Search results for "Charm"

showing 10 items of 390 documents

Electromagnetic form factors of spin 1/2 doubly charmed baryons

2018

We study the electromagnetic form factors of the doubly charmed baryons, using covariant chiral perturbation theory within the extended on-mass-shell (EOMS) scheme. Vector-meson contributions are also taken into account. We present results for the baryon magnetic moments, charge and magnetic radii. While some of the chiral Lagrangian parameters could be set to values determined in previous works, the available lattice results for $\Xi_{cc}^+$ and $\Omega_{cc}^+$ only allow for robust constraints on the low-energy constant (LEC) combination, $c_{89}(=-\frac{1}{3}c_8+4c_9)$. The couplings of the doubly charmed baryons to the vector mesons have been estimated assuming the Okubo--Zweig--Iizuka …

QuarkParticle physicsChiral perturbation theoryMesonHeavy baryon chiral perturbation theoryHigh Energy Physics::LatticeLattice field theoryNuclear TheoryFOS: Physical sciencesComputer Science::Digital Libraries01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Charmed baryonsBaryonHigh Energy Physics - Phenomenology
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Charm quark mass with calibrated uncertainty

2016

We determine the charm quark mass ${\hat m}_c({\hat m}_c)$ from QCD sum rules of moments of the vector current correlator calculated in perturbative QCD. Only experimental data for the charm resonances below the continuum threshold are needed in our approach, while the continuum contribution is determined by requiring self-consistency between various sum rules, including the one for the zeroth moment. Existing data from the continuum region can then be used to bound the theoretical error. Our result is ${\hat m}_c({\hat m}_c) = 1272 \pm 8$ MeV for $\hat\alpha_s(M_Z) = 0.1182$. Special attention is given to the question how to quantify and justify the uncertainty.

QuarkParticle physicsCurrent (mathematics)Physics and Astronomy (miscellaneous)High Energy Physics::LatticeFOS: Physical sciences01 natural sciencesCharm quarkHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesContinuum (set theory)Charm (quantum number)010306 general physicsEngineering (miscellaneous)PhysicsQCD sum rulesContinuum (measurement)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDMoment (mathematics)High Energy Physics - PhenomenologyZeroth law of thermodynamicsHigh Energy Physics::ExperimentSum rule in quantum mechanicsCurrent vectorThe European Physical Journal C
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Flavor physics in the quark sector

2010

218 páginas, 106 figuras, 89 tablas.-- arXiv:0907.5386v2.-- Report of the CKM workshop, Rome 9-13th Sep. 2008.-- et al.

QuarkParticle physicsKobayashi-Maskawa MatrixMesonField (physics)Rare Kaon DecaysHigh Energy Physics::LatticeFlavourGeneral Physics and AstronomyFOS: Physical sciencesPhysics and Astronomy(all)Determination of Cabibbo-Kobayashi & Maskawa (CKM) matrix element01 natural sciencesDirect Cp-ViolationStandard ModelTo-Leading OrderHigh Energy Physics - Phenomenology (hep-ph)Chiral Perturbation-Theory/dk/atira/pure/subjectarea/asjc/31000103 physical sciences010306 general physicsFlavorParticle Physics - PhenomenologyPhysics010308 nuclear & particles physics12.15.Hh Determination of Cabibbo-Kobayashi & Maskawa (CKM) matrix elementsHigh Energy Physics::PhenomenologyELEMENTARY PARTICLE PHYSICSFísicahep-ph13.20.Eb Decays of K mesonsQuantum numberLarge Tan-BetaSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciHigh Energy Physics - Phenomenology13.20.He Decays of bottom mesonsB MESON[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Effective-Field-TheoryCP violationB-Meson DecaysUniversal Extra DimensionsHigh Energy Physics::ExperimentCP VIOLATIONRooted Staggered FermionsCharmed mesons (|C|>0 B=0)
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Quark Structure of the X (4500), X (4700) and χc(4P,5P) States

2021

We study some of the main properties (masses and open-flavor strong decay widths) of 4P and 5P charmonia. While there are two candidates for the χc0(4P,5P) states, the X(4500) and X(4700), the properties of the other members of the χc(4P,5P) multiplets are still completely unknown. With this in mind, we start to explore the charmonium interpretation for these mesons. Our second goal is to investigate if the apparent mismatch between the Quark Model (QM) predictions for χc0(4P,5P) states and the properties of the X(4500) and X(4700) mesons can be overcome by introducing threshold corrections in the QM formalism. According to our coupled-channel model results for the threshold mass shifts, th…

QuarkParticle physicsMesonFormalism (philosophy)QC1-999Materials Science (miscellaneous)BiophysicsStructure (category theory)General Physics and Astronomystrong decayshiukkasfysiikka01 natural sciencesInterpretation (model theory)charmonia phenomenology0103 physical sciencesPhysical and Theoretical Chemistry010306 general physics3P0 modelMathematical PhysicsPhysicsquark modelkvarkit010308 nuclear & particles physicsPhysicsexotic statesQuark modelunquenched quark modelHigh Energy Physics - PhenomenologycharmoniaydinfysiikkaFrontiers in Physics
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MEASUREMENT OF THE FORWARD-BACKWARD ASYMMETRY OF CHARM AND BOTTOM QUARKS AT THE Z-POLE USING D-ASTERISK(+/-)-MESONS

1995

The forward-backward asymmetries for the processes $$e^ + e^ - \to c\bar c$$ and $$e^ + e^ - \to b\bar b$$ at theZ resonance are measured using identifiedD *± mesons. In 905,000 selected hadronic events, taken in 1991 and 1992 with the DEL-PHI detector at LEP, 4757D *+→D 0π+ decays are reconstructed. Thec andb quark forward-backward asymmetries are determined to be: $$\begin{gathered} A_{FB}^{c\bar c} = 0.077 \pm 0.029(stat) \pm 0.012(sys), \hfill \\ A_{FB}^{b\bar b} = 0.059 \pm 0.062(stat) \pm 0.024(sys). \hfill \\ \end{gathered} $$ Constraining theb asymmetry to the value measured by DELPHI using independent analyses, the charm asymmetry is determined to be: $$A_{FB}^{c,const} = 0.068 \pm…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)MesonElectron–positron annihilationHadron01 natural sciencesDECAYSPartícules (Física nuclear)Charm quarkNuclear physicsDELPHI; forward-backward asymmetry; QCD0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]DECAYS; QCDCharm (quantum number)010306 general physicsEngineering (miscellaneous)DELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyWeinberg angleQCDLARGE ELECTRON POSITRON COLLIDERPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderPARTICLE PHYSICSforward-backward asymmetryHigh Energy Physics::ExperimentCol·lisionadors d'hadronsParticle Physics - Experiment
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Very Heavy Flavored Dibaryons

2020

We explore the possibility of very heavy dibaryons with three charm quarks and three beauty quarks, $bbbccc$, using a constituent model which should drive to the correct solution in the limit of hadrons made of heavy quarks. The six-body problem is treated rigorously, in particular taking into account the orbital, color and spin mixed-symmetry components of the wave function. Unlike a recent claim based on lattice QCD, no bound state is found below the lowest dissociation threshold.

QuarkParticle physicswave function[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryHigh Energy Physics::LatticeHadronLattice field theoryNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesdissociationspin01 natural sciencesCharm quarkquarkNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateheavy quark010306 general physicsWave functionconstituentNuclear ExperimentNuclear theoryPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologylattice field theoryLattice QCDcolordibaryon: heavybound stateHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Elementary Particles and FieldsHigh Energy Physics::ExperimenthadroncharmPhysical Review Letters
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Inclusive D* production in gamma-gamma collisions: including the single-resolved contribution with massive quarks

2003

We have calculated the next-to-leading order cross section for the inclusive production of charm quarks as a function of the transverse momentum p_T and the rapidity in two approaches using massive or massless charm quarks. For the single-resolved cross section we have derived the massless limit from the massive theory. We find that this limit differs from the genuine massless version with MS-bar factorization by finite corrections. By adjusting subtraction terms we establish a massive theory with MS-bar subtraction which approaches the massless theory very fast with increasing transverse momentum. With these results and including the equivalent results for the direct cross section obtained…

QuarkPhysicsAlephParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyFOS: Physical sciencesGamma gammaCharm quarkMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationTransverse momentumRapidityHigh Energy Physics::ExperimentEngineering (miscellaneous)
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Molecular and compact four-quark states

2009

5th International Conference on Quarks and Nuclear Physics (QNP09). Inst High Energy Phys Chinese Acad Sci, Beijing, PEOPLES R CHINA, SEP 21-25, 2009

QuarkPhysicsExoticsNuclear and High Energy PhysicsParticle physicsBar (music)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Bound stateQuark-modelsTetraquarksHigh Energy Physics::ExperimentInstrumentationCharmonium
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Elliptic Flow in Pb-Pb Collisions at

2017

We report a precise measurement of the J/ψ elliptic flow in Pb-Pb collisions at sNN=5.02  TeV with the ALICE detector at the LHC. The J/ψ mesons are reconstructed at midrapidity (|y|<0.9) in the dielectron decay channel and at forward rapidity (2.5<y<4.0) in the dimuon channel, both down to zero transverse momentum. At forward rapidity, the elliptic flow v2 of the J/ψ is studied as a function of the transverse momentum and centrality. A positive v2 is observed in the transverse momentum range 2<pT<8  GeV/c in the three centrality classes studied and confirms with higher statistics our earlier results at sNN=2.76  TeV in semicentral collisions. At midrapidity, the J/ψ  v2 is investigated as …

QuarkPhysicsMeson010308 nuclear & particles physicsElliptic flowGeneral Physics and AstronomyQuarkonium01 natural sciencesCharm quarkNuclear physicsMomentum0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physics
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Radiative decays of double heavy baryons in a relativistic constituent three-quark model including hyperfine mixing

2010

We study flavor-conserving radiative decays of double heavy baryons using a manifestly Lorentz covariant constituent three-quark model. Decay rates are calculated and compared to each other in the full theory, keeping masses finite, and also in the heavy quark limit. We discuss in some detail hyperfine mixing effects.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeQuark modelHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesElementary particleFermion01 natural sciencesBaryonNuclear physicsCharmed baryonsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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