Search results for "CONSTRUCTION"

showing 10 items of 2670 documents

Compatibility, effectiveness and susceptibility to degradation of alkoxysilane-based consolidation treatments on a carbonate stone

2021

Abstract Alkoxysilane-based consolidation treatment are commonly employed in restoration and conservation works of Cultural Heritage buildings. However, their poor affinity to carbonate stones is well-known. In this paper, we evaluate three consolidant treatments (two of them modified to incorporate hydrophobic or photocatalytic properties), formulated to circumvent this drawback and their cracking during drying, through a surfactant-assisted synthesis. The consolidants were applied on Noto stone, a biocalcarenite (~95% CaCO3 ) employed in numerous Cultural Heritage buildings of Southern Italy. A comprehensive validation of the three consolidants, compared to a commercial TEOS based consoli…

Noto stoneMaterials scienceConsolidation (soil)Hydrophobicity0211 other engineering and technologies02 engineering and technologyBuilding and ConstructionMechanical resistancePulp and paper industrySettore ICAR/12 - Tecnologia Dell'Architetturachemistry.chemical_compoundPhotocatalysichemistryMechanics of MaterialsSusceptibility021105 building & constructionArchitectureCompatibility (mechanics)CarbonateDegradation (geology)Consolidant021108 energySafety Risk Reliability and QualityCivil and Structural Engineering
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Low-cost method for obtaining medical rapid prototyping using desktop 3d printing : a novel technique for mandibular reconstruction planning

2017

Background Three-dimensional (3D) printing is relatively a new technology with clinical applications, which enable us to create rapid accurate prototype of the selected anatomic region, making it possible to plan complex surgery and pre-bend hardware for individual surgical cases. This study aimed to express our experience with the use of medical rapid prototype (MRP) of the maxillofacial region created by desktop 3D printer and its application in maxillofacial reconstructive surgeries. Material and methods Three patients with benign mandible tumors were included in this study after obtaining informed consent. All patient's maxillofacial CT scan data was processed by segmentation and isolat…

Novel techniqueRapid prototypingmedicine.medical_specialtyReconstructive surgerybusiness.industryComputer scienceResearch3D printing030206 dentistry:CIENCIAS MÉDICAS [UNESCO]Surgical planning03 medical and health sciences0302 clinical medicineSoftware030220 oncology & carcinogenesisComputer graphics (images)UNESCO::CIENCIAS MÉDICASmedicineMedical physicsSegmentationMandibular reconstructionOral SurgerybusinessGeneral Dentistry
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Spatial Reconstruction Algorithm of DT Layer in Cryogenic Targets Using Optical Techniques

2007

The measurements of the solid DT layer, in terms of thickness and roughness, in the LMJ geometry (i.e. in a hohlraum) are not trivial. The DT layer measurements will be done using a Matsukov-Cassegrain telescope placed 39 cm away from the target. This telescope will be used to acquire shadowgraphy images on equators, and interferometric measurements on pole areas using optical coherence tomography (OCT). Optical coherence tomography allows determining the DT layer thickness on a few points, in the polar regions of the target. By scanning around the poles, several points can be acquired in order to calculate the roughness and the local shape of the DT layer at the pole. Both techniques were …

Nuclear and High Energy Physics020209 energy02 engineering and technologySurface finishShadowgraphy01 natural sciences010305 fluids & plasmaslaw.inventionTelescopeOpticsOptical coherence tomographyHohlraumlaw0103 physical sciences0202 electrical engineering electronic engineering information engineeringmedicineGeneral Materials ScienceCivil and Structural EngineeringPhysicsmedicine.diagnostic_testbusiness.industryMechanical EngineeringReconstruction algorithmInterferometryNuclear Energy and EngineeringbusinessLayer (electronics)Fusion Science and Technology
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The experience of building and operating COMPASS RICH-1

2010

COMPASS RICH-1 is a large size gaseous Imaging Cherenkov Detector providing hadron identification in the range from 3 to 55 GeV/c, in the wide acceptance spectrometer of the COMPASS Experiment at CERN SPS. It uses a 3 m long C(4)F(10) radiator, a 21 m(2) large VUV mirror surface and two kinds of photon detectors: MAPMTs and MWPCs with CsI photocathodes, covering a total of 5.5 m(2). It is in operation since 2002 and its performance has increased in time thanks to progressive optimization and mostly to a major upgrade which was implemented in 2006. The main characteristics of COMPASS RICH-1 components are described and some specific aspects related to the radiator gas system, the mirror alig…

Nuclear and High Energy PhysicsCherenkov detectorPhysics::Instrumentation and Detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]COMPASS01 natural sciencesParticle identificationParticle identificationlaw.inventionNuclear physicsCOMPASS; CsI; MAPMT; Photon detection; PID; RICH; Instrumentation; Nuclear and High Energy PhysicsOpticslawCompass0103 physical sciencesCOMPASS experimentCsI photoconverter010306 general physicsRICHInstrumentationEvent reconstructionPhysicsLarge Hadron ColliderSpectrometer010308 nuclear & particles physicsbusiness.industryPIDUpgradePhoton detectionMAPMTCsIParticle identification; COMPASS; RICH; MAPMT; CsI photoconverterHigh Energy Physics::Experimentbusiness
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The measuring method for tests of horizontal two-phase gas–liquid flows, using optical and capacitance tomography

2009

Abstract The paper presents a measurement method in testing horizontal two-phase gas–liquid flows. It also describes the test stand including two tomography measurement systems. The optical and capacitance tomography systems can be used for measurements at the same time. It is necessary to apply two tomography systems working at the same time because of complexity of phenomena occurring in two-phase flows, and a wide range of applicability of the presented method. The optical tomography system in which a tested object is illuminated from five projections. The measurement of luminous intensity is changed into a discrete signal (0 or 1) in the detectors including 64 optical sensors. Next, the…

Nuclear and High Energy PhysicsEngineeringmedicine.diagnostic_testbusiness.industryMechanical EngineeringSystem of measurementDetectorPhase (waves)Iterative reconstructionCapacitanceDiscrete-time signalOpticsNuclear Energy and EngineeringmedicineGeneral Materials ScienceTomographyOptical tomographySafety Risk Reliability and QualitybusinessWaste Management and DisposalNuclear Engineering and Design
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Improvement in fast particle track reconstruction with robust statistics

2014

The IceCube project has transformed one cubic kilometer of deep natural Antarctic ice into a Cherenkov detector. Muon neutrinos are detected and their direction inferred by mapping the light produced by the secondary muon track inside the volume instrumented with photomultipliers. Reconstructing the muon track from the observed light is challenging due to noise, light scattering in the ice medium, and the possibility of simultaneously having multiple muons inside the detector, resulting from the large flux of cosmic ray muons. This manuscript describes work on two problems: (1) the track reconstruction problem, in which, given a set of observations, the goal is to recover the track of a muo…

Nuclear and High Energy PhysicsParticle physicsCherenkov detectorPhysics::Instrumentation and DetectorsFOS: Physical sciencesddc:500.2Neutrino telescopeTrack reconstructionlaw.inventionIceCubelawCoincidentAngular resolutionddc:530InstrumentationInstrumentation and Methods for Astrophysics (astro-ph.IM)Remote sensingIce CubePhysicsMuonTrack (disk drive)DetectorIceCube; Neutrino astrophysics; Neutrino telescope; Robust statistics; Track reconstructionRobust statisticsNeutrino astrophysicsNeutrino detectorHigh Energy Physics::ExperimentNeutrinoAstrophysics - Instrumentation and Methods for AstrophysicsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Updated precision measurement of the average lifetime of B hadrons

1996

The measurement of the average lifetime of B hadrons using inclusively reconstructed secondary vertices has been updated using both an improved processing of previous data and additional statistics from new data. This has reduced the statistical and systematic uncertainties and gives \tau_{\mathrm{B}} = 1.582 \pm 0.011\ \mathrm{(stat.)} \pm 0.027\ \mathrm{(syst.)}\ \mathrm{ps.} Combining this result with the previous result based on charged particle impact parameter distributions yields \tau_{\mathrm{B}} = 1.575 \pm 0.010\ \mathrm{(stat.)} \pm 0.026\ \mathrm{(syst.)}\ \mathrm{ps.}

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationHadron01 natural sciencesb taggingPartícules (Física nuclear)030218 nuclear medicine & medical imagingNuclear physics03 medical and health sciencesinclusive reconstruction0302 clinical medicine0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentDELPHIPhysics010308 nuclear & particles physicsLARGE ELECTRON POSITRON COLLIDERCharged particleB hadrons lifetimeDELPHI; B hadrons lifetime; inclusive reconstruction; b taggingPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearAstrophysics::Earth and Planetary AstrophysicsImpact parameterParticle Physics - Experiment
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Precision Muon Reconstruction in Double Chooz

2014

We describe a muon track reconstruction algorithm for the reactor anti-neutrino experiment Double Chooz. The Double Chooz detector consists of two optically isolated volumes of liquid scintillator viewed by PMTs, and an Outer Veto above these made of crossed scintillator strips. Muons are reconstructed by their Outer Veto hit positions along with timing information from the other two detector volumes. All muons are fit under the hypothesis that they are through-going and ultrarelativistic. If the energy depositions suggest that the muon may have stopped, the reconstruction fits also for this hypothesis and chooses between the two via the relative goodness-of-fit. In the ideal case of a thro…

Nuclear and High Energy PhysicsParticle physicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsFOS: Physical sciencesSTRIPSDouble Chooz; Muon reconstruction; Neutrino detector[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]CHOOZScintillatorHigh Energy Physics - Experimentlaw.inventionNONuclear physicsNeutrino detectorHigh Energy Physics - Experiment (hep-ex)law[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]InstrumentationImage resolutionPhysicsMuonDetectorReconstruction algorithmInstrumentation and Detectors (physics.ins-det)Double ChoozNeutrino detectorPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentMuon reconstruction
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Determining neutrino oscillation parameters from atmospheric muon neutrino disappearance with three years of IceCube DeepCore data

2014

We present a measurement of neutrino oscillations via atmospheric muon neutrino disappearance with three years of data of the completed IceCube neutrino detector. DeepCore, a region of denser instrumentation, enables the detection and reconstruction of atmospheric muon neutrinos between 10 GeV and 100 GeV, where a strong disappearance signal is expected. The detector volume surrounding DeepCore is used as a veto region to suppress the atmospheric muon background. Neutrino events are selected where the detected Cherenkov photons of the secondary particles minimally scatter, and the neutrino energy and arrival direction are reconstructed. Both variables are used to obtain the neutrino oscilla…

Nuclear and High Energy PhysicsParticle physicsPhysics - Instrumentation and DetectorsTELESCOPEPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)TRACK RECONSTRUCTIONMuon neutrinoddc:530Neutrino oscillationPhysicsHigh Energy Physics::PhenomenologyInstrumentation and Detectors (physics.ins-det)Solar neutrino problemPERFORMANCENeutrino detectorPhysics and AstronomyMeasurements of neutrino speedHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsNeutrinoNeutrino astronomySYSTEM
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AGATA-Advanced GAmma Tracking Array

2012

WOS: 000300864200005

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPulse-shape and gamma-ray tracking algorithmsFOS: Physical sciencesSemiconductor detector performance and simulationsIntegrated circuit[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Tracking (particle physics)gamma-Ray tracking01 natural sciencesPulse-shape and γ-ray tracking algorithmslaw.inventionData acquisitionlaw0103 physical sciencesddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsγ-Ray spectroscopyNuclear ExperimentInstrumentationDigital signal processingEvent reconstructiongamma-Ray spectroscopyPhysicssezeleSpectrometerSpectrometers010308 nuclear & particles physicsbusiness.industryDetectorAGATA Digital signals HPGe detectors Pulse-shape Ray trackingHPGe detectorsAlgorithms Crystals Germanium Semiconductor detectors Signal processing Spectrometry Tracking (position)γ-Ray trackingInstrumentation and Detectors (physics.ins-det)Digital signal processingAGATAFísica nuclearbusinessAGATAComputer hardware
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