Search results for "symmetry"

showing 10 items of 3576 documents

A$_{FB}$ in the SMEFT: precision Z physics at the LHC

2021

We study the forward-backward asymmetry $A_{FB}$ in $pp \to \ell^+\ell^-$ at the Z peak within the Standard Model Effective Field Theory (SMEFT). We find that this observable provides per mille level constraints on the vertex corrections of the Z boson to quarks,which close a flat direction in the electroweak precision SMEFT fit. Moreover, we show that current $A_{FB}$ data is precise enough so that its inclusion in the fit improves significantly LEP bounds even in simple New Physics setups. This demonstrates that the LHC can compete with and complement LEP when it comes to precision measurements of the Z boson properties

QuarkNuclear and High Energy PhysicsParticle physicsp p: scatteringangular distribution: asymmetryPhysics beyond the Standard Modelmedia_common.quotation_subjectFOS: Physical sciencesQC770-79801 natural sciencesAsymmetryStandard ModelquarkZ0: productionHigh Energy Physics - Phenomenology (hep-ph)effective field theoryflat directionNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesEffective field theory010306 general physicsmedia_commonPhysicsLarge Hadron Colliderelectroweak interaction010308 nuclear & particles physicsprecision measurementnew physicsElectroweak interactionHigh Energy Physics::PhenomenologyObservableCERN LEP StorEffective Field Theoriescorrection: vertexHigh Energy Physics - Phenomenologyp p --> lepton+ lepton-CERN LHC Coll[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelHigh Energy Physics::Experiment
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D mesic nuclei

2010

The energies and widths of several D-0 meson bound states for different nuclei are obtained using a D-meson selfenergy in the nuclear medium, which is evaluated in a selfconsistent manner using techniques of unitarized coupled-channel theory. The kernel of the meson-baryon interaction is based on a model that treats heavy pseudoscalar and heavy vector mesons on equal footing, as required by heavy quark symmetry. We find D-0 bound states in all studied nuclei, from C-12 up to Pb-208. The inclusion of vector mesons is the keystone for obtaining an attractive D-nucleus interaction that leads to the existence of D-0-nucleus bound states, as compared to previous studies based on SU(4) flavor sym…

QuarkNuclear reactionNuclear and High Energy PhysicsParticle physicsCharmNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesHEAVY-ION COLLISIONS01 natural sciences7. Clean energyBOUND-STATESHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsENERGYHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)ANTIPROTON ANNIHILATION0103 physical sciencesBound stateHeavy quark effective theorySCATTERINGNuclear Experiment (nucl-ex)Basso continuoNuclear Experiment010306 general physicsNuclear ExperimentSUPPRESSIONPhysicsPIONIC ATOMS010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCHIRAL DYNAMICSHeavy quark symmetryETAPseudoscalarHigh Energy Physics - PhenomenologyMesic nucleiPhysics Letters B
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Cosmic QCD Epoch at Nonvanishing Lepton Asymmetry

2018

We investigate how a lepton asymmetry impacts the cosmic trajectory in the QCD phase diagram. We study the evolution of chemical potentials during the QCD epoch of the early Universe using susceptibilities from lattice QCD to interpolate between an ideal quark gas and an ideal hadron resonance gas. The lepton asymmetry affects the evolution of all chemical potentials. The standard cosmic trajectory is obtained assuming tiny lepton and baryon asymmetries. For larger lepton asymmetry, the charge chemical potential exceeds the baryon chemical potential before pion annihilation.

QuarkParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesAsymmetryHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - Lattice0103 physical sciences010306 general physicsmedia_commonQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDUniverseBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Neutrino masses and mixing: a flavour symmetry roadmap

2012

Over the last ten years tri-bimaximal mixing has played an important role in modeling the flavour problem. We give a short review of the status of flavour symmetry models of neutrino mixing. We concentrate on non-Abelian discrete symmetries, which provide a simple way to account for the TBM pattern. We discuss phenomenological implications such as neutrinoless double beta decay, lepton flavour violation as well as theoretical aspects such as the possibility to explain quarks and leptons within a common framework, such as grand unified models

QuarkParticle physicsNuclear TheoryHigh Energy Physics::LatticeFlavourFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesneutrino mixingNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciences010306 general physicsMixing (physics)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaNeutrino massesCommon frameworkSymmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoflavour symmetryLeptonFortschritte der Physik
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Charmed Mesons in Nuclei with Heavy-Quark Spin Symmetry

2012

We study the properties of charmed pseudoscalar and vector mesons in dense matter within a unitary meson-baryon coupled-channel model which incorporates heavy-quark spin symmetry. This is accomplished by extending the SU(3) Weinberg-Tomozawa Lagrangian to SU(8) spin-flavor symmetry and implementing a suitable flavor symmetry breaking. Several resonances with negative parity are generated dynamically by the s-wave interaction between pseudoscalar and vector meson multiplets with $1/2^+$ and $3/2^+$ baryons. Those states are then compared to experimental data as well as theoretical models. Next, Pauli-blocking effects and meson self-energies are introduced in a self-consistent manner to obtai…

QuarkParticle physicsNuclear TheoryMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesUnitary stateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesVector mesonSymmetry breakingNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaParity (physics)Atomic and Molecular Physics and OpticsPseudoscalarBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentFew-Body Systems
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The forward-backward asymmetry for massive bottom quarks at the $Z$ peak at next-to-next-to-leading order QCD

2017

We compute the order $\alpha_s^2$ QCD corrections to the $b$-quark forward-backward asymmetry in $e^+e^-\to b{\bar b}$ collisions at the $Z$ boson resonance, taking the non-zero mass of the $b$ quark into account. We determine these corrections with respect to both the $b$-quark axis and the thrust axis definition of the asymmetry. We compute also the distributions of these axes with respect to the electron beam. If one neglects the flavor singlet contributions to the $b$-quark asymmetry, as was done in previous computations for massless $b$ quarks, then the second-order QCD corrections for $m_b\neq 0$ are smaller in magnitude than the corresponding corrections for $m_b=0$. Including the si…

QuarkParticle physicsNuclear and High Energy Physics530 Physicsmedia_common.quotation_subjectHigh Energy Physics::LatticeFOS: Physical sciences10192 Physics Institute01 natural sciencesAsymmetryResonance (particle physics)Standard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences3106 Nuclear and High Energy Physics010306 general physicsmedia_commonBosonQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)Massless particleHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Inclusive search for same-sign dilepton signatures in pp collisions at $ sqrt {s} = 7 $ TeV with the ATLAS detector

2011

An inclusive search is presented for new physics in events with two isolated leptons (e or mu) having the same electric charge. The data are selected from events collected from p p collisions at root s = 7 TeV by the ATLAS detector and correspond to an integrated luminosity of 34 pb(-1). The spectra in dilepton invariant mass, missing transverse momentum and jet multiplicity are presented and compared to Standard Model predictions. In this event sample, no evidence is found for contributions beyond those of the Standard Model. Limits are set on the cross-section in a fiducial region for new sources of same-sign high-mass dilepton events in the ee, e mu and mu mu channels. Four models predic…

QuarkParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências FísicasPhysics beyond the Standard Model:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.201 natural sciences530High Energy Physics - ExperimentNuclear physicsUniversal extra dimensionHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massddc:530High Energy Physics010306 general physicsCiencias ExactasPhysicsScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsATLAS DetectorSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyFísicaSupersymmetryATLAS16. Peace & justiceMAJORANAproton-proton collisionsHigh Energy Physics::ExperimentFísica nuclearLHCNeutrinoParticle Physics - ExperimentLepton
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Bridging a gap between continuum-QCD and ab initio predictions of hadron observables

2015

Within contemporary hadron physics there are two common methods for determining the momentum-dependence of the interaction between quarks: the top-down approach, which works toward an ab initio computation of the interaction via direct analysis of the gauge-sector gap equations; and the bottom-up scheme, which aims to infer the interaction by fitting data within a well-defined truncation of those equations in the matter sector that are relevant to bound-state properties. We unite these two approaches by demonstrating that the renormalisation-group-invariant running-interaction predicted by contemporary analyses of QCD's gauge sector coincides with that required in order to describe ground-s…

QuarkParticle physicsNuclear and High Energy PhysicsNuclear TheoryHigh Energy Physics::LatticeGribov copiesHadronAb initioFOS: Physical sciencesNuclear Theory (nucl-th)High Energy Physics::TheoryHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Hadron physicsFragmentationBound stateNuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaObservablelcsh:QC1-999High Energy Physics - PhenomenologyDyson–Schwinger equationsDynamical chiral symmetry breakingPreprintlcsh:PhysicsConfinementPhysics Letters B
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Interplay among transversity induced asymmetries in hadron leptoproduction

2015

In the fragmentation of a transversely polarized quark several left-right asymmetries are possible for the hadrons in the jet. When only one unpolarized hadron is selected, it exhibits an azimuthal modulation known as Collins effect. When a pair of oppositely charged hadrons is observed, three asymmetries can be considered, a di-hadron asymmetry and two single hadron asymmetries. In lepton deep inelastic scattering on transversely polarized nucleons all these asymmetries are coupled with the transversity distribution. From the high statistics COMPASS data on oppositely charged hadron-pair production we have investigated for the first time the dependence of these three asymmetries on the dif…

QuarkParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subjectHadronNuclear TheoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesAsymmetryHigh Energy Physics - ExperimentNuclear physicsSubatomär fysikHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Compass0103 physical sciencesSubatomic Physics010306 general physicsNuclear Experimentmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDeep inelastic scatteringlcsh:QC1-999High Energy Physics - PhenomenologyAngular dependenceHigh Energy Physics::ExperimentNucleonlcsh:PhysicsParticle Physics - ExperimentLepton
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Search for neutral and charged Higgs bosons in $e^+ e^-$ collisions at $\sqrt{s}$= 161 GeV and 172 GeV

1998

A search for neutral and charged Higgs bosons has been performed in the data collected by the {\sc DELPHI} detector at centre-of-mass energies of 161~GeV and 172~GeV. The analysis assumes either the pair-production of charged Higgs bosons, ${\mathrm H}^{\pm}$, or the production of the lightest neutral Higgs boson, h, with either a Z or a neutral pseudoscalar Higgs boson, A. All final state topologies expected from the decay of h and A %neutral Higgs particles into hadrons or a pair of $\tau$ leptons, and from the decay of ${\mathrm H}^{\pm}$ %charged Higgs bosons into a pair of quarks or a $\tau \nu_{\tau}$ pair have been considered. %In the case of the associated production with a Z boson,…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)LOWEST ORDER CALCULATIONSElectron–positron annihilationHigh Energy Physics::LatticeHadronMONTE-CARLO SIMULATIONSTANDARD MODEL2-PHOTON PROCESSES01 natural sciencesPartícules (Física nuclear)Nuclear physicsPHYSICS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSNuclear Experiment010306 general physicsEngineering (miscellaneous)SUPERSYMMETRYDELPHIBosonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySupersymmetryE+E-ANNIHILATIONLARGE ELECTRON POSITRON COLLIDERMONTE-CARLO SIMULATION; LOWEST ORDER CALCULATIONS; E+E-ANNIHILATION; RADIATIVE-CORRECTIONS; 2-PHOTON PROCESSES; STANDARD MODEL; Z(0) DECAYS; PHYSICS; SUPERSYMMETRYZ(0) DECAYSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentParticle Physics - ExperimentLepton
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