Abstract
A complete analysis of the essential spectrum of matrix-differential operators of the form \begin{align} \begin{pmatrix} -\displaystyle{\frac{\rm d}{\rm d t}} p \displaystyle{\frac{\rm d}{\rm d t}} + q & -\displaystyle{\frac{\rm d}{\rm d t}} b^* \! + c^* \\[2mm] \hspace{6mm} b \displaystyle{\frac{\rm d}{\rm d t}} + c & \hspace{4mm} D \end{pmatrix} \quad \text{in } \ L^2((α, β)) \oplus \bigl(L^2((α, β))\bigr)^n \label{mo} \end{align} singular at is given; the coefficient functions , are scalar real-valued with , , are vector-valued, and is Hermitian matrix-valued. The so-called "singular part of the essential spectrum" is investigated systematically. Our main results include an explicit description of , criteria for its absence and presence; an analysis of its topological structure and of the essential spectral radius. Our key tools are: the asymptotics of the leading coefficient of the first Schur complement of , a scalar differential operator but non-linear in ; the Nevanlinna behaviour in of certain limits of functions formed out of the coefficients in . The efficacy of our results is demonstrated by several applications; in particular, we prove a conjecture on the essential spectrum of some symmetric stellar equilibrium models.
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