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First principles phase diagram calculations for the octahedral-interstitial system αTiOX, 0≤X≤1/2 AITranslate

National Institute of Standards and Technology (NIST); Brown University
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Publisher: Elsevier
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Abstract AITranslate

First principles based phase diagram calculations were performed for the hexagonal closest packed octahedral-interstitial solid solution system α TiO X , or α Ti [ ] 1 − X O X ([ ]=Vacancy; 0 ≤ X ≤ 1 / 2 ), by the cluster expansion (CE) method. The predicted diagram has ordered ground-state (GS) phases at: X=0 (hcp α Ti , P63mmc); X=1/6 ( Ti 6 O : P 3 ¯ 1 c , R3, R 3 ¯ ); X ≈ 1 / 3 ( Ti 3 O : R 3 ¯ , P 3 ¯ 1 c , R 3 ¯ ′ ); and X=1/2 ( Ti 2 O : Pbcn; contrary to previous reports that it is anti-CdI2). Both at X= 1/6 and X= 1/3 density functional theory (DFT) calculations predict at least triply degenerate GS (three structure energies at each composition that are within ≈ 0.001 eV; i.e. within DFT error). In the CE, this leads to exactly triply degenerate GS at both compositions. The calculated phase diagram includes a broad field between Ti 6 O and Ti 3 O in which the stable phases have layer-structures that are related to the anti-CdI2-structure. It appears that disordering of the Ti 6 O - and Ti 3 O -GS involves cascades of first-order transitions that are suggestive of Devil`s staircases. Highlights ▸ First principles phase diagram calculation for the suboxide system Ti [ ] 1 − X O X ; 0 ≲ X ≲ 1 / 2 . ▸ The prediction of Devil`s staircase order–disorder behavior in Ti6O and Ti3O. ▸ The prediction of a Ti2O ground-state that is not CdI2-related. ▸ The prediction that no CdI2-related phase is stable at elevated temperature.

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DOI:https://doi.org/10.1016/j.calphad.2012.09.004

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First principles based phase diagram calculations were performed for the hexagonal closest packed octahedral-interstitial solid solution system α TiO X , or α Ti [ ] 1 − X O X ([ ]=Vacancy; 0 ≤ X ≤ 1 / 2 ), by the cluster expansion (CE) method. The predicted diagram has ordered ground-state (GS) phases at: X=0 (hcp α Ti , P63mmc); X=1/6 ( Ti 6 O : P 3 ¯ 1 c , R3, R 3 ¯ ); X ≈ 1 / 3 ( Ti 3 O : R 3 ¯ , P 3 ¯ 1 c , R 3 ¯ ′ ); and X=1/2 ( Ti 2 O : Pbcn; contrary to previous reports that it is anti-CdI2). Both at X= 1/6 and X= 1/3 density functional theory (DFT) calculations predict at least triply degenerate GS (three structure energies at each composition that are within ≈ 0.001 eV; i.e. within DFT error). In the CE, this leads to exactly triply degenerate GS at both compositions. The calculated phase diagram includes a broad field between Ti 6 O and Ti 3 O in which the stable phases have layer-structures that are related to the anti-CdI2-structure. It appears that disordering of the Ti 6 O - and Ti 3 O -GS involves cascades of first-order transitions that are suggestive of Devil`s staircases. Highlights ▸ First principles phase diagram calculation for the suboxide system Ti [ ] 1 − X O X ; 0 ≲ X ≲ 1 / 2 . ▸ The prediction of Devil`s staircase order–disorder behavior in Ti6O and Ti3O. ▸ The prediction of a Ti2O ground-state that is not CdI2-related. ▸ The prediction that no CdI2-related phase is stable at elevated temperature.

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GB/T 7714-2015 [1] Benjamin Paul Burton, Axel van de Walle. Calphad, 2012(39). DOI:10.1016/j.calphad.2012.09.004.
MLA [1] Benjamin Paul Burton, and Axel van de Walle. Calphad, no. 39, 2012, https://doi.org/10.1016/j.calphad.2012.09.004.
APA [1] Benjamin Paul Burton, & Axel van de Walle. (2012). Calphad(39). https://doi.org/10.1016/j.calphad.2012.09.004
IEEE [1] Benjamin Paul Burton and Axel van de Walle, Calphad, no. 39, 2012, doi: 10.1016/j.calphad.2012.09.004.