2025/08/12 by Shuijin Zhang, Zhang, Shuijin, Jijie Xu +3
Mathematics · #Nonlinear Partial Differential Equations #Differential Equations and Boundary Problems #Advanced Mathematical Physics Problems
paper · pdf · doi:10.48550/arxiv.2508.08614
We investigate the quantitative stability of the nonlocal Sobolev inequality in Heisenberg group CHL(Q,μ) (∫ℍn∫ℍn\frac|u(ξ)|^Q∗μ|u(η)|^Q∗μ|η-1ξ|μdξdη)^\frac1Q∗μ≤ ∫ℍn|∇Hu|2dξ, ∀ u∈ S1,2(ℍn), where Q=2n+2 is the homogeneous dimension of the Hiesenberg group ℍn, μ∈(0,Q) and Q∗μ=(2Q-μ)/(Q-2) are two parameters corresponding to the Hardy-Littlewood-Sobolev inequality and Folland-Stein inequality on Heisenberg group, CHL(Q,μ) is the sharp constant of the nonlocal-Sobolev inequality. Specifically, when u is close to solving the Euler equation -ΔH u=(∫ℍn\frac|u(η)|^Q∗μ|η-1ξ|μdη)|u|^Q∗μ-2u, ξ,η∈ℍn, the natural distance between u and the the set of optimizers Uλ,ζ, defined as δ(u)=||∇Hu-∇HUλ,ζ||L2, can be linearly bounded by the functional derivative term Γ(u)=‖ΔHu+(∫ℍn\frac|u(η)|^Q∗μ|η-1ξ|μdη)|u|^Q∗μ-2u‖(S1,2(ℍn))-1. And for the weakly interacting bubble solutions \mathop∑i=1νU_λi,ζi, the aforementioned quantitative stability result holds when the dimension Q=4.