Abstract
The hydrodynamic evolution of self-gravitating gaseous stars is governed by the Euler–Poisson equations. We study the structure of the linear approximation of barotropic perturbations around spherically symmetric equilibria based on functional analytic tools. In contrast to folklore, we show that the spectrum of the linearized operator for general perturbations is not of the Sturm–Liouville type unless the perturbations are restricted. Among others, we prove that it is of the Sturm–Liouville type for irrotational perturbations.
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