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PostWysłany: ¦ro 10:11, 06 Kwi 2011    Temat postu: Pauli matrix study using a new method of polarizat

Pauli matrix study using a new method of polarization aberration theory


Angle to, such as from burst to H (P, at, the incident angle of light. ... The component is Et, E,scarpe nike 2011,, there ... () (Type ... coffee a day,)) Fresnel:) where (lack of) buildings) J-... [(psi ... nop - H a ') (3】 (4】 (5) (6) 2 by such rumors, the use of Pault matrix refuse polarization aberration theory study a new method .185 .=: a (pcos (ps.n a H) (r. + rp) / A is the physical picture more clearly, we will be J (p-kun. H) wrote:., a! a [c. mound +2 2 (mock 'a ∞) day l) 112 A D F, and Li = a small angle of incidence (j ≤ 5 ·), the f., f. developed into i the series, taking the former two have a c + ct on one type will be substituted into (7 ), we obtain J =} Tuo ∞ s2 aberration analysis. will be considered on the type of the three aberrations inherent in the three polarization, if Figure 2 shows the linear polarized = () the polarization state distribution in the exit pupil on the three state distribution for the incident polarization effects shown in Figure 3 to 5. Figure shows the big picture in the bud. c stern ellipsoid in () picture bud head in the direction of the electric field. vector length represents the amplitude of the first year ... ', 0, small. vector center of the transmitted light location, and other plans as well. Distribution of the polarization state after 4 Conclusions 1) from (1) shows, the use of Pauli matrices of polarization aberration theory, can be very simple and explicitly given the problems l86 · Jiangxi University University (Natural Science) 1992 Circle 42pH (sin ~ a distribution of emitted light polarized distribution of the polarization after the role of theoretical results, and to ask the shrews of the physical concept is clear, profound physical meaning. 2) Figure 2 5 shows the use of Pauli matrices of polarization aberrations, clear simple and clear physical picture, which further re playing with a sense of polarization aberrations 3) the use of (10) for a known incident polarization beam, the reflected beam's polarization state distribution can be simply given. 4) The calculation shows that (taking i = 5.) ​​Polarized light beam after reflection, the polarization of light emitted is no longer uniformly distributed; linear polarized incident to the transparent medium (glass N = 1.5), the amplitude of the reflectivity difference between the 4 { polarization azimuth difference ~ 2. ; Linear polarized incident to the absorbing medium (copper N A 0.76 a j2.46), a polarized incident light generally becomes elliptical. The elliptical rate distribution in the 0 ~ I. 3} the change in the beam polarization state out of this uneven distribution, the precision optical measurement and design should attract enough attention.
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