Search results for "Vector"

showing 10 items of 2660 documents

Effects of aNcc¯*resonance with hidden charm in theπ−p→D−Σc+reaction near threshold

2015

We study the effect of a hidden charm nuclear excited state ${N}_{c\overline{c}}^{*}$ in the ${\ensuremath{\pi}}^{\ensuremath{-}}p\ensuremath{\rightarrow}{D}^{\ensuremath{-}}{\mathrm{\ensuremath{\Sigma}}}_{c}^{+}$ reaction near threshold using an effective Lagrangian approach. We calculate the background contribution of the $t$ and $u$ channels by the ${D}^{*0}$ vector meson exchange and ${\mathrm{\ensuremath{\Sigma}}}_{c}^{++}$ intermediate state, respectively. We show that the consideration of a ${N}_{c\overline{c}}^{*}$ resonance provides an enhancement of the total cross section close to the reaction threshold. We also evaluate the differential cross section for different energies and w…

PhysicsNuclear and High Energy PhysicsNear thresholdExcited stateHigh Energy Physics::PhenomenologyEffective lagrangianIntermediate stateVector meson dominanceVector mesonCharm (quantum number)Atomic physicsResonance (particle physics)Physical Review C
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Kaonic production of $ \Lambda$ (1405) off deuteron target in chiral dynamics

2009

The K^- induced production of Lambda(1405) is investigated in K^- d to pi Sigma n reactions based on coupled-channels chiral dynamics, in order to discuss the resonance position of the Lambda(1405) in the KbarN channel. We find that the K^-d to Lambda(1405)n process favors the production of Lambda(1405) initiated by the KbarN channel. The present approach indicates that the Lambda(1405) resonance position is 1420 MeV rather than 1405 MeV in the pi Sigma invariant mass spectra of K- d to pi Sigma n reactions. This is consistent with an observed spectrum of the K^- d to pi^+ Sigma^- n with 686-844 MeV/c incident K^- by bubble chamber experiments done in the 70's. Our model also reproduces the…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsFOS: Physical sciencesFísicaSigmaLambda7. Clean energy01 natural sciencesResonance (particle physics)Spectral lineNuclear Theory (nucl-th)Nuclear physicsDeuteriumPosition (vector)0103 physical sciencesBubble chamberInvariant mass010306 general physicsThe European Physical Journal A
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The generalized Gerasimov–Drell–Hearn sum rule for deuteron electrodisintegration

2004

The generalized Gerasimov-Drell-Hearn sum rule $I^{GDH}_{\gamma^*d}(Q^2)$ for deuteron electrodisintegration $d(e,e')np$ as function of the squared four-momentum transfer $Q^2$ is evaluated by explicit integration. The calculation is based on a conventional nonrelativistic framework using a realistic $NN$-potential and including contributions from meson exchange currents, isobar configurations and leading order relativistic terms. Good convergence is achieved. The prominent feature is a deep negative minimum, $I_{\gamma^* d}^{GDH}=-9.5$ mb, at low $Q^2\approx 0.2$ fm$^{-2}$ which is almost exclusively driven by the nucleon isovector anomalous magnetic moment contribution to the magnetic dip…

PhysicsNuclear and High Energy PhysicsNuclear TheoryAnomalous magnetic dipole momentMesonIsovectorMagnetic dipole transitionMomentum transferFOS: Physical sciencesNuclear Theory (nucl-th)Nuclear physicsIsobarSum rule in quantum mechanicsNucleonPhysics Letters B
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Linear response of light deformed nuclei investigated by self-consistent quasiparticle random-phase approximation

2010

We present a calculation of the properties of vibrational states in deformed, axially-symmetric even-even nuclei, within the framework of a fully self-consistent quasiparticle random phase approximation (QRPA). The same Skyrme energy density and density-dependent pairing functionals are used to calculate the mean field and the residual interaction in the particle-hole and particle-particle channels. We have tested our software in the case of spherical nuclei against fully self-consistent calculations published in the literature, finding excellent agreement. We investigate the consequences of neglecting the spin-orbit and Coulomb residual interactions in QRPA. Furthermore we discuss the impr…

PhysicsNuclear and High Energy PhysicsNuclear TheoryIsovectorIsoscalarNuclear TheoryFOS: Physical sciencesNuclear Theory (nucl-th)Mean field theoryQuantum mechanicsPairingQuasiparticleCoulombAtomic physicsSpin (physics)Random phase approximationPhysical Review C
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Energy and system size dependence of subnucleonic fluctuations

2018

The energy evolution of the fluctuating proton structure is studied by solving the JIMWLK renormalization group equation. The initial condition at moderate $x$ is obtained by fitting the charm reduced cross section data from HERA, requiring that the proton size remains compatible with the diffractive vector meson production measurements. Additionally, we show that the nucleon shape fluctuations are visible in exclusive vector meson production off nuclei.

PhysicsNuclear and High Energy PhysicsNuclear Theoryta114Proton010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryHERARenormalization group01 natural sciencesNuclear physicsHigh Energy Physics - Phenomenology0103 physical sciencessubnucleonic fluctuationsInitial value problemHigh Energy Physics::ExperimentVector mesonCharm (quantum number)010306 general physicsNucleonNuclear ExperimentydinfysiikkaEnergy (signal processing)
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Die relative Isotopenlage des Os186

1962

Using three different samples of Os192, Os190 and Os186 enriched to 98.68%, 95.46%, and 61.27%, respectively, the isotopic shiftsΔν(Os192−Os190) andΔν(Os192−Os186) have been measured in four Os I-lines with a recording Fabry-Perot spectrometer. The relative isotopic position of Os186 has been found to be $$\frac{{\Delta \nu (Os^{192} - Os^{186} )}}{{\Delta \nu (Os^{192} - Os^{190} )}} = 3.52 \pm 0.03.$$

PhysicsNuclear and High Energy PhysicsNuclear magnetic resonanceSpectrometerPosition (vector)Analytical chemistryNuclear fusionSpectral shiftZeitschrift f�r Physik
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Measurement of the branching fractions of the rare decaysB0→Ds(*)+π−,B0→Ds(*)+ρ−, andB0→Ds(*)−K(*)+

2008

The authors report the measurement of the branching fractions of the rare decays B{sup 0} {yields} D{sub s}{sup (*)+} {pi}{sup -}, B{sup 0} {yields} D{sub s}{sup (*)+} {rho}{sup -}, and B{sup 0} {yields} D{sub s}{sup (*)-} K{sup (*)+} in a sample of 381 x 10{sup 6} {Upsilon}(4S) decays into B{bar B} pairs collected with the BABAR detector at the PEP-II asymmetric-energy e{sup +}e{sup -} storage ring. They present evidence for the decay B{sup 0} {yields} D{sub s}{sup -} K*{sup +} and the vector-vector decays B{sup 0} {yields} D{sub s}{sup *+} {rho}{sup -} and B{sup 0} {yields} D{sub s}{sup *-} K{sup *+}, as well as the first measurement of the vector meson polarization in these decays. They …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationBranching (polymer chemistry)01 natural sciencesCrystallographyParticle decayTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesVector meson010306 general physicsPhysical Review D
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Lepton-flavour violation in hadronic tau decays and μ-τ conversion in nuclei

2021

Within the Standard Model Effective Field Theory framework, with operators up to dimension 6, we perform a model-independent analysis of the lepton-flavour-violating processes involving tau leptons. Namely, we study hadronic tau decays and $\ell$--$\tau$ conversion in nuclei, with $\ell = e,\mu$. Based on available experimental limits, we establish constraints on the Wilson coefficients of the operators contributing to these processes. Our work paves the way to extract the related information from Belle II and foreseen future experiments.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsFlavourHadronHigh Energy Physics::PhenomenologyEffective Field Theories01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyDimension (vector space)Beyond Standard Model0103 physical sciencesEffective field theorylcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsLepton
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Low-mass vector-meson production at forward rapidity inp+pcollisions ats=200  GeV

2014

The PHENIX experiment at the Relativistic Heavy Ion Collider has measured low-mass vector-meson ,omega, rho, and phi, production through the dimuon decay channel at forward rapidity (1.2 mu mu) = 80 +/- 6(stat) +/- 12(syst)nb and d sigma/dy(phi -> mu mu) = 27 +/- 3(stat) +/- 4(syst)nb. These results are compared with midrapidity measurements and calculations.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsNuclear TheorySigma7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)RapidityVector mesonNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderLow MassPhysical Review D
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Measurement of in oscillation using quantum correlations in at

2015

We report a measurement of the parameter y(CP) in D-0-(D) over bar (0) oscillations performed by taking advantage of quantum coherence between pairs of D-0(D) over bar (0) mesons produced in e(+)e(-) annihilations near threshold. In this work, doubly-tagged D-0(D) over bar (0) events, where one D decays to a CP eigenstate and the other D decays in a semileptonic mode, are reconstructed using a data sample of 2.92 fb(-1) collected with the BESIII detector at the center-of-mass energy of root s = 3.773 GeV. We obtain y(CP) = (-2.0 +/- 1.3 +/- 0.7)%, where the first uncertainty is statistical and the second is systematic. This result is compatible with the current world average.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsOscillationQuantum correlation01 natural sciencesNuclear physicsPion0103 physical sciencesCP violationCoherence (signal processing)High Energy Physics::Experiment010306 general physicsEigenvalues and eigenvectors
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