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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

Professor Fabian Essler

Professorial Research Fellow

Research theme

  • Fields, strings, and quantum dynamics
  • Quantum materials

Sub department

  • Rudolf Peierls Centre for Theoretical Physics

Research groups

  • Condensed Matter Theory
Fabian.Essler@physics.ox.ac.uk
Telephone: 01865 (2)73971
Rudolf Peierls Centre for Theoretical Physics, room 70.12
www-thphys.physics.ox.ac.uk/people/FabianEssler
  • About
  • Publications

Finite temperature and quench dynamics in the Transverse Field Ising Model from form factor expansions

(2020)

Authors:

Etienne Granet, Maurizio Fagotti, Fabian HL Essler
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Yang-Baxter integrable Lindblad equations

SciPost Physics SciPost (2020)

Authors:

Fabian HL Essler, Aleksandra A Ziolkowska

Abstract:

We consider Lindblad equations for one dimensional fermionic models and quantum spin chains. By employing a (graded) super-operator formalism we identify a number of Lindblad equations than can be mapped onto non-Hermitian interacting Yang-Baxter integrable models. Employing Bethe Ansatz techniques we show that the late-time dynamics of some of these models is diffusive.
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On the low-energy description for tunnel-coupled one-dimensional Bose gases

(2020)

Authors:

Yuri D van Nieuwkerk, Fabian HL Essler
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Yang-Baxter integrable Lindblad equations

(2020)

Authors:

Aleksandra A Ziolkowska, Fabian HL Essler
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How order melts after quantum quenches

PHYSICAL REVIEW B 101:4 (2020) 41110

Authors:

Mario Collura, Fabian HL Essler

Abstract:

© 2020 American Physical Society. Injecting a sufficiently large energy density into an isolated many-particle system prepared in a state with long-range order will lead to the melting of the order over time. Detailed information about this process can be derived from the quantum mechanical probability distribution of the order parameter. We study this process for the paradigmatic case of the spin-1/2 Heisenberg XXZ chain. We determine the full quantum mechanical distribution function of the staggered subsystem magnetization as a function of time after a quantum quench from the classical Néel state. We establish the existence of an interesting regime at intermediate times that is characterized by a very broad probability distribution. Based on our findings we propose a simple general physical picture of how long-range order melts.
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