Search results for "vector [form factor]"

showing 10 items of 770 documents

Design and Calculations for the New ECRIS at KVI

2005

In this paper a brief description is given of the on‐going upgrade of the CAPRICE‐type ECRIS injector of the K=600 AGOR cyclotron at KVI. This upgrade is motivated by the new TRIμP program, which requires a significant increase of available beam intensity by up to two orders in magnitude. The upgrade follows the AECR design of the university of Jyvaskyla, which was originally pioneered at LBNL (USA). We will discuss the mechanical design and magnetic field calculations of the solenoidal and the permanent magnetic hexapole fields.

PhysicsNuclear physicsUpgradeSolenoidal vector fieldlawCyclotronCyclotron resonanceMechanical designBeam (structure)Magnetic fieldlaw.inventionAIP Conference Proceedings
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First Exploration of Neutron Shell Structure below Lead and beyond N=126

2020

The nuclei below lead but with more than 126 neutrons are crucial to an understanding of the astrophysical r process in producing nuclei heavier than A∼190. Despite their importance, the structure and properties of these nuclei remain experimentally untested as they are difficult to produce in nuclear reactions with stable beams. In a first exploration of the shell structure of this region, neutron excitations in ^{207}Hg have been probed using the neutron-adding (d,p) reaction in inverse kinematics. The radioactive beam of ^{206}Hg was delivered to the new ISOLDE Solenoidal Spectrometer at an energy above the Coulomb barrier. The spectroscopy of ^{207}Hg marks a first step in improving our…

PhysicsNuclear reactionSpectrometerSolenoidal vector fieldNuclear TheoryGeneral Physics and AstronomyCoulomb barrier01 natural sciencesNuclear physicsLead (geology)0103 physical sciencesr-processPhysics::Accelerator PhysicsNeutron010306 general physicsSpectroscopyNuclear Experimentydinfysiikka
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Impact parameter dependent JIMWLK evolution meets HERA data

2019

We calculate the small-$x$ evolution of protons with finite size by solving numerically the JIMWLK evolution equation. The initial condition is constrained by the HERA measurements of charm reduced cross section and of exclusive vector meson production. We compute the energy dependence of diffractive cross sections in order to access the energy evolution of the event-by-event fluctuating proton density profile. The fundamental problems arising from the regime sensitive to non-perturbatively large dipoles are also discussed.

PhysicsParticle physicsFOS: Physical sciencesHERAhiukkasfysiikkaHigh Energy Physics - PhenomenologyCross section (physics)DipoleHigh Energy Physics - Phenomenology (hep-ph)Initial value problemCharm (quantum number)Vector mesonImpact parameterEnergy (signal processing)Proceedings of International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions — PoS(HardProbes2018)
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Photoproduction of thef2′(1525), a2(1320), andK2*(1430)

2016

Assuming that the ${f}_{2}^{\ensuremath{'}}(1525), {a}_{2}(1320)$, and ${K}_{2}^{*}(1430)$ resonances are dynamically generated states from vector-meson--vector-meson interactions in the $s$-wave with spin $S=2$, we study the $\ensuremath{\gamma}p\ensuremath{\rightarrow}{f}_{2}^{\ensuremath{'}}(1525)p, \ensuremath{\gamma}p\ensuremath{\rightarrow}{a}_{2}^{0}(1320)p$, and $\ensuremath{\gamma}p\ensuremath{\rightarrow}{K}_{2}^{*}(1430)\mathrm{\ensuremath{\Lambda}}(\mathrm{\ensuremath{\Sigma}})$ reactions. These reactions proceed in the following way: the incoming photon first mutates into a ${\ensuremath{\rho}}^{0}, \ensuremath{\omega}$, or $\ensuremath{\phi}$ meson via vector-meson dominance, …

PhysicsParticle physicsGauge bosonProtonMeson010308 nuclear & particles physics0103 physical sciencesVector meson010306 general physics01 natural sciencesOmegaSpin-½Physical Review C
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Measurement of OZI rule violation and spin alignment inϕandωproduction at COMPASS

2012

The COMPASS collaboration at CERN dedicated the 2008 and 2009 run time to hadron spectroscopy measurements with emphasis on the mesonic sector. At 190 GeV/c beam momentum, diffractive and double-Reggeon/Pomeron production mechanisms contribute. Studying vector meson production allows to explore this relatively unknown transition domain. We present results on the ratio of production yields for p p → (1020) p p ϕ and p p → p p ω (782) and its xF dependence where we find an OZI rule violation in the order of a factor of 3. In addition, the spin alignment of ω and ϕ as a function of xF is investigated.

PhysicsParticle physicsLarge Hadron ColliderPhysicsQC1-999High Energy Physics::PhenomenologyNuclear physicsMomentumPomeronOZI ruleCompassHadron spectroscopyHigh Energy Physics::ExperimentVector mesonSpin-½EPJ Web of Conferences
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Semileptonic decays of B(*) , D(*) into νl and pseudoscalar or vector mesons

2018

We perform a study of the ${B}^{(*)}$, ${D}^{(*)}$ semileptonic decays, using a different method than in conventional approaches, where the matrix elements of the weak operators are evaluated and a detailed spin-angular momentum algebra is performed to obtain very simple expressions at the end for the different decay modes. Using only one experimental decay rate in the $B$ or $D$ sectors, the rates for the rest of decay modes are predicted and they are in good agreement with experiment. Some discrepancies are observed in the $\ensuremath{\tau}$ decay mode for which we find an explanation. We perform evaluations for ${B}^{*}$ and ${D}^{*}$ decay rates that can be used in future measurements,…

PhysicsParticle physicsMeson010308 nuclear & particles physics01 natural sciencesPseudoscalar mesonMomentumPseudoscalarMatrix (mathematics)0103 physical sciencesHigh Energy Physics::ExperimentVector mesonAlgebra over a field010306 general physicsPhysical Review D
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Working group on goldstone boson production and decay

2008

This is the summary of the working group on Goldstone Boson Production and Decay of the Chiral Dynamics Workshop in Mainz, September 1–5, 1997. For the production aspects we discuss π0 and η production in nucleon-nucleon collisions and the behaviour of hadrons in various sum rules. For the decays we present a discussion on various K, η and π decay channels. Other aspects discussed are a new treatment of meson-meson scattering, the light-by-light contribution to the muon anomalous magnetic moment and progress in various aspects of the p 6 generating functional in the mesonic sector.

PhysicsParticle physicsMuonAnomalous magnetic dipole momentScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHadronForm factor (quantum field theory)Vector meson dominanceNuclear physicsGoldstone bosonBibliographyHigh Energy Physics::ExperimentNuclear Experiment
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The width of the omega meson in dense matter

2014

We obtain the width of the $\omega$ meson in dense nuclear matter by taking into account (i) the free decay of the $\omega$ into three pions, which is dominated by $\rho \pi$ mode, (ii) the processes induced by a vector-baryon interaction dominated by vector meson exchange, and (iii) the $\omega \to K \bar K$ mechanism in matter. The $\omega$ meson develops an important width in matter, coming from the dominant $\omega \to \rho\pi$ decay mode, with a value of $121 \pm 10$ MeV at normal nuclear matter density for an $\omega$ at rest. At finite momentum, the width of the $\omega$ meson increases moderately with values of 200 MeV at 600 MeV/c.

PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::PhenomenologyNuclear TheoryNuclear matter7. Clean energyOmegaMomentumHigh Energy Physics - PhenomenologyPionHigh Energy Physics::ExperimentVector mesonNuclear ExperimentNuclear ExperimentDense matterBar (unit)Proceedings of XV International Conference on Hadron Spectroscopy — PoS(Hadron 2013)
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THE X(3872) AND OTHER X,Y,Z RESONANCES AS HIDDEN CHARM MESON-MESON MOLECULES

2011

We report on some ideas concerning the nature of the X(3872) resonance and the need for approximately equal charged and neutral components of $D \bar{D}^* +cc$. Then we discuss how some hidden charm states are obtained from the interaction between vector mesons with charm and can be associated to some of the charmonium-like X,Y,Z states. Finally we discuss how the nature of these states could be investigated through different types of radiative decay.

PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::PhenomenologyRadiative decayFOS: Physical sciencesResonanceVector meson dominanceNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)MoleculeHigh Energy Physics::ExperimentCharm (quantum number)Nuclear theoryX(3872)International Journal of Modern Physics: Conference Series
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Exclusive radiative B-meson decays within the aligned two-Higgs-doublet model

2012

In the aligned two-Higgs-doublet model, the alignment of Yukawa matrices in flavour space guarantees the absence of tree-level flavour-changing neutral currents, while allowing at the same time for new sources of CP violation, implying potentially large effects in many low-energy processes. In this work we study the constraints from exclusive radiative $B\to V\gamma$ decays, where $V$ denotes a light vector meson. The current experimental data on the CP-averaged branching ratios and the direct CP and isospin asymmetries are analyzed. It is found that, while the branching ratios and direct CP asymmetries do not constrain the parameter space much further compared to the inclusive $B\to X_{s,d…

PhysicsParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::PhenomenologyYukawa potentialB-physics; Beyond standard model; CP violation; Higgs physics; High Energy Physics - Phenomenology; High Energy Physics - Phenomenology; Nuclear and High Energy PhysicsFOS: Physical sciencesFísicaObservableHiggs physicsParameter spaceB-physicsTwo-Higgs-doublet modelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationIsospinCP violationB mesonHigh Energy Physics::ExperimentVector mesonBeyond standard model
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