0000000000073885

AUTHOR

Adam P. Szczepaniak

showing 14 related works from this author

Dalitz plot analyses of J/ψ→π+π−π0 , J/ψ→K+K−π0 , and J/ψ→Ks0K±π∓ produced via e+e− annihilation with initial-state radiation

2017

We study the processes e^+e^− → γISR J/ψ, where J/ψ → π^+π^−π^0, J/ψ → K^+K^−π^0, and J/ψ → K^0_SK^±π^∓ using a data sample of 519 fb^(−1) recorded with the BABAR detector operating at the SLAC PEP-II asymmetric-energy e^+e^− collider at center-of-mass energies at and near the Υ(nS) (n=2,3,4) resonances. We measure the ratio of branching fractions R_1 = ^(B(J/ψ → K^+K^−π^0)) /_(B(J/ψ → π^+π^−π^0)) and R_2 = ^(B(J/ψ → K^0_SK^±π^∓))/_(B(J/ψ → π^+π^−π^0)). We perform Dalitz plot analyses of the three J/ψ decay modes and measure fractions for resonances contributing to the decays. We also analyze the J/ψ → π^+π^−π^0 decay using the Veneziano model. We observe structures compatible with the pres…

PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationHadronDalitz plot01 natural sciencesNuclear physicsParticle decay0103 physical sciences010306 general physicsDimensionless quantityPhysical Review D
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Determination of the pole position of the lightest hybrid meson candidate

2019

Mapping states with explicit gluonic degrees of freedom in the light sector is a challenge, and has led to controversies in the past. In particular, the experiments have reported two different hybrid candidates with spin-exotic signature, pi1(1400) and pi1(1600), which couple separately to eta pi and eta' pi. This picture is not compatible with recent Lattice QCD estimates for hybrid states, nor with most phenomenological models. We consider the recent partial wave analysis of the eta(') pi system by the COMPASS collaboration. We fit the extracted intensities and phases with a coupled-channel amplitude that enforces the unitarity and analyticity of the S-matrix. We provide a robust extracti…

Particle physicsFísica-Modelos matemáticosMesonPartial wave analysisLattice field theoryGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all); energy; meson photoproductionPhysics and Astronomy (all)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesFísica matemática010306 general physicsS-matrixPOMERONQuantum chromodynamicsPhysicsUnitarityRESTLattice QCDmeson photoproductionETA-PIMODELHigh Energy Physics - PhenomenologyPhysics and AstronomyEXOTICSSTATESWAVEPI(-)PSYSTEMenergy
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Double Polarization Observables in Pentaquark Photoproduction

2019

We investigate the properties of the hidden charm pentaquark-like resonances first observed by LHCb in 2015, by measuring the polarization transfer KLL between the incident photon and the outgoing proton in the exclusive photoproduction of J/psi near threshold. We present a first estimate of the sensitivity of this observable to the pentaquark photocouplings and hadronic branching ratios, and extend our predictions to the case of initial state helicity correlation ALL, using a polarized target. These results serve as a benchmark for the SBS experiment at Jefferson Lab, which proposes to measure for the first time the helicity correlations ALL and KLL in J/psi exclusive photoproduction, in o…

Particle physicsFísica-Modelos matemáticosPhotonHadronpentaquarksFOS: Physical sciences01 natural sciencesexotic hadronsHigh Energy Physics - ExperimentPolarized targetHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPhoton polarizationNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsexotic hadrons; pentaquarks; hadron spectroscopy010308 nuclear & particles physicshadron spectroscopyObservablePolarization (waves)HelicityPentaquarkHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Substructure of Multiquark Hadrons (Snowmass 2021 White Paper)

2022

In recent years there has been a rapidly growing body of experimental evidence for existence of exotic, multiquark hadrons, i.e. mesons which contain additional quarks, beyond the usual quark-antiquark pair and baryons which consist of more than three quarks. In all cases with robust evidence they contain at least one heavy quark Q=c or b, the majority including two heavy quarks. Two key theoretical questions have been triggered by these discoveries: (a) how are quarks organized inside these multiquark states -- as compact objects with all quarks within one confinement volume, interacting via color forces, perhaps with an important role played by diquarks, or as deuteron-like hadronic molec…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::Experimenthep-phParticle Physics - Phenomenology
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Issues and Opportunities in Exotic Hadrons

2016

The last few years have been witness to a proliferation of new results concerning heavy exotic hadrons. Experimentally, many new signals have been discovered that could be pointing towards the existence of tetraquarks, pentaquarks, and other exotic configurations of quarks and gluons. Theoretically, advances in lattice field theory techniques place us at the cusp of understanding complex coupled-channel phenomena, modelling grows more sophisticated, and effective field theories are being applied to an ever greater range of situations. It is thus an opportune time to evaluate the status of the field. In the following, a series of high priority experimental and theoretical issues concerning h…

Nuclear and High Energy PhysicsParticle physicsField (physics)Lattice field theoryhep-latFOS: Physical sciencesAtomic01 natural sciencesComputer Science::Digital Libraries530Particle and Plasma PhysicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclearddc:530010306 general physicsNuclear ExperimentInstrumentationPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Molecularhep-phAstronomy and AstrophysicsExotic hadronNuclear & Particles PhysicsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasmaHigh Energy Physics::Experiment
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Muonic-hydrogen Lamb shift: Dispersing the nucleon-excitation uncertainty with a finite-energy sum rule

2013

We assess the two-photon exchange contribution to the Lamb shift in muonic hydrogen with forward dispersion relations. The subtraction constant (T) over bar (0, Q(2)) that is necessary for a dispersive evaluation of the forward doubly virtual Compton amplitude, through a finite energy sum rule, is related to the fixed J = 0 pole generalized to the case of virtual photons. We evaluated this sum rule using excellent virtual photoabsorption data that are available. We find that the "proton polarizability correction" to the Lamb shift in muonic hydrogen is -(40 +/- 5) mu eV. We conclude that nucleon structure-dependent uncertainty by itself is unlikely to resolve the large (300 mu eV) discrepan…

PhysicsProtonFísicaVirtual particleAtomic and Molecular Physics and OpticsLamb shiftPolarizabilityDispersion relationPhysics::Atomic PhysicsSum rule in quantum mechanicsAtomic physicsNucleonExotic atomPhysical Review A
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Nucleon resonance contributions to unpolarised inclusive electron scattering

2019

The first CLAS12 experiments will provide high-precision data on inclusive electron scattering observables at a photon virtuality Q2 ranging from 0.05 to 12GeV2 and center-of-mass energies W up to 4 GeV. In view of this endeavor, we present the modeling of the resonant contributions to the inclusive electron scattering observables. As input, we use the existing CLAS electrocoupling results obtained from exclusive meson electroproduction data off protons, and evaluate for the first time the resonant contributions based on the experimental results on the nucleon resonance electroexcitation. The uncertainties are given by the data and duly propagated through a Monte Carlo approach. In this way…

PhysicsParticle physicsPhotondeep inelastic scattering; proton structureNuclear TheoryMeson010308 nuclear & particles physicsMonte Carlo methodNuclear TheoryFOS: Physical sciencesPartonObservable01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNucleonNuclear ExperimentNuclear theoryElectron scatteringproton structure
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Regge phenomenology of theN*andΔ*poles

2019

We use Regge phenomenology to study the structure of the poles of the ${N}^{*}$ and ${\mathrm{\ensuremath{\Delta}}}^{*}$ spectrum. We employ the available pole extractions from partial wave analysis of meson scattering and photoproduction data. We assess the importance of the imaginary part of the poles (widths) to obtain a consistent determination of the parameters of the Regge trajectory. We compare the several pole extractions and show how Regge phenomenology can be used to gain insight into the internal structure of baryons. We find that the majority of the states in the parent Regge trajectories are compatible with a mostly compact three-quark state picture.

PhysicsParticle physicsMeson010308 nuclear & particles physicsScatteringHigh Energy Physics::LatticePartial wave analysisHigh Energy Physics::PhenomenologyState (functional analysis)01 natural sciencesBaryonHadron spectroscopy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNucleonPhenomenology (particle physics)Physical Review D
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New analysis of ηπ tensor resonances measured at the COMPASS experiment

2018

We present a new amplitude analysis of the $\eta\pi$ $D$-wave in $\pi^- p\to \eta\pi^- p$ measured by COMPASS. Employing an analytical model based on the principles of the relativistic $S$-matrix, we find two resonances that can be identified with the $a_2(1320)$ and the excited $a_2^\prime(1700)$, and perform a comprehensive analysis of their pole positions. For the mass and width of the $a_2$ we find $M=(1307 \pm 1 \pm 6)$~MeV and $\Gamma=(112 \pm 1 \pm 8)$~MeV, and for the excited state $a_2^\prime$ we obtain $M=(1720 \pm 10 \pm 60)$~MeV and $\Gamma=(280\pm 10 \pm 70)$~MeV, respectively.

M012M311.80.EtCOMPASS01 natural sciencesHigh Energy Physics - ExperimentUNITARITYSubatomär fysikPomeronCompassexcited stateSubatomic PhysicsNuclear and high energy physics; peripheral photoproduction; physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]COMPASS experimentEXCHANGEa2(1320)Nuclear Experimenta2(1700)Quantum chromodynamicsPhysicsUnitarityPP INTERACTIONShep-phamplitude analysisMESONSlcsh:QC1-999analytic propertiesHigh Energy Physics - PhenomenologyAmplitudeS-matrixphysicsParticle Physics - ExperimentAMPLITUDE ANALYSISNuclear and High Energy PhysicsParticle physicsMeson530CONNECTIONPHYSICS14.40.Be[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]pomeron0103 physical sciencesperipheral photoproductionddc:530Tensor010306 general physicsM012W3Particle Physics - PhenomenologyPOMERONhep-ex010308 nuclear & particles physicsM162M11.55.Bq11.55.Fvmeson resonanceM162WPhysics and Astronomy450 GEV/C[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentMATRIXlcsh:PhysicsPhysics Letters B
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Structure of pion photoproduction amplitudes

2018

We derive and apply the finite energy sum rules to pion photoproduction. We evaluate the low energy part of the sum rules using several state-of-the-art models. We show how the differences in the low energy side of the sum rules might originate from different quantum number assignments of baryon resonances. We interpret the observed features in the low energy side of the sum rules with the expectation from Regge theory. Finally, we present a model, in terms of a Regge-pole expansion, that matches the sum rules and the high-energy observables.

Particle physicsStructure (category theory)FOS: Physical sciences01 natural sciencesPOLARIZED PHOTONSCHARGED PIONSPionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesT DISPERSION-RELATIONSPhysics and Astronomy (miscellaneous); high energy; pion photoproduction010306 general physicsCOMPTON-SCATTERINGPhysicsREGGE-POLES010308 nuclear & particles physicsObservablePI0 PHOTOPRODUCTIONQuantum numberBaryonRegge theoryHigh Energy Physics - PhenomenologyAmplitudeBARYON RESONANCESPhysics and AstronomyPI-0 PHOTOPRODUCTIONMESON PHOTOPRODUCTIONENERGY SUM-RULESEnergy (signal processing)
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Finite-energy sum rules in eta photoproduction off a nucleon

2016

The reaction ${\gamma}N \to {\eta}N$ is studied in the high-energy regime (with photon lab energies $E_{\gamma}^{\textrm{lab}} > 4$ GeV) using information from the resonance region through the use of finite-energy sum rules (FESR). We illustrate how analyticity allows one to map the t-dependence of the unknown Regge residue functions. We provide predictions for the energy dependence of the beam asymmetry at high energies.

Particle physicsPhotonmedia_common.quotation_subjectFOS: Physical sciences01 natural sciencesAsymmetryKINEMATIC SINGULARITIESphysics and astronomy (miscellaneous)High Energy Physics - Phenomenology (hep-ph)PION0103 physical sciencesSCATTERINGEXCHANGENuclear Experiment010306 general physicsmedia_commonPhysicsREGGE-POLES010308 nuclear & particles physics3. Good healthHigh Energy Physics - PhenomenologyPhysics and AstronomyHELICITY AMPLITUDESC =-1MESON PHOTOPRODUCTIONHigh Energy Physics::ExperimentFACTORIZATIONQUARK-MODELNucleonPhysical Review D
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Understanding the nature ofΛ(1405)through Regge physics

2016

It appears that there are two resonances with ${J}^{P}=1/{2}^{\ensuremath{-}}$ quantum numbers in the energy region near the $\mathrm{\ensuremath{\Lambda}}(1405)$ hyperon. The nature of these states is a topic of current debate. To provide further insight we use Regge phenomenology to access how these two resonances fit the established hyperon spectrum. We find that only one of these resonances is compatible with a three-quark state.

PhysicsParticle physics010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelHyperonLambdaQuantum number01 natural sciences0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhenomenology (particle physics)Nuclear theoryPhysical Review D
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Studying thePc(4450)resonance inJ/ψphotoproduction off protons

2016

A resonancelike structure, the ${P}_{c}(4450)$, has recently been observed in the $J/\ensuremath{\psi}p$ spectrum by the LHCb Collaboration. We discuss the feasibility of detecting this structure in $J/\ensuremath{\psi}$ photoproduction in the CLAS12 experiment at JLab. We present a first estimate of the upper limit for the branching ratio of the ${P}_{c}(4450)$ to $J/\ensuremath{\psi}p$. Our estimates, which take into account the experimental resolution effects, predict that it will be possible to observe a sizable cross section close to the $J/\ensuremath{\psi}$ production threshold and shed light on the ${P}_{c}(4450)$ resonance in the future photoproduction measurements.

Nuclear physicsPhysicsParticle physics010308 nuclear & particles physicsBranching fraction0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physics01 natural sciencesResonance (particle physics)Nuclear theoryPentaquarkPhysical Review D
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Three-body final state interaction in η→ 3π updated

2017

In view of the recent high-statistic KLOE data for the η→π+π−π0 decay, a new determination of the quark mass double ratio has been done. Our approach relies on a dispersive model that takes into account rescattering effects between three pions via subenergy unitarity. The latter is essential to reproduce the Dalitz plot distribution. A simultaneous description of the KLOE and WASA-at-COSY data is achieved in terms of just two real parameters. From a global fit, we determine Q=21.6±1.1. The predicted slope parameter for the neutral channel α=−0.025±0.004 is in reasonable agreement with the PDG average value.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsDalitz plotValue (computer science)State (functional analysis)01 natural scienceslcsh:QC1-999Nuclear physicsPionDistribution (mathematics)0103 physical sciences010306 general physicsDispersion (water waves)lcsh:PhysicsPhysics Letters B
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