The relation between classical and quantum Lyapunov exponent and the bound on chaos in classically chaotic quantum systems
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| Format: | Preprint |
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2025
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| author | Haneder, Fabian Caspari, Gerrit Urbina, Juan Diego Richter, Klaus |
| author_facet | Haneder, Fabian Caspari, Gerrit Urbina, Juan Diego Richter, Klaus |
| contents | Out-of-Time-Ordered Commutators (OTOCs), representing a key diagnostic for scrambling as a facet of short-time quantum chaos, have attracted wide-ranging interest, from many-body physics to quantum gravity. By means of a suitable form of the Wigner-Moyal expansion, and invoking ensemble equivalence in statistical physics, we provide a consistent approach to the growth rate of the OTOC for many-body systems with chaotic classical limit where both the classical Lyapunov exponent and the quantum nature of the density of states enter. Applying this construction to quantized high-dimensional hyperbolic motion, i.e., a quantum chaotic system that exhibits gravity-like correlation functions in the late-time regime, we compute the OTOC growth rate $Λ$ as a function of the number of degrees of freedom, $f$, and inverse temperature, $β$.
We show that the scaled growth rate, $Λ/f$, can be described by a universal function of $f β$ and displays a cross-over from classical to quantum behavior as we increase $f$ and/or lower the temperature. In the deep quantum regime of infinite $f$, we find maximally fast scrambling in the sense of the Maldacena-Shenker-Stanford bound on chaos. This elucidates the non-perturbative mechanism underlying the saturation of the bound via quantum contributions to the mean density of states, and it provides further support for this dynamical system as a dual to two-dimensional quantum gravity. In this way, we present first evidence of maximally fast scrambling in a quantum chaotic system with a well-defined classical Hamiltonian limit, without invoking any external mechanism such as (disorder) averaging. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2512_19869 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | The relation between classical and quantum Lyapunov exponent and the bound on chaos in classically chaotic quantum systems Haneder, Fabian Caspari, Gerrit Urbina, Juan Diego Richter, Klaus Chaotic Dynamics Statistical Mechanics High Energy Physics - Theory Quantum Physics Out-of-Time-Ordered Commutators (OTOCs), representing a key diagnostic for scrambling as a facet of short-time quantum chaos, have attracted wide-ranging interest, from many-body physics to quantum gravity. By means of a suitable form of the Wigner-Moyal expansion, and invoking ensemble equivalence in statistical physics, we provide a consistent approach to the growth rate of the OTOC for many-body systems with chaotic classical limit where both the classical Lyapunov exponent and the quantum nature of the density of states enter. Applying this construction to quantized high-dimensional hyperbolic motion, i.e., a quantum chaotic system that exhibits gravity-like correlation functions in the late-time regime, we compute the OTOC growth rate $Λ$ as a function of the number of degrees of freedom, $f$, and inverse temperature, $β$. We show that the scaled growth rate, $Λ/f$, can be described by a universal function of $f β$ and displays a cross-over from classical to quantum behavior as we increase $f$ and/or lower the temperature. In the deep quantum regime of infinite $f$, we find maximally fast scrambling in the sense of the Maldacena-Shenker-Stanford bound on chaos. This elucidates the non-perturbative mechanism underlying the saturation of the bound via quantum contributions to the mean density of states, and it provides further support for this dynamical system as a dual to two-dimensional quantum gravity. In this way, we present first evidence of maximally fast scrambling in a quantum chaotic system with a well-defined classical Hamiltonian limit, without invoking any external mechanism such as (disorder) averaging. |
| title | The relation between classical and quantum Lyapunov exponent and the bound on chaos in classically chaotic quantum systems |
| topic | Chaotic Dynamics Statistical Mechanics High Energy Physics - Theory Quantum Physics |
| url | https://arxiv.org/abs/2512.19869 |