Calculate Jones Vector of polarized light thorugh QWP

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SUMMARY

The discussion centers on calculating the Jones vector for vertically polarized light passing through a quarter waveplate (QWP) rotated at an angle of θ = π/4. The Jones matrix for the rotated QWP is defined as J_Q = (1/√2) * [[1, i], [i, 1]]. The user attempts to compute the resulting Jones vector J' by multiplying J_Q with the Jones vector for vertical light (J_VLP), resulting in J' = (1/√2) * [[i], [1]]. However, the expected answer is J' = (1/√2) * [[1], [i]]. The discussion reveals that the discrepancy arises from the orientation of the QWP's fast axis prior to rotation, confirming that the two resulting vectors represent different polarizations.

PREREQUISITES
  • Understanding of Jones vectors and matrices
  • Familiarity with quarter waveplates (QWPs)
  • Knowledge of polarization states of light
  • Basic linear algebra for matrix multiplication
NEXT STEPS
  • Study the properties of Jones matrices in optical systems
  • Learn about the effects of rotating optical elements on polarization
  • Explore the concept of equivalent Jones vectors and their implications
  • Investigate the mathematical derivation of Jones vectors for various polarization states
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Optical physicists, students studying optics, and engineers working with polarized light systems will benefit from this discussion.

mhsd91
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Homework Statement



Find the final polarization in terms of Jones vectors for vertical polarized, coherent light passing through a quarter waveplate rotated \theta = \pi/4. The Jones matrix for the rotated waveplate is given as,

J_Q = \frac{1}{\sqrt{2}} \cdot <br /> \left( \begin{array}{cc}<br /> 1 + i\cos(2\theta) &amp; i\sin(2\theta) \\<br /> i\sin(2\theta) &amp; 1-i\cos(2\theta) \end{array} \right)<br /> <br />

Which for the given angle results in:

<br /> <br /> J_Q = \frac{1}{\sqrt{2}} \cdot <br /> \left( \begin{array}{cc}<br /> 1 &amp; i \\<br /> i &amp; 1 \end{array} \right)<br />


The Attempt at a Solution



Now, this should be straight forward: J&#039; = J_Q J_{VLP}:

<br /> <br /> J&#039; = \frac{1}{\sqrt{2}} \cdot <br /> \left( \begin{array}{cc}<br /> 1 &amp; i \\<br /> i &amp; 1 \end{array} \right) \cdot<br /> <br /> \left( \begin{array}{c}<br /> 0 \\<br /> 1 \end{array} \right)<br /> <br /> <br /> = \frac{1}{\sqrt{2}}\left( \begin{array}{c}<br /> i \\<br /> 1 \end{array} \right)<br /> <br /> <br />

The problem is that I am given the answer, which is not what i got, but rather:

<br /> \frac{1}{\sqrt{2}}\left( \begin{array}{c}<br /> 1 \\<br /> i \end{array} \right)<br />

So I wonder: One of three possible outcomes: (1) since Jones vectors gived us the phase difference are these two vectors equivalent!?

<br /> \left( \begin{array}{c}<br /> 1 \\<br /> i \end{array} \right)<br /> <br /> \equiv<br /> <br /> \left( \begin{array}{c}<br /> i \\<br /> 1 \end{array} \right)<br /> <br />
.. overlooking the normalization constants.

(2) I have calculated wrong: please help!
(3) There is an error in the answer the problem.

Thank you very much!:)
 
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Perhaps your problem may come from some ambiguity as to what the plate was like before rotating. I get

<br /> \frac{1}{\sqrt{2}}\left( \begin{array}{c}<br /> 1 \\<br /> i \end{array} \right)<br />

When I consider the fast axis of the quarter wave plate to be in the vertical direction before rotation.

I get your answer when I consider the quarter wave plate before rotation to have the fast axis horizontal.

And no, they do not represent the same polarization. They do not differ by a phase.
 
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