Search results for "Disordered system"

showing 10 items of 244 documents

Disorder-induced single-mode transmission.

2017

Localized states trap waves propagating in a disordered potential and play a crucial role in Anderson localization, which is the absence of diffusion due to disorder. Some localized states are barely coupled with neighbours because of differences in wavelength or small spatial overlap, thus preventing energy leakage to the surroundings. This is the same degree of isolation found in the homogeneous core of a single-mode optical fibre. Here we show that localized states of a disordered optical fibre are single mode: the transmission channels possess a high degree of resilience to perturbation and invariance with respect to the launch conditions. Our experimental approach allows identification…

Genetics and Molecular Biology (all)Transmission channelAnderson localizationOptical fiberScienceGeneral Physics and AstronomyPerturbation (astronomy)02 engineering and technology01 natural sciencesCondensed Matter::Disordered Systems and Neural NetworksBiochemistryGeneral Biochemistry Genetics and Molecular BiologyArticlelaw.invention010309 opticsPhysics and Astronomy (all)law0103 physical sciencesPhysicsMultidisciplinaryCondensed matter physicsQChemistry (all)Single-mode optical fiberGeneral Chemistry021001 nanoscience & nanotechnologyWavelengthTransverse planeHomogeneousChemistry (all); Biochemistry Genetics and Molecular Biology (all); Physics and Astronomy (all)0210 nano-technologyNature communications
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Defects in glasses

1995

Abstract The absence of long range order in the glass structure allows to define only point defects in these materials. They are: 1) intrinsic defects—atomic size local deviation from short range order; 2) impurity defects—isolated impurity atoms or ions in the glass network; 3) intrinsic impurity defects—complexes consisting of the impurity atoms chemically bonded to one of the intrinsic defect atoms. The latter defects are characteristic for the doped glasses. Presence of point defects in glasses introduces new spectroscopic properties of these solid materials. Defect generation, interaction and recombination reactions resulting from the external influence causes the glass spectroscopic p…

Glass structureNuclear and High Energy PhysicsRange (particle radiation)RadiationMaterials scienceAbsorption spectroscopyCondensed matter physicsbusiness.industryDopingCondensed Matter PhysicsCondensed Matter::Disordered Systems and Neural NetworksCrystallographic defectIonOpticsImpurityGeneral Materials SciencebusinessRecombinationRadiation Effects and Defects in Solids
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Spin Glasses on Thin Graphs

1995

In a recent paper we found strong evidence from simulations that the Isingantiferromagnet on ``thin'' random graphs - Feynman diagrams - displayed amean-field spin glass transition. The intrinsic interest of considering such random graphs is that they give mean field results without long range interactions or the drawbacks, arising from boundary problems, of the Bethe lattice. In this paper we reprise the saddle point calculations for the Ising and Potts ferromagnet, antiferromagnet and spin glass on Feynman diagrams. We use standard results from bifurcation theory that enable us to treat an arbitrary number of replicas and any quenched bond distribution. We note the agreement between the f…

High Energy Physics - TheoryNuclear and High Energy PhysicsSpin glassCondensed Matter (cond-mat)FOS: Physical sciencesCondensed Matter01 natural sciencesCondensed Matter::Disordered Systems and Neural Networks010305 fluids & plasmassymbols.namesakeHigh Energy Physics - LatticeSaddle point0103 physical sciencesAntiferromagnetismFeynman diagram010306 general physicsRandom graphPhysicsBethe latticeCondensed matter physicsHigh Energy Physics - Lattice (hep-lat)Mean field theoryHigh Energy Physics - Theory (hep-th)symbolsIsing modelCondensed Matter::Strongly Correlated Electrons
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Effect of the milling conditions on the degree of amorphization of selenium by milling in a planetary ball mill

2007

The effect of the milling parameters (rotation speed of the milling device and duration of milling) on the phase composition of the products of milling of fully crystalline selenium has been investigated. The milling was conducted using a planetary micromill and the phase composition of the milling products was determined by differential thermal analysis. It has been found that ball milling leads to the partial amorphization of the starting crystalline material. The content of amorphous phase in the milling products depends, in a rather complicated way, on the milling parameters. At the milling parameters adopted in the present study, the milling product was never fully amorphous. The compl…

HistoryMaterials scienceHigh Energy Physics::LatticeMetallurgychemistry.chemical_elementCondensed Matter::Disordered Systems and Neural NetworksComputer Science ApplicationsEducationAmorphous solidlaw.inventionDegree (temperature)Condensed Matter::Materials ScienceGeneral Relativity and Quantum CosmologyHigh Energy Physics::TheorychemistrylawPhase compositionDifferential thermal analysisDeformation (engineering)CrystallizationBall millSeleniumJournal of Physics: Conference Series
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Devitrification of the Kob-Andersen glass former: Competition with the locally favored structure

2018

Abstract Supercooled liquids are kinetically trapped materials in which the transition to a thermodynamically more stable state with long-range order is strongly suppressed. To assess the glass-forming abilities of a liquid empirical rules exist, but a comprehensive microscopic picture of devitrification is still missing. Here we study the crystallization of a popular model glass former, the binary Kob-Andersen mixture, in small systems. We perform trajectory sampling employing the population of the locally favored structure as order parameter. While for large population a dynamical phase transition has been reported, here we show that biasing towards a small population of locally favored s…

HistoryMaterials scienceStatistical Mechanics (cond-mat.stat-mech)media_common.quotation_subjectThermodynamicsFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesLocal structureCondensed Matter::Disordered Systems and Neural NetworksCompetition (biology)Computer Science ApplicationsEducationCondensed Matter::Soft Condensed MatterDevitrification0103 physical sciences010306 general physics0210 nano-technologyCondensed Matter - Statistical Mechanicsmedia_common
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Critical phenomena without “hyper scaling”: How is the finite-size scaling analysis of Monte Carlo data affected?

2010

Abstract The finite size scaling analysis of Monte Carlo data is discussed for two models for which hyperscaling is violated: (i) the random field Ising model (using a model for a colloid-polymer mixture in a random matrix as a representative) (ii) The Ising bi-pyramid in computing surface fields.

Hybrid Monte CarloPhysicsQuantum Monte CarloMonte Carlo methodCondensed Matter::Statistical MechanicsDynamic Monte Carlo methodMonte Carlo integrationIsing modelMonte Carlo method in statistical physicsStatistical physicsPhysics and Astronomy(all)Condensed Matter::Disordered Systems and Neural NetworksMonte Carlo molecular modelingPhysics Procedia
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Slow and fast methyl group rotations in fragile glass-formers studied by NMR

2000

Abstract The spin-lattice relaxation times of the selectively ring deuterated, fragile glass-formers propylene carbonate and toluene were compared with those measured for species which were specifically labeled at the methyl groups. It was found that the dynamics of the CD 3 group is strongly decoupled from that associated with the primary response of toluene, while for propylene carbonate the degree of decoupling is relatively weak. The experimental results could be described successfully using a model which takes into account the ring dynamics as well as those of the methyl group.

Inorganic chemistryRelaxation (NMR)Primary responseGeneral Physics and AstronomyRing (chemistry)Toluene530Condensed Matter::Disordered Systems and Neural NetworksCondensed Matter::Soft Condensed MatterCrystallographychemistry.chemical_compoundchemistryDeuteriumGroup (periodic table)Propylene carbonatePhysical and Theoretical ChemistryPhysics::Chemical PhysicsMethyl group
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The Ultimate Fate of Supercooled Liquids

2010

In recent years it has become widely accepted that a dynamical length scale {\xi}_{\alpha} plays an important role in supercooled liquids near the glass transition. We examine the implications of the interplay between the growing {\xi}_{\alpha} and the size of the crystal nucleus, {\xi}_M, which shrinks on cooling. We argue that at low temperatures where {\xi}_{\alpha} > {\xi}_M a new crystallization mechanism emerges enabling rapid development of a large scale web of sparsely connected crystallinity. Though we predict this web percolates the system at too low a temperature to be easily seen in the laboratory, there are noticeable residual effects near the glass transition that can account …

Length scaleFOS: Physical sciencesCrystal growth02 engineering and technologyCondensed Matter - Soft Condensed Matter010402 general chemistry01 natural sciencesCondensed Matter::Disordered Systems and Neural NetworksArticlelaw.inventionCrystalCrystallinitylawPhysical and Theoretical ChemistryCrystallizationSupercoolingCondensed Matter - Statistical MechanicsPhysicsCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Disordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural Networks021001 nanoscience & nanotechnology0104 chemical sciencesCondensed Matter::Soft Condensed MatterQuantum TheoryThermodynamicsSoft Condensed Matter (cond-mat.soft)0210 nano-technologyGlass transitionCrystallization
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Growing length scales in a supercooled liquid close to an interface

2002

We present the results of molecular dynamics computer simulations of a simple glass former close to an interface between the liquid and the frozen amorphous phase of the same material. By investigating F_s(q,z,t), the incoherent intermediate scattering function for particles that have a distance z from the wall, we show that the relaxation dynamics of the particles close to the wall is much slower than the one for particles far away from the wall. For small z the typical relaxation time for F_s(q,z,t) increases like exp(Delta/(z-z_p)), where Delta and z_p are constants. We use the location of the crossover from this law to the bulk behavior to define a first length scale tilde{z}. A differe…

Length scaleScattering functionStatistical Mechanics (cond-mat.stat-mech)010304 chemical physicsCondensed matter physicsChemistryGeneral Chemical EngineeringRelaxation (NMR)FOS: Physical sciencesGeneral Physics and AstronomyDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural Networks01 natural sciencesAmorphous phaseMolecular dynamics[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]0103 physical sciences010306 general physicsSupercoolingCondensed Matter - Statistical MechanicsAnsatzPhilosophical Magazine B
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Classical and ab-initio molecular dynamic simulation of an amorphous silica surface

2001

We present the results of a classical molecular dynamic simulation as well as of an ab initio molecular dynamic simulation of an amorphous silica surface. In the case of the classical simulation we use the potential proposed by van Beest et al. (BKS) whereas the ab initio simulation is done with a Car-Parrinello method (CPMD). We find that the surfaces generated by BKS have a higher concentration of defects (e.g. concentration of two-membered rings) than those generated with CPMD. In addition also the distribution functions of the angles and of the distances are different for the short rings. Hence we conclude that whereas the BKS potential is able to reproduce correctly the surface on the …

Length scaleSurface (mathematics)Car–Parrinello molecular dynamicsMaterials scienceStatistical Mechanics (cond-mat.stat-mech)Ab initioFOS: Physical sciencesGeneral Physics and AstronomyDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksApproxCondensed Matter::Disordered Systems and Neural NetworksMolecular dynamicsDistribution functionHardware and ArchitectureChemical physicsAmorphous silicaCondensed Matter - Statistical MechanicsComputer Physics Communications
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