ELPH DECOMPOSE: Difference between revisions
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We suggest two different combinations to define matrix elements: | We suggest two different combinations to define matrix elements: | ||
;{{TAGO|ELPH_DECOMPOSE|VDPR}} | ;{{TAGO|ELPH_DECOMPOSE|VDPR}} | ||
:"All-electron" matrix element{{cite|engel:prb:2022}} | :"All-electron" matrix element{{cite|engel:prb:2022}}{{cite|chaput:prb:2019}} | ||
;{{TAGO|ELPH_DECOMPOSE|VDQ}} | ;{{TAGO|ELPH_DECOMPOSE|VDQ}} | ||
:"Pseudo" matrix element{{cite|engel:prb:2022}}{{cite|engel:prb:2020}} | :"Pseudo" matrix element{{cite|engel:prb:2022}}{{cite|engel:prb:2020}} |
Revision as of 12:42, 18 October 2024
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ELPH_DECOMPOSE = [string]
Default: ELPH_DECOMPOSE = VDPR
Description: Chooses which contributions to include in the computation of the electron-phonon matrix elements.
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
- D
- P
- R
- Q
For more details, please refer to Ref.[1].
References
- ↑ a b c d 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).