Thank you, Marcos, for such a quick response.

You are absolutely right about the low level of mesh cutoff that I used, I
used it on purpose to cut down on the calculation time. But there is a
thing that I still don't understand in your explanations: how may any
k-point sampling be related with calculation of dipole moment of my
system? Dipole moment is invariant (with respect of the used system of
coordinates) for electrically neutral system, therefore it should not
depend on the lattice vector determination and, consequently, on any
k-point sampling.
Is it?. Moreover, band structure calculations and dipole moment are
separated things (if only they are not connected somehow through
plane-wave method). So, I can understand why the magnitude of non-zero
dipole moment may vary depending on the mesh cutoff value, but zero should
be equal zero.
The question about dipole moment is important for me because I look for
the reasons which result in errors of my band structure calculation for
graphene ribbon. (Initially I thought that there was something wrong with
my input file information or something like this).

Thank you once again, hope you will help me with that weird thing.

 Artem Baskin,
 PhD student,
 University of Illinois at Chicago






> Artem,
>
> Two things could be hindering your calculation. First, your mesh
> cutoff is quite low. I would use at least 200 Ry to get only decent
> results. In my experience with 300 Ry you get pretty good results for
> a graphitic system. Second, I don't see any k-point sampling along the
> ribbon length. This definitely could be the cause of your fluctuating
> dipole value.
>
> Cheers,
>
> Marcos
>
> On Sat, Mar 13, 2010 at 3:08 AM, [email protected] <[email protected]> wrote:
>> Hi all!
>> I am a new user of Siesta and I'm involved in graphene band structure
>> calculations. I can not obtain the correct band structure for a graphene
>> nanoribon (N=3m+2, armchair passivated by H-atoms). Trying to do that I
>> was overwhelmed  with the fact that the system absolutely symmetrical in
>> Y-axis (finite size, 5 honeycomb rings) has non-zero dipole moment along
>> Y-axix which depends sharply on the Meshcutoff value.
>> Could anyone explain me where it comes from? What are the possible
>> sources
>> of this "effect" and how it may affect the band structure?
>>
>> The replica of my .fdf and .out files are attached below.
>>
>> Thanks for any reasonable help.
>>
>> From input-file
>>
>> NumberOfAtoms       26
>> NumberOfSpecies     2
>>
>> %block ChemicalSpeciesLabel
>>  1  6  C      # Species index, atomic number, species label
>>  2  1  H
>> %endblock ChemicalSpeciesLabel
>> Meshcutoff     100.00 Ry
>> LongOutput T
>> WriteDenchar T
>> AtomicCoordinatesFormat  Ang
>> %block AtomicCoordinatesAndAtomicSpecies
>>  0.00         7.37853644     0.000   1
>>  1.42         7.37853644     0.000   1
>>  -0.71         6.148780367    0.000   1
>>  2.13         6.148780367    0.000   1
>>  0.00         4.919024294    0.000   1
>>  1.42         4.919024294    0.000   1
>>  -0.71         3.68926822     0.000   1
>>  2.13         3.68926822     0.000   1
>>  0.00         2.459512147    0.000   1
>>  1.42         2.459512147    0.000   1
>>  -0.71         1.229756073    0.000   1
>>  2.13         1.229756073    0.000   1
>>  0.00         0.00           0.000   1
>>  1.42         0.00           0.000   1
>>  -0.71        -1.229756073    0.000   1
>>  2.13        -1.229756073    0.000   1
>>  0.00        -2.459512147    0.000   1
>>  1.42        -2.459512147    0.000   1
>>  -0.71        -3.68926822     0.000   1
>>  2.13        -3.68926822     0.000   1
>>  0.00        -4.919024294    0.000   1
>>  1.42        -4.919024294    0.000   1
>>  0.00         5.889024294    0.000   2
>>  0.00        -5.889024294    0.000   2
>>  1.42         5.889024294    0.000   2
>>  1.42        -5.889024294    0.000   2
>> %endblock AtomicCoordinatesAndAtomicSpecies
>>
>> %block PAO.BasisSizes
>>   C     DZP
>>   H     DZP
>> %endblock PAO.BasisSizes
>>
>> LatticeConstant  2.459512147  Ang
>> %block LatticeVectors
>>  1.732050808  0.00    0.0
>>  0.0          80.0    0.0
>>  0.0          0.00    80.0
>>
>> %endblock LatticeVectors
>>
>> %block BandLines
>> 1   -1.0   0.0  0.0
>> 20   0.0   0.0  0.0
>> 20   1.0   0.0  0.0
>> %endblock BandLines
>>
>>
>> From out-file
>>
>> siesta: Electric dipole (a.u.)  =    0.000000   17.412033    0.000000
>> siesta: Electric dipole (Debye) =    0.000000   44.257004    0.000000
>>
>>
>> Artem Baskin,
>> PhD student,
>> University of Illinois at Chicago
>>
>>
>>
>
>


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