Orbital Stability of Standing Waves for a fourth-order nonlinear Schrödinger equation with the mixed dispersions

In this paper, we study the ground state standing wave solutions for the focusing bi-harmonic nonlinear Schrödinger equation with a $μ$-Laplacian term (BNLS). Such BNLS models the propagation of intense laser beams in a bulk medium with a second-order dispersion term. Denote by $Q_p$ the ground state for the BNLS with $μ=0$. We prove that in the mass-subcritical regime $p\in (1,1+\frac{8}{d})$, there exist orbitally stable {ground state solutions} for the BNLS when $μ\in ( -λ_0, \iy)$ for some $λ_0=λ_0(p, d,\|Q_p\|_{L^2})>0$. Moreover, in the mass-critical case $p=1+\frac{8}{d}$\,, we prove the orbital stability on certain mass level below $\|Q^*\|_{L^2}$, provided $μ\in (-\lam_1,0)$, where $\lam_1=\dfrac{4\|\nabla Q^*\|^2_{L^2}}{\|Q^*\|^2_{L^2}}$ and $Q^*=Q_{1+8/d}$. The proofs are mainly based on the profile decomposition and a sharp Gagliardo-Nirenberg type inequality. Our treatment allows to fill the gap concerning existence of the ground states for the BNLS when $μ$ is negative and $p\in (1,1+\frac8d]$.

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