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Phase change of light reflected by a discontinuity in the derivatives ...

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70R. Diamant, M. Fernández-Guasti / Optics Communications 294 (2013) 64–72Fig. 7. Amplitude equation solutions for type C 2 pr<strong>of</strong>iles, a close look at <strong>the</strong> solutions <strong>in</strong> <strong>the</strong> oscillat<strong>in</strong>g regions. (a) Solutions for ‘‘l<strong>in</strong>&cubexpþ’’ and ‘‘cubexp&l<strong>in</strong>þ’’ and(b) solutions for ‘‘l<strong>in</strong>&cubexp ’’ and ‘‘cubexp&l<strong>in</strong> ’’.Table 6Calculated reflectivity and approximate phase difference d between <strong>in</strong>cident and <strong>reflected</strong> waves at <strong>the</strong> reflection plane, z¼0, related to <strong>the</strong> type C 2 pr<strong>of</strong>iles. The symbol s Rstands for <strong>the</strong> reflectivity standard deviation.C 2 function Reflectivity (%) R Reflectivity relativestandard deviation (%) s R 100Rl<strong>in</strong>&cubexpþ 1:33978 10 6 0.0045 p2cubexp&l<strong>in</strong>þ 5:15290 10 8 1.2 p2l<strong>in</strong>&cubexp 5:18475 10 8 0.020 p2cubexp&l<strong>in</strong> 1:33984 10 6 0.014 p2Approximate phase <strong>change</strong>at reflection plane z¼0Offset from <strong>the</strong> exact p 2 orpvalue <strong>in</strong> p units20:00170:0030:00470:0040:01570:0050:01170:005Table 7Type C 3 pr<strong>of</strong>iles. The piecewise junction is always at z¼0. Herepa 4 ¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi pffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi44lnð0:95Þ lnð0:05Þ so that D is <strong>the</strong> <strong>in</strong>terface thickness, <strong>the</strong> distance neededfor n to <strong>change</strong> 90% <strong>of</strong> <strong>the</strong> total Dn ¼ n g n a.Label n(z) d 4 nat <strong>the</strong> junction4dz8l<strong>in</strong>&quartexpþ < n a zo0a 4:4n g ðn g n aÞ expD z zZ0quartexp&l<strong>in</strong>þ8

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