Quantum link models provide an extension of Wilson's lattice gauge theory with a finite-dimensional link Hilbert space. Quantum links are discrete quantum variables endowed with an exact continuous local symmetry. For example, an Abelian U(1) quantum link model is formulated in terms of quantum spins residing in a representation of SU(2). Non-Abelian U(N), SO(N), or SP(N) quantum links are generalized quantum spins residing in an embedding algebra SU(2N), SO(2N), or Sp(2N), respectively. On the one hand, quantum link models possess qualitatively new "crystalline" or "nematic" confined phases with spontaneously broken lattice translation or rotation symmetry. On the other hand, they provide an alternative regularization of asymptotically free continuum theories including CP(N-1) models and QCD. The continuum limit is then reached in the framework of D-theory, in which discrete variables undergo dimensional reduction. In this way, (1+1)-d CP(N-1) models arise from the dimensional reduction of (2+1)-d SU(N) quantum spin ladders with massless Goldstone bosons, while (3+1)-d QCD emerges from a (4+1)-d Coulomb phase with massless gluons. Quarks arise naturally as domain wall fermions. Quantum link models provide a formulation of gauge theories with a minimal number of quantum degrees of freedom, which makes them ideally suited for resource efficient quantum simulation and computation experiments.
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