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Quantum channels and representation theory

In the study of d -dimensional quantum channels ( d ⩾ 2 ) , an assumption which includes many interesting examples, and which has a natural physical interpretation, is that the corresponding Kraus operators form a representation of a Lie algebra. Physically, this is a symmetry algebra for the intera...

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Bibliographic Details
Published in:Journal of mathematical physics 2005-08, Vol.46 (8), p.082103-082103-22
Main Author: Ritter, William Gordon
Format: Article
Language:English
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Summary:In the study of d -dimensional quantum channels ( d ⩾ 2 ) , an assumption which includes many interesting examples, and which has a natural physical interpretation, is that the corresponding Kraus operators form a representation of a Lie algebra. Physically, this is a symmetry algebra for the interaction Hamiltonian. This paper begins a systematic study of channels defined by representations; the famous Werner-Holevo channel is one element of this infinite class. We show that the channel derived from the defining representation of su ( n ) is a depolarizing channel for all n , but for most other representations this is not the case. Since the standard Bloch sphere only exists for the qubit representation of su ( 2 ) , we develop a consistent generalization of Bloch’s technique. By representing the density matrix as a polynomial in Lie algebra generators, we determine a class of positive semidefinite matrices which represent quantum states for various channels defined by finite-dimensional representations of semisimple Lie algebras. We also give a general method for finding positive semidefinite matrices using Lie algebraic trace identities. This includes an analysis of channels based on the exceptional Lie algebra g 2 and the Clifford algebra.
ISSN:0022-2488
1089-7658
DOI:10.1063/1.1945768