0000000001080987

AUTHOR

Karl Johnston

showing 16 related works from this author

Production, isolation and characterization of radiochemically pure 163Ho samples for the ECHo-project

2018

Abstract Several experiments on the study of the electron neutrino mass are based on high-statistics measurements of the energy spectrum following electron capture of the radionuclide 163Ho. They rely on the availability of large, radiochemically pure samples of 163Ho. Here, we describe the production, separation, characterization, and sample production within the Electron Capture in Holmium-163 (ECHo) project. 163Ho has been produced by thermal neutron activation of enriched, prepurified 162Er targets in the high flux reactor of the Institut Laue-Langevin, Grenoble, France, in irradiations lasting up to 54 days. Irradiated targets were chemically processed by means of extraction chromatogr…

ChromatographyChemistryEcho (computing)lanthanide separationneutron activation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010403 inorganic & nuclear chemistryIsolation (microbiology)7. Clean energy01 natural sciencesNeutrino mass determination0104 chemical sciencesCharacterization (materials science)163Ho0103 physical sciencesextraction chromatographyPhysical and Theoretical Chemistry010306 general physicsNeutron activationRadiochimica Acta
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Neodymium-140 DOTA-LM3: Evaluation of an In Vivo Generator for PET with a Non-Internalizing Vector

2017

140Nd (t1/2 = 3.4 days), owing to its short-lived positron emitting daughter 140Pr (t1/2 = 3.4 min), has promise as an in vivo generator for positron emission tomography (PET). However, the electron capture decay of 140Nd is chemically disruptive to macrocycle-based radiolabeling, meaning that an in vivo redistribution of the daughter 140Pr is expected before positron emission. The purpose of this study was to determine how the delayed positron from the de-labeled 140Pr affects preclinical imaging with 140Nd. To explore the effect, 140Nd was produced at CERN-ISOLDE, reacted with the somatostatin analogue, DOTA-LM3 (1,4,7,10- tetraazacyclododecane, 1,4,7- tri acetic acid, 10- acetamide N - p…

BiodistributionPositron emission tomographypositron emission tomographyElectron captureDOTA-LM3030218 nuclear medicine & medical imaging03 medical and health scienceschemistry.chemical_compound0302 clinical medicinePositronin vivo generatorIn vivomedicineDOTAPositron emissionOriginal Research140Prlcsh:R5-920medicine.diagnostic_test140Ndbusiness.industryChemistryGeneral MedicineinternalizationPositron emission tomography030220 oncology & carcinogenesisBiophysicsMedicineNuclear medicinebusinesslcsh:Medicine (General)Preclinical imagingInternalizationFrontiers in Medicine
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Billion-Fold Enhancement in Sensitivity of Nuclear Magnetic Resonance Spectroscopy for Magnesium Ions in Solution

2014

Beta-nuclear magnetic resonance (NMR) spectroscopy is highly sensitive compared to conventional NMR spectroscopy, and may be applied for several elements across the periodic table. Beta-NMR has previously been successfully applied in the fields of nuclear and solid-state physics. In this work, beta-NMR is applied, for the first time, to record an NMR spectrum for a species in solution. 31Mg b-NMR spectra are measured for as few as 10^7 magnesium ions in ionic liquid (EMIM-Ac) within minutes, as a prototypical test case. Resonances are observed at 3882.9 and 3887.2 kHz in an external field of 0.3 T. The key achievement of the current work is to demonstrate that beta-NMR is applicable for the…

RadioisotopesMagnetic Resonance SpectroscopyChemistryCarbon-13 NMR satelliteIonic liquid (EMIM-Ac)Analytical chemistryIonic Liquids31MgNuclear magnetic resonance spectroscopyFluorine-19 NMRNuclear magnetic resonance crystallographyCarbon-13 NMRAtomic and Molecular Physics and OpticsSolutionsnucelar magnetci resonanceSolid-state nuclear magnetic resonanceMagnesiumPräzisionsexperimente - Abteilung BlaumPhysical and Theoretical ChemistryTwo-dimensional nuclear magnetic resonance spectroscopyEarth's field NMR
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Resonant laser ionization of polonium at rilis-isolde for the study of ground- and isomer-state properties

2008

Three new ionization schemes for polonium have been tested with the resonant ionization laser ion source (RILIS) during the on-line production of 196Po in a UCx target at ISOLDE. The saturation of the atomic transitions has been observed and the yields of the isotope chain 193–198,200,202,204Po have been measured. This development provides the necessary groundwork for performing in-source resonant ionization spectroscopy on the neutron-deficient polonium isotopes (Z = 84). ispartof: Nuclear Instruments & Methods in Physics Research B vol:266 issue:19 pages:4403-4406 ispartof: location:FRANCE, Deauville status: published

PoloniumNuclear and High Energy Physicschemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural scienceslaw.inventionlawIonization0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsSpectroscopyNuclear ExperimentInstrumentationPoloniumIsotope010308 nuclear & particles physicsOptical transitionSaturationLaserIon sourcechemistryOptical transitionProduction yieldLaser ionizationAlpha decay[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Atomic physics
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High-voltage monitoring with a solenoid retarding spectrometer at the KATRIN experiment

2014

The KATRIN experiment will measure the absolute mass scale of neutrinos with a sensitivity of m(ν) = 200meV/c(2) by means of an electrostatic spectrometer set close to the tritium β-decay endpoint at 18.6keV. Fluctuations of the energy scale must be under control within ±60mV (±3ppm). Since a precise voltage measurement in the range of tens of kV is on the edge of current technology, a nuclear standard will be deployed additionally. Parallel to the main spectrometer the same retarding potential will be applied to the monitor spectrometer to measure 17.8-keV K-conversion electrons of (83m)Kr. This article describes the setup of the monitor spectrometer and presents its first measurement resu…

PhysicsRange (particle radiation)SpectrometerPhysics::Instrumentation and DetectorsMeasure (physics)High voltageSolenoidNuclear physicsDetectors and Experimental TechniquesNeutrinoInstrumentationMathematical PhysicsKATRINVoltageJournal of Instrumentation
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Measurement of the Be7(n,p) cross section at thermal energy

2019

The Be7(n,p) cross section was measured with an ion-implanted Be7 target at a thermal neutron beam of the research reactor LVR-15 in Řež. The cross section to the ground state of Li7 is σ(n,p0)=43800±1400b and the cross section to the first excited state of Li7 is σ(n,p1)=520±260b.

PhysicsNuclear reaction010308 nuclear & particles physicsbusiness.industry01 natural sciences7. Clean energyNeutron temperatureNuclear physicsCross section (physics)Excited state0103 physical sciencesResearch reactorGround statebusiness010303 astronomy & astrophysicsBeam (structure)Thermal energyPhysical Review C
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Ultra-stable implanted 83Rb/83mKr electron sources for the energy scale monitoring in the KATRIN experiment

2012

The KATRIN experiment aims at the direct model-independent determination of the average electron neutrino mass via the measurement of the endpoint region of the tritium beta decay spectrum. The electron spectrometer of the MAC-E filter type is used, requiring very high stability of the electric filtering potential. This work proves the feasibility of implanted 83Rb/83mKr calibration electron sources which will be utilised in the additional monitor spectrometer sharing the high voltage with the main spectrometer of KATRIN. The source employs conversion electrons of 83mKr which is continuously generated by 83Rb. The K-32 conversion line (kinetic energy of 17.8 keV, natural line width of 2.7 e…

PhysicsPhysics - Instrumentation and DetectorsElectron spectrometerSpectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesHigh voltageElectronInstrumentation and Detectors (physics.ins-det)Inelastic scatteringKinetic energyComputational physicsDetectors and Experimental TechniquesNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationElectron neutrinoMathematical PhysicsKATRIN
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Laser photodetachment of radioactive $^{128}$I$^−$

2017

International audience; The first experimental investigation of the electron affinity (EA) of a radioactive isotope has been conducted at the CERN-ISOLDE radioactive ion beam facility. The EA of the radioactive iodine isotope (128)I (t (1/2) = 25 min) was determined to be 3.059 052(38) eV. The experiment was conducted using the newly developed Gothenburg ANion Detector for Affinity measurements by Laser PHotodetachment (GANDALPH) apparatus, connected to a CERN-ISOLDE experimental beamline. (128)I was produced in fission induced by 1.4 GeV protons striking a thorium/tantalum foil target and then extracted as singly charged negative ions at a beam energy of 20 keV. Laser photodetachment of th…

Nuclear and High Energy PhysicsIon beamFissionPhysics::Instrumentation and Detectors[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]02 engineering and technologyPhoton energy01 natural sciences7. Clean energySecondary electronsISOLDElaw.inventionIonlawElectron affinity0103 physical scienceselectron affinityPhysics::Atomic Physics010306 general physicsNuclear ExperimentPhysicsiodinephotodetachment021001 nanoscience & nanotechnologyLaserAccelerators and Storage RingsBeamlinePhysics::Accelerator PhysicsAtomic physics0210 nano-technology
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Enhanced Quadrupole and Octupole Strength in Doubly Magic Sn132

2018

The first 2+ and 3- states of the doubly magic nucleus Sn132 are populated via safe Coulomb excitation employing the recently commissioned HIE-ISOLDE accelerator at CERN in conjunction with the highly efficient MINIBALL array. The Sn132 ions are accelerated to an energy of 5.49 MeV/nucleon and impinged on a Pb206 target. Deexciting γ rays from the low-lying excited states of the target and the projectile are recorded in coincidence with scattered particles. The reduced transition strengths are determined for the transitions 0g.s.+→21+, 0g.s.+→31-, and 21+→31- in Sn132. The results on these states provide crucial information on cross-shell configurations which are determined within large-sca…

PhysicsLarge Hadron Collider010308 nuclear & particles physicsProjectileMonte Carlo methodGeneral Physics and AstronomyCoulomb excitation01 natural sciencesIonExcited state0103 physical sciencesQuadrupoleAtomic physicsNuclear Experiment010306 general physicsNucleonPhysical Review Letters
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The upgraded ISOLDE yield database – A new tool to predict beam intensities

2020

At the CERN-ISOLDE facility a variety of radioactive ion beams are available to users of the facility. The number of extractable isotopes estimated from yield database data exceeds 1000 and is still increasing. Due to high demand and scarcity of available beam time, precise experiment planning is required. The yield database stores information about radioactive beam yields and the combination of target material and ion source needed to extract a certain beam along with their respective operating conditions. It allows to investigate the feasibility of an experiment and the estimation of required beamtime. With the increasing demand for ever more exotic beams, needs arise to extend the functi…

Radioactive ion beamsNuclear and High Energy PhysicsYieldsComputer sciencecomputer.software_genre114 Physical sciences01 natural sciencesISOLDEDatabaseFLUKACERN0103 physical sciencesddc:530Production Yield010306 general physicsInstrumentationLarge Hadron ColliderDatabase010308 nuclear & particles physicsIn-target productionYield predictionCross sectionsYield (chemistry)ABRABLAIONIZATIONRelease efficiencycomputerRadioactive beamBeam (structure)Radioactive beamsNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Evolution of Octupole Deformation in Radium Nuclei from Coulomb Excitation of Radioactive Ra222 and Ra228 Beams

2020

There is sparse direct experimental evidence that atomic nuclei can exhibit stable "pear" shapes arising from strong octupole correlations. In order to investigate the nature of octupole collectivity in radium isotopes, electric octupole (E3) matrix elements have been determined for transitions in ^{222,228}Ra nuclei using the method of sub-barrier, multistep Coulomb excitation. Beams of the radioactive radium isotopes were provided by the HIE-ISOLDE facility at CERN. The observed pattern of E3 matrix elements for different nuclear transitions is explained by describing ^{222}Ra as pear shaped with stable octupole deformation, while ^{228}Ra behaves like an octupole vibrator.

PhysicsIsotopeNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementCoulomb excitation01 natural sciencesRadiumMatrix (mathematics)chemistryExcited state0103 physical sciencesAtomic nucleusCoulombPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsDeformation (engineering)Nuclear Experiment010306 general physicsPhysical Review Letters
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β decay of In133 : γ emission from neutron-unbound states in Sn133

2019

Excited states in Sn-133 were investigated through the beta decay of In-133 at the ISOLDE facility. The ISOLDE Resonance Ionization Laser Ion Source (RILIS) provided isomer-selective ionization for In-133, allowing us to study separately, and in detail, the beta-decay branch of In-133 J(pi)= (9/2(+)) ground state and its J(pi) = (1/2(-)) isomer.Thanks to the large spin difference of the two beta-decaying states of In-133, it is possible to investigate separately the lower and higher spin states in the daughter, Sn-133, and thus to probe independently different single-particle and single-hole levels. We report here new gamma transitions observed in the decay of In-133, including those assign…

PhysicsSpin states010308 nuclear & particles physicsGamma ray01 natural sciences7. Clean energyBeta decayIon source3. Good healthIonizationExcited state0103 physical sciencesNeutronAtomic physics010306 general physicsGround statePhysical Review C
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The observation of vibrating pear-shapes in radon nuclei

2019

6 pags., 4 fig.s, 1 tab. -- Open Access funded by Creative Commons Atribution Licence 4.0

Physics beyond the Standard ModelScienceNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementRadon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesArticleGeneral Biochemistry Genetics and Molecular BiologyRadiumQuantum state0103 physical sciencesCP: violationground stateNuclear Physics - ExperimentPhysics::Atomic PhysicsExperimental nuclear physicslcsh:Science010306 general physicsnumerical calculationsNuclear ExperimentPhysicsMultidisciplinaryIsotope010308 nuclear & particles physicsnew physicsnucleusQradonGeneral ChemistryPublisher Correctionradiumexotic nucleielectric momentchemistryradioactivityMoment (physics)Atomic nucleusCP violationlcsh:QExotic atoms and moleculesAtomic physicsydinfysiikka
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Coulomb excitation of pear-shaped nuclei

2019

There is a large body of evidence that atomic nuclei can undergo octupole distortion and assume the shape of a pear. This phenomenon is important for measurements of electric-dipole moments of atoms, which would indicate CP violation and hence probe physics beyond the Standard Model of particle physics. Isotopes of both radon and radium have been identified as candidates for such measurements. Here, we have observed the low-lying quantum states in 224Rn and 226Rn by accelerating beams of these radioactive nuclei. We show that radon isotopes undergo octupole vibrations but do not possess static pear-shapes in their ground states. We conclude that radon atoms provide less favourable condition…

PhysicsIsotope010308 nuclear & particles physicsPhysicsQC1-999Physics beyond the Standard Modelchemistry.chemical_elementRadonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural scienceschemistryQuantum state0103 physical sciencesMoment (physics)Atomic nucleusCP violationNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physics010306 general physicsydinfysiikka
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The electron affinity of astatine

2020

One of the most important properties influencing the chemical behavior of an element is the electron affinity (EA). Among the remaining elements with unknown EA is astatine, where one of its isotopes, 211At, is remarkably well suited for targeted radionuclide therapy of cancer. With the At− anion being involved in many aspects of current astatine labeling protocols, the knowledge of the electron affinity of this element is of prime importance. Here we report the measured value of the EA of astatine to be 2.41578(7) eV. This result is compared to state-of-the-art relativistic quantum mechanical calculations that incorporate both the Breit and the quantum electrodynamics (QED) corrections and…

Atomic Physics (physics.atom-ph)ENERGIESGeneral Physics and AstronomyElectron01 natural sciences7. Clean energyPhysics - Atomic PhysicsElectronegativityastatiinielectron affinityPhysics::Atomic Physicslcsh:SciencePhysicsMultidisciplinary010304 chemical physicsIsotopeQELECTRONEGATIVITYMultidisciplinary SciencesHalogenScience & Technology - Other Topicsddc:500Atomic physicsBASIS-SET CONVERGENCE[CHIM.RADIO]Chemical Sciences/RadiochemistryRadioactive decayChemical physicsAstrophysics::High Energy Astrophysical PhenomenaScienceComputer Science::Neural and Evolutionary ComputationOther Fields of PhysicsPOTENTIALSFOS: Physical scienceschemistry.chemical_elementphysics.atom-phGeneral Biochemistry Genetics and Molecular BiologyArticleIonElectron affinity0103 physical sciences[CHIM]Chemical Sciences010306 general physicsAstatineDETECTORScience & TechnologySTABILITYRadiochemistry500General Chemistrychemistrylcsh:Qastatine
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First operational experience of HIE-ISOLDE

2016

The High Intensity and Energy ISOLDE project (HIE-ISOLDE)* is a major upgrade of the ISOLDE facility at CERN. The energy range of the post-accelerator will be extended from 2.85 MeV/u to 9.3 MeV/u for beams with A/q = 4.5 (and to 14.3 MeV/u for A/q = 2.5) once all the cryomodules of the superconducting accelerator are in place. The project has been divided into different phases, the first of which (phase 1a) finished in October 2015 after the hardware and beam commissioning were completed**. The physics campaign followed with the delivery of both radioactive and stable beams to two different experimental stations. The characteristics of the beams (energies, intensities, time structure and b…

kokeiludetectorexperimentdetector; dipole; ion; experiment; targetPhysics::Accelerator Physicsion04 Hadron AcceleratorsNuclear ExperimentAccelerators and Storage RingsdipoletargetAccelerator Physics
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