1,361 research outputs found

    The Heavy Quark Spin Symmetry Partners of the X(3872)

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    We explore the consequences of heavy quark spin symmetry for the charmed meson-antimeson system in a contact-range (or pionless) effective field theory. As a trivial consequence, we theorize the existence of a heavy quark spin symmetry partner of the X(3872), with JPC=2++J^{PC}=2^{++}, which we call X(4012) in reference to its predicted mass. If we additionally assume that the X(3915) is a 0++0^{++} heavy spin symmetry partner of the X(3872), we end up predicting a total of six D(∗)Dˉ(∗)D^{(*)}\bar{D}^{(*)} molecular states. We also discuss the error induced by higher order effects such as finite heavy quark mass corrections, pion exchanges and coupled channels, allowing us to estimate the expected theoretical uncertainties in the position of these new states.Comment: 18 pages; final version accepted for publicatio

    Long-distance structure of the X(3872)

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    We investigate heavy quark symmetries for heavy meson hadronic molecules, and explore the consequences of assuming the X(3872) and Zb(10610)Z_b(10610) as an isoscalar DDˉ∗D\bar D^* and an isovector BBˉ∗B\bar B^* hadronic molecules, respectively. The symmetry allows to predict new hadronic molecules, in particular we find an isoscalar 1++1^{++} BBˉ∗B\bar B^* bound state with a mass about 10580 MeV and the isovector charmonium partners of the Zb(10610)Z_b(10610) and the Zb(10650)Z_b(10650) states. Next, we study the X(3872)→D0Dˉ0π0X(3872) \to D^0 \bar D^0\pi^0 three body decay. This decay mode is more sensitive to the long-distance structure of the X(3872) resonance than its J/ψππJ/\psi\pi\pi and J/ψ3πJ/\psi3\pi decays, which are mainly controlled by the short distance part of the X(3872) molecular wave function. We discuss the D0Dˉ0D^0 \bar D^0 final state interactions, which in some situations become quite important. Indeed in these cases, a precise measurement of this partial decay width could provide precise information on the interaction strength between the D(∗)Dˉ(∗)D^{(*)}\bar D^{(*)} charm mesons.Comment: Talk presented at the "XI International Conference on Hyperons, Charm and Beauty Hadrons (BEACH 2014)", Birmingham (U.K.), July 201

    Renormalization of the Deuteron with One Pion Exchange

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    We analyze the deuteron bound state through the One Pion Exchange Potential. We pay attention to the short distance peculiar singularity structure of the bound state wave functions in coordinate space and the elimination of short distance ambiguities by selecting the regular solution at the origin. We determine the so far elusive amplitude of the converging exponential solutions at the origin. All bound state deuteron properties can then be uniquely deduced from the deuteron binding energy, the pion-nucleon coupling constant and pion mass. This generates correlations among deuteron properties. Scattering phase shifts and low energy parameters in the 3S1-3D1 channel are constructed by requiring orthogonality of the positive energy states to the deuteron bound state, yielding an energy independent combination of boundary conditions. We also analyze from the viewpoint of short distance boundary conditions the weak binding regime on the light of long distance perturbation theory and discuss the approach to the chiral limit.Comment: 22 pages, 11 figure

    Un procedimiento para obtener clusters utilizando la D.V.S. de una matriz. Comparaciones con el biplot y con el modelo Q-factorial

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    Durante las últimas décadas, el análisis de un conjunto de n individuos medidos en p variables, proporcionando una matriz de datos Xn,p, mediante técnicas de representación que utilizan la Descomposición en Valores Singulares de la matriz Xn,p (o alguna derivada), han permitido resumir la información que aportan los datos en alguna forma óptima, siendo muy útil para indicar la presencia de clusters entre los n individuos y/o para prevenir ante posibles clasificaciones erróneas producidas por técnicas de agrupamiento más complejas. En este artículo estudiaremos un procedimiento que puede utilizarse en ocasiones para obtener clasificaciones naturales de un conjunto de datos, basado en la representación biplot y en el modelo Q-factorial que puede obtenerse a partir de la DVS

    Renormalization of chiral two pion exchange NN interactions with delta excitations: correlations in the partial wave expansion

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    In this work we consider the renormalization of the chiral two-pion exchange potential with explicit delta-excitations for nucleon-nucleon scattering at next-to-leading (NLO) and next-to-next-to-leading order (N2LO). Due to the singular nature of the chiral potentials, correlations between different partial waves are generated. In particular we show that two-body scattering by a short distance power like singular attractive interaction can be renormalized in all partial waves with a single counterterm, provided the singularities are identical. A parallel statement holds in the presence of tensor interactions when the eigenpotentials in the coupled channel problem also coincide. While this construction reduces the total number of counterterms to eleven in the case of nucleon-nucleon scattering with chiral two-pion exchange interactions with delta degrees of freedom, the differences in the scattering phases as compared to the case with the uncorrelated partial wave renormalization become smaller as the angular momentum is increased in the elastic scattering region.Comment: 20 pages, 8 figures, a section has been added discussing cut-off dependence. Accepted for publication in PR

    Renormalization of NN Interaction with Relativistic Chiral Two Pion Exchange

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    The renormalization of the NN interaction with the Chiral Two Pion Exchange Potential computed using relativistic baryon chiral perturbation theory is considered. The short distance singularity reduces the number of counter-terms to about a half as those in the heavy-baryon expansion. Phase shifts and deuteron properties are evaluated and a general overall agreement is observed.Comment: 13 pages, 4 figures. Reference included. Typos corrected. Appendix and discussion adde

    Are there three Xi(1950) states?

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    Different experiments on hadron spectroscopy have long suspected the existence of several cascade states in the 1900−2000MeV1900-2000 {\rm MeV} region. They are usually labeled under the common name of Ξ(1950)\Xi (1950). As we argue here, there are also theoretical reasons supporting the idea of several Ξ(1950)\Xi (1950) resonances. In particular, we propose the existence of three Ξ(1950)\Xi(1950) states: one of these states would be part of a spin-parity (1/2)−(1/2)^{-} decuplet and the other two probably would belong to the (5/2)+(5/2)^{+} and (5/2)−(5/2)^{-} octets. We also identify which decay channels are the more appropriate for the detection of each of the previous states.Comment: 5 pages, 3 tables, final version. Published in Phys. Rev. D 85, 017502 (2012

    Nucleon-Nucleon interaction, charge symmetry breaking and renormalization

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    We study the interplay between charge symmetry breaking and renormalization in the NN system for s-waves. We find a set of universality relations which disentangle explicitly the known long distance dynamics from low energy parameters and extend them to the Coulomb case. We analyze within such an approach the One-Boson-Exchange potential and the theoretical conditions which allow to relate the proton-neutron, proton-proton and neutron-neutron scattering observables without the introduction of extra new parameters and providing good phenomenological success.Comment: 15 pages, 6 figure

    Modelos escolásticos dinámicos en las ciencias experimentales

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    For a mathematical model to be a suitable representation of a dynarnical phenomenom in Nature, it must inc1ude its random characteristics as well as the time variable. After reviewing alternative procedures in model formulation, this paper presents a methodology for elaborating a predictive stochastic model from sample observations depending upon the time, on the basis of the Principal Component Analysis of the studied stochastic process. The developed model is then applied to forecast the AIDS incidence rate in European countries.Para que un modelo matemático represente de forma adecuada un fenómeno natural de carácter dinámico, debe recoger la aleatoriedad inherente al mismo, así como la variable de temporalidad. Tras repasar procedimientos alternativos en la formulación de modelos, en el presente trabajo proponemos una metodología para la elaboración de un modelo predictivo de naturaleza estocástica, a partir de observaciones muestrales temporales, basado en el Análisis de Componentes Principales del proceso objeto de estudio. El modelo desarrollado se aplica a predecir la tasa de incidencia de SIDA en países europeos

    Heavy quark spin symmetry and SU(3)-flavour partners of the X (3872)

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    In this work, an Effective Field Theory (EFT) incorporating light SU(3)-flavour and heavy quark spin symmetries is used to describe charmed meson-antimeson bound states. At Lowest Order (LO), this means that only contact range interactions among the heavy meson and antimeson fields are involved. Besides, the isospin violating decays of the X(3872) will be used to constrain the interaction between the D and a (D) over bar* mesons in the isovector channel. Finally, assuming that the X(3915) and Y(4140) resonances are D* (D) over bar* and D-s* (D) over bar (s)* molecular states, we can determine the four Low Energy Constants (LECs) of the EFT that appear at LO and, therefore, the full spectrum of molecular states with isospin I = 0, 1/2 and 1
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