Search results for "Radiative Transfer"

showing 10 items of 551 documents

Spectroscopy, leptonic decays and the nature of heavy quarkonia

2008

We examine the electronic width ratios of Upsilon resonances below the BBbar threshold by means of an effective (Cornell-type) QCD potential incorporating 1/m_b corrections obtained from a prior fit to the bottomonium spectrum. From our analysis we conclude that the Upsilon(2S) and Upsilon(3S) states should belong to the strong-coupling (nonperturbative) regime while the Upsilon(1S) state should belong to the weak-coupling (perturbative) regime, in agreement with a previous study based on radiative decays.

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryRadiative decayFOS: Physical sciencesResonanceFísicaQuarkoniumNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Strong couplingRadiative transferHigh Energy Physics::ExperimentSpectroscopyPhysics Letters B
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QCD radiative corrections to the soft spectator contribution in the wide angle Compton scattering

2014

We derive the complete factorization formula for the leading power contribution in wide angle Compton scattering. It consists of the soft- and hard-spectator contributions. The hard-spectator contribution is well known and defined in the form of the convolution of a hard kernel with the nucleon distribution amplitudes. The soft-spectator contribution describes the scattering which involves the soft modes. We use the soft collinear effective theory in order to define this term in a field theoretical approach. Using the SCET framework we provide the proof of the factorization formula. We also compute the next-to-leading QCD corrections to the hard coefficient function of the soft spectator co…

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsScatteringNuclear TheoryCompton scatteringFOS: Physical sciencesSoft modesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Soft-collinear effective theoryFactorizationRadiative transferNucleonNuclear ExperimentNuclear Physics B
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QCD Radiative Correction to Zero Recoil Sum Rules for Heavy Flavor Transitions in the Small Velocity Limit.

1995

We consider the small velocity sum rules for heavy flavour semileptonic transitions that are used to estimate the zero recoil values of semileptonic heavy flavour form factors. We analyze the complete O($\alpha _S$) radiative correction to these sum rules. The corrections are universal and influence all "model-independent" bounds previously derived for semileptonic form factors at zero recoil.

Quantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)FlavourHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Zero (complex analysis)FOS: Physical sciencesNuclear physicsHigh Energy Physics - PhenomenologyRecoilHigh Energy Physics - Phenomenology (hep-ph)Radiative transferHigh Energy Physics::ExperimentOperator product expansionLimit (mathematics)Nuclear ExperimentFlavor
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B0−B¯0Mixing beyond Factorization in QCD Sum Rules

2003

We present a calculation of the B°-B° mixing matrix element in the framework of QCD sum rules for three-point functions. We compute α s corrections to a three-point function at the three-loop level in QCD perturbation theory, which allows one to extract the matrix element with next-to-leading order (NLO) accuracy. This calculation is imperative for a consistent evaluation of experimentally measured mixing parameters since the coefficient functions of the effective Hamiltonian for B 0 -B 0 mixing are known at NLO. We find that radiative corrections violate factorization at NLO; this violation is under full control and amounts to 10%. The resulting value of the B parameter is found to be B B …

Quantum chromodynamicsPhysicsParticle physicssymbols.namesakeQCD sum rulesFactorizationRadiative transfersymbolsGeneral Physics and AstronomyMatrix elementHamiltonian (quantum mechanics)Physical Review Letters
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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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Heavy-quark production in two-photon collisions

1993

Abstract Heavy quarks are copiously produced in two-photon collisions at e + e − colliders. We present the inclusive production rates and the final state distributions of the quarks, including QCD radiative corrections for the leading subprocesses. The results are compared with recent measurements of charmed particle production at PETRA and PEP, and predictions are given for TRISTAN and LEP energies.

Quantum chromodynamicsQuarkPhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyRadiative transferHigh Energy Physics::ExperimentPhysics Letters B
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On the Importance of Ligand-Centered Excited States in the Emission of Cyclometalated Ir(III) Complexes

2021

The photophysical behavior of the cyclometalating Ir(III) complexes [Ir(ppy)2(bpy)]+, where Hppy is 2-phenylpyridine and bpy is 2,2′-bipyridine (complex 1), and [Ir(diFppy)2(dtb-bpy)]+, where diFppy is 2-(2,4-difluorophenyl)pyridine and dtb-bpy is 4,4′-di-tert-butyl-2,2′-bipyridine (complex 2), has been theoretically investigated by performing density functional theory calculations. The two complexes share the same molecular skeleton, complex 2 being derived from complex 1 through the addition of fluoro and tert-butyl substituents, but present notable differences in their photophysical properties. The remarkable difference in their emission quantum yields (0.196 for complex 1 in dichloromet…

Quantum yieldPhotochemistryArticleInorganic Chemistrychemistry.chemical_compoundBipyridinechemistryExcited statePyridinePotential energy surfaceRadiative transferDensity functional theoryPhysical and Theoretical ChemistryPhosphorescenceInorganic Chemistry
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Radiative axion inflation

2019

Planck data robustly exclude the simple $\lambda\phi^4$ scenario for inflation. This is also the case for models of Axion Inflation in which the inflaton field is the radial part of the Peccei-Quinn complex scalar field. In this letter we show that for the KSVZ model it is possible to match the data taking into account radiative corrections to the tree level potential. After writing down the 1-loop Coleman-Weinberg potential, we show that a radiative plateau is easily generated thanks to the fact that the heavy quarks are charged under $SU(3)_c$ in order to solve the strong CP problem. We also give a numerical example for which the inflationary observables are computed and the heavy quarks …

QuarkNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)FOS: Physical sciences01 natural sciencessymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferPlanck010306 general physicsAxionInflation (cosmology)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyInflatonlcsh:QC1-999High Energy Physics - PhenomenologysymbolsStrong CP problemScalar fieldlcsh:PhysicsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysics Letters
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Form factors of radiative pion decays in nonlocal chiral quark models

2012

We study the radiative pion decay π +→e +ν eγ within nonlocal chiral quark models that include wave function renormalization. In this framework we analyze the momentum dependence of the vector form factor F V(q2) and the slope of the axial-vector form factor F A(q2) at threshold. Our results are compared with available experimental information and with the predictions given by the Nambu-Jona-Lasinio model. In addition we calculate the low energy constants δ 5 and δ 6, comparing our results with the values obtained in chiral perturbation theory.

QuarkNuclear and High Energy PhysicsWave function renormalizationParticle physicsChiral perturbation theoryradiative pion decayHigh Energy Physics::LatticeCiencias FísicasFOS: Physical sciences01 natural sciencesPion form factorPartícules (Física nuclear)Momentum//purl.org/becyt/ford/1 [https]pion form factorLow energyPionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transfer010306 general physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Física//purl.org/becyt/ford/1.3 [https]AstronomíaHigh Energy Physics - PhenomenologyRadiative pion decayFísica nuclearCIENCIAS NATURALES Y EXACTAS
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Joint lattice QCD–dispersion theory analysis confirms the quark-mixing top-row unitarity deficit

2020

Recently, the first ever lattice computation of the $\gamma W$-box radiative correction to the rate of the semileptonic pion decay allowed for a reduction of the theory uncertainty of that rate by a factor of $\sim3$. A recent dispersion evaluation of the $\gamma W$-box correction on the neutron also led to a significant reduction of the theory uncertainty, but shifted the value of $V_{ud}$ extracted from the neutron and superallowed nuclear $\beta$ decay, resulting in a deficit of the CKM unitarity in the top row. A direct lattice computation of the $\gamma W$-box correction for the neutron decay would provide an independent cross-check for this result but is very challenging. Before those…

QuarkParticle physicsNuclear TheoryComputationAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciences530High Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)PionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)0103 physical sciencesRadiative transferddc:530NeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsUnitarity010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentPhysical Review D
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