Search results for "Up quark"

showing 10 items of 19 documents

Light baryons and their electromagnetic interactions in the covariant constituent quark model

2012

We extend the confined covariant constituent quark model that was previously developed by us for mesons to the baryon sector. In our numerical calculation we use the same values for the constituent quark masses and the infrared cutoff as have been previously used in the meson sector. In a first application we describe the static properties of the proton and neutron, and the $\Lambda$-hyperon (magnetic moments and charge radii) and the behavior of the nucleon form factors at low momentum transfers. We discuss in some detail the conservation of gauge invariance of the electromagnetic transition matrix elements in the presence of a nonlocal coupling of the baryons to the three constituent quar…

Nuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryConstituent quarkDown quarkFOS: Physical sciencesPROTONBottom quarkHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentPhysicsCOMPOSITE PARTICLESELASTIC SCATTERINGPOLARIZATION TRANSFERHigh Energy Physics::PhenomenologyHyperonRELATIVISTIC 3-QUARK MODELMAGNETIC FORM-FACTORDEUTERONBaryonHigh Energy Physics - PhenomenologyQuantum electrodynamicsHEAVY BARYONSUp quarkNEUTRONHigh Energy Physics::ExperimentSQUARED 4-MOMENTUM TRANSFERSNucleon
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Quark mean field model for nucleons in nuclei

1998

We propose the quark mean field model for nucleons in nuclei, where the meson mean fields created by other nucleons act on quarks in a nucleon and change the nucleon properties in nuclei. We take the constituent quark model for the nucleon, which naturally allows the direct coupling of pions and in turn other mesons as $\ensuremath{\sigma}$ and $\ensuremath{\omega}$ mesons. We find very good nuclear matter properties with the use of the nonlinear self-energy terms in the meson Lagrangian. We expect the spin-orbit splitting in finite nuclei to be large due to the large reduction of the nucleon mass, which is in agreement with experiment. The nucleon size increases by about 7% at the normal m…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryDown quarkConstituent quarkBottom quarkNuclear physicsStrange matterPionUp quarkHigh Energy Physics::ExperimentNuclear ExperimentNucleonPhysical Review C
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Integrating out strange quarks in ChPT

2007

We study three flavour chiral perturbation theory in a limit where the strange quark mass is much larger than the external momenta and the up and down quark masses, and where the external fields are those of two-flavour chiral perturbation theory. In this case, the theory reduces to the one of SU(2)_L x SU(2)_R. Through this reduction, one can work out the strange quark mass dependence of the LECs in the two-flavour case. We present the pertinent relations at two-loop order for F,B and l_i.

PhysicsNuclear and High Energy PhysicsStrange quarkParticle physicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourNuclear TheoryHigh Energy Physics::PhenomenologyDown quarkFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quark star0103 physical sciencesUp quarkHigh Energy Physics::ExperimentLimit (mathematics)Perturbation theory (quantum mechanics)010306 general physics
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Heavy baryons in the relativistic quark model

2003

Abstract We present a summary of results for exclusive decays of single and double heavy-flavored baryons in the relativistic three-quark model.

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyDown quarkOmega baryonBottom quarkSigma baryonBaryonQuark starUp quarkHigh Energy Physics::ExperimentNuclear ExperimentProgress in Particle and Nuclear Physics
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S-4 model for quarks and leptons with maximal atmospheric angle

2010

We consider a model for quark and lepton masses and mixings based on S-4 flavor symmetry. The model contains six Higgs doublets where three of them give mass to the leptons, and the other three gives mass to the quarks. Charged fermion and quark masses arise from renormalizable interactions while neutrino Majorana masses are generated through effective dimension five Weinberg operator. From the study of the minimization of the scalar potential we found a residual mu tau symmetry in the neutrino sector predicting zero reactor angle and maximal atmospheric angle and for the quark sector we found a four-zero texture. We give a fit of the mass hierarchies and mixing angles in the quark sector.

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeQuark modelHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesUp quarkHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsParticle Physics - PhenomenologyLepton
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Quark-lepton mass relation and CKM mixing in an A(4) extension of the minimal supersymmetric standard model

2013

An interesting mass relation between down-type quarks and charged leptons has been recently predicted within a supersymmetric SU(3)(c) circle times SU(2)(L) circle times U(1)(Y) model based on the A(4) flavor symmetry. Here we propose a simple extension which provides an adequate full description of the quark sector. By adding a pair of vectorlike up quarks, we show how the CKM entries V-ub, V-cb, V-td and V-ts arise from deviations of the unitarity. We perform an analysis including the most relevant observables in the quark sector, such as oscillations and rare decays of kaons, B-d and B-s mesons. In the lepton sector, the model predicts an inverted hierarchy for the neutrino masses, leadi…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsMesonUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryNeutrino masses01 natural sciencesHigh Energy Physics - PhenomenologySymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesUp quarkHigh Energy Physics::Experiment010306 general physicsLepton
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Search for flavor changing neutral currents via quark–gluon couplings in single top quark production using 2.3 fb−1 of pp¯ collisions

2010

We present a search for flavor changing neutral currents via quark-gluon couplings in a sample of single top quark final states corresponding to 2.3 fb(-1) of integrated luminosity collected with the DO detector at the Fermilab Tevatron Collider. We select events containing a single top quark candidates with an additional jet, and obtain separation between signal and background using Bayesian neural networks. We find consistency between background expectation and observed data, and set limits on flavor changing neutral current gluon couplings of the top quark to up quarks (tgu) and charm quarks (tgc). The cross section limits at the 95% C.L. are sigma(tgu) gu) gc) < 3.9 x 10(-3).

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavor-changing neutral currentNuclear TheoryHigh Energy Physics::Phenomenology01 natural sciences7. Clean energyBottom quarkGluonSigma baryonCharm quarkNuclear physics0103 physical sciencesUp quarkHigh Energy Physics::Experiment010306 general physicsPhysics Letters B
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Quark number susceptibilities at high temperatures

2013

We calculate second and fourth order quark number susceptibilities for 2+1 flavor QCD in the high temperature region. In our study we use two improved staggered fermion formulations, namely the highly improved staggered quark formulation, and the so-called p4 formulation, as well as several lattice spacings. Second order quark number susceptibilities are calculated using both improved staggered fermion formulations, and we show that in the continuum limit the two formulations give consistent results. The fourth order quark number susceptibilities are studied only using the p4 formulation and at non-zero lattice spacings. We compare our results on quark number susceptibilities with recent we…

PhysicsQuarkQuantum chromodynamicsNuclear and High Energy PhysicsTop quarkParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesDown quarkTop quark condensateHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Quantum electrodynamicsQuark–gluon plasmaUp quarkStaggered fermionCondensed Matter::Strongly Correlated ElectronsPhysical Review D
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Quark and lepton mixing in weak interactions

1986

The coupling strength of weak interactions between quarks of different flavour shows a clear pattern: couplings between members of the same family are much stronger than the ones between neighbour families and couplings between first and third family haye escaped detection so far. The coupling strength between different families decreases with increasing quark mass, but a theoretical explanation of this pattern is still missing. On the other side, lepton mixing and neutrino oscillations have not been seen in experiments yet. An analysis of experimental data in the framework of simultaneous oscillations of three neutrino fluxes yields limits on the three mixing angles which are about as rest…

PhysicsQuarkTop quarkParticle physicsHigh Energy Physics::PhenomenologyUp quarkDown quarkHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationBottom quarkLepton
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Experimental analysis of weak mixing angles between three or four quark generations

1987

New data on weak quark decays and on weak heavy quark production are used to obtain the allowed ranges of elements of the quark mixing matrix for three or four generations of sequential quarks. The analysis yields allowed ranges for the three mixing angles in the six-quark case and for the six mixing angles in the eight-quark case.

PhysicsQuarkTop quarkParticle physicsPhysics and Astronomy (miscellaneous)Cabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFlavourDown quarkBottom quarkNuclear physicsUp quarkHigh Energy Physics::ExperimentEngineering (miscellaneous)Mixing (physics)Zeitschrift für Physik C Particles and Fields
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