Search results for "Instrumentation"

showing 10 items of 4914 documents

Beamline pulsing system for cyclotrons

1998

Abstract A beamline pulsing system for cyclotrons is presented. The function of this system is to modify the structure of a cyclotron ion beam guided to the desired research target by a beamline. In some in-beam experiments, an adjustment of the time structure of the beam is sometimes needed. This kind of situation occurs if, for example, the life time of the target material is longer than the period corresponding to the beam frequency. In this case, the frequency of the ion pulses hitting the target is 10–21 MHz depending on the frequency of the acceleration voltage. The adjustment of the ion beam pulse frequency is carried out by a beamline deflector. Deflection is achieved by feeding a h…

PhysicsNuclear and High Energy PhysicsIon beambusiness.industryCyclotronAcceleration voltagelaw.inventionIonFrequency dividerSignal levelOpticsBeamlineDeflection (engineering)lawbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Beam phase measurement system for the K130 cyclotron in Jyväskylä

1993

Abstract A phase measurement system for Jyvaskyla new K = 130 heavy ion cyclotron has been designed and realized. The phase measurement is done using a set of capacitive probes to detect phase information from the internal ion beam. This data is vital for tuning purposes to obtain an isochronous magnetic field and to maximize the ion beam intensity.

PhysicsNuclear and High Energy PhysicsIon beambusiness.industrySystem of measurementCyclotronPhase (waves)Fourier transform ion cyclotron resonancelaw.inventionIon beam depositionOpticsPhysics::Plasma PhysicslawAtomic physicsbusinessInstrumentationIon cyclotron resonanceBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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On the resonant neutrinoless double-electron-capture decay of ^{136}Ce

2011

Abstract The double-electron-capture Q value for the 136Ce decay to 136Ba has been determined at JYFLTRAP. The measured value 2378.53(27) keV excludes the energy degeneracy with the 0 + excited state of the decay daughter 136Ba at 2315.32(7) keV in a resonant 0 ν ECEC decay by 11.67 keV. The new Q value differs from the old adopted value 2419(13) keV (Atomic Mass Evaluation 2003) by 40 keV and is 50 times more precise. Our calculations show that the precise Q value renders the resonant 0 ν ECEC decay of 136Ce undetectable by the future underground detectors. We measured also the double-β decay Q value of 136Xe to be 2457.86(48) keV which agrees well with the value 2457.83(37) keV measured a…

PhysicsNuclear and High Energy PhysicsIon beamta114Physics::Instrumentation and DetectorsQ valueElectron captureAstrophysics::High Energy Astrophysical PhenomenaHalf-lifePenning trapAtomic massNuclear physicsExcited stateAtomic physicsPhysics Letters B
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Speeding up liquid-phase heavy element chemistry: Development of a vacuum to liquid transfer chamber (VLTC)

2021

Abstract We present a new system, which is suitable for performing fast liquid phase chemistry experiments and gives access to shorter-lived isotopes of super heavy elements (SHE) than accessible with current techniques. With this novel vacuum to liquid transfer chamber (VLTC), which is mounted behind a physical preseparator, the desired isotopes are transported from the low-pressure side of the recoil separator directly into the liquid phase of a chemical experiment. Simulations on the kinematics of evaporation residues were performed using SRIM, validating the general plausibility of the VLTC concept. Subsequently, the feasibility was demonstrated with 250 , 252 Cf fission fragments, whic…

PhysicsNuclear and High Energy PhysicsIon exchangeFissionEvaporationAnalytical chemistryTransactinide elementchemistry.chemical_compoundchemistryNitric acidChemical stabilityCurrent (fluid)SpectroscopyInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A new method for the labelling of proteins with radioactive arsenic isotopes

2006

Abstract  Radioarsenic labelled radiopharmaceuticals could be a valuable asset to positron emission tomography. In particular, the long half-lives of 72As ( T 1 / 2 = 26 h ) and 74As ( T 1 / 2 = 17.8 d ) allow to investigate slow physiological or metabolical processes, like the enrichment and distribution of monoclonal antibodies (mab) in tumour tissue. In this work, a new method for the labelling of proteins with various radioactive arsenic isotopes was developed. For this purpose, two proteins, namely a chimeric IgG3 monoclonal antibody, ch3G4, directed against anionic phospholipids, and Rituxan (Rituximab), were labelled as a proof of principle with no-carrier-added radioarsenic isotopes…

PhysicsNuclear and High Energy PhysicsIsotopeMolecular massmedicine.drug_classRadiochemistrychemistry.chemical_elementMonoclonal antibodyno keywordsTumour tissuechemistryLabellingmedicineDistribution (pharmacology)InstrumentationArsenic
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Low-lying structure of light radon isotopes

2002

The excited states in the neutron-deficient isotopes Rn have been populated using the Er(Ar,4n), Er(Ar,4n), and Er(Ar,4n) reactions at beam energies of 175, 182, and 177 MeV, respectively. Evaporation residues were selected using an in-flight gas-filled separator and implanted at the focal plane into a 16-element position-sensitive, passivated ion-implanted planar silicon detector. Prompt γ rays were observed at the target position using an array of Compton-suppressed germanium detectors. Correlation with the subsequent radioactive decay of associated recoiling ions in the silicon detector, recoil-γ and recoil-γ-γ coincidences were used to construct decay schemes of light radon isotopes. Me…

PhysicsNuclear and High Energy PhysicsIsotopePhysics::Instrumentation and Detectorschemistry.chemical_elementGermaniumRadonMicrosecondchemistryExcited stateAlpha decayAtomic physicsNuclear ExperimentRadioactive decayPolonium
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Intense beams of mass-separated, neutron-deficient indium, tin, thallium and lead isotopes

1985

A discharge ion source of the FEBIAD-type that delivers intense beams of neutron-deficient isotopes of indium, tin, thallium and lead produced in heavy-ion-induced fusion reactions is described. After mass separation the isotopically pure beams with intensities of up to 3 × 107 ions/s were available for gamma and laser spectroscopy. This corresponds to an overall separation efficiency of about 30%.

PhysicsNuclear and High Energy PhysicsIsotopeRadiochemistrychemistry.chemical_elementIon sourceIonchemistryPhysics::Plasma PhysicsThalliumNeutronAtomic physicsNuclear ExperimentTinInstrumentationIsotopes of indiumIndiumNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Electron-transporter spectrometer for on-line isotope separator

1991

Abstract ELLJ — a conversion-electron and beta-ray spectrometer for an on-line isotope separator - is described. The instrument is a broad-range, high-transmission device consisting of a two-coil magnetic transporter plus a cooled Si(Li) detector. The spectrometer was designed to perform several kinds of coincidence measurements. A number of representative spectra of fission-product activities separated on-line at the IGISOL facility demonstrate the performance of the spectrometer.

PhysicsNuclear and High Energy PhysicsIsotopeSpectrometerPhysics::Instrumentation and DetectorsDetectorAnalytical chemistryElectronSpectral lineNuclear magnetic resonanceNuclear ExperimentInstrumentationSeparator (electricity)Hybrid mass spectrometerNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Atomic beam magnetic resonance apparatus for systematic measurement of hyperfine structure anomalies (Bohr-Weisskopf effect)

1993

Abstract An atomic beam magnetic resonance (ABMR) apparatus has been constructed at Orsay, and has been installed at the CERN PS Booster ISOLDE mass separator facility for “on-line” work with radioactive isotopes in a program to measure hyperfine structure anomalies (the Bohr-Weisskopf effect) over long isotopic chains. The hfs anomalies result from the effect of the spatial distribution of the nuclear magnetization on the atomic hfs interaction. Constructional details of the system are described: emphasis is placed on the measurement of nuclear g-factors by a triple resonance, laser state selected, ABMR method. A precision better than 10−4 for gI values has been obtained in stable atomic b…

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementThermal ionizationMass spectrometryLaserlaw.inventionBohr modelNuclear physicsMagnetizationsymbols.namesakechemistrylawCaesiumsymbolsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsDetectors and Experimental TechniquesAtomic physicsNuclear ExperimentInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Determination of the content in uranium oxide particles by fission track analysis

2004

Abstract One of the most important tasks of nuclear safeguards is to control the activities in nuclear facilities worldwide. These activities include the enrichment of 235 U . To identify enrichments above the maximum authorised level in commercial enrichment plants (usually 5% 235 U ) swipe tests are performed and the 235 U enrichment is determined in the sampled uranium oxide particles. A method is described that allows to measure the 235 U content in small particles (around 1 μm in diameter) by the use of fission tracks. It is based on the fact that in uranium fuel, only 235 U atoms are fissile with thermal neutrons and contribute to the amount of fission tracks counted for individual pa…

PhysicsNuclear and High Energy PhysicsIsotopes of uraniumFissionRadiochemistrychemistry.chemical_elementUraniumEnriched uraniumNuclear physicschemistry.chemical_compoundchemistryUranium-235Uranium oxideParticleNeutronInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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