Open-system Analogy Validates Berry Conjecture, Demonstrating Chaotic Delocalization In Semiclassical Limits

Understanding chaos in physical systems remains a fundamental challenge, and recent work by Yaohua Li, Yunhan Wang from Tsinghua University, and Yong-Chun Liu et al. offers a significant advance in this field. The team establishes a novel connection between open systems and a long-standing conjecture regarding chaos in isolated systems, revealing how steady states in open systems relate to classical chaotic attractors. Their research demonstrates that these steady states exhibit delocalisation over chaotic attractors, and importantly, identifies a new way to detect chaos through entropy divergence, offering a robust alternative to existing methods. This framework provides a universal paradigm for understanding chaotic behaviour in a wide range of open systems, potentially impacting fields from quantum physics to classical dynamics.

Moving beyond studies of isolated quantum systems, scientists explore how chaos manifests in systems constantly interacting with their surroundings. The study builds upon established theoretical frameworks, including Wigner distributions, Floquet theory, and Lindblad master equations, to analyze the complex dynamics of these open quantum systems. Researchers meticulously examine different system behaviors, comparing their findings with existing theories like quantum diffusion and proposing potential experimental setups for verification.

The work demonstrates that understanding dissipative systems is crucial for real-world applications, as most physical systems are not isolated. Scientists propose experimental realizations using nonlinear optical cavities and microcombs, demonstrating the practical relevance of their theoretical findings. This research addresses a significant gap in the field, offering new insights into the behavior of quantum systems driven far from equilibrium. The findings have implications for understanding and engineering dissipative time crystals, systems exhibiting periodic behavior without requiring energy input.

Chaos and Quantum Delocalization in Floquet Systems

Scientists established a framework linking open quantum systems to classical chaotic dynamics, extending a previously proposed idea for isolated systems. The study pioneers a method for examining the quantum state of a system, demonstrating how these states spread out over classical chaotic attractors as the system becomes more closely aligned with classical behavior. Researchers developed a theoretical approach showing that chaotic systems experience additional spreading due to the inherent unpredictability of chaos, unlike regular systems where spreading is limited to quantum fluctuations. To validate this framework, the team investigated the Floquet Kerr oscillator, a nonlinear system driven by periodic forces.

By increasing the strength of this driving force, they observed a transition from a discrete time crystal phase to a regime of quantum chaos. Numerical simulations tracked the evolution of quantum fluctuations, revealing that they remain limited in regular phases but diverge significantly when the system enters the chaotic phase. Scientists computed the quantum entropy of the system, providing clear evidence of chaotic spreading and establishing a robust method for distinguishing between regular and chaotic open quantum systems. This approach offers a significant advantage over traditional methods, as it is computationally less demanding, particularly as the system approaches classical behavior.

Quantum Chaos and Dissipative Attractor Correspondence

This work establishes a novel connection between open quantum systems and the well-known idea that classical chaotic systems evolve towards specific patterns called attractors. Researchers demonstrate that steady states of open quantum systems correspond to these classical dissipative attractors, extending a previously proposed idea for isolated systems. They validated this correspondence using the Floquet Kerr oscillator, a system exhibiting nonlinear behavior driven by periodic forces. Experiments reveal that the quantum probability distribution spreads out over chaotic attractors as the system becomes more closely aligned with classical behavior.

The team meticulously analyzed the system’s dynamics, identifying three distinct phases, regular, double fixed points, and chaos, each characterized by different attractor structures. Measurements of quantum fluctuations demonstrate that they remain stable in the regular phases but diverge dramatically in the chaotic region, confirming that chaotic spreading dominates over fixed quantum fluctuations. Specifically, the quantum fluctuations remain fixed at approximately 0. 01 in the regular phases, while they increase to over 0. 1 in the chaotic phase.

Further quantitative analysis focused on the entropy of the system, revealing a divergence specifically within the chaotic regime. This entropy divergence provides a robust signature of chaos, distinct from approaches based on traditional methods. Researchers also identified the boundaries between quantum phases by determining the point at which energy dissipation ceases, which coincides with predictions from theoretical models and observable measurements. These findings establish a universal paradigm for understanding chaos in open quantum systems and offer new avenues for exploring the transition between quantum and classical behavior.

Chaos, Time Crystals and Wigner Delocalization

This research establishes a connection between classical chaotic attractors and the quantum state of open quantum systems, extending a previously proposed idea for isolated systems. Scientists demonstrated that, as the system becomes more closely aligned with classical behavior, the quantum state spreads out over classical chaotic attractors. They validated this correspondence through the study of the Floquet Kerr oscillator. A key finding is the emergence of a discrete time crystal phase prior to the onset of chaos in this model, which breaks down as driving strength increases. The team further identified that the diverging entropy observed in the chaotic phase arises specifically from this spreading, offering a robust signature of chaos distinct from approaches based on traditional methods.

For systems with discrete energy levels, the entropy of the chaotic state scales with the size of the total quantum state space, a prediction confirmed in recent studies of a specific model system. While traditional methods prove inadequate in describing the Floquet nonlinear oscillator, this work provides a valuable method for characterizing dissipative chaos in continuous variable systems, particularly those lacking a direct classical analogy. Future research may focus on experimentally verifying these predictions, potentially through observations in four-wave mixing experiments within optical or superconducting cavities, where the chaotic spreading and resulting entropy divergence could serve as characteristic phenomena.

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