Nós utilizamos as Regras de Soma da QCD para estudar a natureza dos mésons observados recentemente Y (4260), Y (4360) e Y (4660), e que são candidatos a estados exóticos de tetraquark (c¯cq¯q) ou (c¯cs¯s) com números quânticos JPC = 1. Nós trabalhamos com o termo dominante em s, com as contribuições dos condensados de dimensão mais alta e com termos lineares da massa do quark estranho ms. Nós obtivemos uma massa mY = (4.65 ± 0.11) GeV para o estado (c¯cs¯s) que é compatível com o valor experimental do Y (4660), enquanto que para o estado (c¯cq¯q) n´os obtivemos uma massa mY = (4.49 ± 0.11) GeV, que também é consistente com o valor experimental do Y (4360). Com a estrutura de tetraquark não foi possível explicar o Y (4260). Nós também consideramos os estados moleculares Ds0 ¯D s e D0 ¯D . Para a molécula Ds0 ¯D s nós obtivemos uma massa mDs0 ¯D s = (4.42 ±0.10) GeV que é consistente, considerando a incerteza, com a massa do méson Y (4360) e para a molécula D0 ¯D obtivemos mD0 ¯D = (4.27±0.10) GeV em excelente acordo com a massa do m´eson Y (4260). / We use QCD sum rules to test the nature of the recently observed mesons Y (4260), Y (4360) and Y (4660), assumed to be exotic four-quark (c¯cq¯q) or (c¯cs¯s) states with JPC = 1. We work at leading order in s, consider the contributions of higher dimension condensates and keep terms which are linear in the strange quark mass ms. We find for the (c¯cs¯s) state a mass mY = (4.65 ± 0.10) GeV which is compatible with the experimental candidate Y (4660), while for the (c¯cq¯q) state we find a mass mY = (4.49 ± 0.11) GeV, which is still consistent with the mass of the experimental candidate Y (4360). With the tetraquark structure we are working we can not explain the Y (4260) as a tetraquark state. We also consider molecular Ds0 ¯D s and D0 ¯D states. For the Ds0 ¯D s molecular state we get mDs0 ¯D s = (4.42 ± 0.10) GeV which is consistent, considering the errors, with the mass of the meson Y (4360) and for the D0 ¯D molecular state we get mD0 ¯D = (4.27±0.10) GeV in excelent agreement with the mass of the meson Y (4260).

Submitted by Jaqueline Silva (jtas29@gmail.com) on 2014-09-15T18:48:07Z No. of bitstreams: 2 license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) Ademar Paulo Júnior.pdf: 470454 bytes, checksum: ca666cb4df9cfed260dd792d9b884664 (MD5) / Approved for entry into archive by Jaqueline Silva (jtas29@gmail.com) on 2014-09-15T18:48:28Z (GMT) No. of bitstreams: 2 license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) Ademar Paulo Júnior.pdf: 470454 bytes, checksum: ca666cb4df9cfed260dd792d9b884664 (MD5) / Made available in DSpace on 2014-09-15T18:48:28Z (GMT). No. of bitstreams: 2 license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) Ademar Paulo Júnior.pdf: 470454 bytes, checksum: ca666cb4df9cfed260dd792d9b884664 (MD5) Previous issue date: 2014-02-17 / The Quantum Chromodynamics (QCD) is the current theory that aim to describe the strong interactions in the Standard Model. It is a non-abelian gauge theory where quarks and gluons are the fundamental particles. However, QCD exhibits difficulties when low energy regimes are considered and perturbative methods cannot be employed. Thus, effective models are extremely important and useful when low energy limits are considered. Starting with QCD we develop an effetive model taking into account the second order gluon condensate, ⟨Aa A a ⟩, and quark-antiquark, ⟨ qq⟩. The coupled GAP equations are derived for Ns = 3 and numerical solutions are found for that. Furthermore, a functional expansion from effective potencial to the sixth order is calculated and contributions from that terms inserted into the effective lagrangian. / A Cromodin^amica Qu^antica (QCD) e a atual teoria que busca descrever as intera c~oes fortes dentro do modelo padr~ao. Trata-se de uma teoria de calibre n~ao-abeliana em que os quarks e gl uons constituem as part culas fundamentais. Entretanto, a QCD apresenta di - culdades quando consideram-se regimes de baixas energias em que t ecnicas n~ao perturbativas devem ser utilizadas. Assim, o uso de modelos efetivos e de extrema import^ancia e utilidade para os regimes de baixas energias que s~ao os de interesse deste trabalho. Partindo da QCD desenvolveremos um modelo efetivo para intera c~oes entre quarks levando em conta a presen ca dos condensados de gl uons de ordem dois, ⟨Aa A a ⟩, e de quark-antiquark, ⟨ qq⟩. As equa c~oes do GAP acopladas s~ao obtidas para Ns = 3 e suas solu c~oes num ericas s~ao encontradas. Al em disso, a expans~ao funcional do potencial efetivo at e sexta ordem no campo dos quarks e calculada e as contribui c~oes destes termos consideradas na lagrangeana efetiva.

We investigate charmonium production in the hot medium created by heavy-ion collisions by setting up a framework in which in-medium charmonium properties are constrained by thermal lattice QCD (lQCD) and subsequently implemented into kinetic approaches. A Boltzmann transport equation is employed to describe the time evolution of the charmonium phase space distribution with the loss and gain term accounting for charmonium dissociation and regeneration (from charm quarks), respectively. The momentum dependence of the charmonium dissociation rate is worked out. The dominant process for in-medium charmonium regeneration is found to be a 3-to-2 process. Its corresponding regeneration rates from different input charmquark momentum spectra are evaluated. Experimental data on J/[psi] production at CERN-SPS and BNL-RHIC are compared with our numerical results in terms of both rapidity-dependent inclusive yields and transverse momentum (pt) spectra. Within current uncertainties from (interpreting) lQCD data and from input charm-quark spectra the centrality dependence of J/[psi] production at SPS and RHIC (for both mid-and forward rapidity) is reasonably well reproduced. The J/[psi] pt data are shown to have a discriminating power for in-medium charmonium properties as inferred from different interpretations of lQCD results.

The future of new physics searches at the LHC will be to look for hadronic signals with jets. In order to distinguish a hadronic signal from its background, it is important to develop advanced collider physics techniques that make accurate theoretical predictions. This work centers on phenomenological and formal studies of Quantum Chromodynamics (QCD), including resummation of hadronic observables using Soft Collinear Effective Theory (SCET), calculating anomalous dimensions of multi-Wilson line operators in AdS, and improving jet physics analysis using multiple event interpretations. / Physics

No description available.

Many contemporary experimental QCD results achieve greater accuracy in measurement than equivalent theoretical predictions calculated at leading order. Therefore it is necessary to consider next to leading order (NLO) predictions for many processes in order to compare experiment with theory. Accurate theoretical predictions are also important in order to reduce the uncertainty in QCD parameters such as the coupling constant a, and to test whether QCD is in fact the correct theory to describe the strong interaction. With NLO results it is also possible to separate different clustering algorithms and test non-perturbative effects. This thesis concentrates on the techniques necessary for the calculation of NLO observables from the processes e(^+)e(^-) → 4 jets and pp → γ + X. We formulate a new version of the hybrid subtraction scheme based on the colour antenna structure of the final state to evaluate the necessary phase space integrals for the 4 jet process. The scheme is universal and can be applied to any QCD processes. The general purpose Monte Carlo EERAD2 which incorporates this new technique is compared with both experimental data gathered by the DELPHI collaboration and other groups which have reported similar calculations. A Monte Carlo written for the process pp → γ + X requires a knowledge of the non- perturbative photon fragmentation function, D(_γ), and the second half of this thesis concentrates on a calculation of this process using the ALEPH measurement of D(_γ) based on a democratic algorithm. The Monte Carlo DPRAD incorporates these techniques and results from it are compared with data from the Tevatron.

The resummation of double-logarithmic perturbative contributions produced by soft- gluon radiation (Sudakov resummation) has proved to be an important tool for enlarging the applications of perturbative QCD to a wider range of kinematical regions. In particular, a complete description of W and Z boson production at high-energy hadron colliders requires the resummation of large double logarithms that dominate the transverse momentum (p(_r)) distribution at small p(_r). This can be performed either directly in transverse momentum space or in impact parameter (Fourier transform) b space. The b space method succeeds in resumming all the leading and sub-leading logarithmic terms, but does not allow a smooth transition to fixed-order dominance at high transverse momenta. In contrast, the pr space approach experiences difficulties with resumming more sub-leading logarithms. This thesis concentrates on developing the p(_r) space formalism which completely resums the first four towers of logarithms. The number of fully resummed towers is the same as for the b space method. The results are compared, both analytically and numerically, with the original b space result as well as with results of other p(_r) space methods. Parametrization of the non-perturbative effects in p(_r) space is discussed. Given recent Tevatron data on Z boson production we find good agreement between the data and the theoretical predictions. Using the same formalism, the transverse momentum distributions are also calculated for W and Z boson production at the LHC. Finally, we discuss production of like-sign W pair production in the context of double parton scattering at the LHC.

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.

Zero-point energy is the energy of the vacuum. Disturbing the vacuum results in a change in the zero-point energy. In 1948, Casimir considered the change in the zeropoint energy when the vacuumis disturbed by two parallelmetal plates. The plates disturb the vacuum by restricting the quantum fluctuations of the electromagnetic field. Casimir found that the change in the zero-point energy implies that the plates are attracted to each other. With the recent advances made in the experimental verification of this remarkable result, theoretical interest has been rekindled. In addition to the original parallel plate configuration, several other boundaries have been studied. In this thesis, two novel boundaries are considered: elliptic-cylindrical and spheroidal. The results for these boundaries lead to the conjecture that zero-point energy does not change for small deformations of the boundary that preserve volume. Assuming the conjecture, it is shown that zero-point energy plays a stabilizing role in quantum chromodynamics, the leading theory of the strong interaction.

Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / Alguns aspectos não perturbativos das teorias de Yang-Mills puras em quatro dimensões Euclideanas, quantizadas no calibre de Landau, são estudados analiticamente. Por pura entendemos a teoria na ausência de matéria (férmions). Em particular, ivestigamos a geração dinâmica de massa para os gluons devido a presença de condensados de dimensão dois. Este estudo é feito utilizando a técnica de operadores locais compostos no caso da ação de Yang-Mills, bem como, no caso da ação de Gribov-Zwanziger. Além deste estudo, uma investigação sobre as ambigüidades de Gribov nos calibres lineares covariantes é apresentada. No caso da ação de Yang-Mills, fizemos uma análise detalhada da técnica de opera-dores locais compostos quando introduzidos, simultaneamente, os operadores A&#956;aA&#956;a e fabcc*bcc. Através da teoria da renormalização algébrica, provamos a renormalizabilidade do modelo a todas as ordens em teoria de perturbações. Com o auxílio das equações do grupo de renormalização uma ação quântica efetiva é construída para os condensados <A&#956;aA&#956;a> e <fabcc*bcc>. Esta construção é feita utilizando a regularização dimensional em conjunto com o esquema de renormalização MS. Mostramos que um valor não trivial para estes condensados é favorecido dinamicamente, independentemente da escala escolhida. Cálculos explícitos, a um laço, são apresentados fornecendo estimativas numéricas para estes condensados e para a energia do vácuo. Através de um estudo via identidades de Ward, somos capazes de mostrar formalmente que a presença do condensado Overhauser, <fabcc*bcc>, é responsável pela quebra de transversalidade da polarização do vácuo. Contudo, o propagador do glúon permanece transverso, a todas as ordens em teorias de perturbações. Finalmente, esta análise é terminada com o cálculo explícito da correção, a um laço, à massa do glúon, devido a presença destes condensados. O resultado é que existe uma quebra na degenerescência da massa entre gluons Abelianos e não Abelianos. Esta quebra, devido a massa não Abeliana ser maior que a Abeliana, pode ser interpretada como uma evidência da dominância Abeliana no calibre de Landau. Com relação à ação de Gribov-Zwanziger sem a inclusão de condensados, começamos por efetuar cálculos explícitos. Mostramos formalmente que, a um laço, a energia do vácuo será sempre positiva, independentemente do esquema de renormalização escolhido e da escala. Apresentamos uma discussão sobre a procura de soluções da condição de horizonte no esquema MS, a um e dois laços, e as respectivas dificuldades encontradas. Em seguida, mostramos, através da teoria de renormalização algébrica, que a inclusão do operador A&#956;aA&#956;a na ação de Gribov-Zwanziger via o formalismo LCO é renormalizável a todas as ordens em teoria de perturbações. Tentativas de resolver as equações de gap são apresentadas no esquema de renormalização MS a um laço. Mostramos formalmente que, para a condição de horizonte, não existem soluções para <A&#956;aA&#956;a> < 0 e somente uma solução para <A&#956;aA&#956;a> > 0 pode existir. Contudo, no esquema MS, não fomos capazes de encontrar esta solução explicitamente. Desta forma, uma aprimoração do esquema de renormalização é feita de forma a minimizar a dependência no esquema escolhido. Nesta otimização encontramos a solução no limite MS bem como para o caso em que a dependência no esquema de renormalização é mínima. Em ambos os casos, a energia do vácuo se mostra positiva e o condensado <A&#956;aA&#956;a> > 0. Após os cálculos explícitos, uma discussão sobre as conseqüências físicas de um parâmetro de Gribov não nulo é apresentada. Finalmente, apresentamos um estudo das ambiguidades de Gribov nos calibres lineares covariantes para o caso em que &#945;<<1, onde &#945; é o parâmetro de calibre. Após identificar uma região no espaço funcional das configurações na qual não existem cópias de Gribov próximas, efetuamos a respectiva restrição da integral de caminho. Como efeito no nível árvore, o propagador do glúon transverso se torna suprimido no limite infravermelho devido a presença do horizonte de Gribov. A componente longitudinal se mostra suprimida devido a geração dinâmica de massa, associada ao condensado <A&#956;aA&#956;a>. Ainda, diferentemente do calibre de Landau, o propagador dos campos fantasmas não apresenta conexão com forças de longo alcance. Em contrapartida, uma função de Green singular no infravermelho, relacionada ao horizonte, é identificada e pode ser associada a forças de longo alcance. Por fim, todos os resultados do calibre de Landau são recuperados no limite &#945;&#8594;0.. / Some nonperturbative aspects of Euclidean Yang-Mills theories in four dimensions,quantized in the Landau gauge, are analytically studied. In particular, we investigate the dynamical mass generation for the gluons due to the presence of dimension two condensates. This study is performed in the framework of the local composite operator technique in the case of the Yang-Mills action as well as in the case of the Gribov-Zwanziger action. Further, an investigation of the Gribov ambiguities in the linear covariant gauges is presented. In the case of the Yang-Mills action, we perform a detailed analysis of the local composite operator formalism when the operators AaAa and fabccbcc are simultaneously introduced. Using the algebraic renormalization theory, we prove the renormalizability of the model trough all orders in perturbation theory. With the help of the renormalization group equations, a quantum efective action for the condensates <AaAa> and <fabccbcc> is constructed. This construction is performed by means of the dimensional regularization in the MS renormalization scheme. We show that non vanishing condensates values are dynamically favored, independently of the chosen scale. Explicit one loop computations are then presented, providing estimates for the condensates as well as for the vacuum energy. With the help of suitable Ward identities, we are able to normally show that the presence of the condensate <fabccbcc> is responsible for the breaking of the transversality of the vacuum polarization. However, the gluon propagator remains transverse, trough all orders in perturbation theory. Finally, we end this analysis with the explicit computation of the one loop correction to the efective gluon mass. The result is that, due to the condensate <fabccbcc>, the Abelian and the non Abelian sectors acquire diferent masses. Since the non Abelian mass is larger than the Abelian one, this feature can be interpreted as an evidence for the Abelian dominance principle in the Landau gauge. With respect to the Gribov-Zwanziger action, we start our analysis without taking into account the condensate. We show that, at one loop order, the vacuum energy is always positive, independently of the renormalization scheme and scale. We also present attempts to solve the one and two loops horizon condition in the MS scheme, and also the respective obstacles of it. Later, using the algebraic renormalization theory, we show, to all orders in perturbation theory, the renormalizability of the Gribov-Zwanziger action when the composite operator AaAa is included in the framework of the local composite operator technique. Attempts to solve the one loop gap equations in the MS scheme are then presented. We show that there are no solutions for <AaAa> < 0 while for <AaAai> 0 there is only one possible solution for the horizon condition. However, in the MS scheme, we were not able to find explicitly that solution. As an improvement, an optimization of the renormalization scheme is performed in the sense of minimizing the renormalization scheme dependence. In that approach the MS limit solution was found as well as the solution with minimal dependence on the renormalization scheme. In both cases, the vacuum energy shows itself to be positive while the condensate <AaAa> > 0. A discussion of the consequences of a nonvanishing Gribov parameter is then provided. Finally, we present a study of the Gribov ambiguities in the linear covariant gauges for the case &#945;<<1, where &#945; is the gauge parameter. After the identification of a region in field space where there are no close Gribov copies, we perform the respective restriction in the path integral. As a tree level efect, the transverse gluon propagator turns out to be infrared suppressed, due to the presence of the Gribov horizon. The longitudinal component shows itself to be infrared suppressed due to the dynamical mass, associated with the condensate <AaAa>. Further, diferently of the Landau gauge, the ghost propagator is not related to the appearance of long range forces. Instead, an infrared singular Green function related to the Gribov horizon is identifed. This Green function can be associated with long range forces. At the end, all Landau gauge results can be recovered taking the limit &#945;&#8594;0.