Search results for " Quantum mechanics"

showing 10 items of 245 documents

Strange quark mass from Finite Energy QCD sum rules to five loops

2007

The strange quark mass is determined from a new QCD Finite Energy Sum Rule (FESR) optimized to reduce considerably the systematic uncertainties arising from the hadronic resonance sector. As a result, the main uncertainty in this determination is due to the value of $\Lambda_{QCD}$. The correlator of axial-vector divergences is used in perturbative QCD to five-loop order, including quark and gluon condensate contributions, in the framework of both Fixed Order (FOPT), and Contour Improved Perturbation Theory (CIPT). The latter exhibits very good convergence, leading to a remarkably stable result in the very wide range $s_0 = 1.0 - 4.0 {GeV}^2$, where $s_0$ is the radius of the integration co…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesStrange quarkHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Perturbative QCDFOS: Physical sciencesGluon condensateHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSum rule in quantum mechanicsNuclear Experiment
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LIGHT QUARK MASSES FROM QCD SUM RULES

2013

Recent QCD sum rule determinations of the light quark masses are reviewed. In the case of the strange quark mass, possible uncertainties are discussed in the framework of finite energy sum rules.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsStrange quarkParticle physicsQCD sum rulesHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyAstronomy and AstrophysicsStrangenessBottom quarkHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Sum rule in quantum mechanicsModern Physics Letters A
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Asymptotic 3-loop heavy flavor corrections to the charged current structure functions FLW+−W−(x,Q2) and F2W+−W−(x,Q2)

2016

We derive the massive Wilson coefficients for the heavy flavor contributions to the nonsinglet charged current deep-inelastic scattering structure functions ${F}_{L}^{{W}^{+}}(x,{Q}^{2})\ensuremath{-}{F}_{L}^{{W}^{\ensuremath{-}}}(x,{Q}^{2})$ and ${F}_{2}^{{W}^{+}}(x,{Q}^{2})\ensuremath{-}{F}_{2}^{{W}^{\ensuremath{-}}}(x,{Q}^{2})$ in the asymptotic region ${Q}^{2}\ensuremath{\gg}{m}^{2}$ to 3-loop order in quantum chromodynamics at general values of the Mellin variable $N$ and the momentum fraction $x$. Besides the heavy quark pair production, also the single heavy flavor excitation $s\ensuremath{\rightarrow}c$ contributes. Numerical results are presented for the charm quark contributions, …

Quantum chromodynamicsQuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)01 natural sciencesCharm quarkLoop (topology)Pair production0103 physical sciencesHigh Energy Physics::ExperimentSum rule in quantum mechanics010306 general physicsCharged currentPhysical Review D
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Charm quark mass with calibrated uncertainty

2016

We determine the charm quark mass ${\hat m}_c({\hat m}_c)$ from QCD sum rules of moments of the vector current correlator calculated in perturbative QCD. Only experimental data for the charm resonances below the continuum threshold are needed in our approach, while the continuum contribution is determined by requiring self-consistency between various sum rules, including the one for the zeroth moment. Existing data from the continuum region can then be used to bound the theoretical error. Our result is ${\hat m}_c({\hat m}_c) = 1272 \pm 8$ MeV for $\hat\alpha_s(M_Z) = 0.1182$. Special attention is given to the question how to quantify and justify the uncertainty.

QuarkParticle physicsCurrent (mathematics)Physics and Astronomy (miscellaneous)High Energy Physics::LatticeFOS: Physical sciences01 natural sciencesCharm quarkHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesContinuum (set theory)Charm (quantum number)010306 general physicsEngineering (miscellaneous)PhysicsQCD sum rulesContinuum (measurement)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDMoment (mathematics)High Energy Physics - PhenomenologyZeroth law of thermodynamicsHigh Energy Physics::ExperimentSum rule in quantum mechanicsCurrent vectorThe European Physical Journal C
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Triquark correlations and pentaquarks in a QCD sum rule approach

2005

The role of quark correlations in the description of hadron dynamics in many domains of physics, from low energy dynamics to very hot(dense) systems, is being appreciated. Strong correlations of two quarks (diquark) have been widely investigated in this respect. Recently, we have proposed a dynamical scheme to describe the $\Theta^+$ pentaquark in which also three quark correlations (triquark) were instrumental in producing a low mass exotic state. We perform a study, within the QCD sum rule approach including OPE and direct instanton contributions, of triquark correlations and obtain two quasi-bound light $ud\bar{s}$ color quark clusters of 800 MeV and 930 MeV respectively.

QuarkParticle physicsNuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::LatticeHadronNuclear TheoryQuarksFOS: Physical sciencesHadronsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)InstantonOperator product expansionQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyFísicaPentaquarkPentaquarkDiquarkHigh Energy Physics - PhenomenologyExotic baryonHigh Energy Physics::ExperimentSum rule in quantum mechanics
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Lattice-constrained parametrizations of form factors for semileptonic and rare radiative B decays

1997

We describe the form factors for B to rho lepton neutrino and B to K* gamma decays with just two parameters and the two form factors for B to pi lepton neutrino with a further two or three parameters. The parametrizations are consistent with heavy quark symmetry, kinematic constraints and lattice results, which we use to determine the parameters. In addition, we test versions of the parametrizations consistent (or not) with light-cone sum rule scaling relations at q^2=0.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-latLattice QCD calculationFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsSemileptonic and rare radiative decays of B mesonsHigh Energy Physics - LatticeDetermination of Cabibbo-Kobayashi-Maskawa matrix elementsLattice (order)Radiative transferHigh Energy Physics::ExperimentSum rule in quantum mechanicsNeutrinoScalingHeavy quark effective theoryTwo-formLepton
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Semileptonic decays of theBcmeson

2001

We study the semileptonic transitions ${B}_{c}\ensuremath{\rightarrow}{\ensuremath{\eta}}_{c},$ $J/\ensuremath{\psi},$ D, ${D}^{*},$ B, ${B}^{*},$ ${B}_{s},$ ${B}_{s}^{*}$ in the framework of a relativistic constituent quark model. We use experimental data on leptonic $J/\ensuremath{\psi}$ decay, lattice and QCD sum rule results on leptonic ${B}_{c}$ decay, and experimental data on radiative ${\ensuremath{\eta}}_{c}$ transitions to adjust the quark model parameters. We compute all form factors of the above semileptonic ${B}_{c}$ transitions and give predictions for various semileptonic ${B}_{c}$ decay modes including their $\ensuremath{\tau}$ modes when they are kinematically accessible. Th…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelConstituent quarkBottom quarkLattice (order)High Energy Physics::ExperimentSum rule in quantum mechanicsPhysical Review D
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B and B-s decay constants from QCD duality at three loops

2004

Using special linear combinations of finite energy sum rules which minimize the contribution of the unknown continuum spectral function, we compute the decay constants of the pseudoscalar mesons B and B_s. In the computation, we employ the recent three loop calculation of the pseudoscalar two-point function expanded in powers of the running bottom quark mass. The sum rules show remarkable stability over a wide range of the upper limit of the finite energy integration. We obtain the following results for the pseudoscalar decay constants: f_B=178 \pm 14 MeV and f_{B_s}=200 \pm 14 MeV. The results are somewhat lower than recent predictions based on Borel transform, lattice computations or HQET…

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyLattice (group)FOS: Physical sciencesDuality (optimization)FísicaBottom quarkPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSum rule in quantum mechanics
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Detailed quantum-chromodynamic predictions for high-pTprocesses

1978

High-${p}_{T}$ single-particle inclusive cross section calculations are presented for the CERN ISR and ISABELLE energy ranges, taking into account all lowest-order hard-scattering subprocesses required by quantum chromodynamics (QCD). The input quark and gluon distribution and fragmentation functions were determined from analyses of deep-inelastic lepton data and were subject to various theoretical constraints such as sum rules and SU(3) symmetry. We thoroughly discuss the effects of the individual contributions from fermionic and gluonic subprocesses, as well as those effects stemming from QCD scaling violations in parton distributions and/or fragmentation functions. In particular, the inc…

QuarkQuantum chromodynamicsPhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPartonGluonHigh Energy Physics::ExperimentProduction (computer science)Sum rule in quantum mechanicsNuclear ExperimentEnergy (signal processing)LeptonPhysical Review D
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A QCD calculation of the pion-nucleon sigma-term

1988

We present the results of a QCD sum rule calculation of the pion-nucleon sigma-term. Depending on the uncertain value of the four quark condensate we obtain σ=10...40 MeV.

QuarkQuantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQCD vacuumSigmaElementary particlePionHigh Energy Physics::ExperimentSum rule in quantum mechanicsNuclear ExperimentNucleonEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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