2010
DOI: 10.1063/1.3387249
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A note on wave equation in Einstein and de Sitter space-time

Abstract: We consider the wave propagating in the Einstein and de Sitter space-time. The covariant d’Alembert’s operator in the Einstein and de Sitter space-time belongs to the family of the non-Fuchsian partial differential operators. We introduce the initial value problem for this equation and give the explicit representation formulas for the solutions. We also show the Lp−Lq estimates for solutions.

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Cited by 25 publications
(29 citation statements)
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“…In order to keep down the length of this paper, we postpone applications of Theorem 1.5 to the derivation of the Strichartz estimates and to global well-posedness of the nonlinear generalized Tricomi equation in the metric (17). We note here that γ = −1 for the metric (17) (see [13]) that makes the hypergeometric function polynomial. Moreover, the hypergeometric function is polynomial for γ = −1, −2, .…”
Section: Introductionmentioning
confidence: 98%
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“…In order to keep down the length of this paper, we postpone applications of Theorem 1.5 to the derivation of the Strichartz estimates and to global well-posedness of the nonlinear generalized Tricomi equation in the metric (17). We note here that γ = −1 for the metric (17) (see [13]) that makes the hypergeometric function polynomial. Moreover, the hypergeometric function is polynomial for γ = −1, −2, .…”
Section: Introductionmentioning
confidence: 98%
“…The case of m > 2 covers the beam equation and hyperbolic in the sense of Petrowski (p-evolution ) equations. On the other hand, the Cauchy-Kowalewski theorem guarantees solvability of the problem in the real analytic functions category for the partial differential equation (13) with any positive ℓ and m = 2. Furthermore, the operator A(x, ∂ x ) = |α|≤2 a α (x)∂ α x can be replaced with an abstract operator A acting on some linear topological space of functions.…”
Section: Introductionmentioning
confidence: 99%
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“…There are also numerous works on the field equations in the smooth (without singulatity) FLRW space-times, in particular in the De Sitter universe (see the fundamental work of H. Friedrich [26], and also e.g. [4], [21], [29], [30], [31], [36], [40], [47], [49], [52], [58], [62]). In contrast, surprisingly enough, few mathematical papers deal with the simpler issue of the behaviour of the linear fields near the cosmological singularities.…”
Section: Introductionmentioning
confidence: 99%