Abstract
AbstractIn this article, we consider the upper critical Choquard equation with a local perturbation−Δu=λu+(Iα∗∣u∣p)∣u∣p−2u+μ∣u∣q−2u,x∈RN,u∈H1(RN),∫RN∣u∣2=a,\left\{\begin{array}{l}-\Delta u=\lambda u+\left({I}_{\alpha }\ast | u\hspace{-0.25em}{| }^{p})| u\hspace{-0.25em}{| }^{p-2}u+\mu | u\hspace{-0.25em}{| }^{q-2}u,\hspace{1em}x\in {{\mathbb{R}}}^{N},\\ u\in {H}^{1}\left({{\mathbb{R}}}^{N}),\hspace{1em}{\displaystyle \int }_{{{\mathbb{R}}}^{N}}| u\hspace{-0.25em}{| }^{2}=a,\end{array}\right.whereN≥3N\ge 3,μ>0\mu \gt 0,a>0a\gt 0,λ∈R\lambda \in {\mathbb{R}},α∈(0,N)\alpha \in \left(0,N),p=p¯≔N+αN−2p=\bar{p}:= \frac{N+\alpha }{N-2},q∈2,2+4Nq\in \left(2,2+\frac{4}{N}\right), andIα=C∣x∣N−α{I}_{\alpha }=\frac{C}{| x{| }^{N-\alpha }}withC>0C\gt 0. Whenμaq(1−γq)2≤(2K)qγq−2p¯2(p¯−1)\mu {a}^{\tfrac{q\left(1-{\gamma }_{q})}{2}}\le {\left(2K)}^{\tfrac{q{\gamma }_{q}-2\bar{p}}{2\left(\bar{p}-1)}}withγq=N2−Nq{\gamma }_{q}=\frac{N}{2}-\frac{N}{q}andKKbeing some positive constant, we prove(1)Existence and orbital stability of the ground states.(2)Existence, positivity, radial symmetry, exponential decay, and orbital instability of the “second class” solutions.This article generalized and improved parts of the results obtained for the Schrödinger equation.
Highlights
Introduction and main resultsIn this article, we study standing waves of prescribed mass to the Choquard equation with a local perturbation i∂tψ + Δψ + (Iα ∗ ∣ψ∣p)∣ψ∣p−2 ψ + μ∣ψ∣q−2 ψ = 0, (t, x) ∈ × N, (1.1) where N ≥ 3, ψ :× N →, μ > 0, α ∈ (0, N ), Iα is the Riesz potential defined for every x ∈ N⧹{0} by ( ) Iα(x) ≔ Aα(N ), ( ) ∣x∣N−α Γ N−α Aα(N ) ≔Γ α πN /22α (1.2)with Γ denoting the Gamma function, p and q will be defined later
We study standing waves of prescribed mass to the Choquard equation with a local perturbation i∂tψ + Δψ + (Iα ∗ ∣ψ∣p)∣ψ∣p−2 ψ + μ∣ψ∣q−2 ψ = 0, (t, x) ∈ × N, (1.1)
In [3], Choquard applied it as an approximation to Hartree-Fock theory of one component plasma
Summary
Note that 2 + 4 is the L2-critical exponent in studying normalized solutions to the Schrödinger equation. This article is motivated by [26–29], which considered normalized solutions to the Schrödinger equation with mixed nonlinearities. The following result is about the positivity, radial symmetry, and exponential decay of the “second class” solution. The exponential decay follows the radial symmetry, the estimate of (Iα ∗ ∣u∣p ), and the exponential decay studied in [33] to the Schrödinger equation. Theorem 1.7 plays an important role in proving the following result. The conditions α ≥ N − 4 (i.e., p ≥ 2) and α < N − 2 in Theorems 1.4 and 1.8 are added for obtaining the local existence of solution to (1.1), see Lemma 6.4.
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