Tesis sobre el tema "B mesons Quantum chromodynamics"

This thesis uses a variety of numerical and statistical techniques to perform high precision calculations in high energy physics using quantum field theory. It introduces the experimental motivation for the calculation of B meson form factors and includes a discussion of previous work. It then describes the modern theoretical framework describing these phenomena, outlining quantum chromodynamics and electroweak theory, and then illustrating the procedure of gauge fixing, the quantum effective action and background field gauge which is required for subsequent perturbative work. Details of the basic methodology of lattice quantum field theory are given as well as the specific formulation of the relativistic theory and nonrelativistic approximations used in this work to describe quantum chromodynamics. A comprehensive calculation of the zero recoil B to D* form factor is then presented, using state of the art lattice techniques with relativistic charm sea quarks and light sea quarks with correct physical masses, leading to a discussion of the dominant sources of uncertainty and possible resolutions of experimental tensions. Also included is preliminary work towards the full calculation of nonzero recoil matrix elements, with the aim of outlining possible future work. Finally, this thesis presents the computation of parameters correcting for radiative one loop phenomena and corrections to the kinetic coupling parameters in nonrelativistic quantum chromodynamics in order to achieve a desirable level of precision in future calculations. This is done using Monte-Carlo integration to evaluate integrals from diagrams generated using automated lattice perturbation theory in background field gauge in order to match the coefficients of the effective action between the lattice and the continuum.

We analyze the hadronic phase of QCD using effective thermal field theory techniques. Our goal is to investigate the medium created in heavy ion collisions by calculating the electromagnetic emissivity of strongly interacting matter in the hadronic phase. We proceed through examining the vector meson properties in a thermal bath where the temperature reaches deconfinement and chiral symmetry is restored. In particular we observe the behavior of the rho spectral function in thermal medium and use it as a probe to examine the thermal environment generated in the collision.

We study the hadronic phase of Quantum Chromodynamics within a formalism that uses strongly interacting resonances in the Regge theory approach. Our aim is to investigate the properties of the medium created in a relativistic nucleus-nucleus collision, using the electromagnetic decays of vector mesons as probe. To do so, we first layout the foundations of Regge theory, which is then used to calculate the in-medium properties of vector mesons. This methodology will be used to calculate for the first time the properties of the &phis; meson in a hadronic medium. The properties are contained within the imaginary part of the propagator (IMPP). Since it is related to electromagnetic decay via vector meson dominance, the IMPP is a probe of strongly interacting hadron gas created in the collision.

Orientador: Adriano Antonio Natale
Banca: Atílio Cucchieri
Banca: Márcio José Menon
Banca: Maria Beatriz de Leone Gay Ducati
Banca: Rogério Rosenfeld
Resumo: Através da solução das equações de Schwinger-Dyson (ESD) é possível estudar diversos aspectos importantes da QCD não-perturbativa como confinamento e quebra de simetria quiral; desta forma as ESD são, obviamente, muito interessantes para estudo da fenomenologia das interações hadrônicas. Após uma breve revisão sobre equações de Schwinger-Dyson (ESD) e sobre algumas soluções da ESD do propagador do glúon disponíveis na literatura, apresentamos possíveis testes fenomenológicos para estas soluções. Observaremos que apenas uma das soluções apresentadas descreve satisfatoriamente os dados experimentais, e esta solução é compatível com uma massa dinâmica para o glúon. Finalizando, supomos que o glúon têm uma massa dinâmica e calculamos seus efeitos sobre os decaimentos de quarkônios pesados
Abstract: Through the solution of Schwinger-Dyson equations (SDE) it is possible to study important features of nonperturbative QCD such as confinement and chiral symmetry breaking; in this way SDE are, obviously, very interesting for the study of phenomenology of hadronic interactions. After a brief review on SDE and some Solutions of gluon propagator SDE available in literature, we present possible phenomenological tests for these solutions. We shall observe that only one of the solutions presented describes satisfactorily the experimental data, and such solution is compatible with a dynamical mass for the gluon. Eventually, we assume that the gluon has a dynamical mass and calculate its effects on heavy quarkonia decays
Doutor

La recherche indirecte des effets de la physique au-delà du Modèle Standard à travers les processus de la saveur est complémentaire aux efforts au LHC pour observer directement la nouvelle physique. Dans cette thèse nous discutons plusieurs scénarios au-delà du Modèle Standard (a) en utilisant une approche basée sur les théories de champs effective et (b) en considérant des extensions explicites du Modèle Standard, à savoir les modèles à deux doublets de Higgs et les scénarios postulant l'existence des bosons leptoquarks scalaires à basse énergie. En particulier, nous discutons le phénomène de la brisure de l'universalité des couplages leptoniques dans les désintégrations basées sur les transitions b → sℓℓ et b → cτν, et la possibilité de chercher les signatures de la violation de la saveur leptonique à travers les modes de désintégration similaires. Une proposition pour tester la présence d'un boson pseudoscalaire léger à travers les désintégrations des quarkonia est aussi présentée
Indirect searches of physics beyond the Standard Model through flavor physics processes at low energies are complementary to the ongoing efforts at the LHC to observe the New Physic phenomena directly. In this thesis we discuss several scenarios of physics beyond the Standard Model by (a) reusing the effective field theory approach and (b) by considering explicit extensions of the Standard Model, namely the two-Higgs doublet models and the scenarios involving the low energy scalar leptoquark states. Particular emphasis is devoted to the issue of the lepton flavor universality violation in the exclusive decays based on b → sℓℓ and b → cτν, and to the possibility of searching for signs of lepton flavor violation through similar decay modes. A proposal for testing the presence of the light CP-odd Higgs through quarkonia decays is also made

The scalar mesons have caused much debate amongst hadronic physicists for many years. Even today the number of scalars is hotly contested, and there is almost no agreement on the composition of any of the experimentally observed states, except perhaps for the K*(_0) (1430). This thesis attempts to shed light on both of these problems via the application of analyticity to two different quantities. Recently a number of authors have proposed the existence of a light, strange, scalar meson known as the k. We perform a direct search of the best available πK scattering data to determine whether or not this resonance exists. This is done by constructing contour integrals from these data and determining the number of poles present inside the contour. We do not need to model either the internal dynamics of the state nor the form of the background scattering. The number of poles found tells us the number of resonances present and their positions allow us to estimate the resonance parameters. We find that there is only one resonance in scalar πK scattering below 1800 MeV and this is identified with the established K*(_0)(1430). We find no evidence for the k. Secondly, applying Cauchy's Theorem to the vacuum polarisation function leads to a relation between experimental and theoretical integrals known as a Finite Energy Sum Rule (FESR). FESRs are used to explore the scalar, isoscalar non-strange current and allow us to determine which of the experimentally observed scalar, isoscalar mesons is most likely to be the uũ + dd state. We find that the lightest scalar, isoscalar uũ dd state is not the fo(980) as suggested by some authors, but is rather the light, broad object known as the fo(400 - 1200). We are also able to estimate the average light quark mass and find m(_q)(l GeV(^2)) = 4.7 ± 0.9 MeV which is consistent with the recent estimates of this quantity from unquenched lattice QCD.

We present the new framework based on BFKL and DGLAP evolution equations in which the leading in(Q(_2)) and in(l/x) terms are treated on equal footing. We introduce a pair of coupled integro-difFerential equations for the quark singlet and the unintegrated gluon distribution. The observable structure functions are calculated using high energy factorisation approach. We also include the sub-leading in (l/x) effects via consistency constraint. We argue that the use of this constraint leads to more stable solution to the Pomeron intercept than that based on the NLO calculation of the BFKL equation alone and generates resummation to all orders of the major part of the subleading in (l/x) effects. The global fit to all available deep inelastic data is performed using a simple parametrisation of the non-perturbative region. We also present the results for the longitudinal structure function and the charm component of the F(_2) structure function. Next; we extend this approach to the low Q(^2) domain. At small distances we use the perturbative approach based on the unified BFKL/DGLAP equations and for large distances we use Vector Meson Dominance Model and, for the higher mass qq states, the additive quark approach. We show the results for the total cross section and for the ratio of the longitudinal and transverse structure functions. Finally, we calculate the dijet production and consider the decorrelation effects in the azimuthal distributions caused by the diffusion in the transverse momentum k(_r) of the exchanged gluon. Using the gluon distribution which is fixed by the fit to the DIS data we are able to make absolute predictions. We show the results for the dF(_r)/dɸ, the total cross section and also the distributions in Q(^2) as well as in the longitudinal momentum fraction of the gluon. Our theoretical predictions are confronted with the measurements made using ZEUS detector at HERA.

Aux énergies assez hautes, les processus de QCD peuvent être factorisés en une partie dure, qui peut être calculée en utilisant les méthodes perturbatives des diagrammes de Feynman grâce à la petite valeur de la constante de couplage de l'interaction forte, et une partie non-perturbative qui doit être extraite de données expérimentales, modélisées ou calculées avec d'autres méthodes comme par exemple la QCD sur réseau. Cependant la petite valeur de la constante de couplage dans la partie perturbative peut être compensée par des grands logarithmes émergeant de l'annulation de divergences molles ou colinéaires, ou de la présence d'échelles cinématiques multiples. De telles contributions doivent être resommées, ce qui mène à l'équation d'évolution DGLAP aux énergies modérées et aux équations BFKL et B-JIMWLK dans la limite des hautes énergies. Pour les énergies les plus grandes des effets de recombinaison de gluons amènent à la saturation, qui peut être décrite par le formalisme du CGC ou des ondes de choc. Dans cette thèse, nous nous proposons d'étudier certains processus exclusifs en QCD perturbative afin d'obtenir une meilleure description de la factorisation et des effets de resommation et de saturation. Dans un premier temps nous faisons le premier calcul d'une quantité exclusive au premier ordre sous-dominant (NLO) dans le contexte du formalisme des ondes de choc de QCD. Nous calculons l'amplitude NLO pour la production diffractive ouverte d'une paire quark-antiquark, puis nous parvenons à construire une section efficace finie à l'aide de cette amplitude en étudiant la production diffractive exclusive de deux jets vers l'avant. Des analyses précises phénoménologiques et expérimentales de ce processus devraient améliorer notre compréhension de la resommation à haute énergie grâce à la présence d'un Pomeron échangé en diffraction, ce qui est naturellement décrit par la resommation de logarithmes découlant de la divergence molle de la QCD à haute énergie. Notre résultat reste valable quand l'énergie au centre de masse devient proche de l'échelle de saturation ou lorsque la diffraction a lieu sur une cible dense donc il peut être utilisé pour l'étude des effets de saturation. Dans un deuxième temps, nous montrons que l'étude expérimentale de la photoproduction d'un méson léger et d'un photon à énergies modérées devrait constituer un bon moyen d'appréhender les Distributions de Parton Généralisées (GPDs), l'une des généralisations des blocs non perturbatifs en factorisation collinéaire. En principe une telle étude donnerait accès à la fois aux GPDs conservant l'hélicité ou la renversant. Nous donnons des prédictions numériques pour ce processus à JLAB@12GeV
At high enough energies, QCD processes can be factorized into a hard part, which can be computed by using the smallness of the strong coupling to apply the perturbative Feynman diagram method, and a non-perturbative part which has to be fitted to experimental data, modeled or computed using other tools like for example lattice QCD. However the smallness of the strong coupling in the perturbative part can be compensated by large logarithms which arise from the cancellation of soft or collinear divergences, or by the presence of multiple kinematic scales. Such logarithmically-enhanced contributions must be resummed, leading to the DGLAP evolution at moderate energies and to the BFKL or B-JIMWLK equation in the high energy limit. For the largest energies gluon recombination effects lead to saturation, which can be described in the color glass condensate (CGC) or shockwave formalism. In this thesis, we propose to study several exclusive perturbative QCD processes in order to get a better understanding of factorization, resummation and saturation effects. In the first part we perform the first computation of an exclusive quantity at Next-to-Leading-Order (NLO) accuracy using the QCD shockwave formalism. We calculate the NLO amplitude for the diffractive production of an open quark-antiquark pair, then we manage to construct a finite cross section using this amplitude by studying the exclusive diffractive production of a dijet. Precise phenomenological and experimental analysis of this process should give a great insight on high energy resummation due to the exchange of a Pomeron in diffraction, which is naturally described by the resummation of logarithms emerging from the soft divergences of high energy QCD. Our result holds as the center of mass energy grows towards the saturation scale or for diffraction off a dense target so one could use it to study saturation effects. In the second part we show how the experimental study of the photoproduction of a light meson and a photon at moderate energy should be a good probe for Generalized Parton Distributions (GPDs), one of the generalizations of the non-perturbative building blocks in collinear factorization. In principle such a study would give access to both helicity-conserving and helicity-flip GPDs. We give numerical predictions for this process at JLAB@12GeV

L'objet de cette these est l'etude de la production des mesons charmes a partir du faisceau de sigma moins a 330 gev/c de l'experience wa89 du cern. Le debut de ce manuscrit est consacre a la presentation du contexte theorique et experimental actuel. Suit une description de l'ensemble du dispositif instrumental de wa89. La recherche et l'obtention des mesons d plus, d moins, d zero, anti d zero, d(2010) plus et d(2010) moins font l'objet de la suite de ce travail. Dans chacun des cas sont detaillees les coupures conduisant aux signaux ainsi que les distributions en xf (variable de feynman) et pt (impulsion transverse). Les sections efficaces de production ont ete estimees grace a un monte-carlo. Les resultats sont en accord avec les predictions de qcd et de pythia. Enfin une tentative prometteuse a ete faite en vue d'observer la production de charme associe

We examined strong interactions in the low-energy regime in terms of two complementary non-perturbative approaches: the interplay of large-N_c QCD and chiral perturbation theory was studied. While the expansion in the parameter 1/N_c is based on quark and gluon degrees of freedom, chiral perturbation theory uses hadrons as effective degrees of freedom. The focus of our work was the investigation of mesons and baryons composed from up-, down- and strange quarks. We used the chiral SU(3) Lagrangian with (J^P = 1/2^+)- and (J^P = 3/2^+)-baryon ground states as building blocks. In the SU(3)-flavour limit the latter form an octet and a decuplet, respectively. Studies in chiral perturbation theory hold a challenge: the chiral Lagrangian consists of an infinite number of terms. The treatment of low-energy QCD physics via a perturbation theory requires the ordering of these terms according to their relevance. We used the interplay between large-N_c QCD and chiral perturbation theory to shed light on the structure of the chiral Lagrangian. In the limit of large-N_c the low-energy parameters of the chiral Lagrangian are correlated. For instance the masses of the two baryon multiplets turn degenerate in the SU(3)-flavour limit. This serves as the starting point of our investigations. In this work we analysed the time-ordered product of two scalar and two vector currents in the baryon ground state. The examination of these matrix elements at large-N_c was compared to corresponding results derived in chiral perturbation theory. From this we obtained sum rules for some low-energy parameters of the chiral Lagrangian. The results for the vector correlation function were used to constrain a phenomenological interaction of light vector mesons with the baryon ground states. In the second part of this thesis we addressed a formal problem which arises in a partial wave decomposition of reaction amplitudes for particles with non-vanishing spin. In particular we considered the vector meson photoproduction off the nucleon as it is currently studied by e.g. Jude (2015), Wilson (2015) or Sokhoyan (2015). A decomposition of on-shell production amplitudes into covariant partial wave amplitudes which are both free from kinematical constraints and compatible with the microcausality condition was achieved. A Mathematica code using the FeynCalc package was written and applied to some tree-level contact terms and s-, u- and t-channel processes.

We find evidence for an infrared fixed point in perturbative QCD using two complementary approximations: The Banks-Zaks expansion and the large-b resummations. Analyzing the $e\sp+e\sp-$ annihilation ratio and the polarized Bjorken-sum-rule of deep-inelastic-scattering, we use the recent calculation of the renormalization-group $\beta$-function to four-loops in QCD to confirm that the Banks-Zaks expansion is relevant when extrapolated from sixteen down to two light quark flavors. We also search for indications of infrared 'freezing' in the Borel-renormalon-inspired 'large-b' resummations. We find the 'large-b' approximation also indicates perturbative 'freezing' of the $e\sp+e\sp-$ annihilation ratio and the polarized Bjorken-sum-rule at leading order. Finally, we study the region, $n\sb{f}$ = 2, where the 'large-$n\sb{f}$' resummation and Banks-Zaks expansion complement one another. We conclude that there is strong evidence for the existence of a perturbative infrared fixed point in the Standard Model QCD.

Quantum chromodynamics (QCD), the theory of quarks and gluons, is known to be

the correct description of strong nuclear interactions. At high energy and momenta,

one can use QCD directly to compute quantities of physical interest related to the

strong force. At low energies and momenta, one should use a different description in

terms of the degrees of freedom relevant at that scale. Two approaches to achieve

this end are effective field theories and gauge/gravity dualities. The former involves

a field theory more or less like QCD itself, but with states which are composites

of quarks and gluons. Then a perturbative expansion is made not in terms of the

gauge coupling but instead in terms of the momentum of the fields. This approach

dates back to the 1970s and is on firm theoretical footing. Gauge/gravity dualities

are a newer and less understood technique, which relates the physics of the strong

interactions to a different but likely equivalent theory in a higher dimensional space-

time, where the quantity of interest can be computed more readily. We employ

both effective field theories and gauge/gravity dualities to study the physics of ex-

otic quarkonium states, that is bound states containing a heavy quark-antiquark pair

which nevertheless cannot be be understood working only with the standard quark

model of hadrons. Candidates for such states, long speculated to exist, have recently

been observed at particle colliders, so that the theory of exotic quarkonium is now

of great experimental importance.

Dissertation