|
|
Population dynamics of excited atoms in non-Markovian environments at zero and finite temperature |
Zou Hong-Mei (邹红梅), Fang Mao-Fa (方卯发) |
Key Laboratory of Low-dimensional Quantum Structures and Quantum Control of Ministry of Education, College of Physics and Information Science, Hunan Normal University, Changsha 410081, China |
|
|
Abstract The population dynamics of a two-atom system, which is in two independent Lorentzian reservoirs or in two independent Ohmic reservoirs respectively, where the reservoirs are at zero temperature or finite temperature, is studied by using the time-convolutionless master-equation method. The influences of the characteristics and temperature of a non-Markovian environment on the population of the excited atoms are analyzed. We find that the population trapping of the excited atoms is related to the characteristics and the temperature of the non-Markovian environment. The results show that, at zero temperature, the two atoms can be effectively trapped in the excited state both in the Lorentzian reservoirs and in the Ohmic reservoirs. At finite temperature, the population of the excited atoms will quickly decay to a nonzero value.
|
Received: 18 January 2015
Revised: 04 March 2015
Accepted manuscript online:
|
PACS:
|
03.65.Yz
|
(Decoherence; open systems; quantum statistical methods)
|
|
42.50.Lc
|
(Quantum fluctuations, quantum noise, and quantum jumps)
|
|
42.50.Pq
|
(Cavity quantum electrodynamics; micromasers)
|
|
Fund: Project supported by the Science and Technology Plan of Hunan Province, China (Grant No. 2010FJ3148) and the National Natural Science Foundation of China (Grant No. 11374096). |
Corresponding Authors:
Zou Hong-Mei
E-mail: zhmzc1997@126.com
|
Cite this article:
Zou Hong-Mei (邹红梅), Fang Mao-Fa (方卯发) Population dynamics of excited atoms in non-Markovian environments at zero and finite temperature 2015 Chin. Phys. B 24 080304
|
[1] |
Yoo H I and Eberly J H 1985 Phys. Rep. 118 239
|
[2] |
Radmore P M 1982 Phys. Rev. A 26 2252
|
[3] |
Deng Z and Eberly J H 1986 Phys. Rev. A 34 2492
|
[4] |
Cirac J I and Sánchez-Soto L L 1990 Phys. Rev. A 42 2851
|
[5] |
Cirac J I and Sánchez-Soto L L 1991 Phys. Rev. A 44 3317
|
[6] |
Agarwal G S 1993 Phys. Rev. Lett. 71 1351
|
[7] |
Bergmann K, Theuer H and Shore B W 1998 Rev. Mod. Phys. 70 1003
|
[8] |
Král P, Thanopulos I and Shapiro M 2007 Rev. Mod. Phys. 79 53
|
[9] |
Fleischhauer M, Imamoglu A and Marangos J P 2005 Rev. Mod. Phys. 77 633
|
[10] |
Lukin M D 2003 Rev. Mod. Phys. 75 457
|
[11] |
Mompart J and Corbalan R 2000 J. Opt. B: Quantum Semiclass. Opt. 2 R7
|
[12] |
Lev B, Srinivasan K, Barclay P, Painter O and Mabuchi H 2004 Nanotechnology 15 S556
|
[13] |
Florescu L, John S, Quang T and Wang R 2004 Phys. Rev. A 69 013816
|
[14] |
Reithmaier J P Seogonk G, Löffler A, et al. 2004 Nature 432 197
|
[15] |
John S and Wang J 1990 Phys. Rev. Lett. 64 2418
|
[16] |
John S and Quang T 1994 Phys. Rev. A 50 1764
|
[17] |
Quang T, Woldeyohannes M, John S and Agarwal G S 1997 Phys. Rev. Lett. 79 5238
|
[18] |
Lambropoulos P, Nikolopoulos G M, Nielsen T R and Sären Bay 2000 Rep. Prog. Phys. 63 455
|
[19] |
Weimer H 2010 Ph.D. Dissertation, University of Stuttgart, Germany
|
[20] |
Saffman M, Waller T and Molmer K 2010 Rev. Mod. Phys. 82 2313, and references therein
|
[21] |
Peyronel T, Firstenberg O, Liang Q Y, et al. 2012 Nature 488 57
|
[22] |
Cao L, Ke P, Qiao L Y and Zheng Z G 2014 Chin. Phys. B 23 070501
|
[23] |
Xiang J D, Qin L G and Tian L J 2014 Chin. Phys. B 23 110305
|
[24] |
Qin W, Wang H Y and Long G L 2014 Chin. Phys. B 23 037502
|
[25] |
Fan Z L, Tian J and Zeng H S 2014 Chin. Phys. B 23 060303
|
[26] |
Liu X and Wu W 2014 Chin. Phys. B 23 070303
|
[27] |
Xie D and Wang A M 2014 Chin. Phys. B 23 040302
|
[28] |
Liu Y, Jin J S, Li J, Li X Q and Yan Y J 2013 Sci. China A: Phys. Mech. Astron. 56 1866
|
[29] |
Guo J L, Li H and Long G L 2013 Quantum Inform. Proc. 12 3421
|
[30] |
Guo Y N, Fang M F, Liu X and Yang B Y 2014 Chin. Phys. B 23 034204
|
[31] |
Wang X Y, Ding B F and Zhao H P 2013 Chin. Phys. B 22 040308
|
[32] |
Lu Y, Feng G R, Li Y S, et al. 2015 Sci. Bull. 60 241
|
[33] |
Xiao X, Fang M F and Li Y L 2010 J. Phys. B: At. Mol. Opt. Phys. 43 185505
|
[34] |
Sinayskiy I, Ferraro E, Napoli A, Messina A and Petruccione F 2009 J. Phys. A: Math. Theor. 42 485301
|
[35] |
Ferraro E, Scala M, Migliore R and Napoli A 2009 Phys. Rev. A 80 042112
|
[36] |
Zou H M, Fang M F, Yang B Y, Guo Y N, He W and Zhang S Y 2014 Phys. Scr. 89 115101
|
[37] |
Breuer H P and Petruccione F 2002 The Theory of Open Quantum Systems (Oxford: Oxford University Press)
|
[38] |
Zou H M, Fang M F and Yang B Y 2013 Chin. Phys. B 22 120303
|
[39] |
Dalton B J, Barnett S M and Garraway B M 2001 Phys. Rev. A 64 053813
|
[40] |
Bellomo B, Franco R Lo and Compagno G 2007 Phys. Rev. Lett. 99 160502
|
[41] |
Bellomo B, Franco R Lo and Compagno G 2008 Phys. Rev. A 77 032342
|
[42] |
Eckel J, Reina J H and Thorwart M 2009 New J. Phys. 11 085001
|
[43] |
Cui W, Xi Z R and Pan Y 2009 J. Phys. A: Math. Theor. 42 155303
|
No Suggested Reading articles found! |
|
|
Viewed |
|
|
|
Full text
|
|
|
|
|
Abstract
|
|
|
|
|
Cited |
|
|
|
|
Altmetric
|
blogs
Facebook pages
Wikipedia page
Google+ users
|
Online attention
Altmetric calculates a score based on the online attention an article receives. Each coloured thread in the circle represents a different type of online attention. The number in the centre is the Altmetric score. Social media and mainstream news media are the main sources that calculate the score. Reference managers such as Mendeley are also tracked but do not contribute to the score. Older articles often score higher because they have had more time to get noticed. To account for this, Altmetric has included the context data for other articles of a similar age.
View more on Altmetrics
|
|
|