Reflectance of an absorbing medium for incident light of arbitrary polarization: correlation between the oscillatory behavior and the complex ∊ plane
The reflectance of an absorbing medium R(theta)(ø) for incident light of an arbitrary state of polarization is considered as a function of the compex dielectic constant epsilon; ø is the angle incidence and theta is an incident polarization parameter, for which cos(2)theta and sin(2)theta give the p...
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Veröffentlicht in: | Applied Optics 1990-11, Vol.29 (31), p.4633-4637, Article 4633 |
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creator | Ali, M A Mitwally, K Ahmed, S A |
description | The reflectance of an absorbing medium R(theta)(ø) for incident light of an arbitrary state of polarization is considered as a function of the compex dielectic constant epsilon; ø is the angle incidence and theta is an incident polarization parameter, for which cos(2)theta and sin(2)theta give the power fractions of incident radiation that are p- and s-polarized, respectively. Our objective is to explore the complex epsilon-plane and define the domains for which the different types of R(theta)(ø) vs ø curves (monotonic, single minimum, and secondary maximum and minimum) occur. An ethanolic solution of Rhodamine B, an organic laser dye luminofor with a well-defined resonance absorption spectrum, was chosen as the absorbing medium. We were able to define the criteria for three distinctly different types of behavior of R(theta)(ø). |
doi_str_mv | 10.1364/AO.29.004633 |
format | Article |
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Our objective is to explore the complex epsilon-plane and define the domains for which the different types of R(theta)(ø) vs ø curves (monotonic, single minimum, and secondary maximum and minimum) occur. An ethanolic solution of Rhodamine B, an organic laser dye luminofor with a well-defined resonance absorption spectrum, was chosen as the absorbing medium. 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Our objective is to explore the complex epsilon-plane and define the domains for which the different types of R(theta)(ø) vs ø curves (monotonic, single minimum, and secondary maximum and minimum) occur. An ethanolic solution of Rhodamine B, an organic laser dye luminofor with a well-defined resonance absorption spectrum, was chosen as the absorbing medium. 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Our objective is to explore the complex epsilon-plane and define the domains for which the different types of R(theta)(ø) vs ø curves (monotonic, single minimum, and secondary maximum and minimum) occur. An ethanolic solution of Rhodamine B, an organic laser dye luminofor with a well-defined resonance absorption spectrum, was chosen as the absorbing medium. We were able to define the criteria for three distinctly different types of behavior of R(theta)(ø).</abstract><cop>United States</cop><pmid>20577445</pmid><doi>10.1364/AO.29.004633</doi><tpages>5</tpages></addata></record> |
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source | Alma/SFX Local Collection; Optica Publishing Group Journals |
title | Reflectance of an absorbing medium for incident light of arbitrary polarization: correlation between the oscillatory behavior and the complex ∊ plane |
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