Picometer control of a levitating milligram gravity sensor
Pith reviewed 2026-06-29 11:33 UTC · model grok-4.3
The pith
Linear feedback cooling achieves below 2 picometer amplitudes and below 10 millikelvin temperatures for two modes of a magnetically levitated milligram sensor.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Linear feedback cooling of a magnetically levitated gravity sensor reaches below 2 picometer amplitude and below 10 millikelvin mode temperature for two translational modes simultaneously. The sensor is a levitating permanent magnet in a type I superconducting trap, where its resonance frequencies are measured with a superconducting coil coupled to a DC SQUID. The signal is processed with a lock-in amplifier and a feedback signal drives a piezoelectric actuator to cool the modes at 50.6 and 68.0 Hz, which have Q factors of 3.8 million and 5.5 million. The entire setup sits inside a dry dilution refrigerator with 110-130 dB vibrational attenuation at these frequencies.
What carries the argument
Linear feedback cooling driven by the position signal from a DC SQUID readout to a piezoelectric actuator on a levitated permanent magnet inside a type I superconducting trap.
If this is right
- Simultaneous cooling of two translational modes is possible with the SQUID readout and piezoelectric feedback.
- The high Q factors and vibration isolation support reaching the reported amplitude and temperature limits.
- Future improvements to the setup can enable quantum ground state cooling of the levitated particle.
- The cooled levitated particle remains usable as a gravitational sensor.
Where Pith is reading between the lines
- Ground-state cooling of this system would permit direct tests of gravity acting on macroscopic quantum superpositions.
- The same feedback approach may extend to cooling rotational or other degrees of freedom in the levitated magnet.
- Reduced thermal motion at these levels could increase the force sensitivity of the gravity sensor beyond current thermal-noise limits.
Load-bearing premise
The 110-130 dB vibrational attenuation inside the dilution refrigerator combined with the SQUID readout noise floor is sufficient to allow the reported feedback cooling to reach the stated amplitude and temperature limits without other heating mechanisms dominating.
What would settle it
An independent measurement finding either mode amplitude above 2 picometers or mode temperature above 10 millikelvin when the described feedback is active would falsify the cooling performance.
Figures
read the original abstract
Due to their exceptional isolation from the environment, magnetically levitated particles are explored as extremely sensitive mechanical sensors. For future gravity experiments on quantum superpositions, such systems need to be cooled close to their ground state. To demonstrate the combination of state of the art vibration isolation, milligram levitated high Q mechanical resonators and position detection with low noise, we present linear feedback cooling of a magnetically levitated gravity sensor to below 2 picometer amplitude and below 10 millikelvin mode temperature for two translational modes (the x- and y-mode) simultaneously. The sensor is a levitating permanent magnet in a type I superconducting trap, where its six resonance frequencies are measured with a superconducting coil coupled to a DC SQUID. This signal is measured with a lock-in amplifier and a feedback signal is sent to a piezoelectric actuator, allowing the cooling of resonant modes at 50.6 and 68.0 Hz simultaneously. These two translational modes have Q factors of $3.8 \cdot 10^6$ and $5.5 \cdot 10^6$ respectively. The experiment is mounted inside a dry dilution refrigerator where it is vibrationally attenuated with 110-130 dB at these frequencies. In this work, we discuss future improvements on the setup which may enable quantum ground state cooling on a magnetically levitated particle, that has previously been shown to be a gravitational sensor.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports an experimental demonstration of simultaneous linear feedback cooling of two translational modes (50.6 Hz and 68.0 Hz) of a magnetically levitated milligram permanent magnet in a type-I superconducting trap. Using DC SQUID readout of a superconducting coil and piezoelectric actuation, the authors achieve amplitudes below 2 picometers and mode temperatures below 10 mK for both the x- and y-modes inside a dry dilution refrigerator with 110-130 dB vibrational isolation at the relevant frequencies. The modes exhibit Q factors of 3.8×10^6 and 5.5×10^6. The work discusses prospects for future quantum ground-state cooling toward gravitational sensing applications.
Significance. If the reported performance metrics are substantiated with full calibration and data, the result constitutes a meaningful technical advance in levitated mechanical sensors. It shows the practical integration of milligram-scale high-Q resonators, extreme vibrational isolation, and low-noise SQUID detection to reach picometer amplitudes and millikelvin temperatures on multiple modes simultaneously, directly relevant to proposals for quantum gravity experiments.
major comments (2)
- [Abstract] Abstract: The headline claims of amplitudes below 2 pm and mode temperatures below 10 mK are stated without error bars, raw spectral data, position calibration details, or the explicit procedure used to convert the SQUID signal into these quantities.
- [Experimental setup] Experimental setup paragraph: The claim that 110-130 dB vibrational attenuation plus the SQUID noise floor is sufficient to reach the stated limits without other heating mechanisms dominating is presented without quantitative estimates of residual acceleration noise, heating rates, or direct measurements confirming that these sources do not set the observed floor.
minor comments (1)
- [Abstract] The abstract states that six resonance frequencies are measured but provides Q factors and cooling results for only two; a short statement on the status of the remaining modes would improve completeness without altering the central claim.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the positive assessment of its significance. We address the two major comments point by point below.
read point-by-point responses
-
Referee: [Abstract] Abstract: The headline claims of amplitudes below 2 pm and mode temperatures below 10 mK are stated without error bars, raw spectral data, position calibration details, or the explicit procedure used to convert the SQUID signal into these quantities.
Authors: The abstract is intended as a concise summary of the principal results. The position calibration of the SQUID readout, the explicit conversion procedure from voltage to displacement and temperature, the raw spectral data, and the associated uncertainties (including error bars on the reported amplitudes and temperatures) are all provided in the main text, specifically in the sections describing the readout chain, data acquisition, and results, together with the corresponding figures. To address the referee's concern about clarity, we will revise the abstract to include a brief parenthetical reference to the calibration procedure detailed in the manuscript body. revision: yes
-
Referee: [Experimental setup] Experimental setup paragraph: The claim that 110-130 dB vibrational attenuation plus the SQUID noise floor is sufficient to reach the stated limits without other heating mechanisms dominating is presented without quantitative estimates of residual acceleration noise, heating rates, or direct measurements confirming that these sources do not set the observed floor.
Authors: We agree that the manuscript would benefit from explicit quantitative support for this claim. In the revised version we will add estimates of residual acceleration noise derived from the measured vibrational isolation spectrum, compare these to the observed displacement floor, and include order-of-magnitude heating-rate calculations for the dominant environmental sources to demonstrate that they remain below the level set by the SQUID noise floor at the reported amplitudes. revision: yes
Circularity Check
No significant circularity; experimental report only
full rationale
This paper reports an experimental demonstration of linear feedback cooling on a magnetically levitated milligram-scale permanent magnet inside a dilution refrigerator. The central results (amplitudes <2 pm, mode temperatures <10 mK, Q factors of 3.8e6 and 5.5e6 at 50.6 Hz and 68.0 Hz) are obtained from direct SQUID readout of resonance frequencies, lock-in detection, and piezoelectric feedback, with vibrational isolation quantified at 110-130 dB. No derivation chain, fitted parameter renamed as prediction, self-definitional relation, or load-bearing self-citation is present. The position calibration and temperature inference follow standard relations from measured displacement spectra and are not reduced to quantities defined by the authors' own ansatz or prior self-citations. The result is self-contained against external benchmarks (measured isolation, SQUID noise floor).
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard performance of DC SQUID position detection and piezoelectric actuation in a type I superconducting trap holds under the reported cryogenic conditions.
Reference graph
Works this paper leans on
-
[1]
Quantum ground state and single- phonon control of a mechanical resonator,
A. D. O’Connell, M. Hofheinz, M. Ansmann, R. C. Bial- czak, M. Lenander, E. Lucero, M. Neeley, D. Sank, H. Wang, M. Weides, J. Wenner, J. M. Martinis, and A. N. Cleland, “Quantum ground state and single- phonon control of a mechanical resonator,” Nature464, 697 (2010)
2010
-
[2]
Sideband cooling of micromechanical motion to the quantum ground state,
J. D. Teufel, T. Donner, D. Li, J. W. Harlow, M. S. Allman, K. Cicak, A. J. Sirois, J. D. Whittaker, K. W. Lehnert, and R. W. Simmonds, “Sideband cooling of micromechanical motion to the quantum ground state,” Nature475, 359 (2011)
2011
-
[3]
Laser cooling of a nanomechanical oscillator into its quantum ground state,
J. Chan, T. P. Alegre, A. H. Safavi-Naeini, J. T. Hill, A. Krause, S. Gr¨ oblacher, M. Aspelmeyer, and O. Painter, “Laser cooling of a nanomechanical oscillator into its quantum ground state,” Nature478, 89 (2011)
2011
-
[4]
Observation of quantum motion of a nanomechanical resonator,
A. H. Safavi-Naeini, J. Chan, J. T. Hill, T. P. Alegre, A. Krause, and O. Painter, “Observation of quantum motion of a nanomechanical resonator,” Physical Review Letters108(2012), 10.1103/PhysRevLett.108.033602
-
[5]
Sympathetic cooling of a membrane oscillator in a hybrid mechanical-atomic sys- tem,
A. J¨ ockel, A. Faber, T. Kampschulte, M. Korppi, M. T. Rakher, and P. Treutlein, “Sympathetic cooling of a membrane oscillator in a hybrid mechanical-atomic sys- tem,” Nature Nanotechnology10, 55 (2015)
2015
-
[6]
Laser cooling to the zero-point energy of mo- tion,
F. Diedrich, J. C. Bergquist, W. M. Itano, and D. J. Wineland, “Laser cooling to the zero-point energy of mo- tion,” Physical Review Letters62, 403 (1989)
1989
-
[7]
Resolved- sideband raman cooling of a bound atom to the 3d zero- point energy,
C. Monroe, D. M. Meekhof, B. E. King, S. R. Jefferts, W. M. Itano, D. J. Wineland, and P. Gould, “Resolved- sideband raman cooling of a bound atom to the 3d zero- point energy,” Physical Review Letters75, 4011 (1995)
1995
-
[8]
Quantum dynamics of sin- gle trapped ions,
D. Leibfried and R. Blatt, “Quantum dynamics of sin- gle trapped ions,” Reviews of Modern Physics75, 281 (2003)
2003
-
[9]
Cooling of a levitated nanoparticle to the motional quantum ground state,
U. Deli´ c, M. Reisenbauer, K. Dare, D. Grass, V. Vuleti´ c, N. Kiesel, and M. Aspelmeyer, “Cooling of a levitated nanoparticle to the motional quantum ground state,” Sci- ence367, 892 (2020)
2020
-
[10]
Quantum control of a nanopar- ticle optically levitated in cryogenic free space,
F. Tebbenjohanns, M. L. Mattana, M. Rossi, M. Frim- mer, and L. Novotny, “Quantum control of a nanopar- ticle optically levitated in cryogenic free space,” Nature 595, 378 (2021)
2021
-
[11]
Real-time optimal quantum control of mechanical motion at room temperature,
L. Magrini, P. Rosenzweig, C. Bach, A. Deutschmann- Olek, S. G. Hofer, S. Hong, N. Kiesel, A. Kugi, and M. Aspelmeyer, “Real-time optimal quantum control of mechanical motion at room temperature,” Nature595, 373 (2021)
2021
-
[12]
Simul- taneous ground-state cooling of two mechanical modes of a levitated nanoparticle,
J. Piotrowski, D. Windey, J. Vijayan, C. Gonzalez- Ballestero, A. de los R´ ıos Sommer, N. Meyer, R. Quidant, O. Romero-Isart, R. Reimann, and L. Novotny, “Simul- taneous ground-state cooling of two mechanical modes of a levitated nanoparticle,” Nature Physics19, 1009 (2023)
2023
-
[13]
van Waarde,The lead zeppelin: a force sensor without 6 a handle, Ph.D
B. van Waarde,The lead zeppelin: a force sensor without 6 a handle, Ph.D. thesis, Leiden University (2016)
2016
-
[14]
Chip-based superconducting traps for levitation of micrometer-sized particles in the meissner state,
M. G. Latorre, J. Hofer, M. Rudolph, and W. Wiec- zorek, “Chip-based superconducting traps for levitation of micrometer-sized particles in the meissner state,” Superconductor Science and Technology33(2020), 10.1088/1361-6668/aba6e1
-
[15]
A chip-based superconducting magnetic trap for levitating superconducting microparti- cles,
M. G. Latorre, A. Paradkar, D. Hambraeus, G. Hig- gins, and W. Wieczorek, “A chip-based superconducting magnetic trap for levitating superconducting microparti- cles,” IEEE Transactions on Applied Superconductivity 32(2022), 10.1109/TASC.2022.3147730
-
[16]
J. Hofer, R. Gross, G. Higgins, H. Huebl, O. F. Kieler, R. Kleiner, D. Koelle, P. Schmidt, J. A. Slater, M. Trupke, K. Uhl, T. Weimann, W. Wiec- zorek, and M. Aspelmeyer, “High- q magnetic levi- tation and control of superconducting microspheres at millikelvin temperatures,” Physical Review Letters131 (2023), 10.1103/PhysRevLett.131.043603
-
[17]
M. G. Latorre, G. Higgins, A. Paradkar, T. Bauch, and W. Wieczorek, “Superconducting microsphere magnet- ically levitated in an anharmonic potential with inte- grated magnetic readout,” Physical Review Applied19 (2023), 10.1103/PhysRevApplied.19.054047
-
[18]
Remote sensing of a levitated superconductor with a flux-tunable microwave cavity,
P. Schmidt, R. Claessen, G. Higgins, J. Hofer, J. J. Hansen, P. Asenbaum, M. Zemlicka, K. Uhl, R. Kleiner, R. Gross, H. Huebl, M. Trupke, and M. Aspelmeyer, “Remote sensing of a levitated superconductor with a flux-tunable microwave cavity,” Physical Review Applied 22(2024), 10.1103/PhysRevApplied.22.014078
-
[19]
A. Paradkar, P. Nicaise, K. Dakroury, F. Resare, and W. Wieczorek, “Superconducting flip-chip devices us- ing indium microspheres on au-passivated nb or nbn as under-bump metallization layer,” Applied Physics Let- ters126(2025), 10.1063/5.0235266
-
[20]
Opti- cal interferometric readout of a magnetically levitated superconducting microsphere,
J. J. Hansen, S. Minniberger, D. Ilk, P. Asenbaum, G. Higgins, R. G. Povey, P. Schmidt, J. Hofer, R. Claessen, M. Aspelmeyer, and M. Trupke, “Opti- cal interferometric readout of a magnetically levitated superconducting microsphere,” Physical Review Applied 25, 044080 (2026)
2026
-
[21]
Acceleration sensing with magnetically levitated oscillators above a superconductor,
C. Timberlake, G. Gasbarri, A. Vinante, A. Setter, and H. Ulbricht, “Acceleration sensing with magnetically levitated oscillators above a superconductor,” Applied Physics Letters115(2019), 10.1063/1.5129145
-
[22]
Ultralow me- chanical damping with meissner-levitated ferromagnetic microparticles,
A. Vinante, A. Vinante, P. Falferi, G. Gasbarri, A. Set- ter, C. Timberlake, and H. Ulbricht, “Ultralow me- chanical damping with meissner-levitated ferromagnetic microparticles,” Physical Review Applied13(2020), 10.1103/PhysRevApplied.13.064027
-
[23]
Levitated micromagnets in superconducting traps: A new platform for tabletop fundamental physics experiments,
A. Vinante, C. Timberlake, and H. Ulbricht, “Levitated micromagnets in superconducting traps: A new platform for tabletop fundamental physics experiments,” Entropy 24, 1642 (2022)
2022
-
[24]
Linear cool- ing of a levitated micromagnetic cylinder by vibration,
C. Timberlake, E. Simcox, and H. Ulbricht, “Linear cool- ing of a levitated micromagnetic cylinder by vibration,” Physical Review Research6(2024), 10.1103/PhysRevRe- search.6.033345
-
[25]
Measuring gravity with milligram levi- tated masses,
T. M. Fuchs, D. G. Uitenbroek, J. Plugge, N. V. Hal- teren, P. V. Soest, A. Vinante, H. Ulbricht, and T. H. Oosterkamp, “Measuring gravity with milligram levi- tated masses,” Science Advances2949, 1 (2024)
2024
-
[26]
Using permanent magnets at low temperature,
S. R. Trout and S. Constantinides, “Using permanent magnets at low temperature,” TECHNotes Arnold Mag- netic Technologies0302, 1 (2003)
2003
-
[27]
Sub-khz mechanical resonator passively cooled to 6 mk,
L. van Everdingen, J. Plugge, T. M. Fuchs, G. L. van de Stolpe, D. Benali, T. de Jong, J. Bijl, W. A. Bosch, and T. H. Oosterkamp, “Sub-khz mechanical resonator passively cooled to 6 mk,” Physical Review Research8, L022004 (2026)
2026
-
[28]
Vibration isolation with high thermal conductance for a cryogen-free dilution refrigera- tor,
M. D. Wit, G. Welker, K. Heeck, F. M. Buters, H. J. Eerkens, G. Koning, H. V. der Meer, D. Bouwmeester, and T. H. Oosterkamp, “Vibration isolation with high thermal conductance for a cryogen-free dilution refrigera- tor,” Review of Scientific Instruments90, 015112 (2019)
2019
-
[29]
First search for ultralight dark matter using a magnetically levitated particle,
D. W. Amaral, D. G. Uitenbroek, T. H. Oosterkamp, and C. D. Tunnell, “First search for ultralight dark matter using a magnetically levitated particle,” Physical Review Letters134(2025), 10.1103/PhysRevLett.134.251001
-
[30]
Levitated ferromagnetic magnetometer with energy resolution well below,
F. Ahrens, W. Ji, D. Budker, C. Timberlake, H. Ulbricht, and A. Vinante, “Levitated ferromagnetic magnetometer with energy resolution well below,” Physical Review Let- ters134(2025), 10.1103/PhysRevLett.134.110801
-
[31]
Surpassing the en- ergy resolution limit with ferromagnetic torque sensors,
A. Vinante, C. Timberlake, D. Budker, D. F. Kimball, A. O. Sushkov, and H. Ulbricht, “Surpassing the en- ergy resolution limit with ferromagnetic torque sensors,” Physical Review Letters127(2021), 10.1103/Phys- RevLett.127.070801
-
[32]
Magnetic dipole trapping potential be- tween infinite superconducting plates,
F. J. Headley, “Magnetic dipole trapping potential be- tween infinite superconducting plates,” Physica Scripta 100(2025), 10.1088/1402-4896/adeeda. 7 Supplementary Material: Picometer control of a levitating milligram gravity sensor Dennis G. Uitenbroek, Jurriaan Langendorff, and Tjerk H. Oosterkamp A. Mode identification Currently, for our system, assign...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.