Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Dynamics and entanglement of exotic quantum liquids

Thomas Veness

Published Jan 1, 2017• 0 citations
Publisher

Abstract

This thesis focuses on the one-dimensional Hubbard model, considering both dynamical response functions and also particular entanglement measures of highly excited eigenstates. In Chapter 2 we discuss how to describe the optical conductivity at finite energy scales. In order to calculate the dynamical response of this interacting system, it is necessary to go beyond the conventional Luttinger liquid picture. Using mobile impurity models and integrability we make quantitative predictions which can be compared with numerics. In Chapter 3, we investigate the existence of the so-called "quantum disentangled liquid" (QDL) in the same system. The diagnostic for the QDL involves understanding the bipartite entanglement entropy of highly excited eigenstates. Here we use results from integrability and strong-coupling expansions to argue that such a state of matter is realised in the Hubbard chain in a specific sense.

DOI
10.5287/ora-br44nywgz

Related papers

Quantum disentangled liquid in the half-filled Hubbard model

Thomas Veness, Fabian H. L. Eßler, Matthew P. A. Fisher

Our expectation of thermalization is one borne of experience, and it is interesting to understand how conventional statistical mechanics may fail. The so-called quantum disentangled liquid (QDL) is a paradigm outside of the (Generalized) Gibbs description, but also without spatial disorder, precluding many-body localization. In this paper, the authors provide evidence that this QDL behavior exists in the Hubbard model. The QDL diagnostic involves bipartite entanglement entropies after a partial measurement. Both integrability in 1D and strong-coupling techniques are used to argue that the QDL diagnostic is indeed satisfied.

arXiv:1611.02075•Physical review. B./Physical review. B•Nov 27, 2017•22 citations

Atypical energy eigenstates in the Hubbard chain and quantum disentangled liquids

Thomas Veness, Fabian H. L. Essler, Matthew P. A. Fisher

We investigate the implications of integrability for the existence of quantum disentangled liquid (QDL) states in the half-filled one-dimensional Hubbard model. We argue that there exist finite energy-density eigenstates that exhibit QDL behaviour in the sense of Grover & Fisher (2014 J. Stat. Mech. 2014 , P10010. ( doi:10.1088/1742-5468/2014/10/P10010 )). These states are atypical in the sense that their entropy density is smaller than that of thermal states at the same energy density. Furthermore, we show that thermal states in a particular temperature window exhibit a weaker form of the QDL property, in agreement with recent results obtained by strong-coupling expansion methods in Veness et al. (2016 ( http://arxiv.org/abs/1611.02075 )). This article is part of the themed issue ‘Breakdown of ergodicity in quantum systems: from solids to synthetic matter’.

arXiv:1711.02738•Philosophical Transactions of the Royal Society A Mathematical Physical and Engineering Sciences•Oct 30, 2017•4 citations

Characterization of quasi-Fermi liquids using matrix product state methods in the thermodynamic limit

Joshua D. Baktay

This thesis focuses on the development and application of tensor networks methods for simulating one-dimensional quantum many-body systems. The general aim is to unveil numerical evidence for a new universality class of 1D interacting fermion systems referred to as quasi-Fermi liquids (qFLs). Realizing such systems beyond a purely analytical context and elucidating their peculiar characteristics is the principle value of this thesis.Chapter 1 begins by introducing the essential physics of one-dimensional systems, known as Luttinger liquids relative to their higher dimensional counterparts. Then it introduces non-linear Luttinger liquids juxtaposed against the defining quasi-Fermi liquid (qFL) field theory that motivates the following lattice studies. Chapter 2 provides an in-depth review of matrix product states (MPS), the main methodology used to explore quasi-Fermi liquids. The chapter serves as a pedagogical introduction to the field and details those novel algorithmic developments necessary for the study of fermionic systems. The central result of this chapter is the section on finite entanglement scaling techniques applied to dynamic correlation functions. Chapter 3 begins the study of lattice models that exhibit quasi-Fermi liquid characteristics. Here we explore the ground states exclusively by computing their static correlation functions. The central results include Luttinger parameter phase space diagrams which demonstrate the existence of the quasi-Fermi liquid across multiple lattice models. Chapter 4 studies the excitations of the qFL lattice models. We begin with results from non-MPS based methods which were essential for benchmarking our novel application of MPS to fermionic spectral functions. The central results of the chapter are the power-law exponents that demonstrate the low-energy universality of the qFL and our analysis of the dynamic structure factor. Chapter 5 concludes with a recapitulation of the main results and an outlook on future work. The Appendix contains those tensor diagrams necessary for a numerical implementation of those algorithms introduced in Chapter 2.--Author's abstract

•Jan 1, 2024•0 citations

Quantum impurities in interacting environments

Colin Rylands

The quantum physics of one dimensional systems exhibits many remarkable and exotic physical phenomena. These are the result of the strong correlations which exist in such systems due to the reduced dimensionality and in many cases can be described by Luttinger Liquid theory. Likewise quantum impurity systems, where a bath of particles couples to the same impurity, exhibit well known non perturbative phenomena like the Kondo effect. In this thesis we study the physics of quantum impurities in interacting environments - the intersection of these two areas. Such Luttinger-impurity systems can be realized experimentally in a range of different settings from quantum wires and carbon nano tubes to edges of fractional quantum hall systems and cold atom gases. We show that many of the models used to describe these experiments are integrable and can be studied by means of the Bethe Ansatz. This powerful and exact method provides us with the exact eigenstates and energy levels of the model Hamiltonian. The models considered include two which describe a Lutttinger liquid coupled to a back scattering impurity, the Kane-Fisher and weak tunnelling model as well as Luttinger liquids coupled a quantum dot in various geometries: at the boundary, sidecoupled and embedded. To incorporate both the backscattering nature of the impurities and the interacting bulk particles a new formulation of the Bethe Ansatz is developed and implemented. The eigenstates and spectra of the models are found and used to investigate their ground state and thermodynamic properties.

Bulletin of the American Physical Society•Jan 1, 2018•0 citations

Quantum disentangled liquids

Tarun Grover, Matthew P. A. Fisher

We propose and explore a new finite temperature phase of translationally invariant multi-component liquids which we call a 'Quantum Disentangled Liquid' (QDL) phase. We contemplate the possibility that in fluids consisting of two (or more) species of indistinguishable quantum particles with a large mass ratio, the light particles might 'localize' on the heavy particles. We give a precise, formal definition of this QDL phase in terms of the finite energy density many-particle wavefunctions. While the heavy particles are fully thermalized, for a typical fixed configuration of the heavy particles, the entanglement entropy of the light particles satisfies an area law; this implies that the light particles have not thermalized. Equivalently, but more intuitively, if the positions of all the heavy particles are measured , the projected wavefunction for the unmeasured light particles has as an area law entanglement entropy. Thus, in a QDL phase, thermal equilibration is incomplete, and the canonical assumptions of statistical mechanics are not fully operative. The definition of the QDL phase for heavy/light particles can be readily generalized to other cases with two (or more) conserved currents, such as spin/charge in a system of spin-1/2 fermions (as in a Hubbard model). Indeed, we argue that the finite energy-density eigenstates of the t – J model will generically be in such a spin/charge QDL, although the fate of the QDL in the large U Hubbard model is uncertain. We explore the possibility of QDL in water, with the light proton degrees of freedom becoming 'localized' on the oxygen ions. While we do not presently know whether a local, generic Hamiltonian can have eigenstates of the QDL form, if not, then the non-thermal behavior discussed here will exist as an interesting crossover phenomena at a time scale that diverges as the ratio of the mass of the heavy to the light particles also diverges.

arXiv:1307.2288•Journal of Statistical Mechanics Theory and Experiment•Oct 9, 2014•139 citations

Interplay between charge, spin, and phonons in low dimensional strongly interacting systems

Mohammad Soltanieh-ha

Interacting one-dimensional electron systems are generally referred to as "Luttinger liquids", after the effective low-energy theory in which spin and charge behave as separate degrees of freedom with independent energy scales. The "spin-incoherent Luttinger liquid" describes a finite-temperature regime that is realized when the temperature is very small relative to the Fermi energy, but larger than the characteristic spin energy scale, and it is realized for instance in the strongly interacting Hubbard chain (with U → ∞). Similar physics can take place in the ground-state, when a Luttinger Liquid is coupled to a spin bath, which effectively introduces a "spin temperature" through its entanglement with the spin degree of freedom. We show that the spin-incoherent state can be exactly written as a factorized wave-function, with a spin wave-function that can be described within a valence bond formalism. This enables us to calculate exact expressions for the momentum distribution function and the entanglement entropy. This picture holds not only for two antiferromagnetically coupled t-J chains, but also for the t-J-Kondo chain with strongly interacting conduction electrons. In chapter 3 we argue that this theory is quite universal and may describe a family of problems that could be dubbed "spin-incoherent".

•Jan 1, 2015•0 citations
This thesis focuses on the one-dimensional Hubbard model, considering both dynamical response functions and also particular entanglement measures of highly excited eigenstates. In Chapter 2 we discuss how to describe the optical conductivity at finite energy scales. In order to calculate the dynamical response of this interacting system, it is necessary to go beyond the conventional Luttinger liquid picture. Using mobile impurity models and integrability we make quantitative predictions which can be compared with numerics. In Chapter 3, we investigate the existence of the so-called "quantum disentangled liquid" (QDL) in the same system. The diagnostic for the QDL involves understanding the bipartite entanglement entropy of highly excited eigenstates. Here we use results from integrability and strong-coupling expansions to argue that such a state of matter is realised in the Hubbard chain in a specific sense.
Our expectation of thermalization is one borne of experience, and it is interesting to understand how conventional statistical mechanics may fail. The so-called quantum disentangled liquid (QDL) is a paradigm outside of the (Generalized) Gibbs description, but also without spatial disorder, precluding many-body localization. In this paper, the authors provide evidence that this QDL behavior exists in the Hubbard model. The QDL diagnostic involves bipartite entanglement entropies after a partial measurement. Both integrability in 1D and strong-coupling techniques are used to argue that the QDL diagnostic is indeed satisfied.
We investigate the implications of integrability for the existence of quantum disentangled liquid (QDL) states in the half-filled one-dimensional Hubbard model. We argue that there exist finite energy-density eigenstates that exhibit QDL behaviour in the sense of Grover & Fisher (2014 J. Stat. Mech. 2014 , P10010. ( doi:10.1088/1742-5468/2014/10/P10010 )). These states are atypical in the sense that their entropy density is smaller than that of thermal states at the same energy density. Furthermore, we show that thermal states in a particular temperature window exhibit a weaker form of the QDL property, in agreement with recent results obtained by strong-coupling expansion methods in Veness et al. (2016 ( http://arxiv.org/abs/1611.02075 )). This article is part of the themed issue ‘Breakdown of ergodicity in quantum systems: from solids to synthetic matter’.
This thesis focuses on the development and application of tensor networks methods for simulating one-dimensional quantum many-body systems. The general aim is to unveil numerical evidence for a new universality class of 1D interacting fermion systems referred to as quasi-Fermi liquids (qFLs). Realizing such systems beyond a purely analytical context and elucidating their peculiar characteristics is the principle value of this thesis.Chapter 1 begins by introducing the essential physics of one-dimensional systems, known as Luttinger liquids relative to their higher dimensional counterparts. Then it introduces non-linear Luttinger liquids juxtaposed against the defining quasi-Fermi liquid (qFL) field theory that motivates the following lattice studies. Chapter 2 provides an in-depth review of matrix product states (MPS), the main methodology used to explore quasi-Fermi liquids. The chapter serves as a pedagogical introduction to the field and details those novel algorithmic developments necessary for the study of fermionic systems. The central result of this chapter is the section on finite entanglement scaling techniques applied to dynamic correlation functions. Chapter 3 begins the study of lattice models that exhibit quasi-Fermi liquid characteristics. Here we explore the ground states exclusively by computing their static correlation functions. The central results include Luttinger parameter phase space diagrams which demonstrate the existence of the quasi-Fermi liquid across multiple lattice models. Chapter 4 studies the excitations of the qFL lattice models. We begin with results from non-MPS based methods which were essential for benchmarking our novel application of MPS to fermionic spectral functions. The central results of the chapter are the power-law exponents that demonstrate the low-energy universality of the qFL and our analysis of the dynamic structure factor. Chapter 5 concludes with a recapitulation of the main results and an outlook on future work. The Appendix contains those tensor diagrams necessary for a numerical implementation of those algorithms introduced in Chapter 2.--Author's abstract
The quantum physics of one dimensional systems exhibits many remarkable and exotic physical phenomena. These are the result of the strong correlations which exist in such systems due to the reduced dimensionality and in many cases can be described by Luttinger Liquid theory. Likewise quantum impurity systems, where a bath of particles couples to the same impurity, exhibit well known non perturbative phenomena like the Kondo effect. In this thesis we study the physics of quantum impurities in interacting environments - the intersection of these two areas. Such Luttinger-impurity systems can be realized experimentally in a range of different settings from quantum wires and carbon nano tubes to edges of fractional quantum hall systems and cold atom gases. We show that many of the models used to describe these experiments are integrable and can be studied by means of the Bethe Ansatz. This powerful and exact method provides us with the exact eigenstates and energy levels of the model Hamiltonian. The models considered include two which describe a Lutttinger liquid coupled to a back scattering impurity, the Kane-Fisher and weak tunnelling model as well as Luttinger liquids coupled a quantum dot in various geometries: at the boundary, sidecoupled and embedded. To incorporate both the backscattering nature of the impurities and the interacting bulk particles a new formulation of the Bethe Ansatz is developed and implemented. The eigenstates and spectra of the models are found and used to investigate their ground state and thermodynamic properties.
We propose and explore a new finite temperature phase of translationally invariant multi-component liquids which we call a 'Quantum Disentangled Liquid' (QDL) phase. We contemplate the possibility that in fluids consisting of two (or more) species of indistinguishable quantum particles with a large mass ratio, the light particles might 'localize' on the heavy particles. We give a precise, formal definition of this QDL phase in terms of the finite energy density many-particle wavefunctions. While the heavy particles are fully thermalized, for a typical fixed configuration of the heavy particles, the entanglement entropy of the light particles satisfies an area law; this implies that the light particles have not thermalized. Equivalently, but more intuitively, if the positions of all the heavy particles are measured , the projected wavefunction for the unmeasured light particles has as an area law entanglement entropy. Thus, in a QDL phase, thermal equilibration is incomplete, and the canonical assumptions of statistical mechanics are not fully operative. The definition of the QDL phase for heavy/light particles can be readily generalized to other cases with two (or more) conserved currents, such as spin/charge in a system of spin-1/2 fermions (as in a Hubbard model). Indeed, we argue that the finite energy-density eigenstates of the t – J model will generically be in such a spin/charge QDL, although the fate of the QDL in the large U Hubbard model is uncertain. We explore the possibility of QDL in water, with the light proton degrees of freedom becoming 'localized' on the oxygen ions. While we do not presently know whether a local, generic Hamiltonian can have eigenstates of the QDL form, if not, then the non-thermal behavior discussed here will exist as an interesting crossover phenomena at a time scale that diverges as the ratio of the mass of the heavy to the light particles also diverges.
Interacting one-dimensional electron systems are generally referred to as "Luttinger liquids", after the effective low-energy theory in which spin and charge behave as separate degrees of freedom with independent energy scales. The "spin-incoherent Luttinger liquid" describes a finite-temperature regime that is realized when the temperature is very small relative to the Fermi energy, but larger than the characteristic spin energy scale, and it is realized for instance in the strongly interacting Hubbard chain (with U → ∞). Similar physics can take place in the ground-state, when a Luttinger Liquid is coupled to a spin bath, which effectively introduces a "spin temperature" through its entanglement with the spin degree of freedom. We show that the spin-incoherent state can be exactly written as a factorized wave-function, with a spin wave-function that can be described within a valence bond formalism. This enables us to calculate exact expressions for the momentum distribution function and the entanglement entropy. This picture holds not only for two antiferromagnetically coupled t-J chains, but also for the t-J-Kondo chain with strongly interacting conduction electrons. In chapter 3 we argue that this theory is quite universal and may describe a family of problems that could be dubbed "spin-incoherent".