0000000000315838

AUTHOR

Paweł Moskal

showing 13 related works from this author

Observation of the rare η→e+e−e+e− decay with the KLOE experiment

2011

Abstract We report the first observation of the rare η → e + e − e + e − ( γ ) decay based on 1.7 fb − 1 collected by the KLOE experiment at the DAΦNE ϕ-factory. The selection of the e + e − e + e − final state is fully inclusive of radiation. We have identified 362 ± 29 events resulting in a branching ratio of ( 2.4 ± 0.2 stat + bckg ± 0.1 syst ) × 10 − 5 .

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilation0103 physical sciencesRadiation010306 general physics01 natural sciencesPhysics Letters B
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Drift chamber calibration and particle identification in the P-349 experiment

2019

The goal of the P-349 experiment is to test whether 3.5 GeV/c antiprotons produced in high-energy proton-proton collisions are polarized in view of the preparation of a polarized antiproton beam. In this article, we present the details of the ongoing analysis focused on the drift chambers calibration and particle identification with DIRC.

Physics010308 nuclear & particles physicsPhysicsQC1-99901 natural sciencesParticle identificationNuclear physicsSubatomär fysikAntiproton beamAntiproton0103 physical sciencesSubatomic PhysicsCalibrationPhysics::Accelerator PhysicsHigh Energy Physics::Experimentddc:530Detectors and Experimental Techniques010306 general physicsNuclear Experiment
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Feasibility study for the measurement of πN transition distribution amplitudes at P¯ANDA in p¯p→J/ψπ0

2017

The exclusive charmonium production process in (P) over barp annihilation with an associated pi 0 meson (p) over barp -> J/psi pi(0) is studied in the framework of QCD collinear factorization. The feasibility of measuring this reaction through the J/psi -> e(+) e(-) decay channel with the AntiProton ANnihilation at DArmstadt ((P) over bar ANDA) experiment is investigated. Simulations on signal reconstruction efficiency as well as the background rejection from various sources including the (P) over barp -> pi(+)pi(-)pi(0) and (p) over barp -> J/psi pi(0)pi(0) reactions are performed with PANDAROOT, the simulation and analysis software framework of the (P) over bar ANDA experiment. It is show…

Quantum chromodynamicsPhysicsParticle physicsLuminosity (scattering theory)AnnihilationMeson010308 nuclear & particles physics7. Clean energy01 natural sciencesParticle identificationNuclear physicsFactorizationAntiproton0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsBar (unit)Physical Review D
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Polarization analysis of $\bar{p}$ produced in pA collisions

2019

A quite simple procedure for the generation of a polarized antiproton beam could be worked out if antiprotons are produced with some polarization. In order to investigate this possibility measurements of the polarization of produced antiprotons have been started at a CERN/PS test beam. The polarization will be determined from the asymmetry of the elastic antiproton scattering at a liquid hydrogen target in the CNI region for which the analyzing power is well known. The data are under analysis and an additional measurement is done in 2018. Details on the experiment and the ongoing data analysis will be given.

PhysicsAntiparticle010308 nuclear & particles physicsPhysicsQC1-999Polarization (waves)01 natural sciences7. Clean energyNuclear physicsAntiproton beamAntiproton0103 physical sciencesPhysics::Accelerator Physicsddc:530High Energy Physics::ExperimentPhysics::Atomic Physics010306 general physicsAntihydrogenNuclear Experiment
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Cross section ratio and angular distributions of the reaction p + d -> 3He + eta at 48.8 MeV and 59.8 MeV excess energy

2014

We present new data for angular distributions and on the cross section ratio of the p + d -> 3He + eta reaction at excess energies of Q = 48.8 MeV and Q = 59.8 MeV. The data have been obtained at the WASA-at-COSY experiment (Forschungszentrum J\"ulich) using a proton beam and a deuterium pellet target. While the shape of obtained angular distributions show only a slow variation with the energy, the new results indicate a distinct and unexpected total cross section fluctuation between Q = 20 MeV and Q = 60 MeV, which might indicate the variation of the production mechanism within this energy interval.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryIntermediate EnergiesEta01 natural sciences7. Clean energyNuclear physicsCross section (physics)Tensor Analyzing PowerDeuteriumNear-Threshold0103 physical sciencesEnergy intervalPhysics::Accelerator Physicsddc:530010306 general physicsNuclear ExperimentExcess energyNuclear ExperimentBeam (structure)
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Search for polarization effects in the antiproton production process

2015

For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be produced polarized which will be checked experimentally. The polarization of antiprotons produced under typical conditions for antiproton beam preparation will be measured at the CERN/PS. If the production process creates some polarization a polarized antiproton beam could be prepared by a rather simple modification of the antiproton beam facility. The detection setup and the expected experimental conditions are described. For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be …

PhysicsLarge Hadron ColliderPhysics - Instrumentation and DetectorsFOS: Physical sciencesGeneral Physics and AstronomyParticle acceleratorInstrumentation and Detectors (physics.ins-det)Polarization (waves)law.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Antiproton beamAntiprotonlawPhysics::Accelerator Physicsddc:530High Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Detectors and Experimental TechniquesNuclear ExperimentNuclear Experiment
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Determination of the ηHe3 threshold structure from the low energy pd→ηHe3 reaction

2017

We analyze the data on cross sections and asymmetries for the $pd\ensuremath{\rightarrow}\ensuremath{\eta}\phantom{\rule{0.16em}{0ex}}^{3}\mathrm{He}$ reaction close to threshold and look for bound states of the $\ensuremath{\eta}\phantom{\rule{0.16em}{0ex}}^{3}\mathrm{He}$ system. Rather than parameterizing the scattering matrix, as is usually done, we develop a framework in which the $\ensuremath{\eta}{\phantom{\rule{0.16em}{0ex}}}^{3}\mathrm{He}$ optical potential is the key ingredient, and its strength, together with some production parameters, are fitted to the available experimental data. The relationship of the scattering matrix to the optical potential is established using the Bethe…

PhysicsParticle physicsBethe–Salpeter equation010308 nuclear & particles physicsScatteringScattering length01 natural sciencesLoop (topology)Matrix (mathematics)0103 physical sciencesBound stateProduction (computer science)Atomic physics010306 general physicsS-matrixPhysical Review C
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Spin dependence of {\eta} meson production in proton-proton collisions close to threshold

2018

Taking advantage of the high acceptance and axial symmetry of the WASA-at-COSY detector, and the high degree of the polarized proton beam of COSY, the reaction pp{\to} pp{\eta} has been measured close to threshold to explore the analyzing power Ay. The angular distribution of Ay is determined with the precision improved by more than one order of magnitude with respect to previous results allowing a first accurate comparison with theoretical predictions. The determined analyzing power is consistent with zero for an excess energy of Q = 15 MeV signaling s wave production with no evidence for higher partial waves. At Q = 72 MeV the data reveals strong interference of P s and P p partial waves …

Nuclear TheoryGeneral Physics and Astronomy01 natural sciencesHigh Energy Physics - ExperimentNuclear physics0103 physical sciencesddc:530FACILITYNEAR-THRESHOLD010306 general physicsNUCLEONNuclear ExperimentNuclear theoryNuclear ExperimentPhysicsQUASI-FREE010308 nuclear & particles physicsEta mesonDetectorCOSYPolarization (waves)Near thresholdHigh Energy Physics - PhenomenologyPhysics::Accelerator PhysicsAxial symmetryNucleon
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Physics with the KLOE-2 experiment at the upgraded DAFNE

2010

Investigation at a $\phi$--factory can shed light on several debated issues in particle physics. We discuss: i) recent theoretical development and experimental progress in kaon physics relevant for the Standard Model tests in the flavor sector, ii) the sensitivity we can reach in probing CPT and Quantum Mechanics from time evolution of entangled kaon states, iii) the interest for improving on the present measurements of non-leptonic and radiative decays of kaons and eta/eta$^\prime$ mesons, iv) the contribution to understand the nature of light scalar mesons, and v) the opportunity to search for narrow di-lepton resonances suggested by recent models proposing a hidden dark-matter sector. We…

Particle physicsField theory (Physics)MesonPhysics and Astronomy (miscellaneous)Scalar (mathematics)HadronContinuum (design consultancy)01 natural sciencesPartícules (Física nuclear)Standard ModelGamma gammaHigh Energy Physics - Experiment0103 physical sciencesRadiative transferMesons (Nuclear physics)Teoria quànticaMesons (Física nuclear)010306 general physicsEngineering (miscellaneous); Physics and Astronomy (miscellaneous)Nuclear ExperimentEngineering (miscellaneous)Particles (Nuclear physics)PhysicsQuantum Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTime evolutionTeoria de camps (Física)FísicaKaons3. Good healthHigh Energy Physics - PhenomenologyQuantum theoryHigh Energy Physics::Experiment
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Determination of theη′-Proton Scattering Length in Free Space

2014

Taking advantage of both the high mass resolution of the COSY-11 detector and the high energy resolution of the low-emittance proton beam of the cooler synchrotron COSY, we determine the excitation function for the $pp\ensuremath{\rightarrow}pp{\ensuremath{\eta}}^{\ensuremath{'}}$ reaction close to threshold. Combining these data with previous results, we extract the scattering length for the ${\ensuremath{\eta}}^{\ensuremath{'}}$-proton potential in free space to be $\mathrm{Re}({a}_{p{\ensuremath{\eta}}^{\ensuremath{'}}})=0\ifmmode\pm\else\textpm\fi{}0.43\text{ }\text{ }\mathrm{fm}$ and $\mathrm{Im}({a}_{p{\ensuremath{\eta}}^{\ensuremath{'}}})={0.37}_{\ensuremath{-}0.16}^{+0.40}\text{ }\t…

Excitation functionPhysicsParticle physicsMeson productionProton010308 nuclear & particles physicsGeneral Physics and AstronomyScattering lengthFree space01 natural sciencesProton scattering0103 physical sciencesHigh massHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsHigh energy resolutionPhysical Review Letters
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Status of the analysis for the search of polarization in the antiproton production process

2016

The P-349 experiment aims to test whether for antiprotons the production process itself can be a source of polarization in view of the preparation of a polarized antiproton beam. In this article we present the details of performed measurements and report on the status of the ongoing analysis.

PhysicsAntiparticle010308 nuclear & particles physicsPhysicsQC1-999Polarization (waves)01 natural sciencesEngineering physicsNuclear physicsSubatomär fysikAntiproton beamAntiprotonAntimatter0103 physical sciencesSubatomic PhysicsPhysics::Accelerator PhysicsNuclear Physics - Experimentddc:530010306 general physicsEPJ Web of Conferences
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Physics with Antiprotons at the Future GSI Facility

2003

Recently GSI presented the plans for a major new international research facility (http://www.gsi.de/GSI-future/). Highly luminous secondary beams with excellent quality encompassing the production of antiprotons will be delivered. In a High Energy Storage Ring (HESR) with a bending power of 50 Tm antiprotons will be cooled either stochastically or by electrons. The envisaged limits are a momentum range of 1.5 to 15 GeV/c and a luminosity of 2 × 1032 cm-2 s-1. Four major physical research goals can be addressed: high precision charmonium spectroscopy, medium effects of open and hidden charm, the search for glueballs and hybrids, and the production of hypernuclei.

MomentumPhysicsNuclear physicsInternational researchLuminosity (scattering theory)AntiprotonElectronCharm (quantum number)Condensed Matter PhysicsMathematical PhysicsAtomic and Molecular Physics and OpticsPhysica Scripta
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A new limit on the CP violating decay KS→3π0 with the KLOE experiment

2013

We have carried out a new direct search for the CP violating decay K-S -> 3 pi(0) with 1.7 fb(-1) of e(+)e(-) collisions collected by the KLOE detector at the Phi-factory DA Phi NE. We have searched for this decay in a sample of about 5.9 x 10(8) KSKL events tagging the K-S by means of the K-L interaction in the calorimeter and requiring six prompt photons. With respect to our previous search, the analysis has been improved by increasing of a factor four the tagged sample and by a more effective background rejection of fake K-S tags and spurious clusters. We find no candidates in data and simulated background samples, while we expect 0.12 standard model events. Normalizing to the number of …

PhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physics01 natural sciencesStandard ModelCalorimeterNuclear physics0103 physical sciencesCP violationDirect searchLimit (mathematics)010306 general physicsPhysics Letters B
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