Search results for "Heavy Quark Effective Theory"

showing 10 items of 24 documents

Polarization effects in exclusive semi-leptonic Λc and Λb charm and bottom baryon decays

1992

Abstract We discuss polarization effects in semi-leptonic decays of polarized and unpolarized heavy Λ-type baryons into heavy and into light Λ-type baryons. We use the non-leptonic decay of the daughter baryon and the leptonic decay of the Woff-shell into a lepton pair as polarization analyzers to analyze the polarization of the daughter baryon and the Woff-shell. Technically this is done by writing down joint angular decay distributions. We calculate the values of the various asymmetry parameters that characterize the angular dependence of the angular decay distributions where we use the predictions of the heavy quark effective theory (HQET) supplemented by simple ansatze for the q2-depend…

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectNuclear TheoryHigh Energy Physics::PhenomenologyElementary particlePolarization (waves)AsymmetryBaryonNuclear physicsParticle scatteringHeavy quark effective theoryHigh Energy Physics::ExperimentAngular dependenceNuclear ExperimentLeptonmedia_commonPhysics Letters B
researchProduct

Spectator Effects in the Heavy Quark Effective Theory

1996

We present a complete analysis of the Heavy Quark Effective Theory Lagrangian at order $1/m^2$ in the leading logarithmic approximation, including effects induced by spectator quarks. At this order new correction terms appear in the effective Lagrangian, as four-quark operators containing both heavy and light quark fields. We compute the coefficients of these operators to one-loop order and in the leading-logarithmic approximation. Two of them break the heavy quark spin symmetry and we estimate their contribution to the hyperfine splitting of the heavy mesons in the factorization approximation. We find that they make a positive contribution to the hyperfine splitting of about 10% of the mea…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsLogarithmMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationHeavy quark effective theoryOrder (group theory)High Energy Physics::ExperimentCharm (quantum number)Nuclear ExperimentHyperfine structure
researchProduct

Heavy quark symmetry constraints on semileptonic form factors and decay widths of doubly heavy baryons

2007

We show how heavy quark symmetry constraints on doubly heavy baryon semileptonic decay widths can be used to test the validity of different quark model calculations. The large discrepancies in the results observed between different quark model approaches can be understood in terms of a severe violation of heavy quark spin symmetry constraints by some of those models.

QuarkSemileptonic decayPhysicsParticle physicsNuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelFOS: Physical sciencesFísicaSymmetry (physics)Nuclear Theory (nucl-th)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Heavy quark effective theoryHigh Energy Physics::ExperimentSpin symmetryNuclear ExperimentNuclear theoryPhysics Letters B
researchProduct

Decay constants of B-mesons from non-perturbative HQET with two light dynamical quarks

2014

We present a computation of B-meson decay constants from lattice QCD simulations within the framework of Heavy Quark Effective Theory for the b-quark. The next-to-leading order corrections in the HQET expansion are included non-perturbatively. Based on Nf=2 gauge field ensembles, covering three lattice spacings a (0.08-0.05)fm and pion masses down to 190MeV, a variational method for extracting hadronic matrix elements is used to keep systematic errors under control. In addition we perform a careful autocorrelation analysis in the extrapolation to the continuum and to the physical pion mass limits. Our final results read fB=186(13)MeV, fBs=224(14)MeV and fBs/fB=1.203(65). A comparison with o…

QuarkParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHadronLattice field theoryNuclear Theoryhep-latFOS: Physical sciencesLattice QCD01 natural sciencesNuclear physicsRenormalizationPionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesMeson decayB mesonddc:530010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsHeavy Quark Effective Theory010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologyhep-phLattice QCDHigh Energy Physics - PhenomenologyBottom quarks[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
researchProduct

Nonperturbative effects in semileptonicBcdecays

2001

We discuss the impact of the soft degrees of freedom inside the B_c meson on its rate in the semi-leptonic decay B_c -> X l nu_l where X denotes light hadrons below the D^0 threshold. In particular we identify contributions involving soft hadrons which are non-vanishing in the limit of massless leptons. These contributions become relevant for a measurement of the purely leptonic B_c decay rate, which due to helicity suppression involves a factor m_l^2 and thus is much smaller than the contributions involving soft hadrons.

PhysicsHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesHeavy quark effective theoryHigh Energy Physics::ExperimentBottom quarkPhysical Review D
researchProduct

Masses and decay constants of D(s)* and B(s)* mesons with Nf=2+1+1 twisted mass fermions

2017

We present a lattice calculation of the masses and decay constants of ${D}_{(s)}^{*}$ and ${B}_{(s)}^{*}$ mesons using the gauge configurations produced by the European Twisted Mass Collaboration (ETMC) with ${N}_{f}=2+1+1$ dynamical quarks at three values of the lattice spacing $a\ensuremath{\sim}(0.06\ensuremath{-}0.09)\text{ }\text{ }\mathrm{fm}$. Pion masses are simulated in the range ${M}_{\ensuremath{\pi}}\ensuremath{\simeq}(210--450)\text{ }\text{ }\mathrm{MeV}$, while the strange and charm sea-quark masses are close to their physical values. We compute the ratios of vector to pseudoscalar masses and decay constants for various values of the heavy-quark mass ${m}_{h}$ in the range $0…

PhysicsMeson010308 nuclear & particles physicsFermion01 natural sciencesPseudoscalar mesonPseudoscalarCrystallographyLattice constantPionLattice (order)0103 physical sciencesHeavy quark effective theoryStatistical physics010306 general physicsPhysical Review D
researchProduct

Measurement of theΛb0lifetime in the exclusive decayΛb0→J/ψΛ0inpp¯collisions ats=1.96  TeV

2012

We measure the Lambda_b^0 lifetime in the fully reconstructed decay Lambda_b^0 -> J/psi Lambda^0 using 10.4 fb^-1 of ppbar collisions collected with the D0 detector at sqrt(s)=1.96 TeV. The lifetime of the topologically similar decay channel B^0 -> J/psi K^0_S is also measured. We obtain tau(Lambda_b^0) = 1.303 +- 0.075 (stat.) +- 0.035 (syst.) ps and tau(B^0) = 1.508 +- 0.025 (stat.) +- 0.043 (syst.) ps. Using these measurements, we determine the lifetime ratio of tau(Lambda_b^0)/tau(B^0) = 0.864 +- 0.052 (stat.) +- 0.033 (syst.).

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::Phenomenology0103 physical sciencesHeavy quark effective theoryHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsLambda01 natural sciencesPhysical Review D
researchProduct

The b-quark mass from non-perturbative Nf=2 Heavy Quark Effective Theory at O(1/mh)

2014

Abstract We report our final estimate of the b-quark mass from N f = 2 lattice QCD simulations using Heavy Quark Effective Theory non-perturbatively matched to QCD at O ( 1 / m h ) . Treating systematic and statistical errors in a conservative manner, we obtain m ¯ b MS ¯ ( 2 GeV ) = 4.88 ( 15 ) GeV after an extrapolation to the physical point.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsConservation lawHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryExtrapolationLattice QCDBottom quarkNuclear physicsHeavy quark effective theoryHigh Energy Physics::ExperimentNon-perturbativePhysics Letters B
researchProduct

Using Heavy Quark Fragmentation into Heavy Hadrons to Determine QCD Parameters and Test Heavy Quark Symmetry

1994

We present a detailed analysis of the use of heavy quark fragmentation into heavy hadrons for testing the heavy quark effective theory through comparison of the measured fragmentation parameters of the $c$ and $b$ quarks. Our analysis is entirely model independent. We interpret the known perturbative evolution in a way useful for exploiting heavy quark symmetry at low energy. We first show consistency with perturbative QCD scaling for measurements done solely with $c$ quarks. We then apply the perturbative analysis and the heavy quark expansion to relate measurements from ARGUS and LEP. We place bounds on a nonperturbative quark mass suppressed parameter, and compare the values for the $b$ …

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsArgusHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyPerturbative QCDFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Fragmentation (mass spectrometry)Heavy quark effective theoryHigh Energy Physics::ExperimentNuclear ExperimentScalingcomputercomputer.programming_language
researchProduct

Hidden charm molecules in finite volume

2013

In the present paper we address the interaction of pairs of charmed mesons with hidden charm in a finite box. We use the interaction from a recent model based on heavy-quark spin symmetry that predicts molecules of hidden charm in the infinite volume. The energy levels in the box are generated within this model, and from them some synthetic data are generated. These data are then employed to study the inverse problem of getting the energies of the bound states and phase shifts for D (D) over bar or D*(D) over bar*. Different strategies are investigated using the lowest two levels for different values of the box size, and the errors produced are studied. Starting from the upper level, fits t…

PhysicsNuclear and High Energy PhysicsParticle physicsQuantum-field theories010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Library scienceFOS: Physical sciencesFísica01 natural sciences7. Clean energyHigh Energy Physics - Lattice0103 physical sciencesEnergy spectrumHeavy quark effective theorySpin symmetryCharm (quantum number)010306 general physicsEnergy-spectrum
researchProduct