[Pw_forum] Phonon branch enumeration
Stefano Baroni
baroni at sissa.it
Thu Mar 12 01:46:12 CET 2009
On Mar 11, 2009, at 1:32 PM, Jeffrey Mullen wrote:
>
> Thanks for the recommendation. I have performed the calculation with
> the
> iverbosity set to 1. It will take me a while to parse it and
> understand
> the output, but if I can figure out the relationships, I will
> attempt to
> code the ordering into the application.
that would be really great!
SB
>
>
> Cheers
> Jeff Mullen
> North Carolina State University
>
>
> Dal Corso Andrea wrote:
>
>>
>> It is an interesting idea. I think it is possible to make the
>> symmetry classification of the displacements patterns with the same
>> routine that makes the symmetry classification of the eigenvectors
>> of the dynamical matrix. Presently, this is not done. You can
>> code this feature yourself or just use iverbosity=1. With this option
>> the code writes the displacement patterns and you can
>> check their symmetry.
>>
>> Andrea
>>
>>
>>
>>
>>
>>> Cheers
>>> Jeff
>>>
>>>
>>>
>>> e kb wrote:
>>>
>>>
>>>
>>>> Dear Jeff,
>>>> I am definitely not an expert on the topic but I'd like to
>>>> understand
>>>> your question better.
>>>>
>>>> Mode symmetry, D_6h(6/mmm) point group:
>>>>
>>>> omega( 1 - 1) = -37.4 [cm-1] --> A_2u I
>>>> omega( 2 - 3) = -33.9 [cm-1] --> E_1u I
>>>> omega( 4 - 4) = 863.3 [cm-1] --> B_2g
>>>> omega( 5 - 6) = 1336.0 [cm-1] --> E_2g
>>>>
>>>> So you have the irr. representations and the values for omega
>>>> (values
>>>> are printed with higher precision in the previous part after
>>>> diagonalization as you reported). What exactly do you want to know
>>>> more (that you cannot check from a book on group theory) ?
>>>>
>>>> Emine Kucukbenli, grad. student, SISSA, Italy.
>>>>
>>>> --- On *Tue, 3/10/09, Jeffrey Mullen /<jtmullen at ncsu.edu>/* wrote:
>>>>
>>>> From: Jeffrey Mullen <jtmullen at ncsu.edu>
>>>> Subject: [Pw_forum] Phonon branch enumeration
>>>> To: pw_forum at pwscf.org
>>>> Date: Tuesday, March 10, 2009, 2:34 AM
>>>>
>>>> Greetings
>>>>
>>>> I am testing electron-phonon interaction calculations with
>>>> graphene and
>>>> have encountered a problem enumerating the resulting phonon
>>>> branches.
>>>> When I run the ph.x calculation at the q(0 0 0), the code
>>>> calculates 4
>>>> representations:
>>>>
>>>> Representation # 1 modes # 1 2
>>>> Representation # 2 mode # 3
>>>> Representation # 3 mode # 4
>>>> Representation # 4 modes # 5 6
>>>>
>>>>
>>>> When the values for omega are calculated, the results are:
>>>>
>>>> **************************************************************************
>>>> omega( 1) = -1.119851 [THz] = -37.354451 [cm-1]
>>>> omega( 2) = -1.016557 [THz] = -33.908905
>>>> [cm-1]
>>>> omega( 3) = -1.016557 [THz] = -33.908905 [cm-1]
>>>> omega( 4) = 25.882237 [THz] = 863.344237 [cm-1]
>>>> omega( 5) = 40.051667 [THz] = 1335.988701 [cm-1]
>>>> omega( 6) = 40.051667 [THz] = 1335.988701 [cm-1]
>>>> **************************************************************************
>>>>
>>>>
>>>> with the following mode symmetries:
>>>>
>>>> Mode symmetry, D_6h(6/mmm) point group:
>>>>
>>>> omega( 1 - 1) = -37.4 [cm-1] --> A_2u I
>>>> omega( 2 - 3) = -33.9 [cm-1] --> E_1u I
>>>> omega( 4 - 4) = 863.3 [cm-1] --> B_2g
>>>> omega( 5 - 6) = 1336.0 [cm-1] --> E_2g R
>>>>
>>>>
>>>> My question is one of ordering. How do I extract which omega(##)
>>>> corresponds to which representation/mode?
>>>>
>>>> Thanks
>>>> Jeff Mullen
>>>> North Carolina State
>>>> University
>>>>
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>>>>
>>>>
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---
Stefano Baroni - SISSA & DEMOCRITOS National Simulation Center -
Trieste
http://stefano.baroni.me [+39] 040 3787 406 (tel) -528 (fax) /
stefanobaroni (skype)
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