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dft_tools/doc/guide/transport.rst
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.. _Transport:
Transport calculations
======================
Formalism
---------
The conductivity and the Seebeck coefficient in direction :math:`\alpha\beta` are defined as [#transp]_:
.. math::
\sigma_{\alpha\beta} = \beta e^{2} A_{0,\alpha\beta} \ \ \ \text{and} \ \ \ S_{\alpha\beta} = -\frac{k_B}{|e|}\frac{A_{1,\alpha\beta}}{A_{0,\alpha\beta}},
in which the kinetic coefficients :math:`A_{n,\alpha\beta}` are given by
.. math::
A_{n,\alpha\beta} = N_{sp} \pi \hbar \int{d\omega \left(\beta\omega\right)^n f\left(\omega\right)f\left(-\omega\right)\Gamma_{\alpha\beta}\left(\omega\right)}.
Here :math:`N_{sp}` is the spin factor and :math:`f(\omega)` is the Fermi function. The transport distribution :math:`\Gamma_{\alpha\beta}\left(\omega\right)` is defined as
.. math::
\Gamma_{\alpha\beta}\left(\omega\right) = \frac{1}{V} \sum_k Tr\left(v_{k,\alpha}A_{k}(\omega)v_{k,\beta}A_{k}\left(\omega\right)\right),
where :math:`V` is the unit cell volume. In multi-band systems the velocities :math:`v_{k}` and the spectral function :math:`A(k,\omega)` are matrices in the band indices :math:`i` and :math:`j`.
The frequency depended optical conductivity is given by
.. math::
\sigma(\Omega) = N_{sp} \pi e^2 \hbar \int{d\omega \Gamma_{\alpha\beta}(\omega+\Omega/2,\omega-\Omega/2)\frac{f(\omega-\Omega/2)-f(\omega+\Omega/2)}{\Omega}}.
Prerequisites
-------------
First perform a standard :ref:`DFT+DMFT calculation <dftdmft_selfcons>` for your desired material and obtain the real-frequency self energy by doing an
analytic continuation.
.. note::
It is crucial to perform the analytic continuation in such a way that the obtained real-frequency self energy is accurate around the Fermi energy as only its
low energy structure influences the final results!
Besides the self energy the Wien2k files read by the transport converter (:meth:`convert_transport_input <pytriqs.applications.dft.converters.wien2k_converter.Wien2kConverter.convert_transport_input>`) are:
* :file:`.struct`: The lattice constants specified in the struct file are used to calculate the unit cell volume.
* :file:`.outputs`: In this file the k-point symmetries are given.
* :file:`.oubwin`: Contains the indices of the bands within the projected subspace (written by :program:`dmftproj`) for each k-point.
* :file:`.pmat`: This file is the output of the Wien2k optics package and contains the velocity (momentum) matrix elements between all bands in the desired energy
window for each k-point. How to use the optics package is described below.
* :file:`.h5`: The hdf5 archive has to be present and should contain the dft_input subgroup. Otherwise :meth:`convert_dft_input <pytriqs.applications.dft.converters.wien2k_converter.Wien2kConverter.convert_dft_input>` needs to be called before :meth:`convert_transport_input <pytriqs.applications.dft.converters.wien2k_converter.Wien2kConverter.convert_transport_input>`.
Wien2k optics package
---------------------
The basics steps to calculate the matrix elements of the momentum operator with the Wien2k optics package are:
1) Perform a standard Wien2k calculation for your material.
2) Run `x kgen` to generate a dense k-mesh.
3) Run `x lapw1`.
4) For metals change TETRA to 101.0 in :file:`case.in2`.
5) Run `x lapw2 -fermi`.
6) Run `x optic`.
Additionally the input file :file:`case.inop` is required. A detail description on how to setup this file can be found in the Wien2k user guide [#userguide]_ on page 166.
Here the energy window can be chosen according to the window used for :program:`dmftproj`. However, keep in mind that energies have to be specified in absolute values! Furthermore it is important to set line 6 to ON for printing the matrix elements to the :file:`.pmat` file.
Using the transport code
------------------------
First we have to read the Wien2k files and store the relevant information in the hdf5 archive::
from pytriqs.applications.dft.converters.wien2k_converter import *
from pytriqs.applications.dft.sumk_dft_tools import *
Converter = Wien2kConverter(filename='case', repacking=True)
Converter.convert_transport_input()
SK = SumkDFTTools(hdf_file='case.h5', use_dft_blocks=True)
Additionally we need to read and set the self energy, the chemical potential and the double counting::
ar = HDFArchive('case_Sigma.h5', 'a')
SK.put_Sigma(Sigma_imp = [ar['dmft_transp_output']['Sigma_w']])
SK.chemical_potential = ar['dmft_transp_output']['chemical_potential']
SK.dc_imp = ar['dmft_transp_output']['dc_imp']
del ar
As next step we can calculate the transport distribution :math:`\Gamma_{\alpha\beta}(\omega)`::
SK.transport_distribution(directions=['xx'], Om_mesh=[0.0, 0.1], energy_window=[-0.3,0.3],
with_Sigma=True, broadening=0.0, beta=40)
Here the transport distribution is calculated in :math:`xx` direction for the frequencies :math:`\Omega=0.0` and :math:`0.1`.
To use the previously obtained self energy we set with_Sigma to True and the broadening to :math:`0.0`.
As we also want to calculate the Seebeck coefficient we have to include :math:`\Omega=0.0` in the mesh.
Note that the current version of the code repines the :math:`\Omega` values to the closest values on the self energy mesh.
For complete description of the input parameters see the :meth:`transport_distribution reference <pytriqs.applications.dft.sumk_dft_tools.SumkDFTTools.transport_distribution>`.
The resulting transport distribution is not automatically saved, but this can be easily achieved with::
SK.save(['Gamma_w','Om_meshr','omega','directions'])
SK.load(['Gamma_w','Om_meshr','omega','directions'])
Finally the optical conductivity :math:`\sigma(\Omega)` and the Seebeck coefficient :math:`S` can be obtained with::
SK.conductivity_and_seebeck(beta=40)
SK.save(['seebeck','optic_cond'])
It is strongly advised to check convergence in the number of k-points!
References
----------
.. [#transp] `V. S. Oudovenko, G. Palsson, K. Haule, G. Kotliar, S. Y. Savrasov, Phys. Rev. B 73, 035120 (2006) <http://link.aps.org/doi/10.1103/PhysRevB.73.0351>`_
.. [#userguide] `P. Blaha, K. Schwarz, G. K. H. Madsen, D. Kvasnicka, J. Luitz, ISBN 3-9501031-1-2 <http://www.wien2k.at/reg_user/textbooks/usersguide.pdf>`_