Abstract

We study possible quantum $U(1)$ spin liquids in three dimensions with time-reversal symmetry. We find a total of 7 families of such $U(1)$ spin liquids, distinguished by the properties of their emergent electric/magnetic charges. We show how these spin liquids are related to each other. Two of these classes admit nontrivial protected surface states which we describe. We show how to access all of the 7 spin liquids through slave particle (parton) constructions. We also provide intuitive loop gas descriptions of their ground state wave functions. One of these phases is the `topological Mott insulator' conventionally described as a topological insulator of an emergent fermionic `spinon'. We show that this phase admits a remarkable dual description as a topological insulator of emergent fermionic magnetic monopoles. This results in a new (possibly natural) surface phase for the topological Mott insulator and a new slave particle construction. We describe some of the continuous quantum phase transitions between the different $U(1)$ spin liquids. Each of these seven families of states admits a finer distinction in terms of their surface properties which we determine by combining these spin liquids with symmetry protected topological phases. We discuss lessons for materials such as pyrochlore quantum spin ices which may harbor a $U(1)$ spin liquid. We suggest the topological Mott insulator as a possible ground state in some range of parameters for the quantum spin ice Hamiltonian.

Highlights

  • There has been much recent interest in quantum spin liquid phases of systems of interacting magnetic moments

  • This is enabled by recent advances in our understanding of symmetry-protected topological (SPT) phases of bosons or fermions with global Uð1Þ and time-reversal symmetries

  • (3) The conventional description of the ðEfTMfÞθ is that it is a topological insulator formed by emergent fermionic Kramers doublet spinons that are coupled to the Uð1Þ gauge field as an electric charge

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Summary

Introduction

There has been much recent interest in quantum spin liquid phases of systems of interacting magnetic moments These phases are fascinating examples of ground states characterized by long-range quantum entanglement: The corresponding wave functions cannot be smoothly deformed into a product state of local degrees of freedom. We are concerned with a particular class of three-dimensional quantum spin liquids that supports an emergent gapless “photon” as an excitation. It has long been recognized [1,2] that such a photon may be an emergent excitation of some underlying physical quantum many-body system with short-range interactions.

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