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Physics Letters A

Single-photon space-like antibunching

Thiago Guerreiro, Bruno Sanguinetti, Hugo Zbinden, Nicolas Gisin, Antoine Suárez

Published May 12, 2012• 32 citations
Publisher
DOI
10.1016/j.physleta.2012.05.019

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Quantum antibunching, vital for single-photon sources, enables applications in quantum technology, such as secure communication and quantum computing. This study investigates photon antibunching generation in a Nonlinear coupler (NLC) comprising two coupled waveguides: one linear and one with the second-order nonlinearity. Each waveguide is excited by a coherent laser source, with the second harmonic generation enhancing antibunching. Using the Schrödinger picture, the system's Hamiltonian is transformed into a master equation via the Liouville–von Neumann equation. The master equation is further translated into a Fokker–Planck equation using the positive-P representation and subsequently mapped to stochastic differential equations via Ito rules for numerical analysis. The effects of input parameters on antibunching behavior are examined, showcasing the potential of simple systems like NLCs for precise single-photon manipulation, advancing quantum technology.
Photon statistics divides light sources into three different categories, characterized by bunched, antibunched, or uncorrelated photon arrival times. Single atoms, ions, molecules, or solid state emitters display antibunching of photons, while classical thermal sources exhibit photon bunching. Here we demonstrate a light source in free space, where the photon statistics depends on the direction of observation, undergoing a continuous crossover between photon bunching and antibunching. We employ two trapped ions, observe their fluorescence under continuous laser light excitation, and record spatially resolved the autocorrelation function g^{(2)}(τ) with a movable Hanbury Brown and Twiss detector. Varying the detector position we find a minimum value for antibunching, g^{(2)}(0)=0.60(5) and a maximum of g^{(2)}(0)=1.46(8) for bunching, demonstrating that this source radiates fundamentally different types of light alike. The observed variation of the autocorrelation function is understood in the Dicke model from which the observed maximum and minimum values can be modeled, taking independently measured experimental parameters into account.