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
NEXT STEPS
- 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
USEFUL FOR
Physicists, materials scientists, and researchers focusing on condensed matter physics, particularly those interested in the electronic properties of graphene and quantum mechanics applications.