Search results for "Length"

showing 10 items of 2188 documents

Spiral conical approximations to double reflection Wolter optics

2008

The design of a grazing incidence focusing optic obtained from a spiral approximation to multiple nested cones produces an annular image of a point source. The angular size of the annulus depends mainly on the pitch of the winding and the focal length. For a spiral conical approximation to Wolter optics, the effect is magnified by the double reflection. However, if the two conical spirals are wound one clock-wise and the other counter-clock-wise, then the aberration is partially compensated. We use a ray tracing code to evaluate advantages and disadvantages of this optical design for potential applications of a light weight optics technology based on plastic foils that we are currently inve…

PhysicsX-Ray telescopes plastic foil ray-tracingbusiness.industryPoint sourceParaxial approximationPhysics::OpticsConical surfaceOpticsSettore FIS/05 - Astronomia E AstrofisicaAnnulus (firestop)Reflection (physics)Focal lengthRay tracing (graphics)businessSpiral
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Compton scattering off nucleons near threshold

2008

The energy dependence of the magnetic polarizability β has been evaluated by use of the delta resonance in the s- and u-channel of the Compton scattering amplitude. It was the idea to extract the influence of higher order terms (higher than ω2, ω = |k| being the photon energy) in the analysis of the polarizability. The static paramagnetic polarizability βPara(0) has been substituted by an energy dependent βδPara(k) and the result is compared with experimental data.

PhysicsX-ray Raman scatteringPolarizabilityPhysics::Atomic and Molecular ClustersCompton scatteringCompton wavelengthPhoton energyInelastic scatteringAtomic physicsNucleonResonance (particle physics)
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Thermal shielding of the SIMBOL-X mirror assembly

2007

The thermal modeling of the SIMBOL-X X-ray telescope has shown that thermal shielding of both the telescope ends is one possibility to ensure temperature uniformity of the mirror and to reduce the required heating power. The design of the thermal shielding must minimize the thermal exchange in a trade off between transparency of the shields to soft X-rays and mechanical robustness. We discuss two possible designs of the thermal shielding of the mirror module and show transmission curves at X-ray wavelengths.

PhysicsX-ray astronomybusiness.industryAstrophysics::High Energy Astrophysical PhenomenaShieldsX-ray telescopelaw.inventionTelescopeWavelengthOpticsTransmission (telecommunications)lawElectromagnetic shieldingThermalX-ray Astronomy Simbol-X X-ray filters Thermal shieldsbusinessSPIE Proceedings
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Calibration of the XRT-SOLARB flat mirror samples at the XACT Facility of INAF-OAPA

2004

The X-Ray Telescope (XRT) experiment on-board the Japanese satellite SOLAR-B (launch in 2006) is equipped with a modified Wolter I grazing incidence X-ray telescope (focal length 2700 mm) to image the full Sun at ~ 1.5" angular resolution onto a 2048 x 2048 back illuminated CCD focal plane detector. The X-ray telescope consisting of one single reflecting shell is coated with ion beam sputtered Iridium over a binding layer of Chromium to provide nearly 5 square centimetres effective area at 60 A. We present preliminary results of X-ray calibrations of the XRT flat mirror samples performed at the X-ray Astronomy Calibration and Testing (XACT) facility of INAF-OAPA. We describe the instrumenta…

PhysicsX-ray astronomybusiness.industryX-ray telescopelaw.inventionTelescopeOpticslawAngle of incidence (optics)CalibrationFocal lengthAngular resolutionX-ray Astronomy Instrumentation Grazing incidence optics CalibrationbusinessImage resolution
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Atomic transitions of Rb, D2 line in strong magnetic fields: Hyperfine Paschen–Back regime

2014

An efficient $\lambda/2$-method ($\lambda$ is the resonant wavelength of laser radiation) based on nanometric-thickness cell filled with rubidium is implemented to study the splitting of hyperfine transitions of $^{85}$Rb and $^{87}$Rb $D_2$ lines in an external magnetic field in the range of $B =3$~kG -- 7~kG. It is experimentally demonstrated that at $B > 3$~kG from 38 (22) Zeeman transitions allowed at low $B$-field in $^{85}$Rb ($^{87}$Rb) spectra in the case of $\sigma^+$ polarized laser radiation there remain only 12 (8) which is caused by decoupling of the total electronic momentum $\textbf{J}$ and the nuclear spin momentum $\textbf{I}$ (hyperfine Paschen-Back regime). Note that at $…

PhysicsZeeman effectAtomic Physics (physics.atom-ph)FOS: Physical scienceschemistry.chemical_elementAtomic and Molecular Physics and OpticsSpectral linePhysics - Atomic Physics3. Good healthElectronic Optical and Magnetic MaterialsRubidiumMagnetic fieldMomentumsymbols.namesakeWavelengthchemistrysymbolsPhysics::Atomic PhysicsElectrical and Electronic EngineeringPhysical and Theoretical ChemistryAtomic physicsHyperfine structureLine (formation)Optics Communications
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Hyperfine Paschen-Back regime in alkali metal atoms: consistency of two theoretical considerations and experiment

2013

Simple and efficient "\lambda-method" and "\lambda/2-method" (\lambda is the resonant wavelength of laser radiation) based on nanometric-thickness cell filled with rubidium are implemented to study the splitting of hyperfine transitions of 85Rb and 87Rb D_1 line in an external magnetic field in the range of B = 0.5 - 0.7 T. It is experimentally demonstrated from 20 (12) Zeeman transitions allowed at low B-field in 85Rb (87Rb) spectra in the case of \sigma+ polarized laser radiation, only 6 (4) remain at B > 0.5 T, caused by decoupling of the total electronic momentum J and the nuclear spin momentum I (hyperfine Paschen-Back regime). The expressions derived in the frame of completely uncoupl…

PhysicsZeeman effectAtomic Physics (physics.atom-ph)chemistry.chemical_elementFOS: Physical sciencesStatistical and Nonlinear Physics01 natural sciencesAtomic and Molecular Physics and OpticsSpectral line3. Good healthRubidiumMagnetic fieldPhysics - Atomic Physics010309 opticsMomentumWavelengthsymbols.namesakechemistry0103 physical sciencessymbolsPhysics::Atomic PhysicsAtomic physics010306 general physicsHyperfine structureCircular polarization
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Short-length storage of intense optical pulses in solid by adiabatic passage

2009

We propose a novel scheme of storage of intense pulses which allows a significant reduction of the storage length with respect to standard schemes. This scheme is particularly adapted to store optical information in media with fast relaxations.

Physics[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Atomic Physics (physics.atom-ph)FOS: Physical sciencesShort length01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasPhysics - Atomic PhysicsReduction (complexity)[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]0103 physical sciencesoptical storageAtomic physics010306 general physicsAdiabatic processoptical information processing
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Kerr frequency comb generation in the normal dispersion regime of dispersion oscillating telecom fiber

2013

The generation of optical frequency combs has a variety of applications from optical metrology to spectroscopy and wavelength division multiplexing. Nonlinear methods to generate frequency combs are based on multiple four-wave mixing (FWM) in highly nonlinear waveguides [1]. The mechanism for the generation of a wideband comb from a CW pump is Kerr-induced phase-matching of the FWM interaction or modulation instability (MI), which requires operating in the anomalous dispersion regime. Such restriction can be circumvented with a cavity geometry, where MI [2] and comb generation [3] may also be observed in the normal dispersion region. Alternatively, one may obtain MI and unequally spaced Ker…

Physics[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics][PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Kerr effect[ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryPhysics::OpticsNonlinear optics01 natural sciencesSupercontinuum010309 opticsOptical pumpingFrequency combOpticsWavelength-division multiplexing0103 physical sciencesDispersion (optics)Optoelectronics010306 general physicsTelecommunicationsbusinessComputingMilieux_MISCELLANEOUSPhotonic-crystal fiber
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Experimental investigation of a polarization attractor at telecommunication wavelengths

2008

We report the experimental observation of a polarization attraction process taking place in an optical fiber around 1550 nm and based on a nonlinear interaction between two counter-propagating waves.

Physics[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics][PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Optical fiber[ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]Wave propagationbusiness.industry02 engineering and technology021001 nanoscience & nanotechnologyPolarization (waves)01 natural scienceslaw.invention010309 opticsWavelengthNonlinear systemOpticslawEvolution biology0103 physical sciencesAttractor0210 nano-technologybusinessComputingMilieux_MISCELLANEOUS
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Tailored soliton statistics in supercontinuum generation

2009

Supercontinuum (SC) generation in highly nonlinear photonic crystal fibers (PCF) has stimulated tremendous interest in recent years [1]. Particular results that have received recent widespread attention concern the observation of “optical rogue waves,” statistically rare extreme red-shifted Raman solitons appearing on the long wavelength edge of the SC spectrum [2]. Further numerical analysis of these fluctuations have showed explicitly that the rogue soliton statistics exhibit strongly non-Gaussian extreme-value characteristics [3]. The previous studies of optical rogue wave statistics in SC generation have been carried out considering PCF with only one zero dispersion wavelength (ZDW). It…

Physics[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics][PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryPhysics::OpticsOptical rogue waves02 engineering and technology01 natural sciencesSupercontinuum010309 optics020210 optoelectronics & photonicsZero-dispersion wavelengthOptics0103 physical sciencesStatisticsDispersion (optics)0202 electrical engineering electronic engineering information engineeringNonlinear photonic crystalSolitonRogue wavebusinessNonlinear Sciences::Pattern Formation and SolitonsComputingMilieux_MISCELLANEOUSPhotonic-crystal fiber
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