% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@PHDTHESIS{Stehr:630593,
author = {Stehr, Felix Paul Georg},
othercontributors = {List, Jenny and Moortgat-Pick, Gudrid},
title = {{T}owards {S}pin-{P}olarized {E}lectron {B}eams from a
{L}aser-{P}lasma {A}ccelerator},
school = {University of Hamburg},
type = {Dissertation},
address = {Hamburg},
publisher = {Staats- und Universitätsbibliothek Hamburg Carl von
Ossietzky},
reportid = {PUBDB-2025-01873},
pages = {227},
year = {2025},
note = {Dissertation, University of Hamburg, 2025},
abstract = {The LEAP (Laser Electron Acceleration with Polarization)
project at DESY is a proof-of-principle experiment aiming to
demonstrate the generation -- thus also the transport -- of
spin-polarized electron beams from a laser-plasma
accelerator (LPA). This is expected to be achieved using a
pre-polarized plasma source, generated via the
photodissociation of HCl molecules with an ultraviolet (UV)
dissociation laser. Compton transmission polarimetry is
envisioned for polarization measurements, inferring electron
polarization from the transmission asymmetry of
bremsstrahlung photons through magnetized iron. This thesis
explores three key aspects of LEAP, focusing on development
an experimental realization. First, a feasibility study was
conducted to generate the UV dissociation laser via cascaded
second-harmonic generation in two beta-barium borate
crystals directly from the LPA driver laser. A measured
conversion efficiency of $\eta_{\omega \rightarrow
4\omega}\approx0.8\,\\%$ into the UV demonstrates the
feasibility of this approach. Second, a homogeneous
Cherenkov lead-glass calorimeter was built as an integral
part of the LEAP Compton transmission polarimeter.
Furthermore, it was tested and calibrated with single
electrons at the DESYII Test Beam Facility. The derived
calorimeter energy resolution of $\frac{\sigma_{E}}{\langle
E \rangle} < 2\,\\%$ at TeV-scale total energies meets the
requirement for its application within the LEAP polarimeter.
GEANT4 simulations indicate a nonlinear calorimeter response
to low-energy particles ($<10\,$MeV). The uncertainty of
this response introduces a relative uncertainty of
$\sim1.5\,\\%$ on the simulated analyzing power of the
polarimeter.Finally, the full polarimeter setup, consisting
of a solenoid magnet and the Cherenkov calorimeter, was
commissioned at the FLARE facility using an unpolarized LPA
electron beam. Initial system tests, beam charge and energy
characterization, and operational polarization measurements
were conducted. Simulations determined the analyzing power
of the system to be $A=11.74\pm0.18\,\\%$ ($\frac{\Delta
A}{A} = 1.6\,\\%$) with the dominant uncertainty arising
from the calorimeter response. The actual measurement was
found to be primarily influenced by beam stability and
control. In particular, observed asymmetries -- unrelated to
beam polarization -- can be explained by potential energy
drifts. Extrapolation to realistic polarization measurements
indicates that shot-to-shot charge and energy stability must
be provided at the $\leq 1\,\\%$ level to enable reliable
polarization measurements.},
cin = {FTX / MPA},
cid = {I:(DE-H253)FTX-20210408 / I:(DE-H253)MPA-20200816},
pnm = {PHGS, VH-GS-500 - PIER Helmholtz Graduate School
$(2015_IFV-VH-GS-500)$ / 622 - Detector Technologies and
Systems (POF4-622)},
pid = {$G:(DE-HGF)2015_IFV-VH-GS-500$ / G:(DE-HGF)POF4-622},
experiment = {EXP:(DE-H253)PLASMA-20250101 /
EXP:(DE-H253)TestBeamline24-20150101},
typ = {PUB:(DE-HGF)11},
urn = {urn:nbn:de:gbv:18-ediss-128363},
doi = {10.3204/PUBDB-2025-01873},
url = {https://bib-pubdb1.desy.de/record/630593},
}