Pith. sign in

Creation and characterization of vector vortex modes for classical and quantum communication

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
abstract

Vector vortex beams are structured states of light that are non-separable in their polarisation and spatial mode, they are eigenmodes of free-space and many fibre systems, and have the capacity to be used as a modal basis for both classical and quantum communication. Here we outline recent progress in our understanding of these modes, from their creation to their characterization and detection. We then use these tools to study the propagation behaviour of such modes in free-space and optical fibre and show that modal cross-talk results in a decay of vector states into separable scalar modes, with a concomitant loss of information. We present a comparison between probabilistic and deterministic detection schemes showing that the former, while ubiquitous, negates the very benefit of increased dimensionality in quantum communication while reducing signal in classical communication links. This work provides a useful introduction to the field as well as presenting new findings and perspectives to advance it further.

fields

quant-ph 1

years

2026 1

verdicts

UNVERDICTED 1

representative citing papers

Topological Quantum Interferometry

quant-ph · 2026-06-18 · unverdicted · novelty 6.0

Topological quantum interferometry driven by exchange Berry phase generalizes q-plate methods to arbitrary charges, using BPX as a control parameter to decompose two-photon patterns and witness dimensionality via topological invariants.

citing papers explorer

Showing 1 of 1 citing paper.

  • Topological Quantum Interferometry quant-ph · 2026-06-18 · unverdicted · none · ref 33 · internal anchor

    Topological quantum interferometry driven by exchange Berry phase generalizes q-plate methods to arbitrary charges, using BPX as a control parameter to decompose two-photon patterns and witness dimensionality via topological invariants.