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Dynamics of Partial Differential Equations最新文献

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$W^{1,infty}$ instability of $H^1$-stable peakons in the Novikov equation Novikov方程中$H^1$稳定顶点的$W^{1,infty}$不稳定性
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-11-19 DOI: 10.4310/dpde.2021.v18.n3.a1
R. Chen, D. Pelinovsky
It is known from the previous works that the peakon solutions of the Novikov equation are orbitally and asymptotically stable in $H^1$. We prove, via the method of characteristics, that these peakon solutions are unstable under $W^{1,infty}$-perturbations. Moreover, we show that small initial $W^{1,infty}$-perturbations of the Novikov peakons can lead to the finite time blow-up of the corresponding solutions.
从以前的工作中可以知道,Novikov方程的peakon解在$H^1$中是轨道渐近稳定的。我们用特征方法证明了这些peakon解在$W^{1,infty}$扰动下是不稳定的。此外,我们证明了Novikov peakons的小的初始$W^{1,infty}$扰动可以导致相应解的有限时间爆破。
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引用次数: 6
Laplace Equation 拉普拉斯方程
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-06-23 DOI: 10.1142/9789811202247_0004
C. Ou
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引用次数: 0
FRONT MATTER 前页
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-06-23 DOI: 10.1142/9789811202247_fmatter
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引用次数: 0
Hints and Solutions to Selected Exercises 选定练习的提示和解答
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-06-23 DOI: 10.1887/0750306521/b803b2
Rowan Garnier, John Taylor
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引用次数: 0
BACK MATTER 回到问题
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-06-23 DOI: 10.1142/9789811202247_bmatter
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引用次数: 0
Asymptotic autonomy of kernel sections for Newton–Boussinesq equations on unbounded zonary domains 无界带域上Newton-Boussinesq方程核段的渐近自治
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-01-01 DOI: 10.4310/dpde.2019.v16.n3.a4
Renhai Wang, Yangrong Li
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引用次数: 10
Stability of hyperbolic-parabolic mixed type equations 双曲-抛物混合型方程的稳定性
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-01-01 DOI: 10.4310/dpde.2019.v16.n3.a2
Huashui Zhan, Zhaosheng Feng
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引用次数: 2
Long time behavior of the NLS-Szegő equation nls -塞格格方程的长时间行为
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-01-01 DOI: 10.4310/dpde.2019.v16.n4.a2
Ruoci Sun
. We are interested in the influence of filtering the positive Fourier modes to the integrable non linear Schr¨odinger equation. Equivalently, we want to study the effect of dispersion added to the cubic Szeg˝o equation, leading to the NLS-Szeg˝o equation on the circle S 1 There are two sets of results in this paper. The first result concerns the long time Sobolev estimates for small data. The second set of results concerns the orbital stability of plane wave solutions. Some instability results are also obtained, leading to the wave turbulence phenomenon.
. 我们感兴趣的是正傅立叶模滤波对可积非线性薛定谔方程的影响。同样地,我们想研究色散对三次Szeg“o”方程的影响,从而得到NLS-Szeg“o”方程对圆s1的影响。第一个结果与Sobolev对小数据的长时间估计有关。第二组结果涉及平面波解的轨道稳定性。也得到了一些不稳定的结果,导致波浪湍流现象。
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引用次数: 3
On global attractor of 3D Klein–Gordon equation with several concentrated nonlinearities 若干非线性集中的三维Klein-Gordon方程的全局吸引子
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-01-01 DOI: 10.4310/DPDE.2019.V16.N2.A1
E. Kopylova, A. Komech
. The global attraction is proved for solutions to 3D Klein-Gordon equation coupled to several nonlinear point oscillators. Our main result is a convergence of each finite energy solution to the set of all solitary waves as t → ±∞ . This attraction is caused by the nonlinear energy transfer from lower harmonics to the continuous spectrum and subsequent dispersion radiation. We justify this mechanism by the following strategy based on inflation of spectrum by the nonlinearity . We show that any omega-limit trajectory has the time-spectrum in the spectral gap [ − m,m ] and satisfies the original equation. Then the application of the Titchmarsh convolution theorem reduces the time-spectrum to a single harmonic ω ∈ [ − m,m ].
. 证明了耦合若干非线性点振子的三维Klein-Gordon方程解的全局吸引力。我们的主要结果是当t→±∞时所有孤立波集合的每个有限能量解的收敛性。这种吸引是由低次谐波到连续谱的非线性能量转移和随后的色散辐射引起的。我们通过以下基于非线性谱膨胀的策略来证明这一机制。我们证明了任何ω -极限轨迹在谱隙[−m,m]内都有时间谱,并且满足原方程。然后应用Titchmarsh卷积定理将时间谱约化为单谐波ω∈[- m,m]。
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引用次数: 17
Predual forms, harmonic maps and liquid crystals of $(BMO-Q)$ and $(BMO-Q)^{-1}$ $(BMO-Q)$和$(BMO-Q)^{-1}$的前对偶形式、谐波映射和液晶
IF 1.3 3区 数学 Q2 Mathematics Pub Date : 2019-01-01 DOI: 10.4310/dpde.2019.v16.n4.a3
J. Xiao, Junjie Zhang
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引用次数: 0
期刊
Dynamics of Partial Differential Equations
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