Graphene Hamiltonian: Eq.(1) in PRB 81, 205444

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    Graphene Hamiltonian
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SUMMARY

The Hamiltonian of graphene, as discussed in the context of Eq.(1) in PHYSICAL REVIEW B 81, 205444, is represented as a 2 × 2 matrix comprising the components \langle A|H|A\rangle, \langle A|H|B\rangle, \langle B|H|A\rangle, and \langle B|H|B\rangle. These components are treated as functions and operators in terms of spatial coordinates (x,y) rather than mere parameters. The derivation from the tight-binding model to the Dirac-Weyl equation is elaborated in the review by Castro Neto et al., specifically in Section II.B, and further detailed in supplementary notes available online.

PREREQUISITES
  • Understanding of Hamiltonian mechanics
  • Familiarity with Bloch's theorem
  • Knowledge of the tight-binding model
  • Basic concepts of Dirac-Weyl equations
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  • Study the tight-binding model in detail
  • Review the Dirac-Weyl equation derivation in Castro Neto et al.'s paper
  • Examine the mathematical treatment of operators in quantum mechanics
  • Explore the implications of graphene's Hamiltonian on electronic properties
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hokhani
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As far as I know, the Hamiltonian of graphene in the Bloch's sums |A\rangle and |B\rangle near the points K or K' is a 2 \times 2 matrix with the components: \langle A|H|A\rangle, \langle A|H|B\rangle, \langle B|H|A\rangle,\langle B|H|B\rangle which all are parameters (and not variables). But in the Eq.(1) in PHYSICAL REVIEW B 81, 205444 (2010) (http://journals.aps.org/prb/abstract/10.1103/PhysRevB.81.205444) these components are functions and operators in terms of (x,y). Could anyone please tell me how to obtain this formula?
 
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The tight-binding model to Dirac-Weyl equation derivation is outlined in the review by Castro Neto et al http://arxiv.org/abs/0709.1163 (Sect. II.B), as well as in these notes https://www.tfkp.physik.uni-erlangen.de/download/research/DW-derivation.pdf, which have a few more details of the steps.
 

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