Search results for "QCD"

showing 10 items of 614 documents

Two-parton contribution to the heavy-quark forward–backward asymmetry in NNLO QCD

2006

Forward-backward asymmetries, $A_{FB}^Q$, are important observables for the determination of the neutral-current couplings of heavy quarks in inclusive heavy quark production, $e^+ e^- \to \gamma^*, Z^* \to Q +X$. In view of the measurement perspectives on $A_{FB}^Q$ at a future linear collider, precise predictions of $A_{FB}^Q$ are required for massive quarks. We compute the contribution of the $Q \bar Q$ final state to $A_{FB}^Q$ to order $\as^2$ in the QCD coupling. We provide general formulae, and we show that this contribution to $A_{FB}^Q$ is infrared-finite. We evaluate these two-parton contributions for $b$ and $c$ quarks on and near the $Z$ resonance, and for $t$ quarks above thres…

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::Latticemedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesParton01 natural sciencesAsymmetrylaw.inventionNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesPERTURBATIVE QCDNuclear Experiment010306 general physicsCollidermedia_commonCondensed Matter::Quantum GasesPhysicsQuantum chromodynamicsCouplingASYMMETRY IN NNLO QCD010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyResonanceObservableHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentHEAVY QUARKSRADIATIVE CORRECTIONSNuclear Physics B
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B-physics from non-perturbatively renormalized HQET in two-flavour lattice QCD.

2012

We report on the ALPHA Collaboration's lattice B-physics programme based on N_f=2 O(a) improved Wilson fermions and HQET, including all NLO effects in the inverse heavy quark mass, as well as non-perturbative renormalization and matching, to fix the parameters of the effective theory. Our simulations in large physical volume cover 3 lattice spacings a ~ (0.08-0.05) fm and pion masses down to 190 MeV to control continuum and chiral extrapolations. We present the status of results for the b-quark mass and the B_(s)-meson decay constants, f_B and f_{B_s}.

QuarkNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeFOS: Physical sciences01 natural sciencesRenormalizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticePionLattice (order)0103 physical sciencesEffective field theoryNuclear Experiment010306 general physicsPhysics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyParticle Physics - LatticeFermionLattice QCDAtomic and Molecular Physics and OpticsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Triply heavy baryons and heavy quark spin symmetry

2011

We study the semileptonic $b\to c$ decays of the lowest-lying triply-heavy baryons made from $b$ and $c$ quarks in the limit $m_b, m_c \gg \Lambda_\mathrm{QCD}$ and close to the zero recoil point. The separate heavy quark spin symmetries strongly constrain the matrix elements, leading to single form factors for $ccb\to ccc$, $bbc\to ccb$, and $bbb\to bbc$ baryon decays. We also study the effects on these systems of using a $Y$-shaped confinement potential, as suggested by lattice QCD results for the interaction between three static quarks.

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeLattice field theoryFOS: Physical sciencesLambda01 natural sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentSpin-½PhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)FísicaLattice QCDBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Nucleon structure from Lattice QCD using a nearly physical pion mass

2014

We report the first Lattice QCD calculation using the almost physical pion mass mpi=149 MeV that agrees with experiment for four fundamental isovector observables characterizing the gross structure of the nucleon: the Dirac and Pauli radii, the magnetic moment, and the quark momentum fraction. The key to this success is the combination of using a nearly physical pion mass and excluding the contributions of excited states. An analogous calculation of the nucleon axial charge governing beta decay has inconsistencies indicating a source of bias at low pion masses not present for the other observables and yields a result that disagrees with experiment.

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryLattice field theoryFOS: Physical sciencesLattice QCDNuclear Theory (nucl-th)Nucleon structureNuclear physicssymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Pauli exclusion principlePionddc:530Nuclear ExperimentPhysicsQuantum chromodynamicsIsovectorHigh Energy Physics - Lattice (hep-lat)Form factorsLattice QCDHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentNucleonPhysics Letters B
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Light quark masses and pseudoscalar decay constants from N(f)=2 Lattice QCD with twisted mass fermions

2007

We present the results of a lattice QCD calculation of the average up-down and strange quark masses and of the light meson pseudoscalar decay constants with Nf=2 dynamical fermions. The simulation is carried out at a single value of the lattice spacing with the twisted mass fermionic action at maximal twist, which guarantees automatic O(a)-improvement of the physical quantities. Quark masses are renormalized by implementing the non-perturbative RI-MOM renormalization procedure. Our results for the light quark masses are m_ud^{msbar}(2 GeV)= 3.85 +- 0.12 +- 0.40 MeV, m_s^{msbar}(2 GeV) = 105 +- 3 +- 9 MeV and m_s/m_ud = 27.3 +- 0.3 +- 1.2. We also obtain fK = 161.7 +- 1.2 +- 3.1 MeV and the …

QuarkNuclear and High Energy PhysicsParticle physicsStrange quarkMesonHigh Energy Physics::LatticeWeak decaysLattice field theoryFOS: Physical sciencesLattice QCD[PHYS.HLAT] Physics [physics]/High Energy Physics - Lattice [hep-lat]7. Clean energy01 natural sciencesHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsQuark masses and SM parametersPhysicsUnitarity[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaParticle Physics - LatticeLattice QCDFermionSettore FIS/02 - Fisica Teorica Modelli e Metodi Matematici3. Good healthPseudoscalarHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Kaon physics; Lattice QCD; Quark masses and SM parameters; Weak decaysHigh Energy Physics::ExperimentKaon physics
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Top quarks, axigluons and charge asymmetries at hadron colliders

2007

Final full-text version available at: http://dx.doi.org/10.1103/PhysRevD.77.014003

QuarkNuclear and High Energy PhysicsParticle physicsTop quarkmedia_common.quotation_subjectTevatronFOS: Physical sciencesAsymmetryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Chiral colormedia_commonPhysicsQuantum chromodynamicsGauge bosonHigh Energy Physics::PhenomenologyFísicaTop quarkQCDGluonTevatronHigh Energy Physics - PhenomenologyAxigluonHigh Energy Physics::ExperimentLHC
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Pion radiative weak decays in nonlocal chiral quark models

2010

We analyze the radiative pion decay pi+ -> e+ nu_e gamma within nonlocal chiral quark models that include wave function renormalization. In this framework we calculate the vector and axial-vector form factors FV and FA at q^2=0 --where q^2 is the (e+ ��_e) squared invariant mass-- and the slope a of FV(q^2) at q^2 -> 0. The calculations are carried out considering different nonlocal form factors, in particular those taken from lattice QCD evaluations, showing a reasonable agreement with the corresponding experimental data. The comparison of our results with those obtained in the (local) NJL model and the relation of FV and a with the form factor in pi^0 -> gamma* gamma decays are d…

QuarkNuclear and High Energy PhysicsParticle physicsWave function renormalizationHigh Energy Physics::LatticeFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)RenormalizationPionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio model0103 physical sciencesInvariant mass010306 general physicsPhysics010308 nuclear & particles physicsQuark modelHigh Energy Physics::PhenomenologyFísicaLattice QCDPion radiative weak decaysNonlocal quark modelsHigh Energy Physics - PhenomenologyFísica nuclearHigh Energy Physics::Experiment
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Parton distributions and lattice QCD calculations: A community white paper

2018

Progress in particle and nuclear physics 100, 107 - 160 (2018). doi:10.1016/j.ppnp.2018.01.007

QuarkNuclear and High Energy PhysicsParticle physicsquark: distribution functiondata analysis methodHigh Energy Physics::LatticeLattice field theoryhadron: spinFOS: Physical sciencesparton: distribution functionPartonLattice QCD01 natural sciences530hard scatteringHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)benchmarkFactorization0103 physical sciencesquantum chromodynamicsquantum chromodynamics: factorizationddc:530010306 general physicsGlobal QCD fitsQuantum chromodynamicsPhysicspolarizationgluon: distribution function010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologylattice field theory[ PHYS.HLAT ] Physics [physics]/High Energy Physics - Lattice [hep-lat]ObservableLattice QCDGluonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentUnpolarized/polarized parton distribution functions (PDFs)
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Light- and strange-quark mass dependence of the ρ(770) meson revisited

2020

Recent lattice data on $\pi\pi$-scattering phase shifts in the vector-isovector channel, pseudoscalar meson masses and decay constants for strange-quark masses smaller or equal to the physical value allow us to study the strangeness dependence of these observables for the first time. We perform a global analysis on two kind of lattice trajectories depending on whether the sum of quark masses or the strange-quark mass is kept fixed to the physical point. The quark mass dependence of these observables is extracted from unitarized coupled-channel one-loop Chiral Perturbation Theory. This analysis guides new predictions on the $\rho(770)$ meson properties over trajectories where the strange-qua…

QuarkNuclear and High Energy PhysicsStrange quarkParticle physicsChiral perturbation theoryMeson530 PhysicsHigh Energy Physics::LatticeNuclear TheoryLattice QCDStrangeness01 natural sciencesPseudoscalar mesonHigh Energy Physics - Lattice0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsPhysicsTeoría de los quanta010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyObservableLattice QCDHigh Energy Physics - PhenomenologyChiral LagrangiansPartículaslcsh:QC770-798High Energy Physics::ExperimentJournal of High Energy Physics
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String breaking by light and strange quarks in QCD

2019

The energy spectrum of a system containing a static quark anti-quark pair is computed for a wide range of source separations using lattice QCD with $N_\mathrm{f}=2+1$ dynamical flavours. By employing a variational method with a basis including operators resembling both the gluon string and systems of two separated static mesons, the first three energy levels are determined up to and beyond the distance where it is energetically favourable for the vacuum to screen the static sources through light- or strange-quark pair creation, enabling both these screening phenomena to be observed. The separation dependence of the energy spectrum is reliably parameterised over this saturation region with a…

QuarkNuclear and High Energy PhysicsStrange quarkParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesLattice QCD01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHeavy quarks0103 physical sciences010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDQuarkoniumString breakinglcsh:QC1-999GluonHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics::Experimentlcsh:PhysicsPhysics Letters
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