Search results for "Observable"

showing 10 items of 634 documents

Hadron structure from lattice QCD

2014

Recent progress in lattice QCD calculations of nucleon structure will be presented. Calculations of nucleon matrix elements and form factors have long been difficult to reconcile with experiment, but with advances in both methodology and computing resources, this situation is improving. Some calculations have produced agreement with experiment for key observables such as the axial charge and electromagnetic form factors, and the improved understanding of systematic errors will help to increase confidence in predictions of unmeasured quantities. The long-omitted disconnected contributions are now seeing considerable attention and some recent calculations of them will be discussed.

Quantum chromodynamicsPhysicsParticle physicsNuclear TheoryHigh Energy Physics - Lattice (hep-lat)HadronStructure (category theory)FOS: Physical sciencesCharge (physics)ObservableLattice QCDNuclear Theory (nucl-th)High Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNucleonAIP Conference Proceedings
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Natural constraints on the gluon-quark vertex

2016

In principle, the strong-interaction sector of the Standard Model is characterised by a unique renormalisation-group-invariant (RGI) running interaction and a unique form for the dressed--gluon-quark vertex, $\Gamma_\mu$; but, whilst much has been learnt about the former, the latter is still obscure. In order to improve this situation, we use a RGI running-interaction that reconciles both top-down and bottom-up analyses of the gauge sector in quantum chromodynamics (QCD) to compute dressed-quark gap equation solutions with 1,660,000 distinct Ansaetze for $\Gamma_\mu$. Each one of the solutions is then tested for compatibility with three physical criteria and, remarkably, we find that merely…

Quantum chromodynamicsPhysicsQuarkParticle physicsNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyHadronStrong interactionFOS: Physical sciencesObservable01 natural sciencesGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear theoryPhysical Review D
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Multiparton NLO corrections by numerical methods

2013

In this talk we discuss an algorithm for the numerical calculation of one-loop QCD amplitudes and present results at next-to-leading order for jet observables in electron-positron annihilation calculated with the above-mentioned method. The algorithm consists of subtraction terms, approximating the soft, collinear and ultraviolet divergences of QCD one-loop amplitudes, as well as a method to deform the integration contour for the loop integration into the complex plane to match Feynman's i delta rule. The algorithm is formulated at the amplitude level and does not rely on Feynman graphs. Therefore all ingredients of the algorithm can be calculated efficiently using recurrence relations. The…

Quantum chromodynamicsPhysicsRecurrence relationNumerical analysisFOS: Physical sciencesObservableJet (particle physics)symbols.namesakeHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)symbolsFeynman diagramStatistical physicsComplex plane
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The top quark right coupling in the tbW-vertex

2015

The most general parametrization of the $tbW$ vertex includes a right coupling $V_R$ that is zero at tree level in the standard model. This quantity may be measured at the Large Hadron Collider where the physics of the top decay is currently investigated. This coupling is present in new physics models at tree level and/or through radiative corrections, so its measurement can be sensitive to non standard physics. In this paper we compute the leading electroweak and QCD contributions to the top $V_R$ coupling in the standard model. This value is the starting point in order to separate the standard model effects and, then, search for new physics. We also propose observables that can be address…

Quantum chromodynamicsPhysicsTop quarkParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelElectroweak interactionFísicaFOS: Physical sciencesObservableVertex (geometry)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferEngineering (miscellaneous)
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2019

Abstract Heavy quarkonium related observables are very useful to obtain information about the medium created in relativistic heavy ion collisions. In recent years the theoretical description of quarkonium in a medium has moved towards a more dynamical picture in which decay and recombination processes are very important. In this talk we will discuss the equations that describe the evolution of the heavy quark reduced density matrix in different approximations, highlighting the color dynamics that is absent in the Abelian case, and we will study their semi-classical limit. This will allow us to obtain stochastic equations (similar to Langevin or Boltzmann equations) that can be useful to obt…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyObservableQuarkonium7. Clean energy01 natural sciencesBoltzmann equationsymbols.namesake0103 physical sciencesBoltzmann constantQuark–gluon plasmasymbols010306 general physicsQuantumNuclear Physics A
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Three-jet production at LEP and the bottom quark mass

1994

We consider the possibility of extracting the bottom quark mass from LEP data. The inclusive decay rate for $\zbb +\cdots$ is obtained at order $\as$ by summing up the one-loop two-parton decay rate to the tree-level three-parton rate. We calculate the decay width of the $Z$-boson into two and three jets containing the $b$-quark including complete quark mass effects. In particular, we give analytic results for a slight modification of the JADE clustering algorithm. We also study the angular distribution with respect to the angle formed between the gluon and the quark jets, which has a strong dependence on the quark mass. The impact of higher order QCD corrections on these observables is bri…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaOrder (ring theory)FOS: Physical sciencesObservableJet (particle physics)Bottom quarkJADE (particle detector)GluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentParticle Physics - Phenomenology
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Quark-mass effects for jet production in e+e- collisions at the next-to-leading order: results and applications

1999

We present a detailed description of our calculation of next-to-leading order QCD corrections to heavy quark production in e^+ e^- collisions including mass effects. In particular, we study the observables $R_3^{b\ql}$ and $D_2^{b\ql}$ in the E, EM, JADE and DURHAM jet-clustering algorithms and show how one can use these observables to obtain $m_b(m_Z)$ from data at the $Z$ peak.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesFísicaObservableJet (particle physics)JADE (particle detector)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::Experiment
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Measurements of tt¯ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in pp collisions at s=13  TeV usin…

2018

Measurements are made of differential cross-sections of highly boosted pair-produced top quarks as a function of top-quark and t (t) over bar system kinematic observables using proton-proton collis ...

Quantum chromodynamicsQuarkPhysicsTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHadronStrong interactionPerturbative QCDObservable01 natural sciencesmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesPhysics::Atomic and Molecular ClustersmedicineHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Fermi Liquid with Fermion Condensate

2014

Here we discuss the general properties of FCQPT leading to the emergence of FC. We present a microscopic derivation of the main equations of FC, and show that Fermi systems with FC form an entirely new class of Fermi liquids with its own topological structure, protecting the FC state. We construct the phase diagram, and explore the order parameter of these systems. We show that the fermion condensate has a strong impact on the observable physical properties of systems, where it is realized, up to relatively high temperatures of a few tens kelvin. Two different scenarios of the quantum critical point (QCP), a zero-temperature instability of the Landau state, related to the divergence of the …

Quantum phase transitionPhysicsPhase transitionEffective mass (solid-state physics)Condensed matter physicsQuantum critical pointFermi surfaceObservableFermi liquid theoryFermi gas
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Measurement of trilinear gauge boson couplings WWV, (V Z,gamma) in e(+)e(-) collisions at 189 GeV

2001

Measurements of the trilinear gauge boson couplings WWgamma and WWZ are presented using the data taken by DELPHI in 1998 at a centre-of-mass energy of 189 GeV and combined with DELPHI data at 183 GeV. Values are determined for Delta(g_1^Z) and Delta(kappa_gamma), the differences of the WWZ charge coupling and of the WWgamma dipole coupling from their Standard Model values, and for lambda_gamma, the WWgamma quadrupole coupling. A measurement of the magnetic dipole and electric quadrupole moment of the W is extracted from the results for Delta(kappa_gamma) and lambda_gamma. The study uses data from the final states jjlv, jjjj, lX, jjX and gammaX, where j represents a quark jet, l an identifie…

QuarkNuclear and High Energy PhysicsParticle physicsENERGIESAstrophysics::High Energy Astrophysical Phenomenastandard modelLEP-IIFOS: Physical sciencesLambda7. Clean energy01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentStandard ModelEVENTSHigh Energy Physics - Experiment (hep-ex)BHABHA SCATTERINGMONTE-CARLO0103 physical sciencesOPTIMAL OBSERVABLES[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]W-MASSgauge couplings010306 general physicsDETECTORQCDELPHIPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCharge (physics)LARGE ELECTRON POSITRON COLLIDERFIS/01 - FISICA SPERIMENTALECol·lisions (Física nuclear)QuadrupolePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIOPTIMAL OBSERVABLES; BHABHA SCATTERING; MONTE-CARLO; W-MASS; LEP-II; EVENTS; DETECTOR; DELPHI; E+E-->W+W; ENERGIESelectron-positron collisionPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentE+E-->W+WMagnetic dipoleLepton
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