Search results for "VERTEX"

showing 10 items of 225 documents

Nonlinear dynamics in three-dimensional QED and nontrivial infrared structure

1999

In this work we consider a coupled system of Schwinger-Dyson equations for self-energy and vertex functions in QED_3. Using the concept of a semi-amputated vertex function, we manage to decouple the vertex equation and transform it in the infrared into a non-linear differential equation of Emden-Fowler type. Its solution suggests the following picture: in the absence of infrared cut-offs there is only a trivial infrared fixed-point structure in the theory. However, the presence of masses, for either fermions or photons, changes the situation drastically, leading to a mass-dependent non-trivial infrared fixed point. In this picture a dynamical mass for the fermions is found to be generated c…

PhysicsNuclear and High Energy PhysicsNonlinear systemInfraredQuantum mechanicsBibliographyStructure (category theory)FísicaVertex functionPropagatorFixed pointPhysical Review D
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A measurement of Rb using a lifetime-mass tag

1997

ALEPH's published measurement of R-b = Gamma(Z --> b (b) over bar)/Gamma(Z --> hadrons) using a lifetime tag is updated using the full LEP 1 data sample. Considerable effort has been devoted to understanding systematic effects. Charm background is better controlled by combining the lifetime tag with a tag based on the b/c hadron mass difference. Furthermore, the algorithm used to reconstruct the event primary vertex is designed so as to reduce correlations between the two hemispheres of an event. The value of R-b is measured to be 0.2167 +/- 0.0011(stat) +/- 0.0013(syst). (C) 1997 Published by Elsevier Science B.V. RI ANTONELLI, ANTONELLA/C-6238-2011; Passalacqua, Luca/F-5127-2011; Murtas, …

PhysicsNuclear and High Energy PhysicsParticle physicsAleph010308 nuclear & particles physicsElectron–positron annihilationPhysicsHadron01 natural sciencesVertex (geometry)Nuclear physicsALEPH Experiment0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsALEPH experimentParticle Physics - Experiment
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Pinch technique self-energies and vertices to all orders in perturbation theory

2003

The all-order construction of the pinch technique gluon self-energy and quark-gluon vertex is presented in detail within the class of linear covariant gauges. The main ingredients in our analysis are the identification of a special Green's function, which serves as a common kernel to all self-energy and vertex diagrams, and the judicious use of the Slavnov-Taylor identity it satisfies. In particular, it is shown that the ghost-Green's functions appearing in this identity capture precisely the result of the pinching action at arbitrary order. By virtue of this observation the construction of the quark-gluon vertex becomes particularly compact. It turns out that the aforementioned ghost-Green…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFunction (mathematics)Vertex (geometry)RenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Kernel (statistics)Covariant transformationUniquenessPerturbation theory (quantum mechanics)
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On dynamical gluon mass generation

2007

The effective gluon propagator constructed with the pinch technique is governed by a Schwinger-Dyson equation with special structure and gauge properties, that can be deduced from the correspondence with the background field method. Most importantly the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions, a property which allows for a meanigfull truncation. A linearized version of the truncated Schwinger-Dyson equation is derived, using a vertex that satisfies the required Ward identity and contains massless poles. The resulting integral equation, subject to a properly regularized constraint, is so…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeMass generationHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesPropagatorIntegral equationGluonVertex (geometry)Massless particleHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PinchMathematical physics
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Gauge-Independent Analysis of K_L --> e \mu in Left-Right Models

1997

The lepton-flavour-violating decay K_L --> e \mu is studied in detail within the context of SU(2)_R x SU(2)_L x U(1)_(B-L) models, which include heavy Majorana neutrinos. Particular attention is paid to the gauge independence of this decay process to one loop. In analogy with earlier studies on the K^0\bar{K}^0 mixing, it is explicitly shown how restoration of gauge invariance occurs in the decay amplitude containing the box diagrams, when the relevant Higgs-dependent self-energy and vertex graphs are taken into account in the on-shell skeleton renormalization scheme. Based on the analytic expressions so derived, we find that the branching ratio B(K_L --> e \mu) can be considerably enhanced…

PhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionHigh Energy Physics::PhenomenologyContext (language use)Parameter spaceLoop (topology)RenormalizationMAJORANAHigh Energy Physics - PhenomenologyVertex (curve)High Energy Physics::ExperimentGauge theory
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Hadron structure in the description of electromagnetic reactions

2002

The description of electromagnetic reactions at intermediate energies, such as pion electroproduction or (virtual) Compton scattering, traditionally starts from covariant tree-level Feynman diagrams (Born or pole terms). Internal hadron structure is included by means of (on-shell) form factors in the vertices while free propagators are used. To overcome problems with gauge invariance, simple prescriptions, such as, choosing ${F}_{1}^{V}{(q}^{2}{)=F}_{\ensuremath{\pi}}{(q}^{2})$ in pion electroproduction or the ``minimal substitution,'' are used. We discuss the inherent assumptions of such approaches and study the general structure of electromagnetic vertices and propagators for pions and nu…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryHadronCompton scatteringPropagatorVertex (geometry)symbols.namesakePionsymbolsFeynman diagramGauge theoryNuclear ExperimentMathematical physicsPhysical Review C
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Quantum loops in radiative decays of the a1 and b1 axial-vector mesons

2007

A previous model where the low-lying axial-vector mesons are dynamically generated, implementing unitarity in coupled channels in the vector-pseudoscalar (V P) meson interaction, is applied to evaluate the decay widths of the a1(1260) and b1(1235) axial-vector mesons into �. Unlike the case of the a1, the b1 radiative decay is systematically underestimated at tree level. In this work we evaluate for the first time the loop contribution coming from an initial V P vertex. Despite the large superficial divergence of the loops, the convergence of the relevant loops can be established by using arguments of gauge invariance. The partial decay widths obtained agree with the experimental values wit…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryUnitarityMesonQuantum electrodynamicsRadiative transferGauge theoryPseudovectorQuantumVertex (geometry)Physics Letters B
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CP violation and electric-dipole-moment at low energy tau-pair production

2004

CP violation at low energy is investigated at the tau electromagnetic vertex. High statistics at B factories, and on top of the Upsilon resonances, allows a detailed investigation of CP-odd observables related to the tau-pair production. The contribution of the tau electric dipole moment is considered in detail. We perform an analysis independent from the high energy data by means of correlation and linear spin observables at low energy. We show that different CP-odd asymmetries, associated to the normal-transverse and normal-longitudinal correlation terms can be measured at low energy accelerators, both at resonant and non resonant energies. These observables allow to put stringent and ind…

PhysicsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationTransition dipole momentFOS: Physical sciencesObservableVertex (geometry)High Energy Physics - PhenomenologyElectric dipole momentHigh Energy Physics - Phenomenology (hep-ph)Pair productionLow energyViolació CP (Física nuclear)Quantum electrodynamicsCP violationFísica nuclear
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Complete next-to-leading order gluino contributions to and

2011

Abstract We present the first complete order α s corrections to the Wilson coefficients (at the high scale) of the various versions of magnetic and chromomagnetic operators which are induced by a squark–gluino exchange. For this matching calculation, we work out the on-shell amplitudes b → s γ and b → s g , both in the full and in the effective theory up to order α s 2 . The most difficult part of the calculation is the evaluation of the two-loop diagrams in the full theory; these can be split into two classes: a) diagrams with one gluino and a virtual gluon; b) diagrams with two gluinos or with one gluino and a four-squark vertex. Accordingly, the Wilson coefficients can be split into a pa…

PhysicsNuclear and High Energy PhysicsParticle physicsGluino010308 nuclear & particles physicsBranching fractionHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyBlock (permutation group theory)01 natural sciencesVertex (geometry)GluonRenormalization0103 physical sciencesEffective field theoryOrder (group theory)High Energy Physics::Experiment010306 general physicsNuclear Physics B
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The effective neutrino charge radius in the presence of fermion masses

2005

Abstract We show how the crucial gauge cancellations leading to a physical definition of an effective neutrino charge radius persist in the presence of non-vanishing fermion masses. An explicit one-loop calculation demonstrates that, as happens in the massless case, the pinch technique rearrangement of the Feynman amplitudes, together with the judicious exploitation of the fundamental current relation J α ( 3 ) = 2 ( J Z + sin θ w 2 J γ ) α , leads to a completely gauge independent definition of the effective neutrino charge radius. Using the formalism of the Nielsen identities it is further proved that the same cancellation mechanism operates unaltered to all orders in perturbation theory.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyVertex functionFísicaFermionMassless particlesymbols.namesakeAmplitudeCharge radiusQuantum electrodynamicssymbolsPinchFeynman diagramNeutrino
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