Search results for "43"

showing 10 items of 1438 documents

Spin transport in ferromagnetic/normal-metal tunnel junction arrays

2012

Published version of an article in the journal: Physical Review B. Also available from the publisher:http://dx.doi.org/10.1103/PhysRevB.85.094421 An array of alternating ferromagnetic and normal-metal islands separated by small tunnel junctions is theoretically investigated in the sequential tunneling regime. A numerical Monte Carlo method is used to calculate the transport properties. The spin-dependent tunneling currents give rise to nonequilibrium spin accumulation on the normal island. The tunneling magneto resistance (TMR) is calculated for a large range of array parameters. The TMR oscillates with bias voltage and can become negative for certain array parameters. We show that the long…

PhysicsCondensed matter physicsCoulomb blockadeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsVDP::Mathematics and natural science: 400::Physics: 430Electronic Optical and Magnetic MaterialsMetalSingle electron tunnelingFerromagnetismTunnel junctionvisual_artvisual_art.visual_art_mediumSpin (physics)Physical Review B
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The Fučík spectrum for nonlocal BVP with Sturm–Liouville boundary condition

2014

Boundary value problem of the form x''=-μx++λx-, αx(0)+(1-α)x'(0)=0, ∫01 x(s)ds=0 is considered, where μ,λ∈ R and α∈ [0,1]. The explicit formulas for the spectrum of this problem are given and the spectra for some α values are constructed. Special attention is paid to the spectrum behavior at the points close to the coordinate origin.

PhysicsFucík spectrumApplied MathematicsSturm–Liouville boundary conditionMathematical analysisSpectrum (functional analysis)lcsh:QA299.6-433Sturm–Liouville theorylcsh:AnalysisSpectral lineboundary value problemBoundary value problemAnalysisintegral conditionNonlinear Analysis: Modelling and Control
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Discovery of a jet-like structure with overionized plasma in the SNR IC443

2018

IC443 is a supernova remnant located in a quite complex environment since it interacts with nearby clouds. Indications for the presence of overionized plasma have been found though the possible physical causes of overionization are still debated. Moreover, because of its peculiar position and proper motion, it is not clear if the pulsar wind nebula (PWN) within the remnant is the relic of the IC443 progenitor star or just a rambling one seen in projection on the remnant. Here we address the study of IC443 plasma in order to clarify the relationship PWN-remnant, the presence of overionization and the origin of the latter. We analyzed two \emph{XMM-Newton} observations producing background-su…

PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Jet (fluid)ISM: individual objects: IC443pulsars: individual: CXOU J061705.3+222127010308 nuclear & particles physicsMolecular cloudAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstronomy and AstrophysicsContext (language use)Astrophysics01 natural sciencesPulsar wind nebulaSupernovaNeutron starSpace and Planetary Science0103 physical sciencesEjectaSupernova remnantAstrophysics - High Energy Astrophysical Phenomena010303 astronomy & astrophysicsISM: supernova remnantAstrophysics::Galaxy Astrophysics
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On the critical behavior for inhomogeneous wave inequalities with Hardy potential in an exterior domain

2021

Abstract We study the wave inequality with a Hardy potential ∂ t t u − Δ u + λ | x | 2 u ≥ | u | p in  ( 0 , ∞ ) × Ω , $$\begin{array}{} \displaystyle \partial_{tt}u-{\it\Delta} u+\frac{\lambda}{|x|^2}u\geq |u|^p\quad \mbox{in } (0,\infty)\times {\it\Omega}, \end{array}$$ where Ω is the exterior of the unit ball in ℝ N , N ≥ 2, p > 1, and λ ≥ − N − 2 2 2 $\begin{array}{} \displaystyle \left(\frac{N-2}{2}\right)^2 \end{array}$ , under the inhomogeneous boundary condition α ∂ u ∂ ν ( t , x ) + β u ( t , x ) ≥ w ( x ) on  ( 0 , ∞ ) × ∂ Ω , $$\begin{array}{} \displaystyle \alpha \frac{\partial u}{\partial \nu}(t,x)+\beta u(t,x)\geq w(x)\quad\mbox{on } (0,\infty)\times \partial{\it\Omega}, \e…

PhysicsMathematics::Functional Analysis35b3335b44QA299.6-433critical exponentMathematics::Complex Variables010102 general mathematicsMathematical analysisMathematics::Classical Analysis and ODEshardy potentialMathematics::Spectral Theoryexterior domain01 natural sciencesDomain (software engineering)010101 applied mathematics35l05Settore MAT/05 - Analisi Matematicawave inequalitiesglobal weak solutions0101 mathematicsCritical exponentAnalysisAdvances in Nonlinear Analysis
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Observation of the Resonant Character of theZ(4430)−State

2014

Resonant structures in B-0 -> psi'pi K--(+) decays are analyzed by performing a four-dimensional fit of the decay amplitude, using pp collision data corresponding to 3 fb(-1) collected with the LHCb detector. The data cannot be described with K+pi(-) resonances alone, which is confirmed with a model-independent approach. A highly significant Z(4430)(-) -> psi'pi(-) component is required, thus confirming the existence of this state. The observed evolution of the Z(4430)(-) amplitude with the psi'pi(-) mass establishes the resonant nature of this particle. The mass and width measurements are substantially improved. The spin parity is determined unambiguously to be 1(+).

PhysicsMeson010308 nuclear & particles physicsDetectorGeneral Physics and AstronomyParity (physics)01 natural sciencesNuclear physicsAmplitude0103 physical sciencesHigh Energy Physics::ExperimentZ(4430)Atomic physics010306 general physicsPhysical Review Letters
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On the metal abundances inside mixed-morphology supernova remnants: the case of IC 443  and G166.0+4.3

2009

Recent developments on the study of mixed morphology supernova remnants (MMSNRs) have revealed the presence of metal rich X-ray emitting plasma inside a fraction of these remnant, a feature not properly addressed by traditional models for these objects. Radial profiles of thermodynamical and chemical parameters are needed for a fruitful comparison of data and model of MMSNRs, but these are available only in a few cases. We analyze XMM-Newton data of two MMSNRs, namely IC443 and G166.0+4.3, previously known to have solar metal abundances, and we perform spatially resolved spectral analysis of the X-ray emission. We detected enhanced abundances of Ne, Mg and Si in the hard X-ray bright peak i…

PhysicsMorphology (linguistics)extinctionAstrophysics::High Energy Astrophysical PhenomenaExtinction (astronomy)FOS: Physical sciencesAstronomy and AstrophysicsContext (language use)X-rays: individuals: IC 443AstrophysicsPlasmaAstrophysics - Astrophysics of GalaxiesX-rays: ISMMetalSupernovaISM: dustX-rays: individuals: G166.0+4.3 ISMSpace and Planetary ScienceAstrophysics of Galaxies (astro-ph.GA)visual_artRadiative transfervisual_art.visual_art_mediumSpectral analysisAstrophysics::Galaxy AstrophysicsISM: supernova remnant
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On a differential system arising in the network control theory

2016

We investigate the three-dimensional dynamical system occurring in the network regulatory systems theory for specific choices of regulatory matrix { { 0, 1, 1 } { 1, 0, 1 } { 1, 1, 0 } } and sigmoidal regulatory function f(z) = 1 / (1 + e-μz), where z = ∑ Wij xj - θ. The description of attracting sets is provided. The attracting sets consist of respectively one, two or three critical points. This depends on whether the parameters (μ,θ) belong to a set Ω or to the complement of Ω or to the boundary of Ω, where Ω is fully defined set.

PhysicsNetwork controlPure mathematicsnetwork controlPhase portraitattracting setsApplied Mathematics010102 general mathematicslcsh:QA299.6-433Boundary (topology)phase portraitlcsh:Analysis02 engineering and technology01 natural sciencesdynamical systemSet (abstract data type)Matrix (mathematics)Systems theory0202 electrical engineering electronic engineering information engineering020201 artificial intelligence & image processing0101 mathematicsDynamical system (definition)AnalysisComplement (set theory)Nonlinear Analysis: Modelling and Control
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Photoproduction ofZ(4430)through mesonic Regge trajectories exchange

2011

The recently discovered $Z(4430)$ mesonic resonance is believed to be a strong tetraquark candidate. The photoproduction in the channel $\ensuremath{\gamma}p\ensuremath{\rightarrow}{Z}^{+}(4430)n\ensuremath{\rightarrow}{\ensuremath{\psi}}^{'}{\ensuremath{\pi}}^{+}n$ has been proposed as the most effective way to confirm the $Z(4430)$ presence and to measure its quantum numbers. In this work we present a model for high-energy and forward-angle $Z(4430)$ photoproduction in a effective Lagrangian approach. This model is based on the use of Regge trajectories exchange, thus a Regge propagator replaces the usual Feynman propagator. The differential and total cross sections and the asymmetries ha…

PhysicsNuclear and High Energy PhysicsParticle decayParticle physicsMesonIsospinHigh Energy Physics::PhenomenologyHadronPropagatorHigh Energy Physics::ExperimentZ(4430)TetraquarkQuantum numberPhysical Review C
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Model-independent confirmation of theZ(4430)−state

2015

The decay $B^0\to \psi(2S) K^+\pi^-$ is analyzed using $\rm 3~fb^{-1}$ of $pp$ collision data collected with the LHCb detector. A model-independent description of the $\psi(2S) \pi$ mass spectrum is obtained, using as input the $K\pi$ mass spectrum and angular distribution derived directly from data, without requiring a theoretical description of resonance shapes or their interference. The hypothesis that the $\psi(2S)\pi$ mass spectrum can be described in terms of $K\pi$ reflections alone is rejected with more than 8$\sigma$ significance. This provides confirmation, in a model-independent way, of the need for an additional resonant component in the mass region of the $Z(4430)^-$ exotic sta…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsState (functional analysis)Interference (wave propagation)01 natural sciencesResonance (particle physics)Nuclear physicsReflection (mathematics)Angular distribution0103 physical sciencesMass spectrumZ(4430)010306 general physicsPhysical Review D
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Search for theZ(4430)−atBABAR

2009

We report the results of a search for Z(4430)^- decay to J/Ψ π^- or Ψ(2S)π^- in B(^-.0)→ J/Ψ π^-K^(0.+) and B^(-.0) → Ψ(2S)π^-K^(0.+) decays. The data were collected with the BABAR detector at the SLAC PEP-II asymmetric-energy e^+e^- collider operating at center-of-mass energy 10.58 GeV, and the sample corresponds to an integrated luminosity of 413 fb^(-1). Each K π^- mass distribution exhibits clear K^*(892) and K_2^*(1430) signals, and the efficiency-corrected spectrum is well described by a superposition of the associated Breit-Wigner intensity distributions, together with an S-wave contribution obtained from the LASS I=1/2 K π^- scattering amplitude measurements. Each K π^- angular dist…

PhysicsNuclear and High Energy PhysicsParticle physicsMass distribution010308 nuclear & particles physicsElectron–positron annihilation01 natural scienceslaw.inventionLuminosityNuclear physicsScattering amplitudeReflection (mathematics)law0103 physical sciencesZ(4430)010306 general physicsColliderLegendre polynomialsPhysical Review D
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