Search results for "PARITY"

showing 10 items of 513 documents

Observation of a New Narrow Axial-Vector Mesona1(1420)

2015

The COMPASS Collaboration at CERN has measured diffractive dissociation of 190  GeV/c pions into the π(-)π(-)π(+) final state using a stationary hydrogen target. A partial-wave analysis (PWA) was performed in bins of 3π mass and four-momentum transfer using the isobar model and the so far largest PWA model consisting of 88 waves. A narrow peak is observed in the f0(980)π channel with spin, parity and C-parity quantum numbers J(PC)=1(++). We present a resonance-model study of a subset of the spin-density matrix selecting 3π states with J(PC)=2(++) and 4(++) decaying into ρ(770)π and with J(PC)=1(++) decaying into f0(980)π. We identify a new a1 meson with mass (1414(-13)(+15))  MeV/c2 and wid…

PhysicsQuantum chromodynamicsMeson010308 nuclear & particles physicsPartial wave analysisGeneral Physics and AstronomyParity (physics)Quantum number01 natural sciencesNuclear physicsPion0103 physical sciencesIsobarHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPseudovectorPhysical Review Letters
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Entanglement transfer in a noisy cavity network with parity-deformed fields

2019

We investigate the effects of parity-deformed fields on the dynamics of entanglement transfer to distant noninteracting atomic qubits. These qubits are embedded in two distant lossy cavities connected by a leaky short-length fiber (or additional cavity). The process is studied within a single-excitation subspace, the parity-deformed cavity photons allowing the introduction of static local classical fields, which function as a control. The mechanism of state transfer is analyzed in comparison to the uncontrolled case. We find that the transfer evolution exhibits an asymmetry with respect to atom-field detuning, being sensitive to the sign of the detuning. Under a linear interaction controlle…

PhysicsQuantum networkPhotonQuantum informationmedia_common.quotation_subjectCavity quantum electrodynamicsStatistical and Nonlinear PhysicsQuantum channelQuantum entanglementEntanglement transfer01 natural sciencesAsymmetryAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della Materia010309 opticsQubitQuantum mechanics0103 physical sciencesParity-deformed fieldQuantum informationmedia_common
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The physical origin of a photon-number parity effect in cavity quantum electrodynamics

2021

Abstract The rapidly increasing capability to modulate the physicochemical properties of atomic groups and molecules by means of their coupling to radiation, as well as the revolutionary potential of quantum computing for materials simulation and prediction, fuel the interest for non-classical phenomena produced by atom-radiation interaction in confined space. One of such phenomena is a “parity effect” that arises in the dynamics of an atom coupled to two degenerate cavity field modes by two-photon processes and manifests itself as a strong dependence of the field dynamics on the parity of the initial number of photons. Here we identify the physical origin of this effect in the quantum corr…

PhysicsQuantum opticsPhotonEntropyPhysicsQC1-999Degenerate energy levelsCavity quantum electrodynamicsGeneral Physics and AstronomyParity (physics)Quantum entanglementAtom-field interaction; Entropy; Parity effect; Quantum entanglement; Quantum opticsParity effectQuantum entanglementAtom-field interactionQuantum mechanicsQuantum informationQuantumQuantum computerResults in Physics
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Parity violation correlations in light muonic atoms

1989

The 2 S -1 S transition in light muonic atoms is very sensitive to parity violation correlations induced via neutral currents. Observables depending on these transitions such as the photon polarization and the angular correlation between the emitted radiation and the atom polarization are a clear signal of weak neutral currents in atoms. We find the relation between the lepton and quark couplings and these observables emphasizing the effect of the nuclear spin. The results expected in muonic, atoms μ- 4 He and μ- 3 He are given.

PhysicsQuarkBeam PhysicsPhysics and Astronomy (miscellaneous)Particle Acceleration and DetectionFísicaElementary particleObservableParity (physics)Polarization (waves)Nuclear physicsPhoton polarizationPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsQuantum field theoryEngineering (miscellaneous)Elementary ParticlesLeptonNuclear Physics
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The negative-parity spin-1/2 Λ baryon spectrum from lattice QCD and effective theory

2021

The spectrum of the negative-parity spin-1/2 $\Lambda$ baryons is studied using lattice QCD and hadronic effective theory in a unitarized coupled-channel framework. A direct comparison between the two approaches is possible by considering the hadronic effective theory in a finite volume and with hadron masses and mesonic decay constants that correspond to the situation studied on the lattice. Comparing the energy level spectrum and $SU(3)$ flavor decompositions of the individual states, it is found that the lowest two states extracted from lattice QCD can be identified with one of the two $\Lambda(1405)$-poles and the $\Lambda(1670)$ resonance. The quark mass dependences of these two lattic…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsFinite volume method010308 nuclear & particles physicsHigh Energy Physics::LatticePhysicsQC1-999HadronNuclear TheoryHigh Energy Physics::PhenomenologyParity (physics)Lattice QCD01 natural sciencesBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeLattice (order)0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsPhysics Letters B
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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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Understanding the Low Energy Hadron Spectrum in a Chiral Quark Cluster Model

1999

The low energy N and Δ spectra are studied by means of a chiral quark cluster model. We solve the Schrodinger equation in the hyperspherical harmonic approach. The interacting potential includes Goldstone boson exchanges besides the usual one-gluon exchange. The predicted baryonic spectrum is quite reasonable. However, if consistency with the two-baryon sector is required, the observed inversion of the positive and negative parity excitations of the nucleon cannot be obtained. Alternative solutions are discussed.

PhysicsQuarkParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadronParity (physics)Spectral lineSchrödinger equationBaryonsymbols.namesakeGoldstone bosonsymbolsNucleon
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Discrete symmetries with neutral mesons

2018

Symmetries, and Symmetry Breakings, in the Laws of Physics play a crucial role in Fundamental Science. Parity and Charge Conjugation Violations prompted the consideration of Chiral Fields in the construction of the Standard Model, whereas CP-Violation needed at least three families of Quarks leading to Flavour Physics. In this Lecture I discuss the Conceptual Basis and the present experimental results for a Direct Evidence of Separate Reversal-in-Time T, CP and CPT Genuine Asymmetries in Decaying Particles like Neutral Meson Transitions, using Quantum Entanglement and the Decay as a Filtering Measurement. The eight transitions associated to the Flavour-CP eigenstate decay products of entang…

PhysicsQuarkParticle physicsMeson010308 nuclear & particles physicsmedia_common.quotation_subjectPhysicsQC1-999High Energy Physics::PhenomenologyObservableParity (physics)Quantum entanglement01 natural sciencesAsymmetry0103 physical sciencesHigh Energy Physics::ExperimentSymmetry breakingQuantum field theory010306 general physicsmedia_commonEPJ Web of Conferences
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About the realization of chiral symmetry in QCD2

1992

Two dimensional massless Quantum Chromodynamics presents many features which resemble those of the true theory. In particular the spectrum consists of mesons and baryons arranged in flavor multiplets without parity doubling. We analyze the implications of chiral symmetry, which is not spontaneously broken in two dimensions, in the spectrum and in the quark condensate. We study how parity doubling, an awaited consequence of Coleman's theorem, is avoided due to the dimensionality of space-time and confinement. We prove that a chiral phase transition is not possible in the theory.

PhysicsQuarkQuantum chromodynamicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySpectrum (functional analysis)FOS: Physical sciencesFísicaParity (physics)BaryonMassless particleHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Engineering (miscellaneous)Realization (systems)Zeitschrift f�r Physik C Particles and Fields
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