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@PHDTHESIS{Malyutin:171168,
author = {Malyutin, Dmitriy},
title = {{T}ime {R}esolved {T}ransverse and {L}ongitudinal {P}hase
{S}pace {M}easurements at the {H}igh {B}rightness {P}hoto
{I}njector {PITZ}},
issn = {1435-8085},
school = {University of Hamburg},
type = {Dr.},
address = {Hamburg},
reportid = {DESY-2014-03183, DESY-THESIS-2014-021},
series = {DESY-THESIS},
year = {2014},
note = {PITZ facility; University of Hamburg, Diss., 2014},
abstract = {Short wavelength, high intensity Free Electron Lasers
(FELs) require a high brightness electron beam, i.e. the
beam should have small transverse and longitudinal sizes,
small divergence and energy spread and high peak current.
Therefore, the detailed characterization of the beam is
required.The Photo Injector Test facility at DESY, Zeuthen
site (PITZ), was established as a test stand of the electron
source for Free electron Laser in Hamburg (FLASH) and the
European X ray Free Electron Laser (XFEL). The PITZ beamline
consists of various types of diagnostic devices for the
detailed bunch characterization. Mainly, the transverse
phase space characterization is performed at PITZ, but
longitudinal phase space measurements are also of great
importance for full characterization of high brightness
electron bunches from the photo injector.One of the ways to
measure the longitudinal phase space of electron bunch is an
RF deflector. It deflects particles transversely with
respect to the movement direction of the bunch in a linear
dependence on their longitudinal coordinates within the
bunch. As a result it gives the possibility to perform
measurements of the bunch longitudinal properties in
combination with a following transverse beam
characterization. Using additionally a dispersive section
the longitudinal phase space can be obtained as well.Another
approach to measure the longitudinal phase space of the
bunch is a tomographic method based on measurements of the
momentum spectra while varying the electron bunch energy
chirp. The energy chirp at PITZ can be applied and changed
by varying the RF phase of the CDS booster – the
accelerating structure installed downstream the gun. The
resulting momentum distribution can be measured with a
dipole spectrometer downstream. As a result, the
longitudinal phase space at the entrance and exit of the CDS
booster can be reconstructed over a wide range of bunch
charges. In this thesis both methods for longitudinal phase
space measurements are described in detail. Measurement
techniques are introduced. Numerical simulations of the
measurements are performed and studied. Results of the first
longitudinal phase space measurements at PITZ using the
tomographic technique are presented.},
keywords = {Dissertation (GND)},
cin = {ZEU-PITZ},
cid = {I:(DE-H253)ZEU-PITZ-20120731},
pnm = {541 - Photons (POF2-541)},
pid = {G:(DE-HGF)POF2-541},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)11 / PUB:(DE-HGF)15},
doi = {10.3204/DESY-THESIS-2014-021},
url = {https://bib-pubdb1.desy.de/record/171168},
}