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Institute
- Mathematik (373) (remove)
Über Elementarkettenbrüche, lineare Substitutionen und indefinite binäre quadratische Formen : II.
(1921)
Über Elementarkettenbrüche, lineare Substitutionen und indefinite binäre quadratische Formen : I.
(1919)
Gegenstand dieser Arbeit sind Galoisoperationen auf quasiplatonischen Riemannschen Flächen mit einer Automorphismengruppe isomorph zu PSL(2,F(q)). Quasiplatonische Riemannsche Flächen werden durch torsionsfreie Normalteiler N in einer Dreiecksgruppe D uniformisiert, d.h. N ist die universelle Überlagerungsgruppe und die Flächen, die man auch als algebraische Kurven beschreiben kann, sind isomorph zu N\U, wenn U die obere Halbebene bezeichnet. Bzgl. der Größe der Automorphismengruppen bilden die quasiplatonischen Kurven die lokalen Maxima im Modulraum. Die absoluten Maxima liegen bei den Hurwitz-Kurven; hier hat die Automorphismengruppe die maximale Größe von 84(g-1), wenn g>1 das Geschlecht der Kurve ist. Der Normalisator in PSL(2,R) der Überlagerungsgruppe N ist dann die Dreiecksgruppe mit Signatur (2,3,7). Macbeath hat die Bedingungen dafür gefunden, wann PSL(2,F(q)) eine Hurwitz-Gruppe ist. Von besonderem Interesse ist dabei der Fall, dass q=p eine Primzahl kongruent +-1 mod 7 ist. Hier hat man drei nicht-isomorphe Kurven, die jedoch alle galoiskonjugiert zueinander sind. In der Arbeit werden Bedingungen angegeben, unter denen sich dieses Resultat auf Dreiecksgruppen D mit einer Signatur der Form (2,m_1,m_2) verallgemeinern lässt. Dabei gehen einerseits Ergebnisse von Frye ein, der die Anzahl der verschiedenen torsionsfreien Normalteiler N<D mit Quotienten PSL(2,F(q)) über die Spurtupel der Erzeugenden von D bestimmt hat. Andererseits wird eine Methode von Streit verwendet, mit der man die Galoisoperation auf den Kurven anhand des Verhaltens der Multiplikatoren der Erzeugenden in der Automorphismengruppe nachvollziehen kann. Es zeigt sich, dass sich Spur- und Multiplikatortupel entsprechen, woraus man die Anzahl und Länge der Galois-Orbits erhält. Außerdem lässt sich der Definitionskörper der Kurven bestimmen. Offen bleibt das genaue Verhalten bei Signaturen (m_0,m_1,m_2) mit m_i ungleich 2 für alle i. Hier gibt es zu jedem Multiplikatortupel zwei verschiedene Spurtupel. Kann man die Kurven durch die Multiplikatoren beschreiben, dann erhält man Projektionen D->>PSL(2,F(q)) auch über die Quaternionenalgebra, die die Dreiecksgruppe über ihrem Spurkörper erzeugt. Die Normalteiler erweisen sich dann als Schnitt der Dreiecksgruppe mit einer Hauptkongruenzuntergruppe nach einem Primideal P|char(F(q)) in der Norm-1-Gruppe einer Ordnung der Quaternionenalgebra. Dabei ist das Spurtripel in PSL(2,F(q)) gerade das Spurtripel aus D modulo P. Ändert man P, so erhält man ein anderes Spurtripel in PSL(2,F(q)), also auch einen anderen Normalteiler. Bilden die zugehörigen Kurven eine Bahn unter der Galoisoperation, dann ergeben sich alle Normalteiler auf diese Weise. Die Galoisoperation auf den Tripeln der Multiplikatoren, also die Galoisoperation auf den Kurven, ist verträglich mit der Operation, die die Primideale P|char(F(q)) permutiert. Wir erhalten also eine natürliche Korrespondenz zwischen der Galoisoperation auf den Kurven einerseits und der Operation auf den Primidealen andererseits.
Mixed volumes, mixed Ehrhart theory and applications to tropical geometry and linkage configurations
(2009)
The aim of this thesis is the discussion of mixed volumes, their interplay with algebraic geometry, discrete geometry and tropical geometry and their use in applications such as linkage configuration problems. Namely we present new technical tools for mixed volume computation, a novel approach to Ehrhart theory that links mixed volumes with counting integer points in Minkowski sums, new expressions in terms of mixed volumes of combinatorial quantities in tropical geometry and furthermore we employ mixed volume techniques to obtain bounds in certain graph embedding problems.
Die vorliegende Arbeit untersucht ausgewählte Eigenschaften von Preferential Attachment-Graphen. Darunter verstehen wir eine Klasse komplexer zufälliger Graphen, die mit einer vorgegebenen Konfiguration gestartet werden und anschließend mit jedem Zeitschritt um eine Ecke und m Kanten wachsen. Die Wachstumsregeln sind so gestaltet, dass eine neue Ecke ihre Kanten bevorzugt an Ecken sendet, die bereits mit vielen anderen Ecken verbunden sind, woraus sich die Bezeichnung Preferential Attachment (PA) ableitet. Die Arbeit stellt zunächst heuristisch die Eigenschaft der Skalenfreiheit von PA-Modellen vor und bespricht anschließend einen Beweis zu dieser These. Weiter betrachten wir den Durchmesser von PA-Graphen und untersuchen das Verhalten bei Anwachsen des Graphen. Wir erkennen, dass der Durchmesser bei wachsendem Graphen deutlich langsamer wächst, was wir als Small World-Phänomen bezeichnen. Die zentralen Aussagen und Beweise orientieren sich an den Arbeiten von Remco van der Hofstad, der die bekannten PA-Modelle um einen Parameter erweitert hat. Damit ist es möglich, sowohl logarithmische als auch doppelt-logarithmische Schranken für den Durchmesser zu erhalten.
Local interactions between particles of a collection causes all particles to reorganize in new positions. The purpose of this paper is to construct an energy-based model of self-organizing subgroups, which describes the behavior of singular local moves of a particle. The present paper extends the Hegselmann-Krause model on consensus dynamics, where agents simultaneously move to the barycenter of all agents in an epsilon neighborhood. The Energy-based model presented here is analyzed and simulated on finite metric space. AMS Subject Classifications:81T80; 93A30; 37M05; 68U20
Deformation quantization on symplectic stacks and applications to the moduli of flat connections
(2008)
It is a common problem in mathematical physics to describe and quantize the Poisson algebra on a symplectic quotient [...] given in terms of some moment map [...] on a symplectic manifold [...] with a hamiltonian action by a Lie group G. Among others, problems may arise in two parts of the process: c might be a singular value of the moment map and the quotient might not be well-behaving; in the interesting cases the quotient often is singular. By the famous result of Sjamaar and Lerman ([102]) X is a symplectic stratified space. We are interested in cases for which we can give a deformation quantization of the possibly singular Poisson algebra of X. To that purpose we introduce a Poisson algebra on the associated stack [...] for special cases and consider its deformations and their classification. We dedicate ourselves to use the rather geometric methods introduced by Fedosov for symplectic manifolds in [37]. That leads to the question how to perform differential geometry on a smooth stack. The Lie groupoid atlas of a smooth stack is a nice model for the same space (Tu, Xu and Laurent-Gengoux in [107] and Behrend and Xu in [16]), but both have different topoi. We give a morphism (P,R) that compares the topologies of a smooth stack and its atlas. This yields a method to transport sheaves and their sections between a smooth stack and its Lie groupoid atlas. A symplectic stack is a smooth separated Deligne-Mumford stack with a 2-form which is closed and non-degenerate in an atlas. Via (P,R) a deformation quantization on a symplectic stack can be performed in terms of an atlas. We also give a classification functor for the quantizations in the spirit of Deligne ([35]) based on the geometric interpretation given by Gutt and Rawnsely in [49]. As an application we give a deformation quantization for the moduli stack of flat connections in particular configurations. We use Darboux charts provided by Huebschmann (e.g. in [54]) to construct the corresponding Lie groupoid. This captures the symplectic form arising in the reduction process and differs from other approaches using gerbes of bundles (e.g. Teleman [105]).
In this work, we extend the Hegselmann and Krause (HK) model, presented in [16] to an arbitrary metric space. We also present some theoretical analysis and some numerical results of the condensing of particles in finite and continuous metric spaces. For simulations in a finite metric space, we introduce the notion "random metric" using the split metrics studies by Dress and al. [2, 11, 12].