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Completely positive maps and passive...
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Pasieka, Aron.
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Completely positive maps and passive quantum error correction.
紀錄類型:
書目-語言資料,印刷品 : Monograph/item
正題名/作者:
Completely positive maps and passive quantum error correction./
作者:
Pasieka, Aron.
面頁冊數:
88 p.
附註:
Source: Masters Abstracts International, Volume: 46-03, page: 1554.
Contained By:
Masters Abstracts International46-03.
標題:
Physics, Theory. -
電子資源:
http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=MR33899
ISBN:
9780494338995
Completely positive maps and passive quantum error correction.
Pasieka, Aron.
Completely positive maps and passive quantum error correction.
- 88 p.
Source: Masters Abstracts International, Volume: 46-03, page: 1554.
Thesis (M.Sc.)--University of Guelph (Canada), 2007.
We begin with an examination of the assumptions made in the theory of passive quantum error correction. Physical motivation is discussed for the use of completely positive trace-preserving maps as a description of the evolution of quantum systems. The Lindblad master equation is presented as an example of the dynamics of a system thusly described, in the case of a Markovian system.
ISBN: 9780494338995Subjects--Topical Terms:
1019422
Physics, Theory.
Completely positive maps and passive quantum error correction.
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Completely positive maps and passive quantum error correction.
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Source: Masters Abstracts International, Volume: 46-03, page: 1554.
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We begin with an examination of the assumptions made in the theory of passive quantum error correction. Physical motivation is discussed for the use of completely positive trace-preserving maps as a description of the evolution of quantum systems. The Lindblad master equation is presented as an example of the dynamics of a system thusly described, in the case of a Markovian system.
520
$a
We review noiseless subsystems and decoherence-free subspaces. Building on the generalization of the noiseless subsystem approach, we discuss recent results that provide a robust procedure for finding noiseless subsystems, given a specific, not necessarily unital, channel.
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Unitarily correctable subsystems are introduced, which form a type of active quantum error correction that does not require a measurement. The key result for these systems is that we can apply our procedure for finding noiseless subsystems to find unitarily correctable subsystems, in the case of a unital noise model.
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