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Third‐Order Susceptibility of Lithium Niobate: Influence of Polarons and Bipolarons
The third‐order susceptibility χ(3) of lithium niobate (LiNbO3) is calculated within a Berry‐phase formulation of the dynamical polarization based on the electronic structure obtained within density‐functional theory (DFT). Maximum |χzzzz(3)| values of the order of 10−19 m2 V−2 are calculated for ph...
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Published in: | physica status solidi (b) 2023-02, Vol.260 (2), p.n/a |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The third‐order susceptibility χ(3) of lithium niobate (LiNbO3) is calculated within a Berry‐phase formulation of the dynamical polarization based on the electronic structure obtained within density‐functional theory (DFT). Maximum |χzzzz(3)| values of the order of 10−19 m2 V−2 are calculated for photon energies between 1.2 and 2 eV, i.e., in the lower half of the optical bandgap of lithium niobate. Both free and bound electron (bi)polarons are found to lead to a remarkable enhancement of the third‐order susceptibility for photon energies below 1 eV.
The third‐order susceptibility χ3 of electron polarons in lithium niobate is calculated within a Berry‐phase formulation of the dynamical polarization based on density functional theory. Free and bound electron (bi)polarons lead to a remarkable enhancement of χ3 for photon energies below 1 eV, providing maximum values of the order of 2 × 10−19 m2 V−2. |
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ISSN: | 0370-1972 1521-3951 |
DOI: | 10.1002/pssb.202200453 |