Wave--particle transition and quantum Zeno effect in which-way experiments with a superconducting quantum processor
Pith reviewed 2026-05-10 03:05 UTC · model grok-4.3
The pith
Precise control of which-way measurement strength in a superconducting Mach-Zehnder interferometer demonstrates the wave-to-particle transition of a photon and the quantum Zeno effect under continuous monitoring.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In which-way experiments on a two-dimensional superconducting quantum processor, varying the measurement strength on one path of a Mach-Zehnder interferometer causes a photon to transition from exhibiting wave-like interference to particle-like which-path knowledge. Quantum state tomography on the two path qubits shows that stronger measurements break the entanglement and coherence, leading to information leakage quantified by complementarity relations between entropy and fringe visibility. Continuous application of the which-way measurement during evolution induces the quantum Zeno effect, resulting in nonmonotonic changes in purity and von Neumann entropy as the path is partially blocked.
What carries the argument
The tunable-strength which-way measurement applied to one arm of the Mach-Zehnder interferometer realized with superconducting qubits, which tunes the trade-off between path distinguishability and interference visibility while enabling continuous monitoring for Zeno dynamics.
If this is right
- Increasing which-way measurement strength reduces interference visibility while increasing path distinguishability according to complementarity.
- Which-way measurements destroy entanglement between the two paths and cause measurable information leakage to the environment.
- Continuous which-way monitoring partially obstructs the interferometer path and produces nonmonotonic evolution of purity and von Neumann entropy.
- The derived entropy-visibility relations quantify how measurement strength controls the wave-particle transition in the tomographic data.
Where Pith is reading between the lines
- The platform's controllability over measurement strength could allow systematic tests of other complementarity scenarios, such as delayed-choice variants, without changing hardware.
- The observed link between which-way information and entropy leakage suggests using similar qubit readouts to engineer controlled decoherence in quantum information protocols.
- Nonmonotonic entropy under continuous monitoring points to potential uses in measurement-based state protection schemes where partial obstruction stabilizes certain dynamics.
Load-bearing premise
The superconducting qubits and readout faithfully implement ideal photon paths and which-way detectors without dominant uncontrolled decoherence, calibration errors, or tomography inaccuracies that would mimic the reported transitions and Zeno dynamics.
What would settle it
If the measured fringe visibility fails to decrease monotonically with increasing which-way measurement strength in agreement with the tomographic entropy values, or if continuous monitoring does not produce the predicted nonmonotonic purity and entropy curves, the claimed wave-particle transition and Zeno obstruction would not hold.
Figures
read the original abstract
Wave--particle duality demonstrates the peculiar nature of quantum mechanics. In which-way experiments, depending on the measurement scheme, a particle exhibits either wave-like or particle-like properties, as summarized by Bohr's principle of complementarity. In this work, we implement Mach-Zehnder (MZ) interferometry on a two-dimensional (2D) superconducting quantum processor. With precise control of the which-way measurement strength, we demonstrate the transition of a photon from wave-like to particle-like behavior. Furthermore, by performing quantum state tomography on two qubits located in the two paths, we demonstrate that which-way measurements break the entanglement and coherence between the two paths and cause information leakage from the quantum system to the environment. To capture this behavior quantitatively, we derive complementarity relations between the entropy and the fringe visibility. By applying a continuous which-way measurement during the evolution, we also observe the quantum Zeno effect that partially obstructs the interferometer path, giving rise to nonmonotonic behavior of purity and von Neumann entropy. Our experiments provide a detailed characterization of the full interferometer dynamics, reveal the relation between wave--particle duality and quantum information, and demonstrate the potential of superconducting quantum processors for testing quantum foundations under high precision and controllability.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports an experimental implementation of Mach-Zehnder interferometry on a 2D superconducting quantum processor. By tuning the strength of which-way measurements, it demonstrates the transition from wave-like to particle-like photon behavior. Quantum state tomography on the two path qubits shows entanglement breaking and information leakage to the environment. Complementarity relations are derived between entropy and fringe visibility. Continuous which-way measurements are used to observe the quantum Zeno effect, manifested as nonmonotonic behavior in purity and von Neumann entropy.
Significance. If the central claims hold after addressing controls for device noise, the work offers a controlled superconducting-platform demonstration of wave-particle duality, Bohr complementarity, and the Zeno effect, with explicit connections to quantum-information quantities (entropy, entanglement). The ability to tune measurement strength and perform tomography provides a quantitative link between which-way information gain and loss of coherence, which is valuable for foundations experiments. The platform's controllability could enable extensions to more complex interferometric tests.
major comments (3)
- [Zeno-effect results] The reported nonmonotonic purity and von Neumann entropy under continuous which-way measurement (abstract and results on Zeno dynamics) lack error bars, statistical significance tests, or explicit comparison to zero-measurement-strength controls. Without these, it is unclear whether the nonmonotonicity exceeds fluctuations or uncontrolled decoherence.
- [Experimental implementation and tomography] No device-specific noise model (T1/T2 times, gate infidelities, readout crosstalk) or numerical simulation is presented showing that the observed visibility transition and entropy changes cannot be reproduced by hardware imperfections alone. This is load-bearing for the claim that the behaviors arise from intended which-way information gain and Zeno obstruction rather than artifacts.
- [Complementarity relations] The complementarity relations between entropy and fringe visibility are stated as derived post-experiment, but the manuscript does not show whether they are used to predict or fit the data or remain purely descriptive; this affects the strength of the quantitative link claimed between duality and quantum information.
minor comments (2)
- [Methods] The abstract and methods would benefit from explicit reporting of the number of experimental repetitions, tomography reconstruction method, and how measurement strength is calibrated and verified.
- [Figures] Figure captions should include error estimation procedures and any averaging over runs to improve reproducibility.
Simulated Author's Rebuttal
We thank the referee for their thorough review and constructive comments on our manuscript. We address each major point below and have revised the manuscript to incorporate the requested clarifications and additions.
read point-by-point responses
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Referee: [Zeno-effect results] The reported nonmonotonic purity and von Neumann entropy under continuous which-way measurement (abstract and results on Zeno dynamics) lack error bars, statistical significance tests, or explicit comparison to zero-measurement-strength controls. Without these, it is unclear whether the nonmonotonicity exceeds fluctuations or uncontrolled decoherence.
Authors: We appreciate the referee highlighting the need for statistical rigor in the Zeno-effect section. The nonmonotonic behavior was observed experimentally, but error bars and formal tests were omitted from the initial submission. In the revised manuscript we will add error bars from repeated runs, include statistical significance tests (e.g., t-tests against a null hypothesis of monotonic decay), and present zero-measurement-strength control data to confirm that the observed nonmonotonicity in purity and entropy exceeds fluctuations and uncontrolled decoherence. revision: yes
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Referee: [Experimental implementation and tomography] No device-specific noise model (T1/T2 times, gate infidelities, readout crosstalk) or numerical simulation is presented showing that the observed visibility transition and entropy changes cannot be reproduced by hardware imperfections alone. This is load-bearing for the claim that the behaviors arise from intended which-way information gain and Zeno obstruction rather than artifacts.
Authors: We agree that a quantitative noise model is essential to substantiate the claims. The original manuscript described the device but did not include a comprehensive noise characterization or simulations. The revision will add measured T1/T2 times, gate infidelities, and readout crosstalk values for the qubits involved, together with numerical simulations of the interferometer dynamics that incorporate these parameters. These simulations will demonstrate that the observed visibility transition, entanglement breaking, and Zeno dynamics cannot be reproduced by hardware noise alone. revision: yes
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Referee: [Complementarity relations] The complementarity relations between entropy and fringe visibility are stated as derived post-experiment, but the manuscript does not show whether they are used to predict or fit the data or remain purely descriptive; this affects the strength of the quantitative link claimed between duality and quantum information.
Authors: The complementarity relations were derived from quantum-information principles before the experiments and subsequently applied to the data. To make this explicit, the revised manuscript will show the relations used to fit the measured visibility-versus-entropy data points and will include plots comparing the theoretical curves with experimental results, thereby demonstrating their predictive and quantitative role rather than a purely descriptive one. revision: yes
Circularity Check
No circularity: experimental data and tomography drive claims; derived relations are post-hoc and independent
full rationale
The paper reports direct implementation of MZ interferometry on a 2D superconducting processor, with tunable which-way measurement strength, quantum state tomography on path qubits, and continuous monitoring to observe Zeno-induced nonmonotonic purity/entropy. Complementarity relations between entropy and fringe visibility are derived to quantify observed behavior but are not inputs to data generation, fitting procedures, or predictions that reduce to the same measurements by construction. No self-definitional loops, fitted inputs renamed as predictions, load-bearing self-citations, uniqueness theorems imported from prior author work, or ansatz smuggling appear in the derivation chain. The central results rest on hardware-controlled experiments and tomography rather than tautological reductions, making the logic self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Bohr complementarity and standard unitary evolution plus projective measurements apply to the superconducting circuit implementation.
Forward citations
Cited by 1 Pith paper
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As shown in Fig
The average measurement-induced dephasing rate of Q2 is then given by Γm =− 1 tm ln |ρm 01| |ρref 01 | ,(S5) wheret m is the measurement time. As shown in Fig. S5b,Γm/2πincreases linearly withA 2. In our readout model, the cavity photon numbern(t)follows a driven-dissipative evolution: during the readout pulse (t= 0–100 ns) the intra-cavity population app...
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This choice ensures that the system does not overheat while leaving sufficient range to further bias each qubit to the working and idle points usingZpulses
Measure the DC-bias-dependent spectrum of each qubit and choose a modest DC bias that places each qubit at a suitable frequency. This choice ensures that the system does not overheat while leaving sufficient range to further bias each qubit to the working and idle points usingZpulses
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Then perform Ramsey measurements to finely tune theZ-pulse amplitudeAidle so that each qubit sits at its idle point
Precisely measure theZ-pulse-dependent spectroscopy of each qubit at the chosen DC-bias point with using Zpulses to bias each qubit to its idle frequency and correctZ-pulse distortion. Then perform Ramsey measurements to finely tune theZ-pulse amplitudeAidle so that each qubit sits at its idle point. For qubits that are not used in the experiment, we bias...
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ApplyZ-pulsebiasestoallqubitssimultaneouslyand, foreachqubitinturn, performRamseymeasurements to finely adjust theZ-pulse amplitudeA′ idle to removeZ-pulse crosstalk
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ApplyZpulses to all qubits simultaneously to bias them to the working point for evolution. Compare the experimental evolution with numerical simulation and optimize theZ-pulse amplitudesAworking using the Nelder–Mead algorithm to minimize the effect ofZ-pulse crosstalk and achieve precise frequency alignment for all qubits
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During the experiments, magnetic-field changes or DC drift can shift qubit frequencies
After completing calibration steps 1–4, we begin the experiments. During the experiments, magnetic-field changes or DC drift can shift qubit frequencies. We perform a qubit-frequency calibration approximately every2 hours. For each qubit we apply aZpulse to bias it to its idle point and perform a Ramsey experiment. If a frequency shift is observed, we cor...
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We can obtain the expression for the visibility: V= 2|c ′|.(S19) For a general2×2density matrix of this form, letδp ′ ≡p ′ 1 −p ′
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[79]
The eigenvalues ofρs read λ± = 1 2 1±R ,(S20) 8 whereR≡ p δp′2 +V 2 (0≤R≤1). The purityP s in the single-excitation subspace is given as Ps = Tr(ρ2 s) =λ 2 + +λ 2 − = 1 +R 2 2 .(S21) Thus, we can obtain the complementarity relation 2(1−P s) +V 2 = 1−R 2 +V 2 = 1−(δp ′2 +V 2) +V 2 (S22) = 1−δp ′2 ≤1,(S23) where equality holds if and only ifδp′ = 0(i.e. the...
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[80]
Yan, Z.-Y
Z. Yan, Z.-Y. Ge, R. Li, Y.-R. Zhang, F. Nori, and Y. Nakamura,Characterizing many-body dynamics with projected ensembles on a superconducting quantum processor, Science Advances12, eaeb8213 (2026)
2026
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