Abstract

Anderson localization is an interference effect yielding a drastic reduction of diffusion—including complete hindrance—of wave packets such as sound, electromagnetic waves, and particle wave functions in the presence of strong disorder. In optics, this effect has been observed and demonstrated unquestionably only in dimensionally reduced systems. In particular, transverse localization (TL) occurs in optical fibers, which are disordered orthogonal to and translationally invariant along the propagation direction. The resonant and tube-shaped localized states act as micro-fiber-like single-mode transmission channels. Since the proposal of the first TL models in the early eighties, the fabrication technology and experimental probing techniques took giant steps forwards: TL has been observed in photo-refractive crystals, in plastic optical fibers, and also in glassy platforms, while employing direct laser writing is now possible to tailor and “design” disorder. This review covers all these aspects that are today making TL closer to applications such as quantum communication or image transport. We first discuss nonlinear optical phenomena in the TL regime, enabling steering of optical communication channels. We further report on an experiment testing the traditional, approximate way of introducing disorder into Maxwell’s equations for the description of TL. We find that it does not agree with our findings for the average localization length. We present a new theory, which does not involve an approximation and which agrees with our findings. Finally, we report on some quantum aspects, showing how a single-photon state can be localized in some of its inner degrees of freedom and how quantum phenomena can be employed to secure a quantum communication channel.

Highlights

  • Transverse localization (TL) is found in media in which the refractive index is randomly modulated only orthogonally to the direction of propagation

  • We will report on how a single-photon state localized in some of its inner degrees of freedom could be an effective resource in quantum communication and cryptography, increasing both the amount of information loaded per single particle and the security and performance of protocols based on localized photon quanta

  • We have shown that the potential-type approach, which is analogous to the Schrödinger equation for an electron in a random potential with the potential depending on the spectral parameter E, relies on an approximation, which is only applicable to very weak disorder, and, for transverse disorder, leads to a wavelength dependence of the localization length

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Summary

Introduction

Transverse localization (TL) is found in media in which the refractive index is randomly modulated only orthogonally to the direction of propagation. In these paraxial systems, Anderson localization (AL) sustains nondiffracting beams: confined light tubes showing many potential applications including fiber optics, quantum communication, and endoscopic imaging. Localization of Light in disordered paraxial structures This last result is important as it bridges the physics of Anderson localization to the single-mode properties of optical fibers. In the first proof-of-principle photonic experiments, AL has been observed in the two-photon wave function In this scenario, it could be possible to simulate even the fermionic statistics by proper manipulation of two-photon entangled states generated by single-photon sources

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