Search NASASearch

DOE OSTI · 3391474

String-Breaking Dynamics in Quantum Adiabatic and Diabatic Processes

Surace, Federica Maria [California Institute of Technology (CalTech), Pasadena, CA (United States)] (ORCID:0000000215455230)·Lerose, Alessio [Univ. of Oxford (United Kingdom). Clarendon Lab.; Katholieke Univ. Leuven, Heverlee (Belgium). Inst. for Theoretical Physics] (ORCID:0000000315555327)·Katz, Or [Duke Univ., Durham, NC (United States); Cornell Univ., Ithaca, NY (United States)]·Bennewitz, Elizabeth R. [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.]·Schuckert, Alexander [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000299697391)·Luo, De [Duke Univ., Durham, NC (United States)] (ORCID:0000000248420990)·De, Arinjoy [Duke Univ., Durham, NC (United States); NIST/Univ. of Maryland, College Park, MD (United States). Joint Quantum Inst.]·Ware, Brayden [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000233213198)·Morong, William [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000348808159)·Collins, Kate [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000261598013)·Monroe, Christopher [Duke Univ., Durham, NC (United States)]·Davoudi, Zohreh [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science]·Gorshkov, Alexey V. [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000305093421)

Abstract

Confinement prohibits isolation of color charges, e.g., quarks, in nature via a process called string breaking : the separation of two charges results in an increase in the energy of a color flux, visualized as a string, connecting those charges. Eventually, creating additional charges is energetically favored, hence breaking the string. Such a phenomenon can be probed in simpler models, including quantum spin chains, enabling enhanced understanding of string-breaking dynamics. A challenging task is to understand how string breaking occurs as time elapses, in an out-of-equilibrium setting. This work establishes the phenomenology of dynamical string breaking induced by a gradual increase of string tension over time. It, thus, goes beyond instantaneous quench processes and enables tracking the real-time evolution of strings in a more controlled setting. We focus on domain-wall confinement in a family of quantum Ising chains. Our results indicate that, for sufficiently short strings and slow evolution, string breaking can be described by the transition dynamics of a two-state quantum system akin to a Landau-Zener process. For longer strings, a more intricate spatiotemporal pattern emerges: the string breaks by forming a superposition of bubbles (domains of flipped spins of varying sizes), which involve highly excited states. We finally demonstrate that string breaking driven only by quantum fluctuations can be realized in the presence of sufficiently long-ranged interactions. This work holds immediate relevance for studying string breaking in quantum-simulation experiments.

Explore related subjects

Keep this discovery

BibTeXRIS

Surace, Federica Maria [California Institute of Technology (CalTech), Pasadena, CA (United States)] (ORCID:0000000215455230), Lerose, Alessio [Univ. of Oxford (United Kingdom). Clarendon Lab.; Katholieke Univ. Leuven, Heverlee (Belgium). Inst. for Theoretical Physics] (ORCID:0000000315555327), Katz, Or [Duke Univ., Durham, NC (United States); Cornell Univ., Ithaca, NY (United States)], Bennewitz, Elizabeth R. [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.], Schuckert, Alexander [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000299697391), Luo, De [Duke Univ., Durham, NC (United States)] (ORCID:0000000248420990), De, Arinjoy [Duke Univ., Durham, NC (United States); NIST/Univ. of Maryland, College Park, MD (United States). Joint Quantum Inst.], Ware, Brayden [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000233213198), Morong, William [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000348808159), Collins, Kate [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000261598013), Monroe, Christopher [Duke Univ., Durham, NC (United States)], Davoudi, Zohreh [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science], Gorshkov, Alexey V. [NIST/Univ. of Maryland, College Park, MD (United States). Joint Center for Quantum Information and Computer Science and Joint Quantum Inst.] (ORCID:0000000305093421). 2026-05-18. String-Breaking Dynamics in Quantum Adiabatic and Diabatic Processes. https://doi.org/10.1103/c4zd-lbyq

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

KEEP EXPLORING

Related reports

A Predictive Bubble Point Pressure Model for Porous Liquid Acquisition Device Screens

This article presents a simplified model for porous screen channel liquid acquisition devices based on a maximum bubble point pressure method from Adamson and Gast (1997). To validate the model, three 304 stainless steel (325 × 2300, 450 × 2750, and 510 × 3600) mesh samples were tested in methanol, acetone, isopropyl alcohol, and water. Screen pores are estimated based on analysis from scanning electron microscopy, historical data, and current test data. Results show that the bubble point pressure is proportional to the surface tension of the fluid only when accounting for nonzero contact angles. The previous assumption that bubble point pressure scales inversely with effective pore diameter is shown to be invalid, as the second finest 450 × 2750 produced the highest bubble point of the three screens. The simplified bubble point model can be used to make predictions for any pure fluid when pore diameters are based on bubble point tests and not SEM analysis.

Liquid Acquisition Device

Analytical Model for Steady Flow through a Finite Channel with One Porous Wall with Arbitrary Variable Suction or Injection

This paper presents an exact solution of two-dimensional laminar flow through a finite length channel with one porous wall. It improves upon previous solutions by (1) satisfying the no-slip boundary condition at the channel dead end, (2) adding a turbulent term to the porous wall boundary condition, (3) allowing for arbitrary variable suction or injection across the porous wall, and (4) model validation against new cryogenic liquid hydrogen and oxygen experimental data. Of particular interest in the current work is the modeling of cryogenic propellant flow through a porous liquid acquisition device (LAD) screen and channel inside a propellant tank. First, a detailed review of the literature is presented for previously attempted solutions to channel flow with one porous wall. Next, the governing equations, boundary conditions, and model assumptions are used to derive the analytical flow solution and present general model results for pressure and velocity fields within the channel. Then, the model solution is compared with horizontal LAD channel flow data in liquid oxygen as well as vertical LAD channel flow data in an inverted outflow configuration in liquid hydrogen. Model results are used to update the static cryogenic bubble point pressure model with a dynamic bubble point term which factors in enhanced convection and cooling at the screen during propellant outflow. Convective heat transfer at the LAD screen during outflow is also quantified by comparing model and data. The new analytical flow solution with the dynamic bubble point model is shown to compare well with available cryogenic experimental data

Navier Stokes Equations

Behavior of Ullage Bubbles During Blowdown in Low-g Experiment (BUBBLE): Overview of a Cryogenic Tank Depressurization Test

Behavior of Ullage Bubbles during Blowdown in Low-g Experiment (BUBBLE) is a cryogenic tank depressurization drop tower experiment currently being designed at NASA Glenn Research Center. There is a need for liquid level rise data while venting a cryogenic propellant tank below the liquid saturation pressure in a reduced gravity environment. When a cryogenic tank is vented to a vapor pressure below the liquid saturation pressure, bubbles become entrained in the liquid causing the bulk liquid-vapor interface to rise. In reduced gravity, bubble rise velocity is diminished leading to a larger liquid level rise compared to a 1g environment. The purpose of the experiment is to gain further understanding of tank depressurization fluid physics and obtain high-fidelity data for model validation in 1g and reduced gravity environments. On-orbit cryogenic propellant tanks operating at high fill levels must efficiently manage venting operations to avoid the risk of liquid entrainment in the vent line, which could lead to asymmetric control thruster loads, freezing and clogging, and loss of liquid propellant. Validated models could be used to design settling and venting profiles to reduce risk and increase efficiency for cryogenic storage and transfer operations.

tank venting