The chapter's BK7 singlet

PHYSICS · Multi-part · Fermi University Physics · Optics & Photonics · Geometrical optics and imaging · Fourier optics and image formation

What an Instrument Can See, Ch Aberrations: the phase written on the pupil

Problem

The chapter's 100 mm100\ \mathrm{mm} BK7 singlet, in its best-form bending with the stop at the lens and the object at infinity, has W040=10.6W_{040} = 10.6 waves at 587.6 nm587.6\ \mathrm{nm} when used at f/4. Take the image-space index as n=1n = 1 and the reference-sphere radius as R≈fR \approx f. ((a)) Starting from ε=−(R/n)∇W\boldsymbol{\varepsilon} = -(R/n)\nabla W with W=W040ρ4W = W_{040}\rho^4, show that the marginal ray misses the paraxial focus by TSA=8(f/#) W040\mathrm{TSA} = 8(f/\#)\,W_{040}, with W040W_{040} in length. ((b)) At fixed focal length W040W_{040} grows as the fourth power of the aperture radius in use, and at the best focus pure spherical aberration on a clear pupil leaves an rms of W040/180W_{040}/\sqrt{180}. Find the fastest f-number at which this lens meets Maréchal's criterion σW≤λ/14\sigma_W \le \lambda/14. ((c)) At f/5, find σW\sigma_W at the best focus in waves, and decide whether the Maréchal approximation can be used to estimate the lens's Strehl ratio there.

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