Search results for "Names"

showing 10 items of 6843 documents

A non-relativistic model for the $[cc][\bar{c}\bar{c}]$ tetraquark

2017

We use a non-relativistic model to study the spectroscopy of a tetraquark composed of $[cc][\bar{c}\bar{c}]$ in a diquark-antidiquark configuration. By numerically solving the Schr\"{o}dinger equation with a Cornell-inspired potential, we separate the four-body problem into three two-body problems. Spin-dependent terms (spin-spin, spin-orbit and tensor) are used to describe the splitting structure of the $c\bar{c}$ spectrum and are also extended to the interaction between diquarks. Recent experimental data on charmonium states are used to fix the parameters of the model and a satisfactory description of the spectrum is obtained. We find that the spin-dependent interaction is sizable in the …

QuarkNuclear and High Energy PhysicsParticle physicsinterpretation of experiments: CERN LHC CollcharmoniumsplittingHigh Energy Physics::LatticeFOS: Physical sciencesBELLE01 natural sciencesSchrödinger equationquarksymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)excited state0103 physical sciencesstructureTensor010306 general physicsInstrumentationSpin-½Physics010308 nuclear & particles physicsHigh Energy Physics::Phenomenologymodel: nonrelativisticAstronomy and AstrophysicstetraquarkThree-body problemDiquarkHigh Energy Physics - Phenomenologythree-body problemdiquark[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Excited statesymbolsSchroedinger equationHigh Energy Physics::ExperimentTetraquarkcharmChinese Physics C
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Higgs in space!

2010

We consider the possibility that the Higgs can be produced in dark matter annihilations, appearing as a line in the spectrum of gamma rays at an energy determined by the masses of the WIMP and the Higgs itself. We argue that this phenomenon occurs generally in models in which the the dark sector has large couplings to the most massive states of the SM and provide a simple example inspired by the Randall-Sundrum vision of dark matter, whose 4d dual corresponds to electroweak symmetry-breaking by strong dynamics which respect global symmetries that guarantee a stable WIMP. The dark matter is a Dirac fermion that couples to a Z' acting as a portal to the Standard Model through its strong coupl…

QuarkParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Astrophysics::High Energy Astrophysical PhenomenaDark matter theoryDark matterGamma ray experimentsFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)WIMP0103 physical sciences010306 general physicsParticle Physics - PhenomenologyPhysicsAnnihilation010308 nuclear & particles physicsElectroweak interactionAstronomy and AstrophysicsCosmology of Theories beyond the SMHigh Energy Physics - PhenomenologyDark matter experimentsDirac fermionsymbolsHiggs bosonAstrophysics - Cosmology and Nongalactic AstrophysicsFermi Gamma-ray Space TelescopeJournal of Cosmology and Astroparticle Physics
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Parton distribution functions of heavy mesons on the light front

2019

The parton distribution functions (PDFs) of heavy mesons are evaluated from their light-front wave functions, which are obtained from a basis light-front quantization in the leading Fock sector representation. We consider the mass eigenstates from an effective Hamiltonian consisting of the confining potential adopted from light-front holography in the transverse direction, a longitudinal confinement, and a one-gluon exchange interaction with running coupling. We present the gluon and the sea quark PDFs which we generate dynamically from the QCD evolution of the valence quark distributions.

QuarkParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciencesFock spaceNuclear Theory (nucl-th)Quantization (physics)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessironta010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicskvarkitHigh Energy Physics::PhenomenologyGluonHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentkvanttikenttäteoriaHamiltonian (quantum mechanics)ydinfysiikka
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Ultrarelativistic quark-nucleus scattering in a light-front Hamiltonian approach

2020

We investigate the scattering of a quark on a heavy nucleus at high energies using the time-dependent basis light-front quantization (tBLFQ) formalism, which is the first application of the tBLFQ formalism in QCD. We present the real-time evolution of the quark wave function in a strong classical color field of the relativistic nucleus, described as the color glass condensate. The quark and the nucleus color field are simulated in the QCD SU(3) color space. We calculate the total and the differential cross sections, and the quark distribution in coordinate and color spaces using the tBLFQ approach. We recover the eikonal cross sections in the eikonal limit. We find that the differential cro…

QuarkParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceshiukkasfysiikka01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)Quantization (physics)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessironta010306 general physicsWave functionPhysicsQuantum chromodynamics010308 nuclear & particles physicsEikonal equationkvarkitHigh Energy Physics::PhenomenologyDeep inelastic scatteringHigh Energy Physics - PhenomenologysymbolskvanttikenttäteoriaHamiltonian (quantum mechanics)ydinfysiikkaPhysical Review D
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Spectrum of fully-heavy tetraquarks from a diquark+antidiquark perspective

2019

Using a relativized diquark model Hamiltonian, we calculate the masses of $J^{PC}=0^{++}$ ground-state tetraquarks in the following systems: $b s \bar b \bar s$, $bb \bar n \bar n$ ($n=u, d$), $bb \bar s \bar s$, $cc\bar c \bar c$, $b b \bar b \bar b$, $b c\bar b \bar c$ and $b b \bar c \bar c$. We also compute extensive spectra for the fully-heavy quark flavour combinations. Finally, as a test of the diquark model approach, we compute the masses of fully-heavy baryons in the diquark model. Our results may be compared soon to the forthcoming experimental data for fully-heavy three-quark systems.

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHigh Energy Physics::LatticeNuclear TheoryFOS: Physical scienceslcsh:AstrophysicshiukkasfysiikkaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)lcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)Engineering (miscellaneous)Nuclear theoryNuclear ExperimentPhysicstheoretical physicskvarkitHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)DiquarkBaryonHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentHamiltonian (quantum mechanics)European Physical Journal
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Few-body quark dynamics for doubly heavy baryons and tetraquarks

2018

We discuss the adequate treatment of the 3- and 4-body dynamics for the quark model picture of double-charm baryons and tetraquarks. We stress that the variational and Born-Oppenheimer approximations give energies very close to the exact ones, while the diquark approximation might be rather misleading. The Hall-Post inequalities also provide very useful lower bounds that exclude the possibility of stable tetraquarks for some mass ratios and some color wave functions.

QuarkParticle physicswave functionNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Born–Oppenheimer approximationFOS: Physical sciencestetraquark: energy01 natural sciencesNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsWave functionBorn-Oppenheimer approximation[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]Physicsquark model010308 nuclear & particles physicsQuark modelDynamics (mechanics)High Energy Physics::Phenomenologybaryon: energyMass ratiotetraquark: stabilityBaryonDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]symbolsapproximation: diquark[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]mass ratio
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Extended HQEFT Lagrangian and currents

2000

From the tree-level heavy quark effective Lagrangian keeping particle-antiparticle mixed sectors we derive the vector current coupling to a hard gluonic field allowing for heavy quark-antiquark pair annihilation and creation.

QuarkPhysicsCouplingNuclear and High Energy PhysicsParticle physicsCurrent (mathematics)AnnihilationField (physics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Effective lagrangiansymbolsHigh Energy Physics::ExperimentLagrangian
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Search for strange matter by Rutherford backscattering

1989

According to a number of suggestions, stable strange matter could exist in the form of supermassive nuclei (or 'strange nuggets')1,2. In contrast to ordinary nuclei, which contain only 'up' and 'down' quarks, a piece of strange matter should comprise a mixture of 'up', 'down' and 'strange' quarks in roughly equal proportions. Small amounts of strange matter could have survived from the early stages of the Universe1. Alternatively, strange matter might reach the Earth as a flux of strange nuggets produced in collisions of neutron stars3. Limits to the cosmic flux of strange nuggets with masses in the range from 10−4 to 250 g have been obtained in a search for light produced by the nuggets in…

QuarkPhysicsMultidisciplinaryNuclear TheoryFluxElementary particleNuclear matterNuclear physicssymbols.namesakeStrange mattersymbolsNeutronRutherford scatteringNuclear ExperimentNucleonNature
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On the Pauli-Villars regularisation scheme in the NJL model

1993

Abstract We consider the Nambu-Jona-Lasinio model with a Pauli-Villars cutoff. We point out that previous attempts to use this regularisation have not been consistent and it is shown that if used correctly this approach yields very reasonable values for the cutoff parameter and quark condensate when we demand that ƒπ is fixed to its experimental value. Finally it is argued that because of its covariance and smooth nature this regularisation scheme has significant advantages over other regulators on the market.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryStrong interactionElementary particleCovariancesymbols.namesakePauli exclusion principleRegularization (physics)Quantum electrodynamicssymbolsApplied mathematicsCutoffGauge theoryPhysics Letters B
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Docc¯nn¯bound states exist?

2007

The four-quark system $c\overline{c}n\overline{n}$ is studied in the framework of the constituent quark model. Using different types of quark-quark potentials, we solve the four-body Schr\"odinger equation by means of the hyperspherical harmonic formalism. Exploring the low laying ${J}^{\mathrm{PC}}$ states for different isospin configurations no four-quark bound states have been found. Of particular interest is the possible four-quark structure of the $X(3872)$. We rule out the possibility that this particle is a compact tetraquark system, unless additional correlations, either in the form of diquarks or at the level of the interacting potential, not considered in simple quark models do co…

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelConstituent quarkParticle identificationSchrödinger equationsymbols.namesakeIsospinQuantum mechanicsBound statesymbolsHigh Energy Physics::ExperimentTetraquarkMathematical physicsPhysical Review D
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