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@INPROCEEDINGS{Rentschler:607055,
author = {Rentschler, Christian and Matlis, Nicholas and Demirbas,
Umit and Zhang, Zhelin and Pergament, Mikhail and Zukauskas,
Andrius and Canalias, Carlota and Ishizuki, Hideki and
Pasiskevicius, Valdas and Laurell, Fredrik and Taira,
Takunori and Kärtner, Franz},
editor = {Schunemann, Peter G.},
title = {{P}arameter dependencies in multicycle {TH}z generation
with tunable high-energy pulse trains in large-aperture
crystals},
journal = {Proceedings of SPIE},
volume = {12869},
issn = {0038-7355},
address = {Bellingham, Wash.},
publisher = {SPIE},
reportid = {PUBDB-2024-01754},
isbn = {9781510669987},
pages = {44},
year = {2024},
comment = {Nonlinear Frequency Generation and Conversion: Materials
and Devices XXIII},
booktitle = {Nonlinear Frequency Generation and
Conversion: Materials and Devices
XXIII},
abstract = {Efficiencies of nonlinear optical-to-terahertz (THz)
conversion below one percent remain a limiting factor for
applications of multicycle THz radiation like THz-driven
acceleration and inspired the use of multi-line pump
spectra. To overcome the difficulty of phase stabilization
of multiple narrowband sources required by the multi-line
approach, we exploit its temporal analog, i.e., regular
pulse trains with THz repetition rate, in which the THz
waves generated by rectifying the individual pulses add
coherently. The optical setup producing the pulse trains
consists of motorized interferometers and enables precise
control over the pulse train parameters like pulse spacing
and amplitude. It is operated with a laser providing 400 fs
pulses and energies of up to 110 mJ, which is the highest
yet attempted for a pulse-train-type experiment. Opposed to
earlier work, pulse division is done after amplification
making the system more flexible in terms of tuning the pulse
number. We present initial results of an experimental
campaign of multicycle THz generation in custom periodically
poled crystals with large apertures up to 10x20 mm2. The
available pump energy allows filling these apertures at high
fluences, promising increased THz yields. We investigate the
dependence of the conversion efficiency on the single pulse
duration and aim to find the optimum pulse number for
different crystal lengths to determine the efficiency
limitations in a regime avoiding laser-induced damage. Since
crystal length and pulse number define the bandwidth of the
THz pulses, this work demonstrates a path to an optimized
THz source tunable to different requirements of
applications.},
month = {Jan},
date = {2024-01-29},
organization = {SPIE Photonics West LASE, San
Francisco (United States), 29 Jan 2024
- 31 Jan 2024},
cin = {FS-CFEL-2},
ddc = {620},
cid = {I:(DE-H253)FS-CFEL-2-20120731},
pnm = {631 - Matter – Dynamics, Mechanisms and Control
(POF4-631) / AXSIS - Frontiers in Attosecond X-ray Science:
Imaging and Spectroscopy (609920)},
pid = {G:(DE-HGF)POF4-631 / G:(EU-Grant)609920},
experiment = {EXP:(DE-H253)AXSIS-20200101},
typ = {PUB:(DE-HGF)16 / PUB:(DE-HGF)8 / PUB:(DE-HGF)7},
doi = {10.1117/12.3003195},
url = {https://bib-pubdb1.desy.de/record/607055},
}