Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise

doi:10.1088/1674-1056/a67e9c

中国物理B ›› 2020, Vol. 29 ›› Issue (5): 57305-057305.doi: 10.1088/1674-1056/a67e9c

• CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES • 上一篇下一篇

Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise

Xiong Xu(许雄), Mao-Fa Fang(方卯发)

Synergetic Innovation Center for Quantum Effects and Applications, Key Laboratory of Low-dimensional Quantum Structures and Quantum Control of Ministry of Education, School of Physics and Electronics, Hunan Normal University, Changsha 410081, China

收稿日期:2020-02-05 修回日期:2020-03-03 出版日期:2020-05-05 发布日期:2020-05-05
通讯作者: Mao-Fa Fang E-mail:mffang@hunnu.edu.cn
基金资助:
Project supported by the National Natural Science Foundation of China (Grant No. 11374096).

Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise

Xiong Xu(许雄), Mao-Fa Fang(方卯发)

Synergetic Innovation Center for Quantum Effects and Applications, Key Laboratory of Low-dimensional Quantum Structures and Quantum Control of Ministry of Education, School of Physics and Electronics, Hunan Normal University, Changsha 410081, China

Received:2020-02-05 Revised:2020-03-03 Online:2020-05-05 Published:2020-05-05
Contact: Mao-Fa Fang E-mail:mffang@hunnu.edu.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant No. 11374096).

摘要/Abstract

摘要： We study the dynamics of the entropic uncertainty for three types of three-level atomic systems coupled to an environment modeled by random matrices. The results show that the entropic uncertainty in the Ξ-type atomic system is lower than that in the V-type atomic system which is exactly the same as that in the Λ-type atomic system. In addition, the effect of relative coupling strength on entropic uncertainty is opposite in Markov region and non-Markov region, and the influence of a common environment and independent environments in Markov region and non-Markov region is also opposite. One can reduce the entropic uncertainty by decreasing relative coupling strength or placing the system in two separate environments in the Markov case. In the non-Markov case, the entropic uncertainty can be reduced by increasing the relative coupling strength or by placing the system in a common environment.

关键词: entropic uncertainty, three-level atom, random telegraph noise

Abstract: We study the dynamics of the entropic uncertainty for three types of three-level atomic systems coupled to an environment modeled by random matrices. The results show that the entropic uncertainty in the Ξ-type atomic system is lower than that in the V-type atomic system which is exactly the same as that in the Λ-type atomic system. In addition, the effect of relative coupling strength on entropic uncertainty is opposite in Markov region and non-Markov region, and the influence of a common environment and independent environments in Markov region and non-Markov region is also opposite. One can reduce the entropic uncertainty by decreasing relative coupling strength or placing the system in two separate environments in the Markov case. In the non-Markov case, the entropic uncertainty can be reduced by increasing the relative coupling strength or by placing the system in a common environment.

Key words: entropic uncertainty, three-level atom, random telegraph noise

中图分类号: (Quantum wires)

73.63.Nm

03.67.Hk (Quantum communication) 03.65.Ud (Entanglement and quantum nonlocality) 85.35.Be (Quantum well devices (quantum dots, quantum wires, etc.))

许雄, 方卯发. Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise[J]. 中国物理B, 2020, 29(5): 57305-057305.

Xiong Xu(许雄), Mao-Fa Fang(方卯发). Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise[J]. Chin. Phys. B, 2020, 29(5): 57305-057305.

参考文献 40

[1]	Heisenberg W 1927 Z. Phys. 43 172 doi: 10.1007/BF01397280
[2]	Robertson H P 1929 Phys. Rev. 34 163 doi: 10.1103/PhysRev.34.163
[3]	Maassen H and Uffink J 1988 Phys. Rev. Lett. 60 1103 doi: 10.1103/PhysRevLett.60.1103
[4]	Renes J and Boileau J 2008 Phys. Rev. A 78 032335 doi: 10.1103/PhysRevA.78.032335
[5]	Renes J and Boileau J 2009 Phys. Rev. Lett. 103 020402 doi: 10.1103/PhysRevLett.103.020402
[6]	Berta M, Christandl M, Colbeck R, Renes J M and Renner R 2010 Nat. Phys. 6 659 doi: 10.1038/nphys1734
[7]	Li C F, Xu J S, Xu X Y, Li K and Guo G C 2011 Nat. Phys. 7 752 doi: 10.1038/nphys2047
[8]	Nataf P, Dogan M and Hur K L 2012 Phys. Rev. A 86 043807 doi: 10.1103/PhysRevA.86.043807
[9]	Tomamichel M, Lim C C, Gisin N and Renner R 2012 Nat. Commun. 3 634 doi: 10.1038/ncomms1631
[10]	Dupuis F, Fawzi O and Wehner S 2015 IEEE Trans. Inf. Theory 61 1093 doi: 10.1109/TIT.2014.2371464
[11]	Hu M L and Fan H 2013 Phys. Rev. A 87 022314 doi: 10.1103/PhysRevA.87.022314
[12]	Hu M L and Fan H 2013 Phys. Rev. A 88 014105 doi: 10.1103/PhysRevA.88.014105
[13]	Zou H M, Fang M F, Yang B Y, Guo Y N, He W and Zhang S Y 2014 Phys. Scr. 89 115101 doi: 10.1088/0031-8949/89/11/115101
[14]	Coles P J and Piani M 2014 Phys. Rev. A 89 010302 doi: 10.1103/PhysRevA.89.010302
[15]	Hall M and Wiseman H 2012 New J. Phys. 14 033040 doi: 10.1088/1367-2630/14/3/033040
[16]	Prevedel R, Hamel D R, Colbeck R, Fisher K and Resch K J 2011 Nat. Phys. 7 757 doi: 10.1038/nphys2048
[17]	Hu M and Fan H 2012 Phys. Rev. A 86 032338 doi: 10.1103/PhysRevA.86.032338
[18]	Zhang Y, Fang M, Kang G and Zhou Q 2018 Quantum Inf. Process. 17 172 doi: 10.1007/s11128-018-1939-1
[19]	Xu Z Y, Yang W L and Feng M 2012 Phys. Rev. A 86 012113 doi: 10.1103/PhysRevA.86.012113
[20]	Ming F, Wang D, Shi W N, Huang A J, Sun W Y and Ye L 2018 Quantum Inf. Process. 17 89 doi: 10.1007/s11128-018-1857-2
[21]	Huang A J, Wang D, Wang J M, Shi J D, Sun W Y and Ye L 2017 Quantum Inf. Process. 16 204 doi: 10.1007/s11128-017-1657-0
[22]	Feng J, Zhang Y Z, Gould M D and Fan H 2013 Phys. Lett. B 726 527 doi: 10.1016/j.physletb.2013.08.069
[23]	Jia L J, Tian Z H and Jing J L 2015 Ann. Phys. 353 37 doi: 10.1016/j.aop.2014.10.019
[24]	Zheng X and Zhang G F 2016 Quantum Inf. Process. 16 1
[25]	Guo Y N, Fang M F and Zeng K 2018 Quantum Inf. Process. 17 187 doi: 10.1007/s11128-018-1945-3
[26]	Guo Y N, Fang M F, Tian Q L, Li Z D and Zeng K 2018 Laser Phys. Lett. 15 105205 doi: 10.1088/1612-202X/aadaa3
[27]	Mair A, Vaziri A, Weihs G and Zeilinger A 2001 Nature 412 313 doi: 10.1038/35085529
[28]	Fickler R, Lapkiewicz R, Huber M, Lavery M P, Padgett M J and Zeilinger A 2014 Nat. Commun. 5 4502 doi: 10.1038/ncomms5502
[29]	Molina-Terriza G, Vaziri A, Ursin R and Zeilinger A 2005 Phys. Rev. Lett. 94 040501 doi: 10.1103/PhysRevLett.94.040501
[30]	Inoue R, Yonehara T, Miyamoto Y, Koashi M and Kozuma M 2009 Phys. Rev. Lett. 103 110503 doi: 10.1103/PhysRevLett.103.110503
[31]	Walborn S P, Lemelle D S, Almeida M P and Ribeiro P H S 2006 Phys. Rev. Lett. 96 090501 doi: 10.1103/PhysRevLett.96.090501
[32]	Galperin Y M, Altshuler B L, Bergli J, and Shantsev D V 2006 Phys. Rev. Lett. 96 097009 doi: 10.1103/PhysRevLett.96.097009
[33]	Abel B and Marquardt F 2008 Phys. Rev. B 78 201302 doi: 10.1103/PhysRevB.78.201302
[34]	Joynt R, Zhou D and Wang Q H 2011 Int. J. Mod. Phys. B 25 2115 doi: 10.1142/S0217979211100990
[35]	Rossi M A C and Paris M G A 2016 J. Chem. Phys. 144 024113 doi: 10.1063/1.4939733
[36]	Benedetti C, Buscemi F, Bordone P and Paris M G A 2013 Phys. Rev. A 87 052328 doi: 10.1103/PhysRevA.87.052328
[37]	Paladino E, Galperin Y M, Falci G and Altshuler B L 2014 Rev. Mod. Phys. 86 361 doi: 10.1103/RevModPhys.86.361
[38]	Carrera M, Gorin T and Pineda C 2019 Phys. Rev. A 100 042322 doi: 10.1103/PhysRevA.100.042322
[39]	Arthur T T, Martin T and Fai L C 2017 Int. J. Quantum Inf. 15 1750047 doi: 10.1142/S0219749917500472
[40]	Arthur T T, Martin T and Fai L C 2018 Quantum Inf. Process. 17 37 doi: 10.1007/s11128-017-1800-y

Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise

Dynamics of entropic uncertainty for three types of three-level atomic systems under the random telegraph noise

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