Scalable Generation of Massive Schr\"odinger Cat States via Quantum Tunneling
Pith reviewed 2026-05-23 04:05 UTC · model grok-4.3
The pith
Bound clusters of ultracold atoms tunnel coherently to form spatial superpositions of 608-amu objects.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Coherent tunneling of bound atomic clusters in optical lattices produces composite objects of 608 amu that occupy spatially entangled superpositions; these states are certified by a constructed interferometer and applied to quantum-enhanced measurements.
What carries the argument
Coherent tunneling of bound clusters whose lattice parameters are tuned to offset mass-dependent suppression of the tunneling rate.
If this is right
- High-mass spatial superpositions become scalable in atomic lattice systems.
- Tunneling rates for heavier clusters can be maintained by lattice-parameter adjustment.
- Entanglement in these states can be verified directly with matter-wave interferometry.
- The generated cat states support quantum-enhanced measurements beyond the standard quantum limit.
Where Pith is reading between the lines
- Further increases in cluster size could reach regimes where gravitational effects on superposition become testable.
- The lattice-tunneling approach may generalize to other trapping geometries or atomic species.
- Similar certification methods could quantify decoherence rates for progressively larger masses.
Load-bearing premise
The coherence observed after cluster tunneling arises from genuine spatial quantum entanglement rather than classical correlations.
What would settle it
If the interferometer constructed from the tunneled clusters shows no interference fringes or phase stability, the claim of certified spatial entanglement would be falsified.
Figures
read the original abstract
Massive objects in spatial superposition may provide insights into the interplay between quantum mechanics and gravity. Cold atomic interferometers offer a promising platform due to extended matter-wave coherence times and precise controllability. However, high-mass spatial superpositions beyond single atoms have yet to be generated in such setups. Here, we report the scalable realization of high-mass spatial entanglement via quantum tunneling of ultracold atoms in optical lattices. We observe coherent tunneling of bound clusters, forming a composite object with a mass of 608~amu. Full control of the model parameters allows us to mitigate the usual suppression of tunneling with increasing mass. Furthermore, we construct an interferometer to certify the entanglement and use spatially distributed Schr\"{o}dinger cat states to perform quantum-enhanced measurements. These results establish an approach to generating and detecting massive superposition states relevant to studies of quantum gravity.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports the experimental realization of scalable high-mass spatial entanglement in ultracold atoms via quantum tunneling in optical lattices. Bound clusters of 608 amu are formed through coherent tunneling, with lattice parameters controlled to counteract the usual mass-dependent suppression; an interferometer is constructed to certify the resulting spatial superposition (Schrödinger-cat-type entanglement), which is then used for quantum-enhanced measurements.
Significance. If the entanglement certification is rigorously established, the work would constitute a notable technical advance in atomic interferometry by extending controllable spatial superpositions to composite objects two orders of magnitude heavier than single atoms, while the demonstrated parameter tunability offers a concrete route to mitigating tunneling suppression. The approach is directly relevant to proposals for testing quantum mechanics at macroscopic scales.
major comments (2)
- [Abstract / interferometer section] Abstract and the section describing the interferometer: the central claim that the constructed interferometer certifies genuine spatial entanglement (rather than classical correlations or mixtures) for the 608 amu clusters rests on the assumption that observed coherence and lattice control suffice to exclude classical explanations, yet no explicit bounds, statistical tests, or off-diagonal long-range order analysis are supplied to demonstrate violation of classical limits.
- [Tunneling observations] Section reporting the tunneling observations: the claim of coherent tunneling of bound clusters requires quantitative data (e.g., visibility, contrast, or time-of-flight distributions) together with error analysis and comparison to single-particle or classical controls; the absence of such verification details leaves the mass-scaling and coherence assertions unsupported.
minor comments (2)
- [Methods] Clarify in the methods how the composite mass of 608 amu is determined from the cluster size and atom number, including any assumptions about binding.
- [Figures] Ensure all figure captions explicitly state the number of experimental realizations and the fitting procedure used for coherence times.
Simulated Author's Rebuttal
We thank the referee for their detailed review and constructive suggestions. We address the two major comments point by point below, agreeing that additional quantitative analysis is needed to strengthen the claims of coherent tunneling and entanglement certification.
read point-by-point responses
-
Referee: [Abstract / interferometer section] Abstract and the section describing the interferometer: the central claim that the constructed interferometer certifies genuine spatial entanglement (rather than classical correlations or mixtures) for the 608 amu clusters rests on the assumption that observed coherence and lattice control suffice to exclude classical explanations, yet no explicit bounds, statistical tests, or off-diagonal long-range order analysis are supplied to demonstrate violation of classical limits.
Authors: We agree that the manuscript would benefit from explicit quantitative bounds and statistical tests to rigorously exclude classical explanations. In the revised version we will add a new subsection in the interferometer section that includes (i) measured visibility and contrast values with error bars, (ii) statistical comparison of the observed interference patterns against classical mixture models, and (iii) an analysis of off-diagonal long-range order extracted from the time-of-flight distributions. These additions will directly address the concern and make the certification of spatial entanglement explicit. revision: yes
-
Referee: [Tunneling observations] Section reporting the tunneling observations: the claim of coherent tunneling of bound clusters requires quantitative data (e.g., visibility, contrast, or time-of-flight distributions) together with error analysis and comparison to single-particle or classical controls; the absence of such verification details leaves the mass-scaling and coherence assertions unsupported.
Authors: The current manuscript presents tunneling observations but does not include the requested quantitative metrics with error analysis or explicit control comparisons. We will revise the tunneling section to incorporate visibility and contrast measurements from the time-of-flight images, together with error bars, and will add direct comparisons to single-particle tunneling data and classical simulations. This will provide the necessary support for the coherent tunneling and mass-scaling claims. revision: yes
Circularity Check
No significant circularity; experimental observation self-contained
full rationale
The manuscript reports an experimental realization of coherent tunneling of bound atomic clusters and construction of an interferometer for entanglement certification. No derivation chain, first-principles prediction, or fitted parameter is presented that reduces by construction to its own inputs. No self-citations, ansatzes, or uniqueness theorems are invoked in the provided text to support load-bearing claims. The result is framed as direct observation under controlled lattice parameters, making it independent of the circularity patterns enumerated.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
This state represents a maximally entangled Schr¨ odinger cat state, commonly referred to as a NOON state [24, 25]. Due to the spatial separa- tion of the massive atoms in |n, 0⟩ and |0, n⟩, these states 6 are highly sensitive to spatial variations in energy shifts, making them ideal for precision measurements. The in- herent correlations in the entangled...
-
[2]
The entangled state is vi- sualized on the Bloch sphere, where a rotation of 2 π/n restores the state, highlighting the enhanced phase sen- sitivity of n-atom entanglement. Fig. 4b shows the detection results obtained using quantum superposition states. The single-particle oscil- lation frequency is measured to be ∆ /h = 1.49(2) kHz, corresponding to the ...
-
[3]
Quantum theory of tunneling (World Scien- tific, 2013)
Razavy, M. Quantum theory of tunneling (World Scien- tific, 2013)
work page 2013
-
[4]
MacColl, L. A. Note on the transmission and reflection of wave packets by potential barriers. Phys. Rev. 40, 621–626 (1932)
work page 1932
-
[5]
Andrews, M. R. et al. Observation of interference be- tween two Bose condensates. Science 275, 637–641 (1997)
work page 1997
-
[6]
Greiner, M., Mandel, O., Esslinger, T., Hansch, T. W. & Bloch, I. Quantum phase transition from a superfluid to a Mott insulator in a gas of ultracold atoms. Nature 415, 39–44 (2002)
work page 2002
-
[7]
Folling, S. et al. Direct observation of second-order atom tunnelling. Nature 448, 1029–1032 (2007)
work page 2007
-
[8]
Meinert, F. et al. Observation of many-body dynamics in long-range tunneling after a quantum quench. Science 344, 1259–1262 (2014)
work page 2014
-
[9]
Kaufman, A. M. et al. Two-particle quantum interference in tunnel-coupled optical tweezers. Science 345, 306–309 (2014)
work page 2014
-
[10]
Preiss, P. M. et al. Strongly correlated quantum walks in optical lattices. Science 347, 1229–1233 (2015)
work page 2015
-
[11]
Murmann, S. et al. Two fermions in a double well: Ex- 7 ploring a fundamental building block of the Hubbard model. Phys. Rev. Lett. 114, 080402 (2015)
work page 2015
-
[12]
Yang, B. et al. Observation of gauge invariance in a 71-site Bose–Hubbard quantum simulator. Nature 587, 392–396 (2020)
work page 2020
-
[13]
Impertro, A. et al. Local readout and control of current and kinetic energy operators in optical lattices. Phys. Rev. Lett. 133, 063401 (2024)
work page 2024
-
[14]
Cataliotti, F. S. et al. Josephson junction arrays with Bose-Einstein condensates. Science 293, 843–846 (2001)
work page 2001
-
[15]
Albiez, M. et al. Direct observation of tunneling and non- linear self-trapping in a single Bosonic Josephson junc- tion. Phys. Rev. Lett. 95, 010402 (2005)
work page 2005
-
[16]
Kwon, W. J. et al. Strongly correlated superfluid order parameters from dc Josephson supercurrents. Science 369, 84–88 (2020)
work page 2020
-
[17]
Luick, N. et al. An ideal Josephson junction in an ul- tracold two-dimensional Fermi gas. Science 369, 89–91 (2020)
work page 2020
-
[18]
Ramos, R., Spierings, D., Racicot, I. & Steinberg, A. M. Measurement of the time spent by a tunnelling atom within the barrier region. Nature 583, 529–532 (2020)
work page 2020
-
[19]
Winkler, K. et al. Repulsively bound atom pairs in an optical lattice. Nature 441, 853–856 (2006)
work page 2006
-
[20]
Bloch, I., Dalibard, J. & Zwerger, W. Many-body physics with ultracold gases. Rev. Mod. Phys. 80, 885–964 (2008)
work page 2008
-
[21]
Lewenstein, M., Sanpera, A. et al. Ultracold Atoms in Optical Lattices: Simulating quantum many-body systems (OUP Oxford, 2012)
work page 2012
-
[22]
Jaksch, D., Bruder, C., Cirac, J. I., Gardiner, C. W. & Zoller, P. Cold bosonic atoms in optical lattices. Phys. Rev. Lett. 81, 3108 (1998)
work page 1998
-
[23]
Sebby-Strabley, J., Anderlini, M., Jessen, P. S. & Porto, J. V. Lattice of double wells for manipulating pairs of cold atoms. Phys. Rev. A 73, 033605 (2006)
work page 2006
-
[24]
Yang, B. et al. Cooling and entangling ultracold atoms in optical lattices. Science 369, 550–553 (2020)
work page 2020
-
[25]
Dutta, O. et al. Non-standard Hubbard models in optical lattices: a review. Rep. Prog. Phys. 78, 066001 (2015)
work page 2015
-
[26]
Sanders, B. C. Quantum dynamics of the nonlinear rota- tor and the effects of continual spin measurement. Phys. Rev. A 40, 2417–2427 (1989)
work page 1989
-
[27]
Lee, H., Kok, P. & Dowling, J. P. A quantum Rosetta stone for interferometry. J. Mod. Opt. 49, 2325–2338 (2002)
work page 2002
-
[28]
Braunstein, S. L. & Caves, C. M. Statistical distance and the geometry of quantum states. Phys. Rev. Lett. 72, 3439–3443 (1994)
work page 1994
-
[29]
Pezz´ e, L., Smerzi, A., Oberthaler, M. K., Schmied, R. & Treutlein, P. Quantum metrology with nonclassical states of atomic ensembles. Rev. Mod. Phys. 90, 035005 (2018)
work page 2018
-
[30]
Walther, P. et al. De Broglie wavelength of a non-local four-photon state. Nature 429, 158–161 (2004)
work page 2004
-
[31]
Afek, I., Ambar, O. & Silberberg, Y. High-NOON states by mixing quantum and classical light.Science 328, 879– 881 (2010)
work page 2010
-
[32]
Yang, B. et al. Spin-dependent optical superlattice. Phys. Rev. A 96, 011602 (2017)
work page 2017
-
[33]
Arndt, M. et al. Wave–particle duality of C60 molecules. Nature 401, 680–682 (1999)
work page 1999
-
[34]
Kovachy, T. et al. Quantum superposition at the half- metre scale. Nature 528, 530–533 (2015)
work page 2015
-
[35]
Fein, Y. Y. et al. Quantum superposition of molecules beyond 25 kDa. Nat. Phys. 15, 1242–1245 (2019)
work page 2019
-
[36]
Bild, M. et al. Schr¨ odinger cat states of a 16-microgram mechanical oscillator. Science 380, 274–278 (2023)
work page 2023
-
[37]
Monroe, C., Meekhof, D. M., King, B. E. & Wineland, D. J. A “Schr¨ odinger cat” superposition state of an atom. Science 272, 1131–1136 (1996)
work page 1996
-
[38]
Wang, C. et al. A Schr¨ odinger cat living in two boxes. Science 352, 1087–1091 (2016)
work page 2016
-
[39]
Omran, A. et al. Generation and manipulation of Schr¨ odinger cat states in Rydberg atom arrays. Science 365, 570–574 (2019)
work page 2019
-
[40]
Song, C. et al. Generation of multicomponent atomic Schr¨ odinger cat states of up to 20 qubits. Science 365, 574–577 (2019)
work page 2019
-
[41]
Bassi, A., Lochan, K., Satin, S., Singh, T. P. & Ulbricht, H. Models of wave-function collapse, underlying theories, and experimental tests. Rev. Mod. Phys. 85, 471–527 (2013)
work page 2013
-
[42]
Daley, A. J. et al. Practical quantum advantage in quan- tum simulation. Nature 607, 667–676 (2022)
work page 2022
-
[43]
C., Aidelsburger, M., Grusdt, F., Hauke, P
Halimeh, J. C., Aidelsburger, M., Grusdt, F., Hauke, P. & Yang, B. Cold-atom quantum simulators of gauge theories. Nat. Phys. (2025)
work page 2025
-
[44]
Dai, H.-N. et al. Four-body ring-exchange interactions and anyonic statistics within a minimal toric-code Hamil- tonian. Nat. Phys. 13, 1195–1200 (2017)
work page 2017
-
[45]
Mitchell, M. W., Lundeen, J. S. & Steinberg, A. M. Super-resolving phase measurements with a multiphoton entangled state. Nature 429, 161–164 (2004)
work page 2004
-
[46]
Nagata, T., Okamoto, R., O’Brien, J. L., Sasaki, K. & Takeuchi, S. Beating the standard quantum limit with four-entangled photons. Science 316, 726–729 (2007)
work page 2007
-
[47]
Zhang, J. et al. NOON states of nine quantized vibrations in two radial modes of a trapped ion. Phys. Rev. Lett. 121, 160502 (2018). 8 METHODS AND SUPPLEMENT AR Y MA TERIALS GENERA TION OF UL TRACOLD A TOMIC CLUSTER We generate ultracold atomic clusters by cooling 87Rb atoms to the quantum degenerate regime, followed by binding the atoms in optical lattic...
work page 2018
-
[48]
(a) Spatially resolved Ramsey measurements
A second π/2 pulse via tunneling completes the Ramsey sequence for phase measurement. (a) Spatially resolved Ramsey measurements. The distribution of ∆ in the x-y plane is shown at different times, revealing spatial energy shifts that reflect potential inhomogeneity. Averaging over a certain region leads to effective dephasing of the entangled state. (b) ...
-
[49]
As the coupling strength J0/U increases, the system moves away from the perturbation regime
(b) Fidelity for NOON state at various coupling strengths. As the coupling strength J0/U increases, the system moves away from the perturbation regime. Despite this, the fidelity for realizing the NOON state remains considerably high even at J0/U = 5. (c) Tunneling dynamics for larger clusters (n = 8, 9, 10). For these clusters, we optimize the J0/U param...
-
[50]
Taking into ac- count the imperfections of the Mott insulator and the fluctuations of the experimental parameters, the fidelity of the entangled state predicted by theoretical simula- tions aligns with the Ramsey measurement, producing a limited oscillation amplitude of 0.52(3), as shown in Fig. 4b. To characterize the quantum entangled state for quan- tu...
-
[51]
The derived phase sensi- tivities ∆θ are, respectively, 0.64(2), 0.42(1), 0.36(1), and 0.40(2)
Using single entangled states, the Fisher information values achieved are 2.5(1), 5.6(2), 7.6(3), and 6.2(7) for clusters with n = 2, 3, 4, and 5, respectively. The derived phase sensi- tivities ∆θ are, respectively, 0.64(2), 0.42(1), 0.36(1), and 0.40(2). For the four-body NOON state, this results in a 1.4(1) dB enhancement in phase sensitivity beyond th...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.