal structure was identified by both bulk x-ray diffraction and convergent beam electron diffraction (Fig. 2. A local region within a t-Zr02 grain was subjected to an intense electron beam irradiation which caused partial martensitic transformation of the t-Zr02 to monoclinic(m) symmetry, Fig. 3 A.


Author(s):  
R. B. Queenan ◽  
P. K. Davies

Na ß“-alumina (Na1.67Mg67Al10.33O17) is a non-stoichiometric sodium aluminate which exhibits fast ionic conduction of the Na+ ions in two dimensions. The Na+ ions can be exchanged with a variety of mono-, di-, and trivalent cations. The resulting exchanged materials also show high ionic conductivities.Considerable interest in the Na+-Nd3+-ß“-aluminas has been generated as a result of the recent observation of lasing in the pulsed and cw modes. A recent TEM investigation on a 100% exchanged Nd ß“-alumina sample found evidence for the intergrowth of two different structure types. Microdiffraction revealed an ordered phase coexisting with an apparently disordered phase, in which the cations are completely randomized in two dimensions. If an order-disorder transition is present then the cooling rates would be expected to affect the microstructures of these materials which may in turn affect the optical properties. The purpose of this work was to investigate the affect of thermal treatments upon the micro-structural and optical properties of these materials.


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