Search results for "energy loss"

showing 9 items of 59 documents

Large bulk Micromegas detectors for TPC applications

2009

A large volume TPC will be used in the near future in a variety of experiments including T2K. The bulk Micromegas detector for this TPC is built using a novel production technique particularly suited for compact, thin and robust low mass detectors. The capability to pave a large Surface with a simple mounting Solution and small dead space is of particular interest for these applications. We have built several large bulk Micromegas detectors (36 x 34 cm(2)) and we have tested one in the former HARP field cage with a magnetic field. Prototypes cards of the T2K front end electronics, based on the AFTER ASIC chip, have been used in this TPC test for the first time. Cosmic ray data have been acq…

T2KPhysicsNuclear and High Energy PhysicsEnergy lossField (physics)Physics::Instrumentation and Detectorsbusiness.industryDetectorMicroMegas detectorCosmic rayNuclear physicsOpticsApplication-specific integrated circuitPoint (geometry)TPCbusinessInstrumentationMicromegasHARPNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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First results on ProtoDUNE-SP liquid argon time projection chamber performance from a beam test at the CERN Neutrino Platform

2020

The ProtoDUNE-SP detector was constructed and operated on the CERN Neutrino Platform. We thank the CERN management for providing the infrastructure for this experiment and gratefully acknowledge the support of the CERN EP, BE, TE, EN, IT and IPT Departments for NP04/ProtoDUNE-SP. This documentwas prepared by theDUNEcollaboration using the resources of the Fermi National Accelerator Laboratory (Fermilab), a U.S. Department of Energy, Office of Science, HEP User Facility. Fermilab is managed by Fermi Research Alliance, LLC (FRA), acting under Contract No. DE-AC02-07CH11359. This work was supported by CNPq, FAPERJ, FAPEG and FAPESP, Brazil; CFI, IPP and NSERC, Canada; CERN; MSMT, Czech Republi…

TechnologyHIGH-ENERGYPhysics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsfar detectorbeam transportNoble liquid detectors (scintillation ionization double-phase)Cms Experıment01 natural sciences7. Clean energy09 EngineeringParticle identificationHigh Energy Physics - Experiment030218 nuclear medicine & medical imagingHigh Energy Physics - Experiment (hep-ex)0302 clinical medicineNoble liquid detectors (scintillationDetectors and Experimental TechniquesInstrumentationInstruments & Instrumentationphysics.ins-dettime resolutionMathematical PhysicsPhysics02 Physical SciencesTime projection chamberLarge Hadron ColliderDetectorInstrumentation and Detectors (physics.ins-det)double-phase)Nuclear & Particles PhysicsLIGHTNeutrinoParticle Physics - ExperimentperformanceNoble liquid detectors(scintillation ionization double-phase)noiseCERN LabLarge detector systems for particle and astroparticle physics Noble liquid detectors (scintillation ionization double-phase) Time projection Chambers (TPC)530 Physicsenergy lossTime projection chambersFOS: Physical sciencesParticle detectorNuclear physics03 medical and health sciencesneutrino: deep underground detector0103 physical sciencesionizationDeep Underground Neutrino ExperimentHigh Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]signal processingactivity reportScience & Technology010308 nuclear & particles physicshep-exLarge detector systems for particle and astroparticle physicsTime projection Chambers (TPC)530 Physiksensitivitycalibrationtime projection chamber: liquid argonExperimental High Energy PhysicsLarge detector systems for particle and astroparticle physicsingle-phase)Large detector systems for particle and astroparticle physics; Noble liquid detectors (scintillation ionization double-phase); Time projection Chambers (TPC)High Energy Physics::Experimentphoton: detectorparticle identificationcharged particle: irradiationBeam (structure)
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Carbon Nano-onions: Potassium Intercalation and Reductive Covalent Functionalization

2021

Herein we report the synthesis of covalently functionalized carbon nano-onions (CNOs) via a reductive approach using unprecedented alkali-metal CNO intercalation compounds. For the first time, an in situ Raman study of the controlled intercalation process with potassium has been carried out revealing a Fano resonance in highly doped CNOs. The intercalation was further confirmed by electron energy loss spectroscopy and X-ray diffraction. Moreover, the experimental results have been rationalized with DFT calculations. Covalently functionalized CNO derivatives were synthesized by using phenyl iodide and n-hexyl iodide as electrophiles in model nucleophilic substitution reactions. The functiona…

Thermogravimetric analysisIodideIntercalation (chemistry)02 engineering and technology010402 general chemistryPhotochemistry01 natural sciences7. Clean energyBiochemistryArticleCatalysissymbols.namesakeColloid and Surface ChemistryNucleophilic substitutionchemistry.chemical_classificationElectron energy loss spectroscopytechnology industry and agricultureGeneral Chemistry021001 nanoscience & nanotechnologyEspectroscòpia Raman0104 chemical scienceschemistryCovalent bondsymbolsSurface modificationMaterials nanoestructurats0210 nano-technologyRaman spectroscopyJournal of the American Chemical Society
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Use of transmission electron microscopy to obtain quantitative information about polymers

2005

In the polymer field the electron microscope is frequently used as a tool for obtaining purely qualitative data, but only rarely to obtain quantitative information. In order to discuss the potential of this instrument for the latter purpose it is convenient to separate the discussion into the following sub-sections.

chemistry.chemical_classificationMaterials sciencechemistryTransmission electron microscopylawElectron energy loss spectroscopyAnalytical chemistryIsothermal crystallizationEnergy filtered transmission electron microscopyPolymerElectron microscopeBiological systemlaw.invention
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Synthesis of a quenchable high-pressure form of magnetite (h-Fe3O4) with composition Fe1(Fe2+0.75Mg0.26)Fe2(Fe3+0.70Cr0.15Al0.11Si0.04)2O4

2014

We report the synthesis of h-magnetite, ideally h-Fe 3 O 4 with considerable amounts of substitutional cations (Cr, Mg, Al, Si) and quenchable to ambient conditions. Two types of experiments were performed at 18 GPa and 1800 °C in a multi-anvil press. In one, we used an oxide mixture with a majoritic stoichiometry Mg 1.8 Fe 1.2 (Al 1.4 Cr 0.2 Si 0.2 Mg 0.2 )Si 3 O 12 , with Si and Mg in excess as starting material (MA-367, MA-380). In the second type of experiment (MA-376), we started from an oxide mixture on the composition of the Fe-oxide phase obtained in MA-367. The Fe-oxide phases of both experiments were investigated by electron microprobe and transmission electron microscopy includin…

chemistry.chemical_compoundCrystallographyGeophysicsElectron diffractionGeochemistry and PetrologyChemistryElectron energy loss spectroscopyFormula unitPhase (matter)OxideElectron microprobeWadsleyiteStishoviteAmerican Mineralogist
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Summary of Week VII

2018

International audience; Week VII of the INT program 2018 “Probing Nucleons and Nuclei in High Energy Collisions” was dedicated to topics at the interface of the electron-ion collider (EIC), heavy ion and proton-nucleus collisions. The EIC will provide complementary tools to investigate and constrain the initial state in HIC collisions, as well as transport properties of QCD matter which can be extracted from observables that are sensitive to final states interactions such as pt-broadening and energy loss. The contributed talks and discussions covered a variety of physics topics from saturation physics and the origin of multi-particle correlations in HIC to jet quenching and the strong coupl…

energy: highsmall-x physicsenergy losssaturationnucleuselectron nucleon: colliding beamselectron nucleusfinal-state interactionjet quenchingcorrelation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Jetsstrong couplingtransport theoryholographyjet: quenchingNuclear Experimentnuclear PDFinitial statequantum chromodynamics: matter
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Revealing lattice disorder, oxygen incorporation and pore formation in laser induced two-photon oxidized graphene

2019

Abstract Laser induced two-photon oxidation has proven to be a reliable method to pattern and control the level of oxidation of single layer graphene, which in turn allows the development of graphene-based electronic and optoelectronic devices with an all-optical method. Here we provide a full structural and chemical description of modifications of air-suspended graphene during the oxidation process. By using different laser irradiation doses, we were able to show via transmission electron microscopy, electron energy loss spectroscopy, electron diffraction and Raman spectroscopy how graphene develops from its pristine form up to a completely oxidized, porous and amorphous carbon layer. Furt…

hapetusMaterials sciencesäteilytysEELSOxide02 engineering and technology010402 general chemistryelektronit01 natural scienceslaw.inventionchemistry.chemical_compoundsymbols.namesakeraman spectroscopylawphotonsGeneral Materials Scienceta116energiafotonitta114irradiationGrapheneElectron energy loss spectroscopygrafeenioksidiGeneral Chemistry021001 nanoscience & nanotechnologyLaserphoto-oxidation0104 chemical scienceslaseritchemistryElectron diffractionChemical engineeringAmorphous carbonoxidation (active)Transmission electron microscopysymbolsTEMgraphene oxideelectron diffraction0210 nano-technologyRaman spectroscopylasersCarbon
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Event-by-event picture for the medium-induced jet evolution

2016

We discuss the evolution of an energetic jet which propagates through a dense quark-gluon plasma and radiates gluons due to its interactions with the medium. Within perturbative QCD, this evolution can be described as a stochastic branching process, that we have managed to solve exactly. We present exact, analytic, results for the gluon spectrum (the average gluon distribution) and for the higher n-point functions, which describe correlations and fluctuations. Using these results, we construct the event-by-event picture of the gluon distribution produced via medium-induced gluon branching. In contrast to what happens in a usual QCD cascade in vacuum, the medium-induced branchings are quasi-…

heavy ion: scatteringNuclear Theoryn-point functionHigh Energy Physics::LatticeNuclear TheoryPartonJet (particle physics)gluon: multiplicity01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)scaling: KNONuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]quark gluon: plasmamedia_commonQuantum chromodynamicsPhysicsPhysicsgluon: productionPerturbative QCDmatter: effectjet: asymmetrycascadeHigh Energy Physics - PhenomenologyCERN LHC CollNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]media_common.quotation_subjectQC1-999energy lossFOS: Physical sciencesjet: correlationformulaAsymmetryNuclear physicsNuclear Theory (nucl-th)gluon: spectrum0103 physical sciencesquantum chromodynamicsstochasticquantum chromodynamics: perturbation theory010306 general physicsScalingBranching processquantum chromodynamics: matterta114010308 nuclear & particles physicsgluon: fluctuationHigh Energy Physics::Phenomenologydijet: asymmetrygluon distributionGluonjet: energy losscorrelation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasma[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]gluon: radiationHigh Energy Physics::Experimentjet: quenchingEvent (particle physics)jet evolution
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Extracting qˆ in event-by-event hydrodynamics and the centrality/energy puzzle

2017

In our analysis, we combine event-by-event hydrodynamics, within the EKRT formulation, with jet quenching -ASW Quenching Weights- to obtain high- for charged particles at RHIC and LHC energies for different centralities. By defining a K-factor that quantifies the departure of from an ideal estimate, , we fit the single-inclusive experimental data for charged particles. This K-factor is larger at RHIC than at the LHC but, surprisingly, it is almost independent of the centrality of the collision. peerReviewed

jet quenchingenergy lossevent-by-event hydrodynamicsNuclear Experiment
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