2013
DOI: 10.1063/1.4818475
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First-principles calculations of the electronic structure and defects of Al2O3

Abstract: We present first-principles calculations of the electronic structure of the oxygen vacancies in θ-Al2O3 and amorphous Al2O3 (am-Al2O3) using the screened exchange (sX) hybrid functional. The sX hybrid functional can give correct band gap for both phases. The defect energy levels depend strongly on the charge state, with negative defects lying deep in conduction band. Transition levels between different charge states were determined. The 3-fold coordinated O vacancy dominates in θ-Al2O3 due to the higher format… Show more

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Cited by 29 publications
(40 citation statements)
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“…[1][2][3][4][5] For this reason, native defects in Al 2 O 3 have been the subject of extensive experimental and theoretical investigations aiming at verifying the presence of deep-level traps in the dielectric. [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] The vast majority of theoretical studies performed so far have focused on crystalline phases of Al 2 O 3 . However, Al 2 O 3 in MOS devices is usually deposited via atomic layer deposition, which results in an amorphous phase with electronic properties differing considerably from those of crystalline phases.…”
mentioning
confidence: 99%
“…[1][2][3][4][5] For this reason, native defects in Al 2 O 3 have been the subject of extensive experimental and theoretical investigations aiming at verifying the presence of deep-level traps in the dielectric. [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] The vast majority of theoretical studies performed so far have focused on crystalline phases of Al 2 O 3 . However, Al 2 O 3 in MOS devices is usually deposited via atomic layer deposition, which results in an amorphous phase with electronic properties differing considerably from those of crystalline phases.…”
mentioning
confidence: 99%
“…The above model of defect energy alternating with charging status is supported by the first-principle calculation in Al 2 O 3 and ab initio calculations in GeO 2 [29][30][31], suggesting that EADs are intrinsic in Al 2 O 3 /GeO 2 /Ge structure.…”
Section: A Differences In Defect Energy Distribution In Ge and Simentioning
confidence: 70%
“…43 Similarly, for α-Al 2 O 3 , they reported most interestingly in our terms, that V O and Al i are the dominant defect types located at ∼ 4.1 eV and ∼ 1.9 eV below CBM, respectively, and also transition levels due to Al dangling bonds at ∼ 2.8 eV below CBM. 44 45 However, the latter value also suffered from an underestimation of the bandgap being only 6.2 eV. As we expect to get primarily amorphous alumina from our plasma oxidation process, this latter value is the most important reference here.…”
Section: Kmc-results For Al/alo X /Aumentioning
confidence: 98%
“…Moreover, our barrier height must only be increased by ∼0.15 eV to obtain the "effective" value from experiments, as stated already by Weinberg earlier. 29 45 and the plasma process is likely to form an amorphous oxide. Another possible explanation would be the forming of alumina polymorphs, including several phases of Al 2 O 3 , which exhibit also several energies for the dominant V O or Al i , as cited above.…”
Section: Kmc-results For Al/alo X /Aumentioning
confidence: 99%