Search results for "QUARK MASS"

showing 10 items of 20 documents

Determination of the Chiral Couplings L10 and C87 from Semileptonic τ Decays

2008

Using recent precise hadronic tau-decay data on the V-A spectral function, and general properties of QCD such as analyticity, the operator product expansion and chiral perturbation theory, we get accurate values for the QCD chiral order parameters L_10^r(M_rho) and C_87^r(M_rho). These two low-energy constants appear at order p^4 and p^6, respectively, in the chiral perturbation theory expansion of the V-A correlator. At order p^4 we obtain L_10^r(M_rho) = -(5.22\pm 0.06)10^{-3}. Including in the analysis the two-loop (order p^6) contributions, we get L_10^r(M_rho) = -(4.06\pm 0.39)10^{-3} and C_87^r(M_rho) = (4.89\pm 0.19)10^{-3}GeV^{-2}. In the SU(2) chiral effective theory, the correspon…

High Energy Physics - Lattice (hep-lat)Spectral functionsFOS: Physical sciencesFísicaPerturbation theoryLow-energy constantsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeStrange quark massQCD predictionsHigh Energy Physics::ExperimentUs-vertical-barHadronic width
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Models with three Higgs doublets in the triplet representations of A4 or S4

2013

We consider the quark sector of theories containing three scalar SU(2)(L) doublets in the triplet representation of A(4) (or S-4) and three generations of quarks in arbitrary A(4) (or S-4) representations. We show that for all possible choices of quark field representations and for all possible alignments of the Higgs vacuum expectation values that can constitute global minima of the scalar potential, it is not possible to obtain simultaneously nonvanishing quark masses and a nonvanishing CP-violating phase in the Cabibbo-Kobayashi-Maskawa quark mixing matrix. As a result, in this minimal form, models with three scalar fields in the triplet representation of A(4) or S-4 cannot be extended t…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaDiscrete SymmetriesHigh Energy Physics::ExperimentMaximal CP nonconservationQuark mass matrices
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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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B parameters of the complete set of matrix elements of delta B = 2 operators from the lattice

2001

We compute on the lattice the ``bag'' parameters of the five (Delta B = 2) operators of the supersymmetric basis, by combining their values determined in full QCD and in the static limit of HQET. The extrapolation of the QCD results from the accessible heavy-light meson masses to the B-meson mass is constrained by the static result. The matching of the corresponding results in HQET and in QCD is for the first time made at NLO accuracy in the MSbar(NDR) renormalization scheme. All results are obtained in the quenched approximation.

Nuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeSTANDARD MODELExtrapolationLattice (group)FOS: Physical sciencesQuenched approximationHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareRenormalizationMatrix (mathematics)High Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quantum chromodynamicsPhysicsNONPERTURBATIVE RENORMALIZATIONBasis (linear algebra)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyQUARK MASSHigh Energy Physics::ExperimentHEAVY QUARKS
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Top quark mass measurement in the lepton plus jets channel using a modified matrix element method

2008

We report a measurement of the top quark mass, m(t), obtained from p(p)over bar collisions at root s=1.96 TeV at the Fermilab Tevatron using the CDF II detector. We analyze a sample corresponding to an integrated luminosity of 1.9 fb(-1). We select events with an electron or muon, large missing transverse energy, and exactly four high-energy jets in the central region of the detector, at least one of which is tagged as coming from a b quark. We calculate a signal likelihood using a matrix element integration method, where the matrix element is modified by using effective propagators to take into account assumptions on event kinematics. Our event likelihood is a function of m(t) and a parame…

Nuclear and High Energy PhysicsTop quarkParticle physicsTevatronFOS: Physical sciencesddc:500.2Jet (particle physics)01 natural sciences7. Clean energyBottom quark114 Physical sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPhysicsLuminosity (scattering theory)Muon010308 nuclear & particles physicshep-exPhysicsHigh Energy Physics::PhenomenologyTOP QUARK MASSCDF14.65.HaHigh Energy Physics::ExperimentEnergy (signal processing)Lepton
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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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Yukawa sector of multi-Higgs-doublet models in the presence of Abelian symmetries

2013

A general method for classifying the possible quark models of a multi-Higgs-doublet model, in the presence of Abelian symmetries, is presented. All the possible sets of textures that can be present in a given sector are shown, thus turning the determination of the flavor models into a combinatorial problem. Several symmetry implementations are studied for two and three Higgs doublet models. Some models' implementations are explored in great detail, with a particular emphasis on models known as Branco-Grimus-Lavoura and nearest-neighbor-interaction. Several considerations on the flavor changing neutral currents of multi-Higgs models are also given.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaQuark mass matricesHigh Energy Physics - PhenomenologyNeutral currentsHigh Energy Physics - Phenomenology (hep-ph)Homogeneous spaceHiggs bosonHigh Energy Physics::ExperimentAbelian group
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Invariants and flavour in the general Two Higgs Doublet Model

2012

The flavour structure of the general Two Higgs Doublet Model (2HDM) is analysed and a detailed study of the parameter space is presented, showing that flavour mixing in the 2HDM can be parametrized by various unitary matrices which arise from the misalignment in flavour space between pairs of various Hermitian flavour matrices which can be constructed within the model. This is entirely analogous to the generation of the CKM matrix in the Standard Model (SM). We construct weak basis invariants which can give insight into the physical implications of any flavour model, written in an arbitrary weak basis (WB) in the context of 2HDM. We apply this technique to two special cases, models with MFV…

PhysicsNuclear and High Energy PhysicsParticle physicsfísica010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFlavourFOS: Physical sciencesUnitary matrixCP-violationParameter space01 natural sciencesHermitian matrixQuark mass matricesBaryogenesisHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)Two-Higgs-doublet modelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsParticle Physics - Phenomenology
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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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