TY - JOUR
T1 - BOUNDS OF DIRICHLET EIGENVALUES FOR HARDY-LERAY OPERATOR
AU - Chen, Huyuan
AU - Zhou, Feng
N1 - Publisher Copyright:
© 2024 American Institute of Mathematical Sciences. All rights reserved.
PY - 2024
Y1 - 2024
N2 - The purpose of this paper is to study the eigenvalues {λµ,i}i for the Dirichlet Hardy-Leray operator, i.e. −∆u + µ|x|−2u = λu in Ω, u = 0 on ∂Ω, µ where −∆ + |x|2 is the Hardy-Leray operator with µ ≥ − (N−42)2 and Ω is a smooth bounded domain with 0 ∈ Ω. We provide lower bounds of {λµ,i}i, as well as the Li-Yau’s one when µ > − (N−42)2 and Karachalios’s bounds for µ ∈ [− (N−42)2 , 0). Secondly, we obtain Cheng-Yang’s type upper bounds for λµ,k. Additionally, we get the Weyl’s limit of eigenvalues which is independent of the potential’s parameter µ. This interesting phenomenon indicates that the inverse-square potential does not play an essential role for the asymptotic behavior of the spectrum of the problem under study.
AB - The purpose of this paper is to study the eigenvalues {λµ,i}i for the Dirichlet Hardy-Leray operator, i.e. −∆u + µ|x|−2u = λu in Ω, u = 0 on ∂Ω, µ where −∆ + |x|2 is the Hardy-Leray operator with µ ≥ − (N−42)2 and Ω is a smooth bounded domain with 0 ∈ Ω. We provide lower bounds of {λµ,i}i, as well as the Li-Yau’s one when µ > − (N−42)2 and Karachalios’s bounds for µ ∈ [− (N−42)2 , 0). Secondly, we obtain Cheng-Yang’s type upper bounds for λµ,k. Additionally, we get the Weyl’s limit of eigenvalues which is independent of the potential’s parameter µ. This interesting phenomenon indicates that the inverse-square potential does not play an essential role for the asymptotic behavior of the spectrum of the problem under study.
KW - Dirichlet eigenvalues, Hardy-Leray operator
UR - https://www.scopus.com/pages/publications/85190243599
U2 - 10.3934/dcdss.2023132
DO - 10.3934/dcdss.2023132
M3 - 文章
AN - SCOPUS:85190243599
SN - 1937-1632
VL - 17
SP - 1397
EP - 1418
JO - Discrete and Continuous Dynamical Systems - Series S
JF - Discrete and Continuous Dynamical Systems - Series S
IS - 4
ER -