2021
DOI: 10.1007/978-3-030-75186-9
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A Birman-Schwinger Principle in Galactic Dynamics

Abstract: These are the (somewhat extended) lecture notes for four lectures delivered at the spring school during the thematic programme "Mathematical Perspectives of Gravitation beyond the Vacuum Regime" at ESI Vienna in February 2022. Contents 1 Introduction 2 The Birman-Schwinger principle in quantum mechanics 3 Galactic dynamics: The Vlasov-Poisson system 4 Spherically symmetric solutions 5 Steady state solutions 6 Action angle variables 7 Function spaces 8 Linearization 1 9 The Birman-Schwinger approach 21 10 An ap… Show more

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Cited by 3 publications
(4 citation statements)
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“…During the writing of this manuscript we have been informed that related results were obtained independently by M. Kunze [36].…”
Section: Outline Of the Papermentioning
confidence: 99%
“…During the writing of this manuscript we have been informed that related results were obtained independently by M. Kunze [36].…”
Section: Outline Of the Papermentioning
confidence: 99%
“…Crucial parts of our investigation are based on action-angle type variables, which we introduce in Section 3.3. While action-angle variables are a classical tool in Hamiltonian mechanics [9,32,38], they have been used recently to derive a Birman-Schwinger principle in Newtonian galactic dynamics [25,31] and to analyze phase mixing [51].…”
Section: Methodology and Outline Of The Papermentioning
confidence: 99%
“…As in the non-relativistic setting [25,31], the radial period function T and its properties are crucial to derive a Birman-Schwinger principle. We next show that this function is bounded and bounded away from zero on the steady state support for sufficiently small shells around a Schwarzschild black hole.…”
Section: The Periodic Particle Motions and The Period Functionmentioning
confidence: 99%
“…In the works [16]- [19] the authors developed a methodology use of an additional continuous variable in general relativistic dynamics, and the subsequent transition to the 7dimensional formalism based on the use of "observer time", weakening the need to introduce conditions on the energy manifold [6], [14] in canonical impulses. In this case, the expression for the total Hilbert-Einstein action and the Hamiltonian equations the movements take on a new form (using the formalism of particle distribution functions), as well as the expression for the energy-momentum tensor in Einstein's equations [20]- [26].…”
Section: Introductionmentioning
confidence: 99%