Imagine that we have a nonabsorbing glass plate of index n and thickness Îy, which stands between

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Imagine that we have a nonabsorbing glass plate of index n and thickness Δy, which stands between a source S and an observer P.

(a) If the unobstructed wave (without the plate present) is Eu = Eexp iω(t - y/c), show that with the plate in place the observer sees a wave

Eo exp io [t - (п - 1)Ду/с — у/c] d,

(b) Show that if either n ‰ˆ 1 or Δy is very small, then

E, = E, + о(п — 1)Ду -im/2 - E̟e

The second term on the right may be envisioned as the field arising from the oscillators in the plate.

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Optics

ISBN: 978-0133977226

5th edition

Authors: Eugene Hecht

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