Given an arithmetic function $\theta$, we consider the set
$$ \mathcal{B}_\theta = \Bigl\{n\ge 1: p|n \Rightarrow p\le \theta\Bigl(\prod_{q<p \atop q^\alpha || n} q^\alpha \Bigr) \Bigr\},$$
where $p$ and $q$ denote primes. Depending on the choice of $\theta$, the possible sets $\mathcal{B}_\theta$ include the set of prime powers, almost primes, friable numbers, dense numbers, and practical numbers.
We will discuss (1) asymptotic results for the counting function of $\mathcal{B}_\theta$, (2) a generalization of the Siegel-Walfisz theorem, and (3) the normal order of the number of prime factors of integers in $\mathcal{B}_\theta$.

Let G be a non-compact connected semisimple real Lie group with finite center. Suppose L is a non-compact connected closed subgroup of G acting transitively on a symmetric space G/H such that L\cap H is compact. We will describe the action on L/L\cap H of a Dirac operator D_{G/H}(E) acting on sections of an E-twist of the spin bundle over G/H. We will illustrate the results in an SL(2) example.  This is joint work with Salah Mehdi.

The quantum gauge theory is the current basis for explaining the interactions of elementary particles. Among the four fundamental interactions: electromagnetic, weak, strong, and gravitational, for the last two, a proper mathematical construction does not yet exist. Quantum gauge theory is based on three different branches of mathematics: 1) geometry, 2) group theory, and 3) functional analysis.

The strong interactions are studied in the SU(3) quantum Yang-Mills theory but an axiomatic QFT with the mass gap and color confinement does not yet exist. In the classical field theory model, the gluon^1 is a massless particle but one can not see the color-charge^2 of a particle in nature, and then the gluons must be in the bound states, forming massive particles. This is the mass gap problem. The mass gap is the difference in energy between the vacuum and the next lowest energy state. The energy of the vacuum is zero by definition, and the mass gap is the mass of the lightest particle. However, the color confinement postulated permits only bound states of gluons, it is an obvious contradiction.

In this presentation, I would like to discuss the fact that if we replace: 1)  Minkowskian geometry with the de Sitterian geometry, 2) Poincaré group with de Sitter group and 3) Hilbert space quantization with the Krein space quantization, an axiomatic quantum Yang-Mills theory with a mass gap and the color confinement can be constructed. It is important to note that the ambient space formalism allows us to make this construction possible.

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1 . A gluon is an elementary particle that acts as the exchange particle (or gauge boson) for the strong force between quarks.

2 . Color charge is a property of quarks and gluons that is related to the particles’ strong interactions in the theory of quantum chromodynamics

Considering partial character sums as defining a family of random processes (by choosing the characters randomly from some set), it becomes natural to ask questions about the limiting distribution. I’ll describe this in some contexts and give examples of what we can find in the support. This is largely work of Ayesha Hussain, but also some joint work.

If we have a flat vector bundle E over a compact manifold M, then we can form the de Rham cohomology H(M; E) of the M twisted by E. Given a Riemannian metric on M, this cohomology can be realised as the kernel of a Laplacian, via the Hodge theorem. Using the same Laplacian, In 1971, Ray and Singer defined the analytic torsion of M (now also assumed oriented), twisted by E. If H(M; E) vanishes, then analytic torsion is independent of the Riemannian metric used to define the Laplacian, and therefore a smooth invariant. Ray and Singer’s motivation for this definition was to give an analytic way to realise Reidemeister-Franz torsion, a combinatorial invariant of finite cell complexes. In 1978, Cheeger and Müller proved independently that these two notions of torsion are indeed equal. Fried’s conjecture from 1986 is a relation between analytic torsion and the Ruelle dynamical zeta function of a flow on M with suitable properties. That is a quantity involving the lengths of closed flow curves. So analytic torsion gives us a link between analysis, topology and dynamical systems. Most of this talk is a survey of analytic torsion. I will also mention some recent work with Hemanth Saratchandran on an equivariant version of analytic torsion for proper group actions.

Soit P un polynôme à coefficients entiers, unitaire, irréductible, de degré 4 et de groupe de Galois diédral ou cyclique.
Il existe c = c(P) > 0, tel que P(n) ait un facteur premier supérieur à n^1+c pour une proportion positive d’entiers n.

Il s’agit d’un travail  avec James Maynard.

Let I and J be two orthogonal respectively left and right coideal $*$-subalgebras of a dual pair of Hopf $*$-algebras. We define the Drinfeld double coideal of J and I. Next, we define for $0<q<1$ the unital $*$-algebra $U_q(sl(2,R))$, quantizing the universal enveloping $*$-algebra of $sl(2, R)$, as the Drinfeld double of the equatorial Podles sphere coideal $*$-subalgebra of $O_q(SU(2))$ and its associated orthogonal coideal $*$-subalgebra of $U_q(su(2))$. We finally classify its admissible irreducible $*$-representations.

Répétition du séminaire Bourbaki du vendredi 1er avril.

(Travail commun avec P. Delorme). Soit $G$ un groupe de Lie réductif réel, muni d’une involution $\sigma$ et $\Gamma$ un sous-groupe discret cocompact. Nous établissons une formule des traces relative, en lien avec $\Gamma$ et $H=G^\sigma$, exprimant la somme de  certaines intégrales orbitales de $f\in C_c^\infty(G)$ en terme de  coefficients généralisés de représentations unitaires irréductibles de $G$. Lorsque $G/H$ admet une série discrète relative $\pi_0$, l’existence de pseudocoefficient relatif pour $\pi_0$ à support “petit” implique, via la formule des traces relative,  que $\pi_0$ intervient dans la décomposition spectrale de $L^2(\Gamma\backslash G)$. Nous étudions l’existence de tels pseudocoefficients pour les espaces hyperboliques et les espaces symétriques de type $G(\mathbb{C})/G(\mathbb{R})$.