Search results for "weak interaction"

showing 10 items of 431 documents

Theoretical overview on tau physics

2006

8 páginas, 2 figuras, 1 tabla.-- PACS numbers: 14.60.Fg, 13.30.Ce, 12.20.Fv.-- Comunicación presentada a la International Workshop on Tau-Charm Physics (Charm2006), celebrada del 5 al 7 de Junio de 2006 en Beijing (China).-- arXiv:hep-ph/0609138v1

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionsHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsQCDAtomic and Molecular Physics and OpticsUniversality (dynamical systems)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentLeptonTau lepton
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New Strong Interactions: From QCD to LHC

2006

The concept of strong interactions need not be limited to the sector of physics taken by QCD. While this domain is investigated by RHIC, LHC will be able to probe potential new strong interactions simultaneously: Finding the precise mechanism for electroweak symmetry breaking is one of the prime problems of physics. Intricately linked to this point is the question after the true nature or even the existence of the Higgs boson. Here, we present stronly interacting theories providing an explanation for the hierarchy problem and leading to a light composite Higgs boson, favoured by experimental data. Our variation of the standard model is consistent with precision data. We achieve this accorda…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsHiggs fieldGauge bosonHigh Energy Physics::PhenomenologyElectroweak interactionHiggs bosonGeneral Physics and AstronomyTechnicolorHierarchy problemStandard ModelActa Physica Hungarica A) Heavy Ion Physics
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Next-to-leading order QCD corrections toW+W+andW−W−production in association with two jets

2014

We present a study of ${W}^{+}{W}^{+}jj$ and ${W}^{\ensuremath{-}}{W}^{\ensuremath{-}}jj$ production including leptonic decays in hadron-hadron collisions. The full electroweak and QCD induced contributions and their interferences are calculated at leading order. We find that, for inclusive cuts, the interference effects can be large if the jets are produced with large transverse momentum where, however, the production rate is suppressed. We also discuss the vector-boson-fusion cuts and show the validity of the vector-boson-fusion approximation. The next-to-leading order QCD corrections to the QCD-induced channels are also calculated. Compared to the previous calculation, we allow the inter…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyMonte Carlo methodElectroweak interactionOrder (ring theory)PartonNuclear physicsTransverse momentumHigh Energy Physics::ExperimentProduction (computer science)BosonPhysical Review D
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Alternative large-n limit for QCD and its implications for low-energy nuclear phenomena

1990

The Corrigan-Ramond model for large-{ital N} QCD is analyzed in detail. The spectrum, leading-order results for interactions, and an effective Lagrangian describing large-{ital N} interactions are derived. This Lagrangian, when quantized, provides an effective quantum field theory for mesons and baryons. The applicability of such a theory to low-energy nuclear phenomena is studied. The model has features that distinguish it clearly from standard large-{ital N} QCD.

PhysicsQuantum chromodynamicsParticle physicsMesonComputer Science::Information RetrievalHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaElementary particleFermionWeak interactionPerturbation theory (quantum mechanics)Quantum field theoryBoson
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QCD Condensates for the Light Quark V-A Correlator

2003

We use the procedure of pinched-weight Finite Energy Sum Rules (pFESR) to determine the OPE coefficients a_6, ...,a_16 of the flavor ud V-A correlator in terms of existing hadronic tau decay data. We show by appropriate weight choices that the error on the dominant d=6 contribution, which is known to be related to the K -> Pi Pi matrix elements of the electroweak penguin operator in the chiral limit, may be reduced to below the ~15% level. The values we obtain for the OPE coefficients with d>8 are shown to naturally account for the discrepancies between our results for the d=6 and d=8 terms and those of previous analyses, which were obtained neglecting d>8 contributions.

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsOperator (physics)Electroweak interactionHadronHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciences3. Good healthMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesOperator product expansion010306 general physicsEnergy (signal processing)
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Measurement of the t-channel single top quark production cross section

2009

The D0 collaboration reports direct evidence for electroweak production of single top quarks through the t-channel exchange of a virtual W boson. This is the first analysis to isolate an individual single top quark production channel. We select events containing an isolated electron or muon, missing transverse energy, and two, three or four jets from 2.3 fb^-1 of ppbar collisions at the Fermilab Tevatron Collider. One or two of the jets are identified as containing a b hadron. We combine three multivariate techniques optimized for the t-channel process to measure the t- and s-channel cross sections simultaneously. We measure cross sections of 3.14 +0.94 -0.80 pb for the t-channel and 1.05 +…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quark010308 nuclear & particles physicsHadronElectroweak interactionTevatronFOS: Physical sciences01 natural scienceslaw.inventionStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciencesExperimental High Energy Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysics Letters B
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Resummation prediction on top quark transverse momentum distribution at largepT

2012

We study the factorization and resummation of t-channel top quark transverse momentum distribution at large pT in the SM at both the Tevatron and the LHC with soft-collinear effective theory. The cross section in the threshold region can be factorized into a convolution of hard, jet and soft functions. In particular, we first calculate the NLO soft functions for this process, and give a RG improved cross section by evolving the different functions to a common scale. Our results show that the resummation effects increase the NLO results by about 9%-13% and 4%-9% when the top quark pT is larger than 50 and 70 GeV at the Tevatron and the 8 TeV LHC, respectively. Also, we discuss the scale inde…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsTop quarkHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyElectroweak interactionTevatronFOS: Physical sciencesRenormalization groupNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Soft-collinear effective theoryHigh Energy Physics::ExperimentSymmetry breakingResummationPhysical Review D
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The size of and physics beyond the Standard Model

2005

Abstract We analyse the allowed range of values of χ , both in the Standard Model and in models with new physics, pointing out that a relatively large value of χ , e.g., of order λ , is only possible in models where the unitarity of the 3 × 3 Cabibbo–Kobayashi–Maskawa matrix is violated through the introduction of extra Q = 2 / 3 quarks. We study the interesting case where the extra quark is an isosinglet, determining the allowed range for χ and the effect of a large χ on various low-energy observables, such as CP asymmetries in B meson decays. We also discuss the correlated effects which would be observable at high energy colliders, like decays t → c Z , modifications of the cross section …

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsUnitarityElectron–positron annihilationPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionStandard ModelNuclear physicsCP violationHigh Energy Physics::ExperimentB mesonNuclear Physics B
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Multivariate searches for single top quark production with the D0 detector

2007

We present a search for electroweak production of single top quarks in the s-channel (p-pbar -> t bbar + X) and t-channel (p-pbar -> tq bbar + X) modes. We have analyzed 230 pb^(-1) of data collected with the D0 detector at the Fermilab Tevatron collider at a center-of-mass energy of sqrt(s) = 1.96 TeV. Two separate analysis methods are used: neural networks and a cut-based analysis. No evidence for a single top quark signal is found. We set 95% confidence level upper limits on the production cross sections using Bayesian statistics, based on event counts and binned likelihoods formed from the neural network output. The limits from the neural network (cut-based) analysis are 6.4 pb (1…

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physics14.65.Ha 12.15.Ji 13.85.QkHigh Energy Physics::PhenomenologyElectroweak interactionTevatronFOS: Physical sciences01 natural sciencesParticle identificationHigh Energy Physics - Experiment3. Good healthNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Production (computer science)High Energy Physics::ExperimentFermilab010306 general physicsEnergy (signal processing)
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Search for single top quark production in pp¯ collisions at s=1.96 TeV

2005

We present a search for electroweak production of single top quarks in the s-channel and t-channel using neural networks for signal-background separation. We have analyzed 230 pb(-1) of data collected with the DO detector at the Fermilab Tevatron Collider at a center-of-mass energy of 1.96 TeV and find no evidence for a single top quark signal. The resulting 95% confidence level upper limits on the single top quark production cross sections are 6.4 pb in the s-channel and 5.0 ph in the t-channel. (c) 2005 Elsevier B.V. All rights reserved.

PhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionTevatronParticle accelerator01 natural scienceslaw.inventionNuclear physicsPair productionlaw0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsColliderPhysics Letters B
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