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. La formulation actuelle a été finalisée au milieu des années 1970 à la suite de la confirmation expérimentale des quarks. Depuis, les découvertes du quark top (1995), du neutrino tauique (2000) et du boson de Higgs (2012) ont donné encore plus de crédibilité au modèle standard. Toutes les particules du modèle standard ont désormais été observées expérimentalement. Par son succès à expliquer une large variété de résultats expériment
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La physique des particules ou la physique subatomique est la branche de la physique qui étudie les constituants élémentaires de la matière et les rayonnements, ainsi que leurs interactions. On l'app
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
En physique des particules, un quark est une particule élémentaire et un constituant de la matière observable. Les quarks s'associent entre eux pour former des hadrons, particules composites, dont l
The goal of the course is to introduce relativistic quantum field theory as the conceptual and mathematical framework describing fundamental interactions.
Presentation of the electroweak and strong interaction theories that constitute the Standard Model of particle physics. The course also discusses the new theories proposed to solve the problems of the Standard Model.
New massive long-lived particles (LLP) are predicted by multiple beyond the Standard Model theories. This thesis presents the search of such long-lived particles decaying leptonically in the eμν final state. The search is performed using 2.31 fb−1 of proton-proton collisions collected by the LHCb detector at a center-of-mass energy of s=13 TeV, seeking for displaced vertices of electrons and muons of opposite charges.LLPs with masses between 7 to 50 GeV/c2, and lifetime between 2 and 50 ps, are explored in this search.
Three kinds of LLP production modes are considered: the direct pair production of LLPs from quark interactions, the pair production from a Standard Model like Higgs boson with a mass of 125 GeV/c2, and charged current production from an on-shell W boson with an additional lepton.No evidence of these long-lived states has been observed, upper limits at 95% CL on the production cross-section times branching ratio have been set on the different production mode.
This thesis work presents lifetime measurements of heavy-flavour mesons made with semileptonic B0 and Bs0 decays based on 3fb−1 of data collected with the LHCb detector in proton-proton collisions at centre-of-mass energies of 7 and 8 TeV. The study of meson lifetimes is important to constrain phenomenological models for hadronic interactions based on the Standard Model of particle physics. Better understanding of hadronic interactions is essential for making precise predictions, which can then be confronted to experimental data in order to look for signs of physics beyond the Standard Model.We measure the differences between the decay widths of the Bs0 and B0 mesons, Δ(B), and between that of the Ds− and D− mesons, Δ(D), by analysing approximately 410000 Bs0→Ds(∗)−μ+νμ and 110000 B0→D(∗)−μ+νμ decays, which are partially reconstructed in the same K+K−π−μ+ final state. We measure
Δ(B)=−0.0115±0.0053(stat)±0.0041(syst)ps−1
and
Δ(D)=1.0131±0.0117(stat)±0.0065(syst)ps−1.
Using the obtained values of Δ(D) and Δ(B) and the B0 and D− lifetimes as external inputs, we obtain a measurement of the flavour-specific Bs0 lifetime,
τsfs=1.547±0.013(stat)±0.010(syst)±0.004(τB0)ps,
and of the Ds− lifetime,
τDs−=0.5064±0.0030(stat)±0.0017(syst)±0.0017(τD−)ps,
where the last uncertainties originate from the limited knowledge of the B0 and D− lifetimes, respectively. Both results are compatible with, and improve upon, previous determinations.A feasibility study of a D0 lifetime measurement is performed, by measuring the difference between the decay widths of the D0 and D− mesons, Δ(D)′. We reconstruct approximately 2.2×106B0→D∗−(→Dˉ0(→K+π−)π−)μ+νμ and 1.6×106B0→D(∗)−(→K+π−π−(X))μ+νμ decays. We measure
Δ(D)′=1.4644±0.0043(stat)±0.0132(syst)ps−1
and with the D− lifetime as external input, we get an estimate of the D0 lifetime,
τD0=0.4122±0.0007(stat)±0.0022(syst)±0.0011(τD−)ps.
This result is compatible with, but less precise than, current precision and thus validates the method. We discuss possible improvements with larger simulation samples and data sets.
This thesis presents the results of a time-dependent analysis of B0→D∓π± decays using 3fb−1 of
proton-proton collision data collected
with the LHCb detector at CERN's Large Hadron Collider during Run 1 with a centre-of-mass energy of 7 (2011) and 8 (2012) TeV.
The LHCb experiment is dedicated to the study of the properties
of b-flavoured hadrons, in particular CP violation in the B meson system.
The Standard Model of Particle Physics
describes very precisely the mechanism and the amount of CP violation expected in the Universe.
However, the observed matter-antimatter asymmetry is larger by several order of magnitude
compared to the predictions. This could be explained by the existence of a new source of CP violation, originating in
New Physics beyond the Standard Model.
The time-dependent analysis of B0→D∓π± decays provides constraints on
the angle γ of the Unitarity Triangle, one of the fundamental parameters
of the Standard Model related to CP violation. Since no sizeable high-order Standard Model processes are expected to contribute,
any deviation from the predictions would be an unambiguous signature
of New Physics.
The current experimental precision on γ is significantly lower than that of theoretical predictions.
This motivates the effort for new experimental determinations of γ in order to reduce its uncertainty.
The analysis of \Bz→\Dmp\pipm decays, although not as sensitive as that obtained from decays of
charged B mesons into D(∗)0K(∗)+ final states, represents an independent and uncorrelated estimation of γ
that contributes to the global combination of all γ measurements. The result obtained in this thesis is more precise than previous
determinations from other experiments (BaBar, Belle) using B0→D∓π± decays.
Although based on a very large sample of about half a million signal events, it is still dominated by statistical uncertainties,
indicating good prospects for future improvements in precision with more data from Run 2 and beyond.
In addition to the B0→D∓π± analysis, this thesis also summarizes the studies to improve the
performances of the flavour tagging algorithms used by the LHCb collaboration to infer
the flavour of neutral B mesons in time-dependent analyses.
The performance of these algorithms, being correlated with the kinematics of the reconstructed particles
as well as the complexity of the event (number of tracks and primary vertices), showed a significant
decrease on Run 2 data (2015--2018), which were collected at a centre-of-mass energy of 13TeV.
Thanks to new implementations, these algorithms now have a performance similar to that
obtained with Run 1 data.