2013
DOI: 10.1016/j.actamat.2012.11.044
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Grain boundary complexion transitions in WO3- and CuO-doped TiO2 bicrystals

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Cited by 33 publications
(15 citation statements)
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“…Lastly, we should also recognize the possibility that some of these IGFs exhibit discrete (instead of continuous) thickness (to form Dillon-Harmer GB complexions [23,41]) for certain specific GBs, e.g., some special GBs with low-index grain surfaces, as shown in a prior study for a (001) // (100) GB in a (CuO + SiO 2 ) doped TiO 2 bicrystal specimen [41]. The origin of the discrete thicknesses and the formation of Dillon-Harmer GB complexions can be explained in the same interfacial thermodynamic framework discussed above via incorporating (adding) an oscillatory structural interaction (as a result of a fixed, finite, atomic size using a hard-sphere approximation) in Eq.…”
Section: An Interfacial Thermodynamic Model and The Computed Gb  Diamentioning
confidence: 99%
See 1 more Smart Citation
“…Lastly, we should also recognize the possibility that some of these IGFs exhibit discrete (instead of continuous) thickness (to form Dillon-Harmer GB complexions [23,41]) for certain specific GBs, e.g., some special GBs with low-index grain surfaces, as shown in a prior study for a (001) // (100) GB in a (CuO + SiO 2 ) doped TiO 2 bicrystal specimen [41]. The origin of the discrete thicknesses and the formation of Dillon-Harmer GB complexions can be explained in the same interfacial thermodynamic framework discussed above via incorporating (adding) an oscillatory structural interaction (as a result of a fixed, finite, atomic size using a hard-sphere approximation) in Eq.…”
Section: An Interfacial Thermodynamic Model and The Computed Gb  Diamentioning
confidence: 99%
“…The origin of the discrete thicknesses and the formation of Dillon-Harmer GB complexions can be explained in the same interfacial thermodynamic framework discussed above via incorporating (adding) an oscillatory structural interaction (as a result of a fixed, finite, atomic size using a hard-sphere approximation) in Eq. (3) or the interfacial coefficient f(h) [31,[41][42][43].…”
Section: An Interfacial Thermodynamic Model and The Computed Gb  Diamentioning
confidence: 99%
“…Recently, Harmer et al 3) showed a structural disordering of grain boundary caused by the excess CuO for a CuOdoped TiO 2 bicrystal. The disordering enhances the grain boundary diffusion along and across the grain boundary.…”
Section: Introductionmentioning
confidence: 99%
“…vs. T") observed by HRTEM. Lastly, we should also recognize the possibility that some of these IGFs exhibit discrete (instead of continuous) thickness (to form Dillon-Harmer GB complexions [23,41]) for certain specific GBs, e.g., some special GBs with low-index grain surfaces, as shown in a prior study for a (001)//(100) GB in a (CuO þ SiO 2 ) doped TiO 2 bicrystal specimen [41]. The origin of the discrete thicknesses and the formation of Dillon-Harmer GB complexions can be explained in the same interfacial thermodynamic framework discussed above via incorporating (adding) an oscillatory structural interaction (as a result of a fixed, finite, atomic size using a hard-sphere approximation) in Eq.…”
Section: An Interfacial Thermodynamic Model and The Computed Gb L Diamentioning
confidence: 99%