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The work presented in this thesis addresses a key issue of the CBM experiment at FAIR, which aims to study charm production in heavy ion collisions at energies ranging from 10 to 40 AGeV . For the first time in this kinematical range, open charm mesons will be used as a probe of the nuclear fireball. Despite of their short decay length, which is typically in the order of few 100 µm in the laboratory frame, those mesons will be identified by reconstructing their decay vertex.
The study of the electromagnetic structure of hadrons plays an important role in understanding the nature of matter. In particular the emission of lepton pairs out of the hot and dense collision zone in heavy-ion reactions is a promising probe to investigate in-medium properties of hadrons and in general the properties of matter under such extreme conditions. The first experimental observation of an enhanced di-electron yield in the invariant-mass region 0:3 - 0:7 GeV/c2 in p+Be collisions at 4:9 GeV/u beam energy [2] was announced by the DLS collaboration [1]. Recent results of the HADES collaboration show a moderate enhancement above n Dalitz decay contributions for 12C+12C at 1 and 2 GeV/u [3, 4] confirming the DLS results. There are several theoretical explanations of this observation, most of them focusing on possible in-medium modifications of the properties of vector mesons. At low beam energies the question whether the observed excess is related to any in-medium effects remains open because of uncertainties in the description of elementary di-electron sources. In this work the di-electron production in p+p and d+p reactions at a kinetic beam energy of 1:25 GeV/u measured by the HADES spectrometer is discussed. At Ekin = 1:25 GeV/u, i.e. below the n meson production threshold in proton-proton reactions, the delta Dalitz decay is expected to be the most abundant source above the pi 0 Dalitz decay region. The observed large difference in di-electron production in p+p and d+p collisions suggests that di-electron production in the d+p system is dominated by the n+p interaction. In order to separate delta Dalitz decays and np bremsstrahlung the di-electron yield observed in p+p and n+p reactions, both measured at the same beam energy, has been compared. The main interest here is the investigation of iso-spin effects in baryonic resonance excitations and the off-shell production of vector mesons [5]. We indeed observe a large difference in di-electron production in p+p and n+p reactions. Results of these studies will be compared to recent calculations. We will also present our experimentally defined cocktail for heavy-ion data. At much higher beam energies experimental results of the CERES [6] and NA60 [7] collaborations also show an enhancement in the invariant mass region 0:3 - 0:7 GeV/c2, in principle similar to the situation in DLS. A strong excess of lepton pairs observed by recent high energy heavy-ion dilepton experiments hint to a strong influence of baryons, however no data exist at highly compressed baryonic matter, achievable in heavy-ion collisions from 8 - 45 GeV/u beam energy. These conditions would allow to study the expected restoration of chiral symmetry by measuring in-medium modifications of hadronic properties, an experimental program which is foreseen by the future CBM experiment at FAIR. The experimental challenge is to suppress the large physical background on the one hand and to provide a clean identification of electrons on the other hand. In this work, strategies to reduce the combinatorial background in electron pair measurements with the CBM detector are discussed. The main goal is to study the feasibility of effectively reducing combinatorial background with the currently foreseen experimental setup, which does not provide electron identification in front of the magnetic field.
This work presents the study on the suitability of single-crystal CVD diamond for particle-detection systems in present and future hadron physics experiments. Different characterization methods of the electrical and the structural properties were applied to gain a deeper understanding of the crystal quality and the charge transport properties of this novel semiconductor material. First measurements regarding the radiation tolerance of diamond were performed with sensors heavily irradiated with protons and neutrons. Finally, detector prototypes were fabricated and successfully tested in various experiments as time detectors for minimum ionizing particles as well as for spectroscopy of heavy ions at the energy ranges available at the SIS and the UNILAC facilities of GSI. ...
The HADES (High Acceptance DiElectron Spectrometer) is an experimental
apparatus installed at the heavy-ion synchrotron SIS-18 at GSI, Darmstadt.
The main physics motivation of the HADES experiment is the measurement
of e+e− pairs in the invariant-mass range up to 1 GeV/c2 in heavy-ion collisions
as well as in pion and proton-induced reactions.
The HADES physics program is focused on in-medium properties of the light
vector mesons ρ(770), ω(783) and φ(1020), which decay with a small branching
ratio into dileptons. Dileptons are penetrating probes which allow to study
the in-medium properties of hadrons. However, in heavy-ion collisions, the
measurement of such lepton pairs is difficult because they are rare and have a
very large combinatorial background.
Recently, HADES has been upgraded with new detectors and new electronics
in order to handle higher intensity beams and reactions with heavy nuclei up
to Au.
HADES will continue for a few more years its rich physics program at its
current place at SIS-18 and then move to the upcoming international Facility
for Antiproton and Ion Research (FAIR) accelerator complex. In this context
the physics results presented in this work are important prerequisites for the investigation
of in-medium vector meson properties in p + A and A+A collisions.
This work consists of five chapters. The first chapter introduces the physics
motivation and a review of recent physics results. In the second chapter, the
HADES spectrometer is described and its sub-detectors are presented. Chapter
three deals with the issue of lepton identification and the reconstruction of
the dielectron spectra in p + p collisions is presented. Here, two reactions
are characterized: inclusive and exclusive dilepton production reactions. From
the spectra obtained, the corresponding cross sections are presented with the
respective statistical and systematical errors. A comparison with theoretical
models is included as well. Conclusions are given in chapter four.
The final part of this work is dedicated to the HADES upgrade, whose goal
is among others the achievement of a reliable and fast data acquisition of the
Multiwire Drift Chambers (MDCs). Chapter five presents my contribution to
this successful project during the three years of my stay at GSI.
Ein wesentlicher Forschungsgegenstand der Kernphysik ist die Untersuchung der Eigenschaften von Kernmaterie. Das Verständnis darüber gibt in Teilen Aufschluss über die Erscheinungsweise und Wechselwirkung von Materie. Ein Schlüssel liegt dabei in der Untersuchung der Modifikation der Eigenschaften von Hadronen in dem Medium Kernmaterie, das durch Parameter wie Dichte und Temperatur gekennzeichnet werden kann. Man hofft damit unter anderem Einblick in die Mechanismen zu bekommen, welche zur Massenbildung der Hadronen beitragen. Zur Untersuchung solcher Modifikationen eignen sich insbesondere Vektormesonen, die in e+e- Paare zerfallen. Die Leptonen dieser Paare wechselwirken nicht mehr stark mit der Materie innerhalb der Reaktionszone, und tragen somit wichtige Informationen ungestört nach außen. Das HADES-Spektrometer bei GSI wird dazu verwendet die leichten bei SIS-Energien produzierten Vektormesonen rho, omega und phi zu vermessen. Hierzu wurde zum erste mal das mittelschwere Stoßsystem Ar+KCl bei einer Strahlenergie von 1,76 AGeV gemessen. Die im Vergleich zum früher untersuchten System C+C höhere Spurmultiplizität innerhalb der Spektrometerakzeptanz verlangte eine Anpassung der bisher verwendeten Datenanalyse. Das bisher verwendete Verfahren, mehrere scharfe Schnitte auf verschiedene Observablen seriell anzuwenden, um einzelne Leptonspuren als solche zu identifizieren, wurde durch eine neu entwickelte multivariate Analyse ersetzt. Dabei werden die Informationen aller beteiligten Observablen mit Hilfe eines Algorithmus zeitgleich zusammengeführt, damit Elektronen und Positronen vom hadronischen Untergrund getrennt werden können. Durch Untersuchung mehrerer Klassifizierer konnte ein mehrschichtiges künstliches neuronalen Netz als am besten geeigneter Algorithmus identifiziert werden. Diese Art der Analyse hat den Vorteil, dass sie viel robuster gegenüber Fluktuationen in einzelnen Observablen ist, und sich somit die Effizienz bei gleicher Reinheit steigern lässt. Die Rekonstruktion von Teilchenspuren im HADES-Spektrometer basiert nur auf wenigen Ortsinformationen. Daher können einzelne vollständige Spuren a priori nicht als solche gleich erkannt werden. Vielmehr werden durch verschiedene Kombinationen innerhalb derselben Mannigfaltigkeit von Positionspunkten mehr Spuren zusammengesetzt, als ursprünglich produziert wurden. Zur Identifikation des maximalen Satzes eindeutiger Spuren eines Ereignisses wurde eine neue Methode der Spurselektion entwickelt. Während dieser Prozedur werden Informationen gewonnen, die im weiteren Verlauf der Analyse zur Detektion von Konversions- und pi0-Dalitz-Paaren genutzt werden, die einen großen Beitrag zum kombinatorischen Untergrund darstellen. Als Ergebnis wird das effizienzkorrigierte, und auf die mittlere Zahl der Pionen pro Ereignis normierte, Spektrum der invarianten Elektronpaarmasse präsentiert. Erste Vergleiche mit der konventionellen Analysemethode zeigen dabei eine um etwa 30% erhöhte Rekonstruktionseffizienz. Das Massenspektrum setzt sich aus mehr als 114.000 Paaren zusammen -- über 16.000 davon mit einer Masse größer als 150 MeV. Ein erster Vergleich mit einem einfachen thermischen Modell, welches durch den Ereignisgenerator Pluto dargestellt wird, eröffnet die Möglichkeit, die hier gefundenen Produktionsraten des omega- und phi-Mesons durch m_T-Skalierung an die durch andere Experimente ermittelten Raten des eta zu koppeln. In diesem Zusammenhang findet sich weiterhin ein von der Einschussenergie abhängiger Produktionsüberschluss von F(1,76) = Y_total/Y_PLUTO = 5,3 im Massenbereich M = 0,15...0,5 GeV/c^2. Die theoretische Erklärung dieses Überschusses birgt neue Erkenntnisse zu den in-Medium Eigenschaften von Hadronen.
Das Compressed Baryonic Matter Experiment (CBM) wird im Rahmen der Facility for Antiproton and Ion Research (FAIR) entwickelt, um das Phasendiagramm stark wechselwirkender Materie vorwiegend im Bereich hoher Dichte ausgiebig zu studieren. Dazu sollen Kollisionen schwerer Ionen durchgeführt werden und die Reaktionsprodukte mit hoher Präzision in Teilchendetektoren gemessen und identfiziert werden. Eine wichtige Aufgabe besteht in der Unterscheidung von Elektronen und Pionen, zu der ein Übergangsstrahlungszähler (Transition Radiation Detector) beiträgt. Übergangsstrahlung wird im relevanten Impulsbereich dieser Teilchen nur von Elektronen emittiert und soll im Detektor registriert werden.
In der vorliegenden Arbeit wird die Entwicklung dieses Detektors auf Basis von Vieldrahtproportionalkammern (Multiwire Proportional Chamber ) hauptsächlich anhand von Simulationen diskutiert, aber auch erste Testmessungen eines Prototypen vorgestellt. Der Schwerpunkt der Simulationen eines einzelnen Detektors liegt in der Untersuchung der Effiienz in Abhängigkeit seiner Dicke.
Der Übergangsstrahlungszähler für CBM wird aus mehreren Detektorlagen bestehen. Daher wird außerdem die Effizienz des Gesamtsystems analysiert, indem verschiedene Methoden zur Kombination der einzelnen Signale angewendet werden. Darüber hinaus wird die Effizienz des verfolgten Detektorkonzepts in Abhängigkeit des Radiators, der Anzahl der Detektorlagen, sowie des Teilchenimpulses präsentiert.
Within this thesis, the mechanical integration of the Micro Vertex Detector (MVD) of the Compressed Baryonic Matter (CBM) experiment is developed. The CBM experiment, which is being set up at the future FAIR facility, aims to investigate the phase diagram of strongly interacting matter in the regime of high net-baryon densities and moderate temperatures. Heavy-ion collisions at beam energies in the range of 2 to 45 AGeV, complemented by results from elementary reactions, will allow access to these conditions. The experiments conducted at LHC (CERN, Switzerland) and at RHIC (BNL, USA = does not apply within the Beam Energy Scan program) so far focus on the investigation of the phase diagram in the regime of high temperatures and vanishing net-baryon densities. The high beam intensities provided by FAIR will enable CBM to focus its experimental program on systematical studies of rare particles. Among other particle species, open charm-carrying particles are one of the most promising observables to investigate the medium created in heavy-ion collisions since their charm quarks are exposed to the medium and traverse its whole evolution. The fact that the decay particles of these rare observables are also produced abundantly in direct processes in heavy-ion collisions results in a huge combinatorial background which attributes specific requirements to the detector systems. The call for a high interaction rate leads to a cutting-edge detector system which provides an excellent spatial resolution, thin detector stations and the capability to cope with the induced radiation as well as the high rate of traversing particles and the resulting track density. The required demands are to be implemented by the MVD which will be equipped with four planar stations positioned at 50, 100, 150 and 200 mm downstream the target. The geometrical acceptance, which has to be covered with charge-sensitive material, is defined according to the requirements of CBM in the polar angle range of [2.5°; 25°]. The MVD stations have to contribute as little as possible to the overall material budget. The expected beam intensity and the vicinity close to the target require silicon detectors that provide a hardness against non-ionizing radiation of more than 10^13 n_eq/cm² and against ionizing radiation of more than 1 Mrad. In addition, the read-out time of the sensors has to be as short as possible to avoid potential ambiguities in the particle tracking caused by the pile-up of hits having emerged from different collisions. For the time being, Monolithic Active Pixel Sensors (MAPS) offer the optimal choice of technology required to address the physics program of CBM with respect to the spectroscopy of open charm and di-electrons. The geometrical properties of these sensors define the layout of the detector. To limit the multiple scattering of the produced particles inside the geometrical acceptance, the sensors and the MVD have to operate in a moderate vacuum. The sensors are thinned down to a thickness of 50 µm and, to achieve a maximum polar angle coverage, they are glued onto both sides of dedicated thin carriers. These carriers, which are made of highly thermally conductive materials such as CVD diamond or encapsulated TPG, allow efficient extraction of the power produced in the sensors. This enables their operation at temperatures well below 0 °C as suggested by corresponding radiation hardness studies. Dedicated actively cooled aluminum-based heat sinks are positioned outside of the acceptance to dissipate the heat produced by the sensors and the front-end electronics. The design of the MVD, including the realistic thicknesses of the integrated materials, has been developed and refined in the context of this thesis. It has been transformed into a unique software model which is used to simulate and further optimize the mechanical and thermal properties of the MVD, as well as in sophisticated physics simulations. The model allowed evaluation of the material budget of each individual MVD station in its geometrical acceptance. The calculated averaged material budget values stay well below the material budget target values demanded by the physics cases. The thermal management of the MVD has been simulated on the level of a quadrant of each MVD station – four identically constructed quadrants are forming an MVD station – taking into account material properties of the sensors, the glue and the sensor carrier. The temperature gradients across the pixels of a given sensor area in the direction of the rows and columns were found to be in an acceptable range of below 5 K. A temperature difference between the thermal interface area and the maximum sensor temperature of dT = 5 K on the first and a value of dT = 40 K on the fourth MVD station has been thermally simulated assuming a sensor power dissipation of 0.35 W/cm², highlighting the need to optimize the thermal interface between the involved materials as well as the power dissipation of the sensors. The feasibility of several key aspects required for the construction phase of the MVD has been investigated within the MVD Prototype project. The construction of the MVD Prototype allowed evaluation, testing and validation of the handling and the double-sided integration of ultra-thin sensors – the required working steps for their integration have been specified, evaluated and successfully established – as well as their operation in the laboratory and during a concluding in-beam test using high-energetic pions provided by the CERN-SPS. The thermal characterization of the MVD Prototype during its operation – in a temperature range from [5 °C; 25 °C], not in vacuum – confirmed the corresponding thermal simulations conducted during its design phase and substantiated the results of the thermal simulations for the design of the MVD. The aim of a material budget value of only x/X_0 ~ 0.3% for the MVD Prototype has been accomplished. Analyzing the in-beam data, the nominal sensor performance parameters were successfully reproduced, demonstrating that the proposed integration process does not impair the sensors’ performance. Moreover, no evidence of potential impact on the sensors’ performance arising from mechanical weaknesses of the MVD Prototype mechanics has been found within the analyzed data. Based on the MVD Prototype and the simulations of the material budget as well as the thermal management, this thesis evaluated the work packages, procedures and quality assurance parameters needed to set up the starting version of the MVD and addressed open questions as well as critical procedures to be studied prior to the production phase of the detector, emphasizing the evaluation of the cooling concept in vacuum and the integration of sensors in ladder structures on both sides of the quadrants of the MVD stations.
Sensors for high rate charge particle tracking have to withstand the harsh radiation doses deposited by the particles to be sensed. This holds particularly for the novel CMOS Monolithic Active Pixel Sensors, which are considered a promising sensor technology for future vertex detectors due to their very light material budget and excellent spatial resolution. To resist the radiation doses expected close to the interaction regions of heavy-ion experiments, the sensors have to be hardened against radiation doses, which exceed the native tolerance of CMOS technology significantly. In this thesis, the results of non-ionizing radiation hardness studies at the IKF on sensor prototypes developed at the IPHC in Strasbourg are presented. Our results demonstrate that the CMOS sensors evaluated in the context of this thesis can withstand non-ionizing radiation of up to 5×10^14 neq/cm^2. This hardness qualifies them as promising candidates for use in future vertex detectors.
The first measurement of the fluctuation of the kaon-to-proton ratio in relativistic heavy-ion collisions is presented. This thesis details the analysis procedure for identifying kaons and protons using the NA49 experiment at CERN-SPS and discusses the results in the context of the current state of the field.
In April and May 2012 data on Au+Au collisions at beam energies of Ekin = 1.23A GeV were recorded with the High Acceptance Di-Electron Spectrometer, which is located at the GSI Helmholtz Center for Heavy Ion Research in Darmstadt, Germany. At this beam energy all hadrons containing strangeness are produced below their elementary production threshold. The required energy is not available in binary NN collisions but must be provided by the system e.g. through multi-particle interactions or medium effects like a modified in-medium potential (e.g. KN/ΛN potential). Thus, a high sensitivity to these medium effects is expected in the investigated system.
The baryon-dominated systems created in relativistic heavy-ion collisions (HIC) at SIS18 energies reach densities of about 2-3 times ground state density p0 and may be similar to the properties of matter expected in the inner core of neutron stars. It is in particular the behavior of hadrons containing strangeness, i.e. kaons and hyperons, and their potentials in the dense medium which may have severe implications on astrophysical objects and processes. As ab-initio calculations of quantum chromodynamics (QCD) cannot be performed rigorously on the lattice at finite baryo-chemical potentials due to the fermion sign problem, effective descriptions have to be used in order to model properties of dense systems and the involved particles. The only way to access the in-medium potential of strange hadrons above nuclear ground state density p0 is by comparing data from relativistic HIC to such effective microscopic models. Up to now, not much data on neutral kaons and Λ hyperons are available from heavy collision systems close to their NN production threshold. These two electromagnetically uncharged strange hadrons are in particular well suited to study their potential in a dense nucleon-dominated environment as their kinematic spectra are not affected by Coulomb interactions.
In this thesis, the production of charged kaons and Φ mesons in Au+Au collisions at sqrt sAuAu = 2.4 GeV is studied. At this energy, all particles carrying open and hidden strangeness are produced below their respective free nucleon-nucleon threshold with the corresponding so-called excess energies: sqrt sK+ exc = -0.15 GeV, sqrt sK- exc = -0.46 GeV, sqrt sΦ exc = -0.49 GeVGeV. As a consequence, the production cross sections are very sensitive to medium effects like momentum distributions, two- or multistep collisions, and modification of the in-medium spectral distribution of the produced states [1]. K+ and K- mesons exhibit different properties in baryon dominated matter, since only K- can be resonantly absorbed by nucleons. Although strangeness exchange reactions have been proposed to be the dominant channel for K- production in the analyzed energy regime, the production yield and kinematic distributions could also be explained in smaller systems based on statistical hadronization model fits to the measured particle yields, including a canonical strangeness suppression radius RC, and taking the Φ feed-down to kaons into account [2, 3]. For the first time in central Au+Au collisions at such low energies, it is possible to reconstruct and do a multi differential analysis of K- and Φ mesons. In principle, this should be the ideal environment for strangeness exchange reactions to occur, as the particles are produced deeply sub-threshold in a large and long-living system. Therefore, it is the ultimate test to differentiate between the different sources for K- production in HIC.
In total 7.3x10exp9 of the 40% most central Au(1.23 GeV per nucleon)+Au collisions are analyzed. The data has been recorded with the High Acceptance DiElectron Spectrometer HADES located at Helmholtzzentrum für Schwerionenforschung GSI in April/May 2012. A substantially improved reconstruction method has been employed to reconstruct the hadrons with high purity in a wide phase space region.
The estimated particle multiplicities follow a clear hierarchy of the excess energy: 41.5 ± 2.1|sys protons at mid-rapidity per unit in rapidity, 11.1 ± 0.6|sys ± 0.4|extrapol π-, (3.01 ± 0.03|stat ± 0.15|sys ± 0.30|extrapól) x10 exp -2 K+, (1.94 ± 0.09|stat ± 0.10|sys ± 0.10|extrapol)x10 exp -4 K- and (0.99 ± 0.24|stat ± 0.10|sys ± 0.05|extrapol)x10 exp -4 Φ per event. The multiplicities of the strange hadrons increase more than linear with the mean number of participating nucleons hAparti, supporting the assumption that the necessary energy to overcome the elementary production threshold is accumulated in multi-particle interactions. Transport models predict such an increase, but are overestimating the measured particle yield and are not able to describe the kinematic distributions of K+ mesons perfectly. However, the best description is given by the IQMD model with a density dependent kaonnucleon potential of 40 MeV at nuclear ground state density.
The K-=K+ multiplicity ratio is constant as a function of centrality and follows with (6.45 ± 0.77)x10 exp -3 the trend of increasing with beam energy indicated from previous experiments [4]. The effective temperature of K- TK+eff = (84 ± 6) MeV is found to be systematically lower than the one of K+ TK+eff = (104 ± 1) MeV, which has also been observed by the other experiments.
The Φ=K- ratio is with a value of 0.52 ± 0.16 higher than the one obtained at higher center-of-mass energies and smaller systems. This behavior is predicted from a tuned version of the UrQMD transport model [5], when including higher mass baryonic resonances which can decay into Φ mesons and from statistical hadronization models when suppressing open strangeness canonically. The found ratio is constant as a function of centrality and results with a branching ratio of 48.9%, that ~ 25% of all measured K- originate from Φ feed-down decays. A two component PLUTO simulation, consisting of a pure thermal and a K- contribution originating from Φ decays, can fully explain the observed lower effective temperature in comparison to K+ and the shape of the measured rapidity distribution of K-. As a result, we find no indication for strangeness exchange reactions being the dominant mechanism for K- production in the SIS18 energy regime, if taking the contribution from Φ feed-down decays into account.
The hadron yields for the 20% most central collisions can be described by a statistical hadronization model fit with the chemical freeze-out temperature of Tchem = (68 ± 2) MeV and baryochemical potential of μB = (883 ± 25) MeV, which is higher than expected from previous parameterizations. The analysis of the transverse mass spectra of protons indicate a kinetic freeze-out temperature of Tkin = (70 ± 4) MeV and radial flow velocity of βr = 0.43 ± 0.01, which is in agreement with the parameters obtained from the linear dependence of the effective temperatures on the particle mass Tkin = (71.5 ± 4.2) MeV and βr = 0.28 ± 0.09.
HADES (High Acceptance DiElectron Spectrometer), located at GSI, is a versatile detector for precise spectroscopy of e+ e- pairs and charged hadrons produced on a fixed target in a 1 to 3.5 AGeV kinetic beam energy region. The main experimental goal is to investigate properties of dense nuclear matter created in heavy ion collisions and learn about in-medium hadron properties.
In the HADES set-up 24 Mini Drift Chambers (MDC) allow for track reconstruction and determining the particle momentum by exploiting charged particle deflection in a magnetic field. In addition, the drift chambers contribute to particle identification by measuring the energy loss. The read-out concept foresees each sensing wire to be equipped with a preamplifier, analog pulse shaper and discriminator. In the current front-end electronics, the ASD-8 ASIC comprises the above modules. Due to limitations of the current on-board time to digital converters (TDC), especially regarding higher reaction rates expected at the future FAIR facility (HADES at SIS-100), the electronics need to be replaced by new board featuring multi-hit TDCs. Whereas ASD-8 chips cannot be procured anymore, a promising replacement candidate is the PASTTREC ASIC, developed by JU Krakow, which was tested w.r.t. suitability for MDC read-out in a variety of set-ups and, where possible, in direct comparison to ASD-8.
The timing precision, being the most crucial performance parameter of the joint system of detector and read-out electronics, was assessed in two different set-ups, i.e. a cosmic muon tracking set-up and a beam test at the COSY accelerator at Juelich using a minimum ionizing proton beam.
The beam test results were reproduced and can thus be quantitatively explained in a three dimensional GARFIELD simulation of a HADES MDC drift cell. In particular, the simulation is able to describe the characteristic dependence of the time precision on the track position within the cell.
A circuit simulation (SPICE) was used to closely model the time development of a raw drift chamber pulse, measured as a response to X-rays from a 55 Fe source. The insights gained from this model were used for attributing realistic charge values to the time over threshold values measured with the read-out ASICs in a charge calibration set-up. Furthermore, a high-level circuit simulation of the PASTTREC shaper is implemented to serve as a demonstration of the effect of the individual shaping and tail cancellation stages which are present in both ASICs.
The Compressed Baryonic Matter (CBM) experiment will explore the phase diagram of strongly interacting matter in the region of high net baryonic densities. The matter at these extreme conditions will be produced and studied in heavy-ion collisions with a fixed target set-up.
The present work is dedicated to the main component of the CBM experiment - the Silicon Tracking System (STS). The STS comprises of 8 tracking stations with 1292 double sided silicon microstrip sensors. The STS has to enable the reconstruction of up to 1000 charged particle tracks per nucleus-nucleus interaction at the rate of up to 10 MHz, provide a momentum resolution of Δp/p =1%, and withstand the radiation load of up to 1 x 1014 neq/cm2 (neq — radiation dose of 1 MeV neutron equivalent). Self-triggering read-out electronics will be located on the periphery of the detecting planes, and connected to the sensors with low mass micro-cables.
During the R&D phase, as well as in the pre-series and series production phase, the characterization of the sensors, of the front-end electronics and of the complete detector modules has to be performed. It is evident that characterization of more than 1000 silicon microstrip sensors and later of complete detector modules is very time-consuming, and may even damage the objects if not performed carefully. One of the goals of this work was to develop a systematic procedure for the quality assurance for the double-sided silicon microstrip sensors. This includes static optical inspection and visual tests, passive electrical test (such as leakage current, bulk capacitance, inter-strip capacitance & resistances, bias resistance and coupling capacitance), radiation hardness and long-term stability. A strategy for the quality assurance of these sensors is presented, defining the various tests to be performed and the documentation of the results. The techniques and quality assurance criteria will be applied for the pre-series and series production.
With decreasing feature size and increase in functionality and structures, the classical mechanical probe approach for internal fault detection and functional testing faces increasing challenges. In the field of silicon based chips and sensors there is rarely any analysis on the topic of non-invasive or contact-less probing and characterization, despite the fact that the contact-less probing is becoming more and more important as the fabrication technologies become smaller and more susceptible to the parasitic impact of mechanical probes. The silicon micro-strip double sided sensors used in STS have a complex structure, such as 1024 metal electrodes, 2048 bias resistors, 2048 DC pads and 4098 AC pads for probing, several guard rings, and even more in the 6.2 cm x 6.2 cm prototype sensor. Photo-intrusive technique is the best solution for the characterization and investigation of crucial parameters related to the detector operation and its functionality. A photo-intrusive probing is a method in which a non-invasive pulsed laser of a desired wavelength is used to inject the photon into the bulk and resulting in electron-hole pairs (e-h). In a completely depleted silicon sensor the charge injected (or generated) by the pulsed laser beam could be detected as current and shall be used for characterization.
A non-invasive contact-less Laser Test System (LTS) was developed based on a pulsed laser to investigate properties of the silicon sensors. The set-up is able to inject charge locally and scan sensors(or detector modules) with a pulsed infra-red laser driven by a step motor. The LTS is designed to measure sensor response in an automatized procedure at several thousand positions across the sensor with focused infra-
red laser light (spot size = 12 μm , wavelength = 1060 nm). The duration (10 ns) and power (5 mW) of the laser pulses are selected such that the absorption of the laser light in the 300 μm thick silicon sensors produces a number of about 24000 electrons, which is similar to the charge created by the minimum ionizing particles (MIP) in these sensors. The set-up was used to developed characterization procedures to determine the charge sharing between strips, and to measure a qualitative uniformity of the sensor response over the whole active area. The prototype sensors which are tested with the set-up are small prototype sensors (256 strips, pitch = 50 μm on each side) and full-size detector modules (1024 strips/side and pitch = 58 μm). They are read-out using a self-triggering prototype read-out electronic ASIC called n-XYTER. Laser scans for amplitude response, charge sharing in the inter-strip region, and spot-size determination technique are reported. For the verification of the some design parameters, unique methods of determining coupling capacitance, and inter-strip capacitance have been developed. The modules were also tested with proton beams, and the charge sharing in the inter-strip region has been compared to the laser test results.
Development of prototype components for the Silicon Tracking System of the CBM experiment at FAIR
(2013)
The CBM experiment at future accelerator facility FAIR will investigate the properties of nuclear matter under extreme conditions. The experimental programm is different from the heavy-ion experiments at RHIC (BNL) and LHC (CERN) that create nuclear matter at high temperatures. In contrast, the study of the QCD phase diagram in the region of the highest net baryon densities and moderate temperatures that is weakly explored will be performed with high precision. For this, collisions of different heavy-ion beams at the energies of 10–45GeV/nucleon with nuclear target will be measured.
The physics programme of the CBM experiment includes measurement of both rare probes and bulk observables that originate from various phases of a nucleus-nucleus collision. In particular, decay of particles with charm quarks can be registered by reconstructing the decay vertex detached from the primary interaction point by several hundreds of micrometers (e.g., decay length c Tau = 123 µm for D0 meson). For this, precise tracking and full event reconstruction with up to 600 charged particle tracks per event within acceptance are required. Other rare probes require operation at interaction rate of up to 10MHz. The detector system that performs tracking has to provide high position resolution on the order of 10 µm, operate at high rates and have radiation tolerant design with low material budget.
The Silicon Tracking System (STS) is being designed for charged-particle tracking in a magnetic field. The system consists of eight tracking station located in the aperture of a dipole magnet with 1T field. For tracks with momentum above 1GeV, momentum resolution of such a system is expected to be about 1%. In order to fulfill this task, thorough optimization of the detector design is required. In particular, minimal material budget has to be achieved.
Production of a detector module requires research and development activities with respect to the module components and their integration. A detector module is a basic functional unit that includes a sensor, an analogue microcable and frontend electronics mounted on a support structure. The objective of the thesis is to perform quality assurance tests of the prototype module components in order to validate the concept of the detector module and to demonstrate its operation using radioactive sources and particle beams.
Double-sided silicon microstrip detectors have been chosen as sensor technology for the STS because of the combination of a good spatial resolution, two-dimensional coordinate measurement achieved within low material budget (0.3%X0), high readout speed and sufficient radiation tolerance. Several generations of double-sided silicon microstrip sensors have been manufactured in order to explore the radiation hard design features and the concept of a large-area sensor compatible with ladder-type structure of the detector module. In particular, sensors with double metal layer on both sides and active area of 62×62mm2 have been produced. Electrical characterization of the sensors has been performed in order to establish the overall operability as well as to extract the device parameters. Current-voltage, capacitance-voltage characteristics and interstrip parameters have been measured.
Readout of the sensors has been done using self-triggering front-end electronics. A front-end board has been developed based on the n-XYTER readout chip with data driven architecture and capable of operating at 32MHz readout rate. The front-end board included an external analog-to-digital converter (ADC). Calibration of the ADC has been performed using both 241Am X-ray source and external pulse generator. Threshold calibration and investigation of temperature dependence of chip parameters has been carried out.
Low-mass support structures have been developed using carbon fibre that has the rigidity to hold the detector modules and introduce minimal Coulomb scattering of the particle tracks. Analogue microcables have been produced with aluminium traces on a polyimide substrate, thus combining good electrical connection with low material budget. Microcable structure includes several layers optimized for low trace capacitance and thus low-noise performance.
A demonstrator tracking telescope has been constructed and operated in several beam tests including 2.5GeV proton beam at COSY synchrotron (Jülich). Three tracking stations have been complemented with several beam hodoscopes. Analysis of the beam data has yielded information on analogue and timing response, beam profile. Tracking and alignment information has been obtained. Beam stability has been evaluated using specially developed monitoring tools.
As a result of conducted studies, performance of the module components have been evaluated and requirements to the detector module have been formulated. Practical suggestions have been made with respect to the structure of the detector module, whereas precise definition of the final detector module design was outside of the scope of this thesis.
Understanding the hadron spectrum is one of the primary goals of non-perturbative QCD. Many predictions have experimentally been confirmed, others still remain under experimental investigation. Of particular interest is how gluonic excitations give rise to states with constituent glue. One class of such states are hybrid mesons that are predicted by theoretical models and Lattice QCD calculations. Searching for and understanding the nature of these states is a primary physics goal of the GlueX experiment at the CEBAF accelerator at Jefferson Lab. A search for a JPC = 1−− hybrid meson candidate, the Y(2175), in φ(1020)π+π+ and φ(1020)f0(980) channels in photoproduction on a proton target has been conducted. A first measurement of non-resonant φ(1020)π+π+ and φ(1020)f0(980) total cross sections in photoproduction has been performed. An upper limit on the resonance production cross section for the Y (2175) → φ(1020)π+π+ and Y (2175) → φ(1020)f0(980) channels are estimated. Since the analysis essentially depends on the quality of the charged kaon identification, also an optimization of particle identification through an improvement of the energy loss estimation in the central drift chamber by a truncated mean method has been investigated.
At sufficiently high temperatures and baryon densities, nuclear matter is expected to undergo a transition into the Quark-Gluon-Plasma (QGP) consisting of deconfined quarks and gluons and accompanied by chiral symmetry restoration. Signals of these two fundamental characteristics of Quantum-Chromo-Dynamics (QCD) can be studied in ultra-relativistic heavy-ion collisions producing a relatively large volume of high energy and nucleon densities as existent in the early universe. Dileptons are unique bulk-penetrating sources for this purpose since they penetrate through the surrounding medium with negligible interaction and are created throughout the entire evolution of the initially created fireball. A multitude of experiments at SIS18, SPS and RHIC have taken on the challenging task to measure these rare probes in a heavy-ion environment. NA60's results from high-quality dimuon measurements have identified the broadened ρ spectral function as favorable scenario to explain the low-mass dilepton excess, and partonic sources as dominant at intermediate dilepton masses.
Enabled by the addition of a TOF detector system in 2010, the first phase of the Beam Energy Scan (BES-I) at RHIC allows STAR to conduct an unprecedented energy-dependent study of dielectron production within a homogeneous experimental environment, and hence close the wide gap in the QCD phase diagram between SPS and top RHIC energies. This thesis concentrates on the understanding of the LMR enhancement regarding its invariant mass, transverse momentum and energy dependence. It studies dielectron production in Au+Au collisions at beam energies of 19.6, 27, 39, and 62.4 GeV with sufficient statistics. In conjunction with the published STAR results at top RHIC energy, this thesis presents results on the first comprehensive energy-dependent study of dielectron production.
This includes invariant mass- and transverse momenta-spectra for the four beam energies measured in 0-80% minimum-bias Au+Au collisions with high statistics up to 3.5 GeV/c² and 2.2 GeV/c, respectively. Their comparison with cocktail simulations of hadronic sources reveals a sizeable and steadily increasing excess yield in the LMR at all beam energies. The scenario of broadened in-medium ρ spectral functions proves to not only serve well as dominating underlying source but also to be universal in nature since it quantitatively and qualitatively explains the LMR enhancements measured over the wide range from SPS to top RHIC energies. It shows that most of the enhancement is governed by interactions of the ρ meson with thermal resonance excitations in the late(r)-stage hot and dense hadronic phase. This conclusion is supported by the energy-dependent measurement of integrated LMR excess yields and enhancement factors. The former do not exhibit a strong dependence on beam energy as expected from the approximately constant total baryon density above 20 GeV, and the latter show agreement with the CERES measurement at SPS energy. The consistency in excess yields and agreement with model calculations over the wide RHIC energy regime makes a strong case for LMR enhancements on the order of a factor 2-3.
The extent of the results presented here enables a more solid discussion of its relation to chiral symmetry restoration from a theoretical point of view. High-statistics measurements at BES-II hold the promise to confirm these conclusions along with the LMR enhancment's relation to total baryon density with decreasing beam energy.
The study of meson production in proton-proton collisions in the energy range
up to one GeV above the production threshold provides valuable information about
the nature of the nucleon-nucleon interaction. Theoretical models describe the interaction
between nucleons via the exchange of mesons. In such models, different
mechanisms contribute to the production of the mesons in nucleon-nucleon collisions.
The measurement of total and differential production cross sections provide information
which can help in determining the magnitude of the various mechanisms.
Moreover, such cross section information serves as an input to the transport calculations
which describe e.g. the production of e+e− pairs in proton- and pion-induced
reactions as well as in heavy ion collisions.
In this thesis, the production of ω and η mesons in proton-proton collisions at 3.5
GeV beam energy was studied using the High Acceptance DiElectron Spectrometer
(HADES) installed at the Schwerionensynchrotron (SIS 18) at the Helmholtzzenturm
f¨ur Schwerionenforschung in Darmstadt.
About 80 000 ω mesons and 35 000 η mesons were reconstructed. Total production
cross sections of both mesons were determined. Furthermore, the collected statistics
allowed for extracting angular distributions of both mesons as well as performing
Dalitz plot studies.
The ω and η mesons were reconstructed via their decay into three pions (π+π−π0)
in the exclusive reaction pp −→ ppπ+π−π0. The charged particles were identified
via their characteristic energy loss, via the measurement of their time of flight and
momentum, or using kinematics.
The neutral pion was reconstructed using the missing mass method. A kinematic
fit was applied to improve the resolution and to select events in which a π0 was
produced.
The correction of measured yields for the effects of spectrometer acceptance was done
as a function of four variables (two invariant masses and two angles). Systematic
studies of the acceptance for different input distributions were performed.
The measured yields were normalized to the number of measured events of elastic
scattering. Systematic errors due to the methods of the data analysis and the
background subtraction were investigated.
Production angular distributions of ω and η mesons were measured. Both mesons
exhibit a slightly anisotropic angular distribution.
The Dalitz plot of ω meson production shows indications of resonant production.
However, the deviation of the distribution from the one expected by phase space
simulations is not large.
The Dalitz plot of η meson production shows a signal of the production via the
N(1535) resonance, The contribution of N(1535) to the production was quantified
to be about 47%. The angular distribution of η mesons does not show significant
differences between resonant and non resonant production.
The total production cross section of ω mesons in the reaction pp −→ ppω was
determined to be 106.5 ± 0.9 (stat) ± 7.9 (sys) [μb] where stat indicates statistical
error and sys indicates systematic error, while that of η mesons was determined to
be 136.9 ± 0.9 (stat) ± 10.1 (sys) [μb] in the reaction pp −→ ppη
The upcoming CBM Experiment at FAIR aims at exploring the region of highest net baryonic densities reproducible in energetic heavy ion collisions. Due to the very high beam intensities expected at FAIR, unprecedented data regarding rare observables such as charm quarks and hyperons will be accessible. Open charm mesons are particularly interesting, since they support the reconstruction of the total charm cross-section in order to search for exotic phenomena, e.g. a phase transition towards the quark-gluon plasma which is predicted by several theoretical models. Open charm studies will be performed via secondary vertex reconstruction with a suitable Micro-Vertex Detector (MVD). The CBM-MVD is currently in the development and prototyping phase with primary design goals concentrating on spatial resolution, radiation hardness, material budget, and readout performance. CMOS Monolithic Active Pixel Sensors (MAPS) provide an excellent spatial resolution for the MVD in the order of few um in combination with a low material budget (50 um thickness) and high radiation hardness. The active volume of the devices is formed from the epitaxial layer of standard CMOS wafers. This allows for integration of pixels together with analogue and digital data processing circuits on one single chip. This option was explored with the MIMOSA-26 prototype, which integrates functionalities like pedestal correction, correlated double sampling, discrimination and data sparsification based on zero suppression combined with a small and dense pixel matrix. The pixel array composed of 576 lines of 1152 pixels is read out in a column-parallel rolling shutter mode. One discriminator per column and the digital data processing circuits are located on the same chip in a 3 mm wide area beneath the pixel matrix allowing for binary hit encoding. This area also contains the circuits for pedestal correction and the configuration memory, which is programmed via JTAG. The preprocessed digital data is read out via two 80 Mbit/s LVDS links per sensor, which stream their data continuously based on a low-level protocol.
Within the scope of this thesis, a readout concept of the CBM-MVD is proposed and studied based on the current MIMOSA sensor generation. The backbone of the system is formed by the Readout Controller boards (ROCs) featuring FPGA microchips and optical links. Several ROC prototypes are considered using the synergy with the HADES Experiment. Finally, the TRB3 board is selected as a possible candidate for the initial FAIR experiments. Furthermore, a highly scalable, hardware independent FPGA firmware is implemented in order to steer and read out multiple MIMOSA-26 sensors. The reconfigurable firmware is also designed with the support for future MIMOSA sensor generations. The free-streaming sensor data is deserialized and error-checked, prior to its transmission over a suitable network interface. In order to demonstrate the validity of the concept, a readout network similar to the HADES Data Acquisition (DAQ) system is developed. The ROC is tested on the HADES TRB2 boards and data is acquired using suitable MAPS add-on boards and the TrbNet protocol.
In the context of the CBM-MVD prototype project, a readout network with 12 MIMOSA-26 sensors has been prepared for an in-beam test at the CERN SPS facility. A comprehensive control system is designed comprising customized software tools. The subsequent in-beam test is used to validate the design choices. As a result, the system could be operated synchronously and dead-time free for several days. The readout network behavior in a realistic operating environment has been carefully studied with the outcome the the TrbNet based approach handles the MVD prototype setup without any difficulties. A procedure to keep the sensors synchronous even in case of a data overflow has been pioneered as well. After the beam test, improvements and conceptual changes to the readout systems are being addressed which allow an integration into the global CBM DAQ system.
In this thesis, different physical and electrical aspects of silicon microstrip sensors and low-mass multi-line readout cables have been investigated. These silicon microstrip sensors and readout cables will be used in the Silicon Tracking System (STS) of the fixed-target heavy-ion Compressed Baryonic Matter (CBM) experiment which is under development at the upcoming Facility for Antiproton and ion Research (FAIR) in Darmstadt, Germany. The highly segmented low-mass tracking system is a central CBM detector system to resolve the high tracking densities of charged particles originating from beam-target interactions. Considering the low material budget requirement the double-sided silicon microstrip detectors have been used in several planar tracking stations. The readout electronics is planned to be installed at the periphery of the tracking stations along with the cooling system. Low-mass multi-line readout cables shall bridge the distance between the microstrip sensors and the readout electronics. The CBM running operational scenario suggests that some parts of the tracking stations are expected to be exposed to a total integrated particle fluence of the order of 1e14 neq/cm2. After 1e14 neq/cm2 the damaged modules in the tracking stations will be replaced. Thus radiation hard sensor is an important requirement for the sensors. Moreover, to cope with the high reaction rates, free-streaming (triggerless) readout electronics with online event reconstruction must be used which require high signal-to-noise (SNR) ratio (i.e., high signal efficiency, low noise contributions). Therefore, reduction in noise is a major goal of the sensor and cable development.
For better insight into the different aspects of the silicon microstrip sensors and multi-line readout cables, the simulation study has been performed using SYNOPSYS TCAD tools. 3D models of the silicon microstrip sensors and the readout cables were implemented which is motivated by the stereoscopic construction of the silicon microstrip sensors. For the evaluation of the performance of the silicon microstrip sensors in the harsh radiation environment during experimental operation, a radiation damage model has been included. It reproduces the behavior of the irradiated CBM prototype sensors. In addition to the static characteristics, the interstrip parameters relevant to understand strip isolation and cross-talk issues have been extracted. The transient simulations have been performed to estimate the charge collection performance of the irradiated sensors. The signal transmission in the readout cables has been evaluated with the finite element simulation tool RAPHAEL. Based on the performance of the front-end electronics used for early prototyping in the CBM experiment, capacitive and resistive noise contributions from the silicon microstrip sensors and multi-line readout cables have been extracted.
To validate the aforementioned simulations, numerous tests have been performed both on the multi-line readout cables and silicon microstrip sensors. Characterizations of multi-line readout cables and silicon microstrip sensors in laboratory conditions have been found to agree reasonably well with the simulations. Considering the expected radiation environment the behavior of silicon microstrip sensors have been studied especially in terms of noise and charge collection efficiency. Source-scan of the silicon microstrip sensors using 241Am is presented. In order to test a first system of detector stations including the data acquisition system, slow control and online monitoring software and for track reconstruction, in-beam tests have been performed at the COSY synchrotron of the Research Center Juelich, Germany. Further, different design parameters have been suggested to improve the sensor and readout cable design on the basis of the simulations and the measurements. Many of these parameters have been implemented in the new prototypes under production. These new prototypes will be tested in-beam by the end of 2013.
Im September 2005 wurden von der HADES-Kollaboration an der GSI in Darmstadt Daten der Schwerionen-Reaktion Ar+KCl bei 1,76A GeV aufgenommen. Neben den Pionen und Dileptonen wurden bereits fast alle Teilchen mit Seltsamkeitsinhalt rekonstruiert. In dieser Arbeit wird zum ersten Mal eine Analyse der leichten Fragmente Deuteronen, Tritonen und 3Helium mit HADES durchgeführt.
Die gemessenen Multiplizitäten wurden mit einem statistischen Hadronisationsmodell verglichen und zeigen gute Übereinstimmung mit diesem. Dies legt die Vermutung nahe, dass das System Ar+KCl bei 1,76A GeV einen hohen Grad an Thermalisierung erreicht. Zu einer weiteren Untersuchung dieser Hypothese wurden die sogenannten effektiven Temperaturen Teff der Teilchen der chemischen Ausfriertemperatur aus dem statistischen Modellfit gegenübergestellt. Bei der effektiven Temperatur handelt es sich um die inversen Steigungsparameter von Boltzmann-Fits an die transversalen Massenspektren mt-m0 bei Schwerpunktsrapidität. Diese Temperatur entspricht bei einer isotropen, statischen Quelle der kinetischen Ausfriertemperatur und sollte somit unterhalb oder gleich der chemischen Ausfriertemperatur sein. Im Falle der effektiven Temperaturen der Ar+KCl-Daten liegen diese jedoch systematisch höher und die Teilchen ohne Seltsamkeitsinhalt zeigen einen massenabhängigen Anstieg, welcher eine radiale kollektive Anregung des Systems vermuten lässt.
Die transversalen Massenspektren der leichten Fragmente werden unter der Annahme eines thermalisierten Systems mit Boltzmann-Funktionen angepasst. Daraus werden die effektiven Temperaturen von Teff,Deuteronen = (139,5 ± 34,9) MeV und Teff,T ritonen = (247,9 ± 62,0) MeV extrahiert, was die Annahme von kollektivem Fluss der Teilchen zu unterstützen scheint. Vergleicht man diese Werte mit den effektiven Temperaturen der leichteren Teilchen, kann mithilfe einer linearen Funktion die kinetische Ausfriertemperatur Tkin = (74,7 ± 5,8) MeV und radiale Flussgeschwindigkeit βr = 0,37 ± 0,13 bestimmt werden. In einem zweiten Ansatz werden daher die Spektren mit Siemens-Rasmussen-Funktionen, die eine radiale Ausdehnung mit einbeziehen, angepasst und daraus die globalen Parameter T = (74 ± 7) MeV und βr = 0,36 ± 0,02 bestimmt. Diese Werte liegen an der oberen Grenze in dem für diesen Energiebereich erwarteten Bereich.
Die Siemens-Rasmussen-Funktionen liefern eine bessere Beschreibung der transversalen Massenspektren und werden zur Extrapolation der nicht abgedeckten transversalen Massenbereiche genutzt. Die Integration liefert die Verteilung der Zählrate als Funktion der Rapidität. Diese Verteilung zeigt zwei Maxima nahe Strahl- und Target-Rapidität, was im Widerspruch zu einer statischen, thermischen Quelle der Teilchen steht.
Im Rahmen dieser Arbeit wurde eine JTAG-Ansteuerung für MIMOSA26-Sensoren basierend auf FPGA-Boards entwickelt. Als VHDL-Code ist die Implementierung anpassbar. Jede JTAG-Chain wird durch einen unabhängigen JTAG-Chain-Controller angesteuert, so dass sich begrenzt durch die Zahl der I/O-Leitungen und die Ressourcen die Anzahl der JTAG-Chain-Controller auf einem FPGA einstellen lässt. Die Anpassbarkeit hat sich bereits bei der Strahlzeit am CERN im November 2012 gezeigt, für die eine Version mit drei JTAG-Chain-Controllern auf einem FPGA und Ausgängen auf einem SCSI-Kabel synthetisiert wurde. Dabei wurde die Prototyp-Frontend-Elektronik Version 1 verwendet. Außerdem ist die Größe des pro Sensor verwendeten Speichers (in Zweierpotenzen) im VHDL-Code einstellbar, um auch eventuelle zukünftige Sensoren mit größeren Registern zu unterstützen.
Aus dieser Sicht sollte die Implementierung mit kleinen Anpassungen im finalen MVD verwendbar sein, es gibt jedoch wie immer noch Verbesserungsmöglichkeiten, z.B. die Verwendung eines externen Speichers. Des Weiteren fehlt noch eine grafische Benutzeroberfläche für den finalen MVD, wobei wie bei den anderen Detektoren von CBM dazu eine Steuerung basierend auf EPICS entwickelt werden sollte, um eine einheitliche Oberfläche zu erreichen.
Auf Seiten der Elektronik für ded finalen MVD gibt es noch einige offene Fragen, vor allem bei der Entwicklung der Zuleitungen für die Sensoren. Die Signale auf den Flexprint-Kabeln zeigen bereits bei kurzen JTAG-Chains ein hohes Übersprechen (Abschnitt 9.1.2), das zu hoch werden könnte, wenn man Sensor-Module mit mehr als einem Sensor (wie für den finalen MVD geplant, siehe Kapitel 3) an das bisher verwendete Chain-FPC anschließt.. Es kann jedoch auch gut sein, dass das Übersprechen gar kein Problem darstellen wird. Prinzipiell besteht die Möglichkeit, dass sich das Übersprechen z.B. durch Einfügen einer Masseschicht in Kabel und Boards reduzieren lässt, was in Simulationen gezeigt wurde (siehe Kapitel 8). Jedoch wurden in diesen Simulationen die Steckverbinder und eventuelle Fehlanpassungen der Boards vernachlässigt, weshalb nicht sicher ist, ob bzw. wie gut sich dies praktisch umsetzen lässt. In jedem Fall stellen die betrachteten Möglichkeiten, das Übersprechen zu reduzieren, einen erhöhten Aufwand dar. Daher erscheint es sinnvoll, zuerst eine konkrete Geometrie für die Elektronik des finalen MVD zu entwerfen1, und für diese zu ermitteln, ob das Übersprechen ein Problem darstellt.
Dabei stellt sich die wichtige Frage, wie viele Sensoren auf einem Sensor-Modul mit einem einlagigen Kabel in der zur Verfügung stehenden Breite angeschlossen werden können, da mindestens vier zusätzliche Datenleitungen für jeden weiteren Sensor erforderlich sind.
Lepton pairs emerging from decays of virtual photons represent promising probes of nuclear matter under extreme conditions of temperature and density. These etreme conditions can be reached in heavy-ion collisions in various facilities around the world. Hereby the collision energy in the center-of-mass system (√SNN) varies from few GeV (SIS) to the TeV (LHC). In the energy domain of 1 - 2 GeV per nucleon (GeV/u), the HADES experiment at GSI Helmholtzzentrum für Schwerionenforschung in Darmstadt studies dielectrons and strangeness production.
Various reactions, for example collisions of pions, protons, deuterons and heavy-ions with nuclei have been studied since its installation in the year 2001. Hereby the so called DLS Puzzle was solved experimentally, with remeasuring C+C at 1 and 2 GeV/u and by careful studies of inclusive pp and pn reactions at 1.25 GeV. With these measurements the so-called reference spectrum was established. Measurements of e+ e− production Ar+KCl showed an enhancement on the dilepton spectrum above the trivial NN back-
ground. Theory predicts a strong enhancement of medium radiation with the system size, due to large production of fast decaying baryonic resonances like ∆ and N∗ . The heaviest system measured so far was Au+Au at a kinetic beam energy of 1.23 GeV/u. The precise determination of the medium radiation depends
on a precise knowledge of the underlying hadronic cocktail composed of various sources contributing to the measured dilepton spectrum. In general the medium radiation needs to be separated from contributions coming from long-lived particles, that decay after the freeze out of the system. For a more model independent
understanding of the dilepton cocktail the production cross sections of these particles need to measured independently. In the related energy regime the main contributers are π0 and η Dalitz decays. Both mesons have a dominant decay into two real photons and have been reconstructed successfully in this channel. Since HADES has no electromagnetic calorimeter the mesons can not be identified in this decay channel directly. In this thesis the capability of HADES to detect e+ e− pairs from conversions of real photons is demonstrated.
Therefore not only the conversion probability but also the resulting efficiencies are shown. Furthermore, the reconstruction method for neutral mesons will be explained and the resulting spectra are interpreted. The measurement of neutral pions is compared to the independent measured charged pion distribution, and
extrapolated to full phase space. An integrated approach is used to determine the η yield. Both measurement are compared to the world data and to theory model claculations. Finally, the measurements will be used together with the reconstructed dilepton spectra to determine the amount and the properties of in medium radiation in the Au+Au system.
High-energetic heavy-ion collisions offer the unique opportunity to produce and to study dense nuclear matter in the laboratory. The future Facility for Antiproton and Ion Research (FAIR) in Darmstadt, Germany, will provide beams of heavy nuclei up to kinetic energies of 11 GeV/nucleon. At these energies, the nuclear matter in the collision zone of two nuclei will be compressed to densities of up to 5 − 10 times the saturation density of atomic nuclei, similar to matter densities existing in the core of massive neutron stars. Under those conditions, nucleons are expected to melt and form a new state of matter, which consists of quarks and gluons, the so called Quark-Gluon Plasma (QGP). The search for such a phase transition from hadronic to partonic matter, and the exploration of the nuclear matter equation-of-state at high densities are the major goals of heavy ion experiments worldwide.
The observables, which are proposed to probe the properties of dense nuclear matter and possible phase transitions, include multi-strange hyperons, antibaryons, lepton pairs, collective flow of identified particles, fluctuations and correlations of various particles, particles containing charm quarks, and hypernuclei. These observables have to be measured in multi-dimensions, i.e. as function of collision centrality, rapidity, transverse momentum, energy, emission angle, etc., which requires extremely high statistics. Moreover, some of these particles are produced very rarely.
Therefore, the Compressed Baryonic Matter (CBM) experiment at FAIR is designed to run at collision rates of up to 10 MHz, in order to perform measurements with unprecedented precision. Due to the complicated decay topology of many observables, no hardware trigger can be applied, and the data have to be analysed online in order to filter out the interesting events.
This strategy requires free-streaming read-out electronics, which provides time stamps to all detector signals, a high performance computer center, and high-speed reconstruction algorithms, which provide an online track and event reconstruction based on time and position information of the detector hits (”4-D“ reconstruction).
The core detector of the CBM experiment is the Silicon Tracking System (STS). The main task of the STS is to provide track reconstruction and momentum de- termination of charged particles originating from beam-target interactions. To fulfil the whole tasks the STS is located in the large gap of a superconducting dipole magnet with a bending power of 1 Tm providing momentum measurements for charged particles. The STS comprises 8 detector stations, which are positioned from 30 cm to 100 cm downstream the target. The corresponding active area of the stations grows up from 40×50 cm 2 up to 100×100 cm 2 with a totalarea of 4 m2. The silicon double-sided sensors exhibit 1024 strips on each side with a stereo angle at p-side of 7.5 ◦ and a strip pitch of 58 μm. The strip length ranges from 2 cm for sensors located in a close vicinity to the beam axis, up to 12 cm for other sensors where the flux of the reaction products drops down substantially. In total, the STS consist of 896 sensors mounted on 106 detector ladders. The detector readout electronics dissipates 40 kW and will be equipped with a CO 2 bi-phase cooling system. The detector including electronics will be mounted in a thermal enclosure to allow for sensor operation at below −5 ◦ C which minimizes radiation induced leakage currents.
The task of the STS is to measure the trajectories of up to 800 charged particles per collision with an efficiency of more than 95% and a momentum resolution of 1 − 2%. In order to guarantee the required performance over the full lifetime of the CBM experiment, the detector system has to have a low material budget, a high granularity, a high signal-to-noise (SNR) ratio, and a high radiation tolerance. As a result of optimisation studies, the STS consists of double-sided silicon microstrip sensors, about 300 μm thick, which have to provide a SNR ratio of more than 10, even after radiation with the expected equivalent lifetime fluence of 10 14 1 MeV n eq cm −2.
This thesis is devoted to the characterization of double-sided silicon microstrip sensors with an emphasis on investigation of their radiation hardness. Different prototypes of double sided silicon sensors produced by two vendors have been irradiated by 23 MeV protons up to the double life time fluence for the CBM experiment (2 × 10 14 1 MeV n eq cm −2 ).
The sensor properties have been characterised before and after irradiation. It was found, that after irradiation with a double lifetime fluence the leakage current increased 1000 times, which results in an increased shot noise. Moreover, the relative charge collection efficiency of irradiated with respect to non-irradiated sensors drops down to 85% for the lifetime equivalent fluence, and down to 73% for the double lifetime fluence, both for the p-side and n-side. For non-irradiated sensors the SNR was found to be in the range of 20 − 25, whereas for irradiated sensors it dropped down to 12 − 17.
In addition to the sensor characterization, a part of this thesis was devoted to the optimisation of the sensor readout scheme. In order to investigate the possible increase of SNR, and to reduce the number of readout channels in the outer aperture of STS, three versions of routing lines have been realized for the p-side readout of the sensor prototype, and have been tested in the laboratory and under beam conditions.
The tests have been performed with different inclination angles between beam direction and sensor surface, corresponding to the polar angle acceptance of the CBM experiment, which is from 2.5 ◦ to 25 ◦.
As a result of the studies carried out in this thesis work, the radiation hardness of the double-sided silicon microstrip sensors developed for the CBM STS detector was confirmed. Also the advantage of individual read-out of sensor channels in the lateral regions of the detector was verified. This allowed to start the tendering process for sensor series production in industry, an important step towards the construction of the detector in the coming years.
The Compressed Baryonic Matter (CBM) Experiment will investigate heavy ion collisions and reactions at interaction rates of 100 kHz in a targeted energy range of up to 11 AGeV for systems such as gold-gold or lead-lead. It will be one of the major scientific experiments of the Facility for Antiproton and Ion Research in Europe (FAIR) currently under construction at the site of the GSI Helmholtzzentrum für Schwerionenforschung (GSI) in Darmstadt, Germany. CBM is going to be a fixed target experiment consisting of a superconducting magnet, multiple detectors of various types, and high-performance computing for online event reconstruction and selection. The detector closest to the interaction point of the experiment will be the Micro Vertex Detector (MVD). Consisting of four planar stations equipped with custom CMOS pixel sensors, it will allow to reconstruct the primary vertex with high precision and will help to reconstruct secondary vertices and identify particles originating from conversion in the detector material.
Due to the high interaction rates foreseen for CBM, understanding and minimizing systematic errors due to the detectors’ operating conditions will become all the more important to obtain significant measurement results, as statistical errors in the measurements of many observables are diminishing due to the enormous amount of data available.
Furthermore, the MVD will be the first detector based on CMOS pixel sensors used in a large physics experiment, that will be operated in vacuum. As a result, many aspects of the mechanical and electrical integration of the detector require careful testing and validation.
This thesis addresses both those challenges specifically for the Micro Vertex Detector with the development of a control system for the operation and validation of the MVD prototype “PRESTO” in vacuum. The prototype was selected as device under test as the final MVD is not yet built.
The developed control system helps a) to operate the prototype safely and keep it at the desired working point and b) to record important time-series data of the state of the detector prototype. Those two aspects allow the control system (which might later serve as a ‘blueprint’ for the final detector) to minimize the mentioned systematic errors as much as possible and to contribute to the understanding of remaining systematic errors using correlations with the time-series data. The controlled operation of the prototype in vacuum allowed to validate the integration concepts from a wide range of mechanical and electrical aspects in an endurance test for more than a year with 24/7 operation.
The prototype for this study itself was named “PRESTO” (standing for ‘PREcursor of the Second sTatiOn of the CBM-MVD’). It represents one quadrant of an MVD detector plane, equipped with a total of 15 MIMOSA-26 sensors on the front and back side of a carrier plate. Within this thesis, major parts of the prototype itself were designed. Custom ultra-thin flat flexible cables for data and power were designed and validated. Furthermore, the CNC-machined Aluminium heatsink to mount and cool the prototype design was refined to increase thermal performance. A custom vacuum feedthrough for a total of 21 flat ribbon cables was designed and fabricated. The read-out chain for MIMOSIS-26 was extended to cover a total of 8 sensors with a single and newer TRB-3 FPGA board and was set-up with the prototype. Vacuum equipment including chambers, hoses, pumps, valves and gauges were integrated to form a large vacuum testing system. A cooling circuit for the prototype was assembled comprising an external chiller, hoses, vacuum feedthroughs, as well as temperature, flow and pressure sensors.
The control system was developed to serve the needs of the prototype, while taking the requirements of the final MVD already into account. The main design goals of the control system are:
• compatibility with the other detectors and the overall CBM experiment,
• access to real-time measurements of all necessary parameters (‘process values’),
• reliable, fail-safe operation of the detector,
• recording of all time-series data (‘archiving’),
• cost efficiency and acceptance within the physics community,
• good usability for the users (‘operators’),
• long-term maintainability.
The recorded time-series data of the process variables (i.e. sensor readings) allow a post-measurement analysis of variations in the detector performance. The longterm archiving of all relevant system parameters is therefore of outstanding importance, which is why the software intended for this purpose – called “archiver” – was given special attention in this thesis.
For this reason in particular, it is necessary to implement a comprehensive control system that allows the detector to be operated safely under these conditions and cooled effectively. Before the start of this doctoral thesis, vigilant and extensively trained operators were always necessary for this. The control system that has been developed makes it possible that, after basic training, the detector can also be operated by a less specialised shift supervisor during measurement campaigns.
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Starting from the first observation of the halo phenomenon 20 years ago, more and more neutron-rich light nuclei were observed. The study of unstable nuclear systems beyond the dripline is a relatively new branch of nuclear physics. In the present work, the results of an experiment at GSI (Darmstadt) with relativistic beams of the halo nuclei 8He, 11Li and 14Be with energies of 240, 280 and 305 MeV/nucleon, respectively, impinging on a liquid hydrogen target are discussed. Neutron/proton knockout reactions lead to the formation of unbound systems, followed by their immediate decay. The experimental setup, consisting of the neutron detector LAND, the dipole spectrometer ALADIN and different types of tracking detectors, allows the reconstruction of the momentum vectors of all reaction products measured in coincidence. The properties of unbound nuclei are investigated by reconstructing the relative-energy spectra as well as by studying the angular correlations between the reaction products. The observed systems are 9He, 10He, 10Li, 12Li and 13Li. The isotopes 12Li and 13Li are observed for the first time. They are produced in the 1H(14Be, 2pn)12Li and 1H(14Be, 2p)13Li knockout reactions. The obtained relative-energy spectrum of 12Li is described as a single virtual s-state with a scattering length of as = -22;13.7(1.6) fm. The spectrum of 13Li is interpreted as a resonance at an energy of Er = 1.47(13) MeV and a width of Gamma ~ 2 MeV superimposed on a broad correlated background distribution. The isotope 10Li is observed after one-neutron knockout from the halo nucleus 11Li. The obtained relative-energy spectrum is described by a low-lying virtual s-state with a scattering length as = -22.4(4.8) fm and a p-wave resonance with Er = 0.566(14) MeV and Gamma = 0.548(30) MeV, in agreement with previous experiments. The observation of the nucleus 8He in coincidence with one or two neutrons, as a result of proton knockout from 11Li, allows to reconstruct the relative-energy spectra for the heavy helium isotopes, 9He and 10He. The low-energy part of the 9He spectrum is described by a virtual s-state with a scattering length as = -3.16(78) fm. In addition, two resonance states with l 6= 0 at energies of 1.33(8) and 2.4 MeV are observed. For the 10He spectrum, two interpretations are possible. It can be interpreted as a superposition of a narrow resonance at 1.42(10) MeV and a broad correlated background distribution. Alternatively, the spectrum is being well described by two resonances at energies of 1.54(11) and 3.99(26) MeV. Additionally, three-body energy and angular correlations in 10He and 13Li nuclei at the region of the ground state (0 < ECnn < 3 MeV) are studied, providing information about structure of these unbound nuclear systems.
QCD matter is expected to exist in different phases, when heated to high temperatures and getting highly compressed. Each phase could be characterized by distinct properties. A way to access extreme phases of matter in the laboratory are heavy-ion collisions at (ultra-)relativistic energies. During the collision, the temperature and density is evolving and reaches a maximum temperature and density far beyond the ground state of matter. The matter properties depend on the incident collision energy. Typically, a collision is separated into three collisions stages, namely first chance collisions (I), hot and dense stage (II) and freeze-out stage (III). Out of those, the second one is of major interest, since the extreme states of matter are generated within. For this reason, the most prominent change of the hadrons is expected to appear there in. Those changes are caused by i.e. modification of the hadronic spectral function. However, to retrieve such information is complicated. Hadrons are strongly interacting particles and therefore, carry little information about the hot and dense stage. For that purpose, decays of hadrons (low-mass vector mesons) to e+e- pairs via a virtual photon, so-called dielectrons, are an ideal probe. Electrons and positrons do not interact strongly and transport the information about the hot and dense stage nearly undisturbed to the detector. Unfortunately, the production of dielectrons is suppressed by a branching ratio of ≈ 10^(-5) and requires a precise lepton identification. Nonetheless, previous experiments have extracted a dilepton signal and observed in the low-mass range an excess over the hadronic cocktail. Latter one is expected to be caused by thermal radiation induced by the medium. Up to now, experiments conducted dilepton measurements with a focus on larger collision energies and large collision systems. Measurements of dielectrons at collision energies of around 1-2A GeV were only conducted for small and medium size collision systems. HADES continued the systematic studies by a measurement of Au+Au collisions at 1.23A GeV.
The detection of dielectrons requires detectors that handle high data rates and specific detectors for a high purity lepton identification. In HADES, the strongest separation of electrons or positrons from the hadronic background is provided by a ring imaging Cherenkov detector (RICH). Its electron identification is based on Cherenkov photons, that are emitted in ring like patterns. In this work a new approach, using the time-of-flight information to preselect electrons and the reconstructed particle trajectory to estimate ring positions, is utilized to improve the lepton identification. The concept of the so-called backtracking algorithm will be explained and applied to e+e- identification in Au+Au collisions. The whole analysis chain comprises single lepton identification, pair reconstruction and correction for efficiency and acceptance losses. The final pair spectra will be presented in form of their invariant mass, pt, mt and helicity distributions. Subsequently, transport model calculations as well as results from the recently developed coarse-grained transport approach will be compared to the dielectron spectra. Moreover, the centrality dependence of the excess yield and true (not "blue-shifted") temperature of the fireball will be presented. The results will be put in context to measurements of lighter collisions systems and at higher energies.
The mission of the Compressed Baryonic Matter (CBM) experiment is to investigate the phase diagram of strongly interacting matter in the region of high net-baryon densities and moderate temperatures. According to various transport models, matter densities of more than 5 times saturation density can be reached in collisions between gold nuclei at beam energies between 5 and 11 GeV per nucleon, which will be available at FAIR. The core detector of the CBM experiment is the Silicon Tracking System (STS), which is used to measure the tracks of up to 700 particles per collision with high efficiency (>95%) and good momentum resolution (<1.5%). The technological and experimental challenge is to realize a detector system with very low material budget, in order to reduce multiple scattering of the particles, and a free-streaming data readout chain, in order to achieve reaction rates up to 10 MHz together with an online event reconstruction and selection.
The STS comprises 8 tracking stations positioned between 30 cm and 100 cm downstream the target inside a magnetic field, covering polar emission angles up to 25 degrees. A station consists of vertical structures with increasing number (between 8 and 16, depending on station number), each structure carrying between 2 and 10 double-sided microstrip silicon sensors, which are connected through low-mass microcables to the readout electronics placed at the detector periphery outside the active detector area.
The work presented in this thesis focuses on the detector performance simulation and local hit pattern reconstruction in the STS. For efficient detector design and reconstruction performance, a reliable detector response model is of utmost importance. Within this work, a realistic detector response model was designed and implemented in the CBM software framework. The model includes non-uniform energy loss of an incident particle within a sensor, electric field of a planar p-n junction, Lorentz shift of the charge carriers, their diffusion, and the influence of parasitic capacitances. The developed model has been verified with experimental data from detector tests in a relativistic proton beam. Cluster size distributions at different beam incident angles are sensitive to charge sharing effects and were chosen as an observable for the verification. Taking into account parasitic capacitances further improves the agreement with measured data.
Using the developed detector response model, the cluster position finding algorithm was improved. For two-strip clusters, a new, unbiased algorithm has been developed, which gives smaller residuals than the Centre-Of-Gravity algorithm. For larger clusters, the head-tail algorithm is used as the default one. For an estimate of the track parameters, the Kalman Filter based track fit requires not only hit positions but their uncertainties as an input. A new analytic method to estimate the hit position errors has been designed in this work. It requires as input neither measured spatial resolution nor information about an incident particle track. The method includes all the sources of uncertainties independently, namely: the cluster position finding algorithm itself, the non-uniform energy loss of incident particles, the electronics noise, and the discretisation of charge in the readout chip.
The verification with simulations shows improvements in hit and track pull distributions as well as x²-distributions in comparison to the previous simple approach. The analytic method improves the track parameters reconstruction by 5-10%.
Several STS module prototypes have been tested in a relativistic proton beam. A signal to-noise ratio was obtained at the level of 10-15 for modules made of 30 cm long microcable and of either one or two 6.2 x 6.2 cm² CiS sensors.
First simulations have shown that this signal-to-noise ratio is sufficient to reach the required efficiency and momentum resolution. The high-radiation environment of CBM operation will deteriorate the sensor performance. Radiation hardness of sensors has been studied in the beam with sensors irradiated to 2 x 10[hoch 14] 1MeV [neq/cm²], twice the lifetime dose expected for CBM operation. Charge collection efficiency drops by 17-25%, and simultaneously noise levels increase 1.5-1.75 times. The simulations show that if all sensors in the STS setup are exposed to such a fluence uniformly, the track reconstruction efficiency drops from 95.5% to 93.2% and the momentum resolution degrades from 1.6% to 1.7%.
In this thesis, the emission of protons as well as the production of Λ hyperons, Κ0S mesons and 3ΛH hypernuclei are analyzed multi-differentially as a function of transverse momentum, rapidity and centrality. Therefore, the 3.03 billion 30 % most central Ag(1.58A GeV)+Ag events recorded by HADES are used. Furthermore, the lifetimes of Λ hyperons, Κ0S mesons and 3ΛH hypernuclei are measured. The obtained 3ΛH lifetime of (253 ± 24 ± 42) ps is compatible with the lifetime of free Λ hyperons, as predicted by theoretic calculations due to its low binding energy. Finally, also the double strange Ξ– hyperons are reconstructed. Unfortunately, the fully optimized signals lie below the confidence threshold of 5σ, which is why both an production rate and an upper production limit are estimated using averaged acceptance and efficiency corrections. Never before, 3ΛH or Ξ– were successfully reconstructed and analyzed in heavy-ion collisions at such low energies. The obtained results are compared to previous measurements and put in context with world data form different energies and collision systems.
In this thesis, the flow coefficients vn of the orders n = 1 − 6 are studied for protons and light nuclei in Au+Au collisions at Ebeam = 1.23 AGeV, equivalent to a center-of-mass energy in the nucleon-nucleon system of √sNN = 2.4 GeV. The detailed multi-differential measurement is performed with the HADES experiment at SIS18/GSI. HADES, with its large acceptance, covering almost full azimuth angle, combined with its high mass-resolution and good particle-identification capability, is well equipped to study the azimuthal flow pattern not only for protons, deuterons, and tritons but also for charged pions, kaons, the φ-mesons, electrons/positrons, as well as light nuclei like helions and alphas. The high statistics of more than seven billion Au-Au collisions recorded in April/May 2012 with HADES enables for the first time the measurement of higher order flow coefficients up to the 6th harmonic. Since the Fourier coefficient of 7th and 8th order are beyond the statistical significance only an upper bound is given. The Au+Au collision system is the largest reaction system with the highest particle multiplicities, which was measured so far with HADES. A dedicated correction method for the flow measurement had to be developed to cope with the reconstruction in-efficiencies due to occupancies of the detector system. The systematical bias of the flow measurement is studied and several sources of uncertainties identified, which mainly arise from the quality selection criteria applied to the analyzed tracks, the correction procedure for reconstruction inefficiencies, the procedures for particle identification (PID) and the effects of an azimuthally non-uniform detector acceptance. The systematic point-to-point uncertainties are determined separately for each particle type (proton, deuteron and triton), the order of the flow harmonics vn, and the centrality class. Further, the validity of the results is inspected in the range of their evaluated systematic uncertainties with several consistency checks. In order to enable meaningful comparisons between experimental observations and predictions of theoretical models, the classification of events should be well defined and in sufficiently narrow intervals of impact parameter. Part of this work included the implementation of the procedure to determine the centrality and orientation of the reaction.
In the conclusion the experimental results are discussed, including various scaling properties of the flow harmonics. It is found that the ratio v4/v2 for protons and light nuclei (deuterons and tritons) at midrapidity for all centrality classes approaches values close to 0.5 at high transverse momenta, which was suggested to be indicative for an ideal hydrodynamic behaviour. A remarkable scaling is observed in the pt dependence of v2 (v4) at mid-rapidity of the three hydrogen isotopes, when dividing by their nuclear mass number A (A^2) and pt by A. This is consistent with naive expectations from nucleon coalescence, butraises the question whether this mass ordering can also be explained by a hydrodynamical-inspired approach, like the blast-wave model. The relation of v2 and v4 to the shape of the initial eccentricity of the collision system is studied. It is found that v2 is independent of centrality for all three particle species after dividing it by the averaged second order participant eccentricity v2/⟨ε2⟩. A similar scaling is shown for v4 after division by ⟨ε2⟩^2.
The Compressed Baryonic Matter (CBM) is one of the core experiments at the future Facility for Anti-proton and Ion Research (FAIR), Darmstadt, Germany. Its goal is to investigate nuclear matter characteristics at high net-baryon densities and moderate temperatures. The Silicon Tracking System (STS) is a central detector system of CBM.
It is placed inside a 1Tm magnet and operated at a temperature of about −10 °C to keep radiation-induced bulk current in the 300μm double-sided microstrip silicon sensors low. The design of the STS aims to minimize the material budget in the detector acceptance (2.5° < θ < 25°). In order to do so, the readout electronics is placed outside the active area, and the analog signals are transported via ultra-thin micro-cables. The STS comprises eight tracking stations with 876 modules. Each module is assembled on a carbon fiber ladder, which is subsequently mounted in the C-shaped aluminum frame.
The scope of the thesis focused on developing a modular control system framework that can be implemented for different sizes of experimental setups. The developed framework was used for setups that required a remote operation, like the irradiation of the powering modules for the front-end electronics (FEE), but also in laboratory-based setups where the automation and archiving were needed (thermal cycling of the STS electronics).
The low voltage powering modules will be placed in the vicinity of the experiment, therefore they will experience a total dose of up to 40mGy over the 10 years of STS lifetime.
To estimate the effects of the radiation on the low-voltage module performance, a dedicated irradiation campaign took place. It aimed at estimating the rate of radiation induced soft errors, that lead to the switch off of the FEE.
Regular power cycles of multiple front-end boards (FEBs) pose a risk to the experiment operation. Firstly, such behavior could negatively influence the physics performance but also have deteriorating effects on the hardware. It was further assessed what are the limitations of the FEBs with respect to the thermal cycling and the mechanical stress. The results served as an indication of possible failure modes of the FEB at the end of STS lifetime. Failure modes after repeated cycles and potential reasons were determined (e.g., Coefficient of Thermal Expansion (CTE) difference between the materials).
Due to the conditions inside the STS efficient temperature and humidity monitoring and control are required to avoid icing or water condensation on the electronics or silicon sensors. The most important properties of a suitable sensor candidate are resilience to the magnetic field, ionizing radiation tolerance, and fairly small size.
A general strategy for ambient parameters monitoring inside the STS was developed, and potential sensor candidates were chosen. To characterize the chosen relative humidity sensors the developed control framework was introduced. A sampling system with a ceramic sensor and Fiber Optic Sensors (FOS) were identified as reliable solutions for the distributed sensing system. Additionally, the industrial capacitive sensors will be used as a reference during the commissioning.
Two different designs of FOS were tested: a hygrometer and 5 sensors multiplexed in an array. The FOS hygrometer turned out to be a more reliable solution. One of the possible reasons for a worse performance is a relatively low distance between the subsequent sensors (15 cm) and a thicker coating. The results obtained from the time response study pointed out that the thinner coating of about 15μm should be a good compromise between the humidity sensitivity and the time response.
The implementation of the containerized-based control system framework for the mSTS is described in detail. The deployed EPICS-based framework proved to be a reliable solution and ensured the safety of the detector for almost 1.5 years. Moreover, the data related to the performance of the detector modules were analyzed and significant progress in the quality of modules was noted. Obtained data was also used to estimate the total fluence, which was based on the leakage current changes.
The developed framework provided a unique opportunity to automate and control different experimental setups which provided crucial data for the STS. Furthermore, the work underlines the importance of such a system and outlines the next steps toward the realization of a reliable Detector Control System for STS.
This work focuses on the investigation of K+, K- and ϕ-meson production in Ag(1.58 A GeV)+Ag collisions. The energetically cheapest channel for direct K+ production in binary NN-collisions NN→NΛK+ lies at exactly this energy. For the remaining K- and ϕ-mesons, an excess energy of 0.31 GeV and 0.34 GeV in the centre of mass system has to be provided by the system. This makes these particles an excellent probe for effects inside the medium.
K+ and K- mesons can be reconstructed directly as they possess a cτ of approximately 3.7 m. Using the approximately 3 billion recorded Ag(1.58 A GeV)+Ag 0-30% most central collision events, all reconstructed K+ and K- within the detector acceptance are investigated for their kinematic properties and their particle production rates compared to a selection of existing models.
The search for a modification of hadron properties inside nuclear matter at normal and/or high temperature and density is one of the more interesting issues of modern nuclear physics. Dilepton experiments, by providing interesting results, give insight into the properties of strong interaction and the nature of hadron mass generation. One of these research tools is the HADES spectrometer. HADES is a high acceptance dilepton spectrometer installed at the heavy-ion synchrotron (SIS) at GSI, Darmstadt. The main physics motivation of HADES is the measurement of e+e- pairs in the invariant-mass range up to 1 GeV/c2 in pion- and proton-induced reactions, as well as in heavy-ion collisions. The goal is to investigate the properties of the vector mesons rho, omega and of other hadrons reconstructed from e+e- decay pairs. Dileptons are penetrating probes allowing to study the in-medium properties of hadrons. However, the measurement of such dilepton pairs is difficult because of a very large background from other processes in which leptons are created. This thesis presents the analysis of the data provided by the first physic run done with the HADES spectrometer. For the first time e+e- pairs produced in C+C collisions at an incident energy of 2 GeV per nucleon have been collected with sufficient statistics. This experiment is of particular importance since it allows to address the puzzling pair excess measured by the former DLS experiment at 1.04 AGeV. The thesis consists of five chapters. The first chapter presents the physics case which is addressed in the work. In the second chapter the HADES spectrometer is introduced with the characteristic of specific detectors which are part of the spectrometer. Chapter three focusses on the issue of charged-particle identification. The fourth chapter discusses the reconstruction of the di-electron spectra in C+C collisions. In this part of the thesis a comparison with theoretical models is included as well. The conclusion and final remarks are given in chapter five.