Search results for "Length"

showing 10 items of 2188 documents

Determination of Sulfur in Fertilizers by Inductively Coupled Plasma-Atomic Emission Spectrometry: Spectral and Interelement Effects at Various Wavel…

1996

Abstract Three analytical wavelengths (180.731,182.037, and 182.625 nm) were tested for determination of sulfur in 2 fertilizers by inductively coupled plasmaatomic emission spectrometry (ICP-AES). Variable S results at 182.037 nm were caused by a downward sloping background shift (Fe line at 181.851 nm) during measurement of the sample solutions. At 182.625 nm an emission peak doublet, 182.619/182.635 nm, was observed from which the instrument selected the measurement peak. A shift from calibrated peak 182.619 nm to noncalibrated peak 182.635 nm occurred when the S/B ratios were ≤22-31 in the fertilizer samples examined. For the 3 wavelengths of S investigated, the pattern of spectral and …

PharmacologyChemistryAnalytical chemistrychemistry.chemical_elementSulfurAnalytical ChemistryWavelengthInterference (communication)Environmental ChemistryInductively coupled plasmaOptical emission spectrometryAgronomy and Crop ScienceChemical compositionFood ScienceLine (formation)Atomic emission spectrometryJournal of AOAC INTERNATIONAL
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Determination of Magnesium in Fertilizers by Inductively Coupled Plasma Atomic Emission Spectrometry: Studies of Some Spectral and Interelement Effec…

1995

Abstract Four analytical wavelengths of magnesium were tested for determination of Mg from fertilizers by inductively coupled plasma atomic emission spectroscopy (ICP-AES): 202.528, 285.213, and 383.826 nm (Mg I) and 279.553 (Mg II). The effects of fertilizer matrix elements on Mg determination were examined by adding matrix elements to fertilizer solutions. Multiple linear regression calculations proved a valuable technique for evaluating the effects of matrix elements on Mg determination. The observed interferences at Mg wavelengths may be both spectral and interelement. Interelement effects were typically caused by Na, K, and Ca, and spectral effects, by P, Fe, and S. The best wavelength…

PharmacologyMagnesiumAnalytical chemistrychemistry.chemical_elementAnalytical ChemistryMatrix (chemical analysis)WavelengthchemistryInductively coupled plasma atomic emission spectroscopyEnvironmental ChemistryInductively coupled plasmaOptical emission spectrometryAgronomy and Crop ScienceQuantitative analysis (chemistry)Food ScienceAtomic emission spectrometryJournal of AOAC INTERNATIONAL
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High-repetition-rate source delivering optical pulse trains with a controllable level of amplitude and temporal jitters

2020

International audience; We theoretically propose and numerically validate an all-optical scheme to generate optical pulse trains with varying peak-powers and durations. A shaping of the spectral phase thanks to discrete /2 phase shifts enables an efficient phase-to-intensity conversion of a temporal phase modulation based on a two-tone sinusoidal beating. Experiments carried out at telecommunication wavelengths and at a repetition rate of 10 GHz confirm the ability of our approach to efficiently generate a train made of pulses with properties that vary from pulse-to-pulse. The levels of jitters can be accurately controlled.

Phase (waves)FOS: Physical sciences02 engineering and technologyoptical telecommunications01 natural scienceslcsh:QA75.5-76.95010309 optics020210 optoelectronics & photonicsOptics0103 physical sciences0202 electrical engineering electronic engineering information engineeringhigh-repetition rate optical pulse trainsPhysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]optical component testingRepetition (rhetorical device)business.industryhigh‐repetition rate optical pulse trainsPulse (physics)WavelengthAmplitudelcsh:TA1-2040Trainlcsh:Electronic computers. Computer sciencebusinesslcsh:Engineering (General). Civil engineering (General)Phase modulationOptics (physics.optics)Physics - Optics
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The smectic phase in semiflexible polymer materials: A large scale Molecular Dynamics study

2019

Abstract Semiflexible polymers in concentrated lyotropic solution are studied within a bead-spring model by molecular dynamics simulations, focusing on the emergence of a smectic A phase and its properties. We systematically vary the density of the monomeric units for several contour lengths that are taken smaller than the chain persistence length. The difficulties concerning the equilibration of such systems and the choice of appropriate ensemble (constant volume versus constant pressure, where all three linear dimensions of the simulation box can fluctuate independently) are carefully discussed. Using HOOMD-blue on graphics processing units, systems containing more than a million monomeri…

Phase transitionMaterials scienceGeneral Computer ScienceFOS: Physical sciencesGeneral Physics and Astronomy02 engineering and technologyCondensed Matter - Soft Condensed Matter010402 general chemistry01 natural sciencesMolecular dynamicsLiquid crystalPhase (matter)LyotropicGeneral Materials SciencePersistence lengthGeneral Chemistry021001 nanoscience & nanotechnology0104 chemical sciencesCondensed Matter::Soft Condensed MatterComputational MathematicsMechanics of MaterialsChemical physicsSoft Condensed Matter (cond-mat.soft)0210 nano-technologyStructure factorConstant (mathematics)
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Semiflexible Polymers Interacting with Planar Surfaces: Weak versus Strong Adsorption

2020

Semiflexible polymers bound to planar substrates by a short-range surface potential are studied by Molecular Dynamics simulations to clarify the extent to which these chain molecules can be considered as strictly two-dimensional. Applying a coarse-grained bead-spring model, the chain length N and stiffness &kappa

Phase transitionPolymers and Plastics02 engineering and technology01 natural sciencesMolecular physicsGyrationArticlelcsh:QD241-441Molecular dynamicschain rigiditylcsh:Organic chemistry0103 physical sciencesPerpendicularMolecule010306 general physicspolymersPhysicschemistry.chemical_classificationPersistence lengthQuantitative Biology::Biomoleculesfood and beveragesGeneral ChemistryPolymer021001 nanoscience & nanotechnologymolecular dynamicsphase transitionsCondensed Matter::Soft Condensed MatterDistribution functionchemistryadsorption0210 nano-technologyPolymers
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Properties of dirty two-band superconductors with repulsive interband interaction: Normal modes, length scales, vortices, and magnetic response

2018

Disorder in two-band superconductors with repulsive interband interaction induces a frustrated competition between the phase-locking preferences of the various potential and kinetic terms. This frustrated interaction can result in the formation of an $s+is$ superconducting state, that breaks the time-reversal symmetry. In this paper we study the normal modes and their associated coherence lengths in such materials. We especially focus on the consequences of the soft modes stemming from the frustration and time-reversal-symmetry breakdown. We find that two-bands superconductors with such impurity-induced frustrated interactions display a rich spectrum of physical properties that are absent i…

Phase transitionsuprajohtavuusmedia_common.quotation_subjectmultiband superconductivityFOS: Physical sciencesFrustration02 engineering and technologySoft modes01 natural sciencessuprajohteetSuperconductivity (cond-mat.supr-con)Normal modeCondensed Matter::Superconductivityimpurities in superconductors0103 physical sciences010306 general physicsmedia_commonSuperconductivityPhysicsCondensed matter physicsta114Condensed Matter - Superconductivitysuperconductivityvortices in superconductors021001 nanoscience & nanotechnologySymmetry (physics)Coherence lengthMagnetic fieldCondensed Matter::Strongly Correlated Electrons0210 nano-technologyPhysical Review B
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Ab initio simulations on the atomic and electronic structure of single-walled BN nanotubes and nanoarches

2009

To simulate the perfect single-walled boron nitride nanotubes and nanoarches with armchair- and zigzag-type chiralities and uniform diameter of � 5 nm, we have constructed their one-dimensional (1D) periodic models. In this study, we have compared the calculated properties of nanotubes with those for both hexagonal and cubic phases of bulk: bond lengths, binding energies per B–N bond, effective atomic charges as well as parameters of total and projected one-electron densities of states. For both phases of BN bulk, we have additionally verified their lattice constants. In the density functional theory (DFT), calculations performed using formalism of the localized Gaussian-type atomic functio…

PhononChemistryC. electronic structureBinding energyD. elastic and vibrational properties02 engineering and technologyGeneral ChemistryElectronic structure021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesA. BN nanostructuresOptical properties of carbon nanotubesBond lengthCondensed Matter::Materials ScienceLattice constantAb initio quantum chemistry methodsB. ab initio calculations0103 physical sciencesGeneral Materials ScienceDensity functional theoryAtomic physics010306 general physics0210 nano-technologyJournal of Physics and Chemistry of Solids
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A combined theoretical and experimental determination of the electronic spectrum of acetone

1996

A combined ab initio and experimental investigation has been performed of the main features of the electronic spectrum of acetone. Vertical transition energies have been calculated from the ground to the ny→π∗, π→π∗, σ→π∗, and the n=3 Rydberg states. In addition, the 1A1 energy surfaces have been studied as functions of the CO bond length. The 1A1 3p and 3d states were found to be heavily perturbed by the π→π∗ state. Resonant multiphoton ionization and polarization‐selected photoacoustic spectra of acetone have been measured and observed transitions were assigned on internal criteria. The calculated vertical transition energies to the ny→π∗ and all Rydberg states were found to be in agreeme…

Photoacoustic SpectroscopyOvertoneAb initioGeneral Physics and AstronomyPhotoionizationPhotoionizationSpectral lineAcetoneBond LengthsGround Statessymbols.namesakeRydberg StatesAb initio quantum chemistry methodsPolarizationIonizationPhysics::Atomic PhysicsPhysical and Theoretical Chemistry:FÍSICA::Química física [UNESCO]Carbon MonoxideEnergyChemistryUNESCO::FÍSICA::Química físicaSurfacesBond lengthElectron SpectraRydberg formulasymbolsAb Initio Calculations ; Acetone ; Bond Lengths ; Carbon Monoxide ; Electron Spectra ; Energy ; Ground States ; Multi−Photon Processes ; Photoacoustic Spectroscopy ; Photoionization ; Polarization ; Rydberg States ; SurfacesMulti−Photon ProcessesAtomic physicsAb Initio CalculationsThe Journal of Chemical Physics
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Photo-acoustic phase-delayed excitation of guided waves in coated bone phantoms

2013

Photo-acoustic skeletal quantitative ultrasound enables assessment of the fundamental flexural guided wave (FFGW) propagating in bone. This mode, consistent with the F(1,1) tube mode can now be measured through a coating of soft tissue. Interference due to ultrasound propagation in the soft tissue surrounding the bone is reduced by using phase-delayed ultrasound excitation. Photo-acoustic phase-delayed excitation was done on five axisymmetric bone phantoms (1-5 mm wall thickness), coated by a 5 mm thick soft-tissue mimicking layer. A fiber head comprising a linear array of four optical fibers (400 μm diameter), illuminated by pulsed laser diodes (905 nm wavelength) generated ultrasound. Thi…

Photoacoustic effectOptical fiberMaterials scienceGuided wave testingta114business.industryUltrasoundPhase (waves)01 natural scienceslaw.invention030507 speech-language pathology & audiology03 medical and health sciencesWavelengthTransducerOpticslaw0103 physical sciences0305 other medical sciencebusiness010301 acousticsGroup delay and phase delay
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Characterization of Thin Film Cig(S,Se)2 Submodules Using Solar Simulator and Laser Beam Induced Current Techniques

2015

In this work, the electrical and optical characterization of CIG(S,Se)2 sub-modules using both a solar simulator equipment and the Laser Beam Induced Current (LBIC) technique is presented. By using the solar simulator and a proper set-up, the electrical parameters of the modules at varying irradiance and temperatures are determined. In addition, the LBIC measurements are carried out to analyze the 2D photocurrent uniformity of the modules at two different wavelengths. Dispersion values of extracted parameters can be very useful for practically tuning the modelling stage at device/module level.

PhotocurrentWavelengthOpticsMaterials sciencebusiness.industryDispersion (optics)IrradianceOptoelectronicsSolar simulatorThin filmCurrent (fluid)businessCharacterization (materials science)2015 Fotonica AEIT Italian Conference on Photonics Technologies
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