(a) A microscope objective has and the imaging wavelength is . A microscopist wants…

PHYSICS · Subjective · Fermi University Physics · Optics & Photonics · Fourier optics and image formation · Coherence and statistical optics

What an Instrument Can See, Ch Spatial coherence and the van Cittert-Zernike theorem

Problem

(a) A microscope objective has NAobj=0.90\mathrm{NA}_{\text{obj}} = 0.90 and the imaging wavelength is λ=550 nm\lambda = 550\,\text{nm}. A microscopist wants the highest transmitted spatial frequency to be 2.62.6 cycles per micrometre. Using the coherence-parameter model σc=NAcond/NAobj\sigma_{\mathrm{c}} = \mathrm{NA}_{\text{cond}}/\mathrm{NA}_{\text{obj}} and the cutoff (1+σc)NAobj/λ(1+\sigma_{\mathrm{c}})\mathrm{NA}_{\text{obj}}/\lambda (valid for σc≤1\sigma_{\mathrm{c}}\le1), find the condenser numerical aperture NAcond\mathrm{NA}_{\text{cond}} and the resulting value of σc\sigma_{\mathrm{c}} that are needed. (b) The same laboratory later measures the visibility of an interferometer observing a red giant star at λ=550 nm\lambda = 550\,\text{nm} and finds the first visibility null at a baseline of B0=5.4 mB_0 = 5.4\,\text{m}. Assuming a uniform-disc brightness model, find the fitted angular diameter of the star in milliarcseconds, and state, without recomputing, how a limb-darkened model would change this figure.

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