1996
DOI: 10.1016/0921-5107(96)01584-x
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Numerical simulation of the defect chemistry and electrostatics at grain boundaries in titanate ceramics

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Cited by 33 publications
(18 citation statements)
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“…Figures 8(a) and (b) shows a schematic diagram of the profile of acceptor dopant (A′) and the grain boundary donor‐like surface charge (D • ) for the fine‐ and coarse‐grain samples, respectively. It is well known that acceptor dopants have a strong tendency to segregate in the grain boundary region due to a positive grain boundary surface charge (D • ), that is, high temperature space charge potential 29–31 …”
Section: Resultsmentioning
confidence: 99%
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“…Figures 8(a) and (b) shows a schematic diagram of the profile of acceptor dopant (A′) and the grain boundary donor‐like surface charge (D • ) for the fine‐ and coarse‐grain samples, respectively. It is well known that acceptor dopants have a strong tendency to segregate in the grain boundary region due to a positive grain boundary surface charge (D • ), that is, high temperature space charge potential 29–31 …”
Section: Resultsmentioning
confidence: 99%
“…When the grain growth does not occur at low sintering temperatures most of the added acceptor dopants will be incorporated in the grain boundary region ([A′] GB ) and the solid state diffusion of dopants into the interior of grain is usually very limited 32 . The acceptors incorporated in the grain boundary region ([A′] GB ) are supposed to be charge‐compensated by part of the grain boundary donor like surface charges ([D • ]) 15,30 . Therefore, it would limit the ionic compensation of [A′]≈2[V O •• ] that dominates the conductivity in the coarse‐grain materials.…”
Section: Resultsmentioning
confidence: 99%
“…Parts of the cation vacancies in BaTiO 3 or SrTiO 3 may exist as partially ionized states ͑V Ba Ј , V Sr Ј , and V Ti ٞ͒ at high temperatures, and become fully ionized states (V Ba Љ , V Sr Љ , and V Ti ЉЉ͒ trapping electrons when specimens are cooled to room temperature. [7][8][9][10][11]22 The reported values of the cation vacancies' energy levels from the bottom of the conduction band are 1.8 or 1.3 eV for V Ba Љ , 1.3 or 1.14 eV for V Ti ЉЉ etc. 20,[23][24][25] The bulk Fermi energy level is expressed as…”
Section: B Theoretical Calculation Of Electron and Each Defect Concementioning
confidence: 98%
“…With respect to C GB , the procedure is described by Hagenbeck et al 11 In the subsequent sections of this paper, the impact of R GB will be revealed.…”
Section: (1) Electrostatics Of the Gb Regionmentioning
confidence: 99%