ID: 0909.1735

Infinite Dimensional Multiplicity Free Spaces III: Matrix Coefficients and Regular Functions

September 9, 2009

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Some harmonic analysis on commutative nilmanifolds

September 21, 2019

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Andrea L. Gallo, Linda. V. Saal
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In this work, we consider a family of Gelfand pairs $(K \ltimes N, N)$ (in short $(K,N)$) where $N$ is a two step nilpotent Lie group, and $K$ is the group of orthogonal automorphisms of $N$. This family has a nice analytic property: almost all these 2-step nilpotent Lie group have square integrable representations. In this cases, following Moore-Wolf's theory, we find an explicit expression for the inversion formula of $N$, and as a consequence, we decompose the regular acti...

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Von Neumann Dimensions and Trace Formulas I: Limit Multiplicities

June 5, 2023

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Jun Yang
Representation Theory
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Given a connected semisimple Lie group $G$ and an arithmetic subgroup $\Gamma$, it is well-known that each irreducible representation $\pi$ of $G$ occurs in the discrete spectrum $L^2_{\text{disc}}(\Gamma\backslash G)$ of $L^2(\Gamma\backslash G)$ with at most a finite multiplicity $m_{\Gamma}(\pi)$. While $m_{\Gamma}(\pi)$ is unknown in general, we are interested in its limit as $\Gamma$ is taken to be in a tower of lattices $\Gamma_1\supset \Gamma_2\supset\dots$. For a boun...

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Lie-Poisson theory for direct limit Lie algebras

September 22, 2013

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Mark Colarusso, Michael Lau
Representation Theory

In this paper, we develop the fundamentals of Lie-Poisson theory for direct limits $G=\dirlim G_{n}$ of complex algebraic groups $G_{n}$ and their Lie algebras $\fg=\dirlim \fg_{n}$. We show that $\fg^{*}=\invlim\fg_{n}^{*}$ has the structure of a Poisson provariety and that each coadjoint orbit of $G$ on $\fg^{*}$ has the structure of an ind-variety. We construct a weak symplectic form on every coadjoint orbit and prove that the coadjoint orbits form a weak symplectic foliat...

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Regular Representations of Time-Frequency Groups

January 22, 2013

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Azita Mayeli, Vignon Oussa
Representation Theory

In this paper, we study the Plancherel measure of a class of non-connected nilpotent groups which is of special interest in Gabor theory. Let $G$ be a time-frequency group. More precisely, that is $G=\left\langle T_{k},M_{l}:k\in\mathbb{Z}^{d},l\in B\mathbb{Z}^{d}\right\rangle ,$ $T_{k}$, $M_{l}$ are translations and modulations operators acting in $L^{2}(\mathbb{R}^{d}),$ and $B$ is a non-singular matrix. We compute the Plancherel measure of the left regular representation o...

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Stepwise Square Integrable Representations: the Concept and Some Consequences

November 29, 2015

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Joseph A. Wolf
Representation Theory
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There are some new developments on Plancherel formula and growth of matrix coefficients for unitary representations of nilpotent Lie groups. These have several consequences for the geometry of weakly symmetric spaces and analysis on parabolic subgroups of real semisimple Lie groups, and to (infinite dimensional) locally nilpotent Lie groups. Many of these consequences are still under development. In this note I'll survey a few of these new aspects of representation theory for...

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Finite matrix multiplication algorithms from infinite groups

October 19, 2024

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Jonah Blasiak, Henry Cohn, Joshua A. Grochow, ... , Umans Chris
Group Theory
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The Cohn-Umans (FOCS '03) group-theoretic framework for matrix multiplication produces fast matrix multiplication algorithms from three subsets of a finite group $G$ satisfying a simple combinatorial condition (the Triple Product Property). The complexity of such an algorithm then depends on the representation theory of $G$. In this paper we extend the group-theoretic framework to the setting of infinite groups. In particular, this allows us to obtain constructions in Lie gro...

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Regularity of the Radon-Nikodym Derivative of a Convolution of Orbital Measures on Noncompact Symmetric Spaces

July 22, 2021

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Boudjemaa Anchouche
Representation Theory

Let $G/K$ be a Riemannian symmetric space of noncompact type, and let $\nu_{a_j}$, $j=1,...,r$ be some orbital measures on $G$ (see the definition below). The aim of this paper is to study the $L^{2}$-regularity (resp. $C^k$-smoothness) of the Radon-Nikodym derivative of the convolution $\nu_{a_{1}}\ast...\ast\nu_{a_{r}}$ with respect to a fixed left Haar measure $\mu_G$ on $G$. As a consequence of a result of Ragozin, \cite{ragozin}, we prove that if $r \geq \, \max_{1\leq i...

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Direct limits of infinite-dimensional Lie groups

March 1, 2008

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Helge Glockner
Group Theory
Functional Analysis

Many infinite-dimensional Lie groups of interest can be expressed as a union of an ascending sequence of (finite- or infinite-dimensional) Lie groups. In this survey article, we compile general results concerning such ascending unions, describe the main classes of examples, and explain what the general theory tells us about these. In particular, we discuss: (1) Direct limit properties of ascending unions of Lie groups in the relevant categories; (2) Regularity in Milnor...

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An orbit model for the spectra of nilpotent Gelfand pairs

March 26, 2018

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Holley Friedlander, William Grodzicki, Wayne Johnson, Gail Ratcliff, Anna Romanov, ... , Wessel Brent
Representation Theory

Let $N$ be a connected and simply connected nilpotent Lie group, and let $K$ be a subgroup of the automorphism group of $N$. We say that the pair $(K,N)$ is a nilpotent Gelfand pair if $L^1_K(N)$ is an abelian algebra under convolution. In this document we establish a geometric model for the Gelfand spectra of nilpotent Gelfand pairs $(K,N)$ where the $K$-orbits in the center of $N$ have a one-parameter cross section and satisfy a certain non-degeneracy condition. More specif...

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Sampling Theorems for Some Two-Step Nilpotent Lie Groups

June 30, 2013

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Vignon Oussa
Representation Theory

Let $N$ be a simply connected, connected nilpotent Lie group with the following assumptions. Its Lie Lie algebra $\mathfrak{n}$ is an $n$-dimensional vector space over the reals. Moreover, $\mathfrak{n=z}\oplus\mathfrak{b}\oplus\mathfrak{a}$, $\mathfrak{z}$ is the center of $\mathfrak{n}$, $\mathfrak{z} =\mathbb{R}Z_{n-2d}\oplus\mathbb{R}Z_{n-2d-1}\oplus\cdots\oplus \mathbb{R}Z_{1}, \mathfrak{b} =\mathbb{R}Y_{d}\oplus\mathbb{R} Y_{d-1}\oplus\cdots\oplus\mathbb{R}Y_{1}, \mathf...

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