Search results for "Instrumentation"

showing 10 items of 4914 documents

Angular distribution of scattered electrons associated with collimated bremsstrahlung and the tagging technique

2009

Abstract We investigate the angular correlation between a bremsstrahlung photon and its corresponding post-bremsstrahlung electron within the context of a magnetic tagging spectrometer with the aim of improving the instrument's efficiency. Our results are given in terms of angular distributions of the post-bremsstrahlung electron associated with photons that pass through a circular collimator centered in the forward direction. We start from the fully differential Bethe–Heitler (first Born approximation) cross-section, including the Moliere screening correction, which is then integrated over the photon azimuthal angle and over the photon polar angle defined by the collimator. These integrati…

PhysicsNuclear and High Energy PhysicsPhotonbusiness.industryBremsstrahlungCollimatorElectronSmall-angle approximationCollimated lightlaw.inventionAzimuthOpticslawBorn approximationbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Angular distribution of coherent bremsstrahlung

2012

The angular distribution of the linearly polarised photon beam produced by coherent bremsstrahlung from an aligned diamond radiator has been measured at the MAMI A2 tagged photon facility. The measurements were made with a prototype position sensitive photon detector which utilises the pair production process and a double sided silicon strip detector. This polarised photon beam is used for nuclear and hadronic experiments and in their analysis the polarisation is obtained from a calculation, which matches the experimental intensity spectrum. As the polarisation is related to the photon beam angular distribution, the present measurements can be used to test this calculation. The overall agre…

PhysicsNuclear and High Energy PhysicsPhotonbusiness.industryDetectorHadronBremsstrahlungDiamondengineering.materialOpticsPair productionPosition (vector)engineeringRadiator (engine cooling)businessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The Collinear Fast Beam laser Spectroscopy (Cfbs) experiment at Triumf

2016

Abstract Laser spectroscopy experiments at radioactive ion beam facilities around the world investigate properties of exotic nuclei for scientific endeavours such as, but not limited to, the investigation of nuclear structure. Advancements in experimental sensitivity and performance are continuously needed in order to extend the reach of nuclei that can be measured. The collinear fast beam laser spectroscopy ( Cfbs ) setup at Triumf , coupled to an out-of-plane radio-frequency quadrupole Paul trap, enables measurements of some of the most fundamental nuclear properties for long-lived ground and isomeric states. The first comprehensive overview of the Cfbs experiment is provided along with d…

PhysicsNuclear and High Energy PhysicsPhotonta114Ion beamcollinear laser spectroscopy010308 nuclear & particles physicsbusiness.industrymulti-dimensional data acquisition system01 natural sciences7. Clean energyAcceleration voltagehigh-frequency intensity modulationOpticsData acquisition0103 physical sciencesQuadrupoletime-resolved fluorescence spectroscopyIon trap010306 general physicsSpectroscopybusinessrapid frequency switchingInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Performance of production modules of the Belle II pixel detector in a high-energy particle beam

2021

The Belle II experiment at the Super B factory SuperKEKB, an asymmetric $e^+e^-$ collider located in Tsukuba, Japan, is tailored to perform precision B physics measurements. The centre of mass energy of the collisions is equal to the rest mass of the $\Upsilon(4S)$ resonance of $m_{\Upsilon(4S)} = 10.58\,\rm GeV$. A high vertex resolution is essential for measuring the decay vertices of B mesons. Typical momenta of the decay products are ranging from a few tens of MeV to a few GeV and multiple scattering has a significant impact on the vertex resolution. The VerteX Detector (VXD) for Belle II is therefore designed to have as little material as possible inside the acceptance region. Especial…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsDetectorFOS: Physical sciencesDESYInstrumentation and Detectors (physics.ins-det)01 natural sciences7. Clean energyCharge sharinglaw.inventionB-factoryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciencesInvariant massHigh Energy Physics::Experiment010306 general physicsColliderInstrumentationImage resolutionBeam (structure)
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Determining the neutrino mass with cyclotron radiation emission spectroscopy—Project 8

2017

The most sensitive direct method to establish the absolute neutrino mass is observation of the endpoint of the tritium beta-decay spectrum. Cyclotron Radiation Emission Spectroscopy (CRES) is a precision spectrographic technique that can probe much of the unexplored neutrino mass range with $\mathcal{O}({\rm eV})$ resolution. A lower bound of $m(\nu_e) \gtrsim 9(0.1)\, {\rm meV}$ is set by observations of neutrino oscillations, while the KATRIN Experiment - the current-generation tritium beta-decay experiment that is based on Magnetic Adiabatic Collimation with an Electrostatic (MAC-E) filter - will achieve a sensitivity of $m(\nu_e) \lesssim 0.2\,{\rm eV}$. The CRES technique aims to avoid…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)7. Clean energy01 natural sciencesUpper and lower boundsHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesHigh Energy Physics::ExperimentCyclotron radiationEmission spectrumSensitivity (control systems)Nuclear Experiment (nucl-ex)Neutrino010306 general physicsNeutrino oscillationAdiabatic processNuclear ExperimentKATRIN
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A novel experimental system for the KDK measurement of the 40K decay scheme relevant for rare event searches

2020

Potassium-40 ($^{40}$K) is a long-lived, naturally occurring radioactive isotope. The decay products are prominent backgrounds for many rare event searches, including those involving NaI-based scintillators. $^{40}$K also plays a role in geochronological dating techniques. The branching ratio of the electron capture directly to the ground state of argon-40 has never been measured, which can cause difficulty in interpreting certain results or can lead to lack of precision depending on the field and analysis technique. The KDK (Potassium (K) Decay (DK)) collaboration is measuring this decay. A composite method has a silicon drift detector with an enriched, thermally deposited $^{40}$K source …

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsDecay schemeSilicon drift detectorSpectrometerPhysics::Instrumentation and Detectors010308 nuclear & particles physicsElectron captureBranching fractionDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Scintillator7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentInstrumentationEvent (particle physics)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Production and characterization of a custom-made 228Th source with reduced neutron source strength for the Borexino experiment

2012

A custom-made 228Th source of several MBq activity was produced for the Borexino experiment for studying the external background of the detector. The aim was to reduce the unwanted neutron emission produced via (alpha,n) reactions in ceramics used typically for commercial 228Th sources. For this purpose a ThCl4 solution was converted chemically into ThO2 and embedded into a gold foil. The paper describes the production and the characterization of the custom-made source by means of gamma-activity, dose rate and neutron source strength measurements. From gamma-spectroscopic measurements it was deduced that the activity transfer from the initial solution to the final source was >91% (at 68%…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsDosimeterIsotope530 PhysicsNeutron emission3105 InstrumentationRadiochemistryFOS: Physical sciencesThoriumchemistry.chemical_elementInstrumentation and Detectors (physics.ins-det)10192 Physics InstituteNuclear physicschemistryMeasuring instrumentNeutron source3106 Nuclear and High Energy PhysicsInstrumentationBorexinoIsotopes of thoriumNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The magnetic shielding for the neutron decay spectrometer aSPECT

2014

Abstract Many experiments in nuclear and neutron physics are confronted with the problem that they use a superconducting magnetic spectrometer which potentially affects other experiments by their stray magnetic field. The retardation spectrometer a SPECT consists, inter alia, of a superconducting magnet system that produces a strong longitudinal magnetic field of up to 6.2 T. In order not to disturb other experiments in the vicinity of a SPECT, we had to develop a magnetic field return yoke for the magnet system. While the return yoke must reduce the stray magnetic field, the internal magnetic field and its homogeneity should not be affected. As in many cases, the magnetic shielding for a S…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectromagnetMagnetic energyDemagnetizing fieldForce between magnetsFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)law.inventionComputational physicsNuclear physicsMagnetizationlawMagnetElectromagnetic shieldingMagnetic pressureNuclear Experiment (nucl-ex)InstrumentationNuclear Experiment
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Particle Identification with DIRCs at PANDA

2019

The DIRC technology (Detection of Internally Reflected Cherenkov light) offers an excellent possibility to minimize the form factor of Cherenkov detectors in hermetic high energy detectors. The PANDA experiment at FAIR in Germany will combine a barrel-shaped DIRC with a disc-shaped DIRC to cover an angular range of 5 to 140 degrees. Particle identification for pions and kaons with a separation power of 3 standard deviations or more will be provided for momenta between 0.5 GeV/c and 3.5 GeV/c in the barrel region and up to 4 GeV/c in the forward region. Even though the concept is simple, the design and construction of a DIRC is challenging. High precision optics and mechanics are required to…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsLarge Hadron ColliderPhotonCherenkov detectorbusiness.industryPhysics::Instrumentation and DetectorsDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Particle identificationlaw.inventionOpticslawDetection of internally reflected Cherenkov lightHigh Energy Physics::ExperimentParticle beambusinessInstrumentationCherenkov radiation
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Irradiation study of a fully monolithic HV-CMOS pixel sensor design in AMS 180 nm

2018

Abstract High-Voltage Monolithic Active Pixel Sensors (HV-MAPS) based on a 180 nm HV-CMOS process have been proposed to realize thin, fast and highly integrated pixel sensors. The MuPix7 prototype, fabricated in the commercial AMS H18 process, features a fully integrated on-chip readout, i.e. hit-digitization, zero suppression and data serialization. MuPix7 is the first fully monolithic HV-CMOS pixel sensor that has been tested for the use in high irradiation environments like HL-LHC. We present results from laboratory and test beam measurements of MuPix7 prototypes irradiated with neutrons (up to 5.0 × 1015 neq/cm2) and 24 GeV protons (up to 7.8 × 1015 protons/cm2) and compare the performa…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPixelPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesNoise (electronics)030218 nuclear medicine & medical imagingPhase-locked loop03 medical and health sciences0302 clinical medicineCMOS0103 physical sciencesOptoelectronicsNeutronIrradiationbusinessInstrumentationZero suppressionData transmission
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