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推导出一个关于X结构密度矩阵的量子失协表达式.在单一激发下,给出两个非耦合的量子比特分别与库相互作用构成系统的动力学的精确解,用非马尔科夫主方程方法精确求解了这个系统的耗散动力学.在失谐光谱密度下,讨论和比较不同耦合区域内系统的量子失协动力学特征.结果表明:量子失协表达式适用于任意有X型密度矩阵的物理系统,在失谐光谱密度下,证实两类主方程分别适用于不同的耦合区域.这将为以后更加简便地计算量子失协,以及在不同的耦合区域运用哪一类主方程提供一定的参考依据.

参考文献

[1] Nielsen M A,Chuang Ⅱ.Quantum Computation and Quantum Information[M].England:Cambridge University Press,2006:500-522.
[2] Ma Ganglong,Zha Xinwei.Probabilistic teleportation of four particles W state[J].Chinese Journal of Quantum Electronics (量子电子学报),2010,27(3):308-313 (in Chinese).
[3] Wang Qiong,Liao Jieqian,Zeng Haosheng.Quntum thermal discord in a two-spin-1/2 XXZ model[J].Chin.Phys.B,2010,19(10):100311.
[4] Pan Guixia.Quantum information splitting of arbitrary two-particle state using two GHZ states[J].Chinese Journal of Quantum Electronics (量子电子学报),2010,27(5):573-579 (in Chinese).
[5] Zhang Caihua,Sachuerfu,Gerele.Quantum entanglement in a system of squeezed coherent state light field interacting with two entanglement atoms[J].Chinese Journal of Quantum Electronics (量子电子学报),2010,27(1):57-62 (in Chinese).
[6] Ollivier H,Zurek W H.Quantum discord:A measure of the quantumness of correlation[J].Phys.Rev.Lett.,2001,88(1):017901.
[7] Ji Yinghua,Xu Lin.Entanglement decohernce of coupled superconductor qubits entangled states in nonMarkovian environment[J].Chinese Journal of Quantum Electronics (量子电子学报),2011,28(1):58-64 (in Chinese).
[8] Luo Shunlong.Quantum discord for two-qubit systems[J].Phys.Rev.A,2008,77(4):042303.
[9] Jin Xianmin,R(o)ch Jügen,Yin Juan,et al.Experimental non-local generation of entanglement from independent sources[J].Chin.Phys.Lett.,2009,26(7):070302.
[10] Song Shijie.Maximal violation of Bell inequality and for Werner state[J].Journal of University of Jinan (济南大学报),2011,25(1):0094-0099 (in Chinese).
[11] Werlang T,Souza S,Fanchini F F,et al.Robustness of quantum discord to sudden death[J].Phys.Rev.A,2009,80(2):024103.
[12] Zhang Jian,Shao Bin,Zou Jian.Entanglement of two atoms in two-mode Roman coupled model with intrinsic decoherence[J].Chin.Phys.B,2009,18(12):5179-518g.
[13] Wang Lincheng,Shen jian,Yi Xuexi.Discord under the influence of a quantum phase transition[J].Chin.Phys.B,2011,20(5):050306.
[14] Modi K,Paterek T,Son W,et al.Unified view of quantum and classical correlations[J].Phys.Rev.Lett.,2010,104(8):080501.
[15] Dillenschueiider R,Lutz E.Energetics of quantum correlation[J].Europe Phys.Lett.,2009,88(5):50003.
[16] Satandy M S.Classical correlation and quantum discord in critical systems[J].Phys.Rev.A,2009,80(2):022108.
[17] Cui J,Fan H.Correlation in the Grover search[J].J.Phys.A:Math.Theor.,2009,43(4):045305.
[18] Werlang T,Sonza S,Fanchin F F,et al.Robustness of quantum discord to sudden death[J].Phys.Rev.A,2009,80(2):024103.
[19] Wang B,Xu Z Y,Chen Z Q,et al.Non-Markovian effect on the quantum discord[J].Phys.Rev.A,2010,81(1):014101.
[20] Fanchini F F,Werlang T,Brasil C A,et al.Non-Markovian dynamics of quantum discord[J].Phys.Rev.A,2010,81(5):052107.
[21] Nakajima S.On quantum theory of transport phenomena[J].Prog.Theor.Phys.,1958,20(6):948-959.
[22] Zwanzig R.Ensemble method in the theory of irreversibility[J].J.Chem.Phys.,1960,33(5):1338-1341.
[23] Chaturvedi S,Shibata F.Time-convolutionless projection operator formalism for elimination of fast variable application to Brownian motion[J].Z.Phys.,1979,35(3):297-308.
[24] Breuer H P,Petruccione F.Theory of Open Quantum Systems[M].Oxford University Press,2002:466-468.
[25] Zhou Ling,Yi Xuexi,Song Heshan,et al.Thermai entanglement in 1D optical lattice chains with nonlinear coupling[J].Chin.Phys.B,2005,14(6):1168-1174.
[26] Ferraro E,Scala M,Miqliore R,et al.Non-Markovian dissipative dynamics of two coupled qubits in independent reservoirs:comparison between exact solutions and master equation approaches[J].Phys.Rev.A,2009,80(4):042112.
[27] Ferraro E,Scala M,Migliore R,et al.On the validity of non-Markovian master equation approaches for the entanglement dynamics of two-qubit systems[J].Phys.Scr.,2010,T140:014042.
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