Search results for "W and Z bosons"

showing 10 items of 13 documents

Evidence for a Particle Produced in Association with Weak Bosons and Decaying to a Bottom-Antibottom Quark Pair in Higgs Boson Searches at the Tevatr…

2012

Aaltonen, T. et al.

FERMILAB TEVATRON COLLIDERTop quarkParticle physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Higgs-Boson decaysSTANDARD MODEL; PARTON DISTRIBUTIONS; SYMMETRIES; proton antiproton collisions; FERMILAB TEVATRON COLLIDER; Standard Model Higgs boson; HIGGS-BOSON production; Higgs-Boson decaysSTANDARD MODELGeneral Physics and AstronomyFOS: Physical sciencesElementary particleStandard Model Higgs boson7. Clean energy01 natural sciencesVector bosonStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsTEVATRONBosonStandard-model Higgs bosonsPhysicsHIGGS-BOSON productionHIGGS BOSON010308 nuclear & particles physics[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]High Energy Physics::PhenomenologyScalar bosonW and Z bosonsPARTON DISTRIBUTIONSExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonSYMMETRIESproton antiproton collisionsCDFLimits on production of particlesHigh Energy Physics::Experiment
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10.7 Weak quark mixing and the CKM matrix

2008

Nuclear physicsQuarkPhysicsTop quarkParticle physicsCabibbo–Kobayashi–Maskawa matrixW and Z bosonsCP violationBottom quarkMixing (physics)
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Measurement of Wγ and Zγ production in proton-proton collisions at √s =7 TeV with the ATLAS detector

2011

Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAM

Particle physics:Mathematics and natural science: 400::Physics: 430 [VDP]Nuclear and High Energy PhysicsProtonAtlas detectorFOS: Physical sciencesddc:500.2:Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Hadron-hadron scattering01 natural sciences7. Clean energy530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsPhysicsW BOSONHadron-Hadron Scattering010308 nuclear & particles physicsATLAS experimentHigh Energy Physics::PhenomenologyFísicaATLASHigh energy photonmedicine.anatomical_structureZ BOSONW and Z bosonsHADRON-HADRON COLLISIONSFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Observation of diffractively produced W and Z bosons in p̄p collisions at √s = 1800 GeV

2003

Using the DO detector, we have observed events produced in (p) over barp collisions that contain W or Z bosons in conjunction with very little energy deposition ("rapidity gaps") in large forward regions of the detector. The fraction of W boson events with a rapidity gap (a signature for diffraction) is 0.89 +/- (0.19)(0.17)% and the probability that the non-diffractive background fluctuated to yield the observed diffractive signal is 3 x 10(-14), corresponding to a significance of 7.5 sigma. The Z boson sample has a gap fraction of 1.44 +/- (0.61)(0.52)%, with a significance of 4.4 sigma. The diffractive events have very similar properties to the more common non-diffractive component. (C) …

PhysicsDiffractionNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsScatteringDetectorSigmaHERA01 natural sciencesNuclear physicsW and Z bosonsbiological sciences0103 physical sciencesbacteriaRapidity010306 general physicsBoson
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A measurement of the ratio of the W and Z cross sections with exactly one associated jet in pp collisions at with ATLAS

2012

The ratio of production cross sections of the W and Z bosons with exactly one associated jet is presented as a function of jet transverse momentum threshold. The measurement has been designed to ma ...

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaPerturbative QCDFunction (mathematics)01 natural sciencesStandard ModelNuclear physicsmedicine.anatomical_structureAtlas (anatomy)W and Z bosons0103 physical sciencesTransverse momentummedicineHigh Energy Physics::Experiment010306 general physics
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Electroweak Effective Charges and their relation to Physical Cross Sections

1997

In quantum electrodynamics with fermions f = e,\mu..., knowledge of the vacuum polarization spectral function determined from the tree level e^+e^- -> f^+f^- cross sections, together with a single low energy measurement of the fine structure constant \alpha, enables the construction of the one-loop effective charge \alpha_eff(q^2) for all q^2. It is shown how an identical procedure can be followed in the electroweak sector of the Standard Model to construct three gauge-, scale- and scheme-independent one-loop electroweak effective charges and an effective weak mixing angle from the tree level e^+e^- -> W^+W^-, ZH and e^+\nu_e -> W^+Z, W^+\gamma, W^+H differential cross sections, together wi…

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionFísicaFOS: Physical sciencesFine-structure constantFermionGauge (firearms)Effective nuclear chargeStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)W and Z bosonsVacuum polarization
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Measurement of theWZ→ℓνℓℓcross section and limits on anomalous triple gauge couplings inpp¯collisions ats=1.96TeV

2011

We present a new measurement of the WZ -> lvll (l = e, mu) cross section and limits on anomalous triple gauge couplings. Using 4.1 fb(-1) of integrated luminosity of p (p) over bar collisions at root s = 1.96 TeV, we observe 34 WZ candidate events with an estimated background of 6.0 +/- 0.4 events. We measure the WZ production cross section to be 3.89(-0.90)(+1.07) pb, in good agreement with the standard model prediction. We find no evidence for anomalous WWZ couplings and set 95% C.L. limits on the coupling parameters, -0.077 < lambda(z) < 0.093 and -0.029 < Delta kappa(z) < 0.080 in the HISZ parameterization for a Lambda = 2 TeV form factor scale. These are the best limits to date obtaine…

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsTevatronElementary particleLambda01 natural sciencesStandard ModelNuclear physicsW and Z bosons0103 physical sciencesGrand Unified TheoryHigh Energy Physics::Experiment010306 general physicsBosonPhysics Letters B
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Electroweak and finite width corrections to top quark decays into transverse and longitudinal $ W $-bosons

2002

We calculate the electroweak and finite width corrections to the decay of an unpolarized top quark into a bottom quark and a $ W $-gauge boson where the helicities of the $ W $ are specified as longitudinal, transverse-plus and transverse-minus. Together with the $ O(\alpha_s) $ corrections these corrections may become relevant for the determination of the mass of the top quark through angular decay measurements.

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorTop quark condensateHelicityBottom quarkNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)W and Z bosonsHigh Energy Physics::ExperimentBoson
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Helicity fractions of W bosons from top quark decays

2008

The helicity fractions of the W boson from top quark decays have been determined by the CDF and D0 collaborations at the Tevatron. It is to be expected that the present experimental errors will decrease with larger data samples and in particular with measurements at the LHC. These improvements have to be matched by advances on the theoretical side. In this presentation we present a progress report on the calculation of the next-to-next-to-leading order QCD corrections to the decay width of the top quark into polarised W bosons.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsTop quarkParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyTevatronTop quark condensateHelicityBottom quarkAtomic and Molecular Physics and OpticsNuclear physicsW and Z bosonsHigh Energy Physics::ExperimentBosonNuclear Physics B - Proceedings Supplements
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Search for pair production of heavy top-like quarks decaying to a high-pT W boson and a b quark in the lepton plus jets final state at s=7 TeV with t…

2013

A search is presented for production of a heavy up-type quark (t') together with its antiparticle, assuming a significant branching ratio for subsequent decay into a W boson and a b quark. The search is based on 4.7 fb(-1) of pp collisions root s = 7 TeV recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Data are analyzed in the lepton + jets final state, characterized by a high-transverse-momentum isolated electron or muon, large missing transverse momentum and at least three jets. The analysis strategy relies on the substantial boost of the W bosons in the t'(t') over bar signal when m(t') greater than or similar to 400 GeV. No significant excess of events above t…

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciences7. Clean energyBottom quarkStandard ModelNuclear physicsW and Z bosons0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsBosonPhysics Letters B
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