Search results for "RULE"

showing 10 items of 1403 documents

The physics of glueballs

2008

Glueballs are particles whose valence degrees of freedom are gluons and therefore in their description the gauge field plays a dominant role. We review recent results in the physics of glueballs with the aim set on phenomenology and discuss the possibility of finding them in conventional hadronic experiments and in the Quark Gluon Plasma. In order to describe their properties we resort to a variety of theoretical treatments which include, lattice QCD, constituent models, AdS/QCD methods, and QCD sum rules. The review is supposed to be an informed guide to the literature. Therefore, we do not discuss in detail technical developments but refer the reader to the appropriate references.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsMesonsGlueballsGluonsHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesFísicaLattice QCDQCDGluonquarksHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)QGPQuark–gluon plasmaHigh Energy Physics::ExperimentGauge theoryPhenomenology (particle physics)
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A Tachyonic Gluon Mass: Between Infrared and Ultraviolet

1999

The gluon spin coupling to a Gaussian correlated background gauge field induces an effective tachyonic gluon mass. It is momentum dependent and vanishes in the UV only like 1/p^2. In the IR, we obtain stabilization through a positive m^2_{conf}(p^2) related to confinement. Recently a purely phenomenological tachyonic gluon mass was used to explain the linear rise in the q\bar q static potential at small distances and also some long standing discrepancies found in QCD sum rules. We show that the stochastic vacuum model of QCD predicts a gluon mass with the desired properties.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsStochastic vacuum modelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesCoupling (probability)GluonMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentGauge theorySpin-½
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Comparison between two strictly local QCD sum rules

1989

Two strictly local QCD sum rules, analytic extrapolation by conformal mapping and analytic continuation by duality, are developed and presented in full detail. They allow the extrapolation of the QCD amplitude to a single point near zero in the complex {ital q}{sup 2} plane. Being orthogonal to the usual QCD sum rules, they present a drastic enlargement of phenomenological applications. In addition, the stability of both methods is shown explicitly, a fact which makes them particularly reliable. The difference between the two methods is illustrated in connection with the determination of the hadronic ({ital g}{minus}2) factor of the muon. Their effectiveness is demonstrated in the calculati…

Quantum chromodynamicsPhysicsParticle physicsQCD sum rulesAnalytic continuationZero (complex analysis)ExtrapolationDuality (optimization)Sum rule in quantum mechanicsConnection (algebraic framework)Mathematical physicsPhysical Review D
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B and B(S) decay constants from moments of finite energy sum rules in QCD

2004

We use an appropriate combination of moments of finite energy sum rules in QCD in order to compute the B_q-meson decays constants f_B and f_{B_s}.We perform the calculation using a two-loop computation of the imaginary part of the pseudoscalar two point function in terms of the running bottom quark mass. The results are stable with the so called QCD duality threshold and they are in agreement with the estimates obtained from Borel transform QCD sum rules and lattice computations.

Quantum chromodynamicsPhysicsParticle physicsQCD sum rulesPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice (group)Duality (optimization)Order (ring theory)FOS: Physical sciencesFísicaBottom quarkPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentEngineering (miscellaneous)Energy (signal processing)
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B0−B¯0Mixing beyond Factorization in QCD Sum Rules

2003

We present a calculation of the B°-B° mixing matrix element in the framework of QCD sum rules for three-point functions. We compute α s corrections to a three-point function at the three-loop level in QCD perturbation theory, which allows one to extract the matrix element with next-to-leading order (NLO) accuracy. This calculation is imperative for a consistent evaluation of experimentally measured mixing parameters since the coefficient functions of the effective Hamiltonian for B 0 -B 0 mixing are known at NLO. We find that radiative corrections violate factorization at NLO; this violation is under full control and amounts to 10%. The resulting value of the B parameter is found to be B B …

Quantum chromodynamicsPhysicsParticle physicssymbols.namesakeQCD sum rulesFactorizationRadiative transfersymbolsGeneral Physics and AstronomyMatrix elementHamiltonian (quantum mechanics)Physical Review Letters
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Off-forward Matrix Elements in Light-front Hamiltonian QCD

2002

We investigate the off-forward matrix element of the light cone vector operator for a dressed quark state in light-front Hamiltonian perturbation theory. We obtain the corresponding splitting functions in a straightforward way. We show that the end point singularity is canceled by the contribution from the normalization of state. Considering mixing with the gluon operator, we verify the helicity sum rule in perturbation theory. We show that the quark mass effects are suppressed in the plus component of the matrix element but in the transverse component, they are not suppressed. We emphasize that this is a particularity of the off-forward matrix element and is absent in the forward case.

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsVector operatorFOS: Physical sciencesHelicitysymbols.namesakeHigh Energy Physics - PhenomenologySingularityHigh Energy Physics - Phenomenology (hep-ph)Light conesymbolsSum rule in quantum mechanicsHamiltonian (quantum mechanics)Mathematical physics
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Method of analytic continuation by duality in QCD: Beyond QCD sum rules

1986

We present the method of analytic continuation by duality which allows the approximate continuation of QCD amplitudes to small values of the momentum variables where direct perturbative calculations are not possible. This allows a substantial extension of the domain of applications of hadronic QCD phenomenology. The method is illustrated by a simple example which shows its essential features.

Quantum chromodynamicsPhysicsTheoretical physicsQCD sum rulesParticle physicsContinuationAnalytic continuationSpace timeHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentElementary particleAsymptotic expansionPhenomenology (particle physics)Physical Review D
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Ratio of strange to non-strange quark condensates in QCD

2001

Laplace transform QCD sum rules for two-point functions related to the strangeness-changing scalar and pseudoscalar Green's functions $\psi(Q^2)$ and $\psi_5(Q^2)$, are used to determine the subtraction constants $\psi(0)$ and $\psi_5(0)$, which fix the ratio $R_{su}\equiv \frac{}{}$. Our results are $\psi(0)= - (1.06 \pm 0.21) \times 10^{-3} {GeV}^4$, $\psi_5(0)= (3.35 \pm 0.25) \times 10^{-3} {GeV}^4$, and $R_{su}\equiv \frac{}{} = 0.5 \pm 0.1$. This implies corrections to kaon-PCAC at the level of 50%, which although large, are not inconsistent with the size of the corrections to Goldberger-Treiman relations in $SU(3)\otimes SU(3)$.

Quantum chromodynamicsPseudoscalarPhysicsNuclear and High Energy PhysicsStrange quarkQCD sum rulesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Laplace transformScalar (mathematics)FOS: Physical sciencesHigh Energy Physics::ExperimentMathematical physics
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Exclusive/inclusive ratio of semileptonicΛbdecays

2000

We present theoretical evidence that the exclusive/inclusive ratio of semileptonic ${\ensuremath{\Lambda}}_{b}$ decays exceeds that of semileptonic B decays where the experimental exclusive/inclusive ratio amounts to about 66%. We start from the observation that the spectator quark model provides a lower bound on the leading order Isgur-Wise function of the ${\ensuremath{\Lambda}}_{b}\ensuremath{\rightarrow}{\ensuremath{\Lambda}}_{c}$ transition in terms of the corresponding $\stackrel{\ensuremath{\rightarrow}}{B}{D,D}^{*}$ mesonic Isgur-Wise function. Using experimental data for the $\stackrel{\ensuremath{\rightarrow}}{B}{D,D}^{*}$ mesonic Isgur-Wise functions this bound is established. Ap…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelForm factor (quantum field theory)Order (ring theory)LambdaBaryonHigh Energy Physics::ExperimentSum rule in quantum mechanicsPhysical Review D
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Bottom quark mass from QCD sum rules for the υ system

1999

Abstract The talk presents an update of the bottom quark mass determination from QCD moment sum rules for the ϒ system by the authors [1]. Employing the MS scheme, we fund mb(mb) = 4.19 ± 0.06 GeV. The differences to our previous analysis will be discussed and we comment on the determination of th pole mass for the bottom quark.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHadronQuarkoniumBottom quarkAtomic and Molecular Physics and OpticsPhysics::Fluid DynamicsGrand Unified TheoryHigh Energy Physics::Experiment
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