Camparison of the Hanbury Brown-Twiss effect for bosons and fermions

TL;DR

This paper experimentally compares the Hanbury Brown-Twiss effects for bosonic and fermionic helium isotopes, demonstrating quantum statistical differences in bunching and antibunching behaviors using atom-atom correlation measurements.

Contribution

It provides the first direct experimental comparison of HBT effects for bosons and fermions in the same setup with helium isotopes, highlighting quantum statistical influences.

Findings

Bosonic helium exhibits bunching behavior.

Fermionic helium shows antibunching behavior.

Quantum statistics alone account for the observed effects.

Abstract

Fifty years ago, Hanbury Brown and Twiss (HBT) discovered photon bunching in light emitted by a chaotic source, highlighting the importance of two-photon correlations and stimulating the development of modern quantum optics . The quantum interpretation of bunching relies upon the constructive interference between amplitudes involving two indistinguishable photons, and its additive character is intimately linked to the Bose nature of photons. Advances in atom cooling and detection have led to the observation and full characterisation of the atomic analogue of the HBT effect with bosonic atoms. By contrast, fermions should reveal an antibunching effect, i.e., a tendency to avoid each other. Antibunching of fermions is associated with destructive two-particle interference and is related to the Pauli principle forbidding more than one identical fermion to occupy the same quantum state. Here we report an experimental comparison of the fermion and the boson HBT effects realised in the same apparatus with two different isotopes of helium, 3He (a fermion) and 4He (a boson). Ordinary attractive or repulsive interactions between atoms are negligible, and the contrasting bunching and antibunching behaviours can be fully attributed to the different quantum statistics. Our result shows how atom-atom correlation measurements can be used not only for revealing details in the spatial density, or momentum correlations in an atomic ensemble, but also to directly observe phase effects linked to the quantum statistics in a many body system. It may thus find applications to study more exotic situations >.