Physique au-delà du modèle standard

La physique au-delà du modèle standard se rapporte aux développements théoriques de la physique des particules nécessaires pour expliquer les défaillances du modèle standard, telles que l'origine de la masse, le problème de la violation CP de l'interaction forte, les oscillations des neutrinos, l'asymétrie matière-antimatière, et la nature de la matière noire et de l'énergie noire. Un autre problème réside dans le cadre mathématique du modèle standard lui-même : son incompatibilité avec celui de la relativité générale, au point que l'une ou l'autre ou les deux théories deviennent inopérantes face à certaines conditions, par exemple les singularités gravitationnelles connues de l'espace-temps comme le Big Bang ou l'horizon des événements des trous noirs. Les théories au-delà du modèle standard comprennent de nombreuses extensions du modèle standard jusqu'à la supersymétrie, telles que le modèle standard supersymétrique minimal (en abrégé MSSM pour Minimal Supersymmetric Standard Model) et le Modèle standard supersymétrique quasi-minimal (NMSSM pour Next to Minimal Supersymmetric Standard Model), ou des explications entièrement nouvelles telles que la théorie des cordes, la théorie M et les dimensions supplémentaires. Comme ces théories s'efforcent de reproduire l'intégralité de phénomènes ordinaires, l'identification de celle qui est correcte, ou au moins celle qui constitue la « meilleure avancée » vers la théorie du tout, peut seulement être réglée expérimentalement et constitue l'un des champs de recherche les plus actifs tant en physique théorique qu'en physique expérimentale. 400px|thumbnail|right|Le Modèle standard des particules élémentaires. Bien qu'il constitue la théorie physique la plus réussie à ce jour, le modèle standard n'est pas parfait. Une grande partie des résultats publiés par les physiciens théoriciens consiste à proposer différentes formes d'une nouvelle physique « au-delà du modèle standard », qui modifieraient le modèle standard de façon suffisamment subtile pour qu'il reste compatible avec les données existantes, tout en y apportant des rectifications suffisamment substantielles pour prédire les résultats selon le « modèle non standard » de nouvelles expériences qui seraient proposées.

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Catégories associées (17)

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Personnes associées (62)

Publications associées (3)

Axion

L’axion est une particule hypothétique, supposée stable, neutre et de très faible masse (entre quelques μeV et quelques meV). Son existence découle de la (1977) au problème de violation de la symétrie CP en chromodynamique quantique, située au CERN, mais aussi ADMX et beaucoup d'autres. Comme l'a montré Gerard 't Hooft, la chromodynamique quantique prédit que quelques interactions fortes violeront la symétrie charge+parité.

Weakly interacting massive particles

En astrophysique, les WIMPs (acronyme anglais pour Weakly Interacting Massive Particles, pouvant se traduire par « particules massives interagissant faiblement ») sont des particules hypothétiques constituant une solution au problème de la matière noire. En dehors des interactions gravitationnelles, ces particules interagissent très faiblement avec la matière ordinaire (nucléons, électrons), leur section efficace d'interaction est de l'ordre du picobarn.

Lightest supersymmetric particle

In particle physics, the lightest supersymmetric particle (LSP) is the generic name given to the lightest of the additional hypothetical particles found in supersymmetric models. In models with R-parity conservation, the LSP is stable; in other words, it cannot decay into any Standard Model particle, since all SM particles have the opposite R-parity. There is extensive observational evidence for an additional component of the matter density in the universe, which goes under the name dark matter.

Exploring beyond the Standard Model: the Heavy and the Dark

Kin Shanho Eliaou Mimouni

Physics beyond the Standard Model can appear as new particles too heavy to be produced in experiments (the energy frontier) or interacting too weakly to be seen in our measurements (the intensity frontier). In the first part of this thesis, we study two dark matter models of electroweak WIMP coming from two limiting cases in the MSSM: the Higgsino and the Wino model. The dark matter candidate is a particle too heavy to be directly seen in colliders but it could be seen indirectly by astrophysical observations. Dark matter particles in the galaxy can annihilate to Standard Model particles and be detected by satellites. We consider the charged neutral mass splitting as a free parameter in the theory and investigate its effect on the Sommerfeld enhancement which gives an important boost to the annihilation cross-section, the main observable of indirect detection. In the second part of this thesis, we present an idea of a fixed target experiment so search for dark sector models, a class of model with very weakly interacting particles. This experiment uses the experimental setup needed for a future muon collider but is independent from the muon collider program. We study the reach of our experiment for three benchmark models, the dark photon, the dark Higgs, the heavy neutral lepton and we compare its expected performances to current and future experiments. In the third part of this thesis, we consider a more model-independent approach to the search for new physics. If new states are heavy, they can be integrated out and their leading effects are encoded in effective operators made of Standard Model fields. Assuming baryon and lepton number conservation, one can classify the effective operators of dimension-6 which give the leading contribution and constrain the coefficient of these operators by looking at precision observables. We compile results from LEP-I and LEP-II experiments as well as neutrino scattering and other low-energy observables. We allow all operators to be present with an arbitrary flavour structure. Our result can then be used to translate these constaints to specific models of new physics.

EPFL2019

A search for heavy long-lived staus in the LHCb detector at √s = 7 and 8 TeV

Thi Viet Nga La

The Large Hadron Collider (LHC) has been producing pp collisions at 7 and 8 TeV since 2010 and promises a new era of discoveries in particle physics. One of its experiments, the Large Hadron Collider beauty (LHCb) experiment, was constructed to study CP violation in the B meson system. In addition to B physics, new Physics beyond the Standard Model can also be searched for at this single-arm forward spectrometer. With the different sub-detectors and the high resolution of the tracking system, the LHCb detector has the ability to search for heavy, long-lived and charged particles, which are predicted by extensions of the Standard Model. One of these extensions, the minimal Gauge Mediated Supersymmetry Breaking (mGMSB), proposes such a particle, named stau (τ~) - the SUSY bosonic counterpart of the heavy lepton tau (τ). The theory proposes that the staus may be pair-produced in pp collisions or in the decays of heavier particles, and have only electromagnetic interactions with the atoms of the medium like the muons. Therefore, we expect that at the energy of the LHC these particles can be produced if they do exist and that we have a chance to discover them at LHCb, as well as at the other experiments of the LHC. This thesis is dedicated to the search for stau pairs produced in pp collisions at the centre-of-mass energies √s = 7 and 8 TeV in the LHCb detector. For this purpose, we generated the stau pairs with seven different particle masses ranging from 124 to 309 GeV/c2 and simulated their path through the LHCb detector, as well as their muon background from the decays Z0, γ∗ → μ+μ−. Based on the results from the simulation, a set of cuts are then defined to select the stau pairs. Some muon pairs at high energies will also pass the selection cuts. Thus, to separate the stau pairs from the muon pairs, the Neural Network technique has been used. A first Neural Network has been used to distinguish the stau tracks from the muon tracks using their signals left in the sub-detectors: the VELO silicon detector, the electromagnetic calorimeter, the hadron calorimeter and the RICH detectors. Then, two methods to select the stau pairs have been developed: the first one is based on the product of the two responses from the first Neural Network (NN1) for the two tracks, the second one employs a second Neural Network to separate the stau pairs from the muon pairs by using the above product of the two NN1 responses and the invariant mass of pair. Finally, a favourable region for the staus finding has been defined and the expected numbers of stau and muon pairs in this region have been evaluated. The training of the Neural Network has been achieved with the Monte Carlo variables, then the trained Neural Network has been used to classify the data. The data used in our work were collected by the LHCb experiment in 2011 and 2012 and correspond to integrated luminosities of 1 fb−1 at √s = 7 TeV and of 2 fb−1 at √s = 8 TeV. No significant excess of signal has been observed. Upper limits at 95% CL on the cross section for stau pair production in pp collisions at √s = 7 and 8 TeV have been computed by using the profile likelihood method, which is derived from the well known Feldman and Cousins method.

EPFL2013

Vacuum Stability in Supersymmetric Effective Theories

Leonardo Brizi

The main topics discussed in this thesis are supersymmetric low-energy effective theories and metastability conditions in generic non-renormalizable models with global and local supersymmetry. In the first part we discuss the conditions under which the low-energy expansion in space-time derivatives preserves supersymmetry implying that heavy multiplets can be more efficiently integrated out directly at the superfield level. These conditions translate into the requirements that also fermions and auxiliary fields should be small compared to the heavy mass scale. They apply not only to the matter sector, but also to the gravitational one if present, and imply in that case that the gravitino mass should be small. We finally give a simple prescription to integrate out heavy chiral and vector superfields consisting respectively in imposing stationarity of the superpotential and of the Kähler potential; the procedure holds in the same form both for global and local supersymmetry. In the second part we study general criteria for the existence of metastable vacua which break global supersymmetry in models with local gauge symmetries. In particular we present a strategy to define an absolute upper bound on the mass of the lightest scalar field which depends on the geometrical properties of the Kähler target manifold. This bound can be saturated by properly tuning the superpotential and its positivity therefore represents a necessary and sufficient condition for the existence of metastable vacua. It is derived by looking at the subspace of all those directions in field space for which an arbitrary supersymmetric mass term is not allowed and scalar masses are controlled by supersymmetry-breaking splitting effects. This subspace includes not only the direction of supersymmetry breaking, but also the directions of gauge symmetry breaking and the lightest scalar is in general a linear combination of fields spanning all these directions. Our purpose is to show that the largest value for the lightest mass is in general achieved when the lightest scalar is a combination of the Goldstone and the Goldstino partners. We conclude by computing the effects induced by the integration of heavy multiplets on the light masses. In particular we focus on the sGoldstino partners and we show that heavy chiral multiplets induce a negative level-repulsion effect that tends to compromise vacuum stability, whereas heavy vector multiplets in general induce a positive-definite contribution. Our results find application in the context of string-inspired supergravity models, where metastability conditions can be used to discriminate among different compactification scenarios and supersymmetric effective theories can be used to face the problem of moduli stabilization.

EPFL2011

Modèle standard de la physique des particules

vignette|upright=2.0|Modèle standard des particules élémentaires avec les trois générations de fermions (trois premières colonnes), les bosons de jauge (quatrième colonne) et le boson de Higgs (cinquième colonne). Le modèle standard de la physique des particules est une théorie qui concerne l'électromagnétisme, les interactions nucléaires faible et forte, et la classification de toutes les particules subatomiques connues. Elle a été développée pendant la deuxième moitié du , dans une initiative collaborative mondiale, sur les bases de la mécanique quantique.

Physical cosmology

La cosmologie quantique est une branche spéculative de la cosmologie qui vise à décrire les premiers instants de l'Univers en le considérant comme un objet quantique, c'est-à-dire décrit par les lois de la mécanique quantique et de la théorie quantique des champs. Cette discipline peut être vue comme une branche de la gravité quantique, quoique la connaissance d'une théorie quantique de la gravitation ne soit pas indispensable pour certains résultats de la cosmologie quantique.

Théorie quantique des champs

vignette|296x296px|Ce diagramme de Feynman représente l'annihilation d'un électron et d'un positron, qui produit un photon (représenté par une ligne ondulée bleue). Ce photon se décompose en une paire quark-antiquark, puis l'antiquark émet un gluon (représenté par la courbe verte). Ce type de diagramme permet à la fois de représenter approximativement les processus physiques mais également de calculer précisément leurs propriétés, comme la section efficace de collision.