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二值噪声激励下欠阻尼周期势系统的随机共振
引用本文:马正木,靳艳飞. 二值噪声激励下欠阻尼周期势系统的随机共振[J]. 物理学报, 2015, 64(24): 240502-240502. DOI: 10.7498/aps.64.240502
作者姓名:马正木  靳艳飞
作者单位:北京理工大学宇航学院, 北京 100081
基金项目:国家自然科学基金(批准号: 11272051)资助的课题.
摘    要:研究了二值噪声和周期信号共同激励下欠阻尼周期势系统的随机共振. 利用随机能量法计算了系统的平均输入能量和平均输出信号的振幅和相位差, 讨论了二值噪声对随机共振的影响. 发现随着噪声强度的增大, 平均输入能量曲线存在一个极小值和一个极大值, 系统出现先抑制后共振的现象; 同时, 系统信噪比曲线随噪声强度的增加出现单峰现象, 说明系统存在随机共振现象.

关 键 词:周期势系统  二值噪声  随机共振  随机能量法
收稿时间:2015-07-23

Stochastic resonance in periodic potential driven by dichotomous noise
Ma Zheng-Mu,Jin Yan-Fei. Stochastic resonance in periodic potential driven by dichotomous noise[J]. Acta Physica Sinica, 2015, 64(24): 240502-240502. DOI: 10.7498/aps.64.240502
Authors:Ma Zheng-Mu  Jin Yan-Fei
Affiliation:School of Aerospace Engineering, Beijing Institute of Technology, Beijing 100081, China
Abstract:Periodic potential system is widely used in a lot of areas such as biological ratchet model of motor, Josephson junction in the field of physics, engineering mechanics of the damping pendulum model, etc. Meanwhile, in the study of stochastic resonance, noise is crucial for dynamical system evolution. There are mostly colored Gaussian noises with nonzero correlation times in practical problems. Dichotomous noises belong to the color noises, and they have some simple statistical properties. In this paper, we study the motion of a Brownian particle in a periodic potential, driven by both a periodic signal and a dichotomous noise. The periodic potential system is different from the bistable system, so we use multiple indexes to explain the stochastic resonance. We calculate the average input energy of the system and the average output signal amplitude and phase difference by using stochastic energetics. Then we discuss the influences of the dichotomous noise intensity, noise correlation time and asymmetric coefficient of potential energy on the stochastic resonance. The results show that with the increase of the noise correlation time, a minimum value and a maximum value occur on the curve of the average input energy, meanwhile, the phenomenon of resonance appears in the system. With the increase of the noise intensity, the value of noise correlation time becomes greater when the phenomenon of stochastic resonance appears. Therefore, the region of stochastic resonance becomes bigger as the noise intensity or the asymmetry coefficient increases. Moreover, with the increase of the noise intensity, a mono peak is found for the signal-to-noise ratio (SNR) of the system and the stochastic resonance appears in this system. With the increase of the noise intensity, we compare the change of the SNR, the average input energy, and the average output signal amplitude. We find that the values of the amplitudes of the average output signal and SNR are basically the same, while the values of the amplitude of the average input energy of the system are a little different. This is because during the process of periodic signal doing work to the system, noise does work and passive dissipation energy of the system occures. In addition, when the curves of the amplitude of the average output signal and SNR reach their corresponding minimum values, the phase difference between the output signal and input signal is minimal.
Keywords:periodic potential  dichotomous noise  stochastic resonance  stochastic energetics
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