Dear Deyang,
but it is not entirely clear to me what quantity you are trying to compute.
As you know, solving the BSE provides the electron–hole amplitudes A^lambda_cvk that define each exciton. From these amplitudes, you can construct the excitonic wavefunction as a post-processing step. This is a two-particle wavefunction given by:
\Psi_exc^\lambda(re,rh) = \Sum_cvk A^lambda_cvk \phi_vk(r_v) \phi^*_ck(r_e)
where \phi are the KS states.
The A^lambda_cvk amplitudes are stored in the ndb.BS_diago database and they can be accessed using yambopy.
I hope this clarifies things
Best,
Daniele
Wannier 90 interface in 4.5.2
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Re: Wannier 90 interface in 4.5.2
Dr. Daniele Varsano
S3-CNR Institute of Nanoscience and MaX Center, Italy
MaX - Materials design at the Exascale
http://www.nano.cnr.it
http://www.max-centre.eu/
S3-CNR Institute of Nanoscience and MaX Center, Italy
MaX - Materials design at the Exascale
http://www.nano.cnr.it
http://www.max-centre.eu/