Search results for "Variant"

showing 10 items of 1267 documents

Structure at 2175 MeV ine+e−→ϕf0(980)observed via initial-state radiation

2006

We study the initial-state-radiation processes e+e-→K+K-π+π- γ and e+e-→K+K-π0π0γ using an integrated luminosity of 232fb-1 collected at the Υ(4S) mass with the BABAR detector at SLAC. Even though these reactions are dominated by intermediate states with excited kaons, we are able to study for the first time the cross section for e+e-→ (1020)f0(980) as a function of center-of-mass energy. We observe a structure near threshold consistent with a 1 - resonance with mass m=2.175±0. 010±0.015GeV/c2 and width Γ=58±16±20MeV. We observe no Y(4260) signal and set a limit of BY→ π+π-•ΓeeY<0. 4eV (90% confidence level), which excludes some models. © 2006 The American Physical Society.

PhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsElectron–positron annihilation01 natural sciencesResonance (particle physics)Particle identificationLuminosityNuclear physicsExcited state0103 physical sciencesIntermediate stateInvariant massAtomic physics010306 general physicsPhysical Review D
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Thee+e−→3(π+π−),2(π+π−π0)andK+K−2(π+π−)cross sections at center-of-mass energies from production threshold to 4.5 GeV measured with initial-state rad…

2006

We study the processes e^+e^- → 3(π^+π^-)γ, 2(π^+π^-π^0)γ and K^+K^-2(π^+π^-)γ, with the photon radiated from the initial state. About 20 000, 33 000 and 4000 fully reconstructed events, respectively, have been selected from 232  fb^(-1) of BABAR data. The invariant mass of the hadronic final state defines the effective e^+e^- center-of-mass energy, so that these data can be compared with the corresponding direct e^+e^- measurements. From the 3(π^+π^-), 2(π^+π^-π^0) and K^+K^-2(π^+π^-) mass spectra, the cross sections for the processes e^+e^- → 3(π^+π^-), e^+e^- → 2(π^+π^-π^0) and e^+e^- → K^+K^-2(π^+π^-) are measured for center-of-mass energies from production threshold to 4.5 GeV. The unc…

PhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsElectron–positron annihilationHadronRadiation01 natural sciencesNuclear physics0103 physical sciencesMass spectrumInvariant massAtomic physics010306 general physicsVEPP-2000Physical Review D
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The Crystal Barrel spectrometer at LEAR

1992

The crystal Barrel spectrometer used at LEAR, CERN to study the products of pd annihilations is described. A 1380 element array of Csl crystals measures photons from the decay of π0, η, η′ and ω mesons. A segmented drift chamber in a 1.5T magnetic field is used to identify and measure charged particles. A fast on-line trigger on charged and neutral multiplicities and on the invariant mass of secondary particles is available. The performance of the detector is discussed.

PhysicsNuclear and High Energy PhysicsPhotonLarge Hadron ColliderSpectrometerMesonPhysics::Instrumentation and Detectors010308 nuclear & particles physics01 natural sciencesCharged particleMagnetic fieldNuclear physicsCrystal0103 physical sciencesInvariant mass[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentation
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Structure analysis of the virtual Compton scattering amplitude at low energies

1998

We analyze virtual Compton scattering off the nucleon at low energies in a covariant, model-independent formalism. We define a set of invariant functions which, once the irregular nucleon pole terms have been subtracted in a gauge-invariant fashion, is free of poles and kinematical zeros. The covariant treatment naturally allows one to implement the constraints due to Lorentz and gauge invariance, crossing symmetry, and the discrete symmetries. In particular, when applied to the $ep\to e'p'\gamma$ reaction, charge-conjugation symmetry in combination with nucleon crossing generates four relations among the ten originally proposed generalized polarizabilities of the nucleon.

PhysicsNuclear and High Energy PhysicsPhotonNuclear TheoryLorentz transformationCrossingNuclear TheoryCompton scatteringFOS: Physical sciencesPROTONNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsPIONsymbolsCovariant transformationGauge theoryNucleonNUCLEONNuclear Experiment3RD-ORDER SPIN POLARIZABILITIES
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Photoproduction of neutral pion pairs from the proton

2000

Double neutral pion photoproduction from the proton has been measured at MAMI for photon energies between threshold and 820 MeV. The reaction was identified by an invariant mass and missing mass analysis. From threshold up to 370 MeV the total cross-section does not exceed 30 nb. For higher energies it shows a smooth rise until it reaches a maximum of about 10 μb at Eγ = 740 MeV. Dalitz plots of m2(π0π0) versusm2(p,π0) for seven bins of incident photon energy have been analysed. For Eγ > 610 MeV, a strong contribution of a sequential decay is observed with the Δ(1232)-resonance as intermediate state. A comparison to model calculations shows that these sequential decays presumably originate …

PhysicsNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsNuclear TheoryHadronResonanceDalitz plotPhoton energy7. Clean energy01 natural sciencesNuclear physicsPion0103 physical sciencesInvariant massAtomic physicsNuclear Experiment010306 general physicsThe European Physical Journal A
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Duality-invariant Einstein-Planck relation and the speed of light at very short wavelengths

2011

We propose a generalized Einstein-Planck relation for photons which is invariant under the change $\ensuremath{\lambda}/a{l}_{P}$ to $a{l}_{P}/\ensuremath{\lambda}$, $\ensuremath{\lambda}$ being the photon wavelength, ${l}_{P}$ Planck's length, and $a$ a numerical constant. This yields a wavelength-dependent speed of light $v(\ensuremath{\lambda})=c/(1+{a}^{2}({l}_{P}/\ensuremath{\lambda}{)}^{2})$, with $c$ the usual speed of light in vacuo, indicating that the speed of light should decrease for sufficiently short wavelengths. We discuss the conceptual differences with the previous proposals related to a possible decrease of the speed of light for very short wavelengths based on quantum flu…

PhysicsNuclear and High Energy PhysicsPhotonUncertainty principleInvariant (physics)Lambdasymbols.namesakeWavelengthQuantum mechanicssymbolsQuantum gravityPlanckLight velocity Einstein-Planck relation duality relationsSettore MAT/07 - Fisica MatematicaQuantum fluctuation
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Performance of production modules of the Belle II pixel detector in a high-energy particle beam

2021

The Belle II experiment at the Super B factory SuperKEKB, an asymmetric $e^+e^-$ collider located in Tsukuba, Japan, is tailored to perform precision B physics measurements. The centre of mass energy of the collisions is equal to the rest mass of the $\Upsilon(4S)$ resonance of $m_{\Upsilon(4S)} = 10.58\,\rm GeV$. A high vertex resolution is essential for measuring the decay vertices of B mesons. Typical momenta of the decay products are ranging from a few tens of MeV to a few GeV and multiple scattering has a significant impact on the vertex resolution. The VerteX Detector (VXD) for Belle II is therefore designed to have as little material as possible inside the acceptance region. Especial…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsDetectorFOS: Physical sciencesDESYInstrumentation and Detectors (physics.ins-det)01 natural sciences7. Clean energyCharge sharinglaw.inventionB-factoryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciencesInvariant massHigh Energy Physics::Experiment010306 general physicsColliderInstrumentationImage resolutionBeam (structure)
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Excitation of S11 resonances in pion scattering and pion photoproduction on the proton

2002

A self-consistent analysis of pion scattering and pion photoproduction within a coupled channels dynamical model is presented. In the case of pion photoproduction, we obtain background contributions to the imaginary part of the S-wave multipole which differ considerably from the result based on the K-matrix approximation. Within the dynamical model these background contributions become large and negative in the region of the S_{11}(1535) resonance. Due to this fact much larger resonance contributions are required in order to explain the results of the recent multipole analyses. For the first S_{11}(1535) resonance we obtain as a value of the dressed electromagnetic helicity amplitude: A_{1/…

PhysicsNuclear and High Energy PhysicsProtonNuclear TheoryScatteringNuclear TheoryFOS: Physical sciencesOrder (ring theory)ResonanceHelicityNuclear Theory (nucl-th)Nuclear physicsPionInvariant massHigh Energy Physics::ExperimentMultipole expansionNuclear Experiment
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Study of polarization observables in double pion photoproduction on the proton

2001

Using a model for two pion photoproduction on the proton previously tested in total cross sections and invariant mass distributions, we evaluate here polarization observables on which recent experiments are providing new information. We evaluate cross sections for spin 1/2 and 3/2, which are measured at Mainz and play an important role in tests of the GHD sum rule. We also evaluate the proton polarization asymmetry $\Sigma$ which is currently under investigation at GRAAL in Grenoble.

PhysicsNuclear and High Energy PhysicsProtonNuclear Theorymedia_common.quotation_subjectPolarization observablesNuclear TheoryFísicaFOS: Physical sciencesPolarization (waves)AsymmetryNuclear physicsNuclear Theory (nucl-th)PionInvariant massSum rule in quantum mechanicsNuclear Experimentmedia_commonSpin-½
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Covariant phase-space quantization of the induced 2D gravity

1993

Abstract We study in a parallel way the induced 2D gravity and the Jackiw-Teitelboimmodel on the cylinder from the viewpoint of the covariant description of canonical formalism. We compute explicity thhe symplectic structure of both theories showing that their (reduced) phase spaces are finite-dimensional cotangent bundles. For the Jackiw-Teitelboim model the base space (configuration space) is the space of conjugacy classes of the PSL(2, R ) group. For the induced 2D gravity, and Λ > 0, the (reduced) phase space consist of two (identical) connected components each one isomorphic to the contangent bundle of the space of hyperbolic conjugacy classes of the PSL (2, R ) group, whereas for Λ R …

PhysicsNuclear and High Energy PhysicsPure mathematicsCanonical quantizationHilbert spaceCotangent spacesymbols.namesakeConjugacy classOperator algebraQuantum mechanicsPhase spacesymbolsCovariant transformationConfiguration spaceGeneral Theoretical PhysicsNuclear Physics B
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