0000000001331718

AUTHOR

M Reale

showing 6 related works from this author

B* production in Z decays

1995

The decay B*→Bγ has been observed with the DELPHI detector at LEP, where the B* meson is produced in Z boson decays. The combination of inclusively reconstructed B mesons with well-measured converted photons yields a measurement of the flavour-averaged B*-B mass difference of 45.5±0.3 (stat.) ±0.8 (syst.) MeV/c2. 95% confidence level upper limits at 6 MeV/c2 are placed on both the isospin (i.e. B+-B0) and the Bs-Bud splitting of the mass difference. The production ratio of B* to B mesons in Z decays is measured to be 0.72±0.03 (stat.) ±0.06 (syst.). Limits on the production cross-section of other hypothetical excited B hadron states decaying radiatively are established. The differential B* …

Particle physicsPhotonPhysics and Astronomy (miscellaneous)MesonElectron–positron annihilationHadronElementary particle01 natural sciencesNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physicsNuclear ExperimentEngineering (miscellaneous)BosonDELPHIPhysics010308 nuclear & particles physicsLARGE ELECTRON POSITRON COLLIDERIsospinPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentParticle Physics - Experiment
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Measurements of the Lineshape of the $Z^{0}$ and Determination of Electroweak Parameters from its Hadronic and Leptonic Decays

1994

Abstract: During the LEP running periods in 1990 and 1991 DELPHI has accumulated approximately 450000 Z0 decays into hadrons and charged leptons. The increased event statistics coupled with improved analysis techniques and improved knowledge of the LEP beam energies permit significantly better measurements of the mass and width of the Z0 resonance. Model independent fits to the cross sections and leptonic forward-backward asymmetries yield the following Z0 parameters: the mass and total width M(Z) = 91.187 +/- 0.009 GeV, GAMMA(Z) = 2.486 +/- 0.012 GeV, the hadronic and leptonic partial widths GAMMA(had) = 1.725 +/- 0.012GeV, GAMMA(l) = 83.01 +/- 0.52 MeV, the invisible width GAMMA(inv) = 51…

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationLEP-SLC ENERGIESElementary particle01 natural sciences7. Clean energyPartícules (Física nuclear)PHYSICSNuclear physicsBHABHA SCATTERINGParticle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSLEP-SLC ENERGIES; RADIATIVE-CORRECTIONS; BHABHA SCATTERING; MASS CORRECTIONS; PHYSICS010306 general physicsDetectors de radiacióDELPHIBhabha scatteringPhysics010308 nuclear & particles physicsPhysicsDELPHI; Z0 resonance; mass corrections; radiative correctionsMathematics::History and OverviewHigh Energy Physics::PhenomenologyElectroweak interactionWeinberg angleMASS CORRECTIONSradiative correctionsZ0 resonanceHiggs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentLepton
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Measurement of the Lund jet plane using charged particles in 13 TeV proton-proton collisions with the ATLAS detector

2020

The prevalence of hadronic jets at the LHC requires that a deep understanding of jet formation and structure is achieved in order to reach the highest levels of experimental and theoretical precision. There have been many measurements of jet substructure at the LHC and previous colliders, but the targeted observables mix physical effects from various origins. Based on a recent proposal to factorize physical effects, this Letter presents a double-differential cross-section measurement of the Lund jet plane using 139  fb−1 of √s=13  TeV proton-proton collision data collected with the ATLAS detector using jets with transverse momentum above 675 GeV. The measurement uses charged particles to ac…

:Kjerne- og elementærpartikkelfysikk: 431 [VDP]Protonshowers [parton]13000 GeV-cmsPhysics::Instrumentation and DetectorsHadronGeneral Physics and Astronomyjet: transverse momentumPhysical Effects01 natural sciencestransverse momentum [jet]High Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)Charged ParticlesSubatomic PhysicsComputingMilieux_COMPUTERSANDEDUCATIONscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Parton showerNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)PhysicsSettore FIS/01Jet (fluid)Large Hadron ColliderDouble Differential Cross SectionsDetectorhadronic [jet]Monte Carlo [numerical calculations]ATLASTransverse Momentacharged particleCharged particlemedicine.anatomical_structureCERN LHC Coll:Nuclear and elementary particle physics: 431 [VDP]colliding beams [p p]numerical calculations: Monte CarloParticle Physics - Experimentp p: scatteringCiências Naturais::Ciências Físicas530 Physicsformation [jet]Astrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesMeasurements ofLHC ATLAS High Energy Physicsjet: formation530GeneralLiterature_MISCELLANEOUSMonte Carlo Modelparton: showersNuclear physicsdifferential cross section: measuredAtlas (anatomy)Fragmentationmeasured [differential cross section]0103 physical sciencesmedicineddc:530High Energy Physicsstructure010306 general physicsATLAS CollaborationScience & Technology010308 nuclear & particles physicsComputerSystemsOrganization_COMPUTER-COMMUNICATIONNETWORKSFísicajet: hadronic530 Physikangular resolutionProton Proton CollisionsElementary Particles and FieldsHigh Energy Physics::ExperimentDetector EffectsHadron-hadron collisionsp p: colliding beamsMathematicsofComputing_DISCRETEMATHEMATICSacceptanceexperimental results
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Measurement of inclusive pi(0) production in hadronic Z(0) decays

1996

An analysis is presented of inclusive \pi^0 production in Z^0 decays measured with the DELPHI detector. At low energies, \pi^0 decays are reconstructed by \linebreak using pairs of converted photons and combinations of converted photons and photons reconstructed in the barrel electromagnetic calorimeter (HPC). At high energies (up to x_p = 2 \cdot p_{\pi}/\sqrt{s} = 0.75) the excellent granularity of the HPC is exploited to search for two-photon substructures in single showers. The inclusive differential cross section is measured as a function of energy for {q\overline q} and {b \bar b} events. The number of \pi^0's per hadronic Z^0 event is N(\pi^0)/ Z_{had}^0 = 9.2 \pm 0.2 \mbox{(stat)} \…

Particle physicsPhysics and Astronomy (miscellaneous)LUND MONTE-CARLOStar (game theory)Electron–positron annihilationHadron01 natural sciencesSpectral linePartícules (Física nuclear)JET FRAGMENTATIONNuclear physicsQCD JETSelectromagnetic calorimeter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SPECTRA010306 general physicsParton showerDELPHI; Z0 decay; inclusive pi0 production; electromagnetic calorimeterDELPHIPhysicsDENSITY PROJECTION CHAMBER; LUND MONTE-CARLO; JET FRAGMENTATION; E+E-PHYSICS; QCD JETS; SPECTRAE+E-PHYSICS010308 nuclear & particles physicsinclusive pi0 productionZ0 decayLARGE ELECTRON POSITRON COLLIDERLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSProduction (computer science)Física nuclearDENSITY PROJECTION CHAMBEREnergy (signal processing)Particle Physics - Experiment
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Measurement of Event Shape and Inclusive Distributions at $\sqrt{s} =$ 130 and 136 GeV

1997

Inclusive charged particle and event shape distributions are measured using 321 hadronic events collected with the DELPHI experiment at LEP at effective centre of mass energies of 130 to 136 GeV. These distributions are presented and compared to data at lower energies, in particular to the precise Z data. Fragmentation models describe the observed changes of the distributions well. The energy dependence of the means of the event shape variables can also be described using second order QCD plus power terms. A method independent of fragmentation model corrections is used to determine $\alpha_s$ from the energy dependence of the mean thrust and heavy jet mass. It is measured to be: % %\alpha_s…

High energyParticle physicsZ(0) RESONANCEPhysics and Astronomy (miscellaneous)Electron–positron annihilationHADRONIC Z-DECAYS; E+E-ANNIHILATION; ALPHA-S; POWER CORRECTIONS; Z(0) RESONANCE; MONTE-CARLO; QCD MODELS; ENERGY; FRAGMENTATION; PREDICTIONSHadronPREDICTIONSThrust01 natural sciences7. Clean energyPartícules (Física nuclear)Nuclear physicsENERGYFragmentation (mass spectrometry)POWER CORRECTIONSMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ALPHA-S010306 general physicsDetectors de radiacióDELPHIPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyE+E-ANNIHILATIONLARGE ELECTRON POSITRON COLLIDERCharged particleHADRONIC Z-DECAYSLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIQCD MODELSPARTICLE PHYSICSHigh Energy Physics::ExperimentFRAGMENTATIONParticle Physics - Experiment
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Luca Fonnesu, Per una moralità concreta.

2011

Fonnesu analizza l'interessante tematica della 'Verwirklichung' all'interno della filosofia classica tedesca. Nel contesto della tensione tra la 'Gesinnung' kantiana e la 'politische Gesinnung' hegeliana, l'autore focalizza la sua attenzione sul concetto di seconda natura, la storia fenomenologica della coscienza e la felicità empirica in Fichte ed Hegel. Con un rinnovato approfondimento delle nozioni kantiane di 'Praktische' e 'Materie', 'Welt' e 'Glückseligkeit' l'autore rivendica l'attenzione del filosofo di Königsberg al raggiungimento concreto della moralità.

RealizzazioneKantFichtemoralitàHegel.felicitàseconda naturafenomenologia della coscienzasistema del diritto
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