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- From: "Erik Ylvisaker" <eylvisaker@physics.ucdavis.edu>
- To: <forum@abinit.org>
- Subject: Re: [abinit-forum] What is a LO-TO spliting in phonon calculations?
- Date: Tue, 9 May 2006 11:40:59 -0700
My own understanding of LO-TO splitting is fairly
rudimentary, so anyone feel free to correct me where I'm wrong. But I'll
explain what I understand of it.
Optical phonons at the gamma point involve shifting
of one or more atomic sublattices with respect to another. In
insulating materials, this creates a long range electric field which effectively
increases the spring constant (if you want to think of it that way) and
frequency of the vibrational mode. This causes the LO-TO splitting.
It's not an issue in metals because the electric field is screened
out. In the DFPT formalism, this effect is caused by a term
which has 1/q in it, which presents problems for a Gamma point calculation,
but other q points are treated correctly. The resolution of the problem is
to take the limit at q goes to zero along a particular direction of that
term. This results in LO-TO splitting which depends on direction, which is
relevant for, say, a hexagonal system, but for a cubic system like CsCl I'd
imagine there's only one relevant splitting. LO-TO splitting is important
to have the phonon dispersion along a particular direction be continuous from
q=0 to q != 0
You can't switch on LO-TO splitting in abinit while
doing the phonon calculation. You need to use the post-processing code
anaddb. There's some good discussion of how to do this in the second
half of the response functions 1 tutorial.
|
- What is a LO-TO spliting in phonon calculations?, zhangtingPKU, 05/09/2006
- Re: [abinit-forum] What is a LO-TO spliting in phonon calculations?, Erik Ylvisaker, 05/09/2006
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