Abstract:Given a Hilbert space H, we investigate the well-posedness of the Cauchy problem for the wave equation for operators with a discrete non-negative spectrum acting on H. We consider the cases when the time-dependent propagation speed is regular, Hölder, and distributional. We also consider cases when it is strictly positive (strictly hyperbolic case) and when it is non-negative (weakly hyperbolic case). When the propagation speed is a distribution, we introduce the notion of "very weak solutions" to the Cauchy p… Show more
“…We begin with a reminder of the definition of the group Fourier transform on the Heisenberg group (see many sources, but e.g. [26,27] for its use in similar contexts). For f ∈ S(H n ) the group Fourier transform is defined as…”
This paper deals with the fractional generalization of the integrodifferential diffusion-wave equation for the Heisenberg sub-Laplacian, with homogeneous Bitsadze-Samarskii type time-nonlocal conditions. For the considered problem, we show the existence, uniqueness and the explicit representation formulae for the solution.
“…We begin with a reminder of the definition of the group Fourier transform on the Heisenberg group (see many sources, but e.g. [26,27] for its use in similar contexts). For f ∈ S(H n ) the group Fourier transform is defined as…”
This paper deals with the fractional generalization of the integrodifferential diffusion-wave equation for the Heisenberg sub-Laplacian, with homogeneous Bitsadze-Samarskii type time-nonlocal conditions. For the considered problem, we show the existence, uniqueness and the explicit representation formulae for the solution.
“…One can be started a 'nonharmonic' analysis connected with the singular, in the above sense, operators. Note, that the nonharmonic analysis is developed in the works [2,10,13,15] with applications given in [14,16]. For more general setting of the nonharmonic analysis, see for instance [6].…”
In the work we derive regularized trace formulas which were established in papers of Kanguzhin and Tokmagambetov for the Laplace and m-Laplace operators in a punctured domain with the fixed iterating order m ∈ N. By using techniques of Sadovnichii and Lyubishkin, the authors in that papers described regularized trace formulae in the spatial dimension d = 2. In this note one claims that the formulas are also true for more general operators in the higher spatial dimensions, namely, 2 ≤ d ≤ 2m. Also, we give the further discussions on a development of the analysis associated with the operators in punctured domains. This can be done by using so called 'nonharmonic' analysis.
“…From [4] it follows that the problem (1) has a unique very weak solution. It is given by a family of functions �� � (�, �)� ����� .…”
Section: Numerical Experimentsmentioning
confidence: 99%
“…In this paper, we follow the results of the paper [4] and study the Cauchy-Dirichlet problem for the 1D-Wave Equation The notion of very weak solutions has been introduced in [GR15] to analyse second order hyperbolic equations. In [3] and [5] Ruzhansky and Tokmagambetov applied it to show the wellposedness of the Landau Hamiltonian wave equations in distributional electro-magnetic fields.…”
In this note, we illustrate numerical experiments for the one-dimensional wave equation with �-like (delta like) terms. Our research is connecting the theory with the numerical realisations. By using results on very weak solutions introduced by Michael Ruzhansky with his co-authors, we investigate a corresponding regularized problem. In contrast to our expectations, the experiments show that the solution of the regularized problem has a "good" behaviour. Indeed, numerical experiments show that approximation methods work well in situations where a rigorous mathematical formulation of the problem is difficult in the framework of the classical theory of distributions. The concept of very weak solutions eliminates this difficulty, giving results of correctness for equations with singular coefficients. In the framework of this approach (very weak solutions), the expected physical properties of the equation can be reconstructed, for example, the distribution profile and the decay of the solutions for large times. Finally, we give a number of illustrations.
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