The fresnel prism as polarization interferometer
Here we show that a Fresnel prism can be used as a polarization interferometer. A linearly polarized beam, which is incident in this interferometer, is split into two circularly polarized beams, one right and another left, which generate the interference pattern. Interposing a solution of common sug...
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| Formato: | Capítulo de libro |
| Lenguaje: | Inglés |
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1993
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| Acceso en línea: | Registro en Scopus DOI Handle Registro en la Biblioteca Digital |
| Aporte de: | Registro referencial: Solicitar el recurso aquí |
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| 008 | 190411s1993 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-0027909360 | |
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 100 | 1 | |a Echarri, Rodolfo | |
| 245 | 1 | 4 | |a The fresnel prism as polarization interferometer |
| 260 | |c 1993 | ||
| 270 | 1 | 0 | |m Echarri, R.; Departamento de Fisica, Facultad de Ciencias Exactas y Naturales, Buenos Aires, Argentina |
| 504 | |a Françon, M., Mallick, S., (1971) Polarization Interferometers: Applications in Microscopy and Macroscopy, , Wiley Interscience, New York | ||
| 504 | |a Hecht, Zajac, (1974) Optics, pp. 272-273. , Addison‐Wesley, Reading, MA | ||
| 504 | |a Echarri, R., Simon, J., Simon, M., How to Increase the Sensitivity in a Polarization Interferometer (1991) Applied Optics, 30 | ||
| 506 | |2 openaire |e Política editorial | ||
| 520 | 3 | |a Here we show that a Fresnel prism can be used as a polarization interferometer. A linearly polarized beam, which is incident in this interferometer, is split into two circularly polarized beams, one right and another left, which generate the interference pattern. Interposing a solution of common sugar in the incident beam, the former pattern is shifted because of the circular birefringence of the sugar. Measuring the displacement of the interference pattern, we determine the phase difference between both circular polarizations introduced by the solution. Moreover, we compare this result with that obtained by measuring the rotation power, concluding that they are in good agreement. © 1993 John Wiley & Sons, Inc. Copyright © 1993 Wiley Periodicals, Inc., A Wiley Company |l eng | |
| 593 | |a Departamento de Fisica, Facultad de Ciencias Exactas y Naturales, Buenos Aires, Argentina | ||
| 690 | 1 | 0 | |a FRESNEL PRISM |
| 690 | 1 | 0 | |a INTERFEROMETER |
| 690 | 1 | 0 | |a POLARIZATION |
| 690 | 1 | 0 | |a BIREFRINGENCE |
| 690 | 1 | 0 | |a LIGHT POLARIZATION |
| 690 | 1 | 0 | |a PRISMS |
| 690 | 1 | 0 | |a CIRCULAR POLARIZATION |
| 690 | 1 | 0 | |a FRESNEL PRISMS |
| 690 | 1 | 0 | |a INCIDENT BEAMS |
| 690 | 1 | 0 | |a INTERFERENCE PATTERNS |
| 690 | 1 | 0 | |a POLARIZATION INTERFEROMETERS |
| 690 | 1 | 0 | |a POLARIZED BEAMS |
| 690 | 1 | 0 | |a ROTATION POWER |
| 690 | 1 | 0 | |a INTERFEROMETERS |
| 773 | 0 | |d 1993 |g v. 6 |h pp. 403-407 |k n. 7 |p Microwave Opt Technol Lett |x 08952477 |t Microwave and Optical Technology Letters | |
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| 856 | 4 | 0 | |u https://doi.org/10.1002/mop.4650060706 |x doi |y DOI |
| 856 | 4 | 0 | |u https://hdl.handle.net/20.500.12110/paper_08952477_v6_n7_p403_Echarri |x handle |y Handle |
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| 961 | |a paper_08952477_v6_n7_p403_Echarri |b paper |c PE | ||
| 962 | |a info:eu-repo/semantics/article |a info:ar-repo/semantics/artículo |b info:eu-repo/semantics/publishedVersion | ||