A 1-milligram rotor’s motion is controlled with quantum measurement

Researchers achieved unprecedented quantum control of a 1‑mg rotor, reaching an entropic temperature of 140 nK via continuous measurement and ultra‑low damping.

A 1-milligram rotor’s motion is controlled with quantum measurement

Introduction

A recent experiment has demonstrated that the motion of a milligram‑scale rotor can be steered with quantum‑level precision. By isolating the rotor in an ultra‑high‑vacuum environment and continuously measuring its yaw angle, the team reduced the effective "entropic temperature" of the conditional state to 140 nK—about two orders of magnitude colder than previous tabletop optomechanical results. This breakthrough opens new pathways for testing the quantum‑classical boundary and for probing subtle gravitational effects with macroscopic objects.

Achieving Extreme Isolation and Low Damping

The key to the result is an unprecedented damping rate of 7 nHz, indicating that external disturbances are virtually eliminated. The rotor—made of fused silica and coated with dielectric mirrors—hangs as a torsional pendulum inside a vacuum chamber below 10⁻⁹ mbar. A passive seismic isolation platform (resonance ~0.4 Hz) and active magnetic‑coil feedback further suppress vibrations. Together, these measures allow the researchers to resolve thermal fluctuations that would otherwise be masked by environmental noise.

Continuous Quantum Measurement and Entropic Temperature

Instead of trapping the rotor in a harmonic potential, the experiment relies on a continuous quantum measurement scheme. A double‑optical‑lever system sends counter‑propagating polarized beams onto the rotor; differential signals on a quadrant photodiode track the yaw motion in real time. By feeding this information back through a radiation‑pressure "push" beam, the team can condition the rotor’s state.

The measurement collapses the rotor’s phase‑space distribution into a squeezed conditional state. Using the von Neumann entropy, the researchers assign an entropic temperature to this state:

``` T = \bigl(k_B \frac{\partial S}{\partial E}\bigr)^{-1} ```

At steady state, the entropy‑derived temperature reaches 140 nK, a quantitative metric that can be compared directly to temperatures of trapped oscillators. The analysis also predicts a fundamental lower bound of ~15 nK for this system, set by the limits of position measurement.

Implications for Fundamental Physics

The ability to localize a macroscopic free mass with such precision has several important consequences:

  • Quantum‑gravity tests – The low‑entropy, high‑coherence state provides a clean platform for searching for tiny deviations from standard quantum mechanics that might arise from gravitational effects.
  • Decoherence benchmarking – By achieving decoherence‑to‑entanglement ratios nearly two orders of magnitude better than prior work, the experiment tightens constraints on proposed modifications to quantum theory.
  • Quantum sensing – The technique could be adapted for ultra‑sensitive force or torque measurements, leveraging the rotor’s large mass while retaining quantum‑limited readout.

Practical Outlook

While the current setup is a laboratory prototype, its components—optical levers, radiation‑pressure actuation, and passive isolation—are compatible with scalable designs. Future work may focus on:

  1. Integrating cryogenic environments to push the entropic temperature closer to the theoretical limit.
  2. Exploring multi‑rotor entanglement to test macroscopic quantum correlations.
  3. Applying the measurement protocol to other free‑mass systems, such as levitated nanoparticles, to broaden the range of test masses.

Conclusion

The experiment marks a significant step toward controlling macroscopic objects at the quantum level. By combining extreme environmental isolation with continuous measurement, the researchers have demonstrated that a 1‑mg rotor can be cooled—by entropy—to 140 nK, establishing a new benchmark for quantum control of free particles. This platform promises to deepen our understanding of the quantum‑classical interface and to enable precision tests of fundamental physics that were previously out of reach.

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