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@PHDTHESIS{Loisch:426401,
author = {Loisch, Gregor},
othercontributors = {Gruener, Florian and Oppelt, Anne and Ferrario, Massimo},
title = {{D}emonstrating {H}igh {T}ransformer {R}atio
{B}eam-{D}riven {P}lasma {W}akefield {A}cceleration},
school = {Universität Hamburg},
type = {Dissertation},
address = {Hamburg},
publisher = {Verlag Deutsches Elektronen-Synchrotron},
reportid = {PUBDB-2019-03713, DESY-THESIS-2019-024},
series = {DESY THESIS},
pages = {197},
year = {2019},
note = {Dissertation, Universität Hamburg, 2019},
abstract = {In this work, plasma wakefield acceleration with high
transformer ratios, i.e. highratios between acceleration of
witness particles to deceleration of driver particles, is
investigated experimentally.Particle-beam-driven plasma
wakefield acceleration (PWFA) is one of the primecandidates
for future compact accelerator technologies. In this scheme,
a highbrightness driver particle bunch enters a plasma and
initiates oscillations of plasma electrons by expelling them
from their equilibrium positions. Particles trailing the
driver bunch can be accelerated in the electric field
between regions of negative and positive charge excess
formed in this oscillation. Acceleration gradients of up to
several tens of GV/m have been demonstrated in experiment,
exceeding the gradients of conventional technology by orders
of magnitude. PWFA could thus allow to accordingly shrink
the size of an accelerator, possibly reducing size and cost
of an accelerator facility significantly.One key aspect of a
PWFA is the ratio between acceleration gradient behind the
driver and deceleration gradient inside the driver bunch.
This so-called transformer ratio defines the maximum
acceleration achievable for a given driver energy and is
closely connected to the achievable efficiency. In linear
wakefield theory the transformer ratio is limited to 2 for
longitudinally symmetric driver bunches, which typically
emerge from conventional accelerators. One proposed method
to achieve high transformer ratios (HTR) exceeding this
limit is to employ driver bunches with lengths of multiple
plasma skin depths and sawtooth-like, “triangular”
current profiles. Due to the complexity of shaping such
bunches and beam-plasma instabilities that can inhibit
stable acceleration, HTRs had thus far not been achieved in
PWFA.In the course of the present work, the driving of HTR
PWFA has been accomplished at the Photo-Injector Test
facility at DESY in Zeuthen (PITZ). Existing bunch shaping
capabilities at PITZ, based on photocathode laser pulse
shaping,were extended to the production of HTR-capable
driver bunches. An argon gasdischarge plasma cell was built
and optimised for providing the plasma acceleration medium
for the PITZ electron beam parameters. A novel plasma
density measurement method based on the self-modulation of
long electron bunches was developed and validated, which
enabled determination of plasma densities not accessible
with established methods. Following these preparations, a
transformer ratio of 4.6+2.2−0.7was observed
experimentally and reproduced in numerical simulations.},
cin = {ZEU-PITZ},
cid = {I:(DE-H253)ZEU-PITZ-20120731},
pnm = {631 - Accelerator R $\&$ D (POF3-631)},
pid = {G:(DE-HGF)POF3-631},
experiment = {EXP:(DE-H253)PITZ-20150101},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)29 / PUB:(DE-HGF)11},
doi = {10.3204/PUBDB-2019-03713},
url = {https://bib-pubdb1.desy.de/record/426401},
}