Search results for "Electron cooling"

showing 10 items of 23 documents

Centrifugal Separation of Antiprotons and Electrons

2010

Centrifugal separation of antiprotons and electrons is observed, the first such demonstration with particles that cannot be laser cooled or optically imaged. The spatial separation takes place during the electron cooling of trapped antiprotons, the only method available to produce cryogenic antiprotons for precision tests of fundamental symmetries and for cold antihydrogen studies. The centrifugal separation suggests a new approach for isolating low energy antiprotons and for producing a controlled mixture of antiprotons and electrons.

PhysicsAntiparticleGeneral Physics and AstronomyPlasmaElectronJlaw.inventionNuclear physicsAntiprotonlawAntimatterddc:550Physics::Accelerator PhysicsHigh Energy Physics::ExperimentPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentAntihydrogenLeptonElectron coolingPhysical Review Letters
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Adiabatic Cooling of Antiprotons

2011

Adiabatic cooling is shown to be a simple and effective method to cool many charged particles in a trap to very low temperatures. Up to 3 x 10(6) (p) over bar are cooled to 3.5 K-10(3) times more cold (p) over bar and a 3 times lower (p) over bar temperature than previously reported. A second cooling method cools (p) over bar plasmas via the synchrotron radiation of embedded (p) over bar (with many fewer (p) over bar than (p) over bar) in preparation for adiabatic cooling. No (p) over bar are lost during either process-a significant advantage for rare particles.

PhysicsHigh Energy Physics::PhenomenologyBremsstrahlungGeneral Physics and AstronomySynchrotron radiationElectronAtmospheric temperature rangeCharged particlelaw.inventionJlawAntiprotonddc:550High Energy Physics::ExperimentPhysics::Atomic PhysicsAtomic physicsAdiabatic processElectron cooling
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HITRAP – a facility for experiments on heavy highly charged ions and on antiprotons

2009

HITRAP is a facility for very slow highly-charged heavy ions at GSI. HITRAP uses the GSI relativistic ion beams, the Experimental Storage Ring ESR for electron cooling and deceleration to 4 MeV/u, and consists of a combination of an interdigital H-mode (IH) structure with a radiofrequency quadrupole structure for further deceleration to 6 keV/u, and a Penning trap for accumulation and cooling to low temperatures. Finally, ion beams with low emittance will be delivered to a large variety of atomic and nuclear physics experiments. Presently, HITRAP is in the commissioning phase. The deceleration of heavy-ion beam from the ESR storage ring to an energy of 500 keV/u with the IH structure has be…

PhysicsHistoryLow emittancePenning trapComputer Science ApplicationsEducationIonlaw.inventionNuclear physicslawAntiprotonQuadrupolePhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentBeam (structure)Storage ringElectron coolingJournal of Physics: Conference Series
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The polarized electron-nucleon collider project ENC at GSI/FAIR

2011

The ENC project attempts to realize an electron-nucleon collider at the upcoming Facility for Antiproton and Ion Research FAIR at GSI Darmstadt by utilizing the antiproton high-energy storage ring HESR for polarized proton and deuteron beams. The addition of a 3.3 GeV storage ring for polarized electrons will enable electron-nucleon collisions up to a center-of-mass energy of - s - 14 GeV. In such a configuration peak luminosities in the range of L = 10(32) to 10(33)cm(-')(2)s(-')(1) are feasible . Beam-beam effects in a space-charge dominated regimes in conjunction with high-energy electron cooling represents one of the main challenges for this project. In this paper beam- and spin dynamic…

PhysicsHistoryParticle physicsProtonElectronComputer Science ApplicationsEducationlaw.inventionNuclear physicslawAntiprotonFacility for Antiproton and Ion ResearchPhysics::Accelerator PhysicsHigh Energy Physics::Experimentddc:530NucleonColliderNuclear ExperimentStorage ringElectron cooling
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Laser cooling of stored relativistic ion beams with large momentum spreads using a laser system with a wide scanning range

2014

New results on laser cooling of stored, bunched, relativistic ion beams are presented. For the first time it has been possible to cool an ion beam with large momentum spread without initial electron cooling or scanning of the bunching frequency by using a single cw laser system.

PhysicsHistoryRange (particle radiation)Ion beamResolved sideband coolingbusiness.industryLaserComputer Science ApplicationsEducationIonlaw.inventionMomentumOpticslawLaser coolingPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsbusinessElectron coolingJournal of Physics: Conference Series
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Measurement of the transverse Doppler shift using a stored relativistic7Li+ ion beam

1992

We have performed for the first time precision spectroscopy on a coasting fast7Li+ ion beam in a storage ring. The ion beam moving with 6.4% speed of light was first electron cooled and then merged with two counterpropagating laser beams acting on two different hyperfine transitions sharing a common upper level (λ-system). One laser was frequency locked to thea 3 127J2 hfs frequency component established as a secondary frequency standard at 514 nm. The second laser was tuned over theλ-resonance, which was recorded relative to127J2 hfs components. This experiment is sensitive to the time dilation in fast moving frames and will lead to new limits for the verification of special relatively. Th…

PhysicsNuclear and High Energy PhysicsDye laserSecondary frequency standardIon beambusiness.industryLaserElectromagnetic radiationlaw.inventionsymbols.namesakeOpticslawsymbolsPhysics::Atomic PhysicsAtomic physicsbusinessDoppler effectStorage ringElectron coolingZeitschrift f�r Physik A Hadrons and Nuclei
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New results with stored exotic nuclei at relativistic energies

2004

Recently, much progress has been made with stored exotic nuclei at relativistic velocities ( v c = 0.7 ) . Fragments of 208Pb and 209Bi projectiles and fission products from 238U ions were produced, separated in flight with the fragment separator FRS, and injected into the storage-cooler ring ESR for precision measurements. 114 new masses of neutron-deficient isotopes in the lead region have been measured with time-resolved Schottky Mass Spectrometry (SMS). A new isospin dependence of the pairing energy was observed due to the improved mass accuracy of typically 1.5×10-7 (30 keV). New masses of short-lived neutron-rich fission fragments have been obtained with Isochronous Mass Spectrometry …

PhysicsNuclear and High Energy PhysicsFission productsIsotopeFissionNuclear TheoryMass spectrometrylaw.inventionIonNuclear physicslawIsospinAtomic physicsNuclear ExperimentSpectroscopyElectron coolingNuclear Physics A
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Ion beam preparation of 7Li+ for precision experiments at heavy ion storage rings

1997

Abstract Heavy ion storage rings allow for tests of the structure of local space time via the Doppler effect. At the TSR/Heidelberg an experiment with high resolution laser spectroscopy at 7 Li + is performed. To gain the maximum resolution for saturation spectroscopy new methods of relativistic ion beam preparation and diagnostics have been developed. The laser cooling of the beam allows for precision determination of the mean velocity of the ions. A novel phase synchronous detection scheme, ultimately sensitive to single ions, gives insights into the cooling mechanism and dynamics. With an additional synchronous excitation scheme systematic uncertainties of the test experiment can be dras…

PhysicsNuclear and High Energy PhysicsIon beam depositionResolved sideband coolingIon beamlawLaser coolingAtomic physicsIon gunLaserElectron coolinglaw.inventionIonNuclear Physics A
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Electron and positron cooling of highly charged ions in a cooler Penning trap

2004

Abstract Electron cooling is a well-established technique to increase the phase space density of particle beams in storage rings. In this paper, we discuss the feasibility of electron and positron cooling of ions in a Penning trap. We calculate the cooling times for the cases of trapped bare ions with nuclear charge Z =1 (protons), Z =36 (krypton) and Z =92 (uranium) with the Spitzer formula. Our calculations show that for typical experimental conditions the time for cooling from initial energies of 10 keV per charge down to rest is in the order of a second. We investigate the dependence of the cooling time on the number of ions and electrons, and their charge and mass.

PhysicsNuclear and High Energy PhysicsKryptonchemistry.chemical_elementElectronPenning trapEffective nuclear chargelaw.inventionIonPositronchemistrylawLaser coolingPhysics::Atomic PhysicsAtomic physicsInstrumentationElectron coolingNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Performance of cryogenic microbolometers and calorimeters with on-chip coolers

2000

Astronomical observations of cosmic sources in the far-infrared and X-ray bands require extreme sensitivity. The most sensitive detectors are cryogenic bolometers and calorimeters operating typically at about 100 mK. The last stage of cooling (from 300 mK to 100 mK) often poses significant difficulties in space-borne experiments, both in system complexity and reliability. We address the possibility of using refrigeration based on normal metal/insulator/superconductor (NIS) tunnel junctions as the last stage cooler for cryogenic thermal detectors. We compare two possible schemes: the direct cooling of the electron gas of the detector with the aid of NIS tunnel junctions and the indirect cool…

PhysicsSuperconductivityCondensed Matter - Mesoscale and Nanoscale PhysicsPhysics and Astronomy (miscellaneous)business.industryPhysics::Instrumentation and DetectorsDetectorBolometerRefrigerationFOS: Physical sciencesInsulator (electricity)law.inventionlawCondensed Matter::SuperconductivityMesoscale and Nanoscale Physics (cond-mat.mes-hall)OptoelectronicsbusinessNoise-equivalent powerOrder of magnitudeElectron cooling
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