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showing 10 items of 2571 documents

QCD effective charges from lattice data

2010

We use recent lattice data on the gluon and ghost propagators, as well as the Kugo-Ojima function, in order to extract the non-perturbative behavior of two particular definitions of the QCD effective charge, one based on the pinch technique construction, and one obtained from the standard ghost-gluon vertex. The construction relies crucially on the definition of two dimensionful quantities, which are invariant under the renormalization group, and are built out of very particular combinations of the aforementioned Green's functions. The main non-perturbative feature of both effective charges, encoded in the infrared finiteness of the gluon propagator and ghost dressing function used in their…

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesPropagatorFísicaInvariant (physics)Renormalization groupQCDEffective nuclear chargeVertex (geometry)GluonTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNonperturbative EffectsLattice (order)
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Determination of 55-155-155-1in second order QCD from hadronic Z decays

1992

Distributions of event shape variables obtained from 120600 hadronic Z decays measured with the DELPHI detector are compared to the predictions of QCD based event generators. Values of the strong coupling constant αs are derived as a function of the renormalization scale from a quantitative analysis of eight hadronic distributions. The final result, αs(MZ), is based on second order perturbation theory and uses two hadronization corrections, one computed with a parton shower model and the other with a QCD matrix element model. © 1992 Springer-Verlag.

Quantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsElectron–positron annihilationHadronHigh Energy Physics::Phenomenology01 natural sciencesHadronizationRenormalization0103 physical sciencesHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)010306 general physicsParton showerEngineering (miscellaneous)Event (particle physics)Zeitschrift für Physik C Particles and Fields
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Generalized on-shell renormalization of heavy quarks

1992

A generalized on-shell (GOS) renormalization scheme of QCD is developed to evaluate the renormalization of heavy quark wave functions and currents. All large logarithms arising from the physical range of quark masses and momentum transferq 2 can be absorbed into wave function and vertex renormalization. Our results are more general than those of the heavy quark effective theory and agree with the latter only at zero recoil. The proposed GOS scheme is very suitable for the μ/m Q expansion. As an application we discuss the renormalization of the flavour changing currentsb-c, t-b andt-c.

Quantum chromodynamicsPhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFlavourElementary particleRenormalizationRecoilHigh Energy Physics::ExperimentQuantum field theoryWave functionEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Improving the kinetic couplings in lattice nonrelativistic QCD

2019

We improve the non-relativistic QCD (NRQCD) action by comparing the dispersion relation to that of the continuum through $\mathcal{O}(p^6)$ in perturbation theory. The one-loop matching coefficients of the $\mathcal{O}(p^4)$ kinetic operators are determined, as well as the scale at which to evaluate $\alpha_s$ in the $V$-scheme for each quantity. We utilise automated lattice perturbation theory using twisted boundary conditions as an infrared regulator. The one-loop radiative corrections to the mass renormalisation, zero-point energy and overall energy-shift of an NRQCD $b$-quark are also found. We also explore how a Fat$3$-smeared NRQCD action and changes of the stability parameter $n$ aff…

Quantum chromodynamicsQuarkPhysics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical scienceshep-latKinetic energy01 natural sciencesComputer Science::Digital LibrariesGluonRenormalizationHigh Energy Physics - LatticeLattice (order)0103 physical sciencesHigh Energy Physics::ExperimentVacuum polarization010306 general physicsGluon fieldMathematical physicsPhysical Review
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Quantum counter-propagation in open optical cavities via the quasi-normal-mode approach

2006

By using the quasi-normal-mode (QNM) formalism in a second quantization scheme, the problem of the counter-propagation of electromagnetic fields inside optical cavities is studied. The links between QNM operators and canonical destruction and creation operators describing the external free field, as well as the field correlation functions, are found and discussed. An application of the theory is performed for open cavities whose refractive index satisfies symmetric properties.

Quantum opticsElectromagnetic fieldPhysicsPhysics::OpticsCondensed Matter PhysicsFree fieldWave equationSecond quantizationIndustrial and Manufacturing EngineeringAtomic and Molecular Physics and OpticsWAVE-EQUATIONQuantization (physics)OPEN SYSTEMSNormal modeCOMPLETENESSQuantum mechanicsInstrumentationQuantum2-COMPONENT EIGENFUNCTION EXPANSIONLaser Physics
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Stimulated emission control in Photonic Crystals: Strong coupling regime in QNM approach

2006

Stimulated emission, in strong coupling regime, in a one dimensional photonic crystals is described by considering two counter-propagating pumps. Quasi normal mode approach is used and coherent control of the Rabi splitting is discussed.

Quantum opticsPhysicsNormal modeCoherent controlPhysics::OpticsSpontaneous emissionStimulated emissionAtomic physicsRefractive indexAtomic clockPhotonic crystal2006 Conference on Lasers and Electro-Optics and 2006 Quantum Electronics and Laser Science Conference
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Incommensurate phases of a bosonic two-leg ladder under a flux

2016

A boson two--leg ladder in the presence of a synthetic magnetic flux is investigated by means of bosonization techniques and Density Matrix Renormalization Group (DMRG). We follow the quantum phase transition from the commensurate Meissner to the incommensurate vortex phase with increasing flux at different fillings. When the applied flux is $\rho \pi$ and close to it, where $\rho$ is the filling per rung, we find a second incommensuration in the vortex state that affects physical observables such as the momentum distribution, the rung-rung correlation function and the spin-spin and charge-charge static structure factors.

Quantum phase transitionBosonizationBosonisation[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]IncommensurationsFOS: Physical sciencesGeneral Physics and Astronomychamps de jauge artificiels01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)Condensed Matter - Strongly Correlated ElectronsCorrelation functionGauge fieldsCondensed Matter::Superconductivity0103 physical sciencesBosonizationtranstion commensurable-incommensurable010306 general physicsCommensurate-Incommensurate transitions[PHYS.COND.CM-MSQHE]Physics [physics]/Condensed Matter [cond-mat]/Mesoscopic Systems and Quantum Hall Effect [cond-mat.mes-hall]BosonPhysicsCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsartificial gauge fieldsDensity matrix renormalization groupGauge fields; Incommensurations; Meissner to vortex transition; Physics and Astronomy (all)Vortex stateMagnetic fluxVortexQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality.Quantum Gases (cond-mat.quant-gas)Meissner to vortex transitionCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesQuantum gases. Strongly coupled many-particle systems. Reduced dimensionality
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Nonequilibrium critical scaling in quantum thermodynamics

2016

The emerging field of quantum thermodynamics is contributing important results and insights into archetypal many-body problems, including quantum phase transitions. Still, the question whether out-of-equilibrium quantities, such as fluctuations of work, exhibit critical scaling after a sudden quench in a closed system has remained elusive. Here, we take a novel approach to the problem by studying a quench across an impurity quantum critical point. By performing density matrix renormalization group computations on the two-impurity Kondo model, we are able to establish that the irreversible work produced in a quench exhibits finite-size scaling at quantum criticality. This scaling faithfully …

Quantum phase transitionFOS: Physical sciencesNon-equilibrium thermodynamics02 engineering and technology01 natural sciencesCondensed Matter - Strongly Correlated Electronsquant-phCritical point (thermodynamics)Quantum critical pointQuantum mechanics0103 physical sciencesStatistical physicscond-mat.stat-mech010306 general physicsQuantum thermodynamicsCondensed Matter - Statistical MechanicsPhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Strongly Correlated Electrons (cond-mat.str-el)Density matrix renormalization group021001 nanoscience & nanotechnology2-IMPURITY KONDO PROBLEM; MATRIX RENORMALIZATION-GROUP; JARZYNSKI EQUALITY; CRITICAL-POINT; SYSTEMS; MODELcond-mat.str-elQuantum Physics (quant-ph)0210 nano-technologyKondo modelCritical exponentPhysical Review B
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Flavour Conservation in Two Higgs Doublet Models

2018

In extensions of the Standard Model with two Higgs doublets, flavour changing Yukawa couplings of the neutral scalars may be present at tree level. In this work we consider the most general scenario in which those flavour changing couplings are absent. We re-analyse the conditions that the Yukawa coupling matrices must obey for such \emph{general flavour conservation} (gFC), and study the one loop renormalisation group evolution of such conditions in both the quark and lepton sectors. We show that gFC in the leptonic sector is one loop stable under the Renormalization Group Evolution (RGE) and in the quark sector we present some new Cabibbo like solution also one loop RGE stable. At a pheno…

QuarkCouplingPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesRenormalization group01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLepton
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Renormalization and Scale Evolution of the Soft-Quark Soft Function

2020

Soft functions defined in terms of matrix elements of soft fields dressed by Wilson lines are central components of factorization theorems for cross sections and decay rates in collider and heavy-quark physics. While in many cases the relevant soft functions are defined in terms of gluon operators, at subleading order in power counting soft functions containing quark fields appear. We present a detailed discussion of the properties of the soft-quark soft function consisting of a quark propagator dressed by two finite-length Wilson lines connecting at one point. This function enters in the factorization theorem for the Higgs-boson decay amplitude of the $h\to\gamma\gamma$ process mediated by…

QuarkHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeFOS: Physical sciencesPosition and momentum spaceRenormalizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)FactorizationPerturbative QCDRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. RadioactivityResummationMathematical physicsPhysicsHigh Energy Physics::PhenomenologyPropagatorEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Weierstrass factorization theoremsymbolslcsh:QC770-798High Energy Physics::ExperimentResummation
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