Search results for "gauge boson"

showing 10 items of 171 documents

Case in favor of the N*(1700)(3/2(-))

2013

Using an interaction extracted from the local hidden-gauge Lagrangians, which brings together vector and pseudoscalar mesons, and the coupled channels rho N (s wave), pi N (d wave), pi Delta (s wave), and pi Delta (d wave), we look in the region ofv root s = 1400-1850 MeV and find two resonances dynamically generated by the interaction of these channels, which are naturally associated to N*(1520)(3/2(-)) and N*(1700)(3/2(-)). N*(1700)(3/2(-)) appears neatly as a pole in the complex plane. The free parameters of the theory are chosen to fit the pi N (d-wave) data. Both the real and imaginary parts of the pi N amplitude vanish in our approach in the vicinity of this resonance, which is simila…

Partial-wave análisisPi-nIsobar-modelGauge bosonElectroproductionResonancesAmplitudesTransitionHidden local symmetryDynamics
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Dark photon search in the mass range between 1.5 and 3.4 GeV/c2

2017

Physics letters / B 774, 252 - 257 (2017). doi:10.1016/j.physletb.2017.09.067

Particle physicsBESIII; Dark photon search; Initial state radiation; Nuclear and High Energy PhysicsNuclear and High Energy PhysicsPhotonBESIII детекторElectron–positron annihilationFOS: Physical sciences01 natural sciences530Dark photonVector bosonStandard ModelHigh Energy Physics - ExperimentNONuclear physicsHigh Energy Physics - Experiment (hep-ex)Dark photon search0103 physical sciencesInvariant massddc:530Dark photon search; Initial state radiation; BESIII010306 general physicsNuclear ExperimentPhysicsGauge boson010308 nuclear & particles physicsтемные фотоныBESIIIlcsh:QC1-999BEPCII коллайдерMass spectrumHigh Energy Physics::ExperimentInitial state radiationlcsh:PhysicsPhysics Letters B
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Lattice Calculation of the Decay of Primordial Higgs Condensate

2015

We study the resonant decay of the primordial Standard Model Higgs condensate after inflation into $SU(2)$ gauge bosons on the lattice. We find that the non-Abelian interactions between the gauge bosons quickly extend the momentum distribution towards high values, efficiently destroying the condensate after the onset of backreaction. For the inflationary scale $H = 10^8$ GeV, we find that 90% of the Higgs condensate has decayed after $n \sim 10$ oscillation cycles. This differs significantly from the Abelian case where, given the same coupling strengths, most of the condensate would persist after the resonance.

Particle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)High Energy Physics::LatticeLattice field theoryFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)0103 physical sciences010306 general physicsSpecial unitary groupBosonCoupling constantPhysicsCondensed Matter::Quantum GasesGauge boson010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyAstronomy and AstrophysicsHigh Energy Physics - PhenomenologyHiggs bosonBack-reactionHigh Energy Physics::ExperimentAstrophysics - Cosmology and Nongalactic Astrophysics
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First Observation of Vector Boson Pairs in a Hadronic Final State at the Tevatron Collider

2009

We present the first observation in hadronic collisions of the electroweak production of vector boson pairs (VV, V=W, Z) where one boson decays to a dijet final state. The data correspond to 3.5 fb(-1) of integrated luminosity of pp collisions at s=1.96 TeV collected by the CDF II detector at the Fermilab Tevatron. We observe 1516 +/- 239(stat)+/- 144(syst) diboson candidate events and measure a cross section sigma(pp -> VV+X) of 18.0 +/- 2.8(stat)+/- 2.4(syst)+/- 1.1(lumi) pb, in agreement with the expectations of the standard model.

Particle physicsFinal stateFermilab TevatronTevatronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleddc:500.27. Clean energy01 natural sciences114 Physical sciencesStandard ModelVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Tellurium compounds0103 physical sciences010306 general physicsNuclear ExperimentVECTOR BOSONBosonsBosonPhysicsGauge bosonIntegrated luminosityCross section010308 nuclear & particles physicshep-exPhysicsHadronic collisionsElectroweak interactionHigh Energy Physics::PhenomenologyTevatronVector bosonThe standard modelCDFProduction (computer science)High Energy Physics::ExperimentCollider
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An analysis of the impact of LHC Run I proton–lead data on nuclear parton densities

2016

We report on an analysis of the impact of available experimental data on hard processes in proton-lead collisions during Run I at the Large Hadron Collider on nuclear modifications of parton distribution functions. Our analysis is restricted to the EPS09 and DSSZ global fits. The measurements that we consider comprise production of massive gauge bosons, jets, charged hadrons and pions. This is the first time a study of nuclear PDFs includes this number of different observables. The goal of the paper is twofold: i) checking the description of the data by nPDFs, as well as the relevance of these nuclear effects, in a quantitative manner; ii) testing the constraining power of these data in eve…

Particle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)ProtoneducationHadronNuclear TheoryFOS: Physical sciencesproton-lead collisionsParton114 Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentEngineering (miscellaneous)PhysicsGauge bosonLarge Hadron Collider010308 nuclear & particles physicsObservable3. Good healthHigh Energy Physics - PhenomenologyDistribution functionRegular Article - Theoretical PhysicsThe European Physical Journal. C, Particles and Fields
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Scaling properties of inclusive W $$^\pm $$ ± production at hadron colliders

2016

We consider the hadroproduction of W gauge bosons in their leptonic decay mode. Starting from the leading-order expressions, we show that by defining a suitable scaling variable the centre-of-mass dependence of the cross sections at the LHC energies can be essentially described by a simple power law. The scaling exponent is directly linked to the small-$x$ behaviour of parton distribution functions (PDF) which, at the high virtualities involved in W production, is largely dictated by QCD evolution equations. This entails a particularly simple scaling law for the lepton charge asymmetry and also predicts that measurements in different collision systems (p-p, p-$\bar{\rm p}$, p-Pb Pb-Pb) are …

Particle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)media_common.quotation_subjecteducationFOS: Physical sciencesParton114 Physical sciences7. Clean energy01 natural sciencesAsymmetryPower lawHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesscaling propertiesRapidityNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentScalingEngineering (miscellaneous)media_commonQuantum chromodynamicsPhysicsGauge bosonhadron colliders010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentLeptonThe European Physical Journal C
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Measurement of trilinear gauge couplings in e(+)e(-) collisions at 161 GeV and 172 GeV

1998

Trilinear gauge boson couplings are measured using data taken by DELPHI at 161 GeV and 172 GeV, Values for WWV couplings (V = Z,gamma) are determined from a study of the reactions e(+)e(-) --> W+W- and e(+)e(-) --> We nu, using differential distributions from the WW final state in which one W decays hadronically and the other leptonically, and total cross,section data from other channels, Limits are also derived on neutral ZV gamma couplings from an analysis of the reaction e(+)e(-) --> gamma + invisible particles. (C) 1998 Elsevier Science B.V.

Particle physicsNuclear and High Energy PhysicsElectron–positron annihilation7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesOPTIMAL OBSERVABLES[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentOPTIMAL OBSERVABLES; PHOTON COUPLINGS; ROOT-S=1.8 TEVDELPHIPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyROOT-S=1.8 TEVGauge (firearms)LARGE ELECTRON POSITRON COLLIDERPHOTON COUPLINGSLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentParticle Physics - Experiment
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Search for a muonic dark force at BaBar

2016

Many models of physics beyond the Standard Model predict the existence of new Abelian forces with new gauge bosons mediating interactions between "dark sectors" and the Standard Model. We report a search for a dark boson Z' coupling only to the second and third generations of leptons in the reaction e+e- -> mu+mu- Z', Z' -> mu+mu- using 514 fb-1 of data collected by the BABAR experiment. No significant signal is observed for Z' masses in the range 0.212 - 10 GeV. Limits on the coupling parameter g' as low as 7x10^-4 are derived, leading to improvements in the bounds compared to those previously derived from neutrino experiments.

Particle physicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelDark matterBaBar experimentFOS: Physical sciences01 natural sciencesPartícules (Matèria)Standard ModelHigh Energy Physics - ExperimentNONuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsBosonPhysicsGauge boson010308 nuclear & particles physicshep-exSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::Phenomenologyhep-phHEPHigh Energy Physics - PhenomenologyParticlesDark matter (Astronomy)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]BaBarMatèria fosca (Astronomia)NeutrinoLepton
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Search for high-mass resonances decaying to dilepton final states in pp collisions at √s = 7 TeV with the ATLAS detector

2012

The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z [superscript *] bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb[superscript −1] in the e [superscript +] e [superscript −] channel and 5.0 fb[superscript −1] in the μ [superscript +] μ [superscript −] channel. A Z [superscript ′] boson with Standard Model-like couplings…

Particle physicsNuclear and High Energy PhysicsPhysics::General PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Kaluza–Klein theoryTechnicolorddc:500.27. Clean energy01 natural sciences530Nuclear physics0103 physical sciencesddc:530EXTRA DIMENSIONSHigh Energy Physics010306 general physicsCiencias Exactashadron-hadron scatteringBosonPhysicsddc:539Gauge bosonLarge Hadron ColliderHadron-Hadron scattering; Nuclear and High Energy PhysicsScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyGravitonFísicaATLASExtra dimensionsRandall–Sundrum modelHADRON-HADRON COLLISIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearproton-proton collisionsHigh Energy Physics::ExperimentLHC
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Leptogenesis from oscillations and dark matter

2019

An extension of the Standard Model with Majorana singlet fermions in the 1–100 GeV range can explain the light neutrino masses and give rise to a baryon asymmetry at freeze-in of the heavy states, via their CP-violating oscillations. In this paper we consider extending this scenario to also explain dark matter. We find that a very weakly coupled B−L gauge boson, an invisible QCD axion model, and the singlet majoron model can simultaneously account for dark matter and the baryon asymmetry.

Particle physicsPhysics and Astronomy (miscellaneous)Dark matterFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural sciencesStandard ModelHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetrylcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsEngineering (miscellaneous)AxionMajoronPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyLeptogenesislcsh:QC770-798High Energy Physics::ExperimentNeutrinoThe European Physical Journal C
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