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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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Published in: | Journal of mathematical physics 2005-08, Vol.46 (8), p.082103-082103-22 |
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Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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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. |
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ISSN: | 0022-2488 1089-7658 |
DOI: | 10.1063/1.1945768 |