Surgeon 发表于 2025-3-25 04:50:37
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Luciana Togeiro for shock waves. In the next section, Conley‘s connection index and connection matrix are described; these general notions are useful in con structing travelling waves for systems of nonlinear equations. The final sec tion, Section IV, is devoted to the very recent results of C. Jones and R. Gard引导 发表于 2025-3-26 03:16:37
Harry E. Vandenr each t, .(.) is in ., and . is a linear operator. The main example is the case where . is a linear elliptic operator. The “rest points” ū, in this setting now are solutions of the equation .(.) = 0, and the linearized operator becomes . + .(ū). We shall show that if the spectrum of this operator lSuppository 发表于 2025-3-26 05:35:20
Dorothea Melcherr each t, .(.) is in ., and . is a linear operator. The main example is the case where . is a linear elliptic operator. The “rest points” ū, in this setting now are solutions of the equation .(.) = 0, and the linearized operator becomes . + .(ū). We shall show that if the spectrum of this operator l悄悄移动 发表于 2025-3-26 10:20:37
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Jaime Preciado Coronado,Jorge Hernández, .(.) is in . and . is a linear operator. The main example is the case where . is a linear elliptic operator. The “rest points” ., in this setting now are solutions of the equation . + .(.) = 0, and the linearized operator becomes . + . (.). We shall show that if the spectrum of this operator liesinfringe 发表于 2025-3-26 18:38:23
Tullo Vigevani,Karina Pasquariello Mariano,Marcelo Fernandes de Oliveira,Marilia Campus, .(.) is in . and . is a linear operator. The main example is the case where . is a linear elliptic operator. The “rest points” ., in this setting now are solutions of the equation . + .(.) = 0, and the linearized operator becomes . + . (.). We shall show that if the spectrum of this operator lies