Search results for "Pseudoscalar meson"

showing 10 items of 40 documents

The role of resonances in chiral perturbation theory

1989

32 páginas, 2 figuras, 5 tablas.-- BUTP-88-18 ; CERN-TH-5185-88 ; CPT-2158 ; UWTHPH-1988-29.

Chiral anomalyPhysicsNuclear and High Energy PhysicsChiral perturbation theoryMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFísicaVector meson dominancePseudoscalar mesonPionQuantum electrodynamicsNambu–Jona-Lasinio modelHigh Energy Physics::ExperimentChiral symmetry breakingParticle Physics - Theory
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Three pseudoscalar meson production ine+e−annihilation

2013

Conversations with German Rodrigo on the topic of this paper are warmly acknowledged. We would like to thank Henryk Czyz for fruitful discussions on context of MC PHOKHARA 7.0. We also wish to thank Michael R. Pennington for a careful reading of our manuscript and for his suggestions. Lingyun Dai thanks the China Scholarship Council for their support. This research has been supported in part by the funds of the Polish National Science Centre under decisions DEC-2012/04/M/ST2/00240 and DEC-2011/03/B/ST2/00107 (O. S.) and by the Spanish Government and ERDF funds from the EU Commission [Grants No. FPA2007-60323, No. FPA2011-23778, No. CSD2007-00042 (Consolider Project CPAN)]. This paper has be…

GermanPhysicsNuclear and High Energy PhysicsScholarshipGovernmentParticle physicsEffective lagrangianlanguageLibrary scienceContext (language use)CommissionPseudoscalar mesonlanguage.human_languagePhysical Review D
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Searches for B0 decays to combinations of charmless isoscalar mesons

2004

We search for B meson decays into two-body combinations of eta, eta', omega, and phi mesons from 89 million B B-bar pairs collected with the BaBar detector at the PEP-II asymmetric-energy e+e- collider at SLAC. We find the branching fraction BF(B0 -> eta omega) = (4.0^{+1.3}_{-1.2} +- 0.4) x 10^-6 with a significance of 4.3 sigma. For all the other decay modes we set the following 90% confidence level upper limits on the branching fractions, in units of 10^-6 : BF(B0 -> eta eta)<2.8, BF(B0 -> eta eta')<4.6, BF(B0 -> eta' eta')<10, BF(B0 -> eta'omega)<2.8, BF(B0 -> eta phi)<1.0, BF(B0 -> eta' phi)<4.5, BF(B0 -> phi phi)<1.5.

IsoscalarElectron–positron annihilationBABARGeneral Physics and AstronomyQCD FACTORIZATION01 natural sciencesOmega13.25.Hw 11.30.Er 12.15.HhHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Mathematical modelProbability density function[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PEP2B mesonNuclear ExperimentQCD FACTORIZATION; STANDARD MODEL; BABAR; SLACPhysicsQuantum chromodynamicsSigmaHamiltonianMonte Carlo methodSensitivity analysiPARTICLE PHYSICSBranching fractionSLACParticle physicsMesonSTANDARD MODELQCD FACTORIZATION STANDARD MODELFOS: Physical sciencesLikelihood distributionPARTICLE PHYSICS; PEP2; BABARSolenoidHigh energy physicNuclear physicsPhysics and Astronomy (all)ElectromagnetismElectromagnetic calorimeterPseudoscalar meson0103 physical sciencesPerturbation technique010306 general physicsCalorimeterError analysi010308 nuclear & particles physicsBranching fractionHEPMagnetic fieldHigh Energy Physics::Experiment
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Measurement of branching fractions for D meson decaying into $ϕ$ meson and a pseudoscalar meson

2019

The four decay modes D0→ϕπ0, D0→ϕη, D+→ϕπ+, and D+→ϕK+ are studied by using a data sample taken at the centre-of-mass energy s=3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of 2.93 fb$^{−1}$. The branching fractions of the first three decay modes are measured to be B(D0→ϕπ0)=(1.168±0.028±0.028)×10−3, B(D0→ϕη)=(1.81±0.46±0.06)×10−4, and B(D+→ϕπ+)=(5.70±0.05±0.13)×10−3, respectively, where the first uncertainties are statistical and the second are systematic. In addition, the upper limit of the branching fraction for D+→ϕK+ is given to be 2.1×10−5 at the 90% confidence level. The ratio of B(D0→ϕπ0) to B(D+→ϕπ+) is calculated to be (20.49±0.50±0.45)%, which is c…

Nuclear and High Energy PhysicsBESIII; Branching fractions; D meson; Hadronic decaysMesonAstrophysics::High Energy Astrophysical PhenomenaBESIII; Branching fractions; D meson; Hadronic decays; High Energy Physics - Experiment; High Energy Physics - ExperimentBranching (polymer chemistry)01 natural sciencesPseudoscalar mesonNOHigh Energy Physics - ExperimentSubatomär fysikHadronic decaysD Meson0103 physical sciencesD mesonSubatomic PhysicsHadronic DecaysBranching fractionsddc:530010306 general physicsAstrophysics::Galaxy AstrophysicsPhysics010308 nuclear & particles physicsBranching fractionBESIIIBranching Fractionslcsh:QC1-999D mesonIsospinHigh Energy Physics::ExperimentAtomic physicslcsh:Physics
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Effective Majorana mass matrix from tau and pseudoscalar meson lepton number violating decays

2018

An observation of any lepton number violating process will undoubtedly point towards the existence of new physics and indirectly to the clear Majorana nature of the exchanged fermion. In this work, we explore the potential of a minimal extension of the Standard Model via heavy sterile fermions with masses in the $[ 0.1 - 10]$ GeV range concerning an extensive array of "neutrinoless" meson and tau decay processes. We assume that the Majorana neutrinos are produced on-shell, and focus on three-body decays. We conduct an update on the bounds on the active-sterile mixing elements, $|U_{\ell_\alpha 4} U_{\ell_\beta 4}|$, taking into account the most recent experimental bounds (and constraints) a…

Particle physicsNuclear and High Energy PhysicsMesonPhysics beyond the Standard ModelFOS: Physical sciences7. Clean energy01 natural sciencesPseudoscalar mesonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)double-beta decay: (0neutrino)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino Physics010306 general physicsnumerical calculationslepton number: violationPhysicsneutrino: heavy: decay010308 nuclear & particles physicsnew physicsHigh Energy Physics::Phenomenologyneutrino: Majorana: massFermionneutrino: sterileMass matrixsensitivityLepton numberMAJORANAHigh Energy Physics - Phenomenologypseudoscalar meson: decay[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard Modellcsh:QC770-798neutrino: Majorana[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimenttau: decayNeutrinoneutrino: mixing
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Masses and decay constants of D(s)* and B(s)* mesons with Nf=2+1+1 twisted mass fermions

2017

We present a lattice calculation of the masses and decay constants of ${D}_{(s)}^{*}$ and ${B}_{(s)}^{*}$ mesons using the gauge configurations produced by the European Twisted Mass Collaboration (ETMC) with ${N}_{f}=2+1+1$ dynamical quarks at three values of the lattice spacing $a\ensuremath{\sim}(0.06\ensuremath{-}0.09)\text{ }\text{ }\mathrm{fm}$. Pion masses are simulated in the range ${M}_{\ensuremath{\pi}}\ensuremath{\simeq}(210--450)\text{ }\text{ }\mathrm{MeV}$, while the strange and charm sea-quark masses are close to their physical values. We compute the ratios of vector to pseudoscalar masses and decay constants for various values of the heavy-quark mass ${m}_{h}$ in the range $0…

PhysicsMeson010308 nuclear & particles physicsFermion01 natural sciencesPseudoscalar mesonPseudoscalarCrystallographyLattice constantPionLattice (order)0103 physical sciencesHeavy quark effective theoryStatistical physics010306 general physicsPhysical Review D
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Phenomenological applications of rational approximants

2016

We illustrate the powerfulness of Padé approximants (PAs) as a summation method and explore one of their extensions, the so-called quadratic approximant (QAs), to access both space- and (low-energy) time-like (TL) regions. As an introductory and pedagogical exercise, the function [Formula: see text] is approximated by both kind of approximants. Then, PAs are applied to predict pseudoscalar meson Dalitz decays and to extract [Formula: see text] from the semileptonic [Formula: see text] decays. Finally, the [Formula: see text] vector form factor in the TL region is explored using QAs.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsForm factor (quantum field theory)General Physics and AstronomyAstronomy and AstrophysicsVector meson dominanceFunction (mathematics)Space (mathematics)01 natural sciencesPseudoscalar mesonQuadratic equationQuantum electrodynamics0103 physical sciencesPadé approximantHigh Energy Physics::Experiment010306 general physicsMathematical physicsModern Physics Letters A
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X(2175)as a resonant state of theϕKK¯system

2008

We perform a Faddeev calculation for the three-meson system $\ensuremath{\phi}K\overline{K}$, taking the interaction between two pseudoscalar mesons and between a vector and a pseudoscalar meson from the chiral unitary approach. We obtain a neat resonance peak around a total mass of 2150 MeV and an invariant mass for the $K\overline{K}$ system around 970 MeV, very close to the ${f}_{0}(980)$ mass. The state appears in $I=0$ and qualifies as a $\ensuremath{\phi}{f}_{0}(980)$ resonance. We enlarge the space of states including $\ensuremath{\phi}\ensuremath{\pi}\ensuremath{\pi}$, since $\ensuremath{\pi}\ensuremath{\pi}$ and $K\overline{K}$ build up the ${f}_{0}(980)$, and find moderate changes…

PhysicsNuclear and High Energy PhysicsFaddeev equationsParticle physicsMeson010308 nuclear & particles physicsState (functional analysis)16. Peace & justice01 natural sciencesPseudoscalar mesonResonance (particle physics)PseudoscalarParticle decay0103 physical sciencesInvariant mass010306 general physicsPhysical Review D
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Case in favor of theN*(1700)(3/2−)

2013

Using an interaction extracted from the local hidden-gauge Lagrangians, which brings together vector and pseudoscalar mesons, and the coupled channels rho N (s wave), pi N (d wave), pi Delta (s wave), and pi Delta (d wave), we look in the region ofv root s = 1400-1850 MeV and find two resonances dynamically generated by the interaction of these channels, which are naturally associated to N*(1520)(3/2(-)) and N*(1700)(3/2(-)). N*(1700)(3/2(-)) appears neatly as a pole in the complex plane. The free parameters of the theory are chosen to fit the pi N (d-wave) data. Both the real and imaginary parts of the pi N amplitude vanish in our approach in the vicinity of this resonance, which is simila…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsPartial wave analysisResonanceVector meson dominance01 natural sciencesPseudoscalar mesonPseudoscalarAmplitudeQuantum electrodynamics0103 physical sciences010306 general physicsScalar mesonMathematical physicsPhysical Review C
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Search for newπ0-like particles produced in association with aτ-lepton pair

2014

We report on a search in e^+e^− annihilations for new π^0-like particles produced in association with a τ-lepton pair. These objects, with a similar mass and similar decay modes to π^0 mesons, could provide an explanation for the non-asymptotic behavior of the pion-photon transition form factor observed by the BABAR Collaboration. No significant signal is observed, and limits on the production cross section at the level of 73 fb or 370 fb, depending on the model parameters, are determined at 90% confidence level. These upper limits lie below the cross section values needed to explain the BABAR form factor data.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsAssociation (object-oriented programming)Monte Carlo methodForm factor (quantum field theory)01 natural sciencesPseudoscalar mesonNuclear physicsCross section (physics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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