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@PHDTHESIS{Horst:348998,
author = {Horst, Max Henrik},
title = {{L}aser {S}pectroscopy of ²⁰⁸{B}i⁸²⁺ and
{C}ommissioning of the {HITRAP} {C}ooling {T}rap},
school = {TU Darmstadt},
type = {Dissertation},
address = {Darmstadt},
publisher = {ULB Darmstadt},
reportid = {GSI-2024-00459},
pages = {127},
year = {2023},
note = {Dissertation, TU Darmstadt, 2023},
abstract = {Today, quantum electrodynamics (QED) is considered the most
precisely tested theory in physics. The most precise tests
have been performed mainly on comparatively simple systems
such as the free electron. However, since QED should also be
valid in the most extreme electric and magnetic fields,
according to today’s understanding, tests must be
performed in this regime as well. Heavy and highly charged
ions are suitable for this purpose, because the remaining
electrons near the nucleus are exposed to these extreme
fields. Since such ions do not occur naturally on earth,
they must be produced artificially. This requires high
energies and, especially for the heaviest elements, large
accelerator facilities, such as the GSI Helmholtzzentrum
für Schwerionenforschung in Darmstadt, Germany. In this
work, laser spectroscopy of artificially produced
²⁰⁸Bi⁸²⁺ at relativistic energies was performed at
the storage ring ESR of GSI. This is the first time that
in-flight produced ions have been successfully studied by
laser spectroscopy in a storage ring. The main challenge is
the small amount of ions, which leads to low signal count
rates in the detectors. In part due to the data analysis
performed in this work, the measured background has been
reduced to a point where the energy difference of the
hyperfine splitting can be extracted. The obtained result is
²⁰⁸∆E⁽¹ˢ⁾ = 5598.97(1)(8) meV and represents an
important milestone for the test of QED in the strongest
magnetic fields. The accuracy of laser spectroscopy in
storage rings like the ESR is limited by the velocity
distribution of the ions. To improve the accuracy by several
orders of magnitude, ion traps can be used. However, it is
not possible to directly capture ions produced at
relativistic energies in an ion trap. Therefore, in the
second part of this work, the Cooling Trap of the HITRAP
facility was commissioned. The task of the HITRAP facility
is to decelerate the highly charged ions, to cool them and
to transport them further to the subsequent experiments. The
Cooling Trap is the final step of the deceleration process
and is responsible for the sympathetic cooling of the ions
by electrons. In this work, the Cooling Trap was
commissioned with highly charged ions and electrons from
local sources. Moreover, for the first time, ions and
electrons were simultaneously stored in the Cooling Trap.
This finally led to the first demonstration of cooling
effects of electrons on highly charged ions in a Penning
trap.},
cin = {ATP / DEC},
cid = {I:(DE-Ds200)ATP-20051214OR020 /
I:(DE-Ds200)DEC-20121002OR240},
pnm = {631 - Matter – Dynamics, Mechanisms and Control
(POF4-631)},
pid = {G:(DE-HGF)POF4-631},
experiment = {$EXP:(DE-Ds200)no_experiment-20200803$},
typ = {PUB:(DE-HGF)11},
urn = {urn:nbn:de:tuda-tuprints-263672},
doi = {10.26083/TUPRINTS-00026367},
url = {https://repository.gsi.de/record/348998},
}