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Mocking up a Dephasing Channel with a Minimal-Sized Environment |
WU Zhen** |
State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071 Graduate School of the Chinese Academy of Sciences, Beijing 100049 |
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Cite this article: |
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Abstract In order to model the most general quantum operation on a d-dimensional system, a d2-dimensional environment is usually needed. We focus on the quantum dephasing process and find that this channel can be modeled by an environment with the size of at most d dimensions. An experimentally accessible matrix D is defined to characterize the dephasing channel and the minimal number of Kraus operators of the channel from the matrix D for mocking up the dephasing channel is presented in the minimal-sized environment. An experimental simulation of dephasing channels by means of nuclear magnetic resonance techniques is carried out to justify the idea.
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Received: 29 May 2012
Published: 31 July 2012
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PACS: |
03.65.Yz
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(Decoherence; open systems; quantum statistical methods)
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03.67.Ac
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(Quantum algorithms, protocols, and simulations)
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03.65.Wj
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(State reconstruction, quantum tomography)
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03.67.Lx
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(Quantum computation architectures and implementations)
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[1] Nielsen M A and Chuang I L 2000 Quantum Computation and Quantum Information (Cambridge: Cambridge University Press) p 360 [2] Hwang B and Goan H S 2012 Phys. Rev. A 85 032321 [3] Karasik R I and Wiseman H M 2011 Phys. Rev. Lett. 106 20406 [4] Müller M, Hammerer K, Zhou Y L, Roos C F and Zoller P 2011 New J. Phys. 13 085007 [5] Lloyd S 1996 Science 273 1073 [6] Narang G and Arvind 2007 Phys. Rev. A 75 032305 [7] If the initial state of the environment is prepared in some mixed state, the size of the environment can be further reduced. However, for simplicity of our discussion, we only consider the minimal-sized environment initialized in a pure state. [8] Havel T F, Sharf Y, Viola L and Cory D G 2001 Phys. Lett. A 280 282 [9] Branderhorst M P A, Nunn J, Walmsley I A and Kosut R L 2009 New J. Phys. 11 115010 [10] Horn R A and Johnson C R 1994 Topics in Matrix Analysis (Cambridge: Cambridge University Press) p 73 [11] Gentle J E 1998 Numerical Linear Algebra for Applications in Statistics (Berlin: Springer) p 93 [12] Cory D G, Fahmy A F and Havel T F 1997 Proc. Natl. Acad. Sci. USA 94 1634 [13] Ollivier H and Zurek W H 2001 Phys. Rev. Lett. 88 017901 [14] This conclusion can be deduced by direct calculation with the unital condition ∑kEkEk? =Is for the phase damping channel. [15] Samal J R, Gupta M, Panigrahi P K and Kumar A 2010 J. Phys. B 43 095508 [16] Lee J S 2002 Phys. Lett. A 305 349 [17] Long G L, Yan H Y and Sun Y 2001 J. Opt. B: Quantum Semiclass. Opt. 3 376 [18] Levitt M H 2010 Spin Dynamics (Chichester: John Wiley & Sons) p 405 [19] Wu Z, Li J, Zheng W, Luo J, Feng M and Peng X 2011 Phys. Rev. A 84 042312 |
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