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@PHDTHESIS{Ritzkowsky:597811,
author = {Ritzkowsky, Felix},
othercontributors = {Kärtner, Franz and Küpper, Jochen},
title = {{E}lectronics at {O}ptical {F}requencies},
school = {Universität Hamburg},
type = {Dissertation},
address = {Hamburg},
publisher = {Verlag Deutsches-Elektronen Synchrotron},
reportid = {PUBDB-2023-06679, DESY-THESIS-2023-018},
series = {DESY-THESIS},
pages = {146},
year = {2023},
note = {Dissertation, Universität Hamburg, 2023},
abstract = {With the advent of ultrafast optics and controllable
waveforms consisting of only a few oscillations of the
electric field, the idea of controlling electrons at the
frequency of light was born. This established the potential
of using a controlled optical waveform to switch electronic
circuit elements at the frequency of an optical wave,
typically on the order of 0.1 to 1 petahertz(1015 Hz). This
exceeds the frequency of the fastest electronic devices by
two to three orders of magnitude and the clock rates of
modern computers by up to six orders of magnitude. Tothis
end, many pioneering experiments have shown that optical
waveforms can be used to drive attosecond electron currents
at metal-vacuum interfaces, in dielectric large bandgap
materials or in air. This thesis shows how integrated
metallic nanoantennas are utilized to enhance the electric
field of optical few-cycle pulses in nanometer-sized
hotspots, generating sub-cycle field emission with only
picojoule-level pulse energies. Exploiting the
attosecond-fast currents on the nanoscale, petahertz
bandwidth field sampling with 5 femtojoule sensitivity is
experimentally demonstrated [20]. The influence of antenna
symmetry and device design on the sampling frequency
response is investigated theoretically to guide application
specific design strategies [21]. To further test the
integrated nanoantenna platform, we have developed a
passively CEP-stable sub-2-cycle laser source that produces
16 fs duration pulsesat a central wavelength of 2.7 µm with
> 84 nJ energy at a repetition rate of 50 kHz. The system is
based on adiabatic difference generation [22], and
significantly simplifies previous implementations by relying
solely on material-based compression. Furthermore, the CEP
stability of adiabatic difference generation is measured for
the first time and shows excellent passive stability of 190
mrad rms. We show that by using the newly developed
mid-infrared sub-2-cycle source, the CEP dependent yield of
a single nanoantenna is significantly improved by a factor
of 30 from a previous 0.1 electrons per laser shot to > 3
electrons [10, 23]. Thanks to this significant improvement,
and by illuminating up to 1000 antennas, we produce fully
carrier-envelope phase (CEP) dependent currents of up to
3000 electrons per shot, improving previous results by three
orders of magnitude [23]. The results of this work will open
many interesting avenues for the exploration of optical
frequency electronics based on integrated nanoantennas, such
as ultra-broadband time spectroscopy in the infrared
continuously covering the terahertz to visible spectrum, or
petahertz bandwidth logic circuits.},
cin = {FS-CFEL-2},
cid = {I:(DE-H253)FS-CFEL-2-20120731},
pnm = {631 - Matter – Dynamics, Mechanisms and Control
(POF4-631) / DFG project 453615464 - Dielektrischer
Laserbeschleuniger im mittleren Infrarotbereich (453615464)
/ DFG project 390715994 - EXC 2056: CUI: Advanced Imaging of
Matter (390715994)},
pid = {G:(DE-HGF)POF4-631 / G:(GEPRIS)453615464 /
G:(GEPRIS)390715994},
experiment = {EXP:(DE-H253)AXSIS-20200101},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
doi = {10.3204/PUBDB-2023-06679},
url = {https://bib-pubdb1.desy.de/record/597811},
}