Few-photon transport in many-body photonic systems: A scattering approach

TL;DR

This paper presents a scattering theory approach to analyze multi-photon transport in one-dimensional Bose-Hubbard lattices within QED cavity arrays, enabling direct probing of many-body states through transmitted light properties.

Contribution

It introduces an analytical scattering matrix formalism for multi-photon transport in Bose-Hubbard systems, facilitating the characterization of many-body states via photon scattering properties.

Findings

Two-photon scattering reveals the structure of many-body states.

Resonant two-photon scattering faithfully characterizes many-body states.

Losses and pulse shapes influence scattering outcomes.

Abstract

We study the quantum transport of multi-photon Fock states in one-dimensional Bose-Hubbard lattices implemented in QED cavity arrays (QCAs). We propose an optical scheme to probe the underlying many-body states of the system by analyzing the properties of the transmitted light using scattering theory. To this end, we employ the Lippmann-Schwinger formalism within which an analytical form of the scattering matrix can be found. The latter is evaluated explicitly for the two particle/photon-two site case using which we study the resonance properties of two-photon scattering, as well as the scattering probabilities and the second-order intensity correlations of the transmitted light. The results indicate that the underlying structure of the many-body states of the model in question can be directly inferred from the physical properties of the transported photons in its QCA realization. We find that a fully-resonant two-photon scattering scenario allows a faithful characterization of the underlying many-body states, unlike in the coherent driving scenario usually employed in quantum Master equation treatments. The effects of losses in the cavities, as well as the incoming photons' pulse shapes and initial correlations are studied and analyzed. Our method is general and can be applied to probe the structure of any many-body bosonic models amenable to a QCA implementation including the Jaynes-Cummings-Hubbard, the extended Bose-Hubbard as well as a whole range of spin models.