Orientation of Major Axis for polarized light

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Homework Help Overview

The discussion revolves around the orientation of the major axis for polarized light, specifically focusing on cases involving linear and circular polarization. Participants are exploring the implications of their findings in the context of polarized light behavior.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to understand the undefined angle in case 2 of their problem. Some participants discuss the implications of circular polarization and the conditions under which the angle becomes undefined. Others raise questions about determining the handedness of the circular polarization.

Discussion Status

There is an ongoing exchange of ideas, with some participants confirming each other's reasoning regarding circular polarization. Guidance has been offered about additional considerations, such as identifying the handedness of the polarization, but no consensus has been reached on the specifics of the problem.

Contextual Notes

Participants are navigating the complexities of polarization without complete information about the cases being discussed. The references to external resources suggest a reliance on additional materials for clarification.

Blanchdog
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Homework Statement
Consider the Jones vector: $$\begin{pmatrix}A \\Be^{i \delta}\end{pmatrix}$$ For the following cases, what is the orientation of the major axis, and
what is the ellipticity of the light? Case I: ##A = B = \frac{1}{\sqrt{2}}; \delta = 0;## Case II: ##A = B = \frac{1}{\sqrt{2}}; \delta = \frac{\pi}{2};## Case III: ##A = B = \frac{1}{\sqrt{2}}; \delta = \frac{\pi}{4}##
Relevant Equations
$$\alpha = \frac{1}{2}tan^{-1}(\frac{2 A B cos(\delta)}{A^2-B^2})$$
$$E_{\alpha}=|E_{eff}|\sqrt{A^2 cos^2(\alpha) + B^2 sin^2(\alpha) + 2 A B cos(\delta)sin(2 \alpha)}$$
$$E_{\alpha \pm \frac{pi}{2}}=|E_{eff}|\sqrt{A^2 cos^2(\alpha) + B^2 sin^2(\alpha) - 2 A B cos(\delta)sin(2 \alpha)}$$
Case 1 worked out great, I found it to be linearly polarized light at an angle ##\alpha = \frac{\pi}{4}##, but Case 2 is giving me trouble. As best I can tell, ##\alpha## is undefined in case 2. How do I solve case 2?
 
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I believe I figured it out, though I would love confirmation. Since ##cos(\delta) = cos(\frac{\pi}{2})=0## and ## A = B##, we end up with ## E_\alpha = E_{\alpha_\pm+\frac{pi}{2}}##. That means we have circularly polarized light! So of course ##\alpha## is undefined; a circle has no determined axes!
 
You are correct. Your professor might also want you to say if it is right-hand or left-hand circular polarized. More information can be found here https://en.wikipedia.org/wiki/Jones_calculus
And you can use euler's equation to make the exponential into trig functions and plug in the angle.
 
stephen8686 said:
You are correct. Your professor might also want you to say if it is right-hand or left-hand circular polarized. More information can be found here https://en.wikipedia.org/wiki/Jones_calculus
And you can use euler's equation to make the exponential into trig functions and plug in the angle.
How can I tell the handedness?
 

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