Search results for "physics.ins-det"

showing 10 items of 505 documents

Comparison of different methods for evaluating the transmission function of a two-stage cylindrical mirror analizer in XPS applications

2007

Three different evaluations of the energy dependence of the transmission-detection function of a two-stage cylindrical electron analyzer have been obtained by resorting to three established procedures. Their relative merits have been tested as follows. First they have been used to correct raw XPS spectra of clean Cu, Ag and Au surfaces. Next, the secondary electron background has been subtracted using Tougaard's method. Finally, the primary electron spectra so obtained have been reanalyzed by peak area measurement in the frame of the modern formalism for quantitative XPS analysis. Ideally a constant residual value should thus be obtained. The variability of these residuals with peak energy …

Physics - Instrumentation and Detectorstwo-stage CMAtransmission function[ SPI.MAT ] Engineering Sciences [physics]/MaterialsXPSFOS: Physical sciencescylindrical mirror analyzer[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Instrumentation and Detectors (physics.ins-det)[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][SPI.MAT]Engineering Sciences [physics]/Materials
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Search for Electronic Recoil Event Rate Modulation with 4 Years of XENON100 Data

2017

We report on a search for electronic recoil event rate modulation signatures in the XENON100 data accumulated over a period of 4 years, from January 2010 to January 2014. A profile likelihood method, which incorporates the stability of the XENON100 detector and the known electronic recoil background model, is used to quantify the significance of periodicity in the time distribution of events. There is a weak modulation signature at a period of $431^{+16}_{-14}$ days in the low energy region of $(2.0-5.8)$ keV in the single scatter event sample, with a global significance of $1.9\,\sigma$, however no other more significant modulation is observed. The expected annual modulation of a dark matt…

Physics and Astronomy (all) XENON DARK MATTER MODULATION TPCPhysics - Instrumentation and DetectorsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterGeneral Physics and AstronomyFOS: Physical sciencesElectron01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Recoil0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsPseudovectorInstrumentation and Methods for Astrophysics (astro-ph.IM)Physics010308 nuclear & particles physicsDetectorInstrumentation and Detectors (physics.ins-det)Coupling (probability)ModulationAstrophysics - Instrumentation and Methods for AstrophysicsEvent (particle physics)Astrophysics - Cosmology and Nongalactic Astrophysics
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Characterization and First Test of an i-TED Prototype at CERN n_TOF

2018

International audience; Neutron capture cross section measurements are of fundamental importance for the study of the slow process of neutron capture, so called s-process. This mechanism is responsible for the formation of most elements heavier than iron in the Universe. To this aim, installations and detectors have been developed, as total energy radiation C$_{6}$ D$_{6}$ detectors. However, these detectors can not distinguish between true capture gamma rays from the sample under study and neutron induced gamma rays produced in the surroundings of the setup. To improve this situation, we propose (Domingo Pardo in Nucl Instr Meth Phys Res A 825:78–86, 2016, [1]) the use of the Compton princ…

PhysicsAstrophysics::High Energy Astrophysical PhenomenaDetectorGamma rayi-TED n_TOF characterizationNeutron radiationRadiation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]030218 nuclear medicine & medical imagingNuclear physics03 medical and health sciencesNeutron capture0302 clinical medicineNeutron cross sectionNeutronGamma spectroscopy[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]iTED n_TOF neutron
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Characterization of a Be(p,xn) Neutron Source for Fission Yields Measurements

2013

We report on measurements performed at The Svedberg Laboratory (TSL) to characterize a proton-neutron converter for independent fission yield studies at the IGISOL-JYFLTRAP facility (Jyv\"askyl\"a, Finland). A 30 MeV proton beam impinged on a 5 mm water-cooled Beryllium target. Two independent experimental techniques have been used to measure the neutron spectrum: a Time of Flight (TOF) system used to estimate the high-energy contribution, and a Bonner Sphere Spectrometer able to provide precise results from thermal energies up to 20 MeV. An overlap between the energy regions covered by the two systems will permit a cross-check of the results from the different techniques. In this paper, th…

PhysicsBonner sphereNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsSpectrometerta114010308 nuclear & particles physicsFissionNuclear TheoryNuclear dataFOS: Physical sciencesFission product yieldInstrumentation and Detectors (physics.ins-det)7. Clean energy01 natural sciencesThe Svedberg LaboratoryNuclear physics0103 physical sciencesNeutron sourceNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentNuclear Data Sheets
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Band structure tuning of Heusler compounds: Spin- and momentum-resolved electronic structure analysis of compounds with different band filling

2019

Physical review / B 103(5), 054407 (2021). doi:10.1103/PhysRevB.103.054407

PhysicsCondensed Matter - Materials SciencePhysics - Instrumentation and DetectorsValence (chemistry)Band gapPhotoemission spectroscopyMagnetismMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciences02 engineering and technologyElectronic structureInstrumentation and Detectors (physics.ins-det)021001 nanoscience & nanotechnology01 natural sciences530Brillouin zoneCrystallographyFerromagnetism0103 physical sciencesddc:530Condensed Matter::Strongly Correlated Electrons010306 general physics0210 nano-technologyElectronic band structureValence electron
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Prototype of an angular-selective photoelectron calibration source for the KATRIN experiment

2010

The method of direct neutrino mass determination based on the kinematics of tritium beta decay, which is adopted by the KATRIN experiment, makes use of a large, high-resolution electrostatic spectrometer with magnetic adiabatic collimation. In order to target a sensitivity on the neutrino mass of 0.2 eV/c^2, a detailed understanding of the electromagnetic properties of the electron spectrometer is essential, requiring comprehensive calibration measurements with dedicated electron sources. In this paper we report on a prototype of a photoelectron source providing a narrow energy spread and angular selectivity. Both are key properties for the characterisation of the spectrometer. The angular …

PhysicsElectron spectrometerPhysics - Instrumentation and DetectorsSpectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesElectronInstrumentation and Detectors (physics.ins-det)Magnetic fieldComputational physicsElectric fieldNeutrinoAdiabatic processInstrumentationMathematical PhysicsKATRIN
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Locust: C++ software for simulation of RF detection

2019

The Locust simulation package is a new C++ software tool developed to simulate the measurement of time-varying electromagnetic fields using RF detection techniques. Modularity and flexibility allow for arbitrary input signals, while concurrently supporting tight integration with physics-based simulations as input. External signals driven by the Kassiopeia particle tracking package are discussed, demonstrating conditional feedback between Locust and Kassiopeia during software execution. An application of the simulation to the Project 8 experiment is described. Locust is publicly available at https://github.com/project8/locust_mc.

PhysicsFlexibility (engineering)Modularity (networks)Physics - Instrumentation and Detectorsbiology010308 nuclear & particles physicsbusiness.industrySoftware toolFOS: Physical sciencesGeneral Physics and AstronomyInstrumentation and Detectors (physics.ins-det)Computational Physics (physics.comp-ph)Tracking (particle physics)biology.organism_classification01 natural sciencesParticle detectorSoftware0103 physical sciencesAntenna (radio)010306 general physicsbusinessPhysics - Computational PhysicsComputer hardwareLocust
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Project 8 Phase III Design Concept

2017

We present a working concept for Phase III of the Project 8 experiment, aiming to achieve a neutrino mass sensitivity of $2~\mathrm{eV}$ ($90~\%$ C.L.) using a large volume of molecular tritium and a phased antenna array. The detection system is discussed in detail.

PhysicsHistoryPhysics - Instrumentation and DetectorsPhysicsPhase (waves)FOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Computer Science ApplicationsEducationComputational physicsHigh Energy Physics - ExperimentAntenna arrayHigh Energy Physics - Experiment (hep-ex)Volume (thermodynamics)ddc:530Sensitivity (control systems)Nuclear Experiment (nucl-ex)NeutrinoNuclear Experiment
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Recent Upgrades of the SHIPTRAP Setup: On the Finish Line Towards Direct Mass Spectroscopy of Superheavy Elements

2016

With the Penning-trap mass spectrometer SHIPTRAP at GSI, Darmstadt, it is possible to investigate exotic nuclei in the region of the heaviest elements. Few years ago, challenging experiments led to the direct measurements of the masses of neutron-deficient isotopes with Z = 102,103 around N = 152. Thanks to recent advances in cooling and ion-manipulation techniques, a major technical upgrade of the setup has been recently accomplished to boost its efficiency. At present, the gap to reach more rare and shorter-lived species at the limits of the nuclear landscape has been narrowed. ispartof: pages:423-429 ispartof: Acta Physica Polonica B vol:48 issue:3 pages:423-429 ispartof: location:Zakopa…

PhysicsIsotopePenning trapGeneral Physics and AstronomyFinish lineSuperheavy Elements[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Accelerator Physics and InstrumentationPenning trapMass spectrometry01 natural sciences7. Clean energy010305 fluids & plasmasNuclear physicsUpgrade0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physics
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Search for polarization effects in the antiproton production process

2015

For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be produced polarized which will be checked experimentally. The polarization of antiprotons produced under typical conditions for antiproton beam preparation will be measured at the CERN/PS. If the production process creates some polarization a polarized antiproton beam could be prepared by a rather simple modification of the antiproton beam facility. The detection setup and the expected experimental conditions are described. For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be …

PhysicsLarge Hadron ColliderPhysics - Instrumentation and DetectorsFOS: Physical sciencesGeneral Physics and AstronomyParticle acceleratorInstrumentation and Detectors (physics.ins-det)Polarization (waves)law.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Antiproton beamAntiprotonlawPhysics::Accelerator Physicsddc:530High Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Detectors and Experimental TechniquesNuclear ExperimentNuclear Experiment
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