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Annales Henri Poincaré

, Volume 17, Issue 7, pp 1737–1791 | Cite as

Lieb–Robinson Bounds, Arveson Spectrum and Haag–Ruelle Scattering Theory for Gapped Quantum Spin Systems

  • Sven Bachmann
  • Wojciech Dybalski
  • Pieter Naaijkens
Article

Abstract

We consider translation invariant gapped quantum spin systems satisfying the Lieb–Robinson bound and containing single-particle states in a ground state representation. Following the Haag–Ruelle approach from relativistic quantum field theory, we construct states describing collisions of several particles, and define the corresponding S-matrix. We also obtain some general restrictions on the shape of the energy–momentum spectrum. For the purpose of our analysis, we adapt the concepts of almost local observables and energy–momentum transfer (or Arveson spectrum) from relativistic QFT to the lattice setting. The Lieb–Robinson bound, which is the crucial substitute of strict locality from relativistic QFT, underlies all our constructions. Our results hold, in particular, in the Ising model in strong transverse magnetic fields.

Keywords

Ising Model Mass Shell Local Observable Scatter Theory Asymptotic Completeness 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer Basel 2015

Authors and Affiliations

  • Sven Bachmann
    • 1
  • Wojciech Dybalski
    • 2
  • Pieter Naaijkens
    • 3
  1. 1.Mathematisches Institut der Universität MünchenMünchenGermany
  2. 2.Zentrum MathematikTechnische Universität MünchenGarchingGermany
  3. 3.Institut für Theoretische PhysikLeibniz Universität HannoverHannoverGermany

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