Distinguishability in quantum interference with the squeezed states

TL;DR

This paper develops a theory of distinguishability in quantum interference of squeezed vacuum states, quantifies it via the internal state probability, and applies it to experimental Gaussian boson sampling, revealing how purity affects interference.

Contribution

It introduces a new distinguishability measure based on the symmetric part of the internal state and applies first-order quantization to analyze interference of squeezed states.

Findings

Distinguishability decreases exponentially with the number of photon pairs.

Experimental purity levels significantly influence interference probabilities.

The approach applies to both Gaussian and non-Gaussian squeezed states.

Abstract

Distinguishability theory is developed for quantum interference of the squeezed vacuum states on unitary linear interferometers. It is found that the entanglement of photon pairs over the Schmidt modes is one of the sources of distinguishability. The distinguishability is quantified by the symmetric part of the internal state of $n$ pairs of photons, whose normalization $q_{2n}$ is the probability that $2n$ photons interfere as indistinguishable. For two pairs of photons $q_{4}=(1+ 2\mathbb{P} )/3$, where $\mathbb{P} $ is the purity of the squeezed states ($K=1/\mathbb{P} $ is the Schmidt number). For a fixed purity $\mathbb{P}$, the probability $q_{2n}$ decreases exponentially fast in $n$. For example, in the experimental Gaussian boson sampling of H.-S.~Zhong \textit{et al} [Science \textbf{370}, 1460 (2020)], the achieved purity $\mathbb{P}\approx 0.938$ for the average number of photons $2n\ge 43$ gives $q_{2n}\lesssim 0.5$, i.e., close to the middle line between $n$ indistinguishable and $n$ distinguishable pairs of photons. In derivation of all the results the first-order quantization representation based on the particle decomposition of the Hilbert space of identical bosons serves as an indispensable tool. The approach can be applied also to the generalized (non-Gaussian) squeezed states, such as those recently generated in the three-photon parametric down-conversion.