2019
DOI: 10.1142/s0129055x2050018x
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Finite lifespan of solutions of the semilinear wave equation in the Einstein–de Sitter spacetime

Abstract: We examine the solutions of the semilinear wave equation, and, in particular, of the ϕ p model of quantum field theory in the curved space-time. More exactly, for 1 < p < 4 we prove that solution of the massless self-interacting scalar field equation in the Einstein-de Sitter universe has finite lifespan.

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Cited by 24 publications
(34 citation statements)
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“…Their work also showed the existence of global classical solutions for small ε > 0, if p > p c (n) and either n = 2 or n = 3 and the data are radially symmetric. Finally, we mention that our original equations (1.3) is related to semilinear wave equations in the Einstein-de Sitter spacetime considered by Galstian & Yagdjian [4]. We recall that p 0 (n) in (1.5) is the critical exponent for the semilinear wave equation conjectured by Strauss [11].…”
Section: Introductionmentioning
confidence: 91%
“…Their work also showed the existence of global classical solutions for small ε > 0, if p > p c (n) and either n = 2 or n = 3 and the data are radially symmetric. Finally, we mention that our original equations (1.3) is related to semilinear wave equations in the Einstein-de Sitter spacetime considered by Galstian & Yagdjian [4]. We recall that p 0 (n) in (1.5) is the critical exponent for the semilinear wave equation conjectured by Strauss [11].…”
Section: Introductionmentioning
confidence: 91%
“…If α = 2/3 and µ = 2, our blow-up range of p is the same as 1 < p < p cr (n) in [3]. We note that these upper bounds stated so far are sharp if the power p is dominated by the Strauss exponent or p c (n, α, µ).…”
mentioning
confidence: 64%
“…For the case α = 2/3, µ = 2 and n ≥ 1 in (1.3), it is proved by Galstian and Yagdjian [3] that finite time blow-up occurs if 1 < p < p F (n/3) or 1 < p < p cr (n), where p cr (n) is the positive root of…”
mentioning
confidence: 99%
“…In the related literature (see, for example, [3]), the differential operator with timedependent coefficients on the left-hand side of (1.1) is called the wave operator on the generalized Einstein-de Sitter spacetime. This nomenclature is due to the fact that for k = 2 3 and n = 3 the operator ∂ 2 t − t − 4 3 ∆ + 2t −1 ∂ t coincides with the d'Alembertian operator in Einstein-de Sitter's Lorentzian metric.…”
mentioning
confidence: 99%
“…In recent years, many papers have been devoted to the study of blow-up results and lifespan estimates for the semilinear wave equation in the generalized Einstein -de Sitter (EdS) spacetime with power nonlinearities [3,14] and generalizations [19,20,15]. More specifically, it has been conjectured that the critical exponent for the semilinear Cauchy problem with power nonlinearity |u| p…”
mentioning
confidence: 99%