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Studies electromagnetic waves in and near dielectric surfaces, S whose radii of curvature R are large compared with the surface wavelength 2 pi /K r , for cases when the dielectric constant epsilon <-1. If such gentle bends are convex towards the vacuum the wave is not perfectly bound-it attenuates with decay length K i -1 , the lost energy being radiated to infinity. The radiation appears to emerge tangentially into vacuum from the height z r above S where the wave changes from evanescent to oscillatory. When S is concave to the vacuum it is argued that there should be no attenuation. On general gently bent surfaces the wave energy travels along rays that are geodesics on S. The focusing of families of rays on S are discussed and it is shown that the imperfect focus of a plane wave incident on a general circularly symmetric hill is a cusped caustic with two rainbows as asymptotes. Perfect focusing is also possible and we calculate the shape of the 'geodesic lens' that would produce this.
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Michael Berry (1975) studied this question.
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