A note on the fundamental solution for the Tricomi-type equation in the hyperbolic domain
By Karen Yagdjian. 2004
78 citations recorded by the source corpus.
Abstract Barros-Neto and Gelfand (Duke Math. J. 98 (3) (1999) 465; Duke Math. J. 117 (2) (2003) 561) constructed for the Tricomi operator y ∂ x 2 + ∂ y 2 on the plane the fundamental solutions with the supports in the regions related to the geometry of the characteristics of the Tricomi operator. We give for the Tricomi-type operator ∂ t 2 - t m △ x a fundamental solution relative to an arbitrary point of R n + 1 with the support in the region t ⩾ 0 , where the operator is hyperbolic. Our key observation is that the fundamental solution for the Tricomi-type operator can be written like an integral of the distributions generated by the fundamental solution of the Cauchy problem for the wave equation . The application of that fundamental solution to the L p - L q estimate for the forced Tricomi-type equation is given as well.
Subfields: Applied Mathematics, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/286a80d2929fabb2cda804d173407acc57aaf552
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In Applied Mathematics
In Mathematical Physics
Citations in the corpus
- On the global solution problem for semilinear generalized Tricomi equations, I (2015, background): “For instance, for the linea r generalized Tricomi equation, the authors in [1], [28] and [30] have computed its fundamental s olution explicitly.”
- A competition between Fujita and Strauss type exponents for blow-up of semi-linear wave equations with scale-invariant damping and mass (2019, methodology): “ explicit integral representation formula for solutions to the inhomogeneous linear Cauchy problem in 1d related to (1.5). Here we strongly follow Yagdjian’s Integral Transform Approach of the papers [34, 38, 36, 37]. Finally, in Section 6 we prove Corollary 1.4. Some concluding remarks and open pro”
- Global Existence for the n-Dimensional Semilinear Tricomi-Type Equations (2006, unknown): “To find out that integral equation, we refer to the operator G introduced in (3.6) and (3.7) (Yagdjian, 2004).”