In BerkeleyGW implementation, extended kernel only works with Q = 0. On the other hand, non-zero finite momentum Q only works with TDA. The two features are not compatible. The four conduction bands finite-Q falls into the incompatible regime.
I am doing a calculation with both extended_kernel and exciton_Q_shift turned on. I inspected some indications that BerkeleyGW may not did it correctly. When comparing besmat. h5 generated for Q=0 and |Q1| > 0 , I found when the four band
I am doing a calculation with both extended_kernel and exciton_Q_shift turned on. I inspected some
indications that BerkeleyGW may not did it correctly.
When comparing besmat.h5 generated for Q=0 and |Q1| > 0 , I found when the four band indices are all conduction bands. The head matrix ,wing matrix and body matrix elements of Q=0 calculation are
exactly the same as those of a Q=Q1 calculation. Otherwise, those matrix are different as expected.
I wonder , if BerkeleyGW correctly treat extended kernel with finite Q, especially the extended kernel involves four conduction bands state
--
You received this message because you are subscribed to the Google Groups "BerkeleyGW Help" group.
To unsubscribe from this group and stop receiving emails from it, send an email to
help+uns...@berkeleygw.org.
To view this discussion visit
https://groups.google.com/a/berkeleygw.org/d/msgid/help/1374ea78-942b-4967-83f7-b00e4857ed20n%40berkeleygw.org.