Exciton-phonon coupling and luminescence: Difference between revisions

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  <---> :: Symmetry expanded    :yes
  <---> :: Symmetry expanded    :yes
  .....
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Notice that in the calculation of the electron-phononn coupling you need a number of conduction bands as large as the one that will be used in the Bethe-Salpeter Equation.
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'''Remove all symmetries''':<br>
'''Remove all symmetries''':<br>

Revision as of 11:06, 21 February 2022

This tutorial works only with Yambo version > 6.x

The exciton-phonon part of Yambo does not support symmetries yet!!!

This an advanced tutorial, in order to calculate exciton-phonon coupling and phonon-assisted absorption/emission you need a deep knowledge of the theory and of the Yambo code.
In this tutorial we will calculate phonon-assisted absorption and luminescence including the scattering between exciton and phonon.[1][2][3]

We will consider as example bulk silicon. Notice that parameters of the present tutorial are not at convergence, but are just as a possible example.
The tutorial includes several steps and the calculations can be quite expensive.


Electron-phonon matrix elements:
First of all we calculate electron-phonon matrix elements as explained in the section: Electron-phonon matrix elements but in the last passage of the tutorial we expand the electron-phonon matrix elements in all the Brillouin Zone. In order to do so, when we read the electron-phonon matrix elements from QE with the command ypp_ph -g g we turn on the flag GkkpExpand

gkkp                             # [R] gkkp databases
gkkp_db                          # [R] GKKP database
#GkkpReadBare                  # Read the bare gkkp
DBsPATH= "../elph_dir/"                     # Path to the PW el-ph databases
PHfreqF= "none"                  # PWscf format file containing the phonon frequencies
PHmodeF= "none"                  # PWscf format file containing the phonon modes
GkkpExpand                    # Expand the gkkp in the whole BZ
#UseQindxB                     # Use qindx_B to expand gkkp (for testing purposes) 

if everything worked fine in the log you will find:

....
<---> :: Uniform sampling      :yes
<---> :: Symmetry expanded     :yes
.....

Notice that in the calculation of the electron-phononn coupling you need a number of conduction bands as large as the one that will be used in the Bethe-Salpeter Equation.
Remove all symmetries:
Now we remove all symmetries with the command ypp_ph -y

fixsyms                          # [R] Remove symmetries not consistent with an external perturbation
% Efield1
 0.000000 | 0.000000 | 0.000000 |        # First external Electric Field
%
% Efield2
 0.000000 | 0.000000 | 0.000000 |        # Additional external Electric Field
%
BField= 0.000000           T     # [MAG] Magnetic field modulus
Bpsi= 0.000000             deg   # [MAG] Magnetic field psi angle [degree]
Btheta= 0.000000           deg   # [MAG] Magnetic field theta angle [degree]
RmAllSymm                     # Remove all symmetries
#RmTimeRev                     # Remove Time Reversal
#RmSpaceInv                    # Remove Spatial Inversion
#KeepKGrid                     # Do not expand the k-grid

the code will expand the electronic wave-function and copy the gkkp_expanded databases in the new folder.


References

  1. Theory of phonon-assisted luminescence in solids: Application to hexagonal boron nitride, E. Cannuccia, B. Monserrat and C. Attaccalite, Phys. Rev. B 99, 081109(R) (2019)
  2. Exciton-Phonon Coupling in the Ultraviolet Absorption and Emission Spectra of Bulk Hexagonal Boron Nitride, F. Paleari et al. PRL 122, 187401(2019)
  3. Exciton-Phonon Interaction and Relaxation Times from First Principles, Hsiao-Yi Chen, Davide Sangalli, and Marco Bernardi,Phys. Rev. Lett. 125, 107401(2020)