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首页> 外文期刊>Studies in Applied Mathematics >Eigenfunctions and Very Singular Similarity Solutions of Odd-Order Nonlinear Dispersion PDEs: Toward a 'Nonlinear Airy Function' and Others
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Eigenfunctions and Very Singular Similarity Solutions of Odd-Order Nonlinear Dispersion PDEs: Toward a 'Nonlinear Airy Function' and Others

机译:奇数阶非线性色散PDE的本征函数和非常奇异的相似解:朝“非线性艾里函数”等方向发展

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Asymptotic properties of nonlinear dispersion equations u _t = (|u| ~nu)xxx and u _t = (|u| ~nu)xxx - |u|p-1u in R{double-struck} × R{double-struck} _+ (1) with fixed exponents n > 0 and p > n+ 1, and their (2k+ 1)th-order analogies are studied. The global in time similarity solutions, which lead to "nonlinear eigenfunctions" of the rescaled ordinary differential equations (ODEs), are constructed. The basic mathematical tools include a "homotopy-deformation" approach, where the limit in the first equation in (1) turns out to be fruitful. At n= 0 the problem is reduced to the linear dispersion one: ν _t = ν _(xxx) whose oscillatory fundamental solution via Airy's classic function has been known since the nineteenth century. The corresponding Hermitian linear non-self-adjoint spectral theory giving a complete countable family of eigenfunctions was developed earlier in [1]. Various other nonlinear operator and numerical methods for (1) are also applied. As a key alternative, the "super-nonlinear" limit, with the limit partial differential equation (PDE) (sign _ν) t=ν _(xxx), in terms of the variable ν = |u| ~nu, admitting three almost "algebraically explicit" nonlinear eigenfunctions, is performed. For the second equation in (1), very singular similarity solutions (VSSs) are constructed. In particular, a "nonlinear bifurcation" phenomenon at critical values {p=p _l(n)} _l≥0 of the absorption exponents is discussed.
机译:非线性色散方程u _t =(| u |〜nu)xxx和u _t =(| u |〜nu)xxx-| u | p-1u的渐近性质在R {double-struck}×R {double-struck}中研究了具有固定指数n> 0和p> n + 1的_ +(1)以及它们的(2k + 1)阶类比。构造了全局时间相似度解,该解导致了重新定标的常微分方程(ODE)的“非线性本征函数”。基本的数学工具包括“同态变形”方法,其中在(1)中的第一个方程式中的极限非常有用。在n = 0时,问题简化为线性色散1:ν_t =ν_(xxx)自19世纪以来,通过艾里的经典函数就知道了它的振荡基本解。给出了一个完整可数的本征函数族的相应的埃尔米特线性非自伴谱理论在较早的文献[1]中得到了发展。还适用于(1)的各种其他非线性算子和数值方法。作为主要替代方案,用变量ν= | u |,具有极限偏微分方程(PDE)(符号_ν)t =ν_(xxx)的“超非线性”极限。 nu,允许三个几乎“代数显式”的非线性本征函数被执行。对于(1)中的第二个方程,构造了非常奇异的相似性解决方案(VSSs)。特别地,讨论了在吸收指数的临界值{p = p_l(n)} _l≥0处的“非线性分叉”现象。

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