Search results for "spectrometer"

showing 10 items of 751 documents

The Endcap Disc DIRC detector of PANDA

2019

Abstract At the international FAIR laboratory, an upcoming significant enlargement of the GSI installations near Darmstadt, Germany, the PANDA antiproton experiment will investigate fundamental questions of hadron physics in the charm quark energy range. Antiprotons in the 1.5 to15 GeV/c momentum range will interact with gas jet or pellet fixed targets. The Endcap Disc DIRC (Detection of Internally Reflected Cherenkov light) covers the forward endcap solid angle of the PANDA target spectrometer to positively identify charged kaons. Monte-Carlo simulations indicate that from 1 up to 4 GeV/c one can achieve kaon–pion separation with a separation power of at least 3 standard deviations. For th…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSpectrometerPhysics::Instrumentation and Detectors010308 nuclear & particles physicsDetectorJet (particle physics)01 natural sciences030218 nuclear medicine & medical imagingCharm quarkNuclear physicsMomentum03 medical and health sciences0302 clinical medicineDetection of internally reflected Cherenkov lightAntiproton0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A $B_4C$-silicon target for the detection of neutrino interactions

1998

This note describes the construction of a target for neutrino interactions composed of passive boron carbide plates interleaved with silicon microstrip detectors. The target contains four layers of passive material with a total mass of 45 kg and 600 single--sided silicon microstrip detectors with a total surface of 1.14 m$^2$ distributed over five layers. It is installed in the NOMAD spectrometer at the CERN SPS neutrino beam. During the 1997 run about 8000 \nm\ charged current interactions were estimated to have occurred in the target. For these events it will be possible to perform a precise measurement of both vertex and kinematical variables. This will provide invaluable experience towa…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSpectrometerSiliconPhysics::Instrumentation and DetectorsFísicachemistry.chemical_elementsilicon microstrip detectors; neutrino oscillations; silicon strip sensors; tracking detectors; search; alignmentNuclear physicsNeutrino detectorchemistryMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationInstrumentationCharged currentParticle Physics - Experiment
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Alignment of the NOMAD-STAR detector

2000

Abstract This note describes the alignment of the NOMAD-STAR detector. This is the B 4 C-silicon target installed in the NOMAD spectrometer in 1997. NOMAD-STAR is composed of modules of 12 silicon detectors each giving a total length of 72 cm. Ten of these modules (called ladders) are assembled to form a layer. There are five layers interleaved with passive boron carbide plates. The total surface of silicon is 1.14 m 2 . Energetic muons from the flat-top of the CERN SPS cycle provide the necessary information to perform a very precise software alignment. This alignment is needed to ensure that the impact parameter measurement needed for the identification of taus in a detector like NOMAD-ST…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSpectrometerSiliconbusiness.industryDetectorchemistry.chemical_elementParticle detectorSemiconductor detectorOpticschemistryMeasuring instrumentbusinessInstrumentationSTAR detectorNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The Barrel DIRC detector of PANDA

2019

The PANDA experiment is one of the four large experiments being built at FAIR in Darmstadt. It will use a cooled antiproton beam on a fixed target within the momentum range of 1.5 to 15 GeV/c to address questions of strong QCD, where the coupling constant $\alpha_s \gtrsim 0.3$. The luminosity of up to $2 \cdot 10^{32} cm^{-2}s^{-1}$ and the momentum resolution of the antiproton beam down to \mbox{$\Delta$p/p = 4$\cdot10^{-5}$} allows for high precision spectroscopy, especially for rare reaction processes. Above the production threshold for open charm mesons the production of kaons plays an important role for identifying the reaction. The DIRC principle allows for a compact particle identif…

PhysicsNuclear and High Energy PhysicsLuminosity (scattering theory)Physics - Instrumentation and DetectorsCalorimeter (particle physics)SpectrometerMeson010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesCharged particleParticle identification030218 nuclear medicine & medical imagingNuclear physics03 medical and health sciences0302 clinical medicine0103 physical sciencesHigh Energy Physics::ExperimentPrismNuclear ExperimentInstrumentation
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Precision measurement of the conversion electron spectrum of 83mKr with a solenoid retarding spectrometer

1992

This paper reports on precision measurements of conversion lines in the decay of 83mKr with nuclear transition energies of 32.1 keV and 9.4 keV, respectively. The spectra were taken from a submonolayer surface of 83mKr frozen onto a cold backing, using the new Mainz solenoid retarding spectrometer. The high luminosity and resolution of this instrument enables the observation of all allowed conversion lines up to the N-shell and to fully separate the elastic component from inelastic satellites. The combined analysis of the data yields the transition energies Ey=32151.5±1.1 eV and 9405.9±0.8 eV, respectively. The experiment served also to pilot the application of this spectrometer to the ques…

PhysicsNuclear and High Energy PhysicsLuminosity (scattering theory)SpectrometerSolenoidElectronpacs:29.30.Dnpacs:27.50.+eElectron spectroscopySpectral lineNuclear physicsNuclear fusionddc:530NeutrinoAtomic physics
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Probing short-range nucleon-nucleon correlations with virtual photons at MAMI

2000

Abstract Nucleon-nucleon correlations were studied in two (e, e′pp) experiments. The first one, on 12C, was performed in close to 4π geometry at Ebeam = 705 MeV, ω = 225 MeV, and q = 412 MeV/c. The electrons were observed in a large-acceptance magnetic spectrometer in coincidence with protons detected in a BGO crystal ball. Missing energy and momentum, relative momentum and angular distributions were derived and compared with a facorised two-nucleon emision model. A G-matrix correlation function is favoured by the data. The second experiment was a high resolution study of the reaction 16O(e, e′pp)14C in super-parallel kinematics. Three magnetic spectrometers were used in coincidence at Ebea…

PhysicsNuclear and High Energy PhysicsMissing energySpectrometerNuclear TheoryVirtual particleElectronNuclear physicsMomentumExcited stateAtomic physicsNuclear ExperimentNucleonCrystal BallProgress in Particle and Nuclear Physics
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A broad iron line in the Chandra/HETG spectrum of 4U 1705-44

2004

We present preliminary results from a Chandra 30 ks observation of the atoll sourco 4U 1705 44. In particular we concentrate on the study of the iron Kα line, using the HEG spectrometer. The iron Kα line at ~ 6.6 keV is found to be intrinsically broad (FWHM ~ 1.7 keV); its width can be explained by reflection from a cold accretion disk extending down to ~ 17 km from the neutron star center or by Compton broadening in the hotter (~ 3 – 4 keV) corona.

PhysicsNuclear and High Energy PhysicsNeutron starFull width at half maximumSpectrometerAccretion discK-alphaAstronomyAstrophysicsAtomic and Molecular Physics and Optics
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Die relative Isotopenlage des Os186

1962

Using three different samples of Os192, Os190 and Os186 enriched to 98.68%, 95.46%, and 61.27%, respectively, the isotopic shiftsΔν(Os192−Os190) andΔν(Os192−Os186) have been measured in four Os I-lines with a recording Fabry-Perot spectrometer. The relative isotopic position of Os186 has been found to be $$\frac{{\Delta \nu (Os^{192} - Os^{186} )}}{{\Delta \nu (Os^{192} - Os^{190} )}} = 3.52 \pm 0.03.$$

PhysicsNuclear and High Energy PhysicsNuclear magnetic resonanceSpectrometerPosition (vector)Analytical chemistryNuclear fusionSpectral shiftZeitschrift f�r Physik
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First measurement ofK-shell-electron to internal-pair conversion probability ratios forE0 transitions inf p shell region

1986

Magnetic plus Si(Li) spectrometers designed for high-resolution conversion-electron and internal-pair measurements, are employed to obtainK-shell-electron to internal-pair conversion probability ratios forE0 transitions in54Fe,60Ni,64Zn and70Ge. The results are found to be in good agreement with theoretical predictions.

PhysicsNuclear and High Energy PhysicsNuclear magnetic resonanceSpectrometerShell (structure)Nuclear fusionElectronAtomic physicsZeitschrift f�r Physik A Atomic Nuclei
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Indirect Dark Matter Search with Antideuterons: Progress and Future Prospects for General Antiparticle Spectrometer (GAPS)

2007

We report on recent accelerator testing of a prototype general antiparticle spectrometer (GAPS). GAPS is a novel approach for indirect dark matter searches that exploits the antideuterons produced in neutralino-neutralino annihilations. Many supersymmetry models, as well as other models based on extra dimensions, predict a primary antideuteron flux from dark matter annihilation that is much greater than the secondary and tertiary background sources at low energies. The GAPS method involves capturing antiparticles in a target material into excited energy states. The X-rays that are emitted as the antiparticle cascades to lower energy states before the exotic atom decays serve as a fingerprin…

PhysicsNuclear and High Energy PhysicsParticle physicsAntiparticleAnnihilationSpectrometerDark matterElementary particleAtomic and Molecular Physics and OpticsNuclear physicsExtra dimensionsAntimatterHigh Energy Physics::ExperimentExotic atomNuclear Physics B - Proceedings Supplements
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