ELPH DECOMPOSE: Difference between revisions
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Description: Chooses which contributions to include in the computation of the electron-phonon matrix elements. | Description: Chooses which contributions to include in the computation of the electron-phonon matrix elements. | ||
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Revision as of 14:21, 17 January 2025
ELPH_DECOMPOSE = [string]
Default: ELPH_DECOMPOSE = VDPR
Description: Chooses which contributions to include in the computation of the electron-phonon matrix elements.
| Mind: Available as of VASP 6.5.0 |
The electron-phonon matrix element can be formulated in the projector-augmented-wave (PAW) method in terms of individual contributions[1]. Each contribution can be included by specifying the associated letter in ELPH_DECOMPOSE. We suggest two different combinations to define matrix elements:
ELPH_DECOMPOSE = VDPR- "All-electron" matrix element[1][2]
ELPH_DECOMPOSE = VDQ- "Pseudo" matrix element[1][3]
Available contributions
- V - Derivative of pseudopotential,
- D - Derivative of PAW strength parameters,
- P - Derivative of PAW projectors,
- Failed to parse (unknown function "\begin{split}"): {\displaystyle \begin{split} g^{(\text{P})}_{m \mathbf{k}', n \mathbf{k}, a} & \equiv \sum_{ij} \langle \tilde{\psi}_{m \mathbf{k}'} | \frac{\partial \tilde{p}_{a i}}{\partial u_{a}} \rangle ( D_{a, ij} - \varepsilon_{n \mathbf{k}} Q_{a, ij} ) \langle \tilde{p}_{a j} | \tilde{\psi}_{n \mathbf{k}} \rangle \\ & + \sum_{ij} \langle \tilde{\psi}_{m \mathbf{k}'} | \tilde{p}_{a i} \rangle ( D_{a, ij} - \varepsilon_{m \mathbf{k}'} Q_{a, ij} ) \langle \frac{\partial \tilde{p}_{a j}}{\partial u_{a}} | \tilde{\psi}_{n \mathbf{k}} \rangle \end{split} }
- R - Derivative of PAW partial waves, and
- with
- Q - Derivative of PAW projectors, (different eigenvalues)
- Failed to parse (unknown function "\begin{split}"): {\displaystyle \begin{split} g^{(\text{Q})}_{m \mathbf{k}', n \mathbf{k}, a} & \equiv \sum_{ij} \langle \tilde{\psi}_{m \mathbf{k}'} | \frac{\partial \tilde{p}_{a i}}{\partial u_{a}} \rangle ( D_{a, ij} - \varepsilon_{n \mathbf{k}} Q_{a, ij} ) \langle \tilde{p}_{a j} | \tilde{\psi}_{n \mathbf{k}} \rangle \\ & + \sum_{ij} \langle \tilde{\psi}_{m \mathbf{k}'} | \tilde{p}_{a i} \rangle ( D_{a, ij} - \varepsilon_{n \mathbf{k}} Q_{a, ij} ) \langle \frac{\partial \tilde{p}_{a j}}{\partial u_{a}} | \tilde{\psi}_{n \mathbf{k}} \rangle \end{split} }
Related tags and articles
References
- ↑ a b c M. Engel, H. Miranda, L. Chaput, A. Togo, C. Verdi, M. Marsman, and G. Kresse, Zero-point renormalization of the band gap of semiconductors and insulators using the projector augmented wave method, Phys. Rev. B 106, 094316 (2022).
- ↑ L. Chaput, A. Togo, and I. Tanaka, Finite-displacement computation of the electron-phonon interaction within the projector augmented-wave method, Phys. Rev. B 100, 174304 (2019).
- ↑ M. Engel, M. Marsman, C. Franchini, and G. Kresse, Electron-phonon interactions using the projector augmented-wave method and Wannier functions, Phys. Rev. B 101, 184302 (2020).