Currently, the internal and phase integrals for indefinite polarization produce wrong results. The reason lies in the lack of an interface for elliptic polarizations. Say we want to describe elliptic polarization with a polarization parameter $\xi$, the field reads
$$A^\mu(\phi) = g(\phi)(\epsilon_1\cos\xi\cos\phi + \epsilon_2\sin\xi\sin\phi)$$
Therefore, we should implement a new polarization type, which serves these parameterized polarization vectors.
Currently, the internal and phase integrals for indefinite polarization produce wrong results. The reason lies in the lack of an interface for elliptic polarizations. Say we want to describe elliptic polarization with a polarization parameter$\xi$ , the field reads
Therefore, we should implement a new polarization type, which serves these parameterized polarization vectors.