Search results for "SPECTRA"

showing 10 items of 3542 documents

Magnetostochastic resonance under colored noise condition

2012

Stochastic resonance (SR) is an amplification of the system output in correspondence of well-defined finite values of the noise strength that is injected into the system [Gammaitoni et al., Rev. Mod. Phys. 70, 223 (1998), Grigorenko et al., IEEE Trans. Magn. 31, 2491 (1995), Mantegna et al., J. Appl. Phys. 97, 10E519 (2005)]. In order to clarify the influence of a colored noise, in this paper magnetostochastic resonance (MSR) in magnetic systems described by the dynamic Preisach model is numerically investigated in the presence of colored noise. In this paper it is shown that: a) noise spectrum affects MSR; b) white noise, 1/f and 1/f(2) noise induce in magnetic systems described by the dyn…

PhysicsStochastic resonanceSTOCHASTIC RESONANCEPREISACH MODELNoise spectral densityGeneral Physics and AstronomyResonanceWhite noiseSettore ING-IND/32 - Convertitori Macchine E Azionamenti ElettriciMagnetic hysteresisNuclear magnetic resonanceColors of noiseQuantum mechanicsHYSTERESISNoise (radio)Noise strengthJournal of Applied Physics
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The ALICE Collaboration

2009

The production of mesons containing strange quarks (KS, φ) and both singly and doubly strange baryons ( , , and − + +) are measured at mid-rapidity in pp collisions at √ s = 0.9 TeV with the ALICE experiment at the LHC. The results are obtained from the analysis of about 250 k minimum bias events recorded in 2009. Measurements of yields (dN/dy) and transverse momentum spectra at mid-rapidity for inelastic pp collisions are presented. For mesons, we report yields (〈dN/dy〉) of 0.184 ± 0.002(stat.) ± 0.006(syst.) for KS and 0.021 ± 0.004(stat.) ± 0.003(syst.) for φ. For baryons, we find 〈dN/dy〉 = 0.048 ± 0.001(stat.) ± 0.004(syst.) for , 0.047 ± 0.002(stat.) ± 0.005(syst.) for and 0.0101 ± 0.0…

PhysicsStrange quarkNuclear and High Energy PhysicsLarge Hadron ColliderMeson010308 nuclear & particles physics7. Clean energy01 natural sciencesSpectral lineVisual artsNuclear physicsBaryonMinimum biasTransverse momentum0103 physical sciencesHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsALICE (propellant)Nuclear Experiment010306 general physics
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Orbital-selective Mott transitions in the anisotropic two-band Hubbard model at finite temperatures

2005

The anisotropic degenerate two-orbital Hubbard model is studied within dynamical mean-field theory at low temperatures. High-precision calculations on the basis of a refined quantum Monte Carlo (QMC) method reveal that two distinct orbital-selective Mott transitions occur for a bandwidth ratio of 2 even in the absence of spin-flip contributions to the Hund exchange. The second transition -- not seen in earlier studies using QMC, iterative perturbation theory, and exact diagonalization -- is clearly exposed in a low-frequency analysis of the self-energy and in local spectra.

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsQuantum Monte CarloDegenerate energy levelsFOS: Physical sciencesCondensed Matter PhysicsSpectral lineElectronic Optical and Magnetic MaterialsMott transitionCondensed Matter - Strongly Correlated ElectronsMean field theoryQuantum mechanicsStrongly correlated materialCondensed Matter::Strongly Correlated ElectronsAnisotropy
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Learning from observations of the microwave background at small angular scales

1996

In this paper, we focus our attention on the following question: How well can we recover the power spectrum of the cosmic microwave background from the maps of a given experiment?. Each experiment is described by a a pixelization scale, a beam size, a noise level and a sky coverage. We use accurate numerical simulations of the microwave sky and a cold dark matter model for structure formation in the universe. Angular scales smaller than those of previous simulations are included. The spectrum obtained from the simulated maps is appropriately compared with the theoretical one. Relative deviations between these spectra are estimated. Various contributions to these deviations are analyzed. The…

PhysicsStructure formationCold dark mattermedia_common.quotation_subjectAstrophysics (astro-ph)Cosmic microwave backgroundFOS: Physical sciencesSpectral densityAstronomy and AstrophysicsScale (descriptive set theory)AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsSpace and Planetary ScienceSkyPixelizationMicrowavemedia_common
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Sum Frequency Generation Spectra from Velocity–Velocity Correlation Functions

2017

We developed an expression for the calculation of the sum frequency generation spectra (SFG) of water interfaces that is based on the projection of the atomic velocities on the local normal modes. Our approach permits one to obtain the SFG signal from suitable velocity-velocity correlation functions, reducing the computational cost to that of the accumulation of a molecular dynamics trajectory, and therefore cutting the overhead costs associated with the explicit calculation of the dipole moment and polarizability tensor. Our method permits to interpret the peaks in the spectrum in terms of local modes, also including the bending region. The results for the water-air interface, obtained usi…

PhysicsSum-frequency generation010304 chemical physicsAnalytical chemistryPhase (waves)010402 general chemistry01 natural sciencesProjection (linear algebra)Spectral line0104 chemical sciencesComputational physicsMoment (mathematics)Molecular dynamicsDipoleNormal mode0103 physical sciencesGeneral Materials SciencePhysical and Theoretical ChemistryThe Journal of Physical Chemistry Letters
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Penumbral oscillations in Na D lines

1990

Penumbral oscillations were measured in two opposite parts in the penumbra of a spot, using photographic spectra of Na D lines. Power spectra of velocities show the presence of the 5-min oscillation with lowv rms. Coherence and phase analyses between the velocity fluctuations of the lines are also studied. The results seem to show that the 5-min oscillation is still surviving as a standing or evanescent wave at the height of formation of Na D lines.

PhysicsSunspotEvanescent waveOscillationPenumbraPhase (waves)Astronomy and AstrophysicsAstrophysicsSolar physicsSpectral lineSpace and Planetary ScienceAstrophysics::Solar and Stellar AstrophysicsCoherence (signal processing)Atomic physicsAstrophysics and Space Science
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Frequency-dependent relaxation rate in superconductingYBa2Cu3O6+δ

2000

The submillimeter-wave $3 {\mathrm{cm}}^{\ensuremath{-}1}l\ensuremath{\nu}l40 {\mathrm{cm}}^{\ensuremath{-}1}$ complex conductivity of the reduced ${\mathrm{YBa}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{6+\ensuremath{\delta}}$ film ${(T}_{C}=56.5 \mathrm{K})$ was investigated for temperatures $4 \mathrm{K}lTl300 \mathrm{K}$ and compared to the properties of the same film in the optimally doped state. The frequency dependence of the effective quasiparticle scattering rate $1/{\ensuremath{\tau}}^{*}(\ensuremath{\nu})$ was extracted from the spectra. $1/{\ensuremath{\tau}}^{*}$ is shown to be frequency independent at low frequencies and high temperatures. A gradual change to $1/{\ensuremath{\tau}}^{…

PhysicsSuperconductivityCrystallographySpectral weightCondensed matter physicsRelaxation rateScattering rateQuasiparticleOrder (ring theory)Spectral lineEffective mass (spring–mass system)Physical Review B
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Fluctuation-Limited Noise in a Superconducting Transition-Edge Sensor

2003

In order to investigate the origin of the until now unaccounted excess noise and to minimize the uncontrollable phenomena at the transition in x-ray microcalorimeters we have developed superconducting transition-edge sensors into an edgeless geometry, the so-called Corbino disk, with superconducting contacts in the center and at the outer perimeter. The measured rms current noise and its spectral density can be modeled as resistance noise resulting from fluctuations near the equilibrium superconductor-normal metal boundary. Peer reviewed

PhysicsSuperconductivitynoiseCorbino disksCondensed matter physicsPhysicsGeneral Physics and AstronomyBoundary (topology)Spectral densityNoise (electronics)Current noiseNuclear magnetic resonancesuperconducting transition-edge sensorCondensed Matter::Superconductivitysuperconducting transition-edge sensorTransition edge sensorsuperconducting transition-edge sensors
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Measuring Supermassive Black Hole Masses: Correlation between the Redshifts of the Fe III UV Lines and the Widths of Broad Emission Lines

2019

We test the recently proposed (Mediavilla et al. 2018) black hole mass scaling relationship based on the redshift {with respect to the quasar's rest frame} of the Fe III$\lambda\lambda$2039-2113 line blend. To this end, we fit this feature in the spectra of a well suited sample of quasars, observed with X-shooter at the Very Large Telescope (VLT), whose masses have been independently estimated using the virial theorem. For the quasars of this sample we consistently confirm the redshift of the Fe III$\lambda\lambda$2039-2113 blend and find that it correlates with the squared widths of H$\beta$, H$\alpha$ and Mg II, which are commonly used as a measure of $M_{BH}/R$ to determine masses from t…

PhysicsSupermassive black holeCosmology and Nongalactic Astrophysics (astro-ph.CO)010504 meteorology & atmospheric sciencesFOS: Physical sciencesAstronomy and AstrophysicsQuasarAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesAstrophysics - Astrophysics of GalaxiesSpectral lineVirial theoremRedshiftBaryonBlack holeSpace and Planetary ScienceAstrophysics of Galaxies (astro-ph.GA)0103 physical sciencesEmission spectrum010303 astronomy & astrophysicsAstrophysics::Galaxy Astrophysics0105 earth and related environmental sciencesAstrophysics - Cosmology and Nongalactic Astrophysics
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Multi-Wavelength VLA Observations of the Young Supernova SN 1993J

2003

We present continuum VLA measurements of SN1993J in M81 taken on 17 and 21 December 2000, about 2820 days after the supernova explosion, spanning the frequency range from 0.32 to 14.9 GHz. These observations aimed at discerning the main absorbing processes acting in SN1993J at late epochs. We discuss three models for the late radio emission of SN1993J: (i) a simple power-law spectrum, (ii) a power-law spectrum free-free absorbed by a screen of homogeneously distributed ionized gas, and (iii) a power-law spectrum free-free absorbed by a “clumpy” medium. We find that the best fit to the data is yielded by a power-law spectrum free-free absorbed by either a homogeneous, or a clumpy, distributi…

PhysicsSupernovaSpectral indexlawIonizationRadiative transferAstronomyPlasmaAstrophysicsElectronSynchrotronRadio spectrumlaw.invention
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