scholarly journals Two-term spectral asymptotics for the Dirichlet Laplacian in a Lipschitz domain

2020 ◽  
Vol 2020 (766) ◽  
pp. 195-228 ◽  
Author(s):  
Rupert L. Frank ◽  
Simon Larson

AbstractWe prove a two-term Weyl-type asymptotic formula for sums of eigenvalues of the Dirichlet Laplacian in a bounded open set with Lipschitz boundary. Moreover, in the case of a convex domain we obtain a universal bound which correctly reproduces the first two terms in the asymptotics.

Author(s):  
S. I. Boyarchenko ◽  
S. Z. Levendorskiĭ

We study the Neumann Laplacian in unbounded regions of the form Ω = {(t, x) | t >O,f(t)−1x ∊ Ω′}, where Ω′ ⊂ ℝn−1 is a bounded open set with the Lipschitz boundary and f decays in such a way that the spectrum of is discrete but the counting function N(λ, ) of the spectrum grows faster than a power of λ, a typical example being f(t) = exp (– t In … In t), for t ≧ t0. We compute the principal term of the asymptotics of N(λ, ), with a remainder estimate.


1994 ◽  
Vol 06 (04) ◽  
pp. 515-596 ◽  
Author(s):  
ANNE BOUTET de MONVEL-BERTHIER ◽  
VLADIMIR GEORGESCU ◽  
AVY SOFFER

We study N-body hamiltonians with short and long range potentials which are infinite on compact sets of non-zero measure. We show that the generator of the dilation group is locally conjugated to them away from the threshold energies. The notion of conjugacy has to be interpreted in a very weak sense, but this is enough to deduce an optimal form of the limiting absorption principle, and so absence of singular continuous spectrum and local decay. One of the main technical steps of our approach requires a maximal regularity result for the Dirichlet Laplacian in an open set with irregular boundary. We prove it for a large class of non-smooth domains.


2021 ◽  
Vol 15 (3) ◽  
Author(s):  
Markus Holzmann

AbstractIn this note the three dimensional Dirac operator $$A_m$$ A m with boundary conditions, which are the analogue of the two dimensional zigzag boundary conditions, is investigated. It is shown that $$A_m$$ A m is self-adjoint in $$L^2(\Omega ;{\mathbb {C}}^4)$$ L 2 ( Ω ; C 4 ) for any open set $$\Omega \subset {\mathbb {R}}^3$$ Ω ⊂ R 3 and its spectrum is described explicitly in terms of the spectrum of the Dirichlet Laplacian in $$\Omega $$ Ω . In particular, whenever the spectrum of the Dirichlet Laplacian is purely discrete, then also the spectrum of $$A_m$$ A m consists of discrete eigenvalues that accumulate at $$\pm \infty $$ ± ∞ and one additional eigenvalue of infinite multiplicity.


2015 ◽  
Vol 14 (3) ◽  
pp. 1239-1258 ◽  
Author(s):  
Nicolas Raymond ◽  
Thomas Ourmières-Bonafos ◽  
Monique Dauge

2020 ◽  
Vol 26 ◽  
pp. 42 ◽  
Author(s):  
Mahamadi Warma ◽  
Sebastián Zamorano

We make a complete analysis of the controllability properties from the exterior of the (possible) strong damping wave equation associated with the fractional Laplace operator subject to the non-homogeneous Dirichlet type exterior condition. In the first part, we show that if 0 <s< 1, Ω ⊂ ℝN(N≥ 1) is a bounded Lipschitz domain and the parameterδ> 0, then there is no control functiongsuch that the following system\begin{align} u_{1,n}+ u_{0,n}\widetilde{\lambda}_{n}^++ \delta u_{0,n}\lambda_{n}=\int_0^{T}\int_{\Omc}(g(x,t)+\delta g_t(x,t))e^{-\widetilde{\lambda}_{n}^+ t}\mathcal{N}_{s}\varphi_{n}(x)\d x\d t,\label{39}\\ u_{1,n}+ u_{0,n}\widetilde{\lambda}_{n}^- +\delta u_{0,n}\lambda_{n}=\int_0^{T}\int_{\Omc}(g(x,t)+\delta g_t(x,t))e^{-\widetilde{\lambda}_{n}^- t}\mathcal{N}_{s}\varphi_{n}(x)\d x\d t,\label{40} \end{align}is exact or null controllable at timeT> 0. In the second part, we prove that for everyδ≥ 0 and 0 <s< 1, the system is indeed approximately controllable for anyT> 0 andg∈D(O× (0,T)), whereO⊂ ℝN\ Ω is any non-empty open set.


2005 ◽  
Vol 2005 (6) ◽  
pp. 563-573
Author(s):  
Tetsutaro Shibata

We consider the semilinear elliptic eigenvalue problem−Δu+k(|x|)up=λu,u>0inBR,u=0on∂BR, wherep>1is a constant,BR:={x∈RN:|x|<R}(N≥1), andλ>0is a parameter. We investigate the global structure of the branch of(λ,uλ)of bifurcation diagram from a point of view ofL2-theory. To do this, we establish a precise asymptotic formula forλ=λ(α)asα→∞, whereα:=‖uλ‖2.


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