% 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{Silva:218886,
author = {Silva, Joel},
title = {{D}igital {S}ignal {A}nalysis for {C}s{I}({T}1) {D}etectors
and the {A}ctive-{T}arget at {R}$^3${B}},
school = {Johannes Gutenberg-Universität Mainz},
type = {Dissertation},
reportid = {GSI-2019-00703},
pages = {138 S.},
year = {2016},
note = {Dissertation, Johannes Gutenberg-Universität Mainz , 2016},
abstract = {Modern experimental setups tend to replace analogue
front-end electronics with fully digital systems.The
detector signals are sampled in early stages and most of the
signal processing is performeddigitally. The presented work
is divided into two major subjects involving digital
signalanalysis: firstly employed to correct temperature
dependent gain variations and perform particleidentification
of CsI(T1) based detectors and secondly to test the
functionality of an active-targetprototype (AcTar) for the
Reactions with Relativistic Radioactive Beams (R$^3$B)
setup.In the first part of this work a pulse shape based
method for monitoring the interior temperatureof the CsI(Tl)
crystal is proposed. The method uses the correlation between
the gain and definedpulse shape parameters to correct the
effect of temperature variations in the energy calibration
ofthe corresponding detector system. The suitability of the
method was tested using both, a photomultipliertube (PMT)
and an avalanche photodiode (APD) readout photosensor. The
analysisshows that the gain changes due to temperature
variations can be corrected to a precision betterthan 1\%
with both the PMT and APD photosensors, well below the
CsI(T1) intrinsic resolution for$\sim$1 MeV $\gamma$-rays.
For particle identification, the fuzzy clustering algorithm
is used to compute theprinciple pulse shape associated with
the different particle species in an unsupervised fashion.
Theresults show good discrimination between protons and
$\gamma$-rays.In the second part of this work the
functionality of the AcTar prototype for the R$^3$B setup
has been tested. The objective was to prove the feasibility
and performance of such kind of detector withthe use of
heavy ion beams. As a proof of concept, a $^{58}$Ni beam at
700 MeV/u was impinging on a He-H$_2$ (3\%) gaseous target
mixture. The presented results show the principle
functionalities of thedetector and suggest that pulse shape
analysis can indeed be used to track the recoil particles
andreconstruct the kinematics. It is the first time that an
active-target of such kind has been successfullytested with
beams heavier than carbon.},
cin = {KRA / R3B@FAIR},
cid = {I:(DE-Ds200)KRA-20150901OR349 / I:(DE-Ds200)Coll-FAIR-R3B},
pnm = {613 - Matter and Radiation from the Universe (POF3-613)},
pid = {G:(DE-HGF)POF3-613},
typ = {PUB:(DE-HGF)11},
urn = {urn:nbn:de:hebis:77-diss-1000005377},
url = {https://repository.gsi.de/record/218886},
}