Search results for "Monte Carlo method."

showing 10 items of 1217 documents

Reliability of Monte Carlo event generators for gamma-ray dark matter searches

2013

We study the differences in the gamma-ray spectra simulated by four Monte Carlo event generator packages developed in particle physics. Two different versions of PYTHIA and two of HERWIG are analyzed, namely PYTHIA 6.418 and HERWIG 6.5.10 in Fortran and PYTHIA 8.165 and HERWIG 2.6.1 in C++. For all the studied channels, the intrinsic differences between them are shown to be significative and may play an important role in misunderstanding dark matter signals.

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)FortranMonte Carlo methodDark matterFOS: Physical sciencesGamma ray spectra01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Reliability (semiconductor)0103 physical sciences010303 astronomy & astrophysicsEvent generatorcomputer.programming_languageHigh Energy Astrophysical Phenomena (astro-ph.HE)Physics010308 nuclear & particles physicsGamma rayFísicaHigh Energy Physics - PhenomenologyMonte Carlo SimulationsAstrophysics - High Energy Astrophysical PhenomenacomputerEvent (particle physics)Astrophysics - Cosmology and Nongalactic Astrophysics
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Energy-energy correlations in hadronic final states from Z0 decays

1990

We have studied the energy-energy angular correlations in hadronic final states from Z0 decay using the DELPHI detector at LEP. From a comparison with Monte Carlo calculations based on the exact second order QCD matrix element and string fragmentation we find that Λ(5)/MS = 104-20 +25 (stat.)-20 +25(syst.)-00 +30(theor.) MeV, which corresponds to αs(91 GeV) = 0.106± 0.003 (stat.)±0.003(syst.)-0.000 +0.003(theor.). The theoretical error stems from different choices for the renormalization scale of αs. In the Monte Carlo simulation the scale of αs as well as the fragmentation parameters have been optimized to described reasonably well all aspects of multihadron production.

Nuclear and High Energy PhysicsParticle physicsLUND MONTE-CARLO2ND ORDER QCDElectron–positron annihilationHadronMonte Carlo methodElementary particleSTRONG-COUPLING-CONSTANT; ELECTRON-POSITRON ANNIHILATION; LUND MONTE-CARLO; FREE PERTURBATION-THEORY; 2ND ORDER QCD; E+E-ANNIHILATION; QUANTUM CHROMODYNAMICS; ALPHA-S; FRAGMENTATION MODELS; JET FRAGMENTATIONFRAGMENTATION MODELS01 natural sciencesJET FRAGMENTATIONNuclear physicsParticle decay0103 physical sciencesSTRONG-COUPLING-CONSTANTALPHA-S010306 general physicsNuclear ExperimentELECTRON-POSITRON ANNIHILATIONQuantum chromodynamicsCoupling constantPhysicsQUANTUM CHROMODYNAMICSAnnihilation010308 nuclear & particles physicsE+E-ANNIHILATIONFREE PERTURBATION-THEORYPhysique des particules élémentairesFísica nuclearHigh Energy Physics::ExperimentParticle Physics - Experiment
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Measurement of the semileptonic charge asymmetry in B-0 meson mixing with the D0 detector

2012

We present a measurement of the semileptonic mixing asymmetry for B0 mesons, a^d_{sl}, using two independent decay channels: B0 -> mu+D-X, with D- -> K+pi-pi-; and B0 -> mu+D*-X, with D*- -> antiD0 pi-, antiD0 -> K+pi- (and charge conjugate processes). We use a data sample corresponding to 10.4 fb^{-1} of ppbar collisions at sqrt(s) = 1.96 TeV, collected with the D0 experiment at the Fermilab Tevatron collider. We extract the charge asymmetries in these two channels as a function of the visible proper decay length (VPDL) of the B0 meson, correct for detector-related asymmetries using data-driven methods, and account for dilution from charge-symmetric processes using Monte Car…

Nuclear and High Energy PhysicsParticle physicsMesonmedia_common.quotation_subjectMonte Carlo methodTevatronFOS: Physical sciences01 natural sciencesAsymmetryHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsCollidermedia_commonPhysics010308 nuclear & particles physicsCharge (physics)B-factoryExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentPACS numbers: 11.30.Er 12.15.Ff 14.40.Nd
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A novel method for modeling the recoil in W boson events at hadron collider

2009

We present a new method for modeling the hadronic recoil in W->lnu events produced at hadron colliders. The recoil is chosen from a library of recoils in Z->ll data events and overlaid on a simulated W->lnu event. Implementation of this method requires that the data recoil library describe the properties of the measured recoil as a function of the true, rather than the measured, transverse momentum of the boson. We address this issue using a multidimensional Bayesian unfolding technique. We estimate the statistical and systematic uncertainties from this method for the W boson mass and width measurements assuming 1 fb-1 of data from the Fermilab Tevatron. The uncertainties are found…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHadronMonte Carlo methodTevatronFOS: Physical sciences01 natural sciences7. Clean energylaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Recoillaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderNuclear ExperimentInstrumentationBosonPhysicsLarge Hadron Collider010308 nuclear & particles physicsExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::Experiment
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Overview of the high-level trigger electron and photon selection for the ATLAS experiment at the LHC

2005

texte intégral : http://cdsweb.cern.ch/record/846438; The ATLAS experiment at the Large Hadron Collider (LHC) will face the challenge of efficiently selecting interesting candidate events in$pp$collisions at 14 TeV center-of-mass energy, whilst rejecting the enormous number of background events. The High-Level Trigger (HLT$=$second level trigger and Event Filter), which is a software based trigger will need to reduce the level-1 output rate of$approx75$kHz to$approx200$Hz written out to mass storage. In this talk an overview of the current physics and system performance of the HLT selection for electrons and photons is given. The performance has been evaluated using Monte Carlo simulations …

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsMonte Carlo method02 engineering and technologyElectron01 natural sciencesAtlas (anatomy)Nuclear electronics0103 physical sciences0202 electrical engineering electronic engineering information engineeringmedicine[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic EngineeringDetectors and Experimental TechniquesPhysicsLarge Hadron Collider010308 nuclear & particles physicsEvent (computing)ATLAS experiment020206 networking & telecommunicationsATLASHigh Level TriggerPhotonmedicine.anatomical_structureNuclear Energy and EngineeringFilter (video)Energy (signal processing)14th IEEE-NPSS Real Time Conference, 2005.
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Measurement of the top quark mass in the dilepton channel

2007

We present a measurement of the top quark mass in the dilepton channel based on approximately 370/pb of data collected by the D0 experiment during Run II of the Fermilab Tevatron collider. We employ two different methods to extract the top quark mass. We show that both methods yield consistent results using ensemble tests of events generated with the D0 Monte Carlo simulation. We combine the results from the two methods to obtain a top quark mass m_t = 178.1 +/- 8.2 GeV. The statistical uncertainty is 6.7 GeV and the systematic uncertainty is 4.8 GeV.

Nuclear and High Energy PhysicsParticle physicsTop quarkMonte Carlo methodTevatronFOS: Physical sciences01 natural sciencesBottom quarkHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Atomic and Molecular ClustersFermilab010306 general physicsColliderNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyD0 experimentNonlinear Sciences::Exactly Solvable and Integrable SystemsExperimental High Energy PhysicsHigh Energy Physics::ExperimentCommunication channel
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Electron and Photon Identification in the D0 Experiment

2013

The electron and photon reconstruction and identification algorithms used by the D0 Collaboration at the Fermilab Tevatron collider are described. The determination of the electron energy scale and resolution is presented. Studies of the performance of the electron and photon reconstruction and identification are summarized.

Nuclear and High Energy PhysicsPhotonMonte Carlo methodTevatronFOS: Physical sciencesElectron01 natural sciencesHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderInstrumentationPhysics010308 nuclear & particles physicsResolution (electron density)D0 experiment3. Good healthExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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The Endcap Disc DIRC of PANDA

2017

Abstract The Endcap Disc DIRC (EDD) for PANDA has been designed to identify traversing pions, kaons and protons in the future PANDA experiment. Its central part is a 2 cm thick fused silica plate. Focussing optics are attached to the outer rim of the plate, outside of the acceptance of the experiment. Fast, high-resolution MCP-PMTs, designed to register single Cherenkov photons, have been tested in magnetic field. Filters limit the spectral acceptance of the sensors to reduce dispersion effects and to extend their lifetime. A compact and fast readout is realized with ASICs. Analytical reconstruction algorithms allow for fast particle identification. The angular resolution of a DIRC prototyp…

Nuclear and High Energy PhysicsPhotonPhysics::Instrumentation and DetectorsCherenkov detectorMonte Carlo method01 natural sciencesParticle identificationParticle detector030218 nuclear medicine & medical imaginglaw.inventionNuclear physics03 medical and health sciences0302 clinical medicineOpticslaw0103 physical sciencesAngular resolutionNuclear ExperimentInstrumentationCherenkov radiationPhysics010308 nuclear & particles physicsbusiness.industryDetectorHigh Energy Physics::ExperimentbusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Demonstration of the event identification capabilities of the NEXT-White detector

2019

[EN] In experiments searching for neutrinoless double-beta decay, the possibility of identifying the two emitted electrons is a powerful tool in rejecting background events and therefore improving the overall sensitivity of the experiment. In this paper we present the first measurement of the efficiency of a cut based on the different event signatures of double and single electron tracks, using the data of the NEXT-White detector, the first detector of the NEXT experiment operating underground. Using a 228Th calibration source to produce signal-like and background-like events with energies near 1.6 MeV, a signal efficiency of 71.6 ± 1.5 stat ± 0.3 sys% for a background acceptance of 20.6 ± …

Nuclear and High Energy PhysicsPhysical measurementsPhysics - Instrumentation and DetectorsMonte Carlo methodExtrapolationFísica -- MesuramentsFOS: Physical sciences7. Clean energy01 natural sciencesAtomicMathematical SciencesHigh Energy Physics - ExperimentNuclear physicsTECNOLOGIA ELECTRONICAHigh Energy Physics - Experiment (hep-ex)Particle and Plasma PhysicsDouble beta decay0103 physical sciencesDark Matter and Double Beta Decay (experiments)Calibrationlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclearCalibratge010306 general physicsNuclear ExperimentMathematical PhysicsPhysicsQuantum Physics010308 nuclear & particles physicsDetectorMolecularDetectorsInstrumentation and Detectors (physics.ins-det)Nuclear & Particles PhysicsCalibrationPhysical Scienceslcsh:QC770-798High Energy Physics::ExperimentSensitivity (electronics)Event (particle physics)Energy (signal processing)
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Characterization of a cylindrical plastic {\beta}-detector with Monte Carlo simulations of optical photons

2017

V. Guadilla et al. -- 5 pags., 8 figs., tab.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonTotal absorption spectroscopyoptical photonsTotal absorption spectroscopyMonte Carlo method[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesElectromagnetic radiationMonte Carlo simulationsOptics0103 physical sciencesPlastic scintillators[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]plastic scintillators010306 general physicsAbsorption (electromagnetic radiation)Nuclear ExperimentInstrumentationPhysicsSpectrometerta114010308 nuclear & particles physicsbusiness.industryDetectortotal absorption spectroscopyComputational physicsOptical photonsDynamic Monte Carlo methodbusiness
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