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Common Pitfalls

  • Confusing Fraunhofer and Fresnel diffraction. Fraunhofer (far-field) patterns are Fourier transforms; Fresnel (near-field) patterns involve Fresnel integrals. The transition occurs at Ra2/λR \sim a^2/\lambda.

  • Ignoring the phase in interference calculations. Phase differences determine constructive and destructive interference. Always track the optical path length carefully.

  • Misidentifying Brewster”s angle. Brewster’s angle is for the reflected beam, not the transmitted beam. At Brewster’s angle, the reflected light is purely ss-polarised.

  • Neglecting the difference between intensity and amplitude. Interference patterns depend on amplitudes (add with phases), while intensities add without phases for incoherent sources. The visibility of fringes is determined by the coherence of the source.

  • Forgetting that the Airy pattern involves J1J_1Not J0J_0. The first zero of J1(x)J_1(x) is at x=3.832x = 3.832Not at x=2.405x = 2.405 (which is the first zero of J0J_0).