Symétrie (physique)

En physique la notion de symétrie, qui est intimement associée à la notion d'invariance, renvoie à la possibilité de considérer un même système physique selon plusieurs points de vue distincts en termes de description mais équivalents quant aux prédictions effectuées sur son évolution. Une théorie physique possède alors une symétrie S, si toute équation dans cette théorie décrit tout aussi correctement une particule ρ qu'une particule -ρ 'symétrique' de ρ. La symétrie S considérée peut porter sur la charge électrique de la particule, ou sur toute autre variable, ou combinaison de variables, intervenant dans ses équations. Cet article se propose de passer en revue les principaux types de symétries rencontrés en physique, de décrire brièvement leur implémentation formelle et enfin de présenter les mécanismes par lesquels une symétrie peut être brisée dans la nature, ce qui peut compliquer sa mise en évidence dans la pratique. Histoire de la notion de symétrie en physique

Tackling the Supersymmetric Flavour Problem in String Models

Christopher John Andrey

In this work we address one of the phenomenological issues of beyond the Standard Model scenarios which embed Supersymmetry, namely the Supersymmetric Flavour Problem, in the context of String Theory. Indeed, the addition of new interactions to the Standard Model generically spoils its flavour structure which is one of its major achievements since it for example leads to a very elegant understanding of the absence of flavour changing neutral currents in the leptonic sector and of the stability of the proton, thanks to accidental symmetries. We focus on a subset of the phenomenologically dangerous operators, namely the soft scalar masses. One way out of the Supersymmetric Flavour Problem is to geographically separate the observable and hidden sectors along a fifth dimension, gravity being the only interaction propagating in the bulk. In such scenarios, the soft scalar masses are vanishing at the classical level since there is no direct contact term between the observable and hidden multiplets and tend to be universal at the loop-level. However such setups hardly ever come about in String Theory, which is one of the most promising candidates of quantum gravity. In order to make contact with the five-dimensional picture, we focus on the prototypical case of the E8 × E8 Heterotic M-Theory which, in a certain regime, effectively looks five-dimensional and embeds matter fields on two end-of-the-world branes. In these scenarios, not only gravity but also vector multiplets propagate in the five-dimensional bulk, effectively spoiling the sequestered picture. However, since the contact terms responsible for the appearance of soft scalar masses arise due to the exchange of heavy vectors, they do enjoy a current-current structure which can be exploited to inhibit the emergence of soft scalar masses by postulating a global symmetry in the hidden sector. In order to assess the possibility of realising such a mechanism, we first study the full dependence of the Kähler potential on both the moduli and the matter fields in the case of orbifold and Calabi-Yau compactifications. We then determine whether an effective sequestering may be achieved thanks to a global symmetry and argue that whereas for orbifold models our strategy can naturally be put at work, it can only be implemented in a subset of Calabi-Yau models.

EPFL2011

Particle creation from non-topological solitons

Stephen Clark

Non topological solitons, Q balls can arise in many particle theories with U(1) global symmetries. As was shown by Cohen et al. [2], if the corresponding scalar field couples to massless fermions, large Q-balls are unstable and evaporate, producing a fermion flux proportional to the Q ball's surface. In this work we analyse Q-ball instabilities as a function of Q-ball size and fermion mass. In particular, we construct an exact quantum-mechanical description of the evaporating Q-ball. This new construction provides an alternative method to compute Q-Ball's evaporation rates. We shall also find a new expression for the upper bound on evaporation as a function of the produced fermion mass and study the effects of the size of the Q ball on particle production. We also analyse what happens if external fermion is scattered on a Q ball and demonstrate that it can be converted into antiparticle with a probability of the order of one. This result has important implications for astrophysical applications of dark matter Q balls.

EPFL2006

Tackling the Supersymmetric Flavour Problem in String Models

Christopher John Andrey

EPFL2011

Exploiting symmetries (in images) with graph neural networks

Tackling the Supersymmetric Flavour Problem in String Models

Particle creation from non-topological solitons

Tackling the Supersymmetric Flavour Problem in String Models

Particle creation from non-topological solitons

Exploiting symmetries (in images) with graph neural networks