Search results for "methods [Gene Expression Profiling]"

showing 10 items of 838 documents

Calibration of the XRT-SOLARB flight filters at the XACT facility of INAF-OAPA

2004

The X-Ray Telescope (XRT) experiment on-board the Japanese satellite SOLAR-B (launch in 2006) aimed at providing full Sun field of view at ~ 1.5" angular resolution, will be equipped with two wheels of focal-plane filters to select spectral features of X-ray emission from the Solar corona, and a front-end filter to significantly reduce the visible light contamination. We present the results of the X-ray calibrations of the XRT flight filters performed at the X-ray Astronomy Calibration and Testing (XACT) facility of INAF-OAPA. We describe the instrumental set-up, the adopted measurement technique, and present the transmission vs. energy and position measurements.

PhysicsX-ray astronomybusiness.industryAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Instrumentation and Methods for AstrophysicsField of viewFilter (signal processing)law.inventionTelescopeOpticslawCalibrationAstrophysics::Solar and Stellar AstrophysicsAngular resolutionSatellitebusinessImage resolutionX-ray Astronomy Instrumentation Filters CalibrationRemote sensing
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Thin plastic shell x-ray optics: an update

2003

We present new results from a program to develop large area X-ray telescopes that are made from thin plastic shells. We use multi-shell cylindrical lenses in a point-to-point configuration to form full aperture images of the small focal spot in a an X-ray tube on a microchannel plate detector. The image data are analyzed to yield radial profiles and encircled energy curves. The derived parameters can be extrapolated to the case of a telescope that is a conical approximation to Wolter 1 optics. The plastic shells can be coated with suitable mono- or multilayers that allow for a wideband coverage of X-ray energies. Our current program is focused on the development of a large area, hard X-ray …

Physicsbusiness.industryApertureAstrophysics::High Energy Astrophysical PhenomenaPlastic shell X-ray opticAstrophysics::Instrumentation and Methods for AstrophysicsShell (structure)X-ray opticsX-ray telescopeConical surfaceCondensed Matter PhysicsEncircled energylaw.inventionTelescopePoint-to-point X-ray imagingOpticsApproximate X-ray opticlawMicrochannel plate detectorElectrical and Electronic EngineeringX-ray opticbusiness
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Simbol-X Mirror Module Thermal Shields: I-Design and X-Ray Transmission

2009

The Simbol‐X mission is designed to fly in formation flight configuration. As a consequence, the telescope has both ends open to space, and thermal shielding at telescope entrance and exit is required to maintain temperature uniformity throughout the mirrors. Both mesh and meshless solutions are presently under study for the shields. We discuss the design and the X‐ray transmission.

Physicsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Instrumentation and Methods for AstrophysicsShieldsX- and gamma-ray telescopes and instrumentation Astronomical and space-research instrumentation Optical coatingsParticle detectorlaw.inventionTelescopeOpticsOptical coatingSettore FIS/05 - Astronomia E AstrofisicaTransmission (telecommunications)lawElectromagnetic shieldingThermalMeasuring instrumentbusiness
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Design and implementation of electronics and data acquisition system for Ultra-Fast Flash Observatory

2013

The Ultra-Fast Flash Observatory (UFFO) Pathfinder for Gamma-Ray Bursts (GRBs) consists of two telescopes. The UFFO Burst Alert & Trigger Telescope (UBAT) handles the detection and localization of GRBs, and the Slewing Mirror Telescope (SMT) conducts the measurement of the UV/optical afterglow. UBAT is equipped with an X-ray detector, analog and digital signal readout electronics that detects X-rays from GRBs and determines the location. SMT is equipped with a stepping motor and the associated electronics to rotate the slewing mirror targeting the GRBs identified by UBAT. First the slewing mirror points to a GRB, then SMT obtains the optical image of the GRB using the intensified CCD an…

Physicsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaDetectorAstrophysics::Instrumentation and Methods for AstrophysicsGeneral EngineeringAstronomy and AstrophysicsAstrophysicslaw.inventionTelescopeFlash (photography)Data acquisitionSpace and Planetary ScienceObservatorylawDigital signalElectronicsbusinessGamma-ray burstComputer hardwareEAS Publications Series
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Analytical formula for calculating the focal shift in apodized systems

1998

We report a quite simple analytical formula for the evaluation of the focal shift in apodized systems, with or without rotational invariance. Specifically it is shown that the magnitude of the focal shift is determined by the product of the Fresnel number of the focusing geometry and the standard deviation of a mapped version of the azimuthal average of the pupil transmittance. To illustrate our approach, several examples are examined.

Physicsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsMagnitude (mathematics)Standard deviationAtomic and Molecular Physics and OpticsAzimuthOpticsApodizationProduct (mathematics)TransmittanceFresnel numberRotational invariancebusinessJournal of Modern Optics
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Sodium vapor cell laser guide star experiments for continuous wave model validation

2016

Recent numerical simulations and experiments on sodium Laser Guide Star (LGS) have shown that a continuous wave (CW) laser with circular polarization and re-pumping should maximize the fluorescent photon return flux to the wavefront sensor for adaptive optics applications. The orientation and strength of the geomagnetic field in the sodium layer also play an important role affecting the LGS return ux. Field measurements of the LGS return flux show agreement with the CW LGS model, however, fluctuations in the sodium column abundance and geomagnetic field intensity, as well as atmospheric turbulence, induce experimental uncertainties. We describe a laboratory experiment to measure the photon …

Physicsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsSodium layerLaserPolarization (waves)01 natural scienceslaw.invention010309 opticsLaser linewidthOpticsLaser guide starlaw0103 physical sciencesContinuous wavebusinessAdaptive optics010303 astronomy & astrophysicsCircular polarizationAdaptive Optics Systems V
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Chromatic compensation in the near-field region: shape and size tunability

2005

We report a diffractive-lens triplet with which to achieve wavelength compensation in the near field diffracted by any aperture. On the one hand, the all-diffractive triplet allows us to tune, in a sequential way, the Fresnel-irradiance shape to be achromatized by changing the focal length of one diffractive lens. On the other hand, we can adjust the scale of the chromatically compensated Fresnel diffraction field by shifting the aperture along the optical axis. Within this framework, we present an extremely flexible white-light Fresnel-plane array illuminator based on the kinoform sampling filter. A variable compression ratio and continuous selection of the output pitch are the most appeal…

Physicsbusiness.industryKinoformApertureMaterials Science (miscellaneous)Astrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsNear and far fieldDiffraction efficiencyIndustrial and Manufacturing EngineeringOptical axisOpticsFocal lengthChromatic scaleBusiness and International ManagementbusinessFresnel diffractionApplied Optics
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Passive Polarimetric Imaging

2014

Passive electro-optical polarimetric imaging is a form of remote sensing in which the properties associated with electromagnetic field orientation are exploited as a means to discriminate between objects in an extended scene. The purpose of this chapter is to introduce some fundamental concepts in the science of imaging polarimetry. These concepts include the Stokes-Mueller description of polarized light, the physical mechanisms that contribute to polarimetric image contrast, a mathematical description of several polarimetric imaging systems, and an example target detection algorithm. Polarimetric image contrast is discussed in terms of reflected, emitted, and scattered light. Special empha…

Physicsbusiness.industryOrientation (computer vision)Astrophysics::Instrumentation and Methods for AstrophysicsPolarimetryPolarimeterFresnel equationssymbols.namesakeOpticsComputer Science::Computer Vision and Pattern RecognitionsymbolsAstrophysics::Solar and Stellar AstrophysicsDegree of polarizationStokes parametersRadiometryBidirectional reflectance distribution functionbusinessRemote sensing
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Nonlinear Current Generation in Degenerate Semiconductors Embedded in Constant and Low-Frequency Electric Fields

2006

The explicit analytical forms of nonlinear currents in degenerate semiconductors serving as sources of coherent radiation in the wavelength millimetric and submillimetric ranges are established.

Physicsbusiness.industryPhysics::Medical PhysicsDegenerate energy levelsAstrophysics::Instrumentation and Methods for AstrophysicsGeneral Physics and AstronomyAstrophysics::Cosmology and Extragalactic AstrophysicsRadiationLow frequencyComputational physicsNonlinear systemWavelengthSemiconductorElectric fieldOptoelectronicsbusinessConstant (mathematics)Astrophysics::Galaxy Astrophysics
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Apodization of imaging systems by means of a random spatially nonstationary absorbing screen

1992

The amplitude impulse response (AIR) of coherent imaging systems with random binary apodizers is analyzed. Formulas for the mean value and the variance of the AIR are derived for two statistical one-dimensional models of apodizers: (1) nonuniform low-density shot noise and (2) a nonuniform unipolar synchronous random process. We show that for both models a high signal-to-noise ratio is achieved within the central peak and the low-order sidelobes of the AIR. Apodizers based on the second model permit higher values of the signal-to-noise ratio than those based on the first one.

Physicsbusiness.industryStochastic processAstrophysics::Instrumentation and Methods for AstrophysicsShot noiseImpulse (physics)Atomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialssymbols.namesakeAmplitudeOpticsFourier transformApodizationsymbolsComputer Vision and Pattern RecognitionSpatial frequencybusinessImpulse responseJournal of the Optical Society of America A
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