Search results for "SPECTRA"

showing 10 items of 3542 documents

X-ray spectral and timing characteristics of the stars in the young open cluster IC 2391

2005

We present X-ray spectral and timing analysis of members of the young open cluster IC 2391 observed with the XMM-Newton observatory. We detected 99 X-ray sources by analysing the summed data obtained from MOS1, MOS2 and pn detectors of the EPIC camera; 24 of them are members, or probable members, of the cluster. Stars of all spectral types have been detected, from the early-types to the late-M dwarfs. Despite the capability of the instrument to recognize up to 3 thermal components, the X-ray spectra of the G, K and M members of the cluster are well described with two thermal components (at kT$_1 \sim$ 0.3-0.5 keV and kT$_2 \sim$ 1.0-1.2 keV respectively) while the X-ray spectra of F members…

Physicsopen clusters and associations : individual : IC 2391 OPEN CLUSTERSAstrophysics (astro-ph)X-rayFOS: Physical sciencesstars : late-typeAstronomy and AstrophysicsAstrophysicsX-ray : starAstrophysicsStellar classificationSpectral linePLEIADESstars : activityVARIABILITYStarsSettore FIS/05 - Astronomia E AstrofisicaSpace and Planetary ScienceObservatoryROSATstars; stars : activity; stars : early-type; stars : late-type; open clusters and associations : individual : IC 2391 OPEN CLUSTERS; EMISSION; PLEIADES; VARIABILITY [X-ray]Cluster (physics)stars : early-typeEMISSIONOpen clusterAstronomy & Astrophysics
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Shape from polarization: a method for solving zenithal angle ambiguity

2012

International audience; We report a multispectral based method that permits the evolution of shape from polarization setup applied to 3D shape estimation of transparent objects. The setup is based on a polarization imaging technique which is a recent imaging method based on the analysis of the polarization state of the light in the observed scene. The technique has rapidly evolved with the development of electro-optic components and some polarization cameras are now available on the market. Shape from polarization consists in measuring the azimuthal and zenithal angles characterizing the normal of each point of the observed surface. We focus on the ambiguity in the measurement of the zenith…

Physicspolarization imaging[SPI.OPTI] Engineering Sciences [physics]/Optics / Photonicbusiness.industrymedia_common.quotation_subject010401 analytical chemistryMultispectral imagePolarization imagingAmbiguityPolarization (waves)01 natural sciencesAtomic and Molecular Physics and Optics3D shape0104 chemical sciences010309 opticsAzimuthOpticsComputer Science::Computer Vision and Pattern Recognition0103 physical sciences[SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic[ SPI.OPTI ] Engineering Sciences [physics]/Optics / PhotonicbusinessRefractive indexmedia_common
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Corrigendum: Spectral Entropy Based Neuronal Network Synchronization Analysis Based on Microelectrode Array Measurements

2020

Physicsrat cortical cellsSpectral entropyspectral entropyNeuroscience (miscellaneous)developing neuronal networksMultielectrode arraylcsh:RC321-571Cellular and Molecular NeurosciencecorrelationSynchronization (computer science)Biological neural networkmouse cortical cellsBiological systemsynchronizationlcsh:Neurosciences. Biological psychiatry. NeuropsychiatryFrontiers in Computational Neuroscience
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Chandra observation of the Big Dipper X 1624–490

2006

We present the results of a 73 ks long Chandra observation of the dipping source X 1624-490. During the observation a complex dip lasting 4 hours is observed. We analyse the persistent emission detecting, for the first time in the 1st-order spectra of X 1624-490, an absorption line associated to \ion{Ca}{xx}. We confirm the presence of the \ion{Fe}{xxv} K$_\alpha$ and \ion{Fe}{xxvi} K$_\alpha$ absorption lines with a larger accuracy with respect to a previous XMM observation. Assuming that the line widths are due to a bulk motion or a turbulence associated to the coronal activity, we estimate that the lines have been produced in a photoionized absorber between the coronal radius and the out…

Physicsstars : individual : X 1624-490Absorption spectroscopyAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)FOS: Physical sciencesAstronomy and AstrophysicsRadiusAstrophysicsAstrophysicsaccretion accretion diskstars : neutronBulk motionSpectral lineIonAccretion discSpace and Planetary ScienceX-rays : starX-rays : binarieindividual : X 1624-490; stars : neutron; X-rays : stars; X-rays : binaries; X-rays : general [accretion accretion disks; stars]X-rays : generalLine (formation)Astronomy & Astrophysics
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Relativistically Smeared Iron Lines in the Spectra of Bright NS LMXB

2009

We present preliminary results of a study on three bright accreting low-mass X-ray binaries hosting a neutron star, based on XMM-Newton observations. These sources (GX 340+0, GX 349+2 and SAX J1808.4-3658) show a broad Fe K alpha iron line in their spectra. This feature can be well described by relativistic line profile in each case; the good spectral resolution of the EPIC/PN and the high statistics spectra allow to put very good constraints on the disk geometry and ionization stage of the reflecting matter.

Physicsstars: neutron starAstrophysics::High Energy Astrophysical Phenomenastars: individual: GX 340+0 GX 349+2 SAX J1808.4-3658X-ray: starAstronomyAstrophysicsEPICX-ray: spectrumSpectral lineNeutron starSettore FIS/05 - Astronomia E Astrofisicaindividual: GX 340+0 GX 349+2 SAX J1808.4-3658; stars: neutron stars; X-ray: stars; X-ray: spectrum; [accretion disks; stars]PulsarIonizationSpectral resolutionSpectroscopyaccretion diskLine (formation)
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The bound state in the spectrum of the Lee–Friedrichs Hamiltonian

2000

Abstract The spectrum of the Lee–Friedrichs Hamiltonian, describing a two-level system embedded in a continuum, is considered. An appropriate discretization of the field modes is performed before taking the continuum limit. It is shown that the existence of an eigenstate with negative energy (bound state) is related to the nonanalyticity of the Friedrichs spectral representation. This negative energy state is a dressed state and its physical properties are studied in some significant cases.

Physicssymbols.namesakeSpectral representationDiscretizationQuantum mechanicsBound statesymbolsGeneral Physics and AstronomyNegative energyHamiltonian (quantum mechanics)Eigenvalues and eigenvectorsPhysics Letters A
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Measurements and calculations of Stark broadening parameters for the N I multiplet (1D)3s2D–(1D)3p2Do

2014

Calculations of line broadening parameters of a doubly excited N I transition, based on atomic structure data (taken from the literature), are reported. The obtained results were used for a critical analysis of formerly published experimental data, based on spectra measured in our laboratory. These measured spectra were then again analyzed and new broadening parameters were determined and compared with results of calculations.

Physicssymbols.namesakeStark effectExcited statesymbolsAtomic physicsCondensed Matter PhysicsMultipletMathematical PhysicsAtomic and Molecular Physics and OpticsSpectral lineLine (formation)Physica Scripta
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Stark broadening of hydrogen spectral lines with fine structure effects

2004

Formalism and numerical code have been elaborated for calculation of hydrogen line profiles in conditions of plasma in which Stark broadening and fine energy splitting are comparable and it is not possible to neglect either of them. It corresponds to the range of electron densities $10^{11} < N_e ({\rm cm}^{-3}) < 10^{15}$ . Lamb shift and spontaneous emission effects have also been included. Computer simulation method was applied in the calculations. Final results have been compared with experimental and theoretical findings by other authors.

Physicssymbols.namesakeStark effectOptical physicssymbolsHydrogen lineSpontaneous emissionElectronAtomic physicsHydrogen spectral seriesHyperfine structureAtomic and Molecular Physics and OpticsLamb shiftThe European Physical Journal D - Atomic, Molecular and Optical Physics
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Energy gap of intermediate-valentSmB6studied by point-contact spectroscopy

2001

We have investigated the intermediate valence narrow-gap semiconductor ${\mathrm{SmB}}_{6}$ at low temperatures using both conventional spear-anvil type point contacts as well as mechanically controllable break junctions. The zero-bias conductance varied between less than $0.01 \ensuremath{\mu}\mathrm{S}$ and up to 1 mS. The position of the spectral anomalies, which are related to the different activation energies and band gaps of ${\mathrm{SmB}}_{6},$ did not depend on the the contact size. Two different regimes of charge transport could be distinguished: Contacts with large zero-bias conductance are in the diffusive Maxwell regime. They had spectra with only small nonlinearities. Contacts…

Physicssymbols.namesakeValence (chemistry)Condensed matter physicsBand gapFermi levelsymbolsDensity of statesQuasiparticleConductanceAtomic physicsSpectroscopySpectral linePhysical Review B
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Fourier-transform spectroscopy and coupled-channels deperturbation treatment of theA 1Σ+–b 3Πcomplex of KCs

2010

The laser-induced fluorescence (LIF) A {sup 1{Sigma}+}-b {sup 3{Pi}{yields}}X {sup 1{Sigma}+} spectra of the KCs molecule were recorded in a near infrared region by a Fourier-transform spectrometer with a resolution of 0.03 cm{sup -1}. Overall more than 200 collisionally enhanced LIF spectra were rotationally assigned to {sup 39}K{sup 133}Cs and {sup 41}K{sup 133}Cs isotopomers yielding more than 3400 rovibronic term values of the strongly mixed singlet A {sup 1{Sigma}+} and triplet b {sup 3{Pi}} states with the uncertainty of 0.003-0.01 cm{sup -1}. Experimental data massive starts from the lowest vibrational level v{sub A}=0 of the singlet and nonuniformly covers the energy range E is an e…

Physicssymbols.namesakesymbolsSinglet stateAtomic physicsSpectroscopyGround stateQuantum numberHamiltonian (quantum mechanics)Potential energyOmegaAtomic and Molecular Physics and OpticsSpectral linePhysical Review A
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