Abstract:ForewordIn many areas of applied mathematics and in particular, in applied analysis and differential equations various types of special functions become essential tools for scientists and engineers. They appear in the solutions of initial-value or boundary-value problems of mathematical physics and usually satisfy certain classes of ordinary differential equations. One of the important classes of special functions is of hypergeometric type. It includes all classical hypergeometric functions as the well-known G… Show more
“…where Ξ = τ − cot −1 n and Υ = η − cot −1 n. which is greater than 0.94 (because n ≥ 3), so we can use the asymptotic formulas of the associated Legendre functions [43], thus…”
Section: Curvature Power Spectrum In a Spatially Closed Universe Withmentioning
“…where Ξ = τ − cot −1 n and Υ = η − cot −1 n. which is greater than 0.94 (because n ≥ 3), so we can use the asymptotic formulas of the associated Legendre functions [43], thus…”
Section: Curvature Power Spectrum In a Spatially Closed Universe Withmentioning
We introduce a generalized hybrid integral transformation of the Mehler-Fock type on a segment [0; R] with n conjugate points. We consider examples of application of this transformation to the solution of typical singular boundary-value problems for linear partial differential equations of the second order in piecewise-homogeneous media.
“…where P (μ) −1/2+iβ (cosh y) is the generalized associated Legendre function of the first kind [4], as a solution of the generalized Legendre equation…”
We obtain an analytic representation of a fundamental solution of the Cauchy problem for Petrovskii strictly hyperbolic Λ (μ) -invariant hyperbolic equations and systems of equations in Euclidean spaces and on special Riemann manifolds on the basis of the introduced integral transformations generated by an integral representation of the Dirac measure.
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