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Measurement-Induced Information Freezing: A Numerical Exploration of Quantum Zeno Dynamics and Scrambling Suppression

Taha Kalkat

Published May 22, 2026• 0 citations
Publisher

Abstract

We explore the Quantum Zeno Effect (QZE) as a dynamical mechanism for suppressing quantum information transport in open systems. Moving beyond the phenomenological decay of survival probabilities in zero-dimensional systems, we utilize a continuous measurement effective model governed by the Stochastic Schrödinger Equation (SSE). Our numerical investigations suggest that measurement-induced freezing can be mapped to the behavior of a Liouvillian Exceptional Point (EP). We demonstrate how this non-unitary backaction manifests in our simulations: from suppressing single-particle spatial transmission (showing a trend consistent with T ∝ γ^(-α)), to the qualitative reduction of information scrambling as indicated by the Tripartite Mutual Information (I₃ → 0). Finally, scaling this effective model to finite XXZ spin chains (N ≤ 10), our data indicates a transition-like behavior from volume-law to area-law entanglement scaling. While bounded by finite-size limitations, our results provide numerical evidence supporting the interpretation of Zeno dynamics as a suppressor of information geometry.

DOI
10.5281/zenodo.20348568

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•May 9, 2026•0 citations
We explore the Quantum Zeno Effect (QZE) as a dynamical mechanism for suppressing quantum information transport in open systems. Moving beyond the phenomenological decay of survival probabilities in zero-dimensional systems, we utilize a continuous measurement effective model governed by the Stochastic Schrödinger Equation (SSE). Our numerical investigations suggest that measurement-induced freezing can be mapped to the behavior of a Liouvillian Exceptional Point (EP). We demonstrate how this non-unitary backaction manifests in our simulations: from suppressing single-particle spatial transmission (showing a trend consistent with T ∝ γ^(-α)), to the qualitative reduction of information scrambling as indicated by the Tripartite Mutual Information (I₃ → 0). Finally, scaling this effective model to finite XXZ spin chains (N ≤ 10), our data indicates a transition-like behavior from volume-law to area-law entanglement scaling. While bounded by finite-size limitations, our results provide numerical evidence supporting the interpretation of Zeno dynamics as a suppressor of information geometry.
We present a theoretical and numerical study of measurement-induced phase transitions and quantum Zeno dynamics in continuously monitored open many-body systems. Moving beyond closed unitary systems, we investigate the competition between chaotic unitary evolution and continuous weak measurements by employing the stochastic Schrödinger equation (quantum jump Monte Carlo) formalism and non-hermitian effective Hamiltonians. Our analysis examines the transition from area-law to volume-law entanglement scaling, mutual information properties, and the critical scaling hypothesis near the measurement-rate threshold. Furthermore, we derive original analytical estimates for the quantum correlation damping decrement in the regime of strong Zeno suppression and validate the theoretical findings using stochastic trajectory numerical simulation protocols with finite-size scaling.
We introduce and explore a one-dimensional ``hybrid'' quantum circuit model consisting of both unitary gates and projective measurements. While the unitary gates are drawn from a random distribution and act uniformly in the circuit, the measurements are made at random positions and times throughout the system. By varying the measurement rate we can tune between the volume law entangled phase for the random unitary circuit model (no measurements) and a ``quantum Zeno phase'' where strong measurements suppress the entanglement growth to saturate in an area law. Extensive numerical simulations of the quantum trajectories of the many-particle wave functions (exploiting Clifford circuitry to access systems up to 512 qubits) provide evidence for a stable ``weak measurement phase'' that exhibits volume-law entanglement entropy, with a coefficient decreasing with increasing measurement rate. We also present evidence for a continuous quantum dynamical phase transition between the ``weak measurement phase'' and the ``quantum Zeno phase,'' driven by a competition between the entangling tendencies of unitary evolution and the disentangling tendencies of projective measurements. Detailed steady-state and dynamic critical properties of this quantum entanglement transition are accessed.
Abstract We present a numerical study of measurement-induced suppression of coherent tunneling in a two-level quantum system subject to re peated projective monitoring. The dynamics are simulated using a stochastic quantum-trajectory (Monte-Carlo) unraveling which repro duces the dephasing dynamics of a continuously monitored system. We introduce an effective measurement rate γ ≈ pmeas/dt and demon strate a monotonic reduction of the escaped population as a function of γ/∆, where ∆ is the coherent tunneling amplitude. For a fixed evolution time T = π/2, we observe a clear transition to the quantum Zeno regime for γ ≫ ∆. A log–log analysis of the large-γ data re veals an asymptotic scaling close to Pesc ∝ γ−1, in agreement with the strong-measurement limit of the corresponding Lindblad master equation. Our results provide a compact and programmable numerical platform for investigating measurement-controlled tunneling dynamics and Zeno-based control using gate-level quantum simulation frame works.
The quantum Zeno effect (QZE) reveals that frequent measurements can suppress quantum evolution; however, the impact of measurements on the real-space motion of a single atom remains insufficiently explored experimentally. In this work, we employ an optical trap as a measurement pulse and, by monitoring atomic loss, directly observe the QZE in the real-space motion of a single atom. We find that the action of measurement on the atom consists of a projective measurement followed by subsequent periodic unitary evolution, thereby providing an intuitive physical picture of measurement backaction across different timescales. We further investigate the effects of measurement frequency, strength, and spatial position, demonstrating that measurements pulse not only suppress the spatial spreading of the quantum state but also enable deterministic preparation of distinct motional states. Moreover, by dynamically controlling the trap position, we realize measurement-induced directional transport of a single atom, with a velocity exceeding the maximum allowed by the adiabatic condition. Overall, our results provide a direct experimental demonstration of the QZE in real space and establish a versatile framework for measurement-based control of atomic motion, opening new possibilities for motional-state engineering in cold-atom systems.
It is well known that by repeatedly measuring a quantum system it is possible to completely freeze its dynamics into a well defined state, a signature of the quantum Zeno effect. Here we show that for a many-body system evolving under competing unitary evolution and variable-strength measurements the onset of the Zeno effect takes the form of a sharp phase transition. Using the Quantum Ising chain with continuous monitoring of the transverse magnetization as paradigmatic example we show that for weak measurements the entanglement produced by the unitary dynamics remains protected, and actually enhanced by the monitoring, while only above a certain threshold the system is sharply brought into an uncorrelated Zeno state. We show that this transition is invisible to the average dynamics, but encoded in the rare fluctuations of the stochastic measurement process, which we show to be perfectly captured by a non-Hermitian Hamiltonian which takes the form of a Quantum Ising model in an imaginary valued transverse field. We provide analytical results based on the fermionization of the non-Hermitian Hamiltonian in supports of our exact numerical calculations.
The quantum Zeno effect (QZE) predicts that frequent measurement of an unstable quantum system suppresses its decay by repeatedly collapsing the wavefunction back to the undecayed state. However, experimentally confirmed results show that the QZE is fundamentally unattainable for radioactive or radiative decay, because the measurement rates required would destroy the system. We identify a distinct but phenomenologically analogous mechanism within the Stochastic Rupture (SR) framework: informational isolation. In SR, collapse occurs when the local von Neumann entropy approaches the Bousso-bounded informational capacity, SvN → η IBousso. A system that is informationally isolated from its environment — such as a single atom in vacuum, or a system inside a Casimir cavity with suppressed vacuum modes — has a reduced local saturation fraction I, and therefore a suppressed collapse rate. This is decay suppression without measurement, without observer, and without the destructive back-action that kills the standard QZE for radioactive systems. Unlike CSL and Diósi–Penrose, which predict measurable heating of diffuse cosmological matter at rates incompatible with Lyman-α forest and CMB temperature constraints, the SR mechanism is structurally silent in low-saturation environments: the collapse rate vanishes identically when I ≪ 1, independently of particle number or system mass. Informational isolation is thus not merely an analogue of the quantum Zeno effect — it is the same threshold geometry that resolves the cosmological heating problem of competing collapse models, and constitutes a necessary condition for any objective collapse theory to survive cosmological scrutiny. We derive the SR prediction for the suppression factor as a function of environmental mode density and identify two distinct regimes. In the low-saturation regime (I ≪ 1) accessible to current cavity QED, SR reduces exactly to Purcell physics and is not experimentally distinguishable from standard quantum optics. The genuinely SR-specific signature emerges only in the high-saturation regime (I → η), where the runaway factor (1 − I/η)−1 amplifies environmental modulation nonlinearly. This regime is accessible only at macroscopic mass scales (~109 –1010 amu, the MAQRO regime), where the SR discriminator combines with the σ x −2 scaling signature distinguishing SR from CSL and DP. The Casimir-cavity proposal is therefore reframed as a conceptual benchmark rather than a near-term experiment.