Search results for "scalar meson"

showing 10 items of 61 documents

$${\bar{B}}^0$$ B ¯ 0 , $$B^{-}$$ B - and $${\bar{B}}^0_s$$ B ¯ s 0 decays into $$J/\psi $$ J / ψ and $$K {\bar{K}}$$ K K ¯ or $$\pi \eta $$ π η

2015

We study the $\bar B^0_s \to J/\psi K^+ K^-$, $\bar B^0 \to J/\psi K^+ K^-$, $B^- \to J/\psi K^0 K^-$, $\bar B^0 \to J/\psi \pi^0 \eta$ and $B^- \to J/\psi \pi^- \eta$ decays and compare their mass distributions with those obtained for the $\bar B^0_s \to J/\psi \pi^+ \pi^-$ and $\bar B^0 \to J/\psi \pi^+ \pi^-$. The approach followed consist in a factorization of the weak part and the hadronization part into a factor which is common to all the processes. Then what makes the reactions different are some trivial Cabibbo-Kobayashi-Maskawa matrix elements and the weight by which the different pairs of mesons appear in a primary step plus their final state interaction. These elements are part o…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::PhenomenologyState (functional analysis)HadronizationFactorizationPiHigh Energy Physics::ExperimentInvariant massScalar mesonEngineering (miscellaneous)Bar (unit)The European Physical Journal C
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Charm-beauty meson bound states from B(B*)D(D*) and B(B*)D¯(D¯*) interaction

2017

We evaluate the $s$-wave interaction of pseudoscalar and vector mesons with both charm and beauty to investigate the possible existence of molecular $BD$, ${B}^{*}D$, $B{D}^{*}$, ${B}^{*}{D}^{*}$, $B\overline{D}$, ${B}^{*}\overline{D}$, $B{\overline{D}}^{*}$, or ${B}^{*}{\overline{D}}^{*}$ meson states. The scattering amplitude is obtained implementing unitarity starting from a tree level potential accounting for the dominant vector meson exchange. The diagrams are evaluated using suitable extensions to the heavy flavor sector of the hidden gauge symmetry Lagrangians involving vector and pseudoscalar mesons, respecting heavy quark spin symmetry. We obtain bound states at energies above 7 Ge…

PhysicsParticle physicsUnitarityMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::Phenomenology01 natural sciencesPseudoscalar mesonTree (descriptive set theory)Isospin0103 physical sciencesBound stateHigh Energy Physics::ExperimentVector mesonExotic meson010306 general physicsPhysical Review D
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Unitary chiral dynamics in decays and the role of scalar mesons

2004

We make a theoretical study of the J/psi decays into omegapipi, phipipi, omegaK (K) over bar and phiK (K) over bar using the techniques of the chiral unitary approach stressing the important role of the scalar resonances dynamically generated through the final state interaction of the two pseudoscalar mesons. We also discuss the importance of new mechanisms with intermediate exchange of vector and axial-vector mesons and the role played by the OZI rule in the J/ psi phipipi vertex, quantifying its effects. The results nicely reproduce the experimental data for the invariant mass distributions in all the channels considered. (C) 2004 Elsevier B.V. All rights reserved.

PhysicsPseudoscalarNuclear and High Energy PhysicsParticle physicsOZI ruleMesonHigh Energy Physics::PhenomenologyMass spectrumHigh Energy Physics::ExperimentInvariant massScalar mesonUnitary stateVertex (geometry)Nuclear Physics A
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The low lying scalar resonances in the D0 decays into Ks0 and f0(500), f0(980), a0(980)

2015

Abstract The D 0 decay into K s 0 and a scalar resonance, f 0 ( 500 ) , f 0 ( 980 ) , a 0 ( 980 ) , are studied obtaining the scalar resonances from final state interaction of a pair of mesons produced in a first step in the D 0 decay into K s 0 and the pair of pseudoscalar mesons. This weak decay is very appropriate for this kind of study because it allows to produce the three resonances in the same decay in a process that is Cabibbo-allowed, hence the rates obtained are large compared to those of B ¯ 0 decays into J / ψ and a scalar meson that have at least one Cabibbo-suppressed vertex. Concretely the a 0 ( 980 ) production is Cabibbo-allowed here, while it cannot be seen in the B ¯ s 0 …

PhysicsPseudoscalarNuclear and High Energy PhysicsParticle physicsUnitarityMesonIsospinHigh Energy Physics::PhenomenologyResonanceHigh Energy Physics::ExperimentScalar mesonPseudoscalar mesonVertex (geometry)Physics Letters B
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Perturbative QCD study of Bs decays to a pseudoscalar meson and a tensor meson

2014

We study two-body hadronic B-s -> PT decays, with P(T) being a light pseudoscalar (tensor) meson, in the perturbative QCD approach. The CP-averaged branching ratios and the direct CP asymmetries of the Delta S = 0 modes are predicted, where Delta S is the difference between the strange numbers of final and initial states. We also define and calculate experimental observables for the Delta S = 1 modes under the B-s(0)-(B) over bar (0)(s) mixing, including CP averaged branching ratios, time-integrated CP asymmetries, and the CP observables C-f, D-f and S-f. Results are compared to the B-s -> PV ones in the literature, and to the B -> PT ones, which indicate considerable U-spin symmetry breaki…

PhysicsPseudoscalarNuclear physicsNuclear and High Energy PhysicsParticle physicsMesonHadronPerturbative QCDCP violationHigh Energy Physics::ExperimentObservableSymmetry breakingPseudoscalar mesonPhysics Letters B
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Search for γγ→ηb in e+e− collisions at LEP 2

2002

A search for the pseudoscalar meson eta_b is performed in two-photon interactions at LEP~2 with an integrated luminosity of 699 pb^-1 collected at e+e- centre-of-mass energies from 181 GeV to 209 GeV. One candidate event is found in the six-charged-particle final state and none in the four-charged-particle final state, in agreement with the total expected background of about one event. Upper limits of Gamma_gammagamma(eta_b) * BR(eta_b -> 4 charged particles) 6 charged particles) < 132 eV are obtained at 95% confidence level, which correspond to 95% confidence level upper limits of 9.0% and 25% on these branching ratios.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsQuarkonium01 natural sciencesPseudoscalar mesonConfidence intervalCharged particleNuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysics Letters B
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Including Tetraquark Operators in the Low-Lying Scalar Meson Sectors in Lattice QCD

2019

Lattice QCD allows us to probe the low-lying hadron spectrum in finite-volume using a basis of single- and multi-hadron interpolating operators. Here we examine the effect of including tetraquark operators on the spectrum in the scalar meson sectors containing the $K_0^*(700)$ ($\kappa$) and the $a_0(980)$ in $N_f = 2 + 1$ QCD, with $m_\pi \approx 230$ MeV. Preliminary results of additional finite-volume states found using tetraquark operators are shown, and possible implications of these states are discussed.

PhysicsQuantum chromodynamicsParticle physicsBasis (linear algebra)High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Spectrum (functional analysis)HadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDApproxHigh Energy Physics - LatticeTetraquarkHigh Energy Physics::ExperimentScalar meson
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Pseudoscalar transition form factors: (g − 2) of the muon, pseudoscalar decays into lepton pairs, and the η – η′ mixing

2015

We present our model-independent and data-driven method to describe pseudoscalar meson transition form factors in the space- and (low-energy) time-like regions. The method is general and conforms a toolkit applicable to any other form factor, of one and two variables, with the potential to include both high- and low-energy QCD constraints altogether. The method makes use of analyticity and unitary properties of form factors, it is simple, systematic and can be improved upon by including new data. In the present discussion, the method is used to show the impact of experimental data for precision calculations in the low-energy sector of the Standard Model. In particular, due to its relevance …

PhysicsQuantum chromodynamicsParticle physicsMuonNuclear TheoryAnomalous magnetic dipole moment010308 nuclear & particles physicsPhysics beyond the Standard ModelPhysicsQC1-999High Energy Physics::PhenomenologyForm factor (quantum field theory)01 natural sciencesPseudoscalar mesonHigh Energy Physics - ExperimentPseudoscalarHigh Energy Physics - Phenomenology0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonEPJ Web of Conferences
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Doubly charmed Ξcc molecular states from meson-baryon interaction

2018

Stimulated by the new experimental LHCb findings associated with the ${\mathrm{\ensuremath{\Omega}}}_{c}$ states, some of which we have described in a previous work as being dynamically generated through meson-baryon interaction, we have extended this approach to make predictions for new ${\mathrm{\ensuremath{\Xi}}}_{cc}$ molecular states in the $C=2$, $S=0$, and $I=1/2$ sector. These states manifest themselves as poles in the solution of the Bethe-Salpeter equation in coupled channels. The kernels of this equation were obtained using general Lagrangians coming from the hidden local gauge symmetry or massive Yang-Mills theory, and the interactions are dominated by the exchange of light vect…

PhysicsQuarkParticle physicsMeson010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::Phenomenology01 natural sciencesPseudoscalar mesonOmegaBaryonPseudoscalar0103 physical sciencesVector mesonNuclear Experiment010306 general physicsRealization (systems)Physical Review D
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On the ambiguities of sign determination of the S-matrix from energy levels in a finite box

2013

In a recent paper the authors make a study on the determination of the S-matrix elements for scattering of particles in the infinite volume from the energy levels in a finite box for the case of multiple channels. The study is done with a toy model in 1+1 dimension and the authors find that there is some ambiguity in the sign of nondiagonal matrix elements, casting doubts on whether the needed observables in the infinite volume can be obtained from the energy levels of the box. In this paper I present an easy derivation, confirming the ambiguity of the sign and argue that this, however, does not put restrictions in the determination of observables.

PhysicsStatesNuclear and High Energy PhysicsToy modelVolumemedia_common.quotation_subjectHigh Energy Physics - Lattice (hep-lat)One-dimensional spaceFísicaFOS: Physical sciencesLattice QCDObservableAmbiguityHigh Energy Physics - PhenomenologyScalar MesonsMatrix (mathematics)Theoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Energy (signal processing)media_commonS-matrixSign (mathematics)The European Physical Journal A
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