Search results for "Anisotropy"

showing 10 items of 912 documents

Production and detection of atomic hexadecapole at Earth's magnetic field

2007

Anisotropy of atomic states is characterized by population differences and coherences between Zeeman sublevels. It can be efficiently created and probed via resonant interactions with light, the technique which is at the heart of modern atomic clocks and magnetometers. Recently, nonlinear magneto-optical techniques have been developed for selective production and detection of higher polarization moments, hexadecapole and hexacontatetrapole, in the ground states of the alkali atoms. Extension of these techniques into the range of geomagnetic fields is important for practical applications. This is because hexadecapole polarization corresponding to the $\Delta M=4$ Zeeman coherence, with maxim…

Angular momentumLightEarth PlanetMagnetometerAtomic Physics (physics.atom-ph)TransducersPopulationFOS: Physical sciencesRadiation Dosagelaw.inventionPhysics - Atomic PhysicsMagneticssymbols.namesakelawPhysical Sciences and MathematicsScattering RadiationComputer SimulationPhysics::Atomic PhysicsRadiometryAnisotropyeducationPhysicseducation.field_of_studyZeeman effectEquipment DesignModels TheoreticalPolarization (waves)Atomic and Molecular Physics and OpticsAtomic clockMagnetic fieldEquipment Failure AnalysisBudker [BRII recipient]symbolsComputer-Aided DesignAtomic physicsEnvironmental Monitoring
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A Precessing Ferromagnetic Needle Magnetometer

2016

A ferromagnetic needle is predicted to precess about the magnetic field axis at a Larmor frequency $\Omega$ under conditions where its intrinsic spin dominates over its rotational angular momentum, $N\hbar \gg I\Omega$ ($I$ is the moment of inertia of the needle about the precession axis and $N$ is the number of polarized spins in the needle). In this regime the needle behaves as a gyroscope with spin $N\hbar$ maintained along the easy axis of the needle by the crystalline and shape anisotropy. A precessing ferromagnetic needle is a correlated system of $N$ spins which can be used to measure magnetic fields for long times. In principle, by taking advantage of rapid averaging of quantum unce…

Angular momentumMagnetometerPhysics::Medical PhysicsFOS: Physical sciencesGeneral Physics and Astronomy02 engineering and technology01 natural scienceslaw.inventionComputer Science::RoboticslawMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciences010306 general physicsSpin (physics)PhysicsLarmor precessionQuantum PhysicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsMoment of inertia021001 nanoscience & nanotechnologyMagnetic fieldMagnetic anisotropyPhysics::Space PhysicsPrecessionQuantum Physics (quant-ph)0210 nano-technology
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Effect of laboratory procedures on the integrity of a sandy-loam soil sample for bi-directional measurement of saturated hydraulic conductivity

2011

Practical and validated methods to measure anisotropy of saturated, Ks, or field-saturated, Kfs, soil hydraulic conductivity on a single soil sample are still lacking. The objective of this investigation was to test factors affecting anisotropy measured in a sandy-loam soil by the constant-head laboratory permeameter and the modified cube method. The ratio, RK, between the conductivity results obtained with a long (6 h) and a short (0.5 h) duration run varied from a minimum of 0.29 to a maximum of 0.88 with the considered experimental procedure, differing by both the employed constant-head device (Mariotte bottle, siphon) and the initial soil water content (unsaturated, saturated). Maximum …

Anisotropy Constant head permeameter Saturated soil hydraulic conductivitySettore AGR/08 - Idraulica Agraria E Sistemazioni Idraulico-Forestali
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Wulff shape characterizations in overdetermined anisotropic elliptic problems

2017

We study some overdetermined problems for possibly anisotropic degenerate elliptic PDEs, including the well-known Serrin's overdetermined problem, and we prove the corresponding Wulff shape characterizations by using some integral identities and just one pointwise inequality. Our techniques provide a somehow unified approach to this variety of problems.

Applied Mathematics010102 general mathematicsDegenerate energy levelsMathematical analysisMathematics::Analysis of PDEsElliptic pdesComputer Science::Numerical Analysis01 natural sciencesMathematics::Numerical Analysis010101 applied mathematicsOverdetermined systemMathematics - Analysis of PDEsNonlinear Sciences::Exactly Solvable and Integrable SystemsSettore MAT/05 - Analisi MatematicaOverdetermined problems. Finsler manifold. Wulff shapes. Torsion problem. CapacityFOS: MathematicsMathematics::Differential GeometryFinsler manifold0101 mathematicsAnisotropyAnalysisAnalysis of PDEs (math.AP)Mathematics
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Stress concentration for closely located inclusions in nonlinear perfect conductivity problems

2019

We study the stress concentration, which is the gradient of the solution, when two smooth inclusions are closely located in a possibly anisotropic medium. The governing equation may be degenerate of $p-$Laplace type, with $1<p \leq N$. We prove optimal $L^\infty$ estimates for the blow-up of the gradient of the solution as the distance between the inclusions tends to zero.

Applied Mathematics010102 general mathematicsMathematical analysisDegenerate energy levelsZero (complex analysis)Perfect conductorAnalysiGradient blow-upType (model theory)Conductivity01 natural sciences010101 applied mathematicsNonlinear systemMathematics - Analysis of PDEsFOS: MathematicsFinsler p-Laplacian0101 mathematicsPerfect conductorAnisotropy35J25 35B44 35B50 (Primary) 35J62 78A48 58J60 (Secondary)AnalysisAnalysis of PDEs (math.AP)MathematicsStress concentration
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The Euler–Lagrange equation for the Anisotropic least gradient problem

2016

Abstract In this paper we find the Euler–Lagrange equation for the anisotropic least gradient problem inf { ∫ Ω ϕ ( x , D u ) : u ∈ B V ( Ω ) , u | ∂ Ω = f } being ϕ a metric integrand and f ∈ L 1 ( ∂ Ω ) . We also characterize the functions of ϕ -least gradient as those whose boundary of the level set is ϕ -area minimizing in Ω .

Applied Mathematics010102 general mathematicsMathematical analysisGeneral EngineeringBoundary (topology)General Medicine01 natural sciences010101 applied mathematicsEuler–Lagrange equationComputational MathematicsLevel setMetric (mathematics)0101 mathematicsAnisotropyGeneral Economics Econometrics and FinanceAnalysisMathematicsNonlinear Analysis: Real World Applications
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Rotation of methyl radicals in a solid krypton matrix

2009

Electron spin resonance (ESR) measurements were carried out to study the rotation of methyl radicals (CH(3)) in a solid krypton matrix at 17-31 K temperature range. The radicals were produced by dissociating methane by plasma bursts generated by a focused 193 nm excimer laser radiation during the krypton gas condensation on the substrate. The ESR spectrum exhibits only isotropic features at the temperature range examined, and the intensity ratio between the symmetric (A) and antisymmetric (E) spin state lines exhibits weaker temperature dependence than in a solid argon matrix. However, the general appearance of the methyl radical spectrum depends strongly on temperature due to the pronounce…

ArgonSpin statesKryptonGeneral Physics and Astronomychemistry.chemical_elementlaw.inventionchemistrylawExcited statePhysics::Chemical PhysicsPhysical and Theoretical ChemistryAtomic physicsGround stateAnisotropyElectron paramagnetic resonanceHyperfine structureThe Journal of Chemical Physics
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Rational enantioselective design of chiral heterobimetallic single-chain magnets: synthesis, crystal structures and magnetic properties of oxamato-br…

2011

A new series of neutral oxamato-bridged M(II)Cu(II) chiral chains of general formula [MCuL(x)(S)(m)(H(2)O)(n)]·aS·bH(2)O [L(1)=(M)-1,1'-binaphthalene-2,2'-bis(oxamate) with M=Mn (1a) and Co (1b); L(2)=(P)-1,1'-binaphthalene-2,2'-bis(oxamate) with M=Mn (2a) and Co (2b)] and the analogous racemic chains of formula [MCuL(3)(S)(m)(H(2)O)(n)]·aS·bH(2)O [L(3)=1,1'-binaphthalene-2,2'-bis(oxamate) with M=Mn (3a) and Co (3b)] have been prepared by reaction of the corresponding dianionic oxamatocopper(II) complex [Cu(L(x))](2-) with Mn(2+) or Co(2+) cations in either dimethylformamide (DMF) or dimethyl sulfoxide (DMSO). Solid circular dichroism (CD) spectra of the bimetallic chain compounds were reco…

Arrhenius equation010405 organic chemistryChemistryStereochemistryOrganic ChemistryGeneral ChemistryCrystal structure010402 general chemistry01 natural sciencesCatalysis0104 chemical sciencessymbols.namesakeMagnetic anisotropyMagnetizationchemistry.chemical_compoundCrystallographyEnantiopure drugsymbolsDimethylformamide[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]EnantiomerChirality (chemistry)ComputingMilieux_MISCELLANEOUSChemistry (Weinheim an der Bergstrasse, Germany)
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Coligand Effects on the Field-Induced Double Slow Magnetic Relaxation in Six-Coordinate Cobalt(II) Single-Ion Magnets (SIMs) with Positive Magnetic A…

2019

Two mononuclear cobalt(II) compounds of formula [Co(dmphen)2(OOCPh)]ClO4·1/2H2O·1/2CH3OH (1) and [Co(dmbipy)2(OOCPh)]ClO4 (2) (dmphen = 2,9-dimethyl-1,10-phenanthroline, dmbipy = 6,6'-dimethyl-2,2'-bipyridine and HOOCPh = benzoic acid) are prepared and magnetostructurally investigated. Each cobalt(II) ion is six-coordinate with a distorted octahedral CoN4O2 environment. The complex cations are interlinked leading to supramolecular chains (1) and pairs (2) that grow along the crystallographic c-axis with racemic mixtures of (Δ,Λ)-Co units. FIRMS allowed us to directly measure the zero-field splitting between the two lowest Kramers doublets, which led to axial anisotropy values of 58.3 cm-1 ≤…

Arrhenius equation010405 organic chemistryRelaxation (NMR)chemistry.chemical_element010402 general chemistry01 natural sciences0104 chemical sciencesIonInorganic Chemistrysymbols.namesakeCrystallographyBipyridinechemistry.chemical_compoundMagnetic anisotropychemistrysymbolsPhysical and Theoretical ChemistryRaman spectroscopyAnisotropyCobaltInorganic chemistry
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Mössbauer relaxation spectra in arbitrarily ordered absorbers—Line shape analysis for an iron(II) spincrossover complex in the presence of texture

1989

The stochastic theory of Mossbauer line shapes is formulated in a fashion which allows the evaluation of the spectral shapes for absorbers of arbitrary thickness, texture, and an anisotropic Lamb—Mossbauer factor. The results are specialized to a two-state-relaxation model of fluctuating electric hyperfine interaction in the case of an absorber of axially symmetric texture. The formalism is applied to the line shape analysis of Mossbauer spectra of a textured sample of the spin-crossover complex [Fe(mtz)6] (PF6)2 (mtz=1-methyltetrazole). It is found that between 185 and 240 K the rate constants for the HS→LS conversion are temperature independent, whereas an Arrhenius behaviour is found for…

Arrhenius equationNuclear and High Energy PhysicsMaterials scienceCondensed Matter PhysicsMolecular physicsAtomic and Molecular Physics and OpticsSpectral lineCrystallographysymbols.namesakeReaction rate constantMössbauer spectroscopysymbolsPhysical and Theoretical ChemistryAnisotropyAxial symmetryHyperfine structureShape analysis (digital geometry)Hyperfine Interactions
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