Search results for "Meson production"

showing 10 items of 59 documents

Pion photo- and electroproduction in relativistic baryon chiral perturbation theory and the chiral MAID interface

2013

We present a calculation of pion photo- and electroproduction in manifestly Lorentz-invariant baryon chiral perturbation theory up to and including order ${q}^{4}$. We fix the low-energy constants by fitting experimental data in all available reaction channels. Our results can be accessed via a Web interface, the so-called chiral MAID. We explain how our program works and how it can be used for further analysis.

Chiral anomalyPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMeson productionInterface (Java)High Energy Physics::PhenomenologyNuclear TheoryOrder (ring theory)Nuclear physicsBaryonPionNuclear ExperimentPhysical Review C
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Backward production of mesons associated with? ++(1232) in? + p interactions at 20 GeV/c

1991

We have analyzed backward meson production inπ + p reactions at 20GeV/c, which were measured in the CERN Ω spectrometer triggered by a fast proton (p f ), in experiment WA56. Production via baryon exchange of quasi-two-body final statesΔ ++ (1232)ρ 0 (770),Δ ++ (1232)f 2 (1270), andΔ ++ (1232)ρ 3 0 (1690) is clearly identified. The density matrix elements of meson resonances and ofΔ ++ (1232) are analyzed. We have observed also the reactionsπ + p→Δ ++ (1232)π 0 andπ + p→Δ ++ (1232)ω in thep f π + π 0 andp f π + π + π − π 0 final states.

Density matrixPhysicsBaryonNuclear physicsCrystallographyMeson productionPhysics and Astronomy (miscellaneous)ProtonMesonPiElementary particleEngineering (miscellaneous)OmegaZeitschrift f�r Physik C Particles and Fields
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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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Soft-dielectron excess in proton-proton collisions at $\sqrt{s}$ = 13 TeV

2021

Physical review letters 127(4), 042302 (2021). doi:10.1103/PhysRevLett.127.042302

HadronGeneral Physics and Astronomylow [transverse momentum]dielectron productionscattering [hadron hadron]01 natural sciencesSpectral lineQUARK-GLUON PLASMAHigh Energy Physics - ExperimentMany-body problemHigh Energy Physics - Experiment (hep-ex)ALICEscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]multiplicityInvariant massDielectronNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimenthadron-hadron scatteringAU COLLISIONSPhysicsQuantum chromodynamicsbremsstrahlung: hadronicLarge Hadron Colliderradiation: thermalPhysicsMUON PAIRSPHOTON PRODUCTIONBremsstrahlungELECTRON-PAIR PRODUCTIONddc:hadron: decayCERN LHC CollkinematicsMASS DILEPTON PRODUCTIONmany-body problemMASS DILEPTON PRODUCTION; ELECTRON-PAIR PRODUCTION; SPACE-TIME EVOLUTION; ETA-MESON PRODUCTION; QUARK-GLUON PLASMA; PHOTON PRODUCTION; NUCLEUS COLLISIONS; AU COLLISIONS; P-BE; MUON PAIRShadron hadron: scatteringParticle Physics - ExperimentParticle physicsp p: scatteringETA-MESON PRODUCTIONtransverse momentum: lowFOS: Physical sciencesthermal [radiation]Physics and Astronomy(all)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]5300103 physical sciencesSPACE-TIME EVOLUTIONddc:530Nuclear Physics - ExperimentMultiplicity (chemistry)010306 general physicsenhancementp nucleus: scatteringP-BEhadronic [bremsstrahlung]ALICE particle physics010308 nuclear & particles physicsALICE experimentparametrizationscattering [p nucleus]p p: scattering ; bremsstrahlung: hadronic ; transverse momentum: low ; p nucleus: scattering ; radiation: thermal ; hadron: decay ; hadron hadron: scattering ; CERN LHC Coll ; enhancement ; ALICE ; many-body problem ; parametrization ; multiplicity ; acceptance ; kinematics ; experimental results ; 13000 GeV-cms/nucleon13000 GeV-cms/nucleonHigh Energy Physics::ExperimentNUCLEUS COLLISIONSdecay [hadron]ALICE experiment dielectron production hadron-hadron scatteringacceptanceexperimental results
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Discrete Symmetries CP, T, CPT

2016

The role of Symmetry Breaking mechanisms to search for New Physics is of highest importance. We discuss the status and prospects of the Discrete Symmetries CP, T, CPT looking for their separate Violation in LHC experiments and meson factories.

HistoryParticle physicsMeson productionMesonCPT symmetryQC1-999Physics beyond the Standard ModelGeneral Physics and AstronomyFOS: Physical sciencesQuantum entanglement01 natural sciencesEducationHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesSymmetry breaking010306 general physicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPhysicsOperator (physics)High Energy Physics::PhenomenologyTime evolutionComputer Science ApplicationsB-factoryBaryogenesisStandard Model (mathematical formulation)High Energy Physics - PhenomenologyHomogeneous spaceCP violationHigh Energy Physics::ExperimentEPJ Web of Conferences
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η−3Nproblem with separable interactions

2002

The $\eta$-3N-interaction is studied within the four-body Faddeev-Yakubovsky theory adopting purely separable forms for the two- and three-body subamplitudes, limiting the basic two-body interactions to s-waves only. The corresponding separable approximation for the integral kernels is obtained by using the Hilbert-Schmidt procedure. Results are presented for the $\eta$-$^3$H scattering amplitude and for the total elastic cross section for energies below the triton break-up threshold.

Many-body problemPhysicsScattering amplitudeNuclear and High Energy PhysicsCross section (physics)Meson productionQuantum mechanicsScattering lengthLimitingFew-body systemsMathematical physicsSeparable spacePhysical Review C
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Evidence for B$^{0}_{s}$ meson production in Z$^0$ decays

1992

Seven unambiguous events out of a sample of 270 000 Z0 decays, contain in tile same jet a D(s) meson and a muon at large transverse momentum relative to the et axis. These events are direct evidence for B(s)0 meson production in hadronic Z0 decays. The production rate of these events, relative to all hadronic Z0 decays is ( 18 +/- 8) x 10(-5) this number including the relevant branching fractions of the B(s)0 and D(s). The value of the B(s)0 meson lifetime relative to the average B meson lifetime is measured to be 0.8 +/- 0.4.

Nuclear and High Energy PhysicsParticle physicsMeson productionMesonLUND MONTE-CARLOElectron–positron annihilationNuclear TheoryHadron01 natural sciencesCOLLIDERNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B mesonNuclear Experiment010306 general physicsPhysicsMuonLUND MONTE-CARLO; Z0 DECAYS; COLLIDER010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyZ0 DECAYSTransverse momentumFísica nuclearHigh Energy Physics::ExperimentParticle Physics - ExperimentProduction rate
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Charged lepton induced one kaon production off the nucleon

2013

We study single kaon production off the nucleon induced by electrons (positrons) i.e., e(-) (e(+)) + N -> v(e) ((v) over bar (e)) + (K) over bar (K) + N' at low energies. The possibility of observing these processes with the high luminosity beams available at TJNAF and Mainz is discussed, taking into account that the strangeness conserving electromagnetic reactions have a higher energy threshold for (K) over bar (K) production. The calculations are done using a microscopic model that starts from the SU(3) chiral Lagrangians and includes background terms and the resonant mechanisms associated to the lowest lying resonance Sigma*(1385)

Nuclear and High Energy PhysicsParticle physicsMeson productionNuclear TheoryElectroproductionPhoton energiesNuclear TheoryFOS: Physical sciencesLibrary science7. Clean energy01 natural sciencesPartícules (Física nuclear)Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Chiral perturbation theory0103 physical sciencesNuclear Experiment010306 general physicsNuclear theoryPhysicsGovernmentLambda010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyPhotoproductionHigh Energy Physics::Experiment
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Measurements of forward proton production with incident protons and charged pions on nuclear targets at the CERN Proton Synchroton

2010

Measurements of the double-differential proton production cross-section d(2 sigma)/dpd Omega in the range of momentum 0.5 GeV/c <= p < 8.0 GeV/c and angle 0.05 rad <= theta < 0.25 rad in collisions of charged pions and protons on beryllium, carbon, aluminium, copper, tin, tantalum, and lead are presented. The data were taken with the large acceptance HARP detector in the T9 beam line of the CERN Proton Synchrotron. Incident particles were identified by an elaborate system of beam detectors and impinged on a target of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using the forward spectrometer of the HARP experiment. Results are o…

Nuclear and High Energy Physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Physics::Instrumentation and Detectorsproton; nuclear targets; charged pionsFOS: Physical sciencesddc:500.201 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Basic research0103 physical sciencesCERN[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentInelastic proton scatteringPhysicsLarge Hadron Collider010308 nuclear & particles physicsOther reactions above meson production thresholds[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]FísicaPion-induced reactionsnuclear targetsResearch councilcharged pionsnuclear targetPhysics::Accelerator PhysicsHARP ExperimentHigh Energy Physics::ExperimentHumanitiesHARP Experiment; CERNParticle Physics - Experimentproton
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Study ofB→DsJ(*)+D¯(*)Decays

2004

We report a study of D-sJ(*)(2317)(+) and D-sJ(2460)(+) meson production in B decays. We observe the decays B+--> D-sJ((*)+)(D) over bar ((*)0) and B-0 --> DsJ(*)+D(*)- with the subsequent decays D-sJ(*)(2317)(+)-->D(s)(+)pi(0), D-sJ(2460)(+)-->D(s)(+)gamma, and D-sJ(2460)(+)-->D(s)(*+)pi(0). Based on a data sample of 122.1x10(6) B(B) over bar pairs collected with the BABAR detector at the PEP-II B factory, we obtain branching fractions for these modes, including the previously unseen decays B-->(DsJ(*)+D*). In addition, we perform an angular analysis of D-sJ(2460)(+)-->D(s)(+)gamma decays to test the different D-sJ(2460)(+) spin hypotheses.

Nuclear physicsPhysicsMeson production010308 nuclear & particles physicsElectron–positron annihilation0103 physical sciencesAnalytical chemistryGeneral Physics and Astronomy010306 general physics01 natural sciencesB-factoryPhysical Review Letters
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