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@ARTICLE{Engel:449355,
author = {Engel, Robin and Miedema, Piter S. and Turenne, Diego and
Vaskivskyi, Igor and Brenner, Günter and Dziarzhytski,
Siarhei and Kuhlmann, Marion and Schunck, Jan O. and
Döring, Florian and Styervoyedov, Andriy and Parkin, Stuart
S. P. and David, Christian and Schuessler-Langeheine,
Christian and Duerr, Hermann and Beye, Martin},
title = {{P}arallel {B}roadband {F}emtosecond {R}eflection
{S}pectroscopy at a {S}oft {X}-{R}ay {F}ree-{E}lectron
{L}aser},
journal = {Applied Sciences},
volume = {10},
number = {19},
issn = {2076-3417},
address = {Basel},
publisher = {MDPI},
reportid = {PUBDB-2020-03739},
pages = {6947},
year = {2020},
abstract = {X-ray absorption spectroscopy (XAS) and the directly linked
X-ray reflectivity near absorption edges yield a wealth of
specific information on the electronic structure around the
resonantly addressed element. Observing the dynamic response
of complex materials to optical excitations in pump–probe
experiments requires high sensitivity to small changes in
the spectra which in turn necessitates the brilliance of
free electron laser (FEL) pulses. However, due to the
fluctuating spectral content of pulses generated by
self-amplified spontaneous emission (SASE), FEL experiments
often struggle to reach the full sensitivity and
time-resolution that FELs can in principle enable. Here, we
implement a setup which solves two common challenges in this
type of spectroscopy using FELs: First, we achieve a high
spectral resolution by using a spectrometer downstream of
the sample instead of a monochromator upstream of the
sample. Thus, the full FEL bandwidth contributes to the
measurement at the same time, and the FEL pulse duration is
not elongated by a monochromator. Second, the FEL beam is
divided into identical copies by a transmission grating beam
splitter so that two spectra from separate spots on the
sample (or from the sample and known reference) can be
recorded in-parallel with the same spectrometer, enabling a
spectrally resolved intensity normalization of pulse
fluctuations in pump–probe scenarios. We analyze the
capabilities of this setup around the oxygen K- and nickel
L-edges recorded with third harmonic radiation of the free
electron laser in Hamburg (FLASH), demonstrating the
capability for pump–probe measurements with sensitivity to
reflectivity changes on the per mill level.},
cin = {FS-FLASH / DOOR ; HAS-User / FS-FLASH-B / FS-FLASH-O},
ddc = {600},
cid = {I:(DE-H253)FS-FLASH-20140814 / I:(DE-H253)HAS-User-20120731
/ I:(DE-H253)FS-FLASH-B-20160930 /
I:(DE-H253)FS-FLASH-O-20160930},
pnm = {6211 - Extreme States of Matter: From Cold Ions to Hot
Plasmas (POF3-621) / 6G2 - FLASH (POF3-622) / FS-Proposal:
F-20180568 (F-20180568) / VH-NG-1105 - Novel soft X-ray
spectroscopies for materials science
$(2016_IVF-VH-NG-1105)$},
pid = {G:(DE-HGF)POF3-6211 / G:(DE-HGF)POF3-6G2 /
G:(DE-H253)F-20180568 / $G:(DE-HGF)2016_IVF-VH-NG-1105$},
experiment = {EXP:(DE-H253)F-FL24-20150901},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000587186100001},
doi = {10.3390/app10196947},
url = {https://bib-pubdb1.desy.de/record/449355},
}