LiNbO3-based endless optical polarization control features properties which electronic polarization processors of coherent optical receivers lack: Superior bandwidth, absence of O-E-O conversion, optional stabilization of normalized Stokes space and applicability for quantum key distribution. We review the state-of-the-art.
In this dissertation, the polarization-state control in coherent optical fiber communications is studied. A new automatic polarization-state control scheme called "polarization recombing" is proposed and experimentally verified. The system consists of a polarization beam splitter (a Wallaston prism), a 90° linear polarization rotator, and endless phase shifter, and a beam combiner. It features a very simple (probably the simplest) principle for polarization-state control and endlessness (resetting-free) in control is achieved. IN addition, in this scheme, the polarization-state of output light is always linear with a fixed inclination angle regardless of changes in the polarization-state of the incoming light. Such a characteristic is achieved without the aid of a polarimeter and is particularly useful in homodyne phase diversity receiver because a stable linearly polarized light is necessary for generating two lights having 90° phase difference. This feature has been demonstrated in simulated self-homodyne DPSK phase diversity receiver. It is fund that the scheme functions satisfactorily and the receiver sensitivity fluctuation is kept within 0.5 dB. at 200 Mbits/sec.
Dynamic polarization controllers are key devices with broad applications in many fields. However, most on-chip polarization controllers still rely on traditional blind-search methods, whereas analytical optical-computing approaches remain insufficiently explored, particularly with respect to calibration and endless polarization control. With the accurate relative phase of Mach-Zehnder interferometer (MZI) being fully controllable on an integrated photonics chip, we present an analytical polarization control (APC) method using four phase shifters and optical computing, eliminating the need for the traditional inefficient blind-search procedure. The basic structures and operations of APC are clarified. The proposed calibration method and endless control method enable continuous APC while compensating for phase differences within the MZI structures. We simulate the influence of the endless control unit on polarization control and quantify the effect of the fourth phase difference on the output extinction ratio. With the fourth phase shifter, the phase difference encountered during Stokes vector measurement can be effectively compensated, and rotations around all three axes on the Poincaré sphere can be realized. These results establish a practical APC architecture based on optical computing for photonics chips. The proposed APC methods, combined with a FPGA-based hardware acceleration, will enable high speed on-chip polarization controllers.
We comprehensively review the quantum theory of the polarization properties of light. In classical optics, these traits are characterized by the Stokes parameters, which can be geometrically interpreted using the Poincaré sphere. Remarkably, these Stokes parameters can also be applied to the quantum world, but then important differences emerge: now, because fluctuations in the number of photons are unavoidable, one is forced to work in the three-dimensional Poincaré space that can be regarded as a set of nested spheres. Additionally, higher-order moments of the Stokes variables might play a substantial role for quantum states, which is not the case for most classical Gaussian states. This brings about important differences between these two worlds that we review in detail. In particular, the classical degree of polarization produces unsatisfactory results in the quantum domain. We compare alternative quantum degrees and put forth that they order various states differently. Finally, intrinsically nonclassical states are explored, and their potential applications in quantum technologies are discussed.