The Quantum Double Model with Boundary: Condensations and Symmetries

Associated to every finite group, Kitaev has defined the quantum double model for every orientable surface without boundary. In this paper, we define boundaries for this model and characterize condensations; that is, we find all quasi-particle excitations (anyons) which disappear when they move to t...

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Bibliographic Details
Main Authors: Beigi, Salman (Author), Shor, Peter W. (Contributor), Whalen, Daniel (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Mathematics (Contributor)
Format: Article
Language:English
Published: Springer-Verlag, 2012-07-17T19:43:23Z.
Subjects:
Online Access:Get fulltext
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100 1 0 |a Beigi, Salman  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Mathematics  |e contributor 
100 1 0 |a Shor, Peter W.  |e contributor 
100 1 0 |a Shor, Peter W.  |e contributor 
100 1 0 |a Whalen, Daniel  |e contributor 
700 1 0 |a Shor, Peter W.  |e author 
700 1 0 |a Whalen, Daniel  |e author 
245 0 0 |a The Quantum Double Model with Boundary: Condensations and Symmetries 
260 |b Springer-Verlag,   |c 2012-07-17T19:43:23Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/71667 
520 |a Associated to every finite group, Kitaev has defined the quantum double model for every orientable surface without boundary. In this paper, we define boundaries for this model and characterize condensations; that is, we find all quasi-particle excitations (anyons) which disappear when they move to the boundary. We then consider two phases of the quantum double model corresponding to two groups with a domain wall between them, and study the tunneling of anyons from one phase to the other. Using this framework we discuss the necessary and sufficient conditions when two different groups give the same anyon types. As an application we show that in the quantum double model for S 3 (the permutation group over three letters) there is a chargeon and a fluxion which are not distinguishable. This group is indeed a special case of groups of the form of the semidirect product of the additive and multiplicative groups of a finite field, for all of which we prove a similar symmetry. 
546 |a en_US 
655 7 |a Article 
773 |t Communications in Mathematical Physics