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Explore ion trap experiments, g-factor measurements, laser spectroscopy, and mass measurements with extreme accuracy. Study collisions, surface analysis, and hollow-atom spectroscopy. Discover highly charged ions and antiprotons at low energies. Learn about electron cooling, g-factor traps, and innovative experimental setups.
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Precision Tests of Fundamental Interactions with Ion Trap Experiments Wolfgang Quint GSI Darmstadt and Univ. Heidelberg
HITRAP at the Experimental Storage Ring ESR post- decelerator stripper target UNILAC cooler Penning trap experiments with particles at rest or at low energies 400 MeV/u SIS • EXPERIMENTS WITH HIGHLY CHARGED IONS AND ANTIPROTONS AT EXTREMELY LOW ENERGIES: • g-factor measurements of the bound electron • laser spectroscopy • mass measurements of extreme accuracy • reaction microscope, collisions at very low velocities • surface studies and hollow-atom spectroscopy • x-ray spectroscopy U73+ U91+ U91+ ESR electron coolingand deceleration down to 4 MeV/u
HITRAP facility at ESR g-factortrap SPARC-EBIT Other experimental setups H1-H6 IH-structure Cooler trap Double-drift-buncher RFQ HCI from ESR 4 MeV/u 0.5 MeV/u 6 keV/u
HITRAP: Technical design to experiments matching section and cooler trap Double-drift buncher IH section RFQ section 7m
HITRAP: Inter-digital H-mode (IH) structure deceleration from 4 MeV/u to 0.5 MeV/u 4 MeV/u 0.5 MeV/u 6 keV/u
Commissioning of RFQ decelerator and of cooler trap in progress HITRAP cooler trap RFQ decelerator vertical beam line Experiments LEBT+Cooler-trap IH-structure+MEBT Double-drift-buncher RFQ
HITRAP Cooler Penning trap ● electron cooling ● resistive cooling to T = 4 K cooled HCI to HITRAP experiments highly charged ions from HITRAP decelerator extraction from cooler trap: fast (ms) or slow (ms...sec) U92+ e- e- 3
HITRAP Cooler Penning trap ● electron cooling ● resistive cooling to T = 4 K cooled HCI to HITRAP experiments highly charged ions from HITRAP decelerator extraction from cooler trap: fast (ms) or slow (ms...sec) U92+ e- e- 3
g-Factor of the bound electron in a hydrogen-like ion (nucleus has no spin, e.g. 12C5+, 16O7+, 28Si13+, 40Ca19+) Larmor precession frequency of the bound electron: Ion cyclotron frequency: B →'experimental g-factor' → comparison with theory external input parameter our measurement
Triple Penning Trap System 7mm • Precision trap (PT) • Very homogeneous magnetic field • Analysis trap (AT) • Magnetic bottle for spin detection ~14 cm • Creation trap (CT) • In-trap ion creation of • highly-charged ions
Triple Penning Trap System • Precision trap (PT) • Very homogeneous magnetic field • Analysis trap (AT) • Magnetic bottle for spin detection • Creation trap (CT) • In-trap ion creation of • highly-charged ions
g-Factor trap in Mainz (GSI/Heidelberg collaboration)
High-resolution cyclotron frequency measurement of a single highly charged silicon ion 28Si13+
HILITE: Interaction of High-Intensity Laser Radiation with Trapped Ions Multiphoton Ionization Studies Helmholtz-Institut Jena Friedrich-Schiller-Universität Jena Cooperation with Sugam Kumar and C.P. Safvan, IUAC Delhi
HILITE: Trap Electrodes virtual trap meets real trap Dec 2013
HILITE: Test of single-pass ion detector Penning trap in a dry superconducting magnet @ PHELIX, FLASH (II), JETI, POLARIS,... 1m
Precision Penning trap at HITRAP 7T superconducting magnet
Test ofreservoirtrap in an open Penningtrapwithhighlychargedargonions ArX+ ArX+ ArX+ Argon Gas Electrons Argon Gas ArX+ ArX+ ArX+ Electrons
Transport into Spectroscopy Trap Ar13+ Ar13+ Ar13+ Ar13+
Training in specific new areas, or technical expertise • ion trapping techniques • low-temperature electronics • superconducting magnets • superconducting resonance circuits for particle detection • high-sensitivity optical particle detection
SPARC Collaboration at FAIR (Stored Particles Atomic Research Collaboration) PHELIX FACILITIES SIS100 HESR APPA-Cave ESR CRYRINGHITRAP
Acknowledgements VH-NG-037 Helmholtz-Institut Jena Friedrich-Schiller-Universität Jena Thank you for your attention !