Mode structure of an optical cavity generalize the result
Mode structure of an optical cavity. Generalize the result of the previous problem to the situation in which the cavity length is L but the material medium has length Lc
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linear functions are used to model situations that show a constant rate of change between 2 variables for example the
mode structure of an optical cavity generalize the result of the previous problem to the situation in which the cavity
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quasi-phase-matching generalize the discussion of the text leading from eq 241 to eq 246 by allowing the lengths of the
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