Deformed quantum double realization of the toric code and beyond

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• 作者：Pramod Padmanabhan ; ^{pramod23phys@gmail.com" class="auth_mail" title="E-mail the corresponding author} ; Juan Pablo Ibieta-Jimenez ^{pibieta@if.usp.br" class="auth_mail" title="E-mail the corresponding author} ; Miguel Jorge Bernabe Ferreira ^{migueljb@if.usp.br" class="auth_mail" title="E-mail the corresponding author} ; Paulo Teotonio-Sobrinho ^{teotonio@if.usp.br" class="auth_mail" title="E-mail the corresponding author}
• 关键词：Exactly solvable lattice models ; Anyons ; Topological order ; Quantum error correction ; Lattice gauge theory
• 刊名：Annals of Physics
• 出版年：2016
• 出版时间：September 2016
• 年：2016
• 卷：372
• 期：Complete
• 页码：238-259
• 全文大小：585 K

文摘

Quantum double models, such as the toric code, can be constructed from transfer matrices of lattice gauge theories with discrete gauge groups and parametrized by the center of the gauge group algebra and its dual. For general choices of these parameters the transfer matrix contains operators acting on links which can also be thought of as perturbations to the quantum double model driving it out of its topological phase and destroying the exact solvability of the quantum double model. We modify these transfer matrices with perturbations and extract exactly solvable models which remain in a quantum phase, thus nullifying the effect of the perturbation. The algebra of the modified vertex and plaquette operators now obey a deformed version of the quantum double algebra. The Abelian cases are shown to be in the quantum double phase whereas the non-Abelian phases are shown to be in a modified phase of the corresponding quantum double phase. These are illustrated with the groups Z_n${\mathbb{Z}}_n$ and S₃$S_3$. The quantum phases are determined by studying the excitations of these systems namely their fusion rules and the statistics. We then go further to construct a transfer matrix which contains the other Z₂${\mathbb{Z}}_2$ phase namely the double semion phase. More generally for other discrete groups these transfer matrices contain the twisted quantum double models. These transfer matrices can be thought of as being obtained by introducing extra parameters into the transfer matrix of lattice gauge theories. These parameters are central elements belonging to the tensor products of the algebra and its dual and are associated to vertices and volumes of the three dimensional lattice. As in the case of the lattice gauge theories we construct the operators creating the excitations in this case and study their braiding and fusion properties.