Search results for "Maxim"

showing 10 items of 1236 documents

Coordination and profit rate maximization

1995

We study the effects over the coordination between firms of the choice of another objectivefunction for the firm: the profit rate maximization which seems to be closer to business practice than the classical pure profit maximization. After recalling the effect of the new objective function over the optimum (the optimal production is lower), two cases are considered : perfect competition (the price signal disappear), and duopoly-oligopoly (the functions of reactions may vanish). (FR) Nous étudions les effets sur la coordination inter-firmes du choix d'une autre fonction objectif pour la firme: la maximisation du taux de profit qui semble être plus proche de la pratique des affaires que la cl…

Control theoryCoordinationStatisticsMaximizationProfit[ SHS.ECO ] Humanities and Social Sciences/Economies and financesMicroeconomic behaviours of fishermen[SHS.ECO]Humanities and Social Sciences/Economics and Finance[SHS.ECO] Humanities and Social Sciences/Economics and FinanceProfit rateOperational researchRecherche opérationnelleAutomatique
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In-situ monitoring by Raman spectroscopy of the thermal doping of graphene and MoS2 in O-2-controlled atmosphere

2017

The effects of temperature and atmosphere (air and O2) on the doping of monolayers of graphene (Gr) on SiO2 and Si substrates, and on the doping of MoS2 multilayer flakes transferred on the same substrates have been investigated. The investigations were carried out by in situ micro-Raman spectroscopy during thermal treatments up to 430 °C, and by atomic force microscopy (AFM). The spectral positions of the G and 2D Raman bands of Gr undergo only minor changes during treatment, while their amplitude and full width at half maximum (FWHM) vary as a function of the temperature and the used atmosphere. The thermal treatments in oxygen atmosphere show, in addition to a thermal effect, an effect a…

Controlled atmosphereMaterials science2Analytical chemistrythermal dopingGeneral Physics and Astronomychemistry.chemical_elementtwo-dimensional (2D) materials02 engineering and technologyMoSlcsh:Chemical technology010402 general chemistrylcsh:Technology01 natural sciencesOxygenFull Research Paperlaw.inventionPhysics and Astronomy (all)symbols.namesakelawMonolayerNanotechnologylcsh:TP1-1185General Materials ScienceElectrical and Electronic Engineeringlcsh:ScienceSpectroscopylcsh:TGrapheneSettore FIS/01 - Fisica SperimentaleDopinggraphenetechnology industry and agriculture021001 nanoscience & nanotechnologylcsh:QC1-9990104 chemical sciencesNanoscienceFull width at half maximumTwo-dimensional (2D) materialchemistryRaman spectroscopysymbolslcsh:QMaterials Science (all)0210 nano-technologyRaman spectroscopyMoS2lcsh:Physics
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Singular Double Phase Problems with Convection

2020

We consider a nonlinear Dirichlet problem driven by the sum of a $p$ -Laplacian and of a $q$ -Laplacian (double phase equation). In the reaction we have the combined effects of a singular term and of a gradient dependent term (convection) which is locally defined. Using a mixture of variational and topological methods, together with suitable truncation and comparison techniques, we prove the existence of a positive smooth solution.

ConvectionDirichlet problemPartial differential equationTruncationApplied Mathematics010102 general mathematicsMathematical analysisSingular termFixed pointMathematics::Spectral Theory01 natural sciencesTerm (time)Positive solution010101 applied mathematicsNonlinear system(p q)-LaplacianSettore MAT/05 - Analisi MatematicaNonlinear maximum principle0101 mathematicsLaplace operatorNonlinear regularityMathematicsActa Applicandae Mathematicae
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Positive solutions for nonlinear Robin problems with convection

2019

We consider a nonlinear Robin problem driven by the p-Laplacian and with a convection term f(z,x,y). Without imposing any global growth condition on f(z,·,·) and using topological methods (the Leray-Schauder alternative principle), we show the existence of a positive smooth solution.

ConvectionGeneral Mathematicsnonlinear maximum principlep-LaplacianGeneral Engineering(minimal) positive solutionNonlinear systemEngineering (all)p-LaplacianApplied mathematicsnonlinear regularityMathematics (all)convection termLeray-Schauder alternative principleMathematics
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Propagation of uncertainties in the Skyrme energy-density-functional model

2013

Parameters of nuclear energy-density-functionals (EDFs) are always derived by an optimization to experimental data. For the minima of appropriately defined penalty functions, a statistical sensitivity analysis provides the uncertainties of the EDF parameters. To quantify theoretical errors of observables given by the model, we studied the propagation of uncertainties within the UNEDF0 Skyrme-EDF approach. We found that typically the standard errors rapidly increase towards neutron rich nuclei. This can be linked to large uncertainties of the isovector coupling constants of the currently used EDFs.

Coupling constantPhysicsNuclear and High Energy PhysicsIsovectorEnergy density functionalta114Nuclear Theory010308 nuclear & particles physicsStatistical sensitivityNuclear TheoryCharge densityFOS: Physical sciencesObservable01 natural sciencesMaxima and minimaNuclear physicsNuclear Theory (nucl-th)0103 physical sciencesNeutron010306 general physicsComputer Science::Operating Systems
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Simulated annealing with restrained molecular dynamics using a flexible restraint potential: Theory and evaluation with simulated NMR constraints

1996

A new functional representation of NMR-derived distance constraints, the flexible restraint potential, has been implemented in the program CONGEN (Bruccoleri RE, Karplus M, 1987, Biopolymers 26:137-168) for molecular structure generation. In addition, flat-bottomed restraint potentials for representing dihedral angle and vicinal scalar coupling constraints have been introduced into CONGEN. An effective simulated annealing (SA) protocol that combines both weight annealing and temperature annealing is described. Calculations have been performed using ideal simulated NMR constraints, in order to evaluate the use of restrained molecular dynamics (MD) with these target functions as implemented i…

Coupling constantQuantitative Biology::BiomoleculesChemistryCrambinNuclear magnetic resonance spectroscopyDihedral angleEnergy minimizationBiochemistryMolecular physicsMaxima and minimaMolecular dynamicsCrystallographySimulated annealingMolecular BiologyProtein Science
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Radiation damage in zircon

2003

A single, zoned, Sri Lankan zircon exhibits a range of microstructures from crystalline to nearly amorphous that are the result of radiation damage over a dose range of 2.1–10.1·1015 α-decay events/mg (0.16–0.47 dpa). The zones in the crystal were examined at a variety of length scales using optical microscopy, micro-Raman spectroscopy, electron microprobe analysis, and transmission electron microscopy. Birefringence varies linearly with dose: birefringence = −4.71·10−18 /g· D α + 4.86·10−2. Full width at half maximum (FWHM) measurements of the B1g(ν3) peak, as determined by micro-Raman spectroscopy, were used to estimate the extent of radiation damage in each zone. The radiation dose (calc…

CrystalFull width at half maximumGeophysicsGeochemistry and PetrologyTransmission electron microscopyAnalytical chemistryRadiation damageMineralogyElectron microprobeSpectroscopyGeologyZirconAmorphous solidAmerican Mineralogist
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Photoluminescence excited by ArF and KrF lasers and optical absorption of stishovite mono-crystal

2008

Two photoluminescence bands were found in a stishovite (silicon dioxide) mono-crystal sample under ArF (193 nm) and KrF (248 nm) excitation. The blue band is situated at 3.17 ± 0.02 eV in the case of ArF and at 3 ± 0.2 in the case of KrF. The UV band is at 4.55 ± 0.05 eV in the case of ArF and at 4.5 ± 0.05 eV in the case of KrF. The position of the UV emission band correlates with that excited by x rays. This position is 4.6 ± 0.05 eV with FWHM 0.8 ± 0.05 eV (Truhins et al 2003 Solid State Commun. 127 415). The blue band possesses slow decay kinetics with time constant 16 ± 2 µs and the UV band is fast on the level of 2 ± 0.5 ns, similarly for both lasers. Thermal quenching of both bands b…

CrystalFull width at half maximumPhotoluminescenceChemistryExcited stateGeneral Materials ScienceIrradiationAtomic physicsCondensed Matter PhysicsLuminescenceAbsorption (electromagnetic radiation)StishoviteJournal of Physics: Condensed Matter
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Coupled rotational and translational modes in the mixed molecular crystal KBr1?x (CN) x

1980

TheE g andT 2g acoustic phonon modes of the molecular crystals KBr0.96(CN)0.04 and KBr0.86(CN)0.14 have been investigated by inelastic neutron scattering at 6, 90 and 300 K. Clear resonances due to mode-mode coupling to molecular excitations were observed. In complementary ultrasonic experiments the elastic constants were found to pass through minima as a function of temperature. The results were quantitavely explained by a model which assumes simple forms of the molecular excitation spectrum. An alternative interpretation, though being only qualitative, postulates a freezing of the CN molecules into a glass-like phase.

CrystalMaxima and minimaCouplingMaterials sciencePhononPhase (matter)MoleculeAtomic physicsCondensed Matter PhysicsInelastic neutron scatteringExcitationElectronic Optical and Magnetic MaterialsZeitschrift f�r Physik B Condensed Matter
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(Z)-4-(2-Naphthylamino)pent-3-en-2-one

2011

The title compound, C15H15NO, which was synthesized under solvent-free conditions by the reaction of acetoacetone and 2-naphthylamine, adopts a Z conformation about the C=C bond. The enamine–ketone fragment is approximately planar [maximum deviation = 0.026 (3) Å] and forms a dihedral angle of 39.78 (3)° with the naphthalene ring system. An intramolecular N—H...O hydrogen bond is observed.

CrystallographyHydrogen bondMaximum deviationGeneral ChemistryDihedral angleCondensed Matter PhysicsRing (chemistry)BioinformaticsOrganic Paperschemistry.chemical_compoundCrystallographychemistryQD901-999General Materials ScienceNaphthaleneActa Crystallographica Section E
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