The thickness \(d\) needed to introduce a phase difference \(\Delta \phi = \pi/2\) in a quarter-wave plate is given by:
\[d = \frac{\lambda}{4 \times |n_e - n_o|}\]
where \(n_e\) and \(n_o\) are the refractive indices for the extraordinary and ordinary rays, respectively. Substituting the given values:
\[d = \frac{5893 \times 10^{-10} \, \text{m}}{4 \times |1.65836 - 1.48641|} \approx 8.57 \times 10^{-6} \, \text{m} = 8.57 \times 10^{-4} \, \text{mm}\]
LIST I | LIST II | ||
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A. | d²y/dx² + 13y = 0 | I. ex(c1 + c2x) | |
B. | d²y/dx² + 4dy/dx + 5y = cosh 5x | II. e2x(c1 cos 3x + c2 sin 3x) | |
C. | d²y/dx² + dy/dx + y = cos²x | III. c1ex + c2e3x | |
D. | d²y/dx² - 4dy/dx + 3y = sin 3x cos 2x | IV. e-2x(c1 cos x + c2 sin x) |