4.6 Article

Quantum simulation of lattice gauge theories using Wilson fermions

Journal

QUANTUM SCIENCE AND TECHNOLOGY
Volume 3, Issue 3, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/2058-9565/aac33b

Keywords

quantum simulation; lattice gauge theory; Wilson fermions; ultracold atoms; Bose-Fermi mixture; real-time dynamics; Schwinger mechanism

Funding

  1. DFG Collaborative Research Center [SFB 1225]
  2. ERC Advanced Grant 'AtomicGaugeSimulator' [339220]
  3. ERC Advanced Grant 'EntangleGen' [694561]
  4. DFG [377616843]
  5. Excellence Initiative of the German federal government and the state governments-funding line Institutional Strategy (Zukunftskonzept): DFG project [ZUK 49/U]
  6. European Research Council (ERC) [339220] Funding Source: European Research Council (ERC)

Ask authors/readers for more resources

Quantum simulators have the exciting prospect of giving access to real-time dynamics of lattice gauge theories, in particular in regimes that are difficult to compute on classical computers. Future progress towards scalable quantum simulation of lattice gauge theories, however, hinges crucially on the efficient use of experimental resources. As we argue in this work, due to the fundamental non-uniqueness of discretizing the relativistic Dirac Hamiltonian, the lattice representation of gauge theories allows for an optimization that up to now has been left unexplored. We exemplify our discussion with lattice quantum electrodynamics in two-dimensional space-time, where we show that the formulation through Wilson fermions provides several advantages over the previously considered staggered fermions. Notably, it enables a strongly simplified optical-lattice setup and it reduces the number of degrees of freedom required to simulate dynamical gauge fields. Exploiting the optimal representation, we propose an experiment based on a mixture of ultracold atoms trapped in a tilted optical lattice. Using numerical benchmark simulations, we demonstrate that a state-of-the-art quantum simulator may access the Schwinger mechanism and map out its non-perturbative onset.

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