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@ARTICLE{Vogel:217204,
author = {Vogel, Manuel and Ebrahimi, Mohammad Sadegh and Guo, Zhexi
and Khodaparast, Anahita and Birkl, Gerhard and Quint,
Wolfgang},
title = {{E}lectron {M}agnetic {M}oment in {H}ighly {C}harged
{I}ons: {T}he {ARTEMIS} {E}xperiment},
journal = {Annalen der Physik},
volume = {2018},
issn = {0003-3804},
address = {Berlin},
publisher = {Wiley-VCH},
reportid = {GSI-2018-01053},
pages = {1800211},
year = {2018},
note = {open without ccby},
abstract = {The magnetic moment (g-factor) of the electron is a
fundamental quantity in physics that can be measured with
high accuracy by spectroscopy in Penning traps. Its value
has been predicted by theory, both for the case of the free
(unbound) electron and for the electron bound in a highly
charged ion.Precision measurements of the electron magnetic
moment yield a stringent test of these predictions and can
in turn be used for a determination of fundamental constants
such as the fine structure constant or the atomic mass of
the electron. For the bound-electron magnetic-moment
measurement, two complementary approaches exist, one via the
so-called “continuous Stern–Gerlach effect”, applied
to ions with zero-spin nuclei, and one a spectroscopic
approach, applied to ions with nonzero nuclear spin. Here,
the latter approach is detailed, and an overview of the
experiment and its status is given.},
cin = {ATP},
ddc = {530},
cid = {I:(DE-Ds200)ATP-20051214OR020},
pnm = {6211 - Extreme States of Matter: From Cold Ions to Hot
Plasmas (POF3-621)},
pid = {G:(DE-HGF)POF3-6211},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000471993700001},
doi = {10.1002/andp.201800211},
url = {https://repository.gsi.de/record/217204},
}