TY - JOUR
T1 - Construction and stability of blowup solutions for a non-variational semilinear parabolic system
AU - Ghoul, Tej Eddine
AU - Nguyen, Van Tien
AU - Zaag, Hatem
N1 - Funding Information:
H. Zaag is supported by the ERC Advanced Grant no. 291214, BLOWDISOL and by the ANR project ANAÉ ref. ANR-13-BS01-0010-03.
Funding Information:
H. Zaag is supported by the ERC Advanced Grant no. 291214, BLOWDISOL and by the ANR project ANA? ref. ANR-13-BS01-0010-03.
Publisher Copyright:
© 2018 Elsevier Masson SAS
PY - 2018/9
Y1 - 2018/9
N2 - We consider the following parabolic system whose nonlinearity has no gradient structure: {∂tu=Δu+|v|p−1v,∂tv=μΔv+|u|q−1u,u(⋅,0)=u0,v(⋅,0)=v0, in the whole space RN, where p,q>1 and μ>0. We show the existence of initial data such that the corresponding solution to this system blows up in finite time T(u0,v0) simultaneously in u and v only at one blowup point a, according to the following asymptotic dynamics: {u(x,t)∼Γ[(T−t)(1+[Formula presented])]−[Formula presented],v(x,t)∼γ[(T−t)(1+[Formula presented])]−[Formula presented], with b=b(p,q,μ)>0 and (Γ,γ)=(Γ(p,q),γ(p,q)). The construction relies on the reduction of the problem to a finite dimensional one and a topological argument based on the index theory to conclude. Two major difficulties arise in the proof: the linearized operator around the profile is not self-adjoint even in the case μ=1; and the fact that the case μ≠1 breaks any symmetry in the problem. In the last section, through a geometrical interpretation of quantities of blowup parameters whose dimension is equal to the dimension of the finite dimensional problem, we are able to show the stability of these blowup behaviors with respect to perturbations in initial data.
AB - We consider the following parabolic system whose nonlinearity has no gradient structure: {∂tu=Δu+|v|p−1v,∂tv=μΔv+|u|q−1u,u(⋅,0)=u0,v(⋅,0)=v0, in the whole space RN, where p,q>1 and μ>0. We show the existence of initial data such that the corresponding solution to this system blows up in finite time T(u0,v0) simultaneously in u and v only at one blowup point a, according to the following asymptotic dynamics: {u(x,t)∼Γ[(T−t)(1+[Formula presented])]−[Formula presented],v(x,t)∼γ[(T−t)(1+[Formula presented])]−[Formula presented], with b=b(p,q,μ)>0 and (Γ,γ)=(Γ(p,q),γ(p,q)). The construction relies on the reduction of the problem to a finite dimensional one and a topological argument based on the index theory to conclude. Two major difficulties arise in the proof: the linearized operator around the profile is not self-adjoint even in the case μ=1; and the fact that the case μ≠1 breaks any symmetry in the problem. In the last section, through a geometrical interpretation of quantities of blowup parameters whose dimension is equal to the dimension of the finite dimensional problem, we are able to show the stability of these blowup behaviors with respect to perturbations in initial data.
KW - Blowup profile
KW - Blowup solution
KW - Semilinear parabolic system
KW - Stability
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U2 - 10.1016/j.anihpc.2018.01.003
DO - 10.1016/j.anihpc.2018.01.003
M3 - Article
AN - SCOPUS:85044579803
SN - 0294-1449
VL - 35
SP - 1577
EP - 1630
JO - Annales de l'Institut Henri Poincare (C) Analyse Non Lineaire
JF - Annales de l'Institut Henri Poincare (C) Analyse Non Lineaire
IS - 6
ER -