Investigation of polarization conversion from an anisotropic thin film
碩士 === 國立臺北科技大學 === 光電工程系研究所 === 98 === In this work, we describe the propagation behavior of wave in the birefringence material by Berreman calculus, and use it to confer what the reason to form the phenomenon of polarization conversion in the anisotropic thin film. The polarization convers...
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ndltd-TW-098TIT051240252019-05-15T20:33:24Z http://ndltd.ncl.edu.tw/handle/nv6j44 Investigation of polarization conversion from an anisotropic thin film 非均向性光學薄膜之偏極轉換成因 Wen-Pao Tsai 蔡文堡 碩士 國立臺北科技大學 光電工程系研究所 98 In this work, we describe the propagation behavior of wave in the birefringence material by Berreman calculus, and use it to confer what the reason to form the phenomenon of polarization conversion in the anisotropic thin film. The polarization conversion reflection (PCR) can be enhanced in the prism-coupling configuration (prism/anisotropic thin film/air). We use the Berreman calculus to gradually analysis the reflection coefficient, transmit coefficient and the distribution of electric- magnetic field at isotropic-crystal interface and crystal-isotropic interface, then watch out for the e-ray and o-ray in the anisotropic thin film. To observe above-mentioned variation of intensity and phase, we can differentiate what is the main factor about polarization conversion。 Reality, we substitute low refractive (SiO2) anisotropic thin film to consider taking a contrast for the cause of polarization that conversion between the incident angle of higher polarization conversion reflection and the lower one. And then, we substituted for high refractive (TiO2) anisotropic thin film once again。 Yi-Jun Jen 任貽均 2010 學位論文 ; thesis 51 zh-TW |
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碩士 === 國立臺北科技大學 === 光電工程系研究所 === 98 === In this work, we describe the propagation behavior of wave in the birefringence material by Berreman calculus, and use it to confer what the reason to form the phenomenon of polarization conversion in the anisotropic thin film.
The polarization conversion reflection (PCR) can be enhanced in the prism-coupling configuration (prism/anisotropic thin film/air). We use the Berreman calculus to gradually analysis the reflection coefficient, transmit coefficient and the distribution of electric- magnetic field at isotropic-crystal interface and crystal-isotropic interface, then watch out for the e-ray and o-ray in the anisotropic thin film. To observe above-mentioned variation of intensity and phase, we can differentiate what is the main factor about polarization conversion。
Reality, we substitute low refractive (SiO2) anisotropic thin film to consider taking a contrast for the cause of polarization that conversion between the incident angle of higher polarization conversion reflection and the lower one. And then, we substituted for high refractive (TiO2) anisotropic thin film once again。
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author2 |
Yi-Jun Jen |
author_facet |
Yi-Jun Jen Wen-Pao Tsai 蔡文堡 |
author |
Wen-Pao Tsai 蔡文堡 |
spellingShingle |
Wen-Pao Tsai 蔡文堡 Investigation of polarization conversion from an anisotropic thin film |
author_sort |
Wen-Pao Tsai |
title |
Investigation of polarization conversion from an anisotropic thin film |
title_short |
Investigation of polarization conversion from an anisotropic thin film |
title_full |
Investigation of polarization conversion from an anisotropic thin film |
title_fullStr |
Investigation of polarization conversion from an anisotropic thin film |
title_full_unstemmed |
Investigation of polarization conversion from an anisotropic thin film |
title_sort |
investigation of polarization conversion from an anisotropic thin film |
publishDate |
2010 |
url |
http://ndltd.ncl.edu.tw/handle/nv6j44 |
work_keys_str_mv |
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