[图书][B] Superlinear parabolic problems
P Quittner, P Souplet - 2019 - Springer
Pavol Quittner Philippe Souplet Blow-up, Global Existence and Steady States Second
Edition Page 1 Birkhäuser Advanced Texts Basler Lehrbücher Pavol Quittner Philippe …
Edition Page 1 Birkhäuser Advanced Texts Basler Lehrbücher Pavol Quittner Philippe …
[HTML][HTML] Ground states of nonlinear Schrödinger systems with mixed couplings
J Wei, Y Wu - Journal de Mathématiques Pures et Appliquées, 2020 - Elsevier
We consider the following k-coupled nonlinear Schrödinger systems:{− Δ u j+ λ juj= μ juj
3+∑ i= 1, i≠ jk β i, jui 2 uj in RN, uj> 0 in RN, uj (x)→ 0 as| x|→+∞, j= 1, 2,⋯, k, where N≤ 3 …
3+∑ i= 1, i≠ jk β i, jui 2 uj in RN, uj> 0 in RN, uj (x)→ 0 as| x|→+∞, j= 1, 2,⋯, k, where N≤ 3 …
Least energy solutions for nonlinear Schrödinger systems with mixed attractive and repulsive couplings
Y Sato, ZQ Wang - Advanced Nonlinear Studies, 2015 - degruyter.com
In this paper we study the ground state solutions for a nonlinear elliptic system of three
equations which comes from models in Bose-Einstein condensates. Comparing with existing …
equations which comes from models in Bose-Einstein condensates. Comparing with existing …
Infinitely many nonradial positive solutions for multi-species nonlinear Schrödinger systems in RN
T Li, J Wei, Y Wu - Journal of Differential Equations, 2024 - Elsevier
In this paper, we consider the multi-species nonlinear Schrödinger systems in RN:{− Δ u j+ V
j (x) uj= μ juj 3+∑ i= 1; i≠ jd β i, jui 2 uj in RN, uj (x)> 0 in RN, uj (x)→ 0 as| x|→+∞, j= 1, 2,⋯ …
j (x) uj= μ juj 3+∑ i= 1; i≠ jd β i, jui 2 uj in RN, uj (x)> 0 in RN, uj (x)→ 0 as| x|→+∞, j= 1, 2,⋯ …
Symmetry of components for semilinear elliptic systems
P Quittner, P Souplet - SIAM Journal on Mathematical Analysis, 2012 - SIAM
In this paper, we give sufficient conditions ensuring that any positive classical solution (u,v)
of an elliptic system in the whole space R^n has the symmetry property u=v. As an …
of an elliptic system in the whole space R^n has the symmetry property u=v. As an …
Optimal Liouville-type theorems for noncooperative elliptic Schrödinger systems and applications
P Quittner, P Souplet - Communications in Mathematical Physics, 2012 - Springer
We study multi-component elliptic Schrödinger systems arising in nonlinear optics and Bose-
Einstein condensation phenomena. We prove new Liouville-type nonexistence theorems, as …
Einstein condensation phenomena. We prove new Liouville-type nonexistence theorems, as …
[HTML][HTML] Pattern formation via mixed attractive and repulsive interactions for nonlinear Schrödinger systems
The paper is concerned with the asymptotic behavior of positive least energy vector
solutions to nonlinear Schrödinger systems with mixed couplings which arise from models in …
solutions to nonlinear Schrödinger systems with mixed couplings which arise from models in …
Multiple positive solutions for Schrödinger systems with mixed couplings
Y Sato, ZQ Wang - Calculus of Variations and Partial Differential …, 2015 - Springer
We study the effects of mixed couplings for nonlinear Schrödinger systems. We show due to
the mixed couplings there exist multiple vector positive solutions which exhibit interesting …
the mixed couplings there exist multiple vector positive solutions which exhibit interesting …
Liouville theorems and universal estimates for superlinear elliptic problems without scale invariance
P Quittner, P Souplet - arXiv preprint arXiv:2407.04154, 2024 - arxiv.org
We give applications of known and new Liouville type theorems to universal singularity and
decay estimates for non scale invariant elliptic problems, including Lane-Emden and Schr\" …
decay estimates for non scale invariant elliptic problems, including Lane-Emden and Schr\" …
[HTML][HTML] Entire nonradial solutions for non-cooperative coupled elliptic system with critical exponents in R3
Y Guo, B Li, J Wei - Journal of Differential Equations, 2014 - Elsevier
We consider the following coupled elliptic system:(SN){− Δ u= μ 1 u N+ 2 N− 2+ β u 2 N− 2 v
NN− 2 in RN,− Δ v= μ 2 v N+ 2 N− 2+ β v 2 N− 2 u NN− 2 in RN, u, v> 0, u, v∈ D 1, 2 (RN) …
NN− 2 in RN,− Δ v= μ 2 v N+ 2 N− 2+ β v 2 N− 2 u NN− 2 in RN, u, v> 0, u, v∈ D 1, 2 (RN) …