Inequivalent K and K' points in graphene

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Discussion Overview

The discussion revolves around the inequivalence of K and K' points in monolayer graphene, exploring the theoretical basis for their differences and implications in electronic structure calculations. Participants examine the symmetry properties and the role of these points in the context of band theory and density functional theory (DFT).

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the theoretical difference between K and K' points and seeks clarification on how this difference can be detected.
  • Another participant explains that K and K' points are inequivalent due to their positions in momentum space, describing their relationship to the A and B sublattices of graphene.
  • A different participant raises a concern about the use of the Irreducible Brillouin Zone in DFT calculations, questioning why only the K point is considered despite the inequivalence.
  • It is noted that while the electronic structure at K and K' points is similar, the wavefunctions are related by time reversal symmetry, with different spinor characteristics at each point.
  • One participant elaborates on band theory, stating that K and K' are not equivalent points because their difference is not an integer multiple of reciprocal lattice vectors, despite having the same eigenvalues due to symmetry.

Areas of Agreement / Disagreement

Participants express differing views on the implications of K and K' inequivalence, particularly regarding their treatment in DFT calculations and the nature of their wavefunctions. No consensus is reached on the necessity of considering both points in certain calculations.

Contextual Notes

The discussion highlights limitations in understanding the implications of K and K' points, particularly in relation to the use of the Irreducible Brillouin Zone and the symmetry properties of wavefunctions. There is an acknowledgment of unresolved aspects regarding the treatment of these points in theoretical frameworks.

forever_physicist
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Good evening to everybody!
I have a question concerning monolayer graphene.
In all the papers I read it is well specified that K and K' in graphene are not equivalent points, but I didn't find anywhere where is the difference between them. Can anybody tell me where this difference is coming from theoretically and how can be detected?
 
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The K and K’ points are inequivalent for the same reason the A and B sublattices of graphene are inequivalent. Here’s a picture:
https://images.app.goo.gl/1PnPU5HPaW4FZawD8
In the momentum space picture, remember that only the first (hexagonal) Brillouin zone is shown; the Brillouin zones actually tile the plane. So with that in mind, it’s clear that (e.g.) the K point occurs at a vertex with two hexagons below it and one hexagon above it, and the K’ point occurs at the mirror image vertex, with one hexagon below and two above. In other words, both K and K’ have threefold rotational symmetry, but they’re inversions of each other.
 
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Ok but if this is the case, why when in a DFT calculation we use the Irreducible Brillouin Zone, we only consider K? In principle it is not enough to consider only 1/12 of the hexagon as everybody do, right?
 
The electronic structure (edit: the band energy structure, not the wavefunctions) is going to be the same, but the wavefunction at the K point is related to the wavefunction at the K' point by time reversal symmetry. It's kind of a momentum space analogy to different enantiomers of a molecule: they have the same energy, but they are mirror images of each other. Another way you can think about it is that near the K (K') points, the Hamiltonian ends up having the same form as that of a massless spin 1/2 particle. But the phases of the wavefunction components differ by a sign change. So at the K point, you get a "left-handed"spinor and at the K' point you get a "right-handed" spinor. Here's a pretty good review:
https://cdn.journals.aps.org/files/sample-rmp-revtex4.pdf
 
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In band theory,we label all eigenstates with nk. The k point is defined in the first Brillouin Zone of specific structure, due to equivalence of the two k points whose difference is an integer multiple of reciprocal lattice vectors. In the case you mentioned, K minus K‘ is not an integer multiple of reciprocal lattice vectors, so they are not equivalent points. Although they have same eigenvalues because of symmetry, they are absolutely inequivalent points
 
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