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At what point does spacetime become quantum?

Matt O'Dowd challenges a fundamental assumption in modern physics: that probing the quantum nature of gravity requires building a particle accelerator the size of the solar system. Instead, he argues that the answer might lie in a regular laboratory, where the quantum world is made large enough to meet gravity halfway. This is not just a theoretical pivot; it is a call to action for experimentalists to stop waiting for impossible machinery and start coaxing the mesoscale to reveal its secrets.

The Mesoscale Meeting Ground

O'Dowd begins by dismantling the rigid boundary we often draw between the classical and quantum realms. He notes that "the quantum world is certainly strange. Objects in multiple places and states at once, random transitions between states and places, weird instantaneous communication over large distances, all that good quantum weirdness." Yet, he points out the paradox: "But perhaps the strangest thing about quantum mechanics is that its rules seem so different from the classical large scale world. And yet the latter comes from the former. But how?" The author's central thesis is that the transition isn't a hard wall but a gradient, a "mesos scale" that feels both worlds. As O'Dowd puts it, "Maybe we don't have to wait for that solar system size particle accelerator to do this cool stuff. We'll look at two paths. One is to look for a breakdown in our classical understanding of gravity at the mesos scale. The second will be to look for true quantum effects in as large a system as possible, but also in the mesos scale." This reframing is compelling because it shifts the burden of proof from building the unbuildable to refining the measurable.

If we can get them to meet somewhere in the middle, maybe we can even make gravity quantum.

The author's approach to testing this involves a modern resurrection of the Cavendish experiment. O'Dowd explains that while Henry Cavendish famously "weighed the Earth" in 1798 using lead balls, the real challenge today is shrinking the masses to see if gravity behaves differently at smaller scales. He highlights the immense difficulty: "The gravitational attraction between two electrons is about 42 orders of magnitude weaker than the repulsive electromagnetic force pushing them apart, making it essentially impossible to measure gravity." By detailing the Vienna experiment where physicists measured the gravitational pull of gold spheres weighing less than 100 milligrams, O'Dowd demonstrates that the noise floor is the enemy, not the laws of physics. He notes the extreme measures taken, such as running experiments "mostly between midnight and 5:00 a.m. during the quiet Christmas season" to avoid seismic and gravitational noise from trams and people. This level of detail effectively grounds the abstract theory in the gritty reality of experimental physics.

At what point does spacetime become quantum?

Critics might note that even with these refinements, we are still orders of magnitude away from the Planck mass, where quantum gravity effects are theoretically expected to dominate. The leap from a 100-milligram gold ball to a truly quantum object remains a canyon, not a step. However, O'Dowd acknowledges this, suggesting that while the Cavendish setup has limits, "other approaches like levitating nano particles or cryogenic suspension may make it possible" to bridge the gap.

Entangling the Macroscopic

The second path O'Dowd explores is pushing quantum entanglement into the macroscopic realm. He defines the phenomenon clearly: "Entanglement should exist between large systems, but the larger the system, the harder it is to observe. The correlations between individual particles can be smeared out and lost to the surrounding environment in a process called decoherence." The author's argument here is that decoherence is the primary barrier to a unified theory, and observing it in large systems is the key to understanding the quantum-classical transition. He points to optomechanics, where laser light bouncing between mirrors creates a feedback loop that can entangle the mirrors themselves. "Done carefully enough this correlation can be a true quantum entanglement," O'Dowd writes, citing experiments that have already entangled microscopic membranes.

The pièce de résistance of his argument is the suggestion to use the Laser Interferometer Gravitational-Wave Observatory (LIGO) for this purpose. He argues that since LIGO was built to detect spacetime ripples, "in principle could be used to detect correlations in the oscillations of the mirrors that point to true entanglement between these genuinely macroscopic objects." This is a bold synthesis of two distinct fields: gravitational wave astronomy and quantum information science. O'Dowd emphasizes that "many of the challenges for doing this with LIGO have already been solved," specifically the noise mitigation required to detect gravitational waves. By leveraging existing infrastructure, he transforms a theoretical impossibility into a near-future engineering challenge.

The laws of gravity may not be too different for these subund masses. But since the gold balls used here are more comparable to a baseball in size than to an atom, that may not be too surprising.

Bottom Line

Matt O'Dowd's most persuasive move is reframing the search for quantum gravity from a quest for larger energy scales to a quest for better isolation at smaller mass scales. His argument is strongest when he details the ingenuity required to measure the gravity of a gold bead or the entanglement of a mirror, proving that the "solar system size" collider is not the only path forward. The biggest vulnerability remains the sheer scale of the gap between current mesoscale experiments and the Planck scale, but his proposal to use LIGO offers a tangible, albeit difficult, bridge. Readers should watch for the next generation of optomechanical experiments, as they may well be the first to crack the code of how spacetime becomes quantum.

Sources

At what point does spacetime become quantum?

by Matt O'Dowd · PBS Space Time · Watch video

Thank you to Anyesk for supporting PBS. To observe the quantum nature of gravity and of spaceime itself, we need a particle collider the size of the solar system. Or we could just physics smarter and build one on a lab bench. Here's how.

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The quantum world is certainly strange. Objects in multiple places and states at once, random transitions between states and places, weird instantaneous communication over large distances, all that good quantum weirdness. But perhaps the strangest thing about quantum mechanics is that its rules seem so different from the classical large scale world. And yet the latter comes from the former.

But how? And at what size does that happen? A related mystery is the connection between gravity and the quantum. Gravity seems more in line with the classical world.

It is crisply defined and very non-random. But gravity is the fabric of spaceime which is knit together on scales far smaller than the quantum. So at what point does spacetime itself become quantum? The question of the quantum classical transition and the related quantum gravity connection are notoriously difficult to probe directly due to the challenge of accessing the minuscule quantum world and the minuscular quantum gravity world.

But maybe the answer is not to build tidy experiments or giant colliders, but to make the quantum world big enough to meet gravity and the classical world halfway, perhaps inside a regular laboratory. The known laws of physics can be pretty clearly broken up into these two realms, those describing the large scale classical world and the tiny quantum world. Classical physics works great above about a micrometer where objects are made of many atoms. Everything larger is as we say macroscopic.

Quantum mechanics rules below the nanometer scale. At single molecules and atoms and smaller but the in between scale, the ...