Search NASASearch

DOE OSTI · 2937948

Generalized geometric speed limits for quantum observables

Bringewatt, Jacob [US Naval Academy, Annapolis, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science; National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute; Harvard Univ., Cambridge, MA (United States)] (ORCID:0000000332353444)·Steffen, Zach [Univ. of Maryland, College Park, MD (United States). Maryland Quantum Materials Center; Laboratory for Physical Sciences, College Park, MD (United States)] (ORCID:0000000209710901)·Ritter, Martin A. [Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0000000342350781)·Ehrenberg, Adam [Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science; National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0000000231676519)·Wang, Haozhi [Univ. of Maryland, College Park, MD (United States). Maryland Quantum Materials Center; Laboratory for Physical Sciences, College Park, MD (United States)] (ORCID:000000029788357X)·Palmer, B. S. [Univ. of Maryland, College Park, MD (United States). Maryland Quantum Materials Center; Laboratory for Physical Sciences, College Park, MD (United States)] (ORCID:000000021259995X)·Kollár, Alicia J. [Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0009000320194594)·Gorshkov, Alexey V. [Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science; National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0000000305093421)·García-Pintos, Luis Pedro [Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)] (ORCID:0000000320754996)

Abstract

Leveraging quantum information geometry, we derive generalized quantum speed limits on the rate of change of the expectation values of observables. These bounds subsume and, for Hilbert space dimension ≥3, tighten existing bounds—in some cases by an arbitrarily large multiplicative constant. Our theoretical results are supported by illustrative examples and an experimental demonstration using a superconducting qutrit. We also derive two upper bounds on the generalized quantum Fisher information in terms of the condition number of the density matrix. One of these bounds applies only to coherent dynamics and depends also on the variance of the Hamiltonian. The other bound depends also on the so-called Wigner-Yanase skew information. These bounds generalize well-known bounds on the symmetric logarithmic derivative quantum Fisher information and are tighter than the existing bounds for sufficiently mixed states (e.g., for sufficiently high temperature thermal states).

Explore related subjects

Keep this discovery

BibTeXRIS

Bringewatt, Jacob [US Naval Academy, Annapolis, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science; National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute; Harvard Univ., Cambridge, MA (United States)] (ORCID:0000000332353444), Steffen, Zach [Univ. of Maryland, College Park, MD (United States). Maryland Quantum Materials Center; Laboratory for Physical Sciences, College Park, MD (United States)] (ORCID:0000000209710901), Ritter, Martin A. [Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0000000342350781), Ehrenberg, Adam [Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science; National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0000000231676519), Wang, Haozhi [Univ. of Maryland, College Park, MD (United States). Maryland Quantum Materials Center; Laboratory for Physical Sciences, College Park, MD (United States)] (ORCID:000000029788357X), Palmer, B. S. [Univ. of Maryland, College Park, MD (United States). Maryland Quantum Materials Center; Laboratory for Physical Sciences, College Park, MD (United States)] (ORCID:000000021259995X), Kollár, Alicia J. [Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0009000320194594), Gorshkov, Alexey V. [Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science; National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States); Univ. of Maryland, College Park, MD (United States). Joint Quantum Institute] (ORCID:0000000305093421), García-Pintos, Luis Pedro [Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)] (ORCID:0000000320754996). 2025-09-04. Generalized geometric speed limits for quantum observables. https://doi.org/10.1103/h6lj-d6yt

Cite the original work for its findings. Save a collection to share your selection of sources.

Discover connections

Connections use source metadata and explicit phrase matches, not verified experimental comparisons.

KEEP EXPLORING

Related discoveries

Trajectory-independent speed limits for controlled open quantum systems

Existing quantum speed limits for controlled open quantum systems depend on the specified trajectory. For example, lower bounds on quantum annealing times in the presence of dissipation depend explicitly on the chosen annealing schedule. Recently, schedule-independent speed limits have been derived for annealing in the closed quantum system setting [L. P. García-Pintos et al ., SciPost Phys. 18 , 159 (2025)]. In this work, we generalize these results to open quantum systems, deriving schedule-independent lower bounds for quantum annealing times in systems described by a Lindblad master equation. We analyze the interplay between coherent control and dissipation in single- and two-qubit examples, demonstrating that the derived lower bounds capture key scaling behavior with respect to the strength of the dissipator. Finally, we apply the bound to thermal state preparation and show that the bound matches the expected asymptotic behavior for an Ising model in the high-temperature limit.

open quantum systems & decoherence

Nonequilibrium dynamics of two-level systems directly after cryogenic alternating bias

Two-level systems (TLSs) are a dominant decoherence mechanism in superconducting qubits, microwave kinetic inductance detectors, and quantum dots. TLSs are tunneling states commonly found in amorphous materials and interfaces, which interact electromechanically, leading to energy loss. Fluctuations in the frequency of the TLSs are a significant problem for qubit operation and force recalibration every few hours. In this study, we probe the effect of alternating bias at cryogenic temperatures on TLSs in a purpose-built LC oscillator. When an in situ alternating bias is applied, the steady-state spectra of the TLSs disappear. Spectroscopy reveals transient behavior, in which the TLS frequency fluctuates on the order of minutes. Thermal cycling above 10 K reverses these effects, restoring the TLS spectrum to its original state. Importantly, the intrinsic loss tangent of the LC oscillator remains unchanged before and after the application of the alternating bias. We propose that the disappearance of the steady-state spectrum is caused by nonequilibrium energy buildup from strain in the oxide film introduced by the pulsed voltage-bias sequence. Understanding this nonequilibrium energy could shed light on TLS fluctuations and reduce the calibration requirements for qubits.

general physics

The phase diagram of quantum chromodynamics in one dimension on a quantum computer

The quantum chromodynamics (QCD) phase diagram, which reveals the state of strongly interacting matter at different temperatures and densities, is key to answering open questions in physics, ranging from the behaviour of particles in neutron stars to the conditions of the early universe. However, classical simulations of QCD face significant computational barriers, such as the sign problem at finite matter densities. Quantum computing offers a promising solution to overcome these challenges. Here, we take an important step toward exploring the QCD phase diagram with quantum devices by preparing thermal states in one-dimensional non-Abelian gauge theories. We experimentally simulate the thermal states of SU(2) and SU(3) gauge theories at finite densities on a trapped-ion quantum computer using a variational method. This is achieved by introducing two features: Firstly, we add motional ancillae to the existing qubit register to efficiently prepare thermal probability distributions. Secondly, we introduce charge-singlet measurements to enforce colour-neutrality constraints. This work pioneers the quantum simulation of QCD at finite density and temperature for two and three colours, laying the foundation to explore QCD phenomena on quantum platforms.

Quantum information