Search results for "normalization"

showing 10 items of 632 documents

Perturbative chiral violations for domain-wall QCD with improved gauge actions

2006

We investigate, in the framework of perturbation theory at finite $N_s$, the effectiveness of improved gauge actions in suppressing the chiral violations of domain-wall fermions. Our calculations show substantial reductions of the residual mass when it is compared at the same value of the gauge coupling, the largest suppression being obtained when the DBW2 action is used. Similar effects can also be observed for a power-divergent mixing coefficient which is chirally suppressed. No significant reduction instead can be seen in the case of the difference between the vector and axial-vector renormalization constants when improved gauge actions are used in place of the plaquette action. We also …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFermionGauge (firearms)01 natural sciencesRenormalizationDomain wall (string theory)High Energy Physics - LatticeLattice gauge theory0103 physical sciencesPerturbation theory (quantum mechanics)010306 general physicsMixing (physics)
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Measurement of the strong coupling constant alfa_s from global event-shape variables of hadronic Z decays

1991

Abstract An analysis of global event-shape variables has been carried out for the reaction e+e−→Z0→hadrons to measure the strong coupling constant αs. This study is based on 52 720 hadronic events obtained in 1989/90 with the ALEPH detector at the LEP collider at energies near the peak of the Z-resonance. In order to determine αs, second order QCD predictions modified by effects of perturbative higher orders and hadronization were fitted to the experimental distributions of event-shape variables. From a detailed analysis of the theoretical uncertainties we find that this approach is best justified for the differential two-jet rate, from which we obtain αs(MZ2) = 0.121 ± 0.002(stat.)±0.003(s…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationHadronMeasure (mathematics)Hadronizationlaw.inventionNuclear physicsRenormalizationlawHigh Energy Physics::ExperimentColliderConstant (mathematics)Particle Physics - Experiment
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Form-factors and current correlators: chiral couplingsL10r(μ) andC87r(μ) at NLO in 1/NC

2008

Using the resonance chiral theory Lagrangian, we perform a calculation of the vector and axial-vector two-point functions at the next-to-leading order (NLO) in the 1/N-C expansion. We have analyzed these correlators within the single-resonance approximation and have also investigated the corrections induced by a second multiplet of vector and axial-vector resonance states. Imposing the correct QCD short-distance constraints, one determines the difference of the two correlators Pi(t) equivalent to Pi(VV)(t)-Pi(AA)(t) in terms of the pion decay constant and resonance masses. Its low momentum expansion fixes then the low-energy chiral couplings L 1 0 and C 8 7 at NLO, keeping full control of t…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsFísicaOrder (ring theory)Resonance (particle physics)RenormalizationMomentumPiHigh Energy Physics::ExperimentPion decay constantMultipletJournal of High Energy Physics
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The vector form factor at the next-to-leading order in 1/N(C): chiral couplings L9(mu) and C88(mu) - C90(mu)

2010

24 páginas, 3 figuras, 2 tablas.-- arXiv:1011.5771v1.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeForm factor (quantum field theory)Order (ring theory)ResonanceFOS: Physical sciencesFísica1/N ExpansionQCDRenormalizationMomentumHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPion decay constantNuclear ExperimentChiral lagrangians
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Origin of the Large Perturbative Corrections to Higgs Production at Hadron Colliders

2008

The very large K-factor for Higgs-boson production at hadron colliders is shown to result from enhanced perturbative corrections of the form (C_A\pi\alpha_s)^n, which arise in the analytic continuation of the gluon form factor to time-like momentum transfer. These terms are resummed to all orders in perturbation theory using the renormalization group. After the resummation, the K-factor for the production of a light Higgs boson at the LHC is reduced to a value close to 1.3.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Drell–Yan processFOS: Physical sciencesGluonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonProduction (computer science)High Energy Physics::ExperimentResummation
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Charmonium properties in hot quenched lattice QCD

2012

We study the properties of charmonium states at finite temperature in quenched QCD on large and fine isotropic lattices. We perform a detailed analysis of charmonium correlation and spectral functions both below and above $T_c$. Our analysis suggests that both S wave states ($J/\psi$ and $\eta_c$) and P wave states ($\chi_{c0}$ and $\chi_{c1}$) disappear already at about $1.5 T_c$. The charm diffusion coefficient is estimated through the Kubo formula and found to be compatible with zero below $T_c$ and approximately $1/\pi T$ at $1.5 T_c\lesssim T\lesssim 3 T_c$.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsSpectral representationNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDRenormalizationNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKubo formulaLattice (order)Condensed Matter::SuperconductivityQuark–gluon plasmaCondensed Matter::Strongly Correlated ElectronsHigh Energy Physics::ExperimentNuclear theory
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Gauge-invariant resummation formalism for two-point correlation functions

1996

The consistent description of unstable particles, renormalons, or other Schwinger--Dyson-type of solutions within the framework of perturbative gauge field theories necessitates the definition and resummation of off-shell Green's functions, which must respect several crucial physical requirements. A formalism is presented for resummation of off-shell two-point correlation functions, which is mainly based on arguments of analyticity, unitarity, gauge invariance and renormalizability. The analytic results obtained with various methods, including the background field gauges and the pinch technique are confronted with the physical requirements imposed; to one-loop order the pinch technique appr…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaRenormalization groupRenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Gauge theoryPerturbation theory (quantum mechanics)UniquenessResummationPhysical Review D
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Properties of Hadronic Z-decays and Test of QCD Generators

1992

Distributions are presented of event shape variables, jet roduction rates and charged particle momenta obtained from 53 000 hadronic Z decays. They are compared to the predictions of the QCD + hadronization models JETSET, ARIADNE and HERWIG, and are used to optimize several model parameters. The JETSET and ARIADNE coherent parton shower (PS) models with running alpha(s) and string fragmentation yield the best description of the data. The HERWIG parton shower model with cluster fragmentation fits the data less well. The data are in better agreement with JETSET PS than with JETSET O(alpha(s)2) matrix elements (ME) even when the renormalization scale is optimized.

Quantum chromodynamicsPhysicsParticle physicsAlephPhysics and Astronomy (miscellaneous)Electron–positron annihilationPhysicsHadronHigh Energy Physics::PhenomenologyCharged particleHadronizationNuclear physicsRenormalizationHigh Energy Physics::ExperimentParton showerNuclear ExperimentEngineering (miscellaneous)Particle Physics - Experiment
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New High Order Relations between Physical Observables in Perturbative QCD

1997

We exploit the fact that within massless perturbative QCD the same Green's function determines the hadronic contribution to the $\tau$ decay width and the moments of the $e^+e^-$ cross section. This allows one to obtain relations between physical observables in the two processes up to an unprecedented high order of perturbative QCD. A precision measurement of the $\tau$ decay width allows one then to predict the first few moments of the spectral density in $e^+e^-$ annihilations integrated up to $s\sim m_\tau^2$ with high accuracy. The proposed tests are in reach of present experimental capabilities.

Quantum chromodynamicsPhysicsParticle physicsElectron–positron annihilationHadronFOS: Physical sciencesGeneral Physics and AstronomySpectral densityPerturbative QCDRenormalization groupHigh Energy Physics - ExperimentMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Particle decayHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPhysical Review Letters
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QCD effective charges from lattice data

2010

We use recent lattice data on the gluon and ghost propagators, as well as the Kugo-Ojima function, in order to extract the non-perturbative behavior of two particular definitions of the QCD effective charge, one based on the pinch technique construction, and one obtained from the standard ghost-gluon vertex. The construction relies crucially on the definition of two dimensionful quantities, which are invariant under the renormalization group, and are built out of very particular combinations of the aforementioned Green's functions. The main non-perturbative feature of both effective charges, encoded in the infrared finiteness of the gluon propagator and ghost dressing function used in their…

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesPropagatorFísicaInvariant (physics)Renormalization groupQCDEffective nuclear chargeVertex (geometry)GluonTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNonperturbative EffectsLattice (order)
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