基于大偏差理论的随机动力学研究
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朱金杰 1,2,†( ),陈朕 2,3,孔琛 2,4,刘先斌 2,*( )
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The researches on the stochastic dynamics based on the large deviation theory
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ZHU Jinjie 1,2,†( ),CHEN Zhen 2,3,KONG Chen 2,4,LIU Xianbin 2,*( )
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图3. 对称双势阱随机共振示意图. 其中双势阱势能函数为$V\left(\pmb x \right) = x^4/4 - x^2/2$, 由于周期激励的作用, 势能函数将会变为$V\left(\pmb x \right) = V\left(\pmb x \right) - Ax\sin \left( {\varOmega t} \right)$, $A$为周期激励幅值, $\varOmega $为其频率, $\Delta V$为势阱深度
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