Essential spectrum of singular discrete linear Hamiltonian systems (Q2792259)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Essential spectrum of singular discrete linear Hamiltonian systems |
scientific article; zbMATH DE number 6552183
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Essential spectrum of singular discrete linear Hamiltonian systems |
scientific article; zbMATH DE number 6552183 |
Statements
Essential spectrum of singular discrete linear Hamiltonian systems (English)
0 references
8 March 2016
0 references
linear Hamiltonian difference system
0 references
linear relation
0 references
essential spectrum
0 references
defect index
0 references
square summable solution
0 references
Sturm-Liouville difference equation
0 references
0 references
0 references
0 references
0 references
0 references
0 references
0 references
0 references
0 references
0 references
0 references
The authors characterize all elements of the essential spectrum of the minimal linear relation associated with the linear Hamiltonian difference system NEWLINE\[NEWLINE\mathcal J\Delta y_k-P_k R(y_k)=\lambda\,W_k R(y_k) \tag{1}NEWLINE\]NEWLINE by using square summable solutions of System (1) or of the corresponding nonhomogeneous system. In (1) the index \(k\) belongs to a finite or infinite discrete interval, \(\lambda\in\mathbb{C}\), \(\mathcal{J}:=\begin{pmatrix} 0 & -I\\ I & 0\end{pmatrix}\) with \(I\) being the \(n\times n\) identity matrix, \(\Delta\) denotes the forward difference operator, \(P_k\) are \(2n\times 2n\) Hermitian matrices for all \(k\), \(R(\cdot)\) is the partial shift operator, and \(W_k\) are \(2n\times 2n\) positive semidefinite weight matrices in block diagonal form for all \(k\). Consequently, they obtain analogous results also for any \(2m\)-order vector-valued Sturm-Liouville difference equation.
0 references