By Frank Lloyd Wright
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Additional info for A Visual Encyclopedia of Frank Llyod Wright
3. Novelty filter that uses phase conjugation in a photorefractive material to select changes in a pattern. (a) Configuration of components. (b) Dark output of the novelty filter that occurs when the filter has adapted to the pattern in the spatial light modulator. (c) Output of the filter immediately after a new pattern has been supplied to the spatial light modulator. If the pattern is left unchanged, the output will gradually change to b. (From D. Z. Anderson and M. C. Erie, Resonator memories and optical novelty filters, Opt.
Xn) are the variables of the problem, f is the objective function, gi(x) are the inequality constraints, and hj(x) are the equality constraints. This formulation is general in that the problem of maximizing f(x) is equivalent to minimizing −f(x) and a constraint gi(x) ≥ 0 is equivalent to the constraint −gi(x) ≤ 0. Many modern approaches for solving (1) rely on exploiting the equations that characterize a solution. The most familiar characterization is for the case when the functions f, gi, and hj are all differentiable.
The combination of Faraday’s law with Ampere’s law, as extended by J. C. Maxwell to include so-called electric displacement currents, again gives rise to the phenomenon of a harmonic oscillation inside a cavity. But if the electromagnetic field (or light) is allowed to interact with a collection of excited atoms, a profoundly nonlinear process occurs: The atoms are stimulated to give up their extra energy at a rate that is proportional to the square of the electromagnetic field. The result is a (nonlinear) laser oscillation whose amplitude increases as long as the cavity remains supplied with excited atoms, either from the outside or by the oscillation itself.
A Visual Encyclopedia of Frank Llyod Wright by Frank Lloyd Wright