Search results for "quark masses"

showing 8 items of 8 documents

Numerical Multi-Loop Calculations via Finite Integrals and One-Mass EW-QCD Drell-Yan Master Integrals

2017

We study a recently-proposed approach to the numerical evaluation of multi-loop Feynman integrals using available sector decomposition programs. As our main example, we consider the two-loop integrals for the $\alpha \alpha_s$ corrections to Drell-Yan lepton production with up to one massive vector boson in physical kinematics. As a reference, we evaluate these planar and non-planar integrals by the method of differential equations through to weight five. Choosing a basis of finite integrals for the numerical evaluation with SecDec3 leads to tremendous performance improvements and renders the otherwise problematic seven-line topologies numerically accessible. As another example, basis integ…

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsSpeedupDifferential equationFOS: Physical sciences01 natural sciencesVector bosonHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPerturbative QCDlcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsMathematical physicsPhysicsQuantum chromodynamicsBasis (linear algebra)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMassless particleLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798LeptonQuark Masses and SM Parameters
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Fitting flavour symmetries: the case of two-zero neutrino mass textures

2018

We present a numeric method for the analysis of the fermion mass matrices predicted in flavour models. The method does not require any previous algebraic work, it offers a $\chi^{2}$ comparison test and an easy estimate of confidence intervals. It can also be used to study the stability of the results when the predictions are disturbed by small perturbations. We have applied the method to the case of two-zero neutrino mass textures using the latest available fits on neutrino oscillations, derived the available parameter space for each texture and compared them. Textures $A_{1}$ and $A_{2}$ seem favoured because they give a small $\chi^{2}$, allow for large regions in parameter space and giv…

Nuclear and High Energy PhysicsFOS: Physical sciencesPerturbation (astronomy)Parameter space01 natural sciencesCosmologyPartícules (Física nuclear)Theoretical physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityAlgebraic number010306 general physicsNeutrino oscillationPhysicsCosmologia010308 nuclear & particles physicsFermionHigh Energy Physics - PhenomenologyComputer Science::Computer Vision and Pattern RecognitionHomogeneous spacelcsh:QC770-798NeutrinoQuark Masses and SM Parameters
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Bilarge neutrino mixing and Abelian flavor symmetry

2012

We explore two bilarge neutrino mixing Anzatze within the context of Abelian flavor symmetry theories: (BL1) sin theta(12) similar to lambda, sin theta(13) similar to lambda, sin theta(23) similar to lambda, and (BL2) sin theta(12) similar to lambda, sin theta(13) similar to lambda, sin theta(23) similar to 1 - lambda. The first pattern is proposed by two of us and is favored if the atmospheric mixing angle theta(23) lies in the first octant, while the second one is preferred for the second octant of theta(23). In order to reproduce the second texture, we find that the flavor symmetry should be U(1) x Z(m), while for the first pattern the flavor symmetry should be extended to U(1) x Z(m) x …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsYukawa texturesRelatively large theta(13)High Energy Physics::PhenomenologyFamily symmetryFísicaFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyCP violationHigh Energy Physics - Phenomenology (hep-ph)Nonzero theta (13)0103 physical sciencesLepton mass matricesFermion massesQuark massesAbelian groupNeutrino010306 general physicsHumanitiesMixing (physics)Physical Review D
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Strange Quark Mass Determination from Cabibbo-Suppressed Tau Decays

1999

29 páginas, 10 tablas.-- arXiv:hep-ph/9909244v1

PhysicsNuclear and High Energy PhysicsStrange quarkParticle physicsHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaQCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Invariant massHigh Energy Physics::ExperimentNuclear ExperimentQuark masses and SM parameters
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Quark masses and the chiral condensate with a non-perturbative renormalization procedure

1999

We determine the quark masses and the chiral condensate in the MSbar scheme at NNLO from Lattice QCD in the quenched approximation at beta=6.0, beta=6.2 and beta=6.4 using both the Wilson and the tree-level improved SW-Clover fermion action. We extract these quantities using the Vector and the Axial Ward Identities and non-perturbative values of the renormalization constants. We compare the results obtained with the two methods and we study the O(a) dependence of the quark masses for both actions.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsquark masses QCD latticeHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaQuenched approximationLattice QCDFermionAtomic and Molecular Physics and OpticsAction (physics)FIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIRenormalizationHigh Energy Physics - LatticeBeta (velocity)High Energy Physics::ExperimentNon-perturbative
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V-us determination from hyperon semileptonic decays

2005

16 páginas, 9 tablas.-- arXiv:hep-ph/0509045v2

PhysicsQuarkSystematic errorNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyHyperonFOS: Physical sciencesFísica1/N ExpansionFirst orderQCDHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSymmetry breakingChiral lagrangiansMixing (physics)Quark masses and SM parameters
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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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Lattice quark masses: a non-perturbative measurement

1998

We discuss the renormalization of different definitions of quark masses in the Wilson and the tree-level improved SW-Clover fermionic action. For the improved case we give the correct relationship between the quark mass and the hopping parameter. Using perturbative and non-perturbative renormalization constants, we extract quark masses in the $\MSbar$ scheme from Lattice QCD in the quenched approximation at $\beta=6.0$, $\beta=6.2$ and $\beta=6.4$ for both actions. We find: $\bar{m}^{\MSbar}(2 GeV)=5.7 \pm 0.1 \pm 0.8$ MeV, $m_s^{\MSbar}(2GeV)= 130 \pm 2 \pm 18 $ MeV and $m_c^{\MSbar}(2 GeV) = 1662\pm 30\pm 230$ MeV.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice (group)FOS: Physical sciencesFísicaQuenched approximationLattice QCDRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQCD quark masses latticeBeta (velocity)High Energy Physics::ExperimentNon-perturbativeNuclear ExperimentBar (unit)
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