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@MASTERSTHESIS{Kilinc:607009,
author = {Kilinc, Muharrem and Kärtner, Franz},
othercontributors = {Pergament, Mikhail},
title = {{T}hermal and optical characterization of cryogenically
cooled {Y}b:{YLF} laser},
school = {University of Hamburg},
type = {Masterarbeit},
reportid = {PUBDB-2024-01714},
pages = {93},
year = {2024},
note = {Masterarbeit, University of Hamburg, 2024},
abstract = {This thesis focuses on two fundamental limitations that
affect the power scaling of cryogenically cooled high-power
solid-state lasers: (i) Fractional thermal load (FTL) and
(ii) Thermal and population lensing. For FTL, a novel method
is introduced for the direct measurement of fractional
thermal load in cryogenically cooled laser crystals. The
experimental methodology involves characterizing the liquid
nitrogen evaporation rate in a dewar containing the laser
crystal, which allows the accurate determination of FTL. The
FTL is measured to be 1.7 × quantum defect (QD) for Yb:YLF
and 1.5 × QD for Yb:YAG under continuous wave lasing
conditions. The measured FTL values are then used to
calculate the temperature distribution inside the crystals
as a function of pump power, and the simulation results are
found to be in a very good agreement with the in-situ
temperature measurements using contactless optical
luminescence thermometry. For thermal and population
lensing, this thesis conducts the first detailed study of
thermal and population lensing in cryogenically cooled
Yb:YLF. Using a rod-shaped a-cut Yb:YLF crystal, the thermal
lens strength is measured as a function of absorbed pump
power for both E//a and E//c polarizations for pump power
levels up to 600 W. Our experiments clarified that the
thermal lensing behavior in Yb:YLF is quite asymmetric. For
the E//a polarization, the thermal lens is rather strong and
always converging for both horizontal and vertical axes. For
the E//c configuration, thermal lensing is rather weak, and
its sign could be different in different axes, and
furthermore, the sign of thermal lensing is observed to be
dependent on the absorbed pump power level. Simulations and
detailed experimental measurements show that the observed
peculiar behavior is a result of competition between the
positive photo-elastic effect and negative thermo-optic
effect: as their relative strength varies at different pump
power levels. We have also measured the contribution of
surface bulging into thermal lensing and found it to be
relatively small in our crystals with un-doped end-caps.
Lastly, the population lensing is measured in Yb:YLF for the
first time, and it is found to be quite weak as well, and
the polarizability difference parameter of Yb:YLF is
determined as (3 ± 1.5) × 10−34 m3.},
cin = {FS-CFEL-2},
cid = {I:(DE-H253)FS-CFEL-2-20120731},
pnm = {631 - Matter – Dynamics, Mechanisms and Control
(POF4-631)},
pid = {G:(DE-HGF)POF4-631},
experiment = {EXP:(DE-H253)AXSIS-20200101},
typ = {PUB:(DE-HGF)19},
doi = {10.13140/RG.2.2.20360.43521},
url = {https://bib-pubdb1.desy.de/record/607009},
}