Discussion Overview
The discussion revolves around the concept of wavevector spread in the context of nano optics, specifically addressing the maximum possible spread in the wavevector component k when light converges towards a focus, such as behind a lens. Participants are seeking clarification on the relationship between the wavevector and its spread, as well as the implications of numerical aperture in this context.
Discussion Character
- Exploratory
- Technical explanation
- Debate/contested
Main Points Raised
- Some participants question the substitution of 'k' into 'Δk' as presented in the text, suggesting it may be questionable.
- Others express understanding of equation 1.2 but seek clarification on the reasoning behind the substitution of k into Δk.
- One participant notes that the maximum possible spread in the wavevector component k is constrained by the magnitude of the vector, which cannot exceed k or be less than zero.
- It is proposed that the actual spread will be less than the maximum value and will depend on the angle of the cone of light, as determined by the numerical aperture of the lens.
- Participants reference a footnote in the text, indicating it does not provide relevant clarification on the matter.
- Some express a general dissatisfaction with parts of the book, while noting that other chapters seem clearer.
Areas of Agreement / Disagreement
Participants generally agree on the constraints of the wavevector spread but express differing views on the appropriateness of the substitution in the equations presented in the text. The discussion remains unresolved regarding the justification for this substitution.
Contextual Notes
There are unresolved questions regarding the assumptions made in the text, particularly about the substitution of k into Δk and the implications of numerical aperture on the wavevector spread.