Search results for "Surfaces and Interfaces"

showing 10 items of 939 documents

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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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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Characterization and Tuning of Ultra High Gradient Permanent Magnet Quadrupoles

2009

The application of quadrupole devices with high field gradients and small apertures requires precise control over higher order multipole field components. We present a new scheme for performance control and tuning, which allows the illumination of most of the quadrupole device aperture because of the reduction of higher order field components. Consequently, the size of the aperture can be minimized to match the beam size achieving field gradients of up to $500\text{ }\text{ }\mathrm{T}\text{ }{\mathrm{m}}^{\ensuremath{-}1}$ at good imaging quality. The characterization method based on a Hall probe measurement and a Fourier analysis was confirmed using the high quality electron beam at the M…

Accelerator Physics (physics.acc-ph)electron beamNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorscompactmagneticlensPhysics and Astronomy (miscellaneous)Field (physics)AperturemultipoleFOS: Physical sciencespermanenthalbachx-felNuclear magnetic resonancetuningquadrupolelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadrupole magnetMicrotronPhysicsOrder (ring theory)Surfaces and InterfacesInstrumentation and Detectors (physics.ins-det)beam focusingComputational physicsMagnetQuadrupolelcsh:QC770-798Physics::Accelerator PhysicsPhysics - Accelerator PhysicsMultipole expansion
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Preparation and characterization of bio-organoclays using nonionic surfactant

2015

The present study was aimed at the preparation and characterization of tailor made hybrid materials, whose peculiar hosting capability could be exploited in biotechnological applications. With this purpose, the modification of K10 montmorillonite by intercalation of Tween 20 surfactant, was accomplished. The influence of two internal parameters, namely pH and surfactant/clay ratio, on the surfactant uptake ability by clay was investigated. The adsorption mechanism was elucidated on the basis of complementary kinetic and equilibrium studies and, then, corroborated by the useful information provided by the FT-IR, TGA and XRD characterization. The gathered results allow to draw the conclusion …

Adsorption kineticGeneral Chemical EngineeringIntercalation (chemistry)Drug delivery systemTween 20Dual mode model02 engineering and technology010402 general chemistrycomplex mixtures01 natural scienceschemistry.chemical_compoundAdsorptionPulmonary surfactantOrganic chemistryNonionic surfactantChemical Engineering (all)MontmorilloniteOrgano-clayIsothermHydrophobic drugChemistry (all)Surfaces and InterfacesGeneral Chemistry021001 nanoscience & nanotechnology0104 chemical sciencesCharacterization (materials science)MontmorillonitechemistryChemical engineering0210 nano-technologyHybrid materialSurfaces and Interface
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Fast Measurements of Adsorption on Porous Materials Using Jäntti's Method

1999

In 1972, Jäntti et al. formulated a method to shorten the time taken for adsorption measurements. We suggested at the Kiev International Conference on Vacuum Microbalance Techniques (1999) that the applicability of this method could be widened by considering a number of parallel adsorptions. There is, however, a more complicated but perhaps more interesting variant possible when extra mass transport is considered to occur in series. Such an application could involve adsorption within a porous structure where diffusion must be considered as a process occurring in series with adsorption on the surface.

AdsorptionChemical engineeringChemistryGeneral Chemical Engineeringlcsh:QD450-801lcsh:Physical and theoretical chemistrySurfaces and InterfacesGeneral ChemistryPorous mediumAdsorption Science & Technology
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Effect of Stiffness on the Micellization Behavior of Model H4T4 Surfactant Chains

2006

The micellization behavior of a series of model surfactants, all with four head and tail groups (H4T4) but with different degrees of chain stiffness, was studied using grand canonical Monte Carlo simulations on a cubic lattice. The critical micelle concentration, micellar size, and thermodynamics of micellization were examined. In all cases investigated, the critical micelle concentration was found to increase with increasing temperature as observed for nonionic surfactants in apolar or slightly polar solvents. At a fixed reduced temperature and increasing chain stiffness, in agreement with previous observations, it was found that the critical micelle concentration decreased and the average…

Aggregation numberChemistryCrystal lattices Hydrophobicity Micelles Molecular structure Monte Carlo methods SolventsThermodynamics of micellizationMonte Carlo methodtechnology industry and agricultureThermodynamicsSurfaces and InterfacesCondensed Matter PhysicsMicelleSurface-Active AgentsReduced propertiesPulmonary surfactantCritical micelle concentrationElectrochemistryThermodynamicsOrganic chemistryPolarGeneral Materials ScienceMonte Carlo MethodMicellesSpectroscopySettore CHIM/02 - Chimica FisicaLangmuir
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Preferential localization of Lactococcus lactis cells entrapped in a caseinate/alginate phase separated system.

2013

International audience; This study aimed to entrap bioprotective lactic acid bacteria in a sodium caseinate/sodium alginate aqueous two-phase system. Phase diagram at pH = 7 showed that sodium alginate and sodium caseinate were not miscible when their concentrations exceeded 1% (w/w) and 6% (w/w), respectively. The stability of the caseinate/alginate two-phase system was also checked at pH values of 6.0 and 5.5. Lactococcus lactis subsp. lactis LAB3 cells were added in a 4% (w/w) caseinate/1.5% (w/w) alginate two-phase system at pH = 7. Fluorescence microscopy allowed to observe that the caseinate-rich phase formed droplets dispersed in a continuous alginate-rich phase. The distribution of …

Alginates02 engineering and technologyCell SeparationHydrophobic effectchemistry.chemical_compound0404 agricultural biotechnologyColloid and Surface ChemistryGlucuronic AcidPhase (matter)Fluorescence microscope[SDV.BBM]Life Sciences [q-bio]/Biochemistry Molecular BiologyPhysical and Theoretical ChemistryAqueous solutionChromatographybiologyHexuronic AcidsLactococcus lactisAqueous two-phase systemCaseins04 agricultural and veterinary sciencesSurfaces and InterfacesGeneral MedicineHydrogen-Ion Concentration021001 nanoscience & nanotechnologybiology.organism_classification040401 food scienceLactic acidPhase diagramLactococcus lactisSodium caseinateBiochemistrychemistryAqueous two-phase system0210 nano-technologySodium alginateBacteriaBacterial cells entrapmentBiotechnologyColloids and surfaces. B, Biointerfaces
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The defined adsorption site of sodium on the TiO2(110)–(1×1) surface

2004

The adsorption site of sodium on the TiO2(1 1 0)–(1 × 1) surface was studied by extended X-ray absorption fine structure. For coverage ranging between 0.25 and 0.5 ML, we find that sodium is on an ‘in-between' site where it is bound to two bridging oxygen atoms at 2.25 Å and one in-plane oxygen atom at 2.40 Å, in full agreement with DFT calculations. At higher coverage the site becomes an hollow site where the sodium atom is equidistant to the three oxygen atoms at 2.30 Å, while metallic sodium clusters are also formed at the surface.

Alkali metalsSodiumInorganic chemistrychemistry.chemical_element02 engineering and technologyExtended X-ray absorption fine structure (EXAFS)01 natural sciencesOxygenMetalAdsorption0103 physical sciencesAtomMaterials Chemistry010306 general physicsTitanium oxideExtended X-ray absorption fine structureChemistrySurfaces and Interfaces021001 nanoscience & nanotechnologyCondensed Matter PhysicsAlkali metalSurfaces Coatings and FilmsCrystallographyvisual_artvisual_art.visual_art_mediumAbsorption (chemistry)0210 nano-technologySurface Science
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