Observation-dependent suppression and enhancement of two-photon coincidences by tailored losses

TL;DR

This paper demonstrates experimentally that two-photon coincidence statistics can be tuned from suppression to enhancement by tailored losses, revealing new ways to manipulate multi-particle quantum states for quantum information processing.

Contribution

It introduces a novel method to control two-photon interference effects using tailored dissipation, enabling seamless transition between suppression and enhancement of coincidences.

Findings

Two-photon coincidences can be tuned from suppression to enhancement.

Tailored losses can manipulate quantum interference effects.

New approach for quantum state control in non-Hermitian systems.

Abstract

The uncanny ability of multiple particles to interfere with one another is one of the core principles of quantum mechanics, and serves as foundation for quantum information processing. In particular, the interplay of constructive and destructive interference with the characteristic exchange statistics of indistinguishable particles give rise to the Hong-Ou-Mandel (HOM) effect, where the bunching of bosons can lead to a perfect suppression of two-particle coincidences between the output ports of a balanced beam splitter. Conversely, in the case of two fermions, anti-bunching can systematically enhance these coincidences up to twice the baseline value of distinguishable particles. As such, the respective emergence of dips or peaks in the HOM experiment may at first glance appear to be indicative of the bosonic/fermionic nature of the incident particles. In this work, we demonstrate experimentally that the two-particle coincidence statistics of two bosons can instead be seamlessly tuned from the expected case of suppression to substantial enhancement by an appropriate choice of the observation basis. To this end, our photonic setting leverages birefringent polarization couplers to selectively introduce dissipation in the photons polarization degree of freedom. Notably, the mechanism underpinning this this highly unusual behaviour does not act on the individual phases accumulated by pairs of particles along specific paths, but instead allows them to jointly evade losses, while indistinguishable photons are prevented from being simultaneously detected in orthogonal modes. Our findings reveal a new approach to harnessing non-Hermitian settings for the manipulation of multi-particle quantum states and as functional elements in quantum simulation and information processing.