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1.
The mean first-passage time of a bistable system with time-delayed feedback driven by multiplicative non-Gaussian noise and additive Gaussian white noise is investigated. Firstly, the non-Markov process is reduced to the Markov process through a path-integral approach; Secondly, the approximate Fokker-Planck equation is obtained by applying the unified coloured noise approximation, the small time delay approximation and the Novikov Theorem. The functional analysis and simplification are employed to obtain the approximate expressions of MFPT. The effects of non-Gaussian parameter (measures deviation from Gaussian character) r, the delay time τ, the noise correlation time τ0, the intensities D and α of noise on the MFPT are discussed. It is found that the escape time could be reduced by increasing the delay time τ, the noise correlation time τ0, or by reducing the intensities D and α. As far as we know, this is the first time to consider the effect of delay time on the mean first-passage time in the stochastic dynamical system.  相似文献   

2.
Applying the method of the unified colored noise approximation and phase lock, we study in this paper the stationary intensity distribution of the single-mode laser driven by colored pump noise with cross-correlation between the real and imaginary parts of the quantum noise. We present a thorough discussion of how the cross-correlation λq between the real and imaginary parts of the quantum noise and the self-correlation time τ of the pump noise determine the behaviors of the stationary distribution Qst(I), the mean (I), and the variance λ2(0) of the laser intensity. It is shown that cross-correlation intensity λq of the complex quantum noise can induce a first-order-like transition. When the pump noise is colored noise (τ≠0), improving the pump parameters monotonously will make the curves of Qst(I) exhibit reentrant phase transition. The fluctuations of laser intensity are strongly influenced by λq and τ when the laser is operated near or below threshold. Especially when τ≠0, the heights of the peaks of the curves of λ2(0)-α0 and α3(0)-α0, (here a0 is the net gain coefficient) go up as λq increases. However the entire curves λ2(0)-α0 and λ3(0)-α0 are abruptly suppressed when λq = 1, in similarity to phase transition of stationary intensity distribution.  相似文献   

3.
研究了由色关联的乘性白噪声和加性白噪声驱动的非对称双稳系统中,色关联及非对称性对平均首次穿越时间的影响.数值结果表明乘性噪声强度α和加性噪声强度D及互相关时间τ对首次穿越时间T的影响是一致的,加性和乘性噪声间的互关联强度λ及势阱的非对称性r对T的影响是一致的.τ的增加能提高粒子的逃逸率,λ的增加则减小逃逸率.  相似文献   

4.
The electronic structure of T*-type compounds (Bi0.5Sr1.5)(Y2-xCex)Cu2Oy has been studied by X-ray photoelectron spectroscopy. From analysis of the results, it was found that cation deficiency in Ce4+ introduced holes to conduction planes in the T* phase as in the p-type infinite layer compounds. Some Cu ions in the sample without cation-deficiency contained two-oxygen coordination, which resulted in the incompleteness of the CuO2 sheets. Bi ions in the T* phase cuprates take exact valence of 3+, Pb ions cannot replace them due to the too large an ionic radius of Pb2+/Pb4+.  相似文献   

5.
杨亚强  王参军 《物理学报》2012,61(12):120507-120507
应用统一色噪声理论研究了双色噪声激励下一维FitzHugh-Nagumo (FHN)神经元系统的动力学性质,即稳态概率分布函数和其平均值. 给出了FHN神经元系统的稳态概率密度和平均值的解析表达式. 结果表明: 乘性噪声的自关联时间τ 1、加性噪声的自关联时间τ 2、加性噪声强度α 和乘性噪声强度D都能够诱导非平衡相变的产生. α和D的增大有利于系统从激发态向静息态转换. τ1, τ2的增大有利于系统从静息态向激发态转换. 噪声强度和其自关联时间的作用完全相反.  相似文献   

6.
We calculate one-loop R-parity-violating coupling corrections to the processes H-→τντ and H-→bt. We find that the corrections to the H-→τντ decay mode are generally about 0.1%, and can be negligible. But the corrections to the H-→bt decay mode can reach a few percent for the favored parameters.  相似文献   

7.
By using the linear approximation method, the intensity correlation function and the intensity correlation time are calculated in a gain-noise model of a single-mode laser driven by colored cross-correlated pump noise and quantum noise, each of which is colored. We detect that, when the cross-correlation between both noises is negative, the behavior of the intensity correlation function C(t) versus time t, in addition to decreasing monotonously, also exhibits several other cases, such as one maximum, one minimum, and two extrema (one maximum and one minimum), i.e., some parameters of the noises can greatly change the dependence of the intensity correlation function upon time. Moreover, we find that there is a minimum Tmin in the curve of the intensity correlation time versus the pump noise intensity, and the depth and position of Train strongly depend on the quantum noise self-correlation time T2 and cross-correlation time T3.  相似文献   

8.
对邻苯二甲酸二甲酯(dimethyl phthalate)、邻苯二甲酸二乙酯(diethyl phthalate)、邻苯二甲酸二丁酯(dibutyl phthalate)和邻苯二甲酸二异辛酯 (dioctyl phthalate)系列材料中, α-弛豫的降温介电谱进行了测量, 得出了相应材料α-弛豫的平均弛豫时间ταa 随温度T的变化关系. 通过ταa 的实验结果与经验的Vogel-Fulcher-Tammann)定律ταa = τα0 exp (A/(T-T0))的拟合, 获得了上述系列材料的τα0, A和T0. 分析发现, 随邻苯二甲酸二甲酯系列分子侧链中碳原子数目n的变化, 材料的τα0, A, T0 和Tg 表现出一定的规律性, 具体为随n的增加, 即分子内部自由度的增多, A和Tg 都表现出近乎相同的先减后再增的趋势, 而1/τα0 和T0 则表现出基本相同的先快速减小, 然后保持基本上不变的趋势. 关键词: 玻璃化转变 介电谱 α-弛豫')" href="#">α-弛豫 邻苯二甲酸二甲酯系列材料  相似文献   

9.
通过水解TiCl4制备了锐钛矿结构TiO2纳米粒子, 并用时间分辨荧光光谱研究了5(6)CFL(5(6)-Carboxyfluorescein, 简称5(6)CFL)染料敏化TiO2纳米粒子体系的光致电子转移动力学. 5(6)CFL染料敏化TiO2纳米粒子能形成电荷转移复合物, 这归因于染料分子的激发电子态波函数Ψ(D*)与电荷分离态波函数Ψ(D+ +e-)之间的耦合作用. 当激发5(6)CFL染料敏化TiO2纳米粒子体系时, 电子以两种不同方式注入TiO2纳米粒子导带: 第一, 通过5(6)CFL染料分子的激发态注入; 第二, 从电荷转移复合物(5(6)CFL/TiO2)直接注入. 时间分辨荧光光谱表明, 在水溶液中纯5(6)CFL染料的荧光以寿命为τ1=41 ps (74.4%) 和τ2=3.22 ns (25.6%) 的双e指数衰减, 而5(6)CFL染料敏化TiO2纳米粒子体系的荧光分别以时间常数为τ1=44 ps (90.4%), τ2=478 ps (8.6%) 和τ3=2.41 ns (1.0%) 的三e指数衰减. 本文的研究工作能够为染料敏化太阳能电池的光致电子转移机理提供有价值的参考.  相似文献   

10.
We have studied the barrier crossing dynamics in presence of non-Gaussian noises. It has been observed that multiplicative colored non-Gaussian noise can induce resonant activation (RA). The conspicuous dependence of mean first passage time (MFPT) on correlation time (τ2τ2) of additive colored noise having fixed variance have been analyzed. Beyond a critical value of τ2τ2 the MFPT increases for a given rate of increase of noise strength with τ2τ2 if the additive colored noise is non-Gaussian. The MFPT first decreases with increase of the non-Gaussian parameter (measures deviation from Gaussian character) of multiplicative colored noise followed by an increase exhibiting a minimum. The appearance of the minimum critically depends on the additive noise.  相似文献   

11.
We study the transition problems in a piecewise nonlinear model induced by correlated multiplicative non-Gaussian noise and additive Gaussian white noise. Firstly, applying the path integral approach, the unified colored noise approximation, the analytical expression of the steady-state probability density function (SPD) is derived. Then the change regulation of the SPD is analyzed with the change of the strength and relevance of multiplicative noise and additive noise. From numerical computations we obtain some new nonlinear phenomena: the transition can be induced by the cross-correlation strength between noises, the non-Gaussian noise intensity and the Gaussian noise intensity as well as the non-Gaussian noise deviation parameter. This indicates that the effect of the non-Gaussian noise intensity on SPD is the same as that of the Gaussian noise intensity. Moreover, we also find the correlation time of the non-Gaussian noise can not induce the transition.  相似文献   

12.
We investigate in detail the effects of R-parity lepton number violation on the decay b1→bχ10 in the R-parity violating minimal supersymmetric standard model (Rp-MSSM) under the present experimental constraints on Rp parameters. In our numerical calculations we consider two cases of input parameters of the squark and slepton sectors, Msquark<Mslepton and Msquark>Mslepton, for comparison. The results show that the relative R-parity violating correction is not very sensitive to the mass of the lightest neutralino χ10 and the degenerate R-parity violating coupling parameter λ2, but strongly depends on Msquark, Mslepton, tan β and the degenerate R-parity violating coupling parameter λ1. The relative correction is about -4~3% and can exceed -6% in some region of parameter space. Therefore, precise experiment analyses on the decay b1→bχ10 may provide a probe of the R-parity violation.  相似文献   

13.
沈杰  周静  石国强  杨文才  刘韩星  陈文 《物理学报》2013,62(11):117702-117702
通过对克劳修斯-莫索蒂方程的近似, 分析了钙钛矿结构微波介质陶瓷频率温度系数 (τf) 的主要影响因素, 发现改变材料介电响应中离子位移极化和电子位移极化的比例, 可调节频率温度系数的正负与大小. 通过电子结构计算和容忍因子分析, 预测引入(Zn1/3Nb2/3)4+对具有正温度系数 的CaTiO3进行B位取代将提高材料电子极化响应比例, 调节τf由正变负. 采用偏铌酸盐为前驱体, 通过固相反应法合成了Ca[(Zn1/3Nb2/3)xTi(1-x)]O3钙钛矿结构陶瓷, 并对其进行结构分析和性能测试, 实验结果与理论分析一致, 获得了具有近零频率温度系数的Ca[(Zn1/3Nb2/3)0.7Ti0.3]O3介质陶瓷材料. 关键词: B位复合钙钛矿陶瓷 谐振频率温度稳定性 极化机理 6八面体倾斜')" href="#">BO6八面体倾斜  相似文献   

14.
The Gaussian wave functional method is applied to a boson system with an array of local nonlinear potentials cos[βφ(nR)] to study the phase diagram of its ground state. The stable ground state is determined by the renormalized mass μ which is a function of the parameter γ=β2/4φ, the strength of potential α and the potential concentration c. In different cases γ<γ1, γ1<γ<γ2 and γ>γ2, μ can have different multiplicities, the phase diagram in parameter space is thus depicted. The value γ=γ1 depends on the concentration c, for c→0, it coincides with that of the single impurity model; while γ2=2 coincides with the conclusion of the continuous model.  相似文献   

15.
The SDIFF(T2)local-generalized Kac-Moody \hat G(T2) symmetry is an infinite-dimensional group on the torus membrane, whose Lie algebra is the semi-direct sum of the SDIFF(T2)local algebra and the generalized Kac-Moody algebra \hat g(T2). In this paper, we construct the linearly realized gauge theory of the SDIFF(T2)local-generalized Kac-Moody \hat G(T2) symmetry.  相似文献   

16.
谢文贤  许鹏飞  蔡力  李东平 《物理学报》2013,62(8):80503-080503
针对具有双指数耗散记忆核函数的两自由度耦合系统, 本文利用Laplace变换导出了热宽带噪声激励下该系统响应二阶矩的解析表达式. 并观察到位移二阶矩不同于单自由度情形下的反常扩散:<x2(t)> ∝ tα (0<α<2, α≠1), 而是随时间及噪声等参数变化呈现普遍的振荡扩散现象.分析可得, 阻尼耦合因子B使粒子远离简谐势场的束缚, <x2(t)>随B的增大扩散加剧而摩擦系数增大却使其趋于平稳状态.进一步, 若两热噪声互关联时, 较小的互关联时间对二阶矩的影响较大, 反之作用较小. 伴随互关联强度递增, 位移二阶矩的扩散加剧, 位移间的相关性加强, 与物理直观相符. 关键词: 热噪声 非马尔可夫扩散 广义朗之万方程 关联性  相似文献   

17.
申雅君  郭永峰  袭蓓 《物理学报》2016,65(12):120501-120501
本文主要研究了关联乘性非高斯噪声和加性高斯白噪声共同激励的FHN(Fitz Hugh-Nagumo)神经元系统.利用路径积分法和统一色噪声近似,推导出该系统的定态概率密度函数表达式.通过研究发现,乘性噪声强度D、加性噪声强度Q、噪声自关联时间τ以及互关联系数λ均可以诱导系统产生非平衡相变现象,而非高斯参数q却不可以诱导系统产生非平衡相变现象.此外,我们还发现参数D和λ的增大有利于神经元系统从激发态向静息态转换,Q和τ的增大有利于神经元系统从静息态向激发态转换,q的增大会使得神经元系统停留在静息态的概率增加.  相似文献   

18.
We have studied the effects of non-Gaussian colored noise in a chemical oscillation system, the well-known Brusselator model, in the parameter region close to the supercritical Hopf bifurcation. With the variation of the parameter q, which quantifies the deviation from Gaussian character, the signal-to-noise ratio of noise induced oscillation exhibits a bell-shaped change, indicating the presence of resonant activity. The cooperative effects of q and the correlation time τ on the performance of noise induced oscillation are also investigated. Interestingly, resonance-like behavior can be induced by either q or τ when the other parameter is properly fixed. Stochastic normal form theory is used to analyze these nontrivial effects and the simulation results are well reproduced. This work provides us comprehensive understanding of how non-Gaussian noise influences the dynamics in chemical oscillation systems.  相似文献   

19.
The colored noise in a single-mode laser with injected signal is investigated by the method of two-dimensional unified colored noise approximation. The normalized correlation function λ2(0), the intensity correlation time Tc and effective eigenvalue λeff are calculated. The effects of the injected signal I0, colored noise strength Pˊ and the noise correlation time τ on the dynamical properties of the single-mode laser are discussed.  相似文献   

20.
张静静  靳艳飞 《物理学报》2011,60(12):120501-120501
研究了乘性非高斯噪声和加性高斯白噪声共同激励下非对称双稳系统的平均首次穿越时间和随机共振问题. 利用路径积分法和两态模型理论,推导出平均首次穿越时间和信噪比的表达式. 研究结果表明:势阱非对称性对两个不同方向的平均首次穿越时间的影响是不同的. 信噪比是加性噪声强度和势阱非对称性的非单调函数,系统出现了随机共振现象;信噪比是乘性噪声强度的单调函数,没有共振峰出现. 这说明该系统中乘性噪声强度和加性噪声强度对信噪比的影响是不同的. 关键词: 非高斯噪声 非对称双稳系统 平均首次穿越时间 随机共振  相似文献   

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