Search results for "charm"

showing 10 items of 390 documents

Follow-up on non-leptonic Kaon decays at large $N_c$

2018

We report on the status of our dynamical simulations of a $SU (N_c )$ gauge theory with $N_c=3-6$ and $N_f =4$ fundamental fermions. These ensembles can be used to study the Large $N_c$ scaling of weak matrix elements in the GIM limit $m_c=m_u$, that might shed some light on the origin of the $\Delta I=1/2$ rule. We present preliminary results for the $K \to \pi$ matrix elements in the $N_c=3$ dynamical simulations, where we observe a significant effect of the quark loops that goes in the direction of enhancing the ratio of $A_0/A_2$ amplitudes. Finally, we present the relevant NLO Chiral Perturbation Theory predictions for the relation between $K \to \pi $ and $K \to \pi \pi$ amplitudes in…

PhysicsQuarkParticle physicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFermion01 natural sciencesHigh Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeAmplitude0103 physical sciencesGauge theoryCharm (quantum number)010303 astronomy & astrophysicsScalingProceedings of The 36th Annual International Symposium on Lattice Field Theory — PoS(LATTICE2018)
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Meson resonances in the open and hidden charm sectors

2008

We briefly expose our model for generating open and hidden charm resonances and present the most interesting results.

PhysicsHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Phenomenology (hep-ph)MesonFOS: Physical sciencesFísicaHigh Energy Physics::ExperimentCharm (quantum number)GeneralLiterature_MISCELLANEOUSCharm quark
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One-Pion Charm Baryon Transitions in a Relativistic Three-Quark Model

1998

We study one-pion transitions between charm baryon states in the framework of a relativistic three-quark model. We calculate the charm baryon-pion coupling factors that govern the S-wave, P-wave and D-wave one-pion transitions from the s-wave and the lowest lying p-wave charm baryon states down to the s-wave charm baryon states. For these we obtain: g_{\Sigma_c\Lambda_c\pi}=8.88 GeV^{-1}, f_{\Lambda_{c1}\Sigma_c\pi}=0.52 and f_{\Lambda_{c1}^*\Sigma_c\pi}=21.5 GeV^{-2}. We compare our rate predictions for the one-pion transitions with experimental results.

PhysicsNuclear and High Energy PhysicsParticle physicsQuark modelHigh Energy Physics::PhenomenologyNuclear TheorySigmaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLambdaCoupling (probability)BaryonHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment
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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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Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb–Pb collisions at sNN=5.02 TeV

2020

The differential invariant yield as a function of transverse momentum (pT) of electrons from semileptonic heavy-flavour hadron decays was measured at midrapidity in central (0–10%), semi-central (30–50%) and peripheral (60–80%) lead–lead (Pb–Pb) collisions at sNN=5.02 TeV in the pT intervals 0.5–26 GeV/c (0–10% and 30–50%) and 0.5–10 GeV/c (60–80%). The production cross section in proton–proton (pp) collisions at s=5.02 TeV was measured as well in 0.5<pT<10 GeV/c and it lies close to the upper band of perturbative QCD calculation uncertainties up to pT=5 GeV/c and close to the mean value for larger pT. The modification of the electron yield with respect to what is expected for an inco…

QuarkSemileptonic decayPhysicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronPerturbative QCDParton01 natural sciencesNuclear physics0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsPhysics Letters B
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Odd parity bottom-flavored baryon resonances

2013

The LHCb Collaboration has recently observed two narrow baryon resonances with beauty. Their masses and decay modes look consistent with the quark model orbitally excited states Lambda(b)(5912) and Lambda(b)*(5920), with quantum numbers J(P) = 1/2(-) and 3/2(-), respectively. We predict the existence of these states within a unitarized meson-baryon coupled-channel dynamical model, which implements heavy-quark spin symmetry. Masses, quantum numbers and couplings of these resonances to the different meson-baryon channels are obtained. We find that the resonances Lambda(0)(b)(5912) and Lambda(0)(b)(5920) are heavy-quark spin symmetry partners, which naturally explains their approximate mass de…

Nuclear and High Energy PhysicsParticle physicsCharmNuclear TheoryN-asteriskHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesCHARMNuclear Theory (nucl-th)SUM-RULESHigh Energy Physics - Phenomenology (hep-ph)Heavy-quark symmetryMESON-EXCHANGE0103 physical sciencesChiral dynamicsNuclear Experiment010306 general physicsNuclear theorySpectroscopyKaon-nucleon interactionsPhysicsMeson-exchangeStatesSPECTROSCOPYCoupled-channelN-ASTERISK010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCHIRAL DYNAMICSFísicaCOUPLED-CHANNELHEAVY-QUARK SYMMETRYHigh Energy Physics - PhenomenologySTATESSum-rulesKAON-NUCLEON INTERACTIONSHigh Energy Physics::ExperimentSpin symmetryHumanities
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PREDICTION OF HIDDEN CHARM BARYONS WITH HEAVY QUARK SPIN AND LOCAL HIDDEN GAUGE SYMMETRIES

2014

In our talk, we explore a coupled channel unitary approach to investigate the meson baryon interaction with hidden charm, using constraints of heavy quark spin symmetry. With the full space of states demanded by the heavy quark spin symmetry and the dynamics of the local hidden gauge, we find four basic states which are bound by about 50 MeV with respect to the corresponding [Formula: see text], [Formula: see text], [Formula: see text] and [Formula: see text] thresholds respectively and decay mostly into ηcN and J/ψN. All the states appear in isospin I = 1/2, some of which are degenerated in different momentum J.

PhysicsBaryonQuarkParticle physicsMesonIsospinNuclear TheoryHigh Energy Physics::PhenomenologyCharm (quantum number)Nuclear ExperimentBottom quarkSpin-½J/psi mesonInternational Journal of Modern Physics: Conference Series
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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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Charm and hidden charm scalar mesons in the nuclear medium

2009

We study the renormalization of the properties of low-lying charm and hidden charm scalar mesons in a nuclear medium, concretely of the D-s0(2317) and the theoretical hidden charm state X(3700). We find that for the D-s0(2317), with negligible width at zero density, the width becomes about 100 MeV at normal nuclear-matter density, while in the case of the X(3700) the width becomes as large as 200 MeV. We discuss the origin of this new width and trace it to reactions occurring in the nucleus, while offering a guideline for future experiments testing these changes. We also show how those medium modifications will bring valuable information on the nature of the scalar resonances and the mechan…

Nuclear and High Energy PhysicsParticle physicsTrace (linear algebra)Nuclear TheoryMesonNuclear TheoryScalar (mathematics)FOS: Physical sciencesCHIRAL-SYMMETRY RESTORATIONNuclear Theory (nucl-th)RenormalizationUNITARY APPROACHCharm (quantum number)Nuclear ExperimentNN INTERACTIONPhysicsHEAVY MESONSZero (complex analysis)FísicaLOCAL SYMMETRYMULTIQUARK HADRONSNuclear matterGAUGE BOSONPHI-PHOTOPRODUCTIONHigh Energy Physics::ExperimentPI-PI INTERACTIONNucleonVECTOR-MESONSThe European Physical Journal A
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Observation of an Excited Charm BaryonΩc*Decaying toΩc0γ

2006

We report the first observation of an excited singly-charm baryon OmegaC* (css) in the radiative decay OmegaC0 Gamma, where the OmegaC0 baryon is reconstructed in the decays to the final states Omega-pi+, Omega-pi+pi0, Omega-pi+pi-pi+, and Cascade-K-pi+pi+. This analysis is performed using a dataset of 230.7 fb$-1} collected by the BABAR detector at the PEP-II asymmetric-energy B Factory at the Stanford Linear Accelerator Center. The mass difference between the OmegaC* and the OmegaC0 baryons is measured to be 70.8 +/- 1.0 (stat) +/- 1.1 (syst) MeV/c2. We also measure the ratio of inclusive production cross sections of OmegaC* and OmegaC0 in e+e- annihilation.

PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsElectron–positron annihilationGeneral Physics and Astronomy01 natural sciences7. Clean energyB-factoryCharmed baryonsBaryonNuclear physicsParticle decayPositronPair production0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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