Search results for "Chromodynamics"

showing 10 items of 1030 documents

Microscopic s-wave optical potential for slow pions scattered by a nucleus.

1989

We have done a microscopic calculation of the {ital s}-wave optical potential for the pion-nucleus system at low energies, 0{le}{ital T}{sub {pi}}{le}100 MeV, using a description based on hadronic degrees of freedom. We have obtained, separately, the real and imaginary parts of the optical potential coming from one-body and two-body processes. We have also separated the imaginary part of the potential associated to absorption and to quasielastic channels. We find that the imaginary part of the absorption channel is independent of the energy (within the range of energies considered here) in agreement with a recent empirical determination. We compare our results with phenomenological potentia…

PhysicsQuantum chromodynamicsNuclear reactionNuclear and High Energy PhysicsComputer Science::Information RetrievalIsoscalarNuclear TheoryHadronNuclear physicsPionAmplitudeAbsorption (logic)Atomic physicsEnergy (signal processing)Physical review. C, Nuclear physics
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From stringy particle physics to moduli stabilisation and cosmology

2016

Intersecting D6-branes provide a geometrically intuitive road to stringy particle physics models, where D6-branes stuck at orbifold singularities can lead to the stabilisation of deformation moduli, and the QCD axion can arise from the open string sector in a very constrained way compared to pure field theory. We demonstrate this interplay of different physical features here through an explicit model.

PhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsGeneral Physics and AstronomyInflaton01 natural sciencesModuliHigh Energy Physics::Theory0103 physical sciencesField theory (psychology)Gravitational singularityD-brane010306 general physicsMathematics::Symplectic GeometryAxionOrbifoldFortschritte der Physik
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Identifying spin and parity of charmonia in flight with lattice QCD

2019

The spectrum of charmonium resonances contains a number of unanticipated states along with several conventional quark-model excitations. The hadrons of different quantum numbers $J^P$ appear in a fairly narrow energy band, where $J^P$ refers to the spin-parity of a hadron at rest. This poses a challenge for Lattice QCD studies of (coupled-channel) meson-meson scattering aimed at the determination of scattering amplitudes and resonance pole positions. A wealth of information for this purpose can be obtained from the lattice spectra in frames with nonzero total momentum. These are particularly dense since hadrons with different $J^P$ contribute to any given lattice irreducible representation.…

PhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)ddc:530High Energy Physics::PhenomenologyQuark modelLattice field theoryFOS: Physical sciencesLattice QCD530 PhysikQuantum number01 natural sciencesGood quantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Irreducible representationHadron spectroscopy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Elastic I=3/2 p -wave nucleon-pion scattering amplitude and the Δ(1232) resonance from Nf=2+1 lattice QCD

2018

We present the first direct determination of meson-baryon resonance parameters from a scattering amplitude calculated using lattice QCD. In particular, we calculate the elastic $I=3/2$, $p$-wave nucleon-pion amplitude on a single ensemble of ${N}_{\mathrm{f}}=2+1$ Wilson-clover fermions with ${m}_{\ensuremath{\pi}}=280\text{ }\text{ }\mathrm{MeV}$ and ${m}_{K}=460\text{ }\text{ }\mathrm{MeV}$. At these quark masses, the $\mathrm{\ensuremath{\Delta}}(1232)$ resonance pole is found close to the $N\ensuremath{-}\ensuremath{\pi}$ threshold and a Breit-Wigner fit to the amplitude gives ${g}_{\mathrm{\ensuremath{\Delta}}N\ensuremath{\pi}}^{\mathrm{BW}}=19.0(4.7)$ in agreement with phenomenologica…

PhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryLattice field theoryResonanceFermionLattice QCD01 natural sciencesScattering amplitudePion0103 physical sciences010306 general physicsNucleonPhysical Review D
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A QCD analysis for nuclear PDFs at NNLO

2019

A new QCD analysis for nuclear parton distribution functions (nPDFs) at next-to-leading order (NLO) and next-to-next-to-leading order (NNLO) is presented. The framework of the analysis, including the form of the parameterization as well as the included DIS data sets, are discussed. The results of this QCD analysis are compared to the existing nPDF sets and to the fitted data. The presented framework is based on an open-source tool, xFitter, which has been modified to be applicable also for a nuclear PDF analysis. The required modifications are covered as well. Finally, an outlook for the next developments of the QCD analysis for nuclear PDFs is given.

PhysicsQuantum chromodynamicsParticle physics05 social sciencesHigh Energy Physics::PhenomenologyeducationFOS: Physical sciences020207 software engineeringParton02 engineering and technologyhiukkasfysiikka114 Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution function0202 electrical engineering electronic engineering information engineering0501 psychology and cognitive sciencesHigh Energy Physics::Experimentydinfysiikka050107 human factors
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Measurement of Inclusive Jet Cross Sections inZ/γ*(→e+e−)+jetsProduction inpp¯Collisions ats=1.96   TeV

2008

Inclusive jet cross sections in Z/{gamma}* events, with Z/{gamma}* decaying into an electron-positron pair, are measured as a function of jet transverse momentum and jet multiplicity in p{bar p} collisions at {radical}s - 1.96 TeV with the upgraded Collider Detector at Fermilab in Run II, based on an integrated luminosity of 1.7 fb{sup -1}. The measurements cover the rapidity region |y{sup jet}| 30 GeV/c. Next-to-leading order perturbative QCD predictions are in good agreement with the measured cross sections.

PhysicsQuantum chromodynamicsParticle physicsAnnihilation010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyPerturbative QCDElectron01 natural sciences7. Clean energyNuclear physicsPair production0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentRapidityMultiplicity (chemistry)010306 general physicsCollider Detector at FermilabPhysical Review Letters
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Measurement of Proton Electromagnetic Form Factors in e+e−→pp¯ in the Energy Region 2.00–3.08 GeV

2020

The process of e+e−→pp¯ is studied at 22 center-of-mass energy points (s) from 2.00 to 3.08 GeV, exploiting 688.5 pb−1 of data collected with the BESIII detector operating at the BEPCII collider. The Born cross section (σpp¯) of e+e−→pp¯ is measured with the energy-scan technique and it is found to be consistent with previously published data, but with much improved accuracy. In addition, the electromagnetic form-factor ratio (|GE/GM|) and the value of the effective (|Geff|), electric (|GE|), and magnetic (|GM|) form factors are measured by studying the helicity angle of the proton at 16 center-of-mass energy points. |GE/GM| and |GM| are determined with high accuracy, providing uncertaintie…

PhysicsQuantum chromodynamicsParticle physicsAnnihilationProtonElectron–positron annihilationGeneral Physics and Astronomy01 natural sciencesHelicitylaw.inventionlaw0103 physical sciencesBorn approximation010306 general physicsColliderEnergy (signal processing)Physical Review Letters
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Lattice QCD calculation of hadronic light-by-light scattering

2015

We perform a lattice QCD calculation of the hadronic light-by-light scattering amplitude in a broad kinematical range. At forward kinematics, the results are compared to a phenomenological analysis based on dispersive sum rules for light-by-light scattering. The size of the pion pole contribution is investigated for momenta of typical hadronic size. The presented numerical methods can be used to compute the hadronic light-by-light contribution to the anomalous magnetic moment of the muon. Our calculations are carried out in two-flavor QCD with the pion mass in the range of 270 to 450MeV, and contain so far only the diagrams with fully connected quark lines.

PhysicsQuantum chromodynamicsParticle physicsAnomalous magnetic dipole momentScatteringHigh Energy Physics::LatticeLattice field theoryNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)General Physics and AstronomyFOS: Physical sciencesLattice QCDLight scatteringScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticePionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNuclear Experiment
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Including Tetraquark Operators in the Low-Lying Scalar Meson Sectors in Lattice QCD

2019

Lattice QCD allows us to probe the low-lying hadron spectrum in finite-volume using a basis of single- and multi-hadron interpolating operators. Here we examine the effect of including tetraquark operators on the spectrum in the scalar meson sectors containing the $K_0^*(700)$ ($\kappa$) and the $a_0(980)$ in $N_f = 2 + 1$ QCD, with $m_\pi \approx 230$ MeV. Preliminary results of additional finite-volume states found using tetraquark operators are shown, and possible implications of these states are discussed.

PhysicsQuantum chromodynamicsParticle physicsBasis (linear algebra)High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Spectrum (functional analysis)HadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDApproxHigh Energy Physics - LatticeTetraquarkHigh Energy Physics::ExperimentScalar meson
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anQCD: Fortran programs for couplings at complex momenta in various analytic QCD models

2015

We provide three Fortran programs which evaluate the QCD analytic (holomorphic) couplings $\mathcal{A}_{\nu}(Q^2)$ for complex or real squared momenta $Q^2$. These couplings are holomorphic analogs of the powers $a(Q^2)^{\nu}$ of the underlying perturbative QCD (pQCD) coupling $a(Q^2) \equiv \alpha_s(Q^2)/\pi$, in three analytic QCD models (anQCD): Fractional Analytic Perturbation Theory (FAPT), Two-delta analytic QCD (2$\delta$anQCD), and Massive Perturbation Theory (MPT). The index $\nu$ can be noninteger. The provided programs do basically the same job as the Mathematica package anQCD.m in Mathematica published by us previously, Ref.[1], but are now written in Fortran.

PhysicsQuantum chromodynamicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsHolomorphic functionGeneral Physics and AstronomyPerturbative QCDFOS: Physical sciences01 natural sciencesRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and Architecture0103 physical sciencesHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Invariant (mathematics)010306 general physicsComplex planeMathematical physics
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