Search results for "Spectrometers"

showing 10 items of 29 documents

Commissioning of the vacuum system of the KATRIN Main Spectrometer

2016

The KATRIN experiment will probe the neutrino mass by measuring the β-electron energy spectrum near the endpoint of tritium β-decay. An integral energy analysis will be performed by an electro-static spectrometer (``Main Spectrometer''), an ultra-high vacuum vessel with a length of 23.2 m, a volume of 1240 m[superscript 3], and a complex inner electrode system with about 120 000 individual parts. The strong magnetic field that guides the β-electrons is provided by super-conducting solenoids at both ends of the spectrometer. Its influence on turbo-molecular pumps and vacuum gauges had to be considered. A system consisting of 6 turbo-molecular pumps and 3 km of non-evaporable getter strips ha…

010302 applied physicsPhysicsLight nucleusPhysics - Instrumentation and DetectorsSpectrometerSpectrometersPhysics::Instrumentation and DetectorsVacuum-basedFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesEnergy analysisNuclear physics0103 physical sciencesEnergy spectrumGas systems and purificationNeutrino detectorsddc:620010306 general physicsInstrumentationMathematical PhysicsEngineering & allied operationsKATRINdetectors
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Simulations on time-of-flight ERDA spectrometer performance

2016

The performance of a time-of-flight spectrometer consisting of two timing detectors and an ionization chamber energy detector has been studied using Monte Carlo simulations for the recoil creation and ion transport in the sample and detectors. The ionization chamber pulses have been calculated using Shockley-Ramo theorem and the pulse processing of a digitizing data acquisition setup has been modeled. Complete time-of-flight–energy histograms were simulated under realistic experimental conditions. The simulations were used to study instrumentation related effects in coincidence timing and position sensitivity, such as background in time-of-flight–energy histograms. Corresponding measurement…

010302 applied physicsPhysicsta114SpectrometerPhysics::Instrumentation and Detectorsbusiness.industryInstrumentationMonte Carlo methodDetector7. Clean energy01 natural sciencesMonte Carlo simulationsNuclear physicsTime of flightRecoilOpticsData acquisitiontime-of-flight spectrometers0103 physical sciencesIonization chambersimulations010306 general physicsbusinessInstrumentationReview of Scientific Instruments
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Sun-induced chlorophyll fluorescence III: benchmarking retrieval methods and sensor characteristics for proximal sensing

2019

[EN] The interest of the scientific community on the remote observation of sun-induced chlorophyll fluorescence (SIF) has increased in the recent years. In this context, hyperspectral ground measurements play a crucial role in the calibration and validation of future satellite missions. For this reason, the European cooperation in science and technology (COST) Action ES1309 OPTIMISE has compiled three papers on instrument characterization, measurement setups and protocols, and retrieval methods (current paper). This study is divided in two sections; first, we evaluated the uncertainties in SIF retrieval methods (e.g., Fraunhofer line depth (FLD) approaches and spectral fitting method (SFM))…

010504 meteorology & atmospheric sciencesComputer scienceEconomicsGround spectrometersScience0211 other engineering and technologiesContext (language use)02 engineering and technologyGround spectrometer01 natural sciencesSpectral lineRetrieval methodApproximation errorSun-induced chlorophyll fluorescenceSensitivity (control systems)910 Geography & travelChlorophyll fluorescence021101 geological & geomatics engineering0105 earth and related environmental sciencesRemote sensingRetrieval methodsSpectrometerSun-induced chlorophyll fluorescence; Ground spectrometers; Retrieval methods1900 General Earth and Planetary SciencesQHyperspectral imagingsun-induced chlorophyll fluorescence; ground spectrometers; retrieval methods3. Good health10122 Institute of GeographyFISICA APLICADALine (geometry)General Earth and Planetary Sciencesddc:620Interpolation
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Lanthanide–saccharide chemistry: synthesis and characterisation of Ce(III)–saccharide complexes

2000

A series of nine Ce(III) complexes has been synthesised with seven different monosaccharides (D-glucose, D-fructose, D-galactose, D-mannose, L-sorbose, D-ribose and D-xylose) and two different disaccharides (D-maltose and L-lactose), and these have been characterised with various analytical, spectral, magnetic and electrochemical techniques. The NMR studies have highlighted some interesting features about the metal-ion-binding pattern of the saccharides. Some additional coordination has been proposed along with the chelating groups in the saccharide molecules, based on the shifts in 13C NMR spectra. On the other hand, solution absorption studies and solid-state magnetic susceptibilities hav…

Absorption SpectraLanthanideMagnetic Resonance SpectroscopyStereochemistryMetal ions in aqueous solutionMannoseDisaccharidesBiochemistryAnalytical Chemistrychemistry.chemical_compoundSpectroscopy Fourier Transform InfraredElectrochemistryMonosaccharideOrganic chemistryMoleculeChelating Agentschemistry.chemical_classificationMolecular StructureSpectrometersCircular DichroismMetal IonsMonosaccharidesOrganic ChemistryElectric ConductivityElectron Spin Resonance SpectroscopyFructoseCeriumGeneral MedicineCarbon-13 NMRSorbosechemistrySpectrophotometryMetals Rare EarthElectrochemical AnalysisCarbohydrate Research
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Line intensities of CH3D in the Triad region: 6–10μm

2004

Abstract Line intensities of the three lowest fundamentals of the 12CH3D Triad are modeled with an RMS of 3.2% using over 2100 observed values retrieved by multispectrum fitting of enriched sample spectra recorded with two Fourier transform spectrometers. The band strengths of the Triad in units of 10−18 cm−1/(molecule cm−2) at 296 K are, respectively, 2.33 for ν6 (E) at 1161 cm−1, 1.75 for ν3 (A1) at 1307 cm−1 and 0.571 for ν5 (E) at 1472 cm−1. The total calculated absorption arising from 12CH3D Triad fundamentals is 4.65×10−18 cm−1/(molecule cm−2) at 296 K. In addition, some 740 intensities of nine hotbands are fitted to 8.1%; most of the hotband measurements belong to 2ν6−ν6 and ν3+ν6−ν3…

Absorption spectroscopyChemistryOrganic ChemistryFourier transform spectrometersAnalytical chemistrySpectral responseTriad (anatomy)Spectral lineAnalytical ChemistryInorganic Chemistrymedicine.anatomical_structuremedicineMoleculeAbsorption (electromagnetic radiation)SpectroscopyLine (formation)Journal of Molecular Structure
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Unveiling anion-induced folding in tripodal imidazolium receptors by ion-mobility mass spectrometry.

2021

The anion-induced folding of tripodal imidazolium receptors has been investigated by NMR spectroscopy, electrospray ionization ion mobility mass spectrometry and DFT calculations. Such folding can be switched by anion release upon collision induced dissociation.

Collision-induced dissociationIon-mobility spectrometryChemistryElectrospray ionizationMetals and Alloyselectrospray ionizationion mobility spectrometersGeneral ChemistryNuclear magnetic resonance spectroscopyMass spectrometryPhotochemistryCatalysisSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsIonFolding (chemistry)Materials ChemistryCeramics and CompositesReceptormass spectrometrynuclear magnetic resonance spectroscopyChemical communications (Cambridge, England)
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A Geant4 simulation package for the sage spectrometer

2012

International audience; A comprehensive Geant4 simulation was built for the SAGE spectrometer. The simulation package includes the silicon and germanium detectors, the mechanical structure and the electromagnetic fields present in SAGE. This simulation can be used for making predictions through simulating experiments and for comparing simulated and experimental data to better understand the underlying physics.

Electromagnetic fieldHistorySiliconSpectrometer010308 nuclear & particles physicsComputer sciencePhysics::Instrumentation and DetectorsDetectorchemistry.chemical_elementExperimental dataGermaniumComputerApplications_COMPUTERSINOTHERSYSTEMS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesComputer Science ApplicationsEducationComputational scienceKokeellinen ydinfysiikkachemistry0103 physical sciencesComputer Science::Mathematical Software29.40.Wk Solid-state detectors 29.30.Kv X- and gamma-ray spectroscopy 07.85.Nc X-ray and gamma-ray spectrometers 29.30.Dn Electron spectroscopyExperimental nuclear physics010306 general physics
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Methane and carbon monoxide infrared emissions observed at the Canada-France-Hawaii Telescope during the collision of comet SL-9 with Jupiter

1995

Observations with the Fourier Transform Spectrometer were conducted in spectral ranges from 1.6 to 4.7 µm from July 17 to 21 (UT) on the hot plumes appearing on the limb as well as hours or days after the impacts. We present here an analysis of the methane emission observed at 3.3 µm some 10 min after the C impact, indicating the presence of a very small (less than 100 km wide) hot region with temperatures in the 750–1500 K range within the 0.1- to 0.01-mbar region. We also report the detection of CO emission at 4.7 µm 4.5 hrs after the L impact, indicative of a temperature of 274±10 K at the ∼1016 CO molec cm−2 level. The observations suggest that the stratospheric temperature decreases wi…

InfraredCometFourier transform spectrometersInfrared spectroscopyAtmospheric sciencesMethanelaw.inventionTelescopeJupiterchemistry.chemical_compoundGeophysicschemistrylawGeneral Earth and Planetary SciencesEnvironmental scienceCarbon monoxideGeophysical Research Letters
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High resolution study of AsHD2: Ground state and the three bending fundamental bands v(3), v(4), and v(6)

2006

International audience; For the first time the infrared spectrum of the AsHD2 molecule has been measured in the region of the bending fundamental bands v(3), v(4), and v(6) on a Fourier transform spectrometer with a resolution of 0.0024 cm(-1) and analyzed. More than 5500 transitions with J(max) = 26 have been assigned and used both to obtain "ground state combination differences" and for the determination of upper state ro-vibrational energies of the triad (001000), (000100), and (000001). Rotational parameters including centrifugal distortion coefficients up to octic terms of the ground vibrational state were calculated by fitting more than 500 "ground state combination differences" with …

InfraredFourier transform spectrometersHigh resolution7. Clean energy01 natural sciencessymbols.namesakeNuclear magnetic resonance0103 physical sciencesMoleculespectroscopic parametersPhysical and Theoretical Chemistry010303 astronomy & astrophysicsSpectroscopyPhysics[PHYS.PHYS.PHYS-AO-PH]Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]010304 chemical physicsAtomic and Molecular Physics and Opticsinfrared spectrumisotopic species[ PHYS.PHYS.PHYS-AO-PH ] Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]symbolsAsH3Atomic physicsGround stateHamiltonian (quantum mechanics)fundamental bands
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High-accuracy mass measurements on neutron deficient neon isotopes

2005

International audience; The atomic masses of the short-lived nuclides 17Ne and 19Ne have been measured with the triple-trap mass spectrometer ISOLTRAP at ISOLDE/CERN. The obtained mass excess for both nuclides deviates significantly from the literature value, in the case of 17Ne about 40 keV. The mass value of 17Ne can be applied for a test of the isobaric multiplet mass equation with respect to an isospin T = 3/2 quartet. In addition, both masses can contribute to the data analysis of collinear laser-spectroscopy experiments where mean-square nuclear-charge radii are determined.

Mass excessNuclear Theorychemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyISOLTRAPNuclear physicsNeonnuclei with mass number 6 to 190103 physical sciencesNuclideneon010306 general physicsNuclear ExperimentPhysicsmass spectrometers010308 nuclear & particles physicsneutronsAtomic massMass formulaMass21.10.Dr 27.20.+n 29.30.-hIsotopes of neonchemistrynuclear massAtomic physics
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