2021
DOI: 10.48550/arxiv.2101.12626
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A note on the nonexistence of global solutions to the semilinear wave equation with nonlinearity of derivative-type in the generalized Einstein-de Sitter spacetime

Makram Hamouda,
Mohamed Ali Hamza,
Alessandro Palmieri

Abstract: In this paper, we establish blow-up results for the semilinear wave equation in generalized Einstein-de Sitter spacetime with nonlinearity of derivative type. Our approach is based on the integral representation formula for the solution to the corresponding linear problem in the onedimensional case, that we will determine through Yagdjian's Integral Transform approach. As upper bound for the exponent of the nonlinear term, we discover a Glassey-type exponent which depends both on the space dimension and on the… Show more

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Cited by 4 publications
(8 citation statements)
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“…where θ(n, ℓ, µ, p) is defined in (13) and is a positive quantity thanks to the condition p < p Str (n+ µ ℓ+1 , ℓ) on the exponent of the nonlinear term. Also, for j j 0 and t 2T 1 we arrived at…”
Section: Iteration Argumentmentioning
confidence: 99%
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“…where θ(n, ℓ, µ, p) is defined in (13) and is a positive quantity thanks to the condition p < p Str (n+ µ ℓ+1 , ℓ) on the exponent of the nonlinear term. Also, for j j 0 and t 2T 1 we arrived at…”
Section: Iteration Argumentmentioning
confidence: 99%
“…Moreover, under the same conditions for the parameters as above, also the case with derivative type nonlinearity |∂ t u| p is studied in [13,14,36]. Furthermore, we point out that in [35,36] even the case ℓ −1 with ν 2 = 0 is studied for different semilinear terms.…”
Section: Introductionmentioning
confidence: 99%
“…where the operators A k (x, ∂ x ), k = 1, 2, 3, in general, are the scalar pseudo-differential operators A k (x, ∂ x ) with symbols depending on the spatial variables too. Following [33] we define the generalized Dirac operator as an operator (14) satisfying the condition…”
Section: The Complementary Operatormentioning
confidence: 99%
“…The complementary operator D co (x, t, ∂ t , ∂ x ) for operator (14) is given by the following theorem.…”
Section: The Complementary Operatormentioning
confidence: 99%
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