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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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