Search results for "massless"

showing 10 items of 191 documents

Light-induced anomalous Hall effect in massless Dirac fermion systems and topological insulators with dissipation

2019

Employing the quantum Liouville equation with phenomenological dissipation, we investigate the transport properties of massless and massive Dirac fermion systems that mimics graphene and topological insulators, respectively. The massless Dirac fermion system does not show an intrinsic Hall effect, but it shows a Hall current under the presence of circularly-polarized laser fields as a nature of a optically-driven nonequilibrium state. Based on the microscopic analysis, we find that the light-induced Hall effect mainly originates from the imbalance of photocarrier distribution in momentum space although the emergent Floquet–Berry curvature also has a non-zero contribution. We further compute…

PopulationFOS: Physical sciencesGeneral Physics and AstronomyPosition and momentum spaceanomalous Hall effect01 natural sciencesSettore FIS/03 - Fisica Della Materia010305 fluids & plasmaslaw.inventionsymbols.namesakeHall effectlawMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciences010306 general physicseducationQuantumPhysicseducation.field_of_studyCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsGrapheneFloquet statesopen quantum systemsMassless particleDirac fermionTopological insulatorsymbolsPhysics - OpticsOptics (physics.optics)
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Relativistic quantum thermometry through a moving sensor

2023

Using a two-level moving probe, we address the temperature estimation of a static thermal bath modeled by a massless scalar field prepared in a thermal state. Different couplings of the probe to the field are discussed under various scenarios. We find that the thermometry is completely unaffected by the Lamb shift of the energy levels. We take into account the roles of probe velocity, its initial preparation, and environmental control parameters for achieving optimal temperature estimation. We show that a practical technique can be utilized to implement such a quantum thermometry. Finally, exploiting the thermal sensor moving at high velocity to probe temperature within a multiparameter-est…

Quantum PhysicsQuantum thermometryFOS: Physical sciencesMassless scalar fieldGeneral Physics and AstronomyQuantum Fisher informationQuantum Physics (quant-ph)Moving sensorsSettore FIS/03 - Fisica Della MateriaAnnals of Physics
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Massless bound-state excitations and the Schwinger mechanism in QCD

2011

The gauge invariant generation of an effective gluon mass proceeds through the well-known Schwinger mechanism, whose key dynamical ingredient is the nonperturbative formation of longitudinally coupled massless bound-state excitations. These excitations introduce poles in the vertices of the theory, in such a way as to maintain the Slavnov-Taylor identities intact in the presence of massive gluon propagators. In the present work we first focus on the modifications induced to the nonperturbative three-gluon vertex by the inclusion of massless two-gluon bound-states into the kernels appearing in its skeleton-expansion. Certain general relations between the basic building blocks of these bound-…

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesFísicaYang–Mills existence and mass gapVertex (geometry)GluonMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsBound stateWave functionMathematical physics
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Impact of the pion mass on nonpower expansion for QCD observables

2005

A new set of functions, which form a basis of the massive nonpower expansion for physical observables, is presented in the framework of the analytic approach to QCD at the four-loop level. The effects due to the $\pi$ meson mass are taken into account by employing the dispersion relation for the Adler function. The nonvanishing pion mass substantially modifies the functional expansion at low energies. Specifically, the spacelike functions are affected by the mass of the $\pi$ meson in the infrared domain below few GeV, whereas the timelike functions acquire characteristic plateaulike behavior below the two-pion threshold. At the same time, all the appealing features of the massless nonpower…

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsBasis (linear algebra)MesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesObservableFunction (mathematics)Atomic and Molecular Physics and OpticsMassless particleHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Dispersion relationHigh Energy Physics::ExperimentNuclear Experiment
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First Look at Two-Loop Five-Gluon Scattering in QCD.

2018

We compute the leading colour contributions to five-gluon scattering at two loops in massless QCD. The integrands of all independent helicity amplitudes are evaluated using d-dimensional generalised unitarity cuts and finite field reconstruction techniques. Numerical evaluation of the integral basis is performed with sector decomposition methods to obtain the first benchmark results for all helicity configurations of a 2 to 3 scattering process in QCD.

Quantum chromodynamicsPhysicsHigh Energy Physics - TheoryParticle physicsBasis (linear algebra)Unitarity010308 nuclear & particles physicsScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesHelicityGluonMassless particleDecomposition methods Finite fields Gluon scattering Helicities Scattering process UnitarityHigh Energy Physics - Phenomenology; High Energy Physics - Phenomenology; High Energy Physics - TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciencesPerturbation theory (quantum mechanics)010306 general physicsPhysical review letters
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Infrared Singularities and Soft Gluon Resummation with Massive Partons

2010

Infrared divergences of QCD scattering amplitudes can be derived from an anomalous dimension matrix, which is also an essential ingredient for the resummation of large logarithms due to soft gluon emissions. We report a recent analytical calculation of the anomalous dimension matrix with both massless and massive partons at two-loop level, which describes the two-loop infrared singularities of any scattering amplitudes with an arbitrary number of massless and massive partons, and also enables soft gluon resummation at next-to-next-to-leading-logarithmic order. As an application, we calculate the infrared poles in the q qbar -> t tbar and gg -> t tbar scattering amplitudes at two-loop …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartonAtomic and Molecular Physics and OpticsGluonScattering amplitudeMassless particleMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Gravitational singularityHigh Energy Physics::ExperimentResummationAstrophysics::Galaxy Astrophysics
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Measurement of the isolated diphoton cross section inppcollisions ats=7  TeVwith the ATLAS detector

2012

The ATLAS experiment has measured the production cross section of events with two isolated photons in the final state, in proton-proton collisions at √s=7  TeV. The full data set acquired in 2010 is used, corresponding to an integrated luminosity of 37  pb-1. The background, consisting of hadronic jets and isolated electrons, is estimated with fully data-driven techniques and subtracted. The differential cross sections, as functions of the di-photon mass (mγγ), total transverse momentum (pT,γγ), and azimuthal separation (Δϕγγ), are presented and compared to the predictions of next-to-leading-order QCD.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)Photon010308 nuclear & particles physicsATLAS experiment01 natural sciences7. Clean energyNuclear physicsMassless particleCross section (physics)medicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineNuclear Experiment010306 general physicsLeptonPhysical Review D
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New High Order Relations between Physical Observables in Perturbative QCD

1997

We exploit the fact that within massless perturbative QCD the same Green's function determines the hadronic contribution to the $\tau$ decay width and the moments of the $e^+e^-$ cross section. This allows one to obtain relations between physical observables in the two processes up to an unprecedented high order of perturbative QCD. A precision measurement of the $\tau$ decay width allows one then to predict the first few moments of the spectral density in $e^+e^-$ annihilations integrated up to $s\sim m_\tau^2$ with high accuracy. The proposed tests are in reach of present experimental capabilities.

Quantum chromodynamicsPhysicsParticle physicsElectron–positron annihilationHadronFOS: Physical sciencesGeneral Physics and AstronomySpectral densityPerturbative QCDRenormalization groupHigh Energy Physics - ExperimentMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Particle decayHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPhysical Review Letters
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Two-loop divergences of scattering amplitudes with massive partons

2009

We complete the study of two-loop infrared singularities of scattering amplitudes with an arbitrary number of massive and massless partons in non-abelian gauge theories. To this end, we calculate the universal functions F_1 and f_2, which completely specify the structure of three-parton correlations in the soft anomalous-dimension matrix, at two-loop order in closed analytic form. Both functions are found to be suppressed like O(m^4/s^2) in the limit of small parton masses, in accordance with mass factorization theorems proposed in the literature. On the other hand, they are unsuppressed and diverge logarithmically near the threshold for pair production of two heavy particles. As an applica…

Quantum chromodynamicsPhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyPartonScattering amplitudeMassless particleMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair productionFactorizationQuantum field theory
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Inclusive D* Production in Photon-Photon Collisions at Next-to-Leading Order QCD

2001

The next-to-leading order cross section for the inclusive production of charm quarks in gamma-gamma collisions is calculated as a function of the transverse momentum pT and the rapidity y in approaches using massive or massless charm quarks. For the direct cross section we derive the massless limit from the massive theory with the result that this limit differs from the massless version with MSbar factorization by finite corrections. Subtracting or adding these corrections allows us to compare the two approaches on equal footing. We establish massless and massive versions with 3 and 4 initial flavours which are shown to approach the massless approximations very fast with increasing pT. With…

Quantum chromodynamicsPhysicsParticle physicsPhotonPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyFOS: Physical sciencesCharm quarkMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationTransverse momentumRapidityHigh Energy Physics::ExperimentEngineering (miscellaneous)
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