TY - JOUR
T1 - The Existence and Stability of Normalized Solutions for a Bi-Harmonic Nonlinear Schrödinger Equation with Mixed Dispersion
AU - Luo, Tingjian
AU - Zheng, Shijun
AU - Zhu, Shihui
N1 - Publisher Copyright:
© 2022, Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences.
PY - 2023/3
Y1 - 2023/3
N2 - 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. Denoting by Qp the ground state for the BNLS with μ = 0, we prove that in the mass-subcritical regime p∈(1,1+8d), there exist orbit ally stable ground state solutions for the BNLS when μ ∈ (−λ0, ∞) for some λ0=λ0(p,d,‖Qp‖L2)>0. Moreover, in the mass-critical case p=1+8d, we prove the orbital stability on a certain mass level below ‖Q∗‖L2 provided that μ ∈ (−λ1, 0), where λ1=4‖∇Q∗‖L22‖Q∗‖L22 and Q* = Q1+8/d. The proofs are mainly based on the profile decomposition and a sharp Gagliardo-Nirenberg type inequality. Our treatment allows us to fill the gap concerning the existence of the ground states for the BNLS when μ is negative and p∈(1,1+8d].
AB - 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. Denoting by Qp the ground state for the BNLS with μ = 0, we prove that in the mass-subcritical regime p∈(1,1+8d), there exist orbit ally stable ground state solutions for the BNLS when μ ∈ (−λ0, ∞) for some λ0=λ0(p,d,‖Qp‖L2)>0. Moreover, in the mass-critical case p=1+8d, we prove the orbital stability on a certain mass level below ‖Q∗‖L2 provided that μ ∈ (−λ1, 0), where λ1=4‖∇Q∗‖L22‖Q∗‖L22 and Q* = Q1+8/d. The proofs are mainly based on the profile decomposition and a sharp Gagliardo-Nirenberg type inequality. Our treatment allows us to fill the gap concerning the existence of the ground states for the BNLS when μ is negative and p∈(1,1+8d].
KW - 35J20
KW - 35J35
KW - 35J60
KW - 37K45
KW - bi-harmonic operator
KW - elliptic equations
KW - normalized solutions
KW - profile decomposition
UR - http://www.scopus.com/inward/record.url?scp=85142690169&partnerID=8YFLogxK
U2 - 10.1007/s10473-023-0205-5
DO - 10.1007/s10473-023-0205-5
M3 - Article
AN - SCOPUS:85142690169
SN - 0252-9602
VL - 43
SP - 539
EP - 563
JO - Acta Mathematica Scientia
JF - Acta Mathematica Scientia
IS - 2
ER -