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Derive the Jones matrix, Eq. (14-15),representing a linear polarizer whose transmission axis is at arbitrary angle θ with respect to the horizontal #question: anyone can help to solution it by use method in second image. ***** thoroughly solution ********

M-Linoso, cos2 θ sin θ cos θ sin θ cos θ linear polarizer, TA at θ (14-15) sin 2 θ

tion 14-2 Mathematical Representation of Potarize simultancously present at each point along the axis The fast axis nd slow axis (SA) directions of the plate are also indicated. When the chase difference Δφ-π/2, the retardation plate is called a quarter-wave in a o be ewhen it is π, it is called a half-wave plate. the tion ugh sotatoror has the effecet of rotating the direction of inearly polarized light h on it by some particular angle. Vertical linearly polarized light is on a rotator in Figure 14-10. The effect of the rotator element hunsmit linearly polarized light whose direction of vibration has been, in icu- te- des trans e n rotated counterclockwise by an angleo Figure 14 .desire now to create a set of matrices corresponding to these three types darizers so that just as the optical element alters the polarization mode the actual light beam, an element matrix operating on a Jones vector will cht uce the same result mathematically. We adopt a pragmatic point of view ormulating appropriate matrices. For example, consider a linear polarizer th a transmission axis along the vertical, as in Figure 14-8. Let a 2 x 2 ma- is representing the polarizer operate on vertically polarized light. and let of elements of the matrix to be determined be represented by letters a, b, c. d. The resultant transmitted or product light in this case must again be vertically linearly polarized light. Symbolically This matrix equation -according to the rules of matrix multiplication is a(o) + b(1) 0 c(0) + d(1) 1 equivalent to the algebraic equations 0 and d 1 . To determine elements a and c, let from which we conclude b the same polarizer operate on horizontally polarized light. In this case, no light is transmitted, or The corresponding algebraic egnatoss are now from which a 0 and c 0, We conclude here without further proof. then, that the appropriate matrix is linear polarizer. TAerical(14-13) The matrix for a linear polarizer, TA horizontal, can be obtained in a similar manner and is included in Table 14-2, near the end of this chapter. Suppose ext that the linear polarizer has a TA inclined at 45 to the x-axis. To keep n as simple as possible we consider, in turn, the action of the polarizer t lincarly polarized in the same direction as-and perpendicular he TA of the polarizer. Light polarized along the same direction as s represented by the Jones vector and light with a polarization

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