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The maximum speed of dynamical evolution

Norman Margolus, Lev B. Levitin

Published Jan 1, 1998• 475 citations
OpenAlex

Abstract

We discuss the problem of counting the maximum number of distinct states that an isolated physical system can pass through in a given period of time---its maximum speed of dynamical evolution. Previous analyses have given bounds in terms of the standard deviation of the energy of the system; here we give a strict bound that depends only on E-E0, the system's average energy minus its ground state energy. We also discuss bounds on information processing rates implied by our bound on the speed of dynamical evolution. For example, adding one Joule of energy to a given computer can never increase its processing rate by more than about 3x10^33 operations per second.

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The maximum speed of dynamical evolution

Norman Margolus, Lev B. Levitin

We discuss the problem of counting the maximum number of distinct states that an isolated physical system can pass through in a given period of time — its maximum speed of dynamical evolution. Previous analyses have given bounds in terms of ΔE, the standard deviation of the energy of the system; here we give a strict bound that depends only on E − E0, the system's average energy minus its ground state energy. We also discuss bounds on information processing rates implied by our bound on the speed of dynamical evolution. For example, adding 1 J of energy to a given computer can never increase its processing rate by more than about 3 × 1033 operations per second.

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Quantum speed limits establish fundamental bounds on the minimum time required for a quantum system to evolve from an initial state to a target state. Traditional formulations treat the evolution speed as a single global quantity governed by the system energy uncertainty or average energy. In this paper, we propose the theory of Quantum Speed-Limit Splitting, which posits that a quantum system undergoing complex dynamics does not necessarily evolve along a single speed limit, but may instead exhibit multiple competing, distinct state-evolution speed limits simultaneously. By defining a multi-valued velocity spectrum belonging to the set {v_1, v_2, ..., v_n}, we demonstrate that different geometric pathways in the underlying Hilbert space correspond to distinct temporal boundaries. We formulate the mathematical framework, replacing the traditional scalar evolution time with a set of multi-branch bounds {tau_1, tau_2, ...}. This theoretical extension provides a novel lens for viewing quantum dynamics, with profound implications for quantum control, thermodynamic cost, and the fundamental limits of information processing.

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We discuss the problem of counting the maximum number of distinct states that an isolated physical system can pass through in a given period of time---its maximum speed of dynamical evolution. Previous analyses have given bounds in terms of the standard deviation of the energy of the system; here we give a strict bound that depends only on E-E0, the system's average energy minus its ground state energy. We also discuss bounds on information processing rates implied by our bound on the speed of dynamical evolution. For example, adding one Joule of energy to a given computer can never increase its processing rate by more than about 3x10^33 operations per second.
We discuss the problem of counting the maximum number of distinct states that an isolated physical system can pass through in a given period of time — its maximum speed of dynamical evolution. Previous analyses have given bounds in terms of ΔE, the standard deviation of the energy of the system; here we give a strict bound that depends only on E − E0, the system's average energy minus its ground state energy. We also discuss bounds on information processing rates implied by our bound on the speed of dynamical evolution. For example, adding 1 J of energy to a given computer can never increase its processing rate by more than about 3 × 1033 operations per second.
I report a tight upper bound of the maximum speed of evolution from one quantum state $\ensuremath{\rho}$ to another ${\ensuremath{\rho}}^{\ensuremath{'}}$ with fidelity $F(\ensuremath{\rho},{\ensuremath{\rho}}^{\ensuremath{'}})$ less than or equal to an arbitrary but fixed value under the action of a time-independent Hamiltonian. Since the bound is directly proportional to the average absolute deviation from the median of the energy of the state DE\mathcal{D}EDE, one may interpret DE\mathcal{D}EDE as a meaningful measure of the maximum information-processing capability of a system.
Quantum speed limits set the maximal pace of state evolution. Two well-known limits exist for a unitary time-independent Hamiltonian: the Mandelstam-Tamm and Margolus-Levitin bounds. The former restricts the rate according to the state energy uncertainty, while the latter depends on the mean energy relative to the ground state. Here we report on an additional bound that exists for states with a bounded energy spectrum. This bound is dual to the Margolus-Levitin one in the sense that it depends on the difference between the state's mean energy and the energy of the highest occupied eigenstate. Each of the three bounds can become the most restrictive one, depending on the spread and mean of the energy, forming three dynamical regimes which are accessible in a multilevel system. The new bound is relevant for quantum information applications, since in most of them, information is stored and manipulated in a Hilbert space with a bounded energy spectrum.
Maximum counts of distinct states define important physical quantities, the most famous being entropy. Here we show that energy, momentum and other basic quantities of mechanics are also maximum counts. This generalizes a property familiar in communication with classical waves: frequency-width equals maximum number of distinct values that can be sent, per unit time. Basic mechanical quantities are frequency-widths of wavefunction evolution, and similarly bound number of distinct states. Evolutions that achieve maximum distinctness are effectively discrete. These properties refine our understanding of uncertainty, measurement, classical mechanics, and relativity.
The presence of noise or the interaction with an environment can radically change the dynamics of observables of an otherwise isolated quantum system.We derive a bound on the speed with which observables of open quantum systems evolve.This speed limit is divided into Mandelstam and Tamm's original time-energy uncertainty relation and a time-information uncertainty relation recently derived for classical systems, and both are generalized to open quantum systems.By isolating the coherent and incoherent contributions to the system dynamics, we derive both lower and upper bounds on the speed of evolution.We prove that the latter provide tighter limits on the speed of observables than previously known quantum speed limits and that a preferred basis of speed operators serves to completely characterize the observables that saturate the speed limits.We use this construction to bound the effect of incoherent dynamics on the evolution of an observable and to find the Hamiltonian that gives the maximum coherent speedup to the evolution of an observable.
Quantum speed limits establish fundamental bounds on the minimum time required for a quantum system to evolve from an initial state to a target state. Traditional formulations treat the evolution speed as a single global quantity governed by the system energy uncertainty or average energy. In this paper, we propose the theory of Quantum Speed-Limit Splitting, which posits that a quantum system undergoing complex dynamics does not necessarily evolve along a single speed limit, but may instead exhibit multiple competing, distinct state-evolution speed limits simultaneously. By defining a multi-valued velocity spectrum belonging to the set {v_1, v_2, ..., v_n}, we demonstrate that different geometric pathways in the underlying Hilbert space correspond to distinct temporal boundaries. We formulate the mathematical framework, replacing the traditional scalar evolution time with a set of multi-branch bounds {tau_1, tau_2, ...}. This theoretical extension provides a novel lens for viewing quantum dynamics, with profound implications for quantum control, thermodynamic cost, and the fundamental limits of information processing.