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@INPROCEEDINGS{Schoenberg:642943,
author = {Schoenberg, Arthur and Biesterfeld, Peer and Seitz, Marc
and Jimenez De la vega, Nayla Esmeralda and Lang, Tino and
Seidel, Marcus and Balla, Prannay and Winkelmann, Lutz and
Froehlich, Sven and Mosel, Philip and Hartl, Ingmar and
Calegari, Francesca and Morgner, Uwe and Kovacev, Milutin
and Heyl, Christoph and Trabattoni, Andrea},
title = {{P}ost-{C}ompression of a {Q}-switched laser in a
{M}ulti-{P}ass {C}ell},
address = {[Washington, D.C., USA]},
publisher = {OSA},
reportid = {PUBDB-2025-05733},
isbn = {979-8-3315-1252-1},
series = {Technical digest series / Optica Publishing Group},
pages = {1},
year = {2025},
note = {"1001 papers in 162 sessions" - Einstigsseite der Ressource
(Stand: 19.09.2025); "Co-located meetings: European Quantum
Electronics Conference" - Einstigsseite der Ressource;
Literaturangaben;},
comment = {[Ebook] The European Conference on Lasers and
Electro-Optics : part of 2025 Conference on Lasers and
Electro-Optics Europe and European Quantum Electronics
Conference : 23-27 June 2025, Munich, Germany / Optica ,
[Washington, D.C., USA] : OSA, [2025],},
booktitle = {[Ebook] The European Conference on
Lasers and Electro-Optics : part of
2025 Conference on Lasers and
Electro-Optics Europe and European
Quantum Electronics Conference : 23-27
June 2025, Munich, Germany / Optica ,
[Washington, D.C., USA] : OSA, [2025],},
abstract = {The two most notable methods for producing short laser
pulses are mode-locked and Q-switched lasers.
Whilemode-locked lasers generate pulses in the pico- (ps) to
femtosecond (fs) range, Q-switched lasers typically
producepulses at the nanosecond (ns) or 100 ps level [1].
Thus, mode-locking has been the superior technology
whenultrashort pulses or high peak powers are required. On
the other hand, Q-switched lasers can have great
advantagesowing to their simplicity, compactness, low costs,
and the large pulse energies that can be generated [2]. To
bridgethe parameter gap between mode-locked and Q-switched
lasers, pulse post-compression appears attractive.
Onepossible method is self-phase-modulation (SPM) in optical
fibers [3]. However, stimulated-Raman-scattering limitsthe
possible peak powers to far below 1 kW and thus pulse
energies to lower than μJ level for ns pulses [3].
AnotherSPM-based method are Multi-pass cells (MPCs), which
have become a standard technology for post-compressionof
mode-locked lasers [4]. However, MPCs have not yet been used
to compress Q-switched laser pulses due to theirinherently
low peak powers. Here, we demonstrate a new MPC type,
facilitating post-compression of pulses
withorder-of-magnitude lower peak power than typical
bulk-MPCs [4]. We use a fused silica block as the
nonlinearmedium and compress 1 mJ pulses from the nanosecond
down to the picosecond regime.},
month = {Jun},
date = {2025-06-23},
organization = {The European Conference on Lasers and
Electro-Optics, München (Germany), 23
Jun 2025 - 27 Jun 2025},
cin = {FS-PRI / FS-LA / FS-ATTO},
cid = {I:(DE-H253)FS-PRI-20240109 / I:(DE-H253)FS-LA-20130416 /
I:(DE-H253)FS-ATTO-20170403},
pnm = {631 - Matter – Dynamics, Mechanisms and Control
(POF4-631) / HIRS-0018 - Helmholtz-Lund International School
- Intelligent instrumentation for exploring matter at
different time and length scales (HELIOS)
$(2020_HIRS-0018)$},
pid = {G:(DE-HGF)POF4-631 / $G:(DE-HGF)2020_HIRS-0018$},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)8 / PUB:(DE-HGF)7},
url = {https://bib-pubdb1.desy.de/record/642943},
}