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@ARTICLE{Young:419011,
author = {Young, Linda and Ueda, Kiyoshi and Gühr, Markus and
Bucksbaum, Philip H and Simon, Marc and Mukamel, Shaul and
Rohringer, Nina and Prince, Kevin C and Masciovecchio,
Claudio and Meyer, Michael and Rudenko, Artem and Rolles,
Daniel and Bostedt, Christoph and Fuchs, Matthias and Reis,
David A and Santra, Robin and Kapteyn, Henry and Murnane,
Margaret and Ibrahim, Heide and Légaré, François and
Vrakking, Marc and Isinger, Marcus and Kroon, David and
Gisselbrecht, Mathieu and L’Huillier, Anne and Wörner,
Hans Jakob and Leone, Stephen R},
title = {{R}oadmap of ultrafast x-ray atomic and molecular physics},
journal = {Journal of physics / B},
volume = {51},
number = {3},
issn = {0022-3700},
address = {Bristol},
publisher = {IOP Publ.},
reportid = {PUBDB-2019-00875},
pages = {032003},
year = {2018},
abstract = {X-ray free-electron lasers (XFELs) and table-top sources of
x-rays based upon high harmonic generation (HHG) have
revolutionized the field of ultrafast x-ray atomic and
molecular physics, largely due to an explosive growth in
capabilities in the past decade. XFELs now provide
unprecedented intensity (1020 W cm−2) of x-rays at
wavelengths down to ~1 Ångstrom, and HHG provides
unprecedented time resolution (~50 attoseconds) and a
correspondingly large coherent bandwidth at longer
wavelengths. For context, timescales can be referenced to
the Bohr orbital period in hydrogen atom of 150 attoseconds
and the hydrogen-molecule vibrational period of 8
femtoseconds; wavelength scales can be referenced to the
chemically significant carbon K-edge at a photon energy of
~280 eV (44 Ångstroms) and the bond length in methane of ~1
Ångstrom. With these modern x-ray sources one now has the
ability to focus on individual atoms, even when embedded in
a complex molecule, and view electronic and nuclear motion
on their intrinsic scales (attoseconds and Ångstroms).
These sources have enabled coherent diffractive imaging,
where one can image non-crystalline objects in three
dimensions on ultrafast timescales, potentially with atomic
resolution. The unprecedented intensity available with XFELs
has opened new fields of multiphoton and nonlinear x-ray
physics where behavior of matter under extreme conditions
can be explored. The unprecedented time resolution and pulse
synchronization provided by HHG sources has kindled
fundamental investigations of time delays in
photoionization, charge migration in molecules, and dynamics
near conical intersections that are foundational to AMO
physics and chemistry. This roadmap coincides with the year
when three new XFEL facilities, operating at Ångstrom
wavelengths, opened for users (European XFEL, Swiss-FEL and
PAL-FEL in Korea) almost doubling the present worldwide
number of XFELs, and documents the remarkable progress in
HHG capabilities since its discovery roughly 30 years ago,
showcasing experiments in AMO physics and other
applications. Here we capture the perspectives of 17 leading
groups and organize the contributions into four categories:
ultrafast molecular dynamics, multidimensional x-ray
spectroscopies; high-intensity x-ray phenomena; attosecond
x-ray science.},
cin = {FS-TUX / FS-CFEL-3 / Eur.XFEL},
ddc = {530},
cid = {I:(DE-H253)FS-TUX-20170422 / I:(DE-H253)FS-CFEL-3-20120731
/ $I:(DE-H253)Eur_XFEL-20120731$},
pnm = {6211 - Extreme States of Matter: From Cold Ions to Hot
Plasmas (POF3-621)},
pid = {G:(DE-HGF)POF3-6211},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000419798100001},
doi = {10.1088/1361-6455/aa9735},
url = {https://bib-pubdb1.desy.de/record/419011},
}