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Volumn 92, Issue 4, 2015, Pages

Oxygen deficiency in TiO2: Similarities and differences between the Ti self-interstitial and the O vacancy in bulk rutile and anatase

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EID: 84937899433     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.92.045204     Document Type: Article
Times cited : (62)

References (79)
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    • note
    • In ionic crystals with strong electron-phonon coupling (such as many II-VI semiconductors, alkali halides, oxides, etc.), a charge carrier is dressed in a cloud of virtual phonons and can be considered as a new composite particle, called a polaron. If the phonon cloud corresponds to a strong local relaxation of the lattice, the carrier is essentially trapped in a so-called "small polaron" state and transport can proceed only through thermally activated hopping.
  • 2
    • 84937833731 scopus 로고    scopus 로고
    • note
    • N.B.: we use, e.g., (Equation presented) as notation for the oxidation state, while (Equation presented) denotes an interstitial Ti atom in the triply negative charged state.
  • 5
    • 84937911313 scopus 로고    scopus 로고
    • T. Sarkar, K. Gopinadhan, Zh. Jun, S. Saha, J. M. D. Coey, Y. P. Feng, A. Ariando, and T. Venkatesan (unpublished)
    • T. Sarkar, K. Gopinadhan, Zh. Jun, S. Saha, J. M. D. Coey, Y. P. Feng, A. Ariando, and T. Venkatesan (unpublished).
  • 15
    • 84937895808 scopus 로고    scopus 로고
    • note
    • HF exchange gives a total energy, which is a concave, while local/semi-local DFT is a convex function of the fractional occupation numbers. Proper mixing may lead to linear behavior, with the correlation- and the self-interaction error cancelling each other.
  • 46
    • 84937945850 scopus 로고    scopus 로고
    • note
    • In the Brillouin-zone of orthogonal lattices, this is the point where a tight binding band of the interacting defects is closest to the level of an isolated defect.
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    • 0034339280 scopus 로고    scopus 로고
    • P. Deák, Phys. Status Solidi B 217, 9 (2000). 10.1002/(SICI)1521-3951(200001)217:1%3C9::AID-PSSB9%3E3.0.CO;2-6
    • (2000) Phys. Status Solidi B , vol.217 , pp. 9
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    • D. C. Cronemeyer, Phys. Rev. 113, 1222 (1959). 10.1103/PhysRev.113.1222
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    • note
    • Note that the first and second vertical ionization energies of the EMT states of (Equation presented) are computed to be equal (cf. Table I), and the first adiabatic charge transition in Fig. 5 is (Equation presented). The accuracy of the supercell method is quite limited, in case of shallow EMT states.
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    • M. J. Jackman, P. Deák, K. L. Syres, J. Adell, B. Thiagarajan, A. Levy and A. G. Thomas, arXiv:1406.3385 [cond-mat.mtrl-sci]
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.