GoosHanchen.gif(254 × 191 pixels, file size: 578 KB, MIME type: image/gif, looped, 25 frames, 1.0 s)

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Русский: Сдвиг Гуса-Хенхена для конечной плоской электромагнитной волны на границе оптических сред. Поверхностная волна переносит энергию ниже границы из левой части падающей волны в правую часть отраженной волны. Цветом отображается квадрат напряженности электрического поля. Показатель преломления верхней среды – 2, нижней среды ¬– 1, угол падения 45 градусов. Сдвиг Гуса-Хенхена составляет 0.3 длины волны в вакууме.
English: Goos-Hänchen shift for a finite plane electromagnetic wave at the border of two optical mediums. Surface wave transfers some energy under the border from the left part of the falling wave to the right part of the reflected wave. Bright areas stay for high electric strength square. Upper medium has high refraction index (n = 2), lower medium is air (n = 1), angle of incidence is 45 degrees. Goos-Hänchen shift is equal to 0.3 of wavelength in vacuum.
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Temaotheos

Kogami2

Рисунок отражает результат дипломной работы Сентябовой М.В., Сибирский федеральный университет, ИФО ИИФиРЭ, кафедра фотоники и лазерной технологии http://physmatik.narod.ru/Tasks/_html/Nirs.htm

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current09:26, 1 February 2011Thumbnail for version as of 09:26, 1 February 2011254 × 191 (578 KB)Temaotheos{{Information |Description ={{ru|1=Сдвиг Гуса-Хенхена для конечной плоской электромагнитной волны на границе оптических сред. Поверхностная волна перен

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