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ELPH USERECIP: Difference between revisions

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Add ELPH_USERECIP tag page: reciprocal-space matrix elements, auto-enabled for meta-GGAs
m Huebsch moved page Construction:ELPH USERECIP to ELPH USERECIP without leaving a redirect
 
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{{DISPLAYTITLE|ELPH_USERECIP}}
{{DISPLAYTITLE:ELPH_USERECIP}}
{{TAGDEF|ELPH_USERECIP|logical|.FALSE.}}
{{TAGDEF|ELPH_USERECIP|logical|.FALSE.}}


Description: Computes electron-phonon matrix elements in reciprocal space instead of real space.
Description: Computes electron-phonon matrix elements in reciprocal space instead of real space.
{{Available|6.5.0}}
{{Available|6.5.0}}
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The electron-phonon matrix element
The electron-phonon matrix element
:<math>\langle \psi_{n\mathbf{k}} | \Delta V_{\mathbf{q}} | \psi_{m\mathbf{k}'} \rangle</math>
:<math>\langle \psi_{n\mathbf{k}} | \Delta V_{\mathbf{q}} | \psi_{m\mathbf{k}'} \rangle</math>
can be evaluated either in real space (the default) or in reciprocal space as a contraction over plane-wave coefficients. <code>ELPH_USERECIP = .TRUE.</code> selects the reciprocal-space path.
can be evaluated either in real space (the default) or in reciprocal space as a contraction over plane-wave coefficients. {{TAG|ELPH_USERECIP|.TRUE.}} selects the reciprocal-space path.


'''Automatic activation for meta-GGAs.''' When a meta-GGA functional is used, VASP sets <code>ELPH_USERECIP = .TRUE.</code> automatically. This is required because the kinetic-energy density contribution to the electron-phonon potential is non-local in real space and can only be evaluated in reciprocal space.
'''Automatic activation for meta-GGAs.''' When a meta-GGA functional is used, VASP sets {{TAG|ELPH_USERECIP|.TRUE.}} automatically. This is required because the kinetic-energy density contribution to the electron-phonon potential is non-local in real space and can only be evaluated in reciprocal space.


'''Band structure renormalization.''' The reciprocal-space path can also be beneficial for calculations where the number of bra k-points (<math>n_\mathbf{k}</math>) is much smaller than the number of ket k-points (<math>n_{\mathbf{k}'}</math>), such as band structure renormalization along high-symmetry lines. In this case the real-space path would require an FFT for each bra state, whereas the reciprocal-space path works directly with the stored plane-wave coefficients and avoids these transforms.
'''Band structure renormalization.''' The reciprocal-space path can also be beneficial for calculations where the number of bra k-points (<math>n_\mathbf{k}</math>) is much smaller than the number of ket k-points (<math>n_{\mathbf{k}'}</math>), such as band structure renormalization along high-symmetry lines. In this case the real-space path would require an FFT for each bra state, whereas the reciprocal-space path works directly with the stored plane-wave coefficients and avoids these transforms.


==Related tags and articles==
==Related tags and articles==
* {{TAG|ELPH_MELS}}
* {{TAG|ELPH_USEBLAS}}
* {{TAG|ELPH_USEBLAS}}
* {{TAG|ELPH_RUN}}
* {{TAG|ELPH_RUN}}
[[Category:INCAR tag]][[Category:Electron-phonon interactions]]
[[Category:INCAR tag]][[Category:Electron-phonon interactions]]

Latest revision as of 13:56, 18 June 2026

ELPH_USERECIP = logical
Default: ELPH_USERECIP = .FALSE. 

Description: Computes electron-phonon matrix elements in reciprocal space instead of real space.


The electron-phonon matrix element

[math]\displaystyle{ \langle \psi_{n\mathbf{k}} | \Delta V_{\mathbf{q}} | \psi_{m\mathbf{k}'} \rangle }[/math]

can be evaluated either in real space (the default) or in reciprocal space as a contraction over plane-wave coefficients. ELPH_USERECIP = .TRUE. selects the reciprocal-space path.

Automatic activation for meta-GGAs. When a meta-GGA functional is used, VASP sets ELPH_USERECIP = .TRUE. automatically. This is required because the kinetic-energy density contribution to the electron-phonon potential is non-local in real space and can only be evaluated in reciprocal space.

Band structure renormalization. The reciprocal-space path can also be beneficial for calculations where the number of bra k-points ([math]\displaystyle{ n_\mathbf{k} }[/math]) is much smaller than the number of ket k-points ([math]\displaystyle{ n_{\mathbf{k}'} }[/math]), such as band structure renormalization along high-symmetry lines. In this case the real-space path would require an FFT for each bra state, whereas the reciprocal-space path works directly with the stored plane-wave coefficients and avoids these transforms.

Related tags and articles