An amplitude equation for the conserved-Hopf bifurcation -- derivation, analysis and assessment

Daniel Greve, Uwe Thiele
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Abstract

We employ weakly nonlinear theory to derive an amplitude equation for the conserved-Hopf instability, i.e., a generic large-scale oscillatory instability for systems with two conservation laws. The resulting equation represents the equivalent in the conserved case of the complex Ginzburg-Landau equation obtained in the nonconserved case as amplitude equation for the standard Hopf bifurcation. Considering first the case of a relatively simple symmetric Cahn-Hilliard model with purely nonreciprocal coupling, we derive the nonlinear nonlocal amplitude equation and show that its bifurcation diagram and time evolution well agree with results for the full model. The solutions of the amplitude equation and their stability are obtained analytically thereby showing that in oscillatory phase separation the suppression of coarsening is universal. Second, we lift the restrictions and obtain the amplitude equation in a more generic case, that also shows very good agreement with the full model as exemplified for some transient dynamics that converges to traveling wave states.
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守恒-霍普夫分岔的振幅方程--推导、分析和评估
我们运用弱非线性理论推导出守恒霍普夫不稳定性的振幅方程,即具有两个守恒定律的系统的一般大尺度振荡不稳定性。所得到的方程在守恒情况下等同于在非守恒情况下作为标准霍普夫分岔振幅方程得到的复数金兹堡-朗道方程。首先考虑具有纯粹非互惠耦合的相对简单的对称卡恩-希利亚德模型,我们推导出非线性非局部振幅方程,并证明其分岔图和时间演化与完整模型的结果一致。振幅方程的解及其稳定性是通过分析得到的,从而表明在振荡相分离中,对粗化的抑制是普遍存在的。其次,我们取消了限制,得到了更一般情况下的振幅方程,该方程与完整模型也显示出很好的一致性,例如收敛于行进波形的某些瞬态动力学。
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