2021
DOI: 10.1103/physrevb.104.035128
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Theoretical evidence for the Peierls transition in NbO2

Abstract: We show by advanced electronic structure calculations that NbO 2 essentially is a Peierls-type material. After simulating the rutile as well as the body-centered tetragonal phase with the Bethe-Salpeter equation, we are able to reproduce the experimental values for the electronic properties without adding correlations. Our calculation includes only excitonic corrections and no further interactions. The principal indirect gap is between N and and is found to be 0.98 eV, the direct gap at the point amounts to 1.… Show more

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Cited by 8 publications
(3 citation statements)
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“…The electrical properties of Nb oxides' are highly sensitive to the oxidation state of Nb [10]. NbO 2 has a small band gap (between 0.5 and 1.2 eV) [10] and exhibits Mott-Peierls transition at ∼1081 K [11,12] like VO 2 [13,14], whereas Nb 2 O 5 is a semiconductor with wide band gap [15].…”
Section: Introductionmentioning
confidence: 99%
“…The electrical properties of Nb oxides' are highly sensitive to the oxidation state of Nb [10]. NbO 2 has a small band gap (between 0.5 and 1.2 eV) [10] and exhibits Mott-Peierls transition at ∼1081 K [11,12] like VO 2 [13,14], whereas Nb 2 O 5 is a semiconductor with wide band gap [15].…”
Section: Introductionmentioning
confidence: 99%
“…Ladders are incorporated by solving a Bethe-Salpeter equation (BSE) in the particle-hole charge channel. BSE corrections to the polarizability has proven to be tremendously successful [13,14,[46][47][48][49][50][51] in explaining the optical absorption spectrum of many materials ab-initio. If the electron-hole pairs originate from strongly correlated bands, they can not disperse away and stay sufficiently close together or can even form bound (excitonic) states.…”
Section: Introductionmentioning
confidence: 99%
“…However, it is well known that the one-particle Green's function may not be enough to describe the dielectric response. The vertex in the polarizability is a two-particle object responsible for electronhole attraction, which gives rise, e.g., to excitons and optical absorption below the fundamental gap [14][15][16][17][18][19][20] . When the excitons are weakly bound (Wannier type) they involve mostly states near the edge of the fundamental gap: they are confined to a small volume of k space and thus are spread over many lattice sites.…”
mentioning
confidence: 99%