Search results for "RENORMALIZATION"

showing 10 items of 470 documents

The Hunt for New Physics at the Large Hadron Collider

2010

233 páginas.-- AHEP Group: et al..-- El Pdf del artículo es la versión pre-print: arXiv.1001.2693v1.-- Trabajo presentado al "The International Workshop on Beyond the Standard Model Physics and LHC Signatures (BSM-LHC) celebrado en Boston (USA) del 2 al 4 de junio de 2009.

Nuclear and High Energy PhysicsParticle physicsCold dark matterPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelFOS: Physical sciencesRANDALL-SUNDRUM MODEL01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)R-PARITY BREAKING0103 physical sciencesHigh Energy PhysicsANOMALOUS MAGNETIC-MOMENT010306 general physicsParticle Physics - PhenomenologyPhysicsEXPLICIT CP VIOLATIONDARK-MATTER DETECTIONLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionHigh Energy Physics::PhenomenologyFísicaRENORMALIZATION-GROUP EQUATIONSHierarchy problemSupersymmetryAtomic and Molecular Physics and OpticsGRAND UNIFIED THEORIESSUPERSYMMETRIC STANDARD MODELHidden sectorExtra dimensionsHigh Energy Physics - PhenomenologyMINIMAL FLAVOR VIOLATION[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]PhenomenologyHigh Energy Physics::ExperimentHIGGS-BOSON PRODUCTION
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From transition magnetic moments to majorana neutrino masses

2005

It is well known that a majorana mass induces a (small) transition magnetic moment. The converse is also true; in this paper we estimate the loop contribution of transition magnetic moments $[\mu]_{\alpha \beta}$ to the neutrino mass matrix $[m]_{\alpha \beta}$. We show that for hierarchical neutrino masses, the contribution of $[\mu]_{e \tau}$ to $[m]_{e \tau}$ can exceed the experimental value of $[m]_{e \tau}$.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesmental disorders010306 general physicsM-matrixPhysicsMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaRenormalization groupMass matrixequipment and suppliesLoop (topology)MAJORANAHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]NeutrinoMass hierarchyhuman activities
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Muon Anomaly from Lepton Vacuum Polarization and The Mellin--Barnes Representation

2008

We evaluate, analytically, a specific class of eighth--order and tenth--order QED contributions to the anomalous magnetic moment of the muon. They are generated by Feynman diagrams involving lowest order vacuum polarization insertions of leptons $l=e,\mu$, and $\tau$. The results are given in the form of analytic expansions in terms of the mass ratios $m_e/m_\mu$ and $m_\mu/m_\tau$. We compute as many terms as required by the error induced by the present experimental uncertainty on the lepton masses. We show how the Mellin--Barnes integral representation of Feynman parametric integrals allows for an easy analytic evaluation of as many terms as wanted in these expansions and how its underlyi…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciences01 natural sciencesRenormalizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Vacuum PolarizationMuon Anomaly0103 physical sciencesFeynman diagramVacuum polarization010306 general physicsMathematical physicsPhysicsMuonMellin-Barnes RepresentationAnomalous magnetic dipole moment010308 nuclear & particles physicsConverse MappingRenormalization groupHigh Energy Physics - PhenomenologyMultidimensional Residues[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]symbolsAnomaly (physics)Lepton
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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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Running of the Charm-Quark Mass from HERA Deep-Inelastic Scattering Data

2017

Physics letters / B 775, 233 - 238 (2017). doi:10.1016/j.physletb.2017.11.002

Nuclear and High Energy PhysicsParticle physicsPhotonHigh Energy Physics::LatticeFOS: Physical sciencesContext (language use)53001 natural sciencesCharm quarkrenormalizationNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesddc:530Charm (quantum number)quantum chromodynamics: perturbation theory010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsScatteringPhysicsHigh Energy Physics::Phenomenologyhigher-order: 1charm: productionHERADeep inelastic scatteringlcsh:QC1-999quark: massHigh Energy Physics - PhenomenologyDESY HERA Storscale dependence[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]charmlcsh:Physics
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Charm and hidden charm scalar mesons in the nuclear medium

2009

We study the renormalization of the properties of low-lying charm and hidden charm scalar mesons in a nuclear medium, concretely of the D-s0(2317) and the theoretical hidden charm state X(3700). We find that for the D-s0(2317), with negligible width at zero density, the width becomes about 100 MeV at normal nuclear-matter density, while in the case of the X(3700) the width becomes as large as 200 MeV. We discuss the origin of this new width and trace it to reactions occurring in the nucleus, while offering a guideline for future experiments testing these changes. We also show how those medium modifications will bring valuable information on the nature of the scalar resonances and the mechan…

Nuclear and High Energy PhysicsParticle physicsTrace (linear algebra)Nuclear TheoryMesonNuclear TheoryScalar (mathematics)FOS: Physical sciencesCHIRAL-SYMMETRY RESTORATIONNuclear Theory (nucl-th)RenormalizationUNITARY APPROACHCharm (quantum number)Nuclear ExperimentNN INTERACTIONPhysicsHEAVY MESONSZero (complex analysis)FísicaLOCAL SYMMETRYMULTIQUARK HADRONSNuclear matterGAUGE BOSONPHI-PHOTOPRODUCTIONHigh Energy Physics::ExperimentPI-PI INTERACTIONNucleonVECTOR-MESONSThe European Physical Journal A
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s-wave pion-nucleus optical potential

2007

We calculate the s-wave part of the pion-nucleus optical potential using a unitarized chiral approach that has been previously used to simultaneously describe pionic hydrogen and deuterium data as well as low energy pi N scattering in the vacuum. This energy dependent model allows for additional isoscalar parts in the potential from multiple rescattering. We consider Pauli blocking and pion polarization in an asymmetric nuclear matter environment. Also, higher order corrections of the pi N amplitude are included. The model can accommodate the repulsion required by phenomenological fits, though the theoretical uncertainties are bigger than previously thought. At the same time, we also find a…

Nuclear and High Energy PhysicsParticle physicsscattering amplitude [pi nucleon]Nuclear Theorymedia_common.quotation_subjectIsoscalarpartial waveNuclear TheoryFOS: Physical sciencesAsymmetryrenormalizationNuclear physicsNuclear Theory (nucl-th)symbols.namesakePionPauli exclusion principlemesic atom [deuterium]unitarityddc:530higher-order [Feynman graph]nuclear reaction [pi nucleus]numerical calculationsNuclear Experimentmedia_commonPhysicschiral [symmetry]UnitarityIsovectorN(1440)FísicaNuclear mattermesic atom [hydrogen]propagator [pi]Scattering amplitudenuclear mattersymbolsoptical [potential]correction [vertex function]
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Gluon mass generation in the massless bound-state formalism

2013

We present a detailed, all-order study of gluon mass generation within the massless bound-state formalism, which constitutes the general framework for the systematic implementation of the Schwinger mechanism in non-Abelian gauge theories. The main ingredient of this formalism is the dynamical formation of bound states with vanishing mass, which give rise to effective vertices containing massless poles; these latter vertices, in turn, trigger the Schwinger mechanism, and allow for the gauge-invariant generation of an effective gluon mass. This particular approach has the conceptual advantage of relating the gluon mass directly to quantities that are intrinsic to the bound-state formation its…

Nuclear and High Energy PhysicsRenormalizationBethe–Salpeter equationHigh Energy Physics::LatticeBackground field methodFOS: Physical sciencesPinch techniqueRenormalizationTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeGauge symmetriesQuantum mechanicsGauge theory3-gluon vertexPhysicsBackground field methodDynamical symmetry breakingGlueballsPhysicsHigh Energy Physics - Lattice (hep-lat)Mass generationInvarianceHigh Energy Physics::PhenomenologyPropagatorQCDGluonMassless particleHigh Energy Physics - PhenomenologyFísica nuclear
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Next-to-next-to-leading order corrections to three-jet observables in electron-positron annihilation.

2008

I report on a numerical program, which can be used to calculate any infrared safe three-jet observable in electron-positron annihilation to next-to-next-to-leading order in the strong coupling constant ${\ensuremath{\alpha}}_{s}$. The results are compared to a recent calculation by another group. Numerical differences in three color factors are discussed and explained.

Nuclear physicsQuantum chromodynamicsPhysicsRenormalizationParticle physicsColor modelAnnihilationElectron–positron annihilationGeneral Physics and AstronomyOrder (ring theory)ObservableJet (particle physics)Physical review letters
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State-of-the-art density matrix renormalization group and coupled cluster theory studies of the nitrogen binding curve.

2004

We study the nitrogen binding curve with the density matrix renormalization group (DMRG) and single-reference and multireference coupled cluster (CC) theory. Our DMRG calculations use up to 4000 states and our single-reference CC calculations include up to full connected hextuple excitations. Using the DMRG, we compute an all-electron benchmark nitrogen binding curve, at the polarized, valence double-zeta level (28 basis functions), with an estimated accuracy of 0.03mE_h. We also assess the performance of more approximate DMRG and CC theories across the nitrogen curve. We provide an analysis of the relative strengths and merits of the DMRG and CC theory under different correlation condition…

Numerical linear algebraValence (chemistry)Density matrix renormalization groupGeneral Physics and Astronomychemistry.chemical_elementBasis functioncomputer.software_genreNitrogenCoupled clusterchemistryMatrix algebraQuantum mechanicsCondensed Matter::Strongly Correlated ElectronsPhysical and Theoretical ChemistrycomputerGroup theoryThe Journal of chemical physics
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