Search results for "Number"

showing 10 items of 3939 documents

Exotic meson-meson molecules and compact four-quark states

2009

PACS numbers: 12.39.Jh, 14.40.Lb, 21.45.-v, 31.15.xj.-- ArXiv pre-print avaible at: http://arxiv.org/abs/0903.2949v1

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyQuark modelFOS: Physical sciencesFísicaFew-body systemsHigh Energy Physics - PhenomenologyParticle decayHigh Energy Physics - Phenomenology (hep-ph)Bound stateHigh Energy Physics::ExperimentCharm (quantum number)Exotic mesonPhysical Review D
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Excited nucleons with chirally improved fermions

2003

We study positive and negative parity nucleons on the lattice using the chirally improved lattice Dirac operator. Our analysis is based on a set of three operators chi_i with the nucleon quantum numbers but in different representations of the chiral group and with different diquark content. We use a variational method to separate ground state and excited states and determine the mixing coefficients for the optimal nucleon operators in terms of the chi_i. We clearly identify the negative parity resonances N(1535) and N(1650) and their masses agree well with experimental data. The mass of the observed excited positive parity state is too high to be interpreted as the Roper state. Our results …

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesParity (physics)Dirac operatorQuantum numberDiquarkNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - LatticeVariational methodHigh Energy Physics - Phenomenology (hep-ph)symbolsNucleonGround state
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Classifying Reported and "Missing" Resonances According to Their P and C Properties

2000

The Hilbert space ℋ3q of the three quarks with one excited quark is decomposed into Lorentz group representations. It is shown that the quantum numbers of the reported and "missing" resonances fall apart and populate distinct representations that differ by their parity or/and charge conjugation properties. In this way, reported and "missing" resonances become distinguishable. For example, resonances from the full listing reported by the Particle Data Group are accommodated by Rarita–Schwinger (RS) type representations [Formula: see text] with k=1, 3, and 5, the highest spin states being J=3/2-, 7/2+, and 11/2+, respectively. In contrast to this, most of the "missing" resonances fall into t…

PhysicsQuarkNuclear and High Energy PhysicsSpin statesNuclear TheoryFOS: Physical sciencesAstronomy and AstrophysicsParity (physics)Particle Data GroupCharge (physics)Quantum numberAtomic and Molecular Physics and OpticsLorentz groupNuclear Theory (nucl-th)Quantum mechanicsExcited state
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Improved bounds on heavy quark electric dipole moments

2020

New bounds on the electric dipole moment (EDM) of charm and bottom quarks are derived using the stringent limits on their chromo-EDMs. The new limits, $|d_c|<1.5\times10^{-21}\:e\,\text{cm}$ and $|d_b|< 1.2\times 10^{-20}\:e\,\text{cm}$, improve the previous ones by about three orders of magnitude. These indirect bounds have implications for different models of new physics, including two-Higgs-doublet, leptoquarks, and supersymmetry models.

PhysicsQuarkParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Electric dipole momentDipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective lagrangianOrders of magnitude (speed)High Energy Physics::ExperimentCharm (quantum number)010306 general physics
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Measurements of the charged particle multiplicity distribution in restricted rapidity intervals

1995

Charged particle multiplicity distributions have been measured with the ALFPH detector in restricted rapidity intervals \Y\ less than or equal to 0.5, 1.0, 1.5, 2.0 along the thrust axis and also without restriction on rapidity. The distribution for the full range can be parametrized by a log-normal distribution. For smaller windows one finds a more complicated structure, which is understood to arise from perturbative effects. The negative-binomial distribution fails to describe the data both with and without the restriction on rapidity. The JETSET model is found to describe all aspects of the data while the width predicted by HERWIG is in significant disagreement.

PhysicsQuarkParticle physicsAlephDistribution (number theory)Physics and Astronomy (miscellaneous)010308 nuclear & particles physicsPhysicsDetectorMultiplicity (mathematics)01 natural sciencesCharged particleNuclear physics0103 physical sciencesRange (statistics)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RapidityHigh Energy Physics::Experiment010306 general physicsParticle Physics - Experiment
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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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Studies of Λcproduction in pp and p-Pb collisions 1 with ALICE at 2 the LHC

2017

A Large Ion Collider Experiment (ALICE) was designed to study the strongly interacting medium created in heavy-ion collisions at LHC energies, the Quark Gluon Plasma (QGP). Heavy quarks (charm and beauty), produced in the early stages of the collisions, are among the most powerful probes to study this state of matter. To study the QGP effects, it is important to establish reference data, which is done by analysing results from pp and p-Pb collisions.We report on the charmed baryon Λc measurement in pp collisions at √s = 7 TeV and in p-Pb collisions at √sNN = 5.02 TeV with the ALICE experiment, through the reconstruction of the decay channels Λc + → p K S 0 and Λc + → pK − π + .

PhysicsQuarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsQC1-999Nuclear TheoryHigh Energy Physics::Phenomenology01 natural sciencesIonlaw.inventionNuclear physicsBaryonlaw0103 physical sciencesQuark–gluon plasmaState of matterHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsColliderEPJ Web of Conferences
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Decay widths of the spin-2 partners of the X (3872)

2015

We consider the $X(3872)$ resonance as a $J^{PC}=1^{++}$ $D\bar D^*$ hadronic molecule. According to heavy quark spin symmetry, there will exist a partner with quantum numbers $2^{++}$, $X_{2}$, which would be a $D^*\bar D^*$ loosely bound state. The $X_{2}$ is expected to decay dominantly into $D\bar D$, $D\bar D^*$ and $\bar D D^*$ in $d$-wave. In this work, we calculate the decay widths of the $X_{2}$ resonance into the above channels, as well as those of its bottom partner, $X_{b2}$, the mass of which comes from assuming heavy flavor symmetry for the contact terms. We find partial widths of the $X_{2}$ and $X_{b2}$ of the order of a few MeV. Finally, we also study the radiative $X_2\to …

PhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyHadronFOS: Physical sciencesFísicaOrder (ring theory)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Quantum numberHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Bound stateHigh Energy Physics::ExperimentEngineering (miscellaneous)X(3872)Bar (unit)Spin-½European Physical Journal C
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Neutrinoless double β decay with small neutrino masses

2013

Proceedings of the Corfu Summer Institute 2012 "School and Workshops on Elementary Particle Physicsand Gravity", September 8-27, 2012, Corfu (Greece). PoS(Cofu2012)028.

PhysicsQuarkParticle physicsPhysics beyond the Standard ModelDouble betaHigh Energy Physics::PhenomenologyFísicaNeutrinolessLepton numberPartícules (Física nuclear)Operator (computer programming)Neutrino massDouble beta decayHigh Energy Physics::ExperimentNeutrinoPhenomenology (particle physics)LeptonDouble β
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Chiral dynamics in the low-temperature phase of QCD

2014

We investigate the low-temperature phase of QCD and the crossover region with two light flavors of quarks. The chiral expansion around the point $(T,m=0)$ in the temperature vs. quark-mass plane indicates that a sharp real-time excitation exists with the quantum numbers of the pion. An exact sum rule is derived for the thermal modification of the spectral function associated with the axial charge density; the (dominant) pion pole contribution obeys the sum rule. We determine the two parameters of the pion dispersion relation using lattice QCD simulations and test the applicability of the chiral expansion. The time-dependent correlators are also analyzed using the Maximum Entropy Method, yie…

PhysicsQuarkQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryThermal quantum field theoryHigh Energy Physics::LatticeDynamics (mechanics)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDQuantum numberNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticePionPhase (matter)Quantum electrodynamicsHigh Energy Physics::ExperimentSum rule in quantum mechanicsPhysical Review D
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