Consider a plane wave that is a superposition of two independent orthogonal plane waves that can be written as the eal part of Ē = E, exp[i (kz – wt)]î + E1 exp[i (kz – wt + m)]j where k, w, E1, and E2 are all real. f the plane wave is split and recombined after the two portions, which are polarized in the x- and y-directions, have raveled an optical path difference of 4, the observed average intensity will be proportional to 昭-踢 O (E + E2) O E +E O (E – E2)²

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Chapter1: Units, Trigonometry. And Vectors
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Consider a plane wave that is a superposition of two independent orthogonal plane waves that can be written as the
real part of
E = E, exp[i (kz – wt)|î + E1 exp[i (kz – wt + 1)]}
where k, w, E1, and E, are all real.
If the plane wave is split and recombined after the two portions, which are polarized in the x- and y-directions, have
traveled an optical path difference of , the observed average intensity will be proportional to
O E – E
O (E1 + E2)?
O E + E;
O (E1 – E2)?
Transcribed Image Text:Consider a plane wave that is a superposition of two independent orthogonal plane waves that can be written as the real part of E = E, exp[i (kz – wt)|î + E1 exp[i (kz – wt + 1)]} where k, w, E1, and E, are all real. If the plane wave is split and recombined after the two portions, which are polarized in the x- and y-directions, have traveled an optical path difference of , the observed average intensity will be proportional to O E – E O (E1 + E2)? O E + E; O (E1 – E2)?
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