Search results for "Particle"

showing 10 items of 15225 documents

In-situ observation of beta-ray induced UV optical absorption in a-SiO2: radiation darkening and room temperature recovery

2006

International audience; We studied the optical absorption in the 3.0-6.2 eV range induced in bulk amorphous SiO2 by beta-ray irradiation up to similar to 1 MGy at room temperature. The induced absorption was measured in situ both during irradiation and in the post irradiation time. Our data evidence E', center as the main defect induced by irradiation and the partial decay of their absorption band at about 5.8 eV after irradiation. A quantitative analysis of the time evolution of the induced absorption shows that the transmission recovery observed after irradiation is compatible with the reaction of radiation-induced defects with H-related (H-2, H2O) species diffusing in the amorphous matrix

Absorption spectroscopySilica irradiation effects absorptionAnalytical chemistryOptical spectroscopyWater in glass02 engineering and technology01 natural scienceslaw.inventionAbsorptionlawElectron spin resonance0103 physical sciencesBeta particleMaterials ChemistryOptical fibersIrradiationElectron paramagnetic resonanceAbsorption (electromagnetic radiation)Spectroscopy010302 applied physics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]RadiationPhotoinduced effectsChemistryirradiation effectsSettore FIS/01 - Fisica SperimentaleSilica021001 nanoscience & nanotechnologyCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsAmorphous solidAbsorption bandCeramics and Composites[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]Defects0210 nano-technology
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Detection of deuterated molecules, but not of lithium hydride, in the z = 0.89 absorber toward PKS 1830−211

2020

Deuterium and lithium are light elements of high cosmological and astrophysical importance. In this work we report the first detection of deuterated molecules and a search for lithium hydride, 7LiH, at redshift z=0.89 in the spiral galaxy intercepting the line of sight to the quasar PKS1830-211. We used ALMA to observe several submillimeter lines of ND, NH2D, and HDO, and their related isotopomers NH2, NH3, and H2^18O, in absorption against the southwest image of the quasar, allowing us to derive XD/XH abundance ratios. The absorption spectra mainly consist of two distinct narrow velocity components for which we find remarkable differences. One velocity component shows XD/XH abundances that…

Absorption spectroscopyquasarsFOS: Physical scienceschemistry.chemical_elementAstrophysics01 natural scienceschemistry.chemical_compound0103 physical sciencesISM -galaxiesgalaxiesindividual010303 astronomy & astrophysicsLine (formation)Physics[PHYS]Physics [physics]Spiral galaxy010308 nuclear & particles physicsmolecules -radio linesAstronomy and AstrophysicsQuasarAstrophysics - Astrophysics of GalaxiesRedshift3. Good healthPKS 1830−211 -galaxiesabundances -ISMDeuteriumchemistry13. Climate actionSpace and Planetary ScienceLithium hydride[SDU]Sciences of the Universe [physics]Astrophysics of Galaxies (astro-ph.GA)Lithium[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]absorption lines -quasars
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DENN, EIGENTLICH, ÜBERHAUPT - THREE “PRAGMATIC PARTICLES” IN GERMAN

2015

A peculiarity of the German language is the extensive use of “pragmatic particles” in spoken language. These particles are generally called Abtönungspartikel (“modulating particles”) and are used to modulate the speaker’s attitude. They have an elusive meaning which is quite difficult for non-native speakers to discern, and they are a challenge to translate into Italian due to the lack of equivalents. Three particularly interesting particles are “denn”, “eigentlich” and “überhaupt”, which are typical of the speech act of asking questions. After a general introduction to the vast field of conversational particles (showing how differently German grammars treat this topic), the present contrib…

Abtoenungspartikeln ModalpartikelnSettore L-LIN/14 - Lingua E Traduzione - Lingua TedescaGerman modal particlesparticelle modali particelle communicative
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Present status and first results of the final focus beam line at the KEK Accelerator Test Facility

2011

ATF2 is a final-focus test beam line which aims to focus the low emittance beam from the ATF damping ring to a vertical size of about 37 nm and to demonstrate nanometer level beam stability. Several advanced beam diagnostics and feedback tools are used. In December 2008, construction and installation were completed and beam commissioning started, supported by an international team of Asian, European, and U.S. scientists. The present status and first results are described.

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsLow emittancePhysics and Astronomy (miscellaneous)Nuclear engineering[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]FOS: Physical sciencesbeam transport01 natural sciencesBeam characteristicslaw.inventionNuclear physicslaw0103 physical sciencesddc:530lcsh:Nuclear and particle physics. Atomic energy. RadioactivityBeam handling010306 general physicsAccelerator Test FacilityPhysicsFocus (computing)Research Groups and Centres\Physics\Low Temperature Physics010308 nuclear & particles physicsFaculty of Science\PhysicsBeam commissioningFísicaParticle acceleratorSurfaces and Interfaces29.27.Eg 29.27.Fh 29.20.dbAccelerators and Storage RingsStorage rings and collidersCOLLIDERSTechnology for normal conducting higher energy linear accelerators [9]BeamlineTest beamlcsh:QC770-798Physics - Accelerator PhysicsBeam (structure)
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New exotic beams from the SPIRAL 1 upgrade

2018

Since 2001, the SPIRAL 1 facility has been one of the pioneering facilities in ISOL techniques for reaccelerating radioactive ion beams: the fragmentation of the heavy ion beams of GANIL on graphite targets and subsequent ionization in the Nanogan ECR ion source has permitted to deliver beams of gaseous elements (He, N, O, F, Ne, Ar, Kr) to numerous experiments. Thanks to the CIME cyclotron, energies up to 20 AMeV could be obtained. In 2014, the facility was stopped to undertake a major upgrade, with the aim to extend the production capabilities of SPIRAL 1 to a number of new elements. This upgrade, which is presently under commissioning, consists in the integration of an ECR booster in the…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsNuclear engineering[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]tutkimuslaitteetCyclotronFOS: Physical scienceshiukkaskiihdyttimet[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex7. Clean energy01 natural sciencesIonlaw.inventionion sourceslawIonization0103 physical sciencesIon sourcesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)radioactive ion beams010306 general physicsNuclear ExperimentInstrumentationRadioactive ion beamsphysics.acc-ph[PHYS]Physics [physics]Physics010308 nuclear & particles physicsAccelerators and Storage RingsIon sourceUpgradesäteilyfysiikkaBeamlinePhysics - Accelerator PhysicsAGATABeam (structure)
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Fast photon detection for particle identification with COMPASS RICH-1

2006

Particle identification at high rates is an important challenge for many current and future high-energy physics experiments. The upgrade of the COMPASS RICH-1 detector requires a new technique for Cherenkov photon detection at count rates of several $10^6$ per channel in the central detector region, and a read-out system allowing for trigger rates of up to 100 kHz. To cope with these requirements, the photon detectors in the central region have been replaced with the detection system described in this paper. In the peripheral regions, the existing multi-wire proportional chambers with CsI photocathode are now read out via a new system employing APV pre-amplifiers and flash ADC chips. The ne…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhotomultiplierPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsCherenkov detectorOther Fields of PhysicsFOS: Physical sciencesCOMPASS; RICH; Multi-anode PMT; Particle identificationCOMPASSParticle identificationPhotocathodelaw.inventionParticle identificationNuclear physicsOpticsMulti-anode PMTlawCompassCOMPASS; RICHInstrumentationRICHCherenkov radiationPhysicsbusiness.industryDetectorInstrumentation and Detectors (physics.ins-det)UpgradePhysics - Accelerator PhysicsHigh Energy Physics::Experimentbusiness
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Vertical Beam Polarization at MAMI

2017

For the first time a vertically polarized electron beam has been used for physics experiments at MAMI in the energy range between 180 and 855 MeV. The beam-normal single-spin asymmetry $A_{\mathrm{n}}$, which is a direct probe of higher-order photon exchange beyond the first Born approximation, has been measured in the reaction $^{12}\mathrm C(\vec e,e')^{12}\mathrm C$. Vertical polarization orientation was necessary to measure this asymmetry with the existing experimental setup. In this paper we describe the procedure to orient the electron polarization vector vertically, and the concept of determining both its magnitude and orientation with the available setup. A sophisticated method has …

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonmedia_common.quotation_subjectVertical polarization[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]FOS: Physical sciencesElectron acceleratorElectronMott polarimeter01 natural sciencesAsymmetrylaw.inventionOpticsMøller polarimeterlaw0103 physical sciencesCompton polarimeter[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.PHYS.PHYS-ACC-PH ] Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Born approximation010306 general physicsNuclear Experiment[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Instrumentationmedia_commonPhysicsWien filter010308 nuclear & particles physicsbusiness.industryParticle acceleratorPolarimeterInstrumentation and Detectors (physics.ins-det)Wien filterPolarization (waves)Electron accelerator ; Vertical polarization ; Wien filter ; Compton polarimeter ; Mott polarimeter ; Møller polarimeterPhysics - Accelerator Physicsbusiness
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Polarization-Dependent Disappearance of a Resonance Signal -- Indication for Optical Pumping in a Storage Ring?

2021

We report on laser spectroscopic measurements on Li$^+$ ions in the experimental storage ring ESR at the GSI Helmholtz Centre for Heavy Ion Research. Driving the $2s\,^3\!{S}_1\;(F=\frac{3}{2}) \,\leftrightarrow\,2p\,^3\!P_2\;(F=\frac{5}{2}) \leftrightarrow 2s\,^3\!{S}_1\;(F=\frac{5}{2})$ $\Lambda$-transition in $^7$Li$^+$ with two superimposed laser beams it was found that the use of circularly polarized light leads to a disappearance of the resonance structure in the fluorescence signal. This can be explained by optical pumping into a dark state of polarized ions. We present a detailed theoretical analysis of this process that supports the interpretation of optical pumping and demonstrate…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Atomic Physics (physics.atom-ph)FOS: Physical sciences53001 natural sciencesIonlaw.inventionPhysics - Atomic PhysicsOptical pumpinglaw0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530010306 general physicsCircular polarizationPhysics010308 nuclear & particles physicsSurfaces and InterfacesLaserPolarization (waves)FluorescenceDark statelcsh:QC770-798Physics - Accelerator PhysicsAtomic physicsStorage ring
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Direct Measurement of Focusing Fields in Active Plasma Lenses

2018

Physical review accelerators and beams 21(12), 122801 (2018). doi:10.1103/PhysRevAccelBeams.21.122801

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Field (physics)FOS: Physical sciences01 natural sciences530law.inventionOpticslaw0103 physical sciencesddc:530Thermal emittancelcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsphysics.acc-phPhysics010308 nuclear & particles physicsbusiness.industrySurfaces and InterfacesPlasmaNuclear & Particles PhysicsLens (optics)Physics::Space PhysicsPhysical SciencesCathode raylcsh:QC770-798Physics::Accelerator PhysicsPhysics - Accelerator PhysicsBeam emittancebusinessCharged particle beamBeam (structure)
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Simulations and measurements of beam loss patterns at the CERN Large Hadron Collider

2014

The CERN Large Hadron Collider (LHC) is designed to collide proton beams of unprecedented energy, in order to extend the frontiers of high-energy particle physics. During the first very successful running period in 2010-2013, the LHC was routinely storing protons at 3.5-4 TeV with a total beam energy of up to 146 MJ, and even higher stored energies are foreseen in the future. This puts extraordinary demands on the control of beam losses. An uncontrolled loss of even a tiny fraction of the beam could cause a superconducting magnet to undergo a transition into a normal-conducting state, or in the worst case cause material damage. Hence a multistage collimation system has been installed in ord…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Monte Carlo methodFOS: Physical sciencesSuperconducting magnetTracking (particle physics)law.inventionNuclear physicslawlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)Large Hadron Collider (France and Switzerland)Nuclear ExperimentPhysicsLarge Hadron ColliderColliders (Nuclear physics)Particle acceleratorCollimatorSurfaces and InterfacesAccelerators and Storage RingsOrders of magnitude (time)lcsh:QC770-798Physics::Accelerator PhysicsPhysics - Accelerator PhysicsBeam (structure)
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