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arxiv: 2606.13375 · v1 · pith:WTOIYQO5new · submitted 2026-06-11 · 🪐 quant-ph

Driven-dissipative entanglement of distant giant atoms

Aziza Almanakly , Ariadna Soro , Alejandro Vivas-Via\~na , Beatriz Yankelevich , Caspar Groiseau , David Pahl , Junyoung An , Gabriel Cutter
show 10 more authors
Michael E. Gingras Bethany M. Niedzielski Hannah Stickler Ren\'ee DeP\'encier Pi\~nero Mollie E. Schwartz Kyle Serniak Max Hays Jeffrey A. Grover Anton Frisk Kockum William D. Oliver
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Pith reviewed 2026-06-27 06:17 UTC · model grok-4.3

classification 🪐 quant-ph
keywords giant atomsdriven-dissipative entanglementremote entanglementsuperconducting qubitswaveguide QEDcorrelated dissipationBell statequantum networks
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The pith

Continuous driving of two giant atoms coupled to a waveguide generates remote entanglement, preserved at 0.89 fidelity by frequency tuning that suppresses individual dissipation.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that a pair of distant giant artificial atoms can be entangled remotely by continuously driving them through a shared waveguide while their coupling points create interference that enables correlated dissipation. This process stabilizes the atoms in a protected entangled dark state without needing timed pulses. After the entanglement forms, in-situ tuning of the qubit frequencies turns off the unwanted single-atom decay channels while keeping the joint dissipation active. A reader would care because the method separates entanglement generation from preservation, offering a route to distribute entanglement across networks where dissipation is usually a problem.

Core claim

Engineering two giant atoms with sequential coupling to a waveguide allows tunable individual and correlated dissipation via interference; continuous waveguide driving exploits the correlated channel to generate remote entanglement, after which frequency tuning suppresses individual dissipation to preserve a Bell state with fidelity 0.89 plus or minus 0.02.

What carries the argument

Giant artificial atoms with multiple coupling points to a waveguide, using interference to control the balance between individual and correlated dissipation rates.

If this is right

  • Continuous-wave driving can replace calibrated pulses for generating remote entanglement in waveguide systems.
  • Entanglement generation and preservation can be performed as separate steps by adjusting dissipation channels independently.
  • The protocol applies to atoms separated along the waveguide, enabling distribution without requiring close physical proximity.
  • Driven-dissipative methods become viable for quantum interconnects once individual loss can be selectively suppressed.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same interference-based tuning might extend to chains of more than two atoms to create larger protected entangled states.
  • Combining this dissipation engineering with existing coherent control techniques could improve overall network fidelity.
  • Distance dependence along the waveguide could be tested to determine how far the entanglement remains stable.
  • The approach suggests dissipation can be treated as a controllable resource rather than solely a source of error in quantum networks.

Load-bearing premise

Tuning the qubit frequencies can suppress single-atom dissipation channels while leaving the correlated dissipation and the dark entangled state intact without adding new decoherence.

What would settle it

An experiment that tunes the frequencies as described yet measures Bell-state fidelity well below 0.89 because the correlated dissipation is also lost or new decoherence appears would falsify the claim.

Figures

Figures reproduced from arXiv: 2606.13375 by Alejandro Vivas-Via\~na, Anton Frisk Kockum, Ariadna Soro, Aziza Almanakly, Beatriz Yankelevich, Bethany M. Niedzielski, Caspar Groiseau, David Pahl, Gabriel Cutter, Hannah Stickler, Jeffrey A. Grover, JunYoung An, Kyle Serniak, Max Hays, Michael E. Gingras, Mollie E. Schwartz, Ren\'ee DeP\'encier Pi\~nero, William D. Oliver.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4 [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5 [PITH_FULL_IMAGE:figures/full_fig_p006_5.png] view at source ↗
read the original abstract

Quantum interconnects distribute entanglement via controlled light-matter interactions for quantum computing and sensing applications. Many entanglement generation schemes use coherent, reversible interactions that require precisely calibrated pulses to execute. In contrast, driven-dissipative protocols use a continuous-wave drive in the presence of correlated dissipation to stabilize entanglement in protected (dark) states. However, the same dissipation that generates the entanglement also limits its utility once the stabilization protocol ends. Here, we engineer a superconducting system of two giant artificial atoms coupled sequentially to a waveguide, with tunable individual and correlated dissipation enabled by interference between coupling points. Continuously driving the atoms through the waveguide exploits correlated dissipation to generate remote entanglement. We then tune the qubit frequencies in situ to suppress individual dissipation and thereby preserve the entanglement, achieving a Bell-state fidelity F = 0.89 +/- 0.02. This demonstration indicates that the driven dissipation of giant atoms is a viable approach for distributing entanglement across quantum networks.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript reports an experimental demonstration in a superconducting circuit of two distant giant atoms coupled sequentially to a waveguide. Tunable individual and correlated dissipation is engineered via interference at multiple coupling points. A continuous-wave drive through the waveguide generates remote entanglement in a dark state; subsequent in-situ tuning of the qubit frequencies is used to suppress individual dissipation channels while preserving the correlated dissipation, yielding a Bell-state fidelity of 0.89 ± 0.02.

Significance. If the central experimental claim holds, the work establishes driven-dissipative entanglement stabilization with giant atoms as a viable route for quantum interconnects, offering continuous operation and post-generation preservation without pulsed coherent control. The interference-based separation of dissipation rates is a concrete technical advance that could scale to larger networks.

major comments (2)
  1. [Experimental methods and results on frequency tuning] The protocol for in-situ frequency tuning (described in the experimental methods and results sections) assumes that the relative phases and coupling strengths responsible for correlated dissipation remain unchanged when individual dissipation is suppressed. No explicit data or calculation is provided showing that the correlated decay rate is frequency-independent over the tuned range; any residual frequency dependence would directly compromise the dark-state protection and the reported fidelity.
  2. [Results section on entanglement fidelity] The Bell-state fidelity measurement (reported as F = 0.89 ± 0.02) relies on the preservation of the entangled state after tuning. The manuscript does not include a quantitative comparison of the entanglement generation rate versus the residual individual dissipation rate before and after tuning, which is required to confirm that the observed fidelity is attributable to the intended mechanism rather than other decoherence channels.
minor comments (2)
  1. [Abstract] The abstract states the fidelity with an error bar but does not indicate the number of experimental repetitions or the method used to extract the uncertainty; this detail should be added for reproducibility.
  2. [Figures and captions] Figure captions and axis labels in the main text use inconsistent notation for the individual versus collective decay rates; standardizing the symbols (e.g., Γ_ind vs. Γ_corr) would improve clarity.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the positive assessment of the significance of our work and for the detailed comments. We address each major comment below.

read point-by-point responses

  1. Referee: [Experimental methods and results on frequency tuning] The protocol for in-situ frequency tuning (described in the experimental methods and results sections) assumes that the relative phases and coupling strengths responsible for correlated dissipation remain unchanged when individual dissipation is suppressed. No explicit data or calculation is provided showing that the correlated decay rate is frequency-independent over the tuned range; any residual frequency dependence would directly compromise the dark-state protection and the reported fidelity.

    Authors: The coupling-point positions are lithographically fixed, so the relative phases are set by the waveguide propagation distance at the operating frequency. The in-situ tuning range is narrow relative to the center frequency, and the waveguide dispersion over this interval produces only a small change in the effective phase. We will add an explicit calculation (or supporting measurement) of the correlated decay rate versus frequency across the tuned interval to the revised manuscript. revision: yes

  2. Referee: [Results section on entanglement fidelity] The Bell-state fidelity measurement (reported as F = 0.89 ± 0.02) relies on the preservation of the entangled state after tuning. The manuscript does not include a quantitative comparison of the entanglement generation rate versus the residual individual dissipation rate before and after tuning, which is required to confirm that the observed fidelity is attributable to the intended mechanism rather than other decoherence channels.

    Authors: We agree that a side-by-side rate comparison would strengthen the attribution to the driven-dissipative mechanism. We will include a quantitative comparison of the relevant rates (entanglement generation versus residual individual dissipation) extracted from the measured parameters before and after tuning in the revised results section. revision: yes

Circularity Check

0 steps flagged

No circularity: experimental demonstration with no derivation chain

full rationale

This paper is an experimental report on a superconducting circuit realizing driven-dissipative remote entanglement via giant atoms coupled to a waveguide. The central result is a measured Bell-state fidelity of 0.89 ± 0.02 obtained by tuning frequencies to suppress individual dissipation while preserving correlated dissipation. No mathematical derivation, ansatz, or prediction is claimed that reduces by construction to fitted inputs or self-citations. The protocol relies on physical interference conditions that are directly engineered and measured in the device; success is benchmarked against external experimental outcomes rather than internal consistency alone. The work is therefore self-contained with no load-bearing circular steps.

Axiom & Free-Parameter Ledger

1 free parameters · 0 axioms · 0 invented entities

The paper is an experimental work; the central claim rests on the physical realization of the described system and the measurement of fidelity. No mathematical derivation with free parameters is presented in the abstract.

free parameters (1)
  • qubit frequencies
    Tuned in situ to suppress dissipation, but specific values not given in abstract.

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