Dear Artem

Thank you for your response.I don't now how they are connected (Or not)  I
need to find it out.

Best regards
Akbar



On Fri, Mar 19, 2010 at 11:39 PM, [email protected] <[email protected]> wrote:

> Dear Akbar,
> As to possible relation between band structure calculation and dipole
> moment, that was my desperate assumption how to reconcile the
> contradiction between symmetry and my current results. I think, they are
> not connected (anyhow).
>
> Best,
>  Artem Baskin,
>  PhD student,
>  University of Illinois at Chicago
>
>  On Fri, March 19, 2010 5:39 am, akbar jahangiri wrote:
> > Dear Artem
> >
> > Regarding this sentence, i have a question . Are they  connected through
> > plan-wave method ? if yes why?
> >
> >>>" and structure calculations and dipole moment are
> > separated things (if only they are not connected somehow through
> > plane-wave method). "
> >
> > Best regards
> > Akbar jahangiri
> >
> > 2010/3/16 Marcos Veríssimo Alves <[email protected]>
> >
> >> About the coordinates, I haven't really checked them. If they are
> >> incorrect then it would be the most obvious source of error.
> >>
> >> For the dipole moment, I don't see how the origin of coordinates and
> >> k-point sampling could possibly be related. Surely you are right, the
> >> dipole moment is independent of the origin of coordinates, but the
> >> origin of coordinates and the k-point sampling are ultimately
> >> completely un-related to each other. The issue with k-point sampling
> >> is that it is used for performing a sum over the energies of occupied
> >> bands in k-space, which accounts for the part of the total energy. If
> >> this is wrong, then your total energy is wrong as well. If your total
> >> energy is wrong, then by the Kohn-Sham theorems you have a wrong
> >> charge density distribution. And, if you have a wrong charge density
> >> distribution, then definitely your dipole moment would be wrong.
> >> Fundamentally, this is it.
> >>
> >> Nevertheless, as it has been discussed rather recently in the list,
> >> bear in mind that, in a solid, the dipole would be ill-defined, and to
> >> get a meaningful value you'd need to resort to the Berry's phase
> >> approximation. So, it would be advisable (1) to check your initial
> >> coordinates just in case and (2) see if you get the dipole moment to
> >> converge with an increasing number of k-points along the ribbon's
> >> length.
> >>
> >> Cheers,
> >>
> >> Marcos
> >>
> >>
> >> On Tue, Mar 16, 2010 at 12:22 PM, Roland Gillen
> >> <[email protected]> wrote:
> >> > Artem,
> >> >
> >> > I might be terribly wrong mistaken, but your geometry doesn't look
> >> like
> >> it's
> >> > symmetric. Look at the y-coordinates of your H-atoms. They are about
> >> +5.8
> >> > and -5.8.
> >> > Your left-most carbon atoms are at y=-4.9, but the carbon atoms at the
> >> other
> >> > edge are at y=7.3.
> >> > Btw. the x-positions of the hydrogen atoms don't seem reasonable as
> >> well.
> >> >
> >> > Maybe that is the reason for your wrong band structures?
> >> >
> >> > Cheers
> >> > Roland
> >> >
> >> > [email protected] schrieb:
> >> >>
> >> >> 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     200.00 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
> >> >>>> -0.485       8.218581082    0.000   2
> >>>>>   -0.485      -5.759068935    0.000   2
> >>>>>    1.905        8.218581082    0.000   2
> >>>>>    1.905       -5.759068935    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
> >> >>>> 40   0.0   0.0  0.0
> >> >>>> 40   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
> >> >>>>
> >> >>>>
> >> >>>>
> >> >>>>
> >> >>>
> >> >>>
> >> >>
> >> >>
> >> >>
> >> >
> >> >
> >>
> >
>
>
>

Responder a