0000000000048514

AUTHOR

Klaus Peters

showing 27 related works from this author

The PANDA Barrel DIRC detector

2014

Abstract The PANDA experiment at the new Facility for Antiproton and Ion Research in Europe (FAIR) at GSI, Darmstadt, will study fundamental questions of hadron physics and QCD using high-intensity cooled antiproton beams with momenta between 1.5 and 15 GeV/c. Efficient Particle Identification for a wide momentum range and the full solid angle is required for reconstructing the various physics channels of the PANDA program. Hadronic Particle Identification in the barrel region of the detector will be provided by a DIRC counter. The design is based on the successful BABAR DIRC with important improvements, such as focusing optics and fast photon timing. Several of these improvements, includin…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron ColliderPhysics::Instrumentation and DetectorsHadronDetectorParticle identificationNuclear physicsConceptual designAntiprotonPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Measurement of e+e−→π+π−ψ(3686) from 4.008 to 4.600 GeV and observation of a charged structure in the π±ψ(3686) mass spectrum

2018

We study the process e(+)e(-) -> p(+)p(-)psi(3686) using 5.1 fb(-1) of data collected at 16 center-of-mass energy (root s) points from 4.008 to 4.600 GeV by the BESIII detector operating at the BEPCII collider. The measured Born cross sections for e(+)e(-) -> p(+)p(-)psi(3686) are consistent with previous results, but with much improved precision. A fit to the cross section shows contributions from two structures: the first has M = 4209.5 +/- 7.4 +/- 1.4 MeV/c(2) and Gamma = 80.1 +/- 24.6 +/- 2.9 MeV, and the second has M = 4383.8 +/- 4.2 +/- 0.8 MeV/c(2) and Gamma = 84.2 +/- 12.5 +/- 2.1 MeV, where the first errors are statistical and the second systematic. The lower-mass resonance is obse…

Particle physicsPhotonMesonElectron–positron annihilationGeneral Physics and AstronomyDalitz plot01 natural sciencesResonance (particle physics)law.inventionMomentumNuclear physicslaw0103 physical sciencesPiIntermediate stateInvariant massBorn approximationNuclear Experiment010306 general physicsColliderQuantum chromodynamicsPhysicsLuminosity (scattering theory)Linear polarization010308 nuclear & particles physicsSigmaMagnetic fieldAntimatterIsospinMass spectrumHigh Energy Physics::ExperimentAtomic physicsPhysical Review D
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Search for the radiative leptonic decay D+→γe+νe

2017

Using an electron-positron collision data sample of 2.93 fb(-1) collected at a center-of-mass energy of root s = 3.773 GeV with the BESIII detector, we present the first search for the radiative leptonic decay D+ -> gamma e(+)nu(e). The analysis is performed with a double-tag method. We do not observe a significant D+ -> gamma e(+)nu(e) signal, and obtain an upper limit on the branching fraction of D+ -> gamma e(+)nu(e) decay with the energy of radiative photon larger than 10 MeV of 3.0 x 10(-5) at the 90% confidence level.

PhysicsPhoton010308 nuclear & particles physicsBranching fractionElectron–positron annihilationPhoton energy01 natural sciencesNuclear physicsFactorization0103 physical sciencesRadiative transferHigh Energy Physics::Experiment010306 general physicsEnergy (signal processing)Physical Review D
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Measurement of the absolute branching fraction of D + → K̅ 0 e + ν e via K̅ 0 → π 0 π 0

2016

By analyzing 2.93 fb(-1) data collected at the center-of-mass energy root s = 3.773 GeV with the BESIII detector, we measure the absolute branching fraction of the semileptonic decay D+ -> (K) over bar (0)e(+)nu(e) to be B(D (+) -> (K) over bar (0)e(+)nu(e)) = (8.59 +/- 0.14 +/- 0.21)% using (K) over bar (0) -> K-S(0) -> pi(0) pi(0), where the first uncertainty is statistical and the second systematic. Our result is consistent with previous measurements within uncertainties..

PhysicsSemileptonic decayNuclear and High Energy Physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationAstronomy and Astrophysics01 natural sciencesNuclear physics0103 physical sciencesPi010306 general physicsInstrumentationBar (unit)Chinese Physics C
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Measurement of integrated luminosity and center-of-mass energy of data taken by BESIII at

2017

Chinese physics / C 41(11), 113001 (2017). doi:10.1088/1674-1137/41/11/113001

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical Phenomena01 natural sciences530law.inventionNuclear physicslaw0103 physical sciencesddc:530Nuclear Experiment010306 general physicsColliderInstrumentationAstrophysics::Galaxy AstrophysicsBhabha scatteringPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsDetectorAstronomy and AstrophysicsCollisionData setHigh Energy Physics::ExperimentCenter of massAstrophysics::Earth and Planetary AstrophysicsEnergy (signal processing)
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The PANDA DIRC Detectors at FAIR

2017

The PANDA detector at the international accelerator Facility for Antiproton and Ion Research in Europe (FAIR) addresses fundamental questions of hadron physics. An excellent hadronic particle identification (PID) will be accomplished by two DIRC (Detection of Internally Reflected Cherenkov light) counters in the target spectrometer. The design for the barrel region covering polar angles between 22 deg. to 140 deg. is based on the successful BABAR DIRC with several key improvements, such as fast photon timing and a compact imaging region. The novel Endcap Disc DIRC will cover the smaller forward angles between 5 deg. (10 deg.) to 22 deg. in the vertical (horizontal) direction. Both DIRC coun…

PhotomultiplierPhotonPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsFOS: Physical sciences01 natural sciencesParticle identification030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsDetection of internally reflected Cherenkov light0103 physical sciencesNuclear ExperimentInstrumentationMathematical PhysicsPhysicsSpectrometer010308 nuclear & particles physicsbusiness.industryDetectorInstrumentation and Detectors (physics.ins-det)Facility for Antiproton and Ion ResearchMicrochannel plate detectorHigh Energy Physics::Experimentbusiness
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The PANDA Barrel DIRC

2016

The PANDA detector at the international accelerator Facility for Antiproton and Ion Research in Europe (FAIR) addresses fundamental questions of hadron physics. Experiments concerning charmonium spectroscopy, the search for hybrids and glueballs and the interaction of hidden and open charm particles with nucleons and nuclei will be performed with antiproton beams impinging on hydrogen or nuclear targets. Cooled beams allow the precision scan of resonances in formation experiments. The momentum range of the antiproton beam between 1.5 GeV/c and 15 GeV/c tests predictions by perturbation theory and will reveal deviations originating from strong QCD . An excellent hadronic particle identificat…

PhysicsPhotonLarge Hadron Collider010308 nuclear & particles physicsHadron01 natural sciences7. Clean energyParticle identificationNuclear physicsDetection of internally reflected Cherenkov lightAntiproton0103 physical sciencesPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::Experimentddc:610Nuclear Experiment010306 general physicsInstrumentationMathematical PhysicsCherenkov radiation
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Evidence for e+e−→γηc(1S) at center-of-mass energies between 4.01 and 4.60 GeV

2017

We present first evidence for the process e(+)e(-) -> gamma eta(c)(1S) at six center-of-mass energies between 4.01 and 4.60 GeV using data collected by the BESIII experiment operating at BEPCII. We measure the Born cross section at each energy using a combination of twelve eta(c)(1S) decay channels. We also combine all six energies under various assumptions for the energy-dependence of the cross section. If the process is assumed to proceed via the Y(4260), we measure a peak Born cross section sigma(peak)(e(+)e(-) -> gamma eta(c)(1S)) = 2.11 +/- 0.49 (stat.) +/- 0.36 (syst.) pb with a statistical significance of 4.2 sigma.

PhysicsParticle physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationSigma01 natural sciencesNuclear physicsCross section (physics)0103 physical sciencesHigh Energy Physics::ExperimentCenter of massBorn approximationNuclear Experiment010306 general physicsPhysical Review D
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The PANDA Endcap Disc DIRC

2018

Journal of Instrumentation 13(02), C02002 - C02002 (2018). doi:10.1088/1748-0221/13/02/C02002

particle identification [K]Physics::Instrumentation and Detectors61001 natural sciencesDIRCK: particle identificationOpticsPionDetection of internally reflected Cherenkov light0103 physical sciencesparticle identification [pi]ddc:610010306 general physicsNuclear ExperimentInstrumentationMathematical PhysicsCherenkov radiationPhysicsCherenkov counter: designRange (particle radiation)010308 nuclear & particles physicsbusiness.industryPANDADetectorSolid angleDESYLight guideTest beamdesign [Cherenkov counter]Radiator (engine cooling)Facility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentPhotonicsbusinesspi: particle identificationperformance
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Study of BESIII trigger efficiencies with the 2018 J/psi data

2021

Using a dedicated data sample taken in 2018 on the $J/\psi$ peak, we perform a detailed study of the trigger efficiencies of the BESIII detector. The efficiencies are determined from three representative physics processes, namely Bhabha-scattering, dimuon production and generic hadronic events with charged particles. The combined efficiency of all active triggers approaches $100\%$ in most cases with uncertainties small enough as not to affect most physics analyses.

Nuclear and High Energy Physicshadronic eventsHadron01 natural sciencesNOHigh Energy Physics - ExperimentNuclear physicsSubatomär fysikBESIII; trigger efficiency; Bhabha; dimuon; hadronic events0103 physical sciencesSubatomic PhysicsBhabhaddc:530trigger efficiency010306 general physicsInstrumentationBhabha scatteringPhysicsdimuon010308 nuclear & particles physicsDetectorBESIIIAstronomy and AstrophysicsCharged particleHigh Energy Physics::ExperimentBESIII trigger efficiency Bhabha dimuon hadronic events
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Measurement of e+ e- → DD cross sections at the ψ(3770) resonance

2018

Chinese physics / C High energy physics and nuclear physics C 42(8), 083001 (2018). doi:10.1088/1674-1137/42/8/083001

Particle physicsNuclear and High Energy PhysicsMesoncharm mesonsElectron–positron annihilation01 natural sciencesResonance (particle physics)530BESIII/BEPCIIlaw.inventionHigh Energy Physics - ExperimentNOlaw0103 physical sciencesddc:530010306 general physicsColliderInstrumentationDECAY LIBRARY TAUOLAPhysicsLuminosity (scattering theory)Annihilation010308 nuclear & particles physicsSigmacross sectionsAstronomy and AstrophysicsBESIII/BEPCII; charm mesons; cross sections; Nuclear and High Energy Physics; Instrumentation; Astronomy and AstrophysicsHigh Energy Physics::ExperimentBar (unit)
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Observation of the doubly radiative decay η′→γγπ0

2017

Based on a sample of 1.31 billion J/psi events collected with the BESIII detector, we report the study of the doubly radiative decay eta' -> gamma gamma pi(0) for the first time, where the eta' meson is produced via the J/psi -> gamma eta' decay. The branching fraction of eta' -> gamma gamma pi(0) inclusive decay is measured to be B(eta' -> gamma gamma pi(0))(Incl) = (3.20 +/- 0.07(stat) +/- 0.23(sys)) x 10(-3), while the branching fractions of the dominant process eta' -> gamma omega and the non-resonant component are determined to be B(eta' -> gamma omega) x B(omega -> gamma pi(0)) = (23.7 +/- 1.4(stat) +/- 1.8(sys)) x 10(-4) and B(eta' -> gamma gamma pi(0))(NR) = (6.16 +/- 0.64(stat) +/-…

PhysicsMeson010308 nuclear & particles physicsBranching fractionAstrophysics::High Energy Astrophysical PhenomenaElectron–positron annihilationRadiative decay01 natural sciencesOmegaGamma gammaNuclear physics0103 physical sciencesPiHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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Study of J/ψ and ψ(3686)→Σ(1385)0Σ¯(1385)0 and Ξ0Ξ¯0

2017

Abstract We study the decays of J / ψ and ψ ( 3686 ) to the final states Σ ( 1385 ) 0 Σ ¯ ( 1385 ) 0 and Ξ 0 Ξ ¯ 0 based on a single baryon tag method using data samples of ( 1310.6 ± 7.0 ) × 10 6 J / ψ and ( 447.9 ± 2.9 ) × 10 6 ψ ( 3686 ) events collected with the BESIII detector at the BEPCII collider. The decays to Σ ( 1385 ) 0 Σ ¯ ( 1385 ) 0 are observed for the first time. The measured branching fractions of J / ψ and ψ ( 3686 ) to Ξ 0 Ξ ¯ 0 are in good agreement with, and much more precise than, the previously published results. The angular parameters for these decays are also measured for the first time. The measured angular decay parameter for J / ψ → Σ ( 1385 ) 0 Σ ¯ ( 1385 ) 0 , …

BaryonNuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsAngular distribution010308 nuclear & particles physicsBranching fractionIsospinElectron–positron annihilation0103 physical sciences010306 general physics01 natural sciencesPhysics Letters B
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Recent results with lifetime enhanced microchannel-plate photomultipliers

2018

Abstract The favored photon sensors for the DIRC (detection of internally reflected Cherenkov light) detectors at the PANDA (Anti-proton Annihilation at Darmstadt) experiment at FAIR (Facility for anti-proton and ion research) are micro-channel-plate photomultipliers (MCP-PMTs). The main problem until a few years ago was the limited lifetime of the MCP-PMTs caused by a rapid decrease in quantum efficiency (QE) of the photo cathode (PC) with increasing integrated anode charge (IAC). These limitations are overcome by applying an atomic layer deposition (ALD) coating on the MCPs, as recently done by PHOTONIS and Hamamatsu. During the last years’ tests of lifetime enhanced MCP-PMTs were perform…

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhoton010308 nuclear & particles physicsbusiness.industry01 natural sciencesCathode030218 nuclear medicine & medical imagingAnodelaw.invention03 medical and health sciencesAtomic layer deposition0302 clinical medicineOpticsDetection of internally reflected Cherenkov lightlaw0103 physical sciencesQuantum efficiencyMicrochannel plate detectorbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Improved measurements of branching fractions for ηc→ϕϕ and ωϕ

2017

Using (223.7 +/- 1.4) x 10(6) J / Psi events accumulated with the BESIII detector, we study eta(c) decays to phi phi and omega phi final states. The branching fraction of n(c) -> phi phi is measured to be Br(eta(c) -> phi phi) = (2.5 +/- 0(-0.7)(+0.3) +/- 0.6) X 10(-3,) where the first uncertainty is statistical, the second is systematic, and the third is from the uncertainty of Br(J / Psi -> gamma eta(C)). No significant signal for the double Okubo-Zweig-Iizuka suppressed decay of eta(c) -> omega phi is observed, and the upper limit on the branching fraction is determined to be Br(eta(c) -> omega phi) < 2.5 x 10(-4) at the 90% confidence level.

PhysicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationAnalytical chemistryBranching (polymer chemistry)01 natural sciencesOmega0103 physical sciencesHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsPhysical Review D
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Measurement of branching fractions for ψ(3686)→γη′ , γη , and γπ0

2017

Using a data sample of 448 x 10(6) psi(3686) events collected with the BESIII detector operating at the BEPCII storage ring, the decays psi(3686) -> gamma eta and psi(3686) -> gamma pi(0) are observed with a statistical significance of 7.3 sigma and 6.7 sigma, respectively. The branching fractions are measured to be B(psi(3686) -> gamma eta) = (0.85 +/- 0.18 +/- 0.05) x 10(-6) and B(psi(3686) ->gamma pi(0)) = (0.95 +/- 0.16 +/- 0.05) x 10(-6). In addition, we measure the branching fraction of psi(3686) -> gamma eta' to be B(psi(3686) -> gamma eta') = (125.1 +/- 2.2 +/- 6.2)x10(-6), which represents an improvement of precision over previous results.

PhysicsElectromagnetic calorimeter010308 nuclear & particles physicsBranching fractionElectron–positron annihilation0103 physical sciencesAnalytical chemistryHigh Energy Physics::Experiment010306 general physicsBranching (polymer chemistry)01 natural sciencesAstrophysics::Galaxy AstrophysicsPhysical Review D
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Observation of e + e − → ηψ(2S) at center-of-mass energies from 4.236 to 4.600 GeV

2021

Journal of high energy physics 2021(10), 177 (2021). doi:10.1007/JHEP10(2021)177

ExoticsNuclear and High Energy Physicsmeasured [channel cross section]e+-e− ExperimentsQuarkoniumannihilation [electron positron]QC770-798electron positron: annihilationetaParticle and resonance productionMeasure (mathematics)530Standard deviationNONuclear physicsSubatomär fysikCross section (physics)e+-e��� Experimentsenergy dependence: measured [cross section]Astronomi astrofysik och kosmologiNuclear and particle physics. Atomic energy. RadioactivitySubatomic PhysicsAstronomy Astrophysics and Cosmologyddc:530e+-e− Experiments Exotics Particle and resonance production Quarkoniumpsi(3685)PhysicsBESe(+)-e(-) ExperimentsDetectorstatistical [error]electron positron --> eta psi(3685)e +-e − Experimentselectron positron: colliding beamsBeijing Stor4.236-4.600 GeV-cmsCollisionerror: statisticalYield (chemistry)e-e Experimentselectron positron --&gt; eta psi(3685)colliding beams [electron positron]High Energy Physics::ExperimentCenter of masscross section: energy dependence: measuredchannel cross section: measuredStorage ringexperimental results
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Immunogenicity and safety of a nine-valent human papillomavirus vaccine in women 27–45 years of age compared to women 16–26 years of age: An open-lab…

2021

Abstract: Background: Efficacy of the nine-valent human papillomavirus (9vHPV; HPV types 6/11/16/18/31/33/45/52/58) vaccine was demonstrated in a phase 3 study in women 16 & ndash;26 years of age. We present a phase 3 immunogenicity and safety study of the 9vHPV vaccine in women 27 & ndash;45 versus 16 & ndash;26 years of age. Methods: This international, open-label study (NCT03158220) was conducted in women 16 & ndash;45 years of age. Participants (16 & ndash;26 years, n = 570 and 27 & ndash;45 years, n = 642) received a three-dose 9vHPV vaccination regimen (day 1, month 2, month 6). Month 7 geometric mean titers (GMTs) and seroconversion percentages to anti-HPV 6/11/16/18/31/33/45/52/58 w…

AdultHuman papillomavirusmedicine.medical_specialtyAdolescentAntibodies ViralYoung Adult03 medical and health sciencesNine-valent human papillomavirus vaccineImmunogenicity Vaccine0302 clinical medicine030225 pediatricsInternal medicinemedicineHumansPapillomavirus Vaccines030212 general & internal medicineSeroconversionHPV prophylaxisAdverse effectAgedCervical cancerHuman papillomavirus 16Human papillomavirus 18General VeterinaryGeneral Immunology and Microbiologybusiness.industryPapillomavirus InfectionsAdult vaccinationPublic Health Environmental and Occupational Healthmedicine.diseaseVaccine efficacyConfidence interval3. Good healthVaccinationClinical trialPrecancerRegimenInfectious DiseasesCervical cancerMolecular MedicineFemaleHuman medicinebusinessVaccine
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Observation of ${{e^+e^- \rightarrow D_s^+} \overline{ D}^{\bf (*)0} {K^-}}$ and study of the P -wave ${{D_s}}$ mesons

2018

Studies of $e^+e^- \to D_s^+ \overline{D}{}^{(*)0}K^-$ and the $P$-wave charmed-strange mesons are performed based on an $e^+e^-$ collision data sample corresponding to an integrated luminosity of 567 pb$^{-1}$ collected with the BESIII detector at $\sqrt{s}= 4.600$ GeV. The processes of $e^+e^-\to D_s^+ \overline{D}{*}^{0} K^-$ and $D_s^+ \overline{D}{}^{0} K^-$ are observed for the first time and are found to be dominated by the modes $D_s^+ D_{s1}(2536)^-$ and $D_s^+ D^*_{s2}(2573)^-$, respectively. The Born cross sections are measured to be $\sigma^{B}(e^+e^-\to D_s^+ \overline{D}{*}^{0} K^-) = (10.1\pm2.3\pm0.8) pb$ and $\sigma^{B}(e^+e^-\to D_s^+ \overline{D}{}^{0} K^-) = (19.4\pm2.3\…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationFOS: Physical sciencesAstronomy and Astrophysics01 natural sciencesHigh Energy Physics - ExperimentLuminosityHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesBorn approximation010306 general physicsInstrumentationChinese Physics C
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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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Measurements of the absolute branching fractions forDs+→ηe+νeandDs+→η′e+νe

2016

By analyzing 482 pb(-1) of e(+)e(-) collision data collected at root s = 4.009 GeV with the BESIII detector at the BEPCII collider, we measure the absolute branching fractions for the semileptonic decays D-s(+) -> eta e(+)nu(e) and D-s(+) -> eta ' e(+)nu(e) to be B(D-s(+) -> eta e(+)nu(e)) = (2.30 +/- 0.31 +/- 0.08)% and B(D-s(+) -> eta ' e(+)nu(e)) = (0.93 +/- 0.30 +/- 0.05)%, respectively, and their ratio B(D-s(+) -> eta ' e(+)nu(e)) / B(D-s(+) -> eta ' e(+)nu(e)) = 0.40 +/- 0.14 +/- 0.02, where the first uncertainties are statistical and the second ones are systematic. The results are in good agreement with previous measurements within uncertainties; they can be used to determine the eta…

Physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilation0103 physical sciencesAnalytical chemistryHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsAtomic physicsNuclear Experiment010306 general physicsBranching (polymer chemistry)01 natural sciencesPhysical Review D
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The Barrel DIRC of PANDA

2012

Cooled antiproton beams of unprecedented intensities in the momentum range of 1.5-15 GeV/c will be used for the PANDA experiment at FAIR to perform high precision experiments in the charmed quark sector. The PANDA detector will investigate antiproton annihilations with beams in the momentum range of 1.5 GeV/c to 15 GeV/c on a fixed target. An almost 4π acceptance double spectrometer is divided in a forward spectrometer and a target spectrometer. The charged particle identification in the latter is performed by ring imaging Cherenkov counters employing the DIRC principle.

PhysicsParticle physicsRange (particle radiation)SpectrometerPhysics::Instrumentation and Detectors010308 nuclear & particles physicsDetector01 natural sciences7. Clean energyCharged particleCharm quarkMomentumNuclear physicsAntiproton0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsInstrumentationMathematical PhysicsCherenkov radiationJournal of Instrumentation
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Simulation and reconstruction of the PANDA Barrel DIRC

2014

Hadronic particle identification (PID) in the barrel region of the PANDA experiment at the new Facility for Antiproton and Ion Research in Europe (FAIR) at GSI, Darmstadt will be provided by a DIRC (Detection of Internally Reflected Cherenkov light) counter. To optimize the performance and reduce the detector cost, detailed simulations of different design elements, such as the width of the radiators, the shape of the expansion volume, and the type of focusing system, were performed using Geant. Custom reconstruction algorithms were developed to match the detector geometry. We will discuss the single photon resolution and photon yield as well as the PID performance for the Barrel DIRC baseli…

PhysicsNuclear and High Energy PhysicsPhotonPhysics::Instrumentation and DetectorsCherenkov detectorDetectorBarrel (horology)PID controllerParticle identificationlaw.inventionNuclear physicsDetection of internally reflected Cherenkov lightlawFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Particle identification algorithms for the PANDA Barrel DIRC

2020

The International Conference Instrumentation for Colliding Beam Physics , INSTR2020, Novosibirsk, Russia, 24 Feb 2020 - 28 Feb 2020; Journal of Instrumentation 15(09), C09057 (2020). doi:10.1088/1748-0221/15/09/C09057

Computer scienceBarrel (horology)610ddc:610InstrumentationAlgorithmMathematical PhysicsParticle identificationJournal of Instrumentation
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Study of J/ψ and ψ(3686) decays to π+π−η′

2017

Using the data samples of 1.31 x 10(9) J/psi events and 4.48 x 10(8) psi(3686) events collected with the BESIII detector, partial wave analyses on the decays J/psi and psi(3686) pthornp -> pi(+)pi(-)eta' are performed with a relativistic covariant tensor amplitude approach. The dominant contribution is found to be J/psi and psi(3686) decays to rho eta' In the J/psi decay, the branching fraction B(J/psi -> rho eta') is determined to be (7.90 +/- 0.19(stat) +/- 0.49(sys)) x 10(-5). Two solutions are found in the psi(3686) decay, and the corresponding branching fraction B(psi(3686) -> rho eta') is (1.02 +/- 0.11(stat) +/- 0.24(sys)) x 10(-5) for the case of destructive interference, and (5.69 …

PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationPartial wave analysisAnalytical chemistrySigmaLambda01 natural sciences0103 physical sciencesPiHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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Time imaging reconstruction for the PANDA Barrel DIRC

2020

The innovative Barrel DIRC (Detection of Internally Reflected Cherenkov light) counter will provide hadronic particle identification (PID) in the central region of the PANDA experiment at the new Facility for Antiproton and Ion Research (FAIR), Darmstadt, Germany. This detector is designed to separate charged pions and kaons with at least 3 standard deviations for momenta up to 3.5 GeV/c, covering the polar angle range of 22$^{\circ}$-140$^{\circ}$. An array of microchannel plate photomultiplier tubes is used to detect the location and arrival time of the Cherenkov photons with a position resolution of 2 mm and time precision of about 100 ps. The time imaging reconstruction has been develop…

PhotomultiplierPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsFOS: Physical sciences01 natural sciencesParticle identification030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsDetection of internally reflected Cherenkov light0103 physical sciencesNuclear ExperimentInstrumentationMathematical PhysicsCherenkov radiationPhysics010308 nuclear & particles physicsbusiness.industryDetectorReconstruction algorithmInstrumentation and Detectors (physics.ins-det)Facility for Antiproton and Ion ResearchMicrochannel plate detectorHigh Energy Physics::Experimentbusiness
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Future Physics Programme of BESIII

2020

There has recently been a dramatic renewal of interest in the subjects of hadron spectroscopy and charm physics. This renaissance has been driven in part by the discovery of a plethora of charmonium-like $XYZ$ states at BESIII and $B$ factories, and the observation of an intriguing proton-antiproton threshold enhancement and the possibly related $X(1835)$ meson state at BESIII, as well as the threshold measurements of charm mesons and charm baryons. We present a detailed survey of the important topics in tau-charm physics and hadron physics that can be further explored at BESIII over the remaining lifetime of BEPCII operation. This survey will help in the optimization of the data-taking pla…

Nuclear and High Energy PhysicsParticle physicsX(1835)charmed mesonMesoncharmoniumNuclear TheoryFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNOSubatomär fysikHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron physicsHadron spectroscopySubatomic Physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530Charm (quantum number)charmed baryontau010306 general physicsNuclear ExperimentInstrumentationanti-p pactivity reportPhysicsthreshold: enhancementLuminosity (scattering theory)BES010308 nuclear & particles physicshadron spectroscopyHigh Energy Physics::PhenomenologyThe RenaissanceAstronomy and AstrophysicsBeijing Stor: upgradeBaryonHigh Energy Physics - PhenomenologyUpgradeexperimental equipment[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentluminosity: high
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