Take an incident field along , without loss of generality because this component has the same circular eigenmodes for every direction of input linear polarization. Resolve its Jones vector into equal circular components:
Using the complex amplitude convention , the real circular contributions are
They counter-rotate and add to
In general the tip traces an ellipse with semiaxis lengths and . Equal transmitted circular wave amplitudes produce a line; removal of one circular mode, or , produces a circle. The special zero-output case has no defined polarization of waves.

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