Search results for "FOS"

showing 10 items of 15075 documents

Minimality via second variation for microphase separation of diblock copolymer melts

2017

Abstract We consider a non-local isoperimetric problem arising as the sharp interface limit of the Ohta–Kawasaki free energy introduced to model microphase separation of diblock copolymers. We perform a second order variational analysis that allows us to provide a quantitative second order minimality condition. We show that critical configurations with positive second variation are indeed strict local minimizers of the problem. Moreover, we provide, via a suitable quantitative inequality of isoperimetric type, an estimate of the deviation from minimality for configurations close to the minimum in the L 1 {L^{1}} -topology.

49Q10isoperimetric problemsApplied MathematicsGeneral Mathematics010102 general mathematicsSeparation (aeronautics)Mathematical analysisOrder (ring theory)Type (model theory)01 natural sciences010101 applied mathematicsMathematics - Analysis of PDEsinterfacial problemsFOS: MathematicsCopolymercopolymersLimit (mathematics)0101 mathematicsVariational analysisIsoperimetric inequalityTopology (chemistry)Analysis of PDEs (math.AP)Mathematics
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Wind accretion in the massive X-ray binary 4U 2206+54: abnormally slow wind and a moderately eccentric orbit

2006

Massive X-ray binaries are usually classified depending on the properties of the donor star in classical, supergiant and Be X-ray binaries. The massive X-ray binary 4U 2206+54 does not fit in any of these groups, and deserves a detailed study to understand how the transfer of matter and the accretion on to the compact object take place. To this end we study an IUE spectrum of the donor and obtain a wind terminal velocity (v_inf) of ~350 km/s, which is abnormally slow for its spectral type. We also analyse here more than 9 years of available RXTE/ASM data. We study the long-term X-ray variability of the source and find it to be similar to that observed in the wind-fed supergiant system Vela …

4U 2206+54X-ray binaryBinary numberFOS: Physical sciencesOutflows Emission-lineOrbital eccentricityAstrophysicsWindsCompact starUNESCO::ASTRONOMÍA Y ASTROFÍSICAVelaAstrophysicsIndividual starsPhysicsAstrophysics (astro-ph)BD +53◦2790BeAstronomy and AstrophysicsOrbital period:ASTRONOMÍA Y ASTROFÍSICA::Cosmología y cosmogonia [UNESCO]Accretion (astrophysics)X-rays binariesX-rays individualsX-rays binaries ; X-rays individuals ; 4U 2206+54 ; Individual stars ; BD +53◦2790 ; Winds ; Outflows Emission-line ; BeSpace and Planetary ScienceUNESCO::ASTRONOMÍA Y ASTROFÍSICA::Cosmología y cosmogoniaSupergiant:ASTRONOMÍA Y ASTROFÍSICA [UNESCO]
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Photon emissivity of the quark-gluon plasma: A lattice QCD analysis of the transverse channel

2022

We present results for the thermal photon emissivity of the quark-gluon plasma derived from spatially transverse vector correlators computed in lattice QCD at a temperature of 250 MeV. The analysis of the spectral functions, performed at fixed spatial momentum, is based on continuum-extrapolated correlators obtained with two flavours of dynamical Wilson fermions. We compare the next-to-leading order perturbative QCD correlators, as well as the ${\cal N}=4$ supersymmetric Yang-Mills correlators at infinite coupling, to the correlators from lattice QCD and find them to lie within $\sim10\%$ of each other. We then refine the comparison, performing it at the level of filtered spectral functions…

530 PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyQuark-gluon plasmaFOS: Physical scienceshep-lathep-phParticle Physics - LatticeLattice QCD530 PhysikHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics::Experimentquark productionPhoton lepton &ampParticle Physics - Phenomenology
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Sterile neutrinos as dark matter candidates

2021

In these brief lecture notes, we introduce sterile neutrinos as dark matter candidates. We discuss in particular their production via oscillations, their radiative decay, as well as possible observational signatures and constraints.

530 PhysicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::PhenomenologyFOS: Physical scienceshep-ph530 Physik01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsParticle Physics - PhenomenologySciPost Physics Lecture Notes
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A Universal Length-Dependent Vibrational Mode in Graphene Nanoribbons

2019

Graphene nanoribbons (GNRs) have attracted considerable interest as their atomically tunable structure makes them promising candidates for future electronic devices. However, obtaining detailed information about the length of GNRs has been challenging and typically relies on low-temperature scanning tunneling microscopy. Such methods are ill-suited for practical device application and characterization. In contrast, Raman spectroscopy is a sensitive method for the characterization of GNRs, in particular for investigating their width and structure. Here, we report on a length-dependent, Raman active low-energy vibrational mode that is present in atomically precise, bottom-up synthesized armch…

530 Physicssubstrate transferSTMFOS: Physical sciencesGeneral Physics and Astronomy02 engineering and technology010402 general chemistryDFT01 natural sciencessymbols.namesakegraphene nanoribbons; Raman spectroscopy; length-dependent mode; STM; substrate transfer; vibrational modes; DFT540 ChemistryMesoscale and Nanoscale Physics (cond-mat.mes-hall)General Materials Sciencevibrational modesCondensed Matter - Materials ScienceCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industryGeneral EngineeringMode (statistics)Materials Science (cond-mat.mtrl-sci)021001 nanoscience & nanotechnology3. Good health0104 chemical sciencesMolecular vibrationRaman spectroscopysymbols570 Life sciences; biologyOptoelectronicslength-dependent mode0210 nano-technologybusinessRaman spectroscopyGraphene nanoribbonsgraphene nanoribbons
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Ahlfors-regular distances on the Heisenberg group without biLipschitz pieces

2015

We show that the Heisenberg group is not minimal in looking down. This answers Problem 11.15 in `Fractured fractals and broken dreams' by David and Semmes, or equivalently, Question 22 and hence also Question 24 in `Thirty-three yes or no questions about mappings, measures, and metrics' by Heinonen and Semmes. The non-minimality of the Heisenberg group is shown by giving an example of an Ahlfors $4$-regular metric space $X$ having big pieces of itself such that no Lipschitz map from a subset of $X$ to the Heisenberg group has image with positive measure, and by providing a Lipschitz map from the Heisenberg group to the space $X$ having as image the whole $X$. As part of proving the above re…

53C17 22F50 22E25 14M17General MathematicsSpace (mathematics)Heisenberg group01 natural sciencesMeasure (mathematics)Image (mathematics)Set (abstract data type)Ahlfors-regular distancesMathematics - Metric Geometry53C170103 physical sciencesClassical Analysis and ODEs (math.CA)FOS: MathematicsHeisenberg groupMathematics::Metric GeometryMathematics (all)22E250101 mathematicsMathematicsDiscrete mathematicsmatematiikkamathematicsMathematics::Complex Variables010308 nuclear & particles physicsta111010102 general mathematicsMetric Geometry (math.MG)Lipschitz continuityMetric spaceMathematics - Classical Analysis and ODEsBounded function14M17; 22E25; 22F50; 53C17; Mathematics (all)14M1722F50
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Multiple facets of inverse continuity

2021

International audience; Inversion of various inclusions that characterize continuity in topological spaces results in numerous variants of quotient and perfect maps. In the framework of convergences, the said inclusions are no longer equivalent, and each of them characterizes continuity in a different concretely reflective subcategory of convergences. On the other hand, it turns out that the mentioned variants of quotient and perfect maps are quotient and perfect maps with respect to these subcategories. This perspective enables use of convergence-theoretic tools in quests related to quotient and perfect maps, considerably simplifying the traditional approach. Similar techniques would be un…

54A20 54C10General Topology (math.GN)FOS: Mathematics[MATH] Mathematics [math][MATH]Mathematics [math]Mathematics - General Topology
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Group topologies coarser than the Isbell topology

2011

Abstract The Isbell, compact-open and point-open topologies on the set C ( X , R ) of continuous real-valued maps can be represented as the dual topologies with respect to some collections α ( X ) of compact families of open subsets of a topological space X . Those α ( X ) for which addition is jointly continuous at the zero function in C α ( X , R ) are characterized, and sufficient conditions for translations to be continuous are found. As a result, collections α ( X ) for which C α ( X , R ) is a topological vector space are defined canonically. The Isbell topology coincides with this vector space topology if and only if X is infraconsonant. Examples based on measure theoretic methods, t…

54C35 54C40 54A10Function spaceGroup (mathematics)HyperspaceGeneral Topology (math.GN)Isbell topologyInfraconsonanceTopological spaceFunction spaceTopologyTopological vector spaceTopological groupFunctional Analysis (math.FA)Mathematics - Functional AnalysisHyperspaceFOS: MathematicsTopological groupGeometry and TopologyConsonanceTopology (chemistry)Vector spaceMathematicsMathematics - General Topology
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Variations of selective separability II: Discrete sets and the influence of convergence and maximality

2012

A space $X$ is called selectively separable(R-separable) if for every sequence of dense subspaces $(D_n : n\in\omega)$ one can pick finite (respectively, one-point) subsets $F_n\subset D_n$ such that $\bigcup_{n\in\omega}F_n$ is dense in $X$. These properties are much stronger than separability, but are equivalent to it in the presence of certain convergence properties. For example, we show that every Hausdorff separable radial space is R-separable and note that neither separable sequential nor separable Whyburn spaces have to be selectively separable. A space is called \emph{d-separable} if it has a dense $\sigma$-discrete subspace. We call a space $X$ D-separable if for every sequence of …

54D65 54A25 54D55 54A20H-separable spaceSubmaximalD+-separable spaceSequential spaceFUNCTION-SPACESSeparable spaceSpace (mathematics)INVARIANTSSeparable spaceCombinatoricsGN-separable spaceStrong fan tightnessM-separable spaceMaximal spaceConvergence (routing)Radial spaceFOS: MathematicsFréchet spaceCountable setStratifiable spaceWhyburn propertyTOPOLOGIESDH+-separable spaceTightnessMathematics - General TopologyMathematicsDH-separable spaceD-separable spaceSequenceExtra-resolvable spaceGeneral Topology (math.GN)Hausdorff spaceResolvableR-separable spaceLinear subspaceResolvable spaceSequentialDiscretely generated spaceSubmaximal spaceGeometry and TopologyTOPOLOGIES; FUNCTION-SPACES; INVARIANTSSS+ spaceFan tightnessCrowded spaceSubspace topologyTopology and its Applications
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Spectral sequence associated with a symplectic manifold

2006

A method of computation of its terms is presented together with some stabilization results. As an application a characterization of symplectic harmonic manifolds is given and a relationship with the C-spectral sequence is indicated.

55 T05Mathematics - Geometric Topology53D05Mathematics - Symplectic GeometryFOS: MathematicsSymplectic Geometry (math.SG)Geometric Topology (math.GT)53D05; 55 T05Mathematics::Symplectic Geometry
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