Electron Phonon Coupling: Difference between revisions

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1. In '''scf''' we run a standard scf calculation choosing the a large k-grid in such a way to converge density. Do not forget to set ''force_symmorphic=.true.'', because not symmorphic symmetries are not supported yet in Yambo.
1. In '''scf''' we run a standard scf calculation choosing the a large k-grid in such a way to converge density. Do not forget to set ''force_symmorphic=.true.'', because not symmorphic symmetries are not supported yet in Yambo.
 
Notice that because the present system is two-dimensional we added the flag ''assume_isolated="2D"'' in such a way correct phonons in 2D.
2. Go in the '''nscf''' folder, and then copy the ${PREFIX}.save folder from '''scf''' to '''nscf''', in the present example just do ''cp -r ../scf/bn.save ./''.
2. Go in the '''nscf''' folder, and then copy the ${PREFIX}.save folder from '''scf''' to '''nscf''', in the present example just do ''cp -r ../scf/bn.save ./''.
In the nscf input you have to choose the number of k-points and bands you will use for the electron-phonon coupling and Yambo calculations.
In the nscf input you have to choose the number of k-points and bands you will use for the electron-phonon coupling and Yambo calculations.

Revision as of 12:36, 17 December 2020

Here we show step-by-step how to use Quantum Espresso to calculate phonons and electron-phonon matrix-elements on a regular q-grid, with the final aim to allow Yambo to read these databases and calculate the temperature-dependent correction to the electronic states. This tutorial is quite complicated, take your time to follow all the steps

Calculations will be divided in different folders:

  • pseudo the pseudo potential folder
  • scf for the self-consistent calculation
  • nscf for the non-self-consistent calcaultion with a larger number of bands
  • phonon for the phonons calculations
  • dvscf for the calculation of electron-phonon matrix elements

In this tutorial we will show how to calculate electron-phonon induced corrections to the bands and optical properties of 2D hexagonal boron nitride. All input file are availabe in the following tgz file: hBN.epc.tgz

1. In scf we run a standard scf calculation choosing the a large k-grid in such a way to converge density. Do not forget to set force_symmorphic=.true., because not symmorphic symmetries are not supported yet in Yambo. Notice that because the present system is two-dimensional we added the flag assume_isolated="2D" in such a way correct phonons in 2D. 2. Go in the nscf folder, and then copy the ${PREFIX}.save folder from scf to nscf, in the present example just do cp -r ../scf/bn.save ./. In the nscf input you have to choose the number of k-points and bands you will use for the electron-phonon coupling and Yambo calculations.


&inputph
              tr2_ph = 1e-16
              prefix = '6HSiC'
            fildvscf = '6HSiC-dvscf'
              fildyn = '6HSiC.dyn'
     electron_phonon = 'dvscf',
               epsil = .true.
               trans = .true.
               ldisp = .true.
           verbosity = 'high'
         nq1=10, nq2 =10, nq3=2
/

3. In nscf folder I run an nscf calculation, setting the number of bands nbnd equal to the desired band number, force_symmorphic=.true. and the same q grid as before. A ${PREFIX}.save folder will be automatically created.

4. In the main directory I copy and then overwrite the previous ${PREFIX}.save directory with the new one. Now I run an elph calculation setting electron_phonon = ‘yambo’, and the q grid.

&inputph
    fildvscf = '6HSiC-dvscf'
    fildyn = '6HSiC.dyn'
           verbosity = 'high'
               epsil = .true.
               ldisp = .true.
              tr2_ph = 1e-16
              prefix = '6HSiC'
     electron_phonon = 'yambo',
               trans = .false.
         nq1=10, nq2 =10, nq3=2
/