ElPhonTransport
This page gives hints on how to compute transport properties that are determined by the electron-phonon interaction (electrical resistivity, superconductivity, thermal conductivity) with the ABINIT package.
Introduction¶
Warning : this topic concerns metals only.
The calculation of bulk transport quantities (electrical and thermal resistivities - the part that is determined by the electron-phonon interaction) is possible using anaddb. Analogous quantities are obtained from the conducti post-processor, but due to electron-electron scattering, instead of electron-phonon.
A preliminary calculation of the derivatives of the wavefunctions with respect to k-vector must be carried out. After generating a GKK file (see topic_ElPhonInt), the Electron-Phonon Coupling (EPC) analysis is performed in anaddb, setting elphflag variable to 1. Most of the procedure is automatic, but can be lengthy if a large number of k-points is being used.
For the superconductivity calculations, The electron-phonon interaction is
interpolated in reciprocal space, then integrated over the Fermi surface to
give the Eliashberg function. Several quadrature methods are available. The
default (telphint=1) is to use Gaussian weighting, with a width
elphsmear. Another option is the improved tetrahedron
[Bloechl1994a] (telphint=0). Finally
(telphint=2), one can integrate a given set of electron bands,
between ep_b_max and ep_b_min. The resulting integrated
quantities are the Eliashberg function (in a file suffixed _A2F
), and the EPC
strength λ which is printed in the main output file.
The transport calculation is turned on by setting ifltransport to 1
in anaddb. The transport quantities depend on the Fermi velocity for each
band, and the electronic band-dependence of the matrix elements must be
preserved before integration, by setting ep_keepbands to 1. This
increases the memory used, by the square of the number of bands crossing EF.
The results are the transport Eliashberg function (in file _A2F_TR
), the
electrical resistivity (in file _RHO
), and the thermal conductivity (in file _WTH
).
It is also possible to consider the temperature dependence of the Fermi energy: cubic spline interpolation (ep_nspline) enables to linearly interpolate the transport arrays and reduce the memory usage. Besides setting the Fermi level with elph_fermie (in Hartree), it is also possible to specify the extra electrons per unit cell, (i.e., the doping concentration often expressed in cm-3) with ep_extrael.
Some details about the calculation of electron-phonon quantities in ABINIT and ANADDB can be found here.
Related Input Variables¶
compulsory:
- elphflag ELectron-PHonon FLAG
basic:
- ep_keepbands Electron-Phonon KEEP dependence on electron BANDS
- ifltransport IFLag for TRANSPORT
- kptrlatt K PoinT Reciprocal LATTice
- telphint Technique for ELectron-PHonon INTegration
useful:
- a2fsmear Alpha2F SMEARing factor
- elph_fermie ELectron-PHonon FERMI Energy
- elphsmear ELectron-PHonon SMEARing factor
- ep_b_max Electron Phonon integration Band MAXimum
- ep_b_min Electron Phonon integration Band MINimum
- ep_extrael Electron-Phonon EXTRA ELectrons
- ep_nspline Electron Phonon Number for SPLINE interpolation
- mustar MU STAR
- prtfsurf PRinT the Fermi SURFace
- prtvol PRinT VOLume
expert:
- band_gap BAND GAP
- ep_nqpt Electron Phonon Number of Q PoinTs
- kptrlatt_fine K PoinT Reciprocal LATTice for FINE grid
Selected Input Files¶
v5:
- tests/v5/Input/t88.in
- tests/v5/Input/t89.in
- tests/v5/Input/t90.in
- tests/v5/Input/t91.in
- tests/v5/Input/t92.in
- tests/v5/Input/t93.in
- tests/v5/Input/t94.in
- tests/v5/Input/t95.in
- tests/v5/Input/t99.in
v6:
v7:
Tutorials¶
- The tutorial on the electron-phonon interaction presents the use of the utility MRGKK and ANADDB to examine the electron-phonon interaction and the subsequent calculation of superconductivity temperature (for bulk systems).