On an application of the generalized Floquet theory to the transformation of the equation into its associated equation
Staněk, Svatoslav (1979)
Sborník prací Přírodovědecké fakulty University Palackého v Olomouci. Matematika
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Displaying similar documents to “On the theory of phases of academican O. Borůvka”
On an application of the generalized Floquet theory to the transformation of the equation into its associated equation
Remark to the comparison of solution properties of Love's equation with those of wave equation
Věra Radochová (1978)
Aplikace matematiky
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In the paper some solution properties of the Love's equation are compared with those of the classical wave equation for a certain class of boundary conditions. The method of small parameter is used.
Fibration of the phase space for the Korteweg-de Vries equation
Thomas Kappeler (1991)
Annales de l'institut Fourier
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In this article we prove that the fibration of by potentials which are isospectral for the 1-dimensional periodic Schrödinger equation, is trivial. This result can be applied, in particular, to -gap solutions of the Korteweg-de Vries equation (KdV) on the circle: one shows that KdV, a completely integrable Hamiltonian system, has global action-angle variables.
Propagation, reflection and refraction of singularities for a hyperbolic transmission problem in two adjacent angular regions
Lorenza Diomeda, Benedetta Lisena (1987)
Rendiconti del Seminario Matematico della Università di Padova
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Rough maximal functions and rough singular integral operators applied to integrable radial functions.
Peter Sjögren, Fernando Soria (1997)
Revista Matemática Iberoamericana
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Let Ω be homogeneous of degree 0 in R and integrable on the unit sphere. A rough maximal operator is obtained by inserting a factor Ω in the definition of the ordinary maximal function. Rough singular integral operators are given by principal value kernels Ω(y) / |y|, provided that the mean value of Ω vanishes. In an earlier paper, the authors showed that a two-dimensional rough maximal operator is of weak type (1,1) when restricted to radial functions. This result is now extended to...