Search results for "Standing wave"

showing 10 items of 30 documents

Atomic Coherence Effects in Doppler-Broadened Three-Level Systems with Standing-Wave Drive

2001

We study atomic coherence effects (e.g., electromagnetically induced transparency, EIT, and amplification without inversion, AWI) for a probe travelling-wave (TW) laser field in closed Doppler-broadened three-level systems driven by a standingwave (SW) laser field of moderate intensity (its Rabi frequencies are smaller than the Doppler width of the driven transition). We show that probe windows of transparency occur only for values of the probe to drive field frequency ratio R close to half integer values. For optical transitions and typical values of Doppler broadening for atoms in a vapor cell, we show that for R > 1 a SW drive field is appreciably more efficient than a TW drive in induci…

Physicsbusiness.industryElectromagnetically induced transparencyLaserAtomic coherencelaw.inventionStanding wavesymbols.namesakeOpticsCascadelawsymbolsHalf-integerPhysics::Atomic PhysicsAtomic physicsbusinessDoppler effectDoppler broadening
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Investigation of Phosphorylation-Induced Folding of an Intrinsically Disordered Protein by Coarse-Grained Molecular Dynamics

2021

Apart from being the most common mechanism of regulating protein function and transmitting signals throughout the cell, phosphorylation has an ability to induce disorder-to-order transition in an intrinsically disordered protein. In particular, it was shown that folding of the intrinsically disordered protein, eIF4E-binding protein isoform 2 (4E-BP2), can be induced by multisite phosphorylation. Here, the principles that govern the folding of phosphorylated 4E-BP2 (pT37pT46 4E-BP2(18–62)) are investigated by analyzing canonical and replica exchange molecular dynamics trajectories, generated with the coarse-grained united-residue force field, in terms of local and global motions and the time…

Protein isoformPhysicsProtein functionProtein Folding010304 chemical physicsMolecular Dynamics Simulation01 natural sciencesForce field (chemistry)ArticleComputer Science ApplicationsFolding (chemistry)Standing waveIntrinsically Disordered Proteinssymbols.namesakeMolecular dynamicsChemical physics0103 physical sciencessymbolsPhosphorylationThermodynamicsPhysical and Theoretical ChemistryPhosphorylationNonlinear Schrödinger equation
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A theoretical approach of the propagation through geometrical constraints in cardiac tissue

2007

International audience; The behaviour of impulse propagation in the presence of non-excitable scars and boundaries is a complex phenomenon and induces pathological consequences in cardiac tissue. In this article, a geometrical con¯guration is considered so that cardiac waves propagate through a thin strand, which is connected to a large mass of cells. At this interface, waves can slow down or even be blocked depending on the width of the strand. We present an analytical approach leading to determine the blockade condition, by introducing planar travelling wavefront and circular stationary wave. Eventually, the in°uence of the tissue geometry is examined on the impulse propagation velocity.

Quantitative Biology::Tissues and Organs[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS]Physics::Medical PhysicsBlockade phenomenon[MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]Geometry030204 cardiovascular system & hematologyImpulse (physics)Circular stationary waveStanding waveCardiac tissue.03 medical and health sciences0302 clinical medicinePlanar[SDV.MHEP.CSC]Life Sciences [q-bio]/Human health and pathology/Cardiology and cardiovascular system[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]FitzHugh–Nagumo model[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]Engineering (miscellaneous)Cardiac tissue030304 developmental biologyWavefrontPhysicsTravelling wavefront0303 health sciencesApplied Mathematics[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Mechanics[ SDV.MHEP.CSC ] Life Sciences [q-bio]/Human health and pathology/Cardiology and cardiovascular system[PHYS.MPHY] Physics [physics]/Mathematical Physics [math-ph][SDV.MHEP.CSC] Life Sciences [q-bio]/Human health and pathology/Cardiology and cardiovascular systemModeling and Simulation[ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]
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Electromagnetically induced transparency in Doppler-broadened three-level systems with resonant standing wave drive

2005

Summary form only given. Electromagnetically induced transparency (EIT) and related phenomena such as lasing without inversion (LWI) are topics of increasing interest in quantum optics. In EIT, an otherwise absorbing medium is made transparent to a weak coherent field on resonance with a certain atomic transition by applying an intense coherent "driving" field to an adjacent transition. There has been a large number of theoretical papers and EIT was demonstrated experimentally. Up to now, most theoretical papers dealing with EIT in gas media have considered only the case of a traveling (TW) driving field. In contrast, we study EIT in Doppler broadened three-level media with standing wave (S…

Quantum opticsPhysicsField (physics)Electromagnetically induced transparencybusiness.industryPhysics::OpticsResonanceStanding wavesymbols.namesakeOpticssymbolsAstrophysics::Solar and Stellar AstrophysicsFocus (optics)businessDoppler effectDoppler broadeningConference Digest. 2000 International Quantum Electronics Conference (Cat. No.00TH8504)
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MgO/Ag(100): confined vibrational modes in the limit of ultrathin films

2003

The vibrational modes of clean MgO films are investigated vs film thickness by means of high-resolution electron energy-loss spectroscopy. For thin films (20\char21{}30 monolayers) we observe, in accord with the literature, the Fuchs-Kliewer phonon at $677{\mathrm{cm}}^{\ensuremath{-}1}$ and the Wallis mode at $524{\mathrm{cm}}^{\ensuremath{-}1}.$ For ultrathin films standing wave optical phonons confined in the overlayer are present, whose frequencies depend strongly on film thickness. Comparison with theoretical calculations for MgO slabs on a perfect conductor shows that the experimental frequencies are lower than expected, indicating the presence of compressive stress. At and below one-…

Standing waveMaterials scienceNuclear magnetic resonanceCondensed matter physicsPhononMolecular vibrationMonolayerElectronThin filmSpectroscopyOverlayer
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2019

Energy-level alignment at organic-metal interfaces plays a crucial role for the performance of organic electronic devices. However, reliable models to predict energetics at strongly coupled interfaces are still lacking. We elucidate contact formation of 1,2,5,6,9,10-coronenehexone (COHON) to the (1 1 1)-surfaces of coinage metals by means of ultraviolet photoelectron spectroscopy, x-ray photoelectron spectroscopy, the x-ray standing wave technique, and density functional theory calculations. While for low COHON thicknesses, the work-functions of the systems vary considerably, for thicker organic films Fermi-level pinning leads to identical work functions of 5.2 eV for all COHON-covered meta…

Standing waveMaterials scienceX-ray photoelectron spectroscopyChemical physicsX-ray standing wavesCoinage metalsGeneral Materials ScienceWork functionDensity functional theorySubstrate (electronics)Condensed Matter PhysicsUltraviolet photoelectron spectroscopyJournal of Physics: Condensed Matter
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EMERGENCE OF TRAVELLING WAVES IN SMOOTH NERVE FIBRES

2008

International audience; An approximate analytical solution characterizing initial condi- tions leading to action potential ¯ring in smooth nerve ¯bres is determined, using the bistable equation. In the ¯rst place, we present a non-trivial sta- tionary solution wave. Then, we extract the main features of this solution to obtain a frontier condition between the initiation of the travelling waves and a decay to the resting state. This frontier corresponds to a separatrix in the projected dynamics diagram depending on the width and the amplitude of the stationary wave.

StationarityBistability[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][ NLIN.NLIN-CD ] Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD][MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]01 natural sciencesNerve fibresStanding waveOptics[ MATH.MATH-AP ] Mathematics [math]/Analysis of PDEs [math.AP]0103 physical sciencesTraveling wave[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Discrete Mathematics and Combinatorics[MATH.MATH-AP] Mathematics [math]/Analysis of PDEs [math.AP]0101 mathematics010306 general physicsProjected dynamicsPhysicsSeparatrixbusiness.industry[SCCO.NEUR]Cognitive science/NeuroscienceApplied Mathematics[SCCO.NEUR] Cognitive science/NeuroscienceDiagramDynamics (mechanics)Mechanics010101 applied mathematics[NLIN.NLIN-CD] Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD]Amplitude[NLIN.NLIN-CD]Nonlinear Sciences [physics]/Chaotic Dynamics [nlin.CD][ SCCO.NEUR ] Cognitive science/NeuroscienceAction potential firingbusinessAnalysis
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ANALYTICAL DETERMINATION OF INITIAL CONDITIONS LEADING TO FIRING IN NERVE FIBERS

2007

International audience; An analytical solution characterizing initial conditions leading to action potential firing in smooth nerve fibers is determined, using the bistable equation. In the first place, we present a nontrivial stationary solution wave, then, using the perturbative method, we analyze the stability of this stationary wave. We show that it corresponds to a frontier between the initiation of the travelling waves and a decay to the resting state. Eventually, this analytical approach is extended to FitzHugh-Nagumo model.

StationarityBistability[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph][MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS][ MATH.MATH-DS ] Mathematics [math]/Dynamical Systems [math.DS][MATH.MATH-DS] Mathematics [math]/Dynamical Systems [math.DS]01 natural sciencesStability (probability)010305 fluids & plasmasStanding waveOptics[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]0103 physical sciencesReaction–diffusion systemTraveling wave[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]0101 mathematicsEngineering (miscellaneous)PhysicsQuantitative Biology::Neurons and Cognitionbusiness.industry[SCCO.NEUR]Cognitive science/Neurosciencenerve fibersApplied Mathematics[SCCO.NEUR] Cognitive science/Neurosciencereaction-diffusion[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Mechanics[PHYS.MPHY] Physics [physics]/Mathematical Physics [math-ph]010101 applied mathematicsModeling and Simulation[ SCCO.NEUR ] Cognitive science/Neuroscience[ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]Action potential firingbusinessStationary solutionnerve fibers.International Journal of Bifurcation and Chaos
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Growth, domain structure, and atomic adsorption sites of hBN on the Ni(111) surface

2021

One of the most important functionalities of the atomically thin insulator hexagonal boron nitride (hBN) is its ability to chemically and electronically decouple functional materials from highly reactive surfaces. It is therefore of utmost importance to uncover its structural properties on surfaces on an atomic and mesoscopic length scale. In this paper, we quantify the relative coverages of structurally different domains of a hBN layer on the Ni(111) surface using low-energy electron microscopy and the normal incidence x-ray standing wave technique. We find that hBN nucleates on defect sites of the Ni(111) surface and predominantly grows in two epitaxial domains that are rotated by ${60}^{…

Surface (mathematics)Length scaleMesoscopic physicsMaterials sciencePhysics and Astronomy (miscellaneous)Structure (category theory)EpitaxyStanding waveCrystallographyAdsorptionDomain (ring theory)Physics::Atomic and Molecular ClustersGeneral Materials Scienceddc:530
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Multiple positive normalized solutions for nonlinear Schrödinger systems

2018

We consider the existence of multiple positive solutions to the nonlinear Schr\"odinger systems sets on $H^1(\mathbb{R}^N) \times H^1(\mathbb{R}^N)$, \[ \left\{ \begin{aligned} -\Delta u_1 &= \lambda_1 u_1 + \mu_1 |u_1|^{p_1 -2}u_1 + \beta r_1 |u_1|^{r_1-2} u_1|u_2|^{r_2}, -\Delta u_2 &= \lambda_2 u_2 + \mu_2 |u_2|^{p_2 -2}u_2 + \beta r_2 |u_1|^{r_1} |u_2|^{r_2 -2} u_2, \end{aligned} \right. \] under the constraint \[ \int_{\mathbb{R}^N}|u_1|^2 \, dx = a_1,\quad \int_{\mathbb{R}^N}|u_2|^2 \, dx = a_2. \] Here $a_1, a_2 >0$ are prescribed, $\mu_1, \mu_2, \beta>0$, and the frequencies $\lambda_1, \lambda_2$ are unknown and will appear as Lagrange multipliers. Two cases are studied, the first …

geographygeography.geographical_feature_categoryApplied Mathematics010102 general mathematicsGeneral Physics and AstronomyStatistical and Nonlinear Physics01 natural sciences010101 applied mathematicsStanding waveSet (abstract data type)Constraint (information theory)Nonlinear systemsymbols.namesakeMathematics - Analysis of PDEsCompact spaceLagrange multipliersymbolsApplied mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]Mountain pass0101 mathematicsMathematical PhysicsSchrödinger's catComputingMilieux_MISCELLANEOUSMathematics
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