Search results for "Mathematica"

showing 10 items of 7971 documents

Quark Structure of the X (4500), X (4700) and χc(4P,5P) States

2021

We study some of the main properties (masses and open-flavor strong decay widths) of 4P and 5P charmonia. While there are two candidates for the χc0(4P,5P) states, the X(4500) and X(4700), the properties of the other members of the χc(4P,5P) multiplets are still completely unknown. With this in mind, we start to explore the charmonium interpretation for these mesons. Our second goal is to investigate if the apparent mismatch between the Quark Model (QM) predictions for χc0(4P,5P) states and the properties of the X(4500) and X(4700) mesons can be overcome by introducing threshold corrections in the QM formalism. According to our coupled-channel model results for the threshold mass shifts, th…

QuarkParticle physicsMesonFormalism (philosophy)QC1-999Materials Science (miscellaneous)BiophysicsStructure (category theory)General Physics and Astronomystrong decayshiukkasfysiikka01 natural sciencesInterpretation (model theory)charmonia phenomenology0103 physical sciencesPhysical and Theoretical Chemistry010306 general physics3P0 modelMathematical PhysicsPhysicsquark modelkvarkit010308 nuclear & particles physicsPhysicsexotic statesQuark modelunquenched quark modelHigh Energy Physics - PhenomenologycharmoniaydinfysiikkaFrontiers in Physics
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Quark gap equation with non-Abelian Ball-Chiu vertex

2018

The full quark-gluon vertex is a crucial ingredient for the dynamical generation of a constituent quark mass from the standard quark gap equation, and its non-transverse part may be determined exactly from the nonlinear Slavnov-Taylor identity that it satisfies. The resulting expression involves not only the quark propagator, but also the ghost dressing function and the quark-ghost kernel, and constitutes the non-abelian extension of the so-called "Ball-Chiu vertex", known from QED. In the present work we carry out a detailed study of the impact of this vertex on the gap equation and the quark masses generated from it, putting particular emphasis on the contributions directly related with t…

QuarkPhysics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyMultiplicative functionFOS: Physical sciencesPropagatorConstituent quark01 natural sciencesGluonHigh Energy Physics - PhenomenologyNonlinear systemHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentAbelian group010306 general physicsPion decay constantMathematical physicsPhysical Review D
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Finite-size scaling of the quark condensate in quenched lattice QCD

1999

We confront the finite volume and small quark mass behaviour of the scalar condensate, determined numerically in quenched lattice QCD using Neuberger fermions, with predictions of quenched chiral perturbation theory. We find that quenched chiral perturbation theory describes the numerical data well, allowing us to extract the infinite volume, chiral limit scalar condensate, up to a multiplicative renormalization constant.

QuarkPhysicsCondensed Matter::Quantum GasesNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesParticle Physics - LatticeFermionLattice QCDRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)ScalingMathematical physics
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Nucleon Form Factors at high q2 within constituent quark models

2000

The nucleon form factors are calculated using a non-relativistic description in terms of constituent quarks. The emphasis is put on the reliability of present numerical methods used to solve the three-body problem in order to correctly reproduce the expected asymptotic behavior of form factors. Nucleon wave functions obtained in the hyperspherical formalism or employing Faddeev equations have been considered. While a q**(-8) behavior is expected at high q for a quark-quark force behaving like 1/r at short distances, it is found that the hypercentral approximation in the hyperspherical formalism (K=0) leads to a q**(-7) behavior. An infinite set of waves is required to get the correct behavi…

QuarkPhysicsFaddeev equationsInfinite set010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Numerical analysisNuclear Theory01 natural sciencesAtomic and Molecular Physics and OpticsMomentumAmplitude0103 physical sciencesFísica nuclear010306 general physicsNucleonWave functionMathematical physics
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Heavy quark decomposition of the S matrix and its relation to the pinch technique.

1995

We propose a decomposition of the S-matrix into individually gauge invariant sub-amplitudes, which are kinematically akin to propagators, vertices, boxes, etc. This decompsition is obtained by considering limits of the S-matrix when some or all of the external particles have masses larger than any other physical scale. We show at the one-loop level that the effective gluon self-energy so defined is physically equivalent to the corresponding gauge independent self-energy obtained in the framework of the pinch technique. The generalization of this procedure to arbitrary gluonic $n$-point functions is briefly discussed.

QuarkPhysicsHigh Energy Physics - TheoryParticle physicsWilson loop010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::LatticePropagatorFísicaFOS: Physical sciences01 natural sciencesMatrix (mathematics)Self-energyHigh Energy Physics - Theory (hep-th)0103 physical sciencesGauge theoryInvariant (mathematics)010306 general physicsS-matrixMathematical physicsPhysical review. D, Particles and fields
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Flavour Symmetries and SUSY Soft Breaking in the LHC Era

2007

The so-called supersymmetric flavour problem does not exist in isolation to the Standard Model flavour problem. We show that a realistic flavour symmetry can simultaneously solve both problems without ad hoc modifications of the SUSY model. Furthermore, departures from the SM expectations in these models can be used to discriminate among different possibilities. In particular we present the expected values for the electron EDM in a flavour model solving the supersymmetric flavour and CP problems.

QuarkPhysicsHistoryParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFlavourFOS: Physical sciencesSupersymmetryExpected valueSymmetry (physics)Computer Science ApplicationsEducationHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Homogeneous spaceHigh Energy Physics::ExperimentMixing (physics)LeptonProgress of Theoretical Physics Supplement
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Two-loop gluino corrections to the inclusive decayB→Xsγin theCPviolating MSSM with largetanβ

2004

We investigate two-loop gluino corrections to the effective Lagrangian for b{yields}s+{gamma}(g) in the minimal supersymmetric extension of the standard model (MSSM) at large tan{beta}, including the contributions in which quark flavor change is mediated by charginos. Using the translation invariance of loop momenta and the Ward-Takahashi identities that are required by the SU(3){sub c}xU(1){sub em} gauge invariance, we simplify our expressions to concise forms. As an example, we discuss two-loop gluino corrections to the CP asymmetry of inclusive B{yields}X{sub s}{gamma} decay in CP violating MSSM.

QuarkPhysicsNuclear and High Energy PhysicsGluinoParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySuperpartnerSupersymmetry01 natural sciencesStandard Model (mathematical formulation)0103 physical sciencesCP violationHigh Energy Physics::ExperimentB mesonGauge theory010306 general physicsPhysical Review D
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Non-perturbative renormalization of the quark condensate in Ginsparg-Wilson regularizations

2001

We present a method to compute non-perturbatively the renormalization constant of the scalar density for Ginsparg-Wilson fermions. It relies on chiral symmetry and is based on a matching of renormalization group invariant masses at fixed pseudoscalar meson mass, making use of results previously obtained by the ALPHA Collaboration for O(a)-improved Wilson fermions. Our approach is quite general and enables the renormalization of scalar and pseudoscalar densities in lattice regularizations that preserve chiral symmetry and of fermion masses in any regularization. As an application we compute the non-perturbative factor which relates the renormalization group invariant quark condensate to its …

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParticle Physics - LatticeQuenched approximationFermionRenormalization groupPseudoscalar mesonRenormalizationPseudoscalarHigh Energy Physics - LatticeRegularization (physics)Mathematical physicsJournal of High Energy Physics
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Nonperturbative renormalization in coordinate space

2003

We present an exploratory study of a gauge-invariant non-perturbative renormalization technique. The renormalization conditions are imposed on correlation functions of composite operators in coordinate space on the lattice. Numerical results for bilinears obtained with overlap and O(a)-improved Wilson fermions are presented. The measurement of the quark condensate is also discussed.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)field theory gauge theory lattice renormalizationFOS: Physical sciencesFísicaParticle Physics - LatticeFermionAtomic and Molecular Physics and OpticsComposite operatorRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeLattice (order)Non-perturbativeCoordinate spaceMathematical physics
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Docc¯nn¯bound states exist?

2007

The four-quark system $c\overline{c}n\overline{n}$ is studied in the framework of the constituent quark model. Using different types of quark-quark potentials, we solve the four-body Schr\"odinger equation by means of the hyperspherical harmonic formalism. Exploring the low laying ${J}^{\mathrm{PC}}$ states for different isospin configurations no four-quark bound states have been found. Of particular interest is the possible four-quark structure of the $X(3872)$. We rule out the possibility that this particle is a compact tetraquark system, unless additional correlations, either in the form of diquarks or at the level of the interacting potential, not considered in simple quark models do co…

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelConstituent quarkParticle identificationSchrödinger equationsymbols.namesakeIsospinQuantum mechanicsBound statesymbolsHigh Energy Physics::ExperimentTetraquarkMathematical physicsPhysical Review D
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