Discussion Overview
The discussion centers around the relationship between energy bands in k-space and their representation in real space, particularly in the context of solid-state physics. Participants explore the implications of this relationship for electron behavior in a periodic structure and the transformation of wave functions.
Discussion Character
- Technical explanation
- Conceptual clarification
- Debate/contested
Main Points Raised
- One participant questions how energy bands with dispersion in k-space translate to real space.
- Another participant asserts that bands exist solely in k-space, as the effective mean field Hamiltonian is diagonal in k-space but not in real space.
- It is proposed that transforming eigenstates into real space yields Wannier orbitals, which resemble atomic orbitals but do not diagonalize the Hamiltonian, leading to a lack of a direct e(r) relationship.
- A further contribution discusses the behavior of an electron in a perfect crystal under a constant external electric field, noting that the E vs k relationship influences the electron's motion in a complex manner.
- There is a suggestion regarding the integration over the entire Brillouin Zone to obtain Wannier orbitals, indicating that one wave function is part of a broader set of orbitals.
Areas of Agreement / Disagreement
Participants express differing views on the existence and representation of energy bands in k-space versus real space, with no consensus reached on the implications of these transformations.
Contextual Notes
The discussion involves assumptions about the nature of the crystal and the behavior of electrons, particularly regarding the effects of periodic structures and external fields. The relationship between k-space and real space representations remains unresolved.