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arXiv:2305.15230 · Physical Review A

Universal limit on spatial quantum superpositions with massive objects due to phonons

Carsten Henkel, R. Folman

Published Oct 25, 2024• 27 citations
arXivHTMLPDF

Abstract

It has been a long-standing goal to bring massive objects into a superposition of different locations in real space, not only to confirm quantum theory in new regimes, but also to explore the interface with gravity. The main challenge is usually thought to arise from forces or scattering due to environmental fields and particles that decohere the large object's wave function into a statistical mixture. We unveil a decoherence channel which cannot be eliminated by improved isolation from the environment. It originates from sound waves within the object, which are excited as part of any splitting process and carry partial information. This puts stringent constraints on future spatial superpositions of large objects. Published by the American Physical Society 2024

DOI
10.1103/physreva.110.042221

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Probing quantum mechanics and quantum aspects of general relativity, along with the sensing and constraining of classical gravity, can all be enabled by unprecedented spatial sizes of superpositions of massive objects. In this paper, we show that there is a feasible setup sourced by realizable magnetic field gradients O(10–100)TO(10\text{--}100)\phantom{\rule{0.16em}{0ex}}\mathrm{T}O(10–100)T ${\mathrm{m}}^{\ensuremath{-}1}$ to construct a large spatial superposition of $O({10}^{\ensuremath{-}4}\text{--}{10}^{\ensuremath{-}8})\phantom{\rule{0.16em}{0ex}}\mathrm{m}$ for $O({10}^{\ensuremath{-}17}\text{--}{10}^{\ensuremath{-}14})\phantom{\rule{0.16em}{0ex}}\mathrm{kg}$ masses within a time of up to 0.1--10 seconds. The scale of superpositions is unrestricted as long as quantum coherence can be maintained for a required amount of time.
Preparing and detecting spatially extended quantum superpositions of a massive object comprises an important fundamental test of quantum theory. These quantum states are extremely fragile and tend to quickly decay into incoherent mixtures due to the environmental decoherence. Experimental setups considered up to date address this threat in a conceptually straightforward way---by eliminating the environment, i.e., by isolating an object in a sufficiently high vacuum. We show that another option exists: decoherence is suppressed in the presence of a strongly interacting environment if this environment is superfluid. Indeed, as long as an object immersed in a pure superfluid at zero temperature moves with a velocity below the critical one, it does not create, absorb, or scatter any excitations of the superfluid. Hence, in this idealized situation the decoherence is absent. In reality the decoherence will be present due to thermal excitations of the superfluid and impurities contaminating the superfluid. We examine various decoherence channels in the superfluid 4He^{4}\text{He}4He. It is shown that the total decoherence time can be as large as tens of seconds for a 106{10}^{6}106 amu nanoparticle delocalized over 300 nm in helium at 1 mK. Performing interference experiments in superfluid helium can provide certain practical advantages compared to conventional schemes, e.g., compensation of gravity by the buoyancy force and effective cooling.
We present a simple calculation leading to the quantum gravitationally-induced decoherence of a spatial superposition of a massive object in the linear coupling regime. The point of this calculation is to illustrate that the gravitationally-induced collapse could be of the same origin as any other collapse, i.e. due to the entanglement between the system (here a massive object) and its environment (in this case gravity, but it could well be the electromagnetic or any other field). We then point out that, in some cases, one has to be careful when concluding that matter-wave interference of large masses (to be quantified) would be prevented by their coupling to the gravitational field. We discuss how to experimentally discriminate between decoherence due to entanglement, decoherence due to classical dephasig as well as a genuine collapse of quantum superpositions (if such a process exists at all).