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@ARTICLE{Linker:632800,
author = {Linker, Thomas M. and Halavanau, Aliaksei and Kroll, Thomas
and Benediktovitch, Andrei and Zhang, Yu and Michine, Yurina
and Chuchurka, Stasis and Abhari, Zain and Ronchetti,
Daniele and Fransson, Thomas and Weninger, Clemens and
Fuller, Franklin D. and Aquila, Andy and Alonso-Mori,
Roberto and Boutet, Sebastien and Guetg, Marc W. and
Marinelli, Agostino and Lutman, Alberto A. and Yabashi,
Makina and Inoue, Ichiro and Osaka, Taito and Yamada, Jumpei
and Inubushi, Yuichi and Yamaguchi, Gota and Hara, Toru and
Babu, Ganguli and Salpekar, Devashish and Sayed, Farheen N.
and Ajayan, Pulickel M. and Kern, Jan and Yano, Junko and
Yachandra, Vittal K. and Kling, Matthias F. and Pellegrini,
Claudio and Yoneda, Hitoki and Rohringer, Nina and Bergmann,
Uwe},
title = {{A}ttosecond {I}nner-{S}hell {L}asing at {A}ngstrom
{W}avelengths},
reportid = {PUBDB-2025-02225, arXiv:2409.06914},
year = {2025},
abstract = {Since the invention of the laser nonlinear effects such as
filamentation, Rabi-cycling and collective emission have
been explored in the optical regime leading to a wide range
of scientific and industrial applications. X-ray free
electron lasers (XFELs) have led to the extension of many
optical techniques to X-rays for their advantages of
angstrom scale spatial resolution and elemental specificity.
One such example is XFEL driven population inversion of 1s
core hole states resulting in inner-shell K$α$ (2p to 1s)
X-ray lasing in elements ranging from neon to copper, which
has been utilized for nonlinear spectroscopy and development
of next generation X-ray laser sources. Here we show that
strong lasing effects, similar to those observed in the
optical regime, can occur at 1.5 to 2.1 angstrom wavelengths
during high intensity (> ${10^{19}}$ W/cm${^{2}}$) XFEL
driven inner-shell lasing and superfluorescence of copper
and manganese. Depending on the temporal substructure of the
XFEL pump pulses(containing ${~10^{6}}$ - ${10^{8}}$
photons) i, the resulting inner-shell X-ray laser pulses can
exhibit strong spatial inhomogeneities as well as spectral
splitting, inhomogeneities and broadening. Through 3D
Maxwell Bloch theory we show that the observed spatial
inhomogeneities result from X-ray filamentation, and that
the spectral splitting and broadening is driven by Rabi
cycling with sub-femtosecond periods. Our simulations
indicate that these X-ray pulses can have pulse lengths of
less than 100 attoseconds and coherence properties that open
the door for quantum X-ray optics applications.},
cin = {FS-TUX},
cid = {I:(DE-H253)FS-TUX-20170422},
pnm = {631 - Matter – Dynamics, Mechanisms and Control
(POF4-631) / AIM, DFG project G:(GEPRIS)390715994 - EXC
2056: CUI: Advanced Imaging of Matter (390715994) /
HIDSS-0002 - DASHH: Data Science in Hamburg - Helmholtz
Graduate School for the Structure of Matter
$(2019_IVF-HIDSS-0002)$},
pid = {G:(DE-HGF)POF4-631 / G:(GEPRIS)390715994 /
$G:(DE-HGF)2019_IVF-HIDSS-0002$},
experiment = {EXP:(DE-MLZ)External-20140101 /
EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)25},
eprint = {2409.06914},
howpublished = {arXiv:2409.06914},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2409.06914;\%\%$},
doi = {10.3204/PUBDB-2025-02225},
url = {https://bib-pubdb1.desy.de/record/632800},
}