Search results for "Vector"

showing 10 items of 2660 documents

Radiative decay intoγPof the low lying axial-vector mesons

2008

We evaluate the radiative decay into a pseudoscalar meson and a photon of the whole set of the axial-vector mesons dynamically generated from the vector-pseudoscalar meson interaction. We take into account tree level and loop diagrams coming from the axial-vector decay into a vector and a pseudoscalar meson. We find a large span for the values of the radiative widths of the different axial-vector mesons. In particular, we evaluate the radiative decay into K{gamma} of the two K{sub 1}(1270) states, recently claimed theoretically, and discuss the experimental values quoted so far on the assumption of only one state.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryState (functional analysis)Pseudoscalar mesonNuclear physicsTree (descriptive set theory)symbols.namesakesymbolsRadiative transferFeynman diagramHigh Energy Physics::ExperimentPseudovectorPhysical Review D
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Single-spin asymmetries of $d(\gamma,\pi)NN$ in the first resonance region

2003

Incoherent photoproduction of pions on the deuteron in the first resonance region is investigated with special emphasis on single-spin asymmetries. For the elementary pion production operator an effective Lagrangian model which includes the standard pseudovector Born terms and a resonance contribution from the $\Delta$(1232)-excitation is used. Single-spin asymmetries, both for charged and neutral pion photoproduction on the deuteron, are analyzed and calculated for the first time in the first resonance region. The linear photon asymmetry $\Sigma$, vector target asymmetry $T_{11}$ and tensor target asymmetries $T_{20}$, $T_{21}$, and $T_{22}$ for the reaction $d(\gamma,\pi)NN$ are predicted…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonNuclear TheoryOperator (physics)media_common.quotation_subjectNuclear TheoryResonance (particle physics)AsymmetryNuclear physicsPionHigh Energy Physics::ExperimentTensorSpin (physics)Nuclear ExperimentPseudovectormedia_common
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Photoproduction of theωmeson on the proton near threshold

2015

An experimental study of omega photoproduction on the proton was conducted by using the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. The gamma p -> omega p differential cross sections are measured from threshold to the incident-photon energy E-gamma = 1.40 GeV (W = 1.87 GeV for the center-of-mass energy) with 15-MeV binning in E-gamma and full production-angle coverage. The quality of the present data near threshold gives access to a variety of interesting physics aspects. As an example, an estimation of the omega N scattering length alpha(omega p) is provided.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonProtonMesonVector meson dominanceScattering length7. Clean energyOmegaNuclear physicsNuclear ExperimentMicrotronCrystal BallPhysical Review C
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Heavy neutrino mixing and single production at linear collider

1997

We study the single production of heavy neutrinos via the processes $e^-e^+ \to \nu N$ and $e^-\gamma \to W^- N$ at future linear colliders. As a base of our considerations we take a wide class of models, both with vanishing and non-vanishing left-handed Majorana neutrino mass matrix $m_L$. We perform a model independent analyses of the existing experimental data and find connections between the characteristic of heavy neutrinos (masses, mixings, CP eigenvalues) and the $m_L$ parameters. We show that with the present experimental constraints heavy neutrino masses almost up to the collision energy can be tested in the future experiments.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesMass matrix01 natural sciences7. Clean energylaw.inventionBase (group theory)High Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Neutrino010306 general physicsColliderEigenvalues and eigenvectorsMixing (physics)Physics Letters B
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Implications of a Rotating Mass Matrix

2001

The fermion mass matrix, in addition to having eigenvalues (masses) which run, also changes its orientation (rotates) with changing energy scales. This means that its eigenstates at one scale will no longer be eigenstates at another scale, leading to effects where fermions of different flavours can ``transmute'' into one another. In this paper, the implications of a rotating mass matrix are analysed and possible transmuation effects are investigated both in the Standard Model (SM) and in the so-called Dualized Standard Model (DSM) that we advocate, arriving at the conclusion that some transmutational decays such as $\psi \longrightarrow \mu \tau$, $\Upsilon \longrightarrow \mu \tau$ or $\pi…

PhysicsNuclear and High Energy PhysicsParticle physicsScale (ratio)Electron–positron annihilationFísicaFOS: Physical sciencesFermionMass matrixStandard ModelOrientation (vector space)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Energy (signal processing)Eigenvalues and eigenvectors
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On the universal bundle for gravity

1991

Abstract We construct a supergravity type theory based on a superspace whose odd directions consist of a vector, together with a scalar representing a topological BRST shift symmetry. As such, the resulting theory is a theory of topological gravity. The gravitino is interpreted as a ghost field for this shift symmetry and plays the usual role of gauge field for local supersymmetry. Our construction is within the bundle of frames approach to superspace where covariant torsion constraints are analyzed, and we find that the resulting theory contains additional fields which are not present in existing theories of topological gravity. In particular, a minimal solution exists which contains a BRS…

PhysicsNuclear and High Energy PhysicsParticle physicsSupergravityScalar (mathematics)Vector bundleSupersymmetrySuperspaceBRST quantizationGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheoryTheoretical physicsGauge theoryScalar fieldGeneral Theoretical Physics
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The baryonic spectrum in a constituent quark model including a three-body force

1992

We analyze, within a non-relativistic quark model, the low energy part of the baryonic spectrum in the octet and decuplet flavour representations. The relevance of a strong Coulomb potential is emphasized in order to explain its general features. The addition of a three-body force allows to solve the ‘Roper puzzle’, giving a consistent explanation to its relative position in the spectrum.

PhysicsNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Octet010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuark modelFlavourConstituent quark01 natural sciencesBottom quarkThree-body forceBaryonPosition (vector)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsZeitschrift f�r Physik A Hadrons and Nuclei
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Spin-dipole nuclear matrix elements for double beta decays and astro-neutrinos

2014

Spin-dipole (SD) nuclear matrix elements (NMEs) M±(SD2) for unique first forbidden β±2−→0+ ground-state-to-ground-state transitions are studied by using effective microscopic two-nucleon interactions in realistic single-particle model spaces. The observed values of the NMEs Mexp±(SD2) are compared with the values of the single-quasiparticle NMEs Mqp±(SD2) without nucleon spin–isospin (στ) correlation and the QRPA NMEs MQRPA±(SD2) with the στ correlation. The observed SD matrix elements are found to be reduced by the factor k≈0.2 with respect to Mqp±(SD2) and by the factor kNM≈0.5 with respect to MQRPA±(SD2). We then infer that the SD NME is reduced considerably partly by the nucleon στ corr…

PhysicsNuclear and High Energy PhysicsParticle physicsta114Renormalization of the axial-vector weak coupling constantPhysics::Medical PhysicsNuclear Theorycoupling constantdouble beta decayrenormalization of the axial-vector weakDouble beta decayspin-dipole matrix elementNuclear physicsDipoleMatrix (mathematics)Double beta decaySpin-dipole matrix elementBeta (velocity)Neutrinounique forbidden beta decayNuclear ExperimentSpin (physics)NucleonUnique forbidden beta decayPhysics Letters B
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Measurements ofe+e−→K+K−η,K+K−π0, andKs0K±π∓cross sections using initial state radiation events

2008

This paper reports measurements of processes: e+e-→γKS0K±π∓, e+e-→γK+K-π0, e+e-→γϕη, and e+e-→γϕπ0. The initial-state radiated photon allows to cover the hadronic final state in the energy range from thresholds up to ≈4.6  GeV. The overall size of the data sample analyzed is 232  fb-1, collected by the BABAR detector running at the PEP-II e+e- storage ring. From the Dalitz plot analysis of the KS0K±π∓ final state, moduli, and relative phase of the isoscalar and the isovector components of the e+e-→KK*(892) cross section are determined. Parameters of ϕ and ρ recurrences are also measured, using a global fitting procedure which exploits the interconnection among amplitudes, moduli, and phases…

PhysicsNuclear and High Energy PhysicsPhotonIsovector010308 nuclear & particles physicsElectron–positron annihilationIsoscalarHadronDalitz plot01 natural sciencesNuclear physicsAmplitude0103 physical sciences010306 general physicsVEPP-2000Physical Review D
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Angular distribution of coherent bremsstrahlung

2012

The angular distribution of the linearly polarised photon beam produced by coherent bremsstrahlung from an aligned diamond radiator has been measured at the MAMI A2 tagged photon facility. The measurements were made with a prototype position sensitive photon detector which utilises the pair production process and a double sided silicon strip detector. This polarised photon beam is used for nuclear and hadronic experiments and in their analysis the polarisation is obtained from a calculation, which matches the experimental intensity spectrum. As the polarisation is related to the photon beam angular distribution, the present measurements can be used to test this calculation. The overall agre…

PhysicsNuclear and High Energy PhysicsPhotonbusiness.industryDetectorHadronBremsstrahlungDiamondengineering.materialOpticsPair productionPosition (vector)engineeringRadiator (engine cooling)businessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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