0000000000117958

AUTHOR

A. Husson

showing 7 related works from this author

PIPERADE: A double Penning trap for mass separation and mass spectrometry at DESIR/SPIRAL2

2021

International audience; A double Penning trap is being commissioned at CENBG Bordeaux for the future DESIR/SPIRAL2 facility of GANIL. The setup is designed to perform both high-resolution mass separation of the ion beam for trap-assisted spectroscopy, and high-accuracy mass spectrometry of short-lived nuclides. In this paper, the technical details of the new device are described. First offline tests with the purification trap are also presented, showing a mass resolving power of about 105.

PhysicsNuclear and High Energy PhysicsSpeichertechnik - Abteilung BlaumMass spectrometryIon beamPenning trap010401 analytical chemistryMass spectrometryPenning trap01 natural sciencesMass separation0104 chemical sciencesNuclear physicsTrap (computing)0103 physical sciencesBeam purificationNew device[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclide010306 general physicsSpectroscopyInstrumentationDESIR/SPIRAL2
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Accumulation of positrons from a LINAC based source

2020

International audience; The GBAR experiment aims to measure the gravitational acceleration of antihydrogen H̅. It will use H̅+ ions formed by the interaction of antiprotons with a dense positronium cloud, which will require about 1010 positrons to produce one H̅+. We present the first results on the positron accumulation, reaching 3.8±0.4×108 e+ collected in 560 s.

010302 applied physicsPhysicsMeasure (physics)General Physics and Astronomy02 engineering and technology021001 nanoscience & nanotechnologyGravitational acceleration01 natural sciencesLinear particle acceleratorPositroniumNuclear physicsPositronPositron plasma; Positron accumulation; Antimatter; Penning-Malmberg trap; Greaves-Surko trap; GBAR[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]AntiprotonAntimatter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Accelerator PhysicsPhysics::Atomic Physics0210 nano-technologyAntihydrogenComputingMilieux_MISCELLANEOUSActa Physica Polonica A
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A pulsed high-voltage decelerator system to deliver low-energy antiprotons

2021

International audience; The GBAR (Gravitational Behavior of Antihydrogen at Rest) experiment at CERN requires efficient deceleration of 100 keV antiprotons provided by the new ELENA synchrotron ring to synthesize antihydrogen. This is accomplished using electrostatic deceleration optics and a drift tube that is designed to switch from -99 kV to ground when the antiproton bunch is inside – essentially a charged particle “elevator” – producing a 1 keV pulse. We describe the simulation, design, construction and successful testing of the decelerator device at -92 kV on-line with antiprotons from ELENA.

Nuclear and High Energy PhysicsDrift tubeGeneral RelativityIon-optic simulationsCERN Labdrift tubeAstrophysics::High Energy Astrophysical Phenomena[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Charged-particle opticsfabrication7. Clean energy01 natural sciencesanti-p: decelerationlaw.inventionNuclear physicslaw0103 physical sciencessynchrotronPhysics::Atomic Physics010306 general physicsAntihydrogennumerical calculationsInstrumentationaccelerator: designPhysicsantihydrogenLarge Hadron Collider010308 nuclear & particles physicsHigh voltageCharged particleSynchrotron[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Pulse (physics)beam opticsAntiprotonPhysics::Accelerator Physics
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Towards a test of the weak equivalence principle of gravity using anti-hydrogen at CERN

2016

International audience; The aim of the GBAR (Gravitational Behavior of Antimatter at Rest) experiment is to measure the free fall acceleration of an antihydrogen atom, in the terrestrial gravitational field at CERN and therefore test the Weak Equivalence Principle with antimatter. The aim is to measure the local gravity with a 1% uncertainty which can be reduced to few parts of 10-3.

Free fallGravity (chemistry)Particle physicsPhysics::General PhysicsAntimatterCERN LabGravityacceleration measurementterrestrial gravitational fieldfree fall acceleration01 natural sciencesantihydrogen: accelerationweak equivalence principle010305 fluids & plasmasparticle trapsAtomic measurementsGravitationGeneral Relativity and Quantum Cosmologyhydrogen: ionGravitational fieldLaser transitionsAtom (measure theory)0103 physical sciencesPhysics::Atomic and Molecular Clusters[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsAntihydrogenantihydrogen atomPhysicsIonsatomProductionEquivalence principle (geometric)laserequivalence principleAntimatter[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc]talk: Ottawa 2016/07/10gravitation: localhydrogen ionsCoolingGravitation
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Positron production using a 9 MeV electron linac for the GBAR experiment

2020

For the GBAR (Gravitational Behaviour of Antihydrogen at Rest) experiment at CERN's Antiproton Decelerator (AD) facility we have constructed a source of slow positrons, which uses a low-energy electron linear accelerator (linac). The driver linac produces electrons of 9 MeV kinetic energy that create positrons from bremsstrahlung-induced pair production. Staying below 10 MeV ensures no persistent radioactive activation in the target zone and that the radiation level outside the biological shield is safe for public access. An annealed tungsten-mesh assembly placed directly behind the target acts as a positron moderator. The system produces $5\times10^7$ slow positrons per second, a performan…

safetyAntimatterNuclear and High Energy PhysicsCERN LabPhysics - Instrumentation and DetectorstungstenPositronAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesElectron01 natural sciences7. Clean energyLinear particle acceleratorpositron: particle source010305 fluids & plasmaselectron: pair productionNuclear physicselectron: linear acceleratorPositronPositron; Linear accelerator; Antimatter; Antihydrogen; Gravitation0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental TechniquesNuclear Experiment010306 general physicsAntihydrogenphysics.ins-detInstrumentationenergy: lowantihydrogenPhysicsLarge Hadron Collidergravitation 2Instrumentation and Detectors (physics.ins-det)linear acceleratorAntiproton DeceleratorPair productionradioactivityAntimattergravitation: accelerationPhysics::Accelerator PhysicsHigh Energy Physics::Experimentperformancepositron: yieldGravitationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Odd-odd neutron-rich rhodium isotopes studied with the double Penning trap JYFLTRAP

2022

Precision mass measurements of neutron-rich rhodium isotopes have been performed at the JYFLTRAP Penning trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility. We report results on ground- and isomeric-state masses in $^{110,112,114,116,118}$Rh and the very first mass measurement of $^{120}$Rh. The isomeric states were separated and measured for the first time using the phase-imaging ion-cyclotron-resonance (PI-ICR) technique. For $^{112}$Rh, we also report new half-lives for both the ground state and the isomer. The results are compared to theoretical predictions using the BSkG1 mass model and discussed in terms of triaxial deformation.

Nuclear Theory (nucl-th)isotoopitmassaspektrometriaNuclear TheoryFOS: Physical sciencesNuclear Experiment (nucl-ex)ydinfysiikkaNuclear Experiment
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Development of a PbWO 4 detector for single-shot positron annihilation lifetime spectroscopy at the GBAR experiment

2020

International audience; We have developed a PbWO 4 (PWO) detector with a large dynamic range to measure the intensity of a positron beam and the absolute density of the ortho-positronium (o-Ps) cloud it creates. A simulation study shows that a setup based on such detectors may be used to determine the angular distribution of the emission and reflection of o-Ps to reduce part of the uncertainties of the measurement. These will allow to improve the precision in the measurement of the cross section for the (anti) hydrogen formation by (anti) proton-positronium charge exchange and to optimize the yield of antihydrogen ion which is an essential parameter in the GBAR experiment.

PhysicsPhysics::Instrumentation and Detectors[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]DetectorMeasure (physics)General Physics and Astronomy7. Clean energyIonNuclear physicsCross section (physics)[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]PACS: 78.70.Bj 41.75.Fr 36.10.DrYield (chemistry)Reflection (physics)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]AntihydrogenSpectroscopyComputingMilieux_MISCELLANEOUS
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