Discussion Overview
The discussion revolves around the concept of energy bands in solids, particularly focusing on the number of bands, their completeness, and the implications for quantum mechanics. Participants explore the relationship between the bands near the Fermi surface and the overall band structure of solids, including the completeness of eigenwavefunctions.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
Main Points Raised
- Some participants propose that while solids theoretically have infinitely many energy levels, only the bands near the Fermi surface are typically discussed.
- There is a question regarding the completeness of eigenwavefunctions when considering only certain bands, such as Gamma25', and whether this leads to a complete basis in quantum mechanics.
- One participant asserts that all wavefunctions in solids are approximate due to the complexity of many atoms involved.
- Another participant clarifies that the lines in band structure diagrams represent dispersion curves for each band, not eigenstates or basis functions.
- It is noted that while there are infinitely many bands, most are unoccupied, which raises questions about their relevance in practical scenarios.
Areas of Agreement / Disagreement
Participants express differing views on the nature of eigenwavefunctions and the completeness of basis sets in quantum mechanics. There is no consensus on whether using only certain bands can lead to a complete basis, indicating an unresolved debate.
Contextual Notes
The discussion highlights limitations in understanding the relationship between band structure and quantum mechanics, particularly regarding the definitions and roles of eigenstates and basis functions. Some assumptions about the tight-binding approximation and its implications for band structure are also noted but remain unresolved.