Search results for "width [Lambda(1405)]"

showing 10 items of 330 documents

Non-Markovian dynamics and steady-state entanglement of cavity arrays in finite-bandwidth squeezed reservoirs

2014

When two chains of quantum systems are driven at their ends by a two-mode squeezed reservoir, they approach a steady state characterized by the formation of many entangled pairs. Each pair is made of one element of the first and one of the second chain. This effect has been already predicted under the assumption of broadband squeezing. Here we investigate the situation of finite-bandwidth reservoirs. This is done by modeling the driving bath as the output field of a non-degenerate parametric oscillator. The resulting non-Markovian dynamics is studied within the theoretical framework of cascade open quantum systems. It is shown that the formation of pair-entangled structures occurs as long a…

PhysicsQuantum PhysicsTheoryofComputation_COMPUTATIONBYABSTRACTDEVICESQuantum decoherenceStatistical Mechanics (cond-mat.stat-mech)Bandwidth (signal processing)Markov processFOS: Physical sciencesQuantum entanglementQuantum PhysicsAtomic and Molecular Physics and Opticssymbols.namesakeQuantum mechanicssymbolsStatistical physicsParametric oscillatorQuantum Physics (quant-ph)Computer Science::DatabasesCondensed Matter - Statistical MechanicsOptics (physics.optics)Physics - Optics
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Towards direct measurements of remitted photon path lengths in skin: kinetic studies in the range 520-800 nm

2019

Skin-remitted picosecond laser pulses have been detected at variable input-output fiber distances (8 … 20 mm) in the spectral range 520-800 nm, with subsequent analysis of the pulse shape changes. Transfer functions representing the temporal responses of remitted photons to infinitely narrow δ-pulse excitation have been calculated. Parameters related to the photon path length in skin – input-output pulse peak delays, pulse FWHM, travel times of the “initial” photons and distributions of the remitted photon path lengths – are presented and analyzed. The measurement results are in general agreement with the photon propagation model expectations

PhysicsRange (particle radiation)Full width at half maximumPhotonOpticsPath lengthbusiness.industryPhysics::OpticsbusinessKinetic energyTransfer functionExcitationPulse (physics)Novel Biophotonics Techniques and Applications V
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Perturber's charge effect on Stark broadened hydrogen lines in helium plasmas

2002

Abstract The Stark line profiles for hydrogen Ly α , Ly β , Hα, and Hβ are calculated using the computer simulation method for helium plasmas in the range of electron concentration from 1018 to 10 19 cm −3 at increasing temperature values kT from 7 to 10 eV , according to the experimental measurements in dense plasmas (Bochum experiment). The calculation was carried out at two limiting assumptions about the perturbers: (a) in the helium plasma only singly ionized helium ions occur, and (b) in the plasma the doubly ionized ions exclusively exist. In the paper the ratio of the calculated full half-widths, FWHM(b)/FWHM(a), for these lines are presented. The ratio equals about to 1.1 for Lyβ an…

PhysicsRange (particle radiation)RadiationHydrogenchemistry.chemical_elementPlasmaAtomic and Molecular Physics and OpticsIonFull width at half maximumchemistryIonizationAtomic physicsSpectroscopyHeliumLine (formation)Journal of Quantitative Spectroscopy and Radiative Transfer
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A three-colour scheme to generate isolated attosecond pulses

2009

We propose a new scheme to produce isolated attosecond pulses, involving the use of three laser pulses: a fundamental laser field of intensity I = 3.5 × 1014 W cm−2 and of wavelength λ = 820 nm, and two properly chosen weak lasers with wavelengths 1.5λ and 0.5λ. The three lasers have a Gaussian envelope of 36 fs full width at half maximum. The resulting total field is an asymmetric electric field with an isolated peak. We show that a model atom, interacting with the above-defined total field, generates an isolated attosecond pulse as short as 1/10 of a laser period, i.e. approximately 270 as.

PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciField (physics)business.industryAttosecondAttosecond pulses lasersCondensed Matter PhysicsLaserAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della Materialaw.inventionWavelengthFull width at half maximumOpticslawElectric fieldAtombusinessEnvelope (waves)
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Photonically assisted RF generator with incoherent sources

2008

An RF waveform generator operating with incoherent broadband light is successfully implemented. Complex RF ~10 GHz bandwidth waveforms are generated by means of incoherent wavelength-to-time mapping. Our technique can be scaled to the mm-wave range.

PhysicsSignal generatorbusiness.industryBandwidth (signal processing)ComputingMilieux_PERSONALCOMPUTINGElectrical engineeringBroadband communicationOpticsBroadbandHardware_INTEGRATEDCIRCUITSWaveformBroadband amplifiersRadio frequencyPhotonicsbusinessOECC/ACOFT 2008 - Joint Conference of the Opto-Electronics and Communications Conference and the Australian Conference on Optical Fibre Technology
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Reconfigurable RF waveform generation using optical incoherent sources

2008

An RF waveform generator operating with incoherent broadband light is successfully implemented. Complex RF ~10 GHz bandwidth waveforms are generated by means of incoherent wavelength-to-time mapping. Our technique can be scaled to the mm-wave range.

PhysicsSignal generatorbusiness.industryBandwidth (signal processing)ComputingMilieux_PERSONALCOMPUTINGPulse amplifiersOpticsBroadbandHardware_INTEGRATEDCIRCUITSWaveformRadio frequencybusinessMicrowave photonicsPulse-width modulation2008 Conference on Lasers and Electro-Optics
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PON Monitoring Technique Based on 2D Encoders and Wavelength-to-Time Mapping

2020

A PON monitoring technique is demonstrated based on an OTDR-like device and FBG-encoders having a unique combination of central wavelength and reflection bandwidth. This results in more compact and cost-efficient encoders than previous proposals.

PhysicsSignal processingbusiness.industryBandwidth (signal processing)Data_CODINGANDINFORMATIONTHEORY02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesPassive optical network010309 opticsWavelengthOpticsMode-lockingFiber Bragg gratingFiber optic sensor0103 physical sciences0210 nano-technologybusinessEncoderFrontiers in Optics / Laser Science
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Millimeter-wave and microwave signal generation by low-bandwidth electro-optic phase modulation

2009

We propose, analyze and numerically illustrate a photonic-based technique for waveform generation of electrical signals approaching the 50 GHz bandwidth with time apertures as large as a few nanoseconds, by low-frequency, up to 2 GHz, electro-optic phase modulation of time-stretched optical pulses. Synthesis of the electrical waveform relies on phase-to-amplitude conversion of the modulated signal by a group delay dispersion circuit designed to behave as a transversal filter with N taps. Although arbitrary waveform generation capabilities are limited, a wide variety of user-defined signals are numerically demonstrated by appropriately designing the low-frequency signal driving the electro-o…

PhysicsSignal processingbusiness.industryBandwidth (signal processing)Numerically controlled oscillatorSignalAtomic and Molecular Physics and OpticsOpticsHardware_GENERALChirpWaveformPhotonicsbusinessPhase modulation
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Lossless equalization of frequency combs

2008

Frequency combs obtained by sinusoidal phase modulation of narrow-band continuous-wave lasers are widely used in the field of optical communications. However, the resulting spectral envelope of the comb is not at. In this Letter, we propose a general and eficient approach to achieve at frequency combs with tunable bandwidth. The idea is based on a two-step process. First, eficient generation of a train with temporal at-top-pulse profile is required. Second, we use large parabolic phase modulation in every train period in order to map the temporal intensity shape into the spectral domain. In this way, the resulting spectral envelope is at and the size is tunable with the chirping rate. Two d…

PhysicsSignal processingbusiness.industryBandwidth (signal processing)Optical communicationPhysics::OpticsAtomic and Molecular Physics and OpticsOpticsNarrowbandÒptica físicaSpectral envelopeWavelength-division multiplexingChirpbusinessPhase modulation
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Performance evaluation of a very high resolution small animal PET imager using silicon scatter detectors

2007

A very high resolution positron emission tomography (PET) scanner for small animal imaging based on the idea of inserting a ring of high-granularity solid-state detectors into a conventional PET scanner is under investigation. A particularly interesting configuration of this concept, which takes the form of a degenerate Compton camera, is shown capable of providing sub-millimeter resolution with good sensitivity. We present a Compton PET system and estimate its performance using a proof-of-concept prototype. A prototype single-slice imaging instrument was constructed with two silicon detectors 1 mm thick, each having 512 1.4 mm x 1.4 mm pads arranged in a 32 x 16 array. The silicon detector…

PhysicsSiliconScannerPhotonRadiological and Ultrasound TechnologySiliconbusiness.industryDetectorResolution (electron density)chemistry.chemical_elementEquipment DesignFull width at half maximumOpticschemistryPositron-Emission TomographyAnimalsRadiology Nuclear Medicine and imagingbusinessSensitivity (electronics)Image resolutionPhysics in Medicine and Biology
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