Solutions for semilinear elliptic equations with critical exponents and Hardy potential
By Daomin Cao, Pigong Han. 2004
163 citations recorded by the source corpus.
Subfields: Applied Mathematics, Computational Theory and Mathematics, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/06d4c2b23d34a31571e722af5af6bfa2f990cff8
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In Applied Mathematics
- Zhitao Zhang
- Shuangjie Peng
- Chang-Lin Xiang
- Thomas Bartsch
- Nikolaos S. Papageorgiou
- Tobias Weth
- Vicentiu D. Rădulescu
- Wenming Zou
In Computational Theory and Mathematics
- Shuangjie Peng
- Chang-Lin Xiang
- Thomas Bartsch
- Zhitao Zhang
- Nikolaos S. Papageorgiou
- Tobias Weth
- Vicentiu D. Rădulescu
- Zhaoli Liu
In Mathematical Physics
- Shuangjie Peng
- Zhitao Zhang
- Chang-Lin Xiang
- Thomas Bartsch
- Wenming Zou
- Nicola Soave
- Louis Jeanjean
- Jean Van Schaftingen
Citations in the corpus
- Asymptotic behaviors of solutions to quasilinear elliptic equations with critical Sobolev growth and Hardy potential (2015, methodology): “s both a weak subsolution and a weak supersolution. Equation (1.1) and its variants have been extensively studied in the literature. For the existence of solutions to equation (1.1), we refer to e.g. [3, 4, 7, 8, 9, 10, 11, 16, 17, 19, 20, 26]. For the uniqueness of solutions to equation (1.1), we r”
- Solutions to critical elliptic equations with multi-singular inverse square potentials (2006, unknown): “For any 0 ̄, ∫ ( |∇ua , |2 − (ua , ) 2 |x − a|2 ) dx = S N 2 + O ( 2 √ ̄− ) , (3.10) D. Cao, P. Han / J. Differential Equations 224 (2006) 332–372 355∫ |ua , |2 ∗ dx = S N 2 + O ( 2N N−2 √ ̄− ) (3.11) and for any ∈ RN\{0}, ∫ |u0 , |2 |x + |2 dx = ⎧⎪⎪⎪⎪⎨⎪⎪⎪⎪⎩ 2 | |2 ∫ RN U2 ,0(x) dx + o( 2) if ”
- Infinitely many solutions for an elliptic problem involving critical Sobolev growth and Hardy potential (2010, unknown): “solution of (1.1) is singular at x = 0i fμ � 0( see [ 8 ,9]).”
- Existence and non-existence of solutions to elliptic equations related to the Caffarelli–Kohn–Nirenberg inequalities (2007, background): “5) −∆u = μ u |x|2 + |x|βup(β)−1 + f(x, u), x ∈ Ω, u(x) = 0, x ∈ ∂Ω, where 0 ≤ μ < (N − 2)(2)/4, p(β) = 2(N + β)/(N − 2), −2 < β ≤ 0, f(x, u) is a subcritical perturbation; see [1, 8, 10, 11, 15, 19, 20, 23, 24, 25, 26] et al.”