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When using the noise of n-order time derivative as an internal thermal noise to drive a generalized Langevin equation, if the nonergodicty strength of the noise satisfies b ≠ 0 and the system is in thermal equilibrium, then the stationary velocity variable of the system can be used as a non-ergodic noise. The spectra of the non-ergodic noise is infinite at zero frequency. The one-dimensional semi-unbounded coupled harmonic oscillator chains connected with the gas molecules act as the non-ergodic noise, which is an example of non-ergodic noise. Finally regarding the non-ergodic noise as an external noise to drive the particles in the titled periodic potential, it is found that there appears superballistic diffusion with the effective diffusion index exceeding a ballistic value of 2. It is also found that the velocity distribution of the system displays two motion states, the “locked state” and the “running state”. And in the “running state” there occurs a bimodal phenomenon, which is a relatively new phenomenon.
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Keywords:
- non-ergodic noise /
- the noise of n-order time derivative /
- the spectra of the noise /
- superballistic diffusion
[1] Bao J D 2009 Random Simulation Method of Classical and Quantum Dissipation System (Beijing: Science Press) p80 (in Chinese) [包景东 2009 经典和量子耗散系统的随机模拟方法 (北京: 科学出版社) 第80页]
[2] Saubamea B, Leduc M, Cohen-Tannoudji C 1999 Phys. Rev. Lett. 83 3796
[3] Brokmann X, Hermier J P, Messin G, Deebiolles P, Bouchard J P, Dahan M 2003 Phys. Rev. Lett. 90 120601
[4] Bao J D, Zhou Y Z 2003 Phys. Rev. Lett. 91 138104
[5] Bao J D, Bai Z W 2005 Chin. Phys. Lett. 22 1845
[6] Leggett A J 1980 Theor. Phys. Suppl. 69 80
[7] Lu H, Qin L, Bao J D 2009 Acta Phys. Sin. 58 8127 (in Chinese) [卢宏, 覃莉, 包景东 2009 58 8127]
[8] Lu H, Bao J D 2013 Chin. Phys. Lett. 30 010502
[9] Reimann P 2002 Phys. Rep. 361 57
[10] Moreira A A, Luís A, Amaral N 2005 Phys. Rev. Lett. 94 218702
[11] Bai Z W, Meng G Q 2008 Acta Phys. Sin. 57 7477 (in Chinese) [白占武, 蒙高庆 2008 57 7477]
[12] Bao J D, Hänggi P, Zhou Y Z 2005 Phys. Rev. E 72 061107
[13] Bao J D, Song Y L, Zhou Y Z 2005 Phys. Rev. E 72 011113
[14] Ford G W, Kac M, Mazur P 1965 J. Math. Phys. 6 504
[15] Ford G W, Lewis J T, O'Connell R F 1988 J. Stat. Phys. 53 439
[16] Ford G W, Lewis J T, O'Connell R F 1988 Phys. Rev. A 37 4419
[17] Rosa J, Beims M W 2008 Phys. Rev. E 78 031126
[18] Zwanzig R W 1960 J. Chem. Phys. 32 1173
[19] Weiss U 1999 Quantum Dissipative Systems (2nd Ed.) (Singapore: World Scientific)
[20] L K, Bao J D 2007 Phys. Rev. E 76 061119
[21] Bao J D, Liu J 2013 Phys. Rev. E 88 022153
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[1] Bao J D 2009 Random Simulation Method of Classical and Quantum Dissipation System (Beijing: Science Press) p80 (in Chinese) [包景东 2009 经典和量子耗散系统的随机模拟方法 (北京: 科学出版社) 第80页]
[2] Saubamea B, Leduc M, Cohen-Tannoudji C 1999 Phys. Rev. Lett. 83 3796
[3] Brokmann X, Hermier J P, Messin G, Deebiolles P, Bouchard J P, Dahan M 2003 Phys. Rev. Lett. 90 120601
[4] Bao J D, Zhou Y Z 2003 Phys. Rev. Lett. 91 138104
[5] Bao J D, Bai Z W 2005 Chin. Phys. Lett. 22 1845
[6] Leggett A J 1980 Theor. Phys. Suppl. 69 80
[7] Lu H, Qin L, Bao J D 2009 Acta Phys. Sin. 58 8127 (in Chinese) [卢宏, 覃莉, 包景东 2009 58 8127]
[8] Lu H, Bao J D 2013 Chin. Phys. Lett. 30 010502
[9] Reimann P 2002 Phys. Rep. 361 57
[10] Moreira A A, Luís A, Amaral N 2005 Phys. Rev. Lett. 94 218702
[11] Bai Z W, Meng G Q 2008 Acta Phys. Sin. 57 7477 (in Chinese) [白占武, 蒙高庆 2008 57 7477]
[12] Bao J D, Hänggi P, Zhou Y Z 2005 Phys. Rev. E 72 061107
[13] Bao J D, Song Y L, Zhou Y Z 2005 Phys. Rev. E 72 011113
[14] Ford G W, Kac M, Mazur P 1965 J. Math. Phys. 6 504
[15] Ford G W, Lewis J T, O'Connell R F 1988 J. Stat. Phys. 53 439
[16] Ford G W, Lewis J T, O'Connell R F 1988 Phys. Rev. A 37 4419
[17] Rosa J, Beims M W 2008 Phys. Rev. E 78 031126
[18] Zwanzig R W 1960 J. Chem. Phys. 32 1173
[19] Weiss U 1999 Quantum Dissipative Systems (2nd Ed.) (Singapore: World Scientific)
[20] L K, Bao J D 2007 Phys. Rev. E 76 061119
[21] Bao J D, Liu J 2013 Phys. Rev. E 88 022153
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