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arXiv:1004.4755 · Communications in Mathematical Physics

On the Extension of Stringlike Localised Sectors in 2+1 Dimensions

Pieter Naaijkens

Published Feb 1, 2011• 3 citations
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Abstract

In the framework of algebraic quantum field theory, we study the category $${\Delta_{{\rm BF}}^{\mathfrak{A}}}$$ of stringlike localised representations of a net of observables $${\mathcal{O} \mapsto \mathfrak{A}(\mathcal{O})}$$ in three dimensions. It is shown that compactly localised (DHR) representations give rise to a non-trivial centre of $${\Delta_{{\rm BF}}^{\mathfrak{A}}}$$ with respect to the braiding. This implies that $${\Delta_{{\rm BF}}^{\mathfrak{A}}}$$ cannot be modular when non-trivial DHR sectors exist. Modular tensor categories, however, are important for topological quantum computing. For this reason, we discuss a method to remove this obstruction to modularity.Indeed, the obstruction can be removed by passing from the observable net $${\mathfrak{A}(\mathcal{O})}$$ to the Doplicher-Roberts field net $${\mathfrak{F}(\mathcal{O})}$$ . It is then shown that sectors of $${\mathfrak{A}}$$ can be extended to sectors of the field net that commute with the action of the corresponding symmetry group. Moreover, all such sectors are extensions of sectors of $${\mathfrak{A}}$$ . Finally, the category $${\Delta_{{\rm BF}}^{\mathfrak{F}}}$$ of sectors of $${\mathfrak{F}}$$ is studied by investigating the relation with the categorical crossed product of $${\Delta_{{\rm BF}}^{\mathfrak{A}}}$$ by the subcategory of DHR representations. Under appropriate conditions, this completely determines the category $${\Delta_{{\rm BF}}^{\mathfrak{F}}}$$ .

DOI
10.1007/s00220-011-1200-6

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In the framework of algebraic quantum field theory, we study the category ΔBFA{\Delta_{{\rm BF}}^{\mathfrak{A}}}ΔBFA​ of stringlike localised representations of a net of observables O↦A(O){\mathcal{O} \mapsto \mathfrak{A}(\mathcal{O})}O↦A(O) in three dimensions. It is shown that compactly localised (DHR) representations give rise to a non-trivial centre of ΔBFA{\Delta_{{\rm BF}}^{\mathfrak{A}}}ΔBFA​ with respect to the braiding. This implies that ΔBFA{\Delta_{{\rm BF}}^{\mathfrak{A}}}ΔBFA​ cannot be modular when non-trivial DHR sectors exist. Modular tensor categories, however, are important for topological quantum computing. For this reason, we discuss a method to remove this obstruction to modularity.Indeed, the obstruction can be removed by passing from the observable net A(O){\mathfrak{A}(\mathcal{O})}A(O) to the Doplicher-Roberts field net F(O){\mathfrak{F}(\mathcal{O})}F(O) . It is then shown that sectors of A{\mathfrak{A}}A can be extended to sectors of the field net that commute with the action of the corresponding symmetry group. Moreover, all such sectors are extensions of sectors of A{\mathfrak{A}}A . Finally, the category ΔBFF{\Delta_{{\rm BF}}^{\mathfrak{F}}}ΔBFF​ of sectors of F{\mathfrak{F}}F is studied by investigating the relation with the categorical crossed product of ΔBFA{\Delta_{{\rm BF}}^{\mathfrak{A}}}ΔBFA​ by the subcategory of DHR representations. Under appropriate conditions, this completely determines the category ΔBFF{\Delta_{{\rm BF}}^{\mathfrak{F}}}ΔBFF​ .
Abstract We study Kitaev’s quantum double model for arbitrary finite gauge group in infinite volume, using an operator-algebraic approach. The quantum double model hosts anyonic excitations which can be identified with equivalence classes of ‘localized and transportable endomorphisms’, which produce anyonic excitations from the ground state. Following the Doplicher–Haag–Roberts (DHR) sector theory from AQFT, we organize these endomorphisms into a braided monoidal category capturing the fusion and braiding properties of the anyons. We show that this category is equivalent to RepfD(G)\textbf{Rep}_f {{\mathcal {D}}}(G)Repf​D(G) Rep f D ( G ) , the representation category of the quantum double of G . This establishes for the first time the full DHR structure for a class of 2d quantum lattice models with non-abelian anyons.
Let A be a local conformal net of factors on S 1 with the split property. We provide a topological construction of soliton representations of the n-fold tensor product A ⊗ · · · ⊗ A, that restrict to true representations of the cyclic orbifold (A ⊗ · · · ⊗ A) Zn. We prove a quantum index theorem for our sectors relating the Jones index to a topological degree. Then A is not completely rational iff the symmetrized tensor product (A ⊗ A) flip has an irreducible representation with infinite index. This implies the following dichotomy: if all irreducible sectors of A have a conjugate sector then either A is completely rational or A has uncountably many different irreducible sectors. Thus A is rational iff A is completely rational. In particular, if the µ-index of A is finite then A turns out to be strongly additive. By [30], if A is rational then the tensor category of representations of A is automatically modular, namely the braiding symmetry is non-degenerate. In interesting cases, we compute the fusion rules of the topological solitons and show that they determine all twisted sectors of the cyclic orbifold.
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Abstract For a G-crossed braided extension of a unitary modular tensor category C\mathcal {C}C C —as in one representing a (2+1)D symmetry enriched topological order (SETO)—preservation of global on-site group symmetry after condensation by a commutative Q-system object A∈CA \in \mathcal {C}A∈C A ∈ C necessitates the existence of a G-equivariant structure on A. When interpreted spatially, the condensation boundary has its own internal topological symmetries. We elaborate an algebraic framework for describing the internal topological symmetries of compatible (1+1)D gapped boundaries for (2+1)D topologically ordered systems in terms of hypergroup actions. Then, we investigate the coherence of global on-site bulk symmetries and boundary symmetries. We present a categorical obstruction to the preservation of symmetry in a way which is coherent in terms of lifts of categorical actions to a certain 2-group of bulk symmetries. We give a characterization of this obstruction in the case of condensation by a Lagrangian algebra and boundary symmetries given by subalgebras of the convolution algebra associated with a Lagrangian algebra object.
We investigate the algebraic theory of symmetry-enriched topological (SET) order in (2+1)D bosonic topological phases of matter and its applications to topological quantum computing. Our goal is twofold: first, to demonstrate how an abstract categorical approach can be applied to understand phenomena in (2+1)D topological phases of matter, and second, to show how ideas from physics can be useful for categorification.After reviewing modular tensor categories (MTCs) and their role as algebraic theories of anyons in topological phases of matter, we recall their associated quantum representations and their interpretation as quantum gates for a topological quantum computer. Next we recall the characterization of SET order in terms of GGG-crossed braided extensions of MTCs and the mathematical formalism of topological quantum computing (TQC) with anyons and symmetry defects.We then apply modular tensor category theory to construct algebraic models of symmetry defects in multi-layer (2+1)D topological order with layer-exchange permutation symmetry. Our main result frames a correspondence between bilayer symmetry enriched topological order and monolayer topological order on surfaces with genus, illuminating a connection between quantum symmetry and topological order that first appeared in the work of condensed matter theorists Barkeshi, Ji, and Qian.
We analyze a class of quantum field theory models illustrating some of the possibilities that have emerged in the general study of the short distance properties of superselection sectors, performed in a previous paper (together with R. Verch). In particular, we show that for each pair (G, N), with G a compact Lie group and N a closed normal subgroup, there is a net of observable algebras which has (a subset of) DHR sectors in 1-1 correspondence with classes of irreducible representations of G, and such that only the sectors corresponding to representations of G/N are preserved in the scaling limit. In the way of achieving this result, we derive sufficient conditions under which the scaling limit of a tensor product theory coincides with the product of the scaling limit theories.