@wsc answer is interesting but misses a key point. Jones vector are defined upto a global phase, which gives us enough degree of freedom to solve your problem.
Since your operation corresponds to a π2-rotation around the Y axis in the Poincaré sphere, it is physically doable.
Algebraically, after the first to equations, the matrix is determined to be
1√2[1eiϕ−iieiϕ].
The third condition
imposes
ϕ=−π2, which gives the final matrix
M=1√2[1−i−i1].
M is fully determined and consistent with the fourth condition.
Edited to add: A little linear agebra will show you that this matrix corresponds to a quarter wave plate rotated with a π4 angle relatively to the vertical direction.
Of course, it is easy to give physical intuition after I deduced it from the algebra:
- a quarter wave plate is needed to transform a circular polarization into a linear polarization and vice-versa;
- Applying twice the transformation swaps |H⟩ and |V⟩. This is what a half-wave plate at a π4-angle does. And a half-wave plate is nothing more that 2 stacked quarter-wave plates (at least in theory). This gives the π4-angle needed for our quarter-wave plate. QED without algebra.
This post imported from StackExchange Physics at 2017-10-08 21:12 (UTC), posted by SE-user Frédéric Grosshans