Dear Emanuel,
a few pointers here:
- in the calculations, you have a real space unit cell A (whatever it
is; it can be the primitive one, or a larger one); its corresponding
Brillouin Zone B is sampled with a k1xk2xk3 monkhorst-pack mesh, with
k1/k2/k3 integers. In principle, k1/k2/k3 are integers that should be
very large/go to infinity; in practice they are finite, but large enough
to make sure your calculations are converged.
- the MLWFs live in a supercell S that is k1xk2xk3 times larger than the
unit cell A of your calculation. The MLWFs are by definition periodic
with the periodicity of this supercell S. If S is large enough (i.e. if
the combination of your unit cell A and your k-sampling is fine enough -
e.g. primitive with 8x8x8 sampling, for silicon, or - exactly
equivalently - a unit cell A double the primitive one in each direction,
and 4x4x4 sampling), the MLWFs will be able to decay to almost zero
before they rise again (since, remember, they are in themselves periodic
with the periodicity of S).
- the MLWFs will have the localization that the physics of the system
tells them to have (I'm assuming here we are dealing with MLWFs in an
insulator, obtained transforming the valence bands). They will be
localized, but typically do not got to zero from their maximum after a
distanca as short as a half primitive cell. Much longer. But they do
decay exponentially.
- an interesting quantity to monitor is the matrix element of your
operator of choice (e.g. the Hamiltonian) between the same MLWFs, but
localized in different unit cells, or between different unit cells. Of
course, once the unit cells get very far away, these matrix elements
with rise again, because of the overall periodicity in S for the MLWFs
Some of these issues were discussed in here
https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.95.076804
but are explained better in Young-Su Lee PhD thesis - see e.g. Fig 4.11
and 4.14 in https://dspace.mit.edu/handle/1721.1/37371
Hope this clarifies some of your doubts - important to make sure you
master the points above if you want to work on this topic. The Rev Mod
Phys from 2012 might be also a good starting point, with its
introductory sections:
https://journals.aps.org/rmp/abstract/10.1103/RevModPhys.84.1419
nicola
On 01/08/2022 15:19, EMANUEL ALBERTO MARTINEZ wrote:
Hello everyone,
I have a simple question regarding to the localization of WFs. It seems
to be intuitive that an individual spread for each MLWF less than the
size of unit-cell ensures that it is localized well-within the
unit-cell. I need to justify some models I'm creating and I recently
realized that It could exist rare systems in which the MLWFs can surpass
the size of the unit-cell or even have another periodicity. These cases
will break my approximations. Could you give me any references about the
spread values and the localization within the unit-cell? I know It could
sound senseless, but I need to make it as clear as possible.
Thanks in advance!
--
Emanuel A. Martínez
Departamento de Física de Materiales
Universidad Complutense de Madrid
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--
----------------------------------------------------------------------
Prof Nicola Marzari, Chair of Theory and Simulation of Materials, EPFL
Director, National Centre for Competence in Research NCCR MARVEL, SNSF
Head, Laboratory for Materials Simulations, Paul Scherrer Institut
Contact info and websites at http://theossrv1.epfl.ch/Main/Contact
_______________________________________________
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people and expresses its concerns about the devastating
effects that the Russian military offensive has on their
country and on the free and peaceful scientific, cultural,
and economic cooperation amongst peoples
_______________________________________________
Quantum ESPRESSO is supported by MaX (www.max-centre.eu)
users mailing list [email protected]
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