Classical Gravity Distorts Quantum Snapshots express

Original: "Tomography of a Macroscopic Quantum State influenced by Classical Self-Gravity"
arXiv:2607.06967 · 2026-07-08 · CC BY 4.0 · 1 min
A new method distinguishes quantum gravity from classical by anomalies in measurements.

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Photographing hummingbird wings with an ordinary camera gives a blurry smudge. For a sharp picture, you take many rapid shots from different angles and piece them together: that's how a quantum 'snapshot' is made. In the lab, scientists 'feel' the vibrations of a tiny mirror with a laser beam. By tracking changes in the light, they reconstruct the quantum state of this motion.

But gravity might behave differently. The Schrödinger–Newton theory suggests it remains a classical field. Then the mirror's own gravity makes it jiggle in sync with the measurement, like a camera shaking in unison with the subject. The resulting 'photograph' violates a fundamental ban, the Heisenberg uncertainty limit, like an impossibly ultra-sharp frame. Such anomalies would be a signal: if they appear, gravity is classical. It's a way to test the nature of gravity in the lab; if it turns out to be quantum, gravitational waves would appear as a stream of particles.

According to the Schrödinger-Newton theory, every object gravitationally attracts itself, and this tiny force can distort a quantum experiment.

\Delta x \Delta p \geq \frac{\hbar}{2}
The uncertainty in position (Δx) and momentum (Δp) cannot be less than half the reduced Planck constant (ħ). This is a fundamental limit on the precision of any measurement.
Scientists
Werner HeisenbergKip ThorneNiels BohrPascual JordanJohn Stewart BellJacob Bekenstein
Concepts
semiclassical gravity quantum measurement theory Schrödinger equation newtonian gravity schrodinger cat state tomography gaussian states semiclassical quantum cosmology classical physics newtonian limit no-cloning theorem macroscopic superposition john von neumann equation of state function classical model scanning tunneling microscope supergravity gravitational constant time evolution