Search results for "electromagnetic"

showing 10 items of 1595 documents

Photon and dilepton production rate in the quark-gluon plasma from lattice QCD

2023

The photon emissivity of the quark-gluon plasma (QGP) is an important input to predict the photon yield in heavy-ion collisions, particularly for transverse momenta in the range of 1 to 2 GeV. Photon production in the QGP can be probed non-perturbatively in lattice QCD via (Euclidean) time-dependent correlators. Analyzing the spatially transverse channel, as well as the difference of the transverse and longitudinal channels as a consistency check, we determine the photon emissivity based on continuum-extrapolated correlators in two-flavour QCD. Estimates of the lepton-pair production rate can be derived by combining the two aforementioned channels. © Copyright owned by the author(s) under t…

PhotonsColliding beam acceleratorElectromagnetic wave emissionHeavy ion
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Subpicosecond transient signal spectroscopy of Prodan in dimethylformamide solution.

2008

We report a pump-probe experiment revealing the temporal evolution of subpicosecond evolution of Prodan's excited-state absorption in dimethylformamide. Also, we present calculation of the first spectral moment of this spectral band and estimation of different relaxation components on the subpicosecond time scale.

PhotonsModels StatisticalTime FactorsChemistryPhotochemistryGeneral NeuroscienceLasersRelaxation (NMR)Analytical chemistryDimethylformamideSpectral bandsEquipment DesignMolecular physicsGeneral Biochemistry Genetics and Molecular BiologyAbsorptionchemistry.chemical_compoundKineticsSpectrometry FluorescenceHistory and Philosophy of Science2-NaphthylamineDimethylformamideSpectroscopyAbsorption (electromagnetic radiation)Transient signalFluorescent DyesAnnals of the New York Academy of Sciences
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Red Spectral Forms of Chlorophylls in Green Plant PSI - A Site-Selective and High-Pressure Spectroscopy Study

2003

One of the special spectroscopic characteristics of photosystem I (PSI) complexes is that they possess absorption and emission bands at lower energy than those of the reaction center. In this paper, the red pigment pools of PSI-200, PSI-core, and LHCI complex from Arabidopsis thaliana have been characterized at low temperatures by means of spectrally selective (hole-burning and fluorescence line-narrowing) and high-pressure spectroscopic techniques. It was shown that the green plant PSI-200 complex has at least three red pigment pools, from which two are located in the PSI-core and one, in the peripheral light-harvesting complex I (LHCI). All of the red pigment pools are characterized by st…

Photosynthetic reaction centrePhysics::Biological PhysicsChlorophyll a/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyAnalytical chemistryAstrophysics::Cosmology and Extragalactic AstrophysicsPhotosystem IPhotosynthesisSurfaces Coatings and Filmschemistry.chemical_compoundPigmentchemistryAbsorption bandvisual_artMaterials Chemistryvisual_art.visual_art_mediumAstrophysics::Solar and Stellar AstrophysicsSDG 7 - Affordable and Clean EnergyPhysical and Theoretical ChemistrySpectroscopyAbsorption (electromagnetic radiation)
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Dynamic stabilization of the magnetic field surrounding the neutron electric dipole moment spectrometer at the Paul Scherrer Institute

2014

The Surrounding Field Compensation (SFC) system described in this work is installed around the four-layer Mu-metal magnetic shield of the neutron electric dipole moment spectrometer located at the Paul Scherrer Institute. The SFC system reduces the DC component of the external magnetic field by a factor of about 20. Within a control volume of approximately 2.5m x 2.5m x 3m disturbances of the magnetic field are attenuated by factors of 5 to 50 at a bandwidth from $10^{-3}$ Hz up to 0.5 Hz, which corresponds to integration times longer than several hundreds of seconds and represent the important timescale for the nEDM measurement. These shielding factors apply to random environmental noise f…

Physics - Instrumentation and DetectorsNeutron electric dipole momentAtomic Physics (physics.atom-ph)FOS: Physical sciencesGeneral Physics and AstronomyShields[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesPhysics - Atomic Physics0103 physical sciencesNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentMoore–Penrose pseudoinverse010302 applied physicsPhysics[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Spectrometermagnetic field compensation systemInstrumentation and Detectors (physics.ins-det)Magnetic fieldComputational physicsElectromagnetic shieldingDC biasJournal of Applied Physics
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Miniature Cavity-Enhanced Diamond Magnetometer

2017

We present a highly sensitive miniaturized cavity-enhanced room-temperature magnetic-field sensor based on nitrogen-vacancy (NV) centers in diamond. The magnetic resonance signal is detected by probing absorption on the 1042\,nm spin-singlet transition. To improve the absorptive signal the diamond is placed in an optical resonator. The device has a magnetic-field sensitivity of 28 pT/$\sqrt{\rm{Hz}}$, a projected photon shot-noise-limited sensitivity of 22 pT/$\sqrt{\rm{Hz}}$ and an estimated quantum projection-noise-limited sensitivity of 0.43 pT/$\sqrt{\rm{Hz}}$ with the sensing volume of $\sim$ 390 $\mu$m $\times$ 4500 $\mu$m$^{2}$. The presented miniaturized device is the basis for an e…

Physics - Instrumentation and DetectorsPhotonMaterials scienceMagnetometerGeneral Physics and AstronomyFOS: Physical sciences02 engineering and technologyengineering.material01 natural sciencesSignallaw.inventionlaw0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)[ PHYS.PHYS.PHYS-GEN-PH ] Physics [physics]/Physics [physics]/General Physics [physics.gen-ph][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsAbsorption (electromagnetic radiation)[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Quantum PhysicsCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industryDiamondInstrumentation and Detectors (physics.ins-det)021001 nanoscience & nanotechnology[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Highly sensitiveOptical cavityengineeringOptoelectronics0210 nano-technologybusinessQuantum Physics (quant-ph)Sensitivity (electronics)
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Readiness of the ATLAS liquid argon calorimeter for LHC collisions

2010

The ATLAS liquid argon calorimeter has been operating continuously since August 2006. At this time, only part of the calorimeter was readout, but since the beginning of 2008, all calorimeter cells have been connected to the ATLAS readout system in preparation for LHC collisions. This paper gives an overview of the liquid argon calorimeter performance measured in situ with random triggers, calibration data, cosmic muons, and LHC beam splash events. Results on the detector operation, timing perfor-mance, electronics noise, and gain stability are presented. High energy deposits from radiative cosmic muons and beam splash events allow to check the intrinsic constant term of the energy resolutio…

Physics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)large hadron colliderPhysics::Instrumentation and DetectorsMonte Carlo method7. Clean energy01 natural sciences010305 fluids & plasmasHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Radiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesDetectors de radiacióPhysicsLarge Hadron ColliderAcceleradors de partículesDetectorSettore FIS/01 - Fisica SperimentaleInstrumentation and Detectors (physics.ins-det)ATLASLHC Collisionsmedicine.anatomical_structurePhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCNoise (radio)chemistry.chemical_elementFOS: Physical sciencesComputer Science::Digital Libraries530Partícules (Física nuclear)Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineATLAS; liquid argon; calorimeter; LHC; collisionsFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasArgónArgonCalorimeter (particle physics)010308 nuclear & particles physicsFísicachemistryExperimental High Energy PhysicsHigh Energy Physics::Experimentelectromagnetic shower
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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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Electron performance measurements with the ATLAS detector using the 2010 LHC proton-proton collision data

2012

Acknowledgements We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; ARTEMIS, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNAS, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT, Greece; ISF, MINERVA, GIF, DIP and Benoziyo…

Physics and Astronomy (miscellaneous)ProtonPhysics::Instrumentation and DetectorsLarge hadron colliderNuclear physicsMODULE-0Electron7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentCharge (physics)Luminosity (scattering theory)High Energy Physics - Experiment (hep-ex)ELECTROMAGNETIC CALORIMETER[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]GeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Detectors de radiacióddc:539PhysicsLuminosity (scattering theory)Large Hadron ColliderResolution (electron density)PhysicsSettore FIS/01 - Fisica SperimentaleDetectorResolution (electron density)LinearityATLASATLAS detector; LHC; proton-proton collision8. Economic growthPhysical SciencesFísica nuclearLHCProtonParticle Physics - ExperimentCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530ElectronPartícules (Física nuclear)Nuclear physicsACELERADOR DE PARTÍCULASLinearity0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Science & Technology010308 nuclear & particles physicsFísicaCharge (physics)DetectorCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::Experiment
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Excitonic absorption and Urbach's tail in bismuth sulfide single crystals

1988

The absorption coefficient of bismuth sulfide single crystals has been measured through more than four orders of magnitude and in the range of energies from 1.25 to 1.70 eV. A detailed study as a function of temperature has been carried out from 29 to 300 K. An Urbach tail for low values of absorption has been found. This tail and its temperature evolution fit the expression for ionic materials. An excitonic region appears at low temperature and the shape of the exciton peak is Gaussian, which corresponds to a strong exciton-phonon coupling. The exciton binding energy is estimated (28±3 meV) and then the energy gap at 29 K is obtained (Eg=1.523±0.003 eV). The fundamental electronic transiti…

Physics and Astronomy (miscellaneous)business.industryChemistryBand gapExcitonGeneral EngineeringGeneral ChemistryMolecular physicsMolecular electronic transitionOpticsAbsorption edgeAttenuation coefficientAbsorptanceGeneral Materials SciencebusinessAbsorption (electromagnetic radiation)Single crystalApplied Physics A: Solids and Surface
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Limiting neutrino magnetic moments with Borexino Phase-II solar neutrino data

2017

A search for the solar neutrino effective magnetic moment has been performed using data from 1291.5 days exposure during the second phase of the Borexino experiment. No significant deviations from the expected shape of the electron recoil spectrum from solar neutrinos have been found, and a new upper limit on the effective neutrino magnetic moment of $\mu_{\nu}^{eff}$ $<$ 2.8$\cdot$10$^{-11}$ $\mu_{B}$ at 90\% c.l. has been set using constraints on the sum of the solar neutrino fluxes implied by the radiochemical gallium experiments.Using the limit for the effective neutrino moment, new limits for the magnetic moments of the neutrino flavor states, and for the elements of the neutrino magne…

Physics and Astronomy (miscellaneous)neutrino: solarPhysics::Instrumentation and DetectorsSolar neutrino01 natural sciencesHigh Energy Physics - ExperimentNeutrino detectorHigh Energy Physics - Experiment (hep-ex)SPIN ROTATIONHigh Energy Physics - Phenomenology (hep-ph)electron: recoil[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Astrophysics::Solar and Stellar AstrophysicsBorexinoS066MGMgalliumPhysicsMagnetic momentneutrino: magnetic momentHigh Energy Physics - Phenomenologyneutrino: momentNeutrino detectorneutrino: flavorneutrino: MajoranaMeasurements of neutrino speedBorexinoNeutrinoupper limitParticle physicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesSolar neutrinoDECAYSMagnetic momentNuclear physicsstatistical analysis[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesddc:530010306 general physicsNeutrino oscillationDETECTORELECTROMAGNETIC PROPERTIES010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySolar neutrino problemMAJORANA NEUTRINOS[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]electron: energy spectrum[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentexperimental resultsPhysical Review D
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