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首页> 外文期刊>Physica, D. Nonlinear phenomena >Nested mixed-mode oscillations, part II: Experimental and numerical study of a classical Bonhoeffer-van der Pol oscillator
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Nested mixed-mode oscillations, part II: Experimental and numerical study of a classical Bonhoeffer-van der Pol oscillator

机译:嵌套混合模式振荡,第II部分:经典BONHOEFFER-VAN DER POL振荡器的实验性和数值研究

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The dynamics of Bonhoeffer-van der Pol (BVP) oscillators are known to be equivalent to those of the FitzHugh-Nagumo model and have been extensively studied for many years. In a previous work (Inaba and Kousaka, 2020), we discovered nested mixed-mode oscillations (MMOs) generated by a piecewise-smooth driven Bonhoeffer-van der Pol oscillator. In this study, we focus on the MMOs that occur between the 1(s)- and 1(s+1)-generating regions for s = 2 and 3 in a classical BVP oscillator where the nonlinear conductor is expressed as a third-order polynomial function, and we confirm the occurrence of nested mixed-mode oscillation-incrementing bifurcations (MMOIBs) that are at least doubly nested. Simple (un-nested), singly nested, and doubly nested MMOIBs generate [1(s), 1(s+1)xn](n+1), [A(1), B(1)xn], and [A(2), B(2)xn] MMO sequences, respectively, for successive n. A(1) = [1(s), 1(s+1)xm](m+1) and B-1 = [1(s), 1(s+)1x(m+1)](m+2) in the singly nested case for integers m and A(2) = [[1(s), 1(s+1)xl](l+1), [1(s), 1(s+1)x (l + 1)](l+2) x m]((l+2)m+(l+1)) and B-2 = [[1(s), 1(s+1) x l](l+1), [1(s), 1(s+1) x (l + 1)](l+2 x) (m + 1)]((l+2)(m+1)+(l+1)) in the doubly nested case for integers l and m. In particular, we numerically confirm that m = 1 with s = 2 and 3 cases for the singly nested MMOIBs and that l = 1, m = 1 with s = 2 and 3 cases for the doubly nested MMOIBs. We also show that both the simple (un-nested) and nested MMOIB-generated MMOs have asymmetric Farey characteristics. In addition, we find that these numerical results are well-explained by effectively one-dimensional (1D) Poincare return maps derived numerically from the dynamics of a constrained driven BVP oscillator that includes a diode with grazing-sliding characteristics. Finally, we verify these numerical results for the classical and constrained BVP oscillators in circuit experiments and derive the first return plots and 1D Poincare return maps based on laboratory measurements. (C) 2020 The Authors. Published by Elsevier B.V.
机译:已知Bonhoeffer-van der Pol(BVP)振荡器的动态相当于Fitzhugh-Nagumo模型的动态,并且已经广泛研究了多年。在以前的工作(Inaba和Kousaka,2020)中,我们发现了由分段光滑的驱动Bonhoeffer-van der Pol振荡器产生的嵌套混合模式振荡(MMOS)。在这项研究中,我们专注于在经典BVP振荡器中为S = 2和3的S = 2和3之间发生的MMO,其中非线性导体表示为三阶多项式函数,我们确认了至少双嵌合的嵌套混合模式振荡递增分叉分叉(MMoIB)的发生。简单(未嵌套),单独嵌套和双嵌套MMoIB生成[1(s),1(s + 1)xn](n + 1),[a(1),b(1)xn]和[ A(2),B(2)XN] MMO序列,用于连续n。 a(1)= [1(s),1(s + 1)xm](m + 1)和b-1 = [1(s),1(s +)1x(m + 1)](m + 2 )在整数m的单嵌套案例中m和(2)= [[1(s),1(s + 1)xl](l + 1),[1(s),1(s + 1)x( L + 1)](1 + 2)XM]((L + 2)M +(L + 1))和B-2 = [[1(S),1(S + 1)XL](L + 1) ,[1(s),1(s + 1)x(l + 1)](l + 2 x)(m + 1)]((l + 2)(m + 1)+(l + 1))在整数l和m的双嵌套案例中。特别是,我们使用S = 2和3例为单独嵌套MMoIB的数字证实M = 1,其中L = 1,M = 1,S = 2和3例嵌套MMoIB。我们还表明,简单(未嵌套)和嵌套MMOIB生成的MMO具有不对称的Farey特征。此外,我们发现这些数值结果是通过有效的一维(1D)Poincare返回地图从由约束驱动的BVP振荡器的动态导出的有效的一维(1D)Poincare返回地图来解释,所述电流的被驱动的BVP振荡器的动态包括具有用于放射滑动特性的二极管。最后,我们在电路实验中验证了经典和约束的BVP振荡器的这些数值结果,并导出了基于实验室测量的第一个返回地块和1D Poincare返回地图。 (c)2020作者。 elsevier b.v出版。

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