Search results for "Lier"

showing 10 items of 906 documents

Design and implementation of the UFFO burst alert and trigger telescope

2012

The Ultra Fast Flash Observatory pathfinder (UFFO-p) is a telescope system designed for the detection of the prompt optical/UV photons from Gamma-Ray Bursts (GRBs), and it will be launched onboard the Lomonosov spacecraft in 2012. The UFFO-p consists of two instruments: the UFFO Burst Alert and Trigger telescope (UBAT) for the detection and location of GRBs, and the Slewing Mirror Telescope (SMT) for measurement of the UV/optical afterglow. The UBAT isa coded-mask aperture X-ray camera with a wide field of view (FOV) of 1.8 sr. The detector module consists of the YSO(Yttrium Oxyorthosilicate) scintillator crystal array, a grid of 36 multi-anode photomultipliers (MAPMTs), and analog and digi…

PhysicsPhotomultiplierScintillationbusiness.industryApertureAstrophysics::High Energy Astrophysical PhenomenaDetectorAstrophysics::Instrumentation and Methods for AstrophysicsScintillatorlaw.inventionTelescopeOpticslawObservatoryGamma-ray burstbusinessSPIE Proceedings
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Atmospheric Background Measurement in the 300–400 nm Band with a Balloon Borne Experiment during a Nocturnal Flight

2001

The balloon borne experiment, named BABY (BAckground BYpass) belongs to a wider program, AIRWATCH-OWL, intended for the observation of high energy Cosmic Rays from space, detecting the faint UV fluorescence light emitted by the atmospheric Nitrogen as final result of a complex hadronic cascade. In this framework, one of the fundamental information concern the knowledge of the background level. This is one of the main parameters that contribute to the sensitivity of any kind of instrument. The apparatus used for the BABY experiment was designed and completely built at the IFCAI-CNR in Palermo. The instrument is composed by two filtered and collimated photomultipliers (PMT) that detect the UV…

PhysicsPhotomultiplierWavelengthOpticsCascadebusiness.industryDetectorUltra-high-energy cosmic raybusinessBalloonSensitivity (electronics)Collimated lightRemote sensing
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Ultra-Fast Flash Observatory for detecting the early photons from gamma-ray bursts

2011

Gamma-ray bursts (GRBs) are the most luminous transient events with short intense flashes that have been detected in random directions in the sky once or twice per day. Their durations have been measured in seconds, especially short GRBs with duration of < 2 sec. The Ultra-Fast Flash Observatory (UFFO) space mission aims to detect the earliest moments of an explosion which presents the nature of GRBs, resulting into the enhancement of GRB mechanism understanding. The UFFO consists of a couple of wide Field-of-View (FOV) trigger telescopes, a narrow-FOV Slewing Mirror Telescope (SMT) for the fast measurement of the UV-optical photons from GRBs, and a gamma-ray monitor for energy measurement.…

PhysicsPhotomultiplierX-ray astronomyApertureAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Instrumentation and Methods for AstrophysicsAstronomyGamma-ray astronomyAstrophysicsOptical telescopelaw.inventionTelescopelawObservatoryGamma-ray burst2011 2nd International Conference on Space Technology
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A facility to validate photomultipliers for the upgrade of the Pierre Auger Observatory.

2020

The Pierre Auger Observatory is undergoing a major upgrade named AugerPrime with the primary aim to add sensitivity to the mass-composition discrimination of ultrahigh-energy cosmic rays. Two different photomultipliers will be added to each water-Cherenkov station of the surface detector of Observatory. To achieve the scientific goals of AugerPrime these photomultipliers have to ensure a linear response to input-light in a wide range. This paper describes a system developed for the validation of AugerPrime-photomultipliers.

PhysicsPierre Auger ObservatoryPhotomultiplierbusiness.industryLasersSettore FIS/01 - Fisica SperimentaleLaservisible and IR photons (vacuum) (photomultipliersPhoton detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others)OpticsUpgradeHPDsFront-end electronics for detector readoutothers)businessPhoton detectors for UVInstrumentationMathematical PhysicsJournal of Instrumentation
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First Compton imaging tests with i-TED

2019

The objective of this work is to demonstrate the Compton imaging capabilities of a novel gamma-ray Total-Energy Detector called i-TED. The latter is intended for neutron-capture cross-sections measurements of astrophysical interest, thereby enhancing detection sensitivity by means of the simultaneous combination of Time-of-Flight with Compton-imaging techniques. The developed i-TED demonstrator comprises five position-sensitive radiation detection modules of high energy resolution, which feature an overall position-sensitive field-of-view of 125 cm2, and thus a high efficiency. Each detector module is based on 50x50 mm2 large LaCl 3 (Ce) monolithic crystals optically coupled to 8x8 pixels s…

PhysicsPixelPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryDetectorResolution (electron density)01 natural sciencesParticle detector030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineSilicon photomultiplierOptics0103 physical sciencesAngular resolutionbusinessImage resolutionEnergy (signal processing)2019 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC)
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Ultrarelativistic (Cauchy) spectral problem in the infinite well

2016

We analyze spectral properties of the ultrarelativistic (Cauchy) operator $|\Delta |^{1/2}$, provided its action is constrained exclusively to the interior of the interval $[-1,1] \subset R$. To this end both analytic and numerical methods are employed. New high-accuracy spectral data are obtained. A direct analytic proof is given that trigonometric functions $\cos(n\pi x/2)$ and $\sin(n\pi x)$, for integer $n$ are {\it not} the eigenfunctions of $|\Delta |_D^{1/2}$, $D=(-1,1)$. This clearly demonstrates that the traditional Fourier multiplier representation of $|\Delta |^{1/2}$ becomes defective, while passing from $R$ to a bounded spatial domain $D\subset R$.

PhysicsQuantum PhysicsOperator (physics)FOS: Physical sciencesGeneral Physics and AstronomyCauchy distributionMathematical Physics (math-ph)Eigenfunction01 natural sciences010305 fluids & plasmasMultiplier (Fourier analysis)Mathematics - Spectral Theorysymbols.namesakeFourier transformIntegerBounded function0103 physical sciencesFOS: MathematicssymbolsTrigonometric functionsQuantum Physics (quant-ph)010306 general physicsSpectral Theory (math.SP)Mathematical PhysicsMathematical physicsActa Physica Polonica B
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Silicon photomultiplier properties at cryogenic temperatures

2015

Abstract The properties of different types of silicon photomultipliers (SiPMs) were studied at cryogenic temperatures. In liquid nitrogen at 77 K, problems with quenching in Hamamatsu SiPMs and with the protective epoxy layer, covering Zecotek SiPMs, were observed. Tests with one Zecotek SiPM were successful after removal of the epoxy layer. In liquid helium at 4 K, fast signals with pulse lengths shorter than 50 ns were observed, the dark count rate was below 10 Hz and no after-pulses were detected. The gain, as a function of over-voltage, was comparable to room temperature. The SiPM׳s response to photons was found to be linear with intensity for low light levels and single-photon detectio…

PhysicsQuenchingNuclear and High Energy PhysicsPhotonbusiness.industryLiquid heliumEpoxyLiquid nitrogenlaw.inventionSilicon photomultiplierOpticslawvisual_artvisual_art.visual_art_mediumOptoelectronicsbusinessInstrumentationIntensity (heat transfer)Dark currentNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Next generation of the Albira small animal PET based on high density SiPM arrays

2015

A new design of the small animal PET Albira system which detectors are based on arrays of SiPMs and monolithic LYSO scintillator is presented here. The system is made out of 3 rings of 8 detectors each, resulting on an axial and transaxial FOVs of 148 and 80 mm, respectively. The scanner is thermally stabilized using air-cooling. Working temperatures around 22–25°C are reached with individual detector variations around 0.2°C minimizing dark count rates and gain drifts. One of the most significant improvements of the current system is the accurate photon impact determination within the crystal volume, specially its depth of interaction. This allows the calculation of the true line of respons…

PhysicsScannerPhotonOpticsSilicon photomultiplierbusiness.industryDetectorbusinessParallaxSensitivity (electronics)Image resolutionImaging phantom2015 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC)
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Cosmic ray effect on the X-ray Trigger Telescope of UFFO/Lomonosov using YSO scintillation crystal array in space

2017

UFFO Burst Alert and Trigger telescope (UBAT) is the X-ray trigger telescope of UFFO/Lomonosov to localize X-ray source with coded mask method and X-ray detector. Its X-ray detector is made up of 36 8×8 pixels Yttrium OxyorthoSilicate (Y2SiO5:Ce, YSO) scintillation crystal arrays and 36 64-channel Multi-Anode PhotoMultiplier Tubes (MAPMTs) for space mission. Its effective detection area is 161cm2 and energy range is several keV to 150 keV. It was successfully launched in April 28, 2016. In several calibration run, we got several X-ray background data. We already knew X-ray background flux is 2-3 counts/cm2/sec in space. However our X-ray background data shows approximately 7-8 times higher …

PhysicsScintillationPhotomultiplierPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDetectorAstronomyFluxCosmic rayAstrophysicslaw.inventionTelescopeCrystallawCalibrationProceedings of 35th International Cosmic Ray Conference — PoS(ICRC2017)
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Existence and orbital stability of standing waves to nonlinear Schr��dinger system with partial confinement

2018

We are concerned with the existence of solutions to the following nonlinear Schr\"odinger system in $\mathbb{R}^3$: \begin{equation*} \left\{ \begin{aligned} -\Delta u_1 + (x_1^2+x_2^2)u_1&= \lambda_1 u_1 + \mu_1 |u_1|^{p_1 -2}u_1 + \beta r_1|u_1|^{r_1-2}u_1|u_2|^{r_2}, \\ -\Delta u_2 + (x_1^2+x_2^2)u_2&= \lambda_2 u_2 + \mu_2 |u_2|^{p_2 -2}u_2 +\beta r_2 |u_1|^{r_1}|u_2|^{r_2 -2}u_2, \end{aligned} \right. \end{equation*} under the constraint \begin{align*} \int_{\mathbb{R}^3}|u_1|^2 \, dx = a_1>0,\quad \int_{\mathbb{R}^3}|u_2|^2 \, dx = a_2>0, \end{align*} where $\mu_1, \mu_2, \beta >0, 2 1, r_1 + r_2 < \frac{10}{3}$. In the system, the parameters $\lambda_1, \lambda_2 \in \R$ are unknown …

PhysicsSequence010102 general mathematicsStatistical and Nonlinear Physics01 natural sciencesSchrödinger equation010101 applied mathematicsConstraint (information theory)symbols.namesakeNonlinear systemCompact spaceMathematics - Analysis of PDEsLagrange multiplier35J50 35J60symbolsFOS: Mathematics[MATH.MATH-AP]Mathematics [math]/Analysis of PDEs [math.AP]0101 mathematicsComputingMilieux_MISCELLANEOUSMathematical PhysicsSchrödinger's catMathematical physicsEnergy functionalAnalysis of PDEs (math.AP)
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