Search results for "Variant"

showing 10 items of 1267 documents

Summary of the HypHI Phase 0 experiment and future plans with FRS at GSI (FAIR Phase 0)

2016

WOS: 000381331200014

PhysicsNuclear and High Energy PhysicsCOLLISIONSLifetime measurement010308 nuclear & particles physicsInvariant massLIFETIMEHeavy ion induced reactionHYPERNUCLEAR SPECTROSCOPY01 natural sciencesNuclear physicsShort lifetimeStatistical analysesFRS and Super-FRS0103 physical sciencesRI-beamHeavy ionInvariant massLIGHT HYPERFRAGMENTS010306 general physicsSpectroscopyRELATIVISTIC HYPERNUCLEINuclear Physics A
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The HypHI Phase 0 experiment

2010

10th International Conference on Hypernuclear and Strange Particle Physics -- SEP 14-18, 2009 -- Tokai, JAPAN

PhysicsNuclear and High Energy PhysicsCarbon graphiteProjectilehypernuclear spectroscopyPhase (waves)LambdaNuclear physicsheavy ion induced reactioninvariant massHeavy ionENERGY NUCLEAR COLLISIONSAtomic physicsSpectroscopyNuclear Physics A
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Locality properties of Neuberger's lattice Dirac operator

1998

The gauge covariant lattice Dirac operator D which has recently been proposed by Neuberger satisfies the Ginsparg-Wilson relation and thus preserves chiral symmetry. The operator also avoids a doubling of fermion species, but its locality properties are not obvious. We now prove that D is local (with exponentially decaying tails) if the gauge field is sufficiently smooth at the scale of the cutoff. Further analytic and numerical studies moreover suggest that the locality of the operator is in fact guaranteed under far more general conditions.

PhysicsNuclear and High Energy PhysicsChiral symmetryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)LocalityFOS: Physical sciencesFísicaParticle Physics - LatticeFermionDirac operatorsymbols.namesakeHigh Energy Physics - LatticeLattice (order)symbolsCutoffCovariant transformationGauge theoryMathematical physics
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Observation of the exclusive reactione+e−→ϕηats=10.58  GeV

2006

The authors report the observation of e{sup +}e{sup -} {yields} {phi}{eta} near {radical}s = 10.58 GeV with 6.5 {sigma} significance in the K{sup +}K{sup -}{gamma}{gamma} final state in a data sample of 224 fb{sup -1} collected by the BABAR experiment at the PEP-II e{sup +}e{sup -} storage rings. They measure the restricted radiation-corrected cross section to be {sigma}(e{sup +}e{sup -} {yields} {phi}{eta}) = 2.1 {+-} 0.4(stat) {+-} 0.1(syst) fb within the range |cos{theta}*| < 0.8, where {theta}* is the center-of-mass polar angle of the {phi} meson. The {phi} meson is required to be in the invariant mass range of 1.008 < m{sub {phi}} < 1.035 GeV/c{sup 2}. The radiation corrected cross sec…

PhysicsNuclear and High Energy PhysicsCrystallographyParticle physicsMeson010308 nuclear & particles physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant massNuclear Experiment010306 general physics01 natural sciencesPhysical Review D
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Fully covariant and conformal formulation of the Z4 system in a reference-metric approach: Comparison with the BSSN formulation in spherical symmetry

2014

We adopt a reference-metric approach to generalize a covariant and conformal version of the Z4 system of the Einstein equations. We refer to the resulting system as ``fully covariant and conformal", or fCCZ4 for short, since it is well suited for curvilinear as well as Cartesian coordinates. We implement this fCCZ4 formalism in spherical polar coordinates under the assumption of spherical symmetry using a partially-implicit Runge-Kutta (PIRK) method and show that our code can evolve both vacuum and non-vacuum spacetimes without encountering instabilities. Our method does not require regularization of the equations to handle coordinate singularities, nor does it depend on constraint-preservi…

PhysicsNuclear and High Energy PhysicsCurvilinear coordinates010308 nuclear & particles physicsFOS: Physical sciencesSpherical coordinate systemGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmologylaw.inventionGeneral Relativity and Quantum CosmologyNumerical relativityClassical mechanicsHamiltonian constraintlaw0103 physical sciencesGravitational singularityCartesian coordinate systemCovariant transformationCircular symmetry010306 general physicsPhysical Review D
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Λ(1405)production in theπ−p→K0πΣreaction

2003

We discuss the mechanisms that lead to $\ensuremath{\Lambda}(1405)$ production in the ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}{K}^{0}\ensuremath{\pi}\ensuremath{\Sigma}$ reaction. The problem has gained renewed interest after different works converge to the conclusion that there are two resonances around the region of $1400\phantom{\rule{0.3em}{0ex}}\text{MeV}$, rather than one, and that they couple differently to the $\ensuremath{\pi}\ensuremath{\Sigma}$ and $\overline{K}N$ channels. We look at the dynamics of that reaction and find two mechanisms which eventually filter each one of the resonances, leading to very different shapes of the $\ensuremath{\pi}\ensuremath{\S…

PhysicsNuclear and High Energy PhysicsDistribution (mathematics)FactorizationUnitarityQuantum mechanicsHyperonSigmaProduction (computer science)Invariant massLambdaMathematical physicsPhysical Review C
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X(2175)as a resonant state of theϕKK¯system

2008

We perform a Faddeev calculation for the three-meson system $\ensuremath{\phi}K\overline{K}$, taking the interaction between two pseudoscalar mesons and between a vector and a pseudoscalar meson from the chiral unitary approach. We obtain a neat resonance peak around a total mass of 2150 MeV and an invariant mass for the $K\overline{K}$ system around 970 MeV, very close to the ${f}_{0}(980)$ mass. The state appears in $I=0$ and qualifies as a $\ensuremath{\phi}{f}_{0}(980)$ resonance. We enlarge the space of states including $\ensuremath{\phi}\ensuremath{\pi}\ensuremath{\pi}$, since $\ensuremath{\pi}\ensuremath{\pi}$ and $K\overline{K}$ build up the ${f}_{0}(980)$, and find moderate changes…

PhysicsNuclear and High Energy PhysicsFaddeev equationsParticle physicsMeson010308 nuclear & particles physicsState (functional analysis)16. Peace & justice01 natural sciencesPseudoscalar mesonResonance (particle physics)PseudoscalarParticle decay0103 physical sciencesInvariant mass010306 general physicsPhysical Review D
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Diagnostic Potential of Cosmic-Neutrino Absorption Spectroscopy

2004

Annihilation of extremely energetic cosmic neutrinos on the relic-neutrino background can give rise to absorption lines at energies corresponding to formation of the electroweak gauge boson $Z^{0}$. The positions of the absorption dips are set by the masses of the relic neutrinos. Suitably intense sources of extremely energetic ($10^{21}$ -- $10^{25}$-eV) cosmic neutrinos might therefore enable the determination of the absolute neutrino masses and the flavor composition of the mass eigenstates. Several factors--other than neutrino mass and composition--distort the absorption lines, however. We analyze the influence of the time-evolution of the relic-neutrino density and the consequences of …

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsCosmologiaPhysics::Instrumentation and Detectorsmedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaDark matterAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysicsPartícules (Física nuclear)UniverseCosmic neutrino backgroundHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedInvariant massHigh Energy Physics::ExperimentAbsorption (logic)Neutrinomedia_common
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Theoretical framework to analyze searches for hidden light gauge bosons in electron scattering fixed target experiments

2013

Motivated by anomalies in cosmic ray observations and by attempts to solve questions of the Standad Model of particle physics like the (g-2)_mu discrepancy, U(1) extensions of the Standard Model have been proposed in recent years. Such U(1) extensions allow for the interaction of Dark Matter by exchange of a photon-like massive force carrier \gamma' not included in the Standard Model. In order to search for \gamma' bosons various experimental programs have been started. One approach is the dedicated search at fixed-target experiments at modest energies as performed at MAMI or at the Jefferson Lab. In these experiments the process e(A,Z)->e(A,Z)l^+l^- is investigated and a search for a very …

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsOrder (ring theory)FOS: Physical sciencesParameter spaceResonance (particle physics)High Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Invariant massU-1Boson
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Set of sum rules for anomalous gauge boson couplings

1999

The dependence of the differential cross-section for on-shell W-pair production on the anomalous trilinear gauge couplings invariant under C and P is examined. It is shown that the contributions of the anomalous magnetic moments of the W boson due to the photon and the Z can be individually projected out by means of two appropriately constructed polynomials. The remaining four anomalous couplings are shown to satisfy a set of model-independent sum rules. Specific models which predict special relations among the anomalous couplings are then studied; in particular, the composite model of Brodsky and Hiller, and the linear and non-linear effective Lagrangian approaches. The relations predicted…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsPhotonElectron–positron annihilationForm factor (quantum field theory)FOS: Physical sciencesFísicaGauge (firearms)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BibliographySum rule in quantum mechanicsInvariant (mathematics)Particle Physics - Phenomenology
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