Search results for "scattering"

showing 10 items of 8332 documents

Thermal Aggregation of Bovine Serum Albumin in Trehalose and Sucrose Aqueous Solutions

2012

We report results of static and dynamic light scattering measurements performed on bovine serum albumin (BSA) in saccharide (trehalose and sucrose) solutions. Our aim is to study the effects of the two disaccharides on the first steps of thermal aggregation of BSA in aqueous solutions at two protein concentrations (1 and 30 mg/mL) at increasing sugar/water ratio. Results show that sugars modify early stages of aggregation mainly by perturbing the thermodynamic behavior of the solvent (i.e., general solvent effects) without involving direct, specific sugar-protein interactions. This agrees with current hypotheses on sugar action in protein solutions. (1-3) The linear correlation detected bet…

SucroseSucrosechemistry.chemical_compoundDynamic light scatteringMaterials ChemistryAnimalsTransition TemperaturePhysical and Theoretical ChemistryBovine serum albuminProtein Structure QuaternarySugarChromatographyAqueous solutionbiologyTemperatureTrehaloseWaterSerum Albumin BovineTrehaloseSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Surfaces Coatings and FilmsSolutionsSolventtrehalose protein aggregation solvent effects light scatteringchemistrySolventsbiology.proteinCattleProtein MultimerizationSolvent effectsThe Journal of Physical Chemistry B
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Solid-State Analog of an Optical Interferometer

2004

To some extend one may treat a metal ring with two probes as a solid-state analog of an optical interferometer. One node can be considered as a beam splitter (bi-prism, for example), and the electric current at the other node as an equivalent to a light intensity of an interference pattern formed at a screen. In optics, to obtain a stationary pattern one should use a monochromatic source of radiation, as afterwards in a conventional passive media (i.e. air) the phase of the radiation is preserved. On the contrary, in solids the phase of a conducting electron wavefunction is randomly altered due to inelastic collisions (mainly phonons at high temperatures). Hence, to satisfy the condition of…

Superconducting coherence lengthPhysicsSuperconductivityLight intensityMagnetoresistanceCondensed matter physicsMagnetic flux quantumPhase (waves)ElectronInelastic scattering
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Antiferromagnetism and the node structure of the superconducting order parameter of UPd Al

2000

The node structure of the superconducting order parameter of the heavy-fermion system is analyzed within the weak-coupling theory. A pairing interaction induced by the exchange of antiferromagnetic spin excitations is assumed as suggested by recent inelastic neutron scattering experiments and tunneling spectroscopy. The multi-sheeted Fermi surface is taken into account. Based on a model susceptibility for the simple antiferromagnetic structure of , line nodes result at the rim of the magnetic Brillouin zone.

SuperconductivityBrillouin zonePhysicsCondensed matter physicsPairingAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsFermi surfaceCondensed Matter PhysicsMagnetic susceptibilityInelastic neutron scatteringElectronic Optical and Magnetic MaterialsSpin-½The European Physical Journal B
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Macroscopic persistent currents in laser ablated YBa2Cu3O7-x films

2011

AbstractThin films of YBa2Cu3O7-x have been produced in situ by laser ablation. As the condensation of the superconducting film is done onto hot substrates (600 - 780°C) at high oxygen pressures (~ 1 mbar), this techniques does not require any special postannealing step. Thus the total process time amounts to less than 10 min. Films were found to be polycrystalline with the c-axis preferentially oriented normal to the substrate plane on single crystalline (001) SrTiO3 and (random) ZrO2, as measured by ion channeling (Xmin = 5.5 % on SrTiO3), x-ray scattering and TEM. Complete superconducting transitions above 90 K with transition widths of about 1 K have been observed even on YSZ substrates…

SuperconductivityMaterials scienceLaser ablationScatteringAnalytical chemistryNanotechnologyPersistent currentddc:530Substrate (electronics)CrystalliteThin filmRing current
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Investigation of the epitaxy of thin YBa2Cu3O7-delta films

1990

Abstract The degree of epitaxy of thin sputtered and laser ablated films have been investigated by Raman spectroscopy. Using the selection rules for Raman scattering for the different phonons in YBa 2 Cu 3 O 7−δ the superconducting films on SrTiO 3 and MgO are found to be epitaxially grown with the c -axis perpendicular to the substrate. On ZrO 2 the films also grow with their c -axis perpendicular to the substrate, but with randomly oriented a / b -directions in the plane of the film.

SuperconductivityMaterials sciencePhononbusiness.industryAnalytical chemistryEnergy Engineering and Power TechnologySubstrate (electronics)Condensed Matter PhysicsEpitaxyLaserElectronic Optical and Magnetic Materialslaw.inventionsymbols.namesakeCondensed Matter::Materials ScienceOpticslawCondensed Matter::SuperconductivitysymbolsPerpendicularddc:530Electrical and Electronic EngineeringRaman spectroscopybusinessRaman scattering
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Raman scattering studies of ultrathin-layer YBa2Cu3O7/PrBa2Cu3O7 superlattices

1994

We present Raman scattering studies ofc-oriented ultrathin-layer superconducting (YBa2Cu3O7) m /(PrBa2Cu3O7) n superlattices. For the superlattice with (m=2,n=1) sequence, Raman spectra reveal a new line in the spectral region around 320 cm−1. It is interpreted as a mode representing a combination of IR optical phonons of the Y-sublayers with an admixture of aB1g type Raman active vibration in the Pr sublayers. This new line, which is similar to those from the interior of the Brillouin zone of the original lattice, does not exhibit superconductivity-induced self-energy effects, although its counterpart in the pure substance does. No additional line is found in the (m=1,n=2) superlattice in …

SuperconductivityMaterials sciencePhysics and Astronomy (miscellaneous)Condensed matter physicsPhononSuperlatticeCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsBrillouin zoneCondensed Matter::Materials Sciencesymbols.namesakeCondensed Matter::SuperconductivityLattice (order)symbolsThin filmRaman spectroscopyRaman scatteringJournal of Superconductivity
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Superconductivity mediated by spin fluctuations in the heavy-fermion compound UPd2 Al3

1999

It is well known that any weak attractive electron–electron interaction in metals can in principle cause the formation of Cooper pairs, which then condense into a superconducting ground state1. In conventional superconductors, this attractive interaction is mediated by lattice vibrations (phonons). But for the heavy-fermion and high-temperature superconductors, alternative pairing interactions are considered to be possible2. For example, the low-temperature properties of heavy-fermion systems are dominated by antiferromagnetic spin fluctuations, which have been considered theoretically3 as a possible cause for Cooper-pair formation. This picture recently received some experimental support: …

SuperconductivityMultidisciplinaryCondensed matter physicsPhononChemistryCondensed Matter::SuperconductivityPairingAntiferromagnetismCooper pairInelastic neutron scatteringQuantum tunnellingSpin-½Nature
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Superconductivity in palladium-based Heusler compounds

2009

This work reports on four more Heusler superconductors: ${\text{Pd}}_{2}\text{ZrAl}$, ${\text{Pd}}_{2}\text{HfAl}$, ${\text{Pd}}_{2}\text{ZrIn}$, and ${\text{Pd}}_{2}\text{HfIn}$. These compounds exhibit superconducting transition temperatures ranging from 2.4--3.8 K as determined by resistivity measurements. According to their behavior in an external magnetic field, all compounds are type II bulk superconductors. The occurrence of superconductivity was predicted for these compounds using electronic structure calculations. The electronic structures exhibit van Hove singularities (saddle points) at the $L$ point. These lead to a maximum in the corresponding density of states and superconduct…

SuperconductivityPhysicsCondensed matter physicsScatteringTransition temperatureFermi energyElectronic structureCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsElectrical resistivity and conductivityCondensed Matter::SuperconductivityDensity of statesCondensed Matter::Strongly Correlated ElectronsElectron scatteringPhysical Review B
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Change of the vortex core structure in two-band superconductors at the impurity-scattering-driven s±/s++ crossover

2017

We report a nontrivial transition in the core structure of vortices in two-band superconductors as a function of interband impurity scattering. We demonstrate that, in addition to singular zeros of the order parameter, the vortices there can acquire a circular nodal line around the singular point in one of the superconducting components. It results in the formation of the peculiar ``moat''-like profile in one of the superconducting gaps. The moat-core vortices occur generically in the vicinity of the impurity-induced crossover between ${s}_{\ifmmode\pm\else\textpm\fi{}}$ and ${s}_{++}$ states.

SuperconductivityPhysicsCondensed matter physicsta114ScatteringCrossovermultiband superconductivityOrder (ring theory)vortices in superconductors02 engineering and technologySingular point of a curve021001 nanoscience & nanotechnology01 natural sciencesVortexImpurityCondensed Matter::Superconductivityimpurities in superconductors0103 physical sciencess-wave010306 general physics0210 nano-technologyLine (formation)Physical Review B
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Field dependence of the vortex core size probed by scanning tunneling microscopy

2016

We study the spatial distribution of the density of states (DOS) at zero bias N(r) in the mixed state of single and multigap superconductors. We provide an analytic expression for N(r) based on deGennes' relationship between DOS and the order parameter that reproduces well scanning tunneling microscopy (STM) data in several superconducting materials. In the single gap superconductor β-Bi2Pd, we find that N(r) is governed by a length scale ξH=φ0/2πH, which decreases in rising fields. The vortex core size C, defined via the slope of the order parameter at the vortex center, C (dΔ/dr|r→0)-1, differs from ξH by a material dependent numerical factor. The new data on the tunneling conductance and…

SuperconductivityPhysicsLength scaleCondensed matter physicsScatteringFísica02 engineering and technology021001 nanoscience & nanotechnology01 natural sciences7. Clean energyVortexlaw.inventionlawCondensed Matter::SuperconductivityLattice (order)0103 physical sciencesDensity of statesScanning tunneling microscopeScanning tunneling microscopySuperconductivitat010306 general physics0210 nano-technologyAnisotropyVortex core sizePhysical Review B
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