Search results for " electromagnetic"

showing 10 items of 102 documents

“Symptoms associated with environmental factors” (SAEF) – Towards a paradigm shift regarding “idiopathic environmental intolerance” and related pheno…

2020

Health conditions characterized by symptoms associated with chemical, physical and biological environmental factors unrelated to objectifiable pathophysiological mechanisms are often labelled by the general term “idiopathic environmental intolerances”. More specific, exposure-related terms are also used, e.g. “multiple chemical sensitivities”, “electromagnetic hypersensitivity” and “candidiasis hypersensitivity”. The prevalence of the conditions varies from a few up to more than 50%, depending on definitions and populations. Based on evolving knowledge within this field, we provide arguments for a paradigm shift from terms focusing on exposure and intolerance/(hyper-)sensitivity towards a t…

Nocebomedia_common.quotation_subjectPSYCHOLOGICAL MECHANISMSMultiple chemical sensitivitiesILLNESSREPORTED SYMPTOMSPsykiatriElectromagnetic hypersensitivityEMF03 medical and health sciences0302 clinical medicineMEDIA REPORTSPerceptionHealth careElectromagnetic hypersensitivitymedicineVDP::Medisinske Fag: 700Paradigm shiftEXPOSURE030212 general & internal medicineHEALTH WORRIESHYPERSENSITIVITYmedia_commonPsychiatryScience & TechnologyHealth professionalsbusiness.industryNoceboparadigm shift ; electromagnetic hypersensitivity ; multiple chemical sensitivities ; environmental sensitivities ; symptom perception ; NoceboELECTROMAGNETIC-FIELDSIdiopathic environmental intoleranceEnvironmental sensitivitiesPREVALENCEPeer reviewVDP::Medical disciplines: 700Psychiatry and Mental healthClinical PsychologyParadigm shiftSymptom perceptionmedicine.symptomPsychologybusinessLife Sciences & Biomedicine030217 neurology & neurosurgeryClinical psychologyJournal of Psychosomatic Research
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Diquark correlations in hadron physics: Origin, impact and evidence

2020

The last decade has seen a marked shift in how the internal structure of hadrons is understood. Modern experimental facilities, new theoretical techniques for the continuum bound-state problem and progress with lattice-regularised QCD have provided strong indications that soft quark+quark (diquark) correlations play a crucial role in hadron physics. For example, theory indicates that the appearance of such correlations is a necessary consequence of dynamical chiral symmetry breaking, viz. a corollary of emergent hadronic mass that is responsible for almost all visible mass in the universe; experiment has uncovered signals for such correlations in the flavour-separation of the proton's elect…

Nuclear TheoryHigh Energy Physics::LatticeHadronNuclear Theoryhiukkasfysiikka01 natural sciencesHigh Energy Physics - ExperimentBroad spectrumHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysicsDiquark correlationsBaryon spectra and structureHigh Energy Physics - Lattice (hep-lat)symmetry breaking: chiralDyson-Schwinger equationsDiquarkbound statediquark: correlationHigh Energy Physics - PhenomenologyQuark modelsChiral symmetry breakingPhenomenology (particle physics)QuarkNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]diquark correlationsNuclear Theory (nucl-th)High Energy Physics - Latticehadron physics0103 physical sciencesquantum chromodynamics010306 general physicsBaryon spectra and structure; Diquark correlations; Dyson-Schwinger equations; Lattice quantum chromodynamics; Quantum chromodynamics; Quark modelskvarkit010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]hadron spectroscopyHigh Energy Physics::PhenomenologyLattice quantum chromodynamicsform factor: electromagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Measurement of the phase between strong and electromagnetic amplitudes of J/ψ decays

2019

Kolcu, Onur Buğra (Arel Author)

Nuclear and High Energy PhysicsJ/Psi decayElectron–positron annihilationBESIII; Electromagnetic amplitude; J/ψ decay; Phase; Strong amplitude; High Energy Physics - Experiment; High Energy Physics - Experiment01 natural sciencesHigh Energy Physics - ExperimentNOSubatomär fysikSubatomic Physics0103 physical sciencesJ/ψ decayStrong amplitudeBorn approximation010306 general physicsPhysicsBESIII Electromagnetic amplitude J/ψ decay Phase Strong amplitudeAnnihilation010308 nuclear & particles physicsBranching fractionBESIIIlcsh:QC1-999BESIII; Electromagnetic amplitude; J/ψ decay; Phase; Strong amplitudeAmplitudeElectromagnetic amplitudePhaseHigh Energy Physics::ExperimentRelative phaseAtomic physicsJ/Psi Decaylcsh:Physics
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Measurements of Sigma(+) and Sigma(-) time-like electromagnetic form factors for center-of-mass energies from 2.3864 to 3.0200 GeV

2021

Physics letters / B 814, 136110 (2021). doi:10.1016/j.physletb.2021.136110

Nuclear and High Energy Physicselectric [form factor]Electron–positron annihilationFOS: Physical sciencesSigma hyperonannihilation [electron positron]BESIII; Cross section; Electromagnetic form factor; Σ hyperonhyperon53001 natural sciencesHigh Energy Physics - ExperimentNOSubatomär fysikHigh Energy Physics - Experiment (hep-ex)Angular distributionAstronomi astrofysik och kosmologi0103 physical sciencesSubatomic PhysicsAstronomy Astrophysics and Cosmologyddc:530angular distributionstructure010306 general physicsElectromagnetic form factorPhysics2.3864-3.0200 GeV-cmsBESelectron positron --> Sigma+ Sigma-Cross section010308 nuclear & particles physicsHyperonBESIIIBeijing Storlcsh:QC1-999Sigma HyperonBaryonΣ hyperonmagnetic [form factor]ratio [form factor]valence [quark]colliding beams [electron positron]High Energy Physics::Experimentpair production [Sigma+]Atomic physicsform factor [Sigma-]electromagnetic [form factor]lcsh:Physicsform factor [Sigma+]experimental results
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Numerical Investigations of an Implicit Leapfrog Time-Domain Meshless Method

2014

Numerical solution of partial differential equations governing time domain simulations in computational electromagnetics, is usually based on grid methods in space and on explicit schemes in time. A predefined grid in the problem domain and a stability step size restriction need. Recently, the authors have reformulated the meshless framework based on smoothed particle hydrodynamics, in order to be applied for time domain electromagnetic simulation. Despite the good spatial properties, the numerical explicit time integration introduces, also in a meshless context, a severe constraint. In this paper, at first, the stability condition is addressed in a general way by allowing the time step inc…

Numerical AnalysisRegularized meshless methodApplied MathematicsMeshless methodsMathematical analysisGeneral EngineeringGridTheoretical Computer ScienceComputational MathematicsAlternating direction implicit methodSettore MAT/08 - Analisi NumericaSettore ING-IND/31 - ElettrotecnicaComputational Theory and MathematicsProblem domainADI leapfrog methodSmoothed particle electromagneticsComputational electromagneticsMeshfree methodsTime domainSoftwareMathematicsNumerical partial differential equations
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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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High-Precision Determination of the Electric and Magnetic Form Factors of the Proton

2010

New precise results of a measurement of the elastic electron-proton scattering cross section performed at the Mainz Microtron MAMI are presented. About 1400 cross sections were measured with negative four-momentum transfers squared up to Q^2=1 (GeV/c)^2 with statistical errors below 0.2%. The electric and magnetic form factors of the proton were extracted by fits of a large variety of form factor models directly to the cross sections. The form factors show some features at the scale of the pion cloud. The charge and magnetic radii are determined to be r_E=0.879(5)(stat.)(4)(syst.)(2)(model)(4)(group) fm and r_M=0.777(13)(stat.)(9)(syst.)(5)(model)(2)(group) fm.

Particle physicsProtonMesonelastic electron scattering13.40.Gp 14.20.Dh 25.30.BfHadronGeneral Physics and AstronomyFOS: Physical sciencesElementary particle[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicselastic electron scattering; proton electromagnetic form factors010308 nuclear & particles physicsForm factor (quantum field theory)Charge (physics)NATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Crystallographyproton electromagnetic form factorsHigh Energy Physics::ExperimentNucleonDimensionless quantity
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Accelerated stabilization of coherent photon states

2018

| openaire: EC/H2020/681311/EU//QUESS Control and utilization of coherent states of microwave photons is a ubiquitous requirement for the present and near-future implementations of solid-state quantum computers. The rate at which the photon state responds to external driving is limited by the relaxation rate of the storage resonator, which poses a trade-off between fast control and long storage time. Here, we present a control scheme that is designed to drive an unknown photon state to a desired coherent state much faster than the resonator decay rate. Our method utilizes a tunable environment which acts on an ancillary qubit coupled to the resonator. By periodically resetting the qubit and…

PhotonDephasingGeneral Physics and Astronomy02 engineering and technologycoherent statescircuit quantum electrodynamics7. Clean energy01 natural sciencesResonatorphoton statesCircuit quantum electrodynamics0103 physical scienceskvanttifysiikka010306 general physicsQuantum computerPhysicsfotonitbusiness.industryResonator mode021001 nanoscience & nanotechnologyquantum information processingtunable electromagnetic environmentsQubitOptoelectronicsCoherent statesquantum state preparationdissipative quantum systems0210 nano-technologybusinessquantum control
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Extraction of the Muon Signals Recorded with the Surface Detector of the Pierre Auger Observatory Using Recurrent Neural Networks

2021

The Pierre Auger Observatory, at present the largest cosmic-ray observatory ever built, is instrumented with a ground array of 1600 water-Cherenkov detectors, known as the Surface Detector (SD). The SD samples the secondary particle content (mostly photons, electrons, positrons and muons) of extensive air showers initiated by cosmic rays with energies ranging from $10^{17}~$eV up to more than $10^{20}~$eV. Measuring the independent contribution of the muon component to the total registered signal is crucial to enhance the capability of the Observatory to estimate the mass of the cosmic rays on an event-by-event basis. However, with the current design of the SD, it is difficult to straightfo…

PhotonPhysics::Instrumentation and DetectorsAstronomyElectron01 natural sciencesHigh Energy Physics - ExperimentAugerHigh Energy Physics - Experiment (hep-ex)mass [cosmic radiation]surface [detector]Observatory[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]photon: cosmic radiationInstrumentationMathematical PhysicsPhysicsAGASAPhysicsSettore FIS/01 - Fisica SperimentaleDetectorcosmic radiation [photon]Astrophysics::Instrumentation and Methods for AstrophysicsMonte Carlo [numerical calculations]electromagnetic [showers]Augerobservatorycosmic radiation [electron]Analysis and statistical methodsnumerical calculations: Monte CarloAnalysis and statistical methodperformancepositron: cosmic radiationatmosphere [showers]Cherenkov detectordata analysis methodAnalysis and statistical methods; Calibration and fitting methods; Cherenkov detectors; Cluster finding; Large detector systems for particle and astroparticle physics; Pattern recognitionCherenkov counter: waterairneural networkAstrophysics::High Energy Astrophysical Phenomena610FOS: Physical sciencesCosmic raycosmic radiation [positron]cosmic radiation: massCalibration and fitting methodNuclear physicsstatistical analysisPattern recognition0103 physical sciencesshowers: electromagneticddc:530ddc:610High Energy Physics010306 general physicsZenithPierre Auger ObservatoryCalibration and fitting methodscosmic radiation [muon]Muonshowers: atmosphere010308 nuclear & particles physicsdetector: surfacehep-exLarge detector systems for particle and astroparticle physicswater [Cherenkov counter]Cherenkov detectorsCluster findingelectron: cosmic radiationRecurrent neural networkmuon: cosmic radiationLarge detector systems for particle and astroparticle physicExperimental High Energy PhysicsHigh Energy Physics::ExperimentRAIOS CÓSMICOSexperimental results
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A detector for CLIC: main parameters and performance

2019

Together with the recent CLIC detector model CLICdet a new software suite was introduced for the simulation and reconstruction of events in this detector. This note gives a brief introduction to CLICdet and describes the CLIC experimental conditions at 380 GeV and 3 TeV, including beam-induced backgrounds. The simulation and reconstruction tools are introduced, and the physics performance obtained is described in terms of single particles, particles in jets, jet energy resolution and flavour tagging. The performance of the very forward electromagnetic calorimeters is also discussed.

Physics - Instrumentation and Detectorsbackground: inducedFOS: Physical sciencesjet: energy resolutionInstrumentation and Detectors (physics.ins-det)Advanced software [3]Accelerators and Storage RingsprogrammingHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)calorimeter: electromagneticCERN CLIC[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Accelerator PhysicsHigh Energy Physics::Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]numerical calculationsdetector: designperformance
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