Zobrazeno 1 - 10
of 128
pro vyhledávání: '"Yanheng Ding"'
Publikováno v:
Electronic Journal of Differential Equations, Vol 2004, Iss 100, Pp 1-18 (2004)
We prove a critical-point result which provides conditions for the existence of infinitely many critical points of a strongly indefinite functional with perturbed symmetries. Then we apply this result to obtain infinitely many solutions of non-symmet
Externí odkaz:
https://doaj.org/article/29fa1cea1c2d491e97c2e4cc16101bb7
Autor:
Yanheng, Ding, Tian, Xu
Publikováno v:
Calculus of Variations and Partial Differential Equations (2014) 51: 17-44
We study the semi-classical ground states of the nonlinear Maxwell-Dirac system: \[ \left\{ \begin{aligned} &\al\cdot\big(i\hbar\nabla+ q(x)\fa(x)\big) w-a\bt w -\omega w - q(x)\phi(x) w = P(x)g(\jdz{w}) w\\ &-\Delta\phi=q(x)\jdz{w}^2\\ &-\Delta{A_k}
Externí odkaz:
http://arxiv.org/abs/1412.5061
Autor:
Yanheng Ding, Hua-Yang Wang
Publikováno v:
Journal of Differential Equations. 365:636-666
Autor:
Yanheng Ding
This unique book focuses on critical point theory for strongly indefinite functionals in order to deal with nonlinear variational problems in areas such as physics, mechanics and economics. With the original ingredients of Lipschitz partitions of uni
Publikováno v:
Advanced Nonlinear Studies. 22:248-272
In the present article, we study multiplicity of semi-classical solutions of a Yukawa-coupled massive Dirac-Klein-Gordon system with the general nonlinear self-coupling, which is either subcritical or critical growth. The number of solutions obtained
Publikováno v:
The Journal of Geometric Analysis. 33
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Publikováno v:
SIAM Journal on Mathematical Analysis. 53:5731-5755
We show existence and multiplicity results for nonlinear Dirac--Klein--Gordon systems with two different nonlinear interaction terms. Both the Dirac field and the Klein--Gordon field considered her...
Publikováno v:
Nonlinearity. 33:6695-6728
In this paper we are interested in the existence of semiclassical states for the Choquard type equation − ε 2 Δ u + V ( x ) u = ∫ R N G ( u ( y ) ) | x − y | μ d y g ( u ) in R N , where 0 < μ < N, N ⩾ 3, ɛ is a positive parameter and G