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Volatility clustering and fat tails are prominently observed in financial markets. Here, we analyze the underlying mechanisms of three agent-based models explaining these stylized facts in terms of market instabilities and compare them on empirical grounds. To this end, we first develop a general framework for detecting tail events in stock markets. In particular, we introduce Hawkes processes to automatically identify and date onsets of market turmoils which result in increased volatility. Second, we introduce three different indicators to predict those onsets. Each of the three indicators is derived from and tailored to one of the models, namely quantifying information content, critical slowing down or market risk perception. Finally, we apply our indicators to simulated and real market data. We find that all indicators reliably predict market events on simulated data and clearly distinguish the different models. In contrast, a systematic comparison on the stocks of the Forbes 500 companies shows a markedly lower performance. Overall, predicting the onset of market turmoils appears difficult, yet, over very short time horizons high or rising volatility exhibits some predictive power.
With increasing heterogeneity of modern hardware, different requirements for 3d applications arise. Despite the fact that real-time rendering of photo-realistic images is possible using today’s graphics cards, still large computational effort is required. Furthermore, smart-phones or computers with older, less powerful graphics cards may not be able to reproduce these results. To retain interactive rendering, usually the detail of a scene is reduced, and so less data needs to be processed. This removal of data, however, may introduce errors, so called artifacts. These artifacts may be distracting for a human spectator when gazing at the display. Thus, the visual quality of the presented scene is reduced. This is counteracted by identifying features of an object that can be removed without introducing artifacts. Most methods utilize geometrical properties, such as distance or shape, to rate the quality of the performed reduction. This information used to generate so called Levels Of Detail (LODs), which are made available to the rendering system. This reduces the detail of an object using the precalculated LODs, e.g. when it is moved into the back of the scene. The appropriate LOD is selected using a metric, and it is replaced with the current displayed version. This exchange must be made smoothly, requiring both LOD-versions to be drawn simultaneously during a transition. Otherwise, this exchange will introduce discontinuities, which are easily discovered by a human spectator. After completion of the transition, only the newly introduced LOD-version is drawn and the previous overhead removed. These LOD-methods usually operate with discrete levels and exploit limitations of both the display and the spectator: the human.
Humans are limited in their vision. This ranges from being unable to distinct colors at varying illumination scenarios to the limitation to focus only at one location at a time. Researchers have developed many applications to exploit these limitations to increase the quality of an applied compression. Some popular methods of vision-based compression are MPEG or JPEG. For example, a JPEG compression exploits the reduced sensitivity of humans regarding color and so encodes colors with a lower resolution. Also, other fields, such as auditive perception, allow the exploitation of human limitations. The MP3 compression, for example, reduces the quality of stored frequencies if other frequencies are masking it. For representation of perception various computer models exist. In our rendering scenario, a model is advantageous that cannot be influenced by a human spectator, such as the visual salience or saliency.
Saliency is a notion from psycho-physics that determines how an object “pops out” of its surrounding. These outstanding objects (or features) are important for the human vision and are directly evaluated by our Human Visual System (HVS). Saliency combines multiple parts of the HVS and allows an identification of regions where humans are likely to look at. In applications, saliency-based methods have been used to control recursive or progressive rendering methods. Especially expensive display methods, such as pathtracing or global illumination calculations, benefit from a perceptual representation as recursions or calculations can be aborted if only small or unperceivable errors are expected to occur. Yet, saliency is commonly applied to 2d images, and an extension towards 3d objects has only partially been presented. Some issues need to be addressed to accomplish a complete transfer.
In this work, we present a smart rendering system that not only utilizes a 3d visual salience model but also applies the reduction in detail directly during rendering. As opposed to normal LOD-methods, this detail reduction is not limited to a predefined set of levels, but rather a dynamic and continuous LOD is created. Furthermore, to apply this reduction in a human-oriented way, a universal function to compute saliency of a 3d object is presented. The definition of this function allows to precalculate and store object-related visual salience information. This stored data is then applicable in any illumination scenario and allows to identify regions of interest on the surface of a 3d object. Unlike preprocessed methods, which generate a view-independent LOD, this identification includes information of the scene as well. Thus, we are able to define a perception-based, view-specific LOD. Performance measures of a prototypical implementation on computers with modern graphic cards achieved interactive frame rates, and several tests have proven the validity of the reduction.
The adaptation of an object is performed with a dynamic data structure, the TreeCut. It is designed to operate on hierarchical representations, which define a multi-resolution object. In such a hierarchy, the leaf nodes contain the highest detail while inner nodes are approximations of their respective subtree. As opposed to classical hierarchical rendering methods, a cut is stored and re-traversal of a tree during rendering is avoided. Due to the explicit cut representation, the TreeCut can be altered using only two core operations: refine and coarse. The refine-operation increases detail by replacing a node of the tree with its children while the coarse-operation removes the node along with its siblings and replaces them with their parent node. These operations do not rely on external information and can be performed in a local manner. These only require direct successor or predecessor information. Different strategies to evolve the TreeCut are presented, which adapt the representation using only information given by the current cut. These evaluate the cut by assigning either a priority or a target-level (or bucket) to each cut-node. The former is modelled as an optimization problem that increases the average priority of a cut while being restricted in some way, e.g. in size. The latter evolves the cut to match a certain distribution. This is applied in cases where a prioritization of nodes is not applicable. Both evaluation strategies operate with linear time complexity with respect to the size of the current TreeCut.
The data layout is chosen to separate rendering data and hierarchy to enable multi-threaded evaluation and display. The object is adapted over multiple frames while the rendering is not interrupted by the used evaluation strategy. Therefore, we separate the representation of the hierarchy from the rendering data. Due to its design, this overhead imposed to the TreeCut data structure does not influence rendering performance, and a linear time complexity for rendering is retained. The TreeCut is not only limited to alter geometrical detail of an object. The TreeCut has successfully been applied to create a non-photo-realistic stippling display, which draws the object with equal sized points in varying density. In this case the bucket-based evaluation strategy is utilized, which determines the distribution of the cut based on local illumination information. As an alternative, an attention drawing mechanism is proposed, which applies the TreeCut evaluation strategies to define the display style of a notification icon. A combination of external priorities is used to derive the appropriate icon version. An application for this mechanism is a messaging system that accounts for the current user situation.
When optimizing an object or scene, perceptual methods allow to account for or exploit human limitations. Therefore, visual salience approaches derive a saliency map, which encodes regions of interest in a 2d map. Rendering algorithms extract importance from such a map and adapt the rendering accordingly, e.g. abort a recursion when the current location is unsalient. The visual salience depends on multiple factors including the view and the illumination of the scene. We extend the existing definition of the 2d saliency and propose a universal function for 3d visual salience: the Bidirectional Saliency Weight Distribution Function (BSWDF). Instead of extracting the saliency from 2d image and approximate 3d information, we directly compute this information using the 3d data. We derive a list of equivalent features for the 3d scenario and add them to the BSWDF. As the BSWDF is universal, also 2d images are covered with the BSWDF, and the calculation of the important regions within images is possible.
To extract the individual features that contribute to visual salience, capabilities of modern graphics card in combination with an accumulation method for rendering is utilized. Inspired from point-based rendering methods local features are summed up in a single surface element (surfel) and are compared with their surround to determine whether they “pop out”. These operations are performed with a shader-program that is executed on the Graphics Processing Unit (GPU) and has direct access to the 3d data. This increases processing speed because no transfer of the data is required. After computation, each of these object-specific features can be combined to derive a saliency map for this object. Surface specific information, e.g. color or curvature, can be preprocessed and stored onto disk. We define a sampling scheme to determine the views that need to be evaluated for each object. With these schemes, the features can be interpolated for any view that occurs during rendering, and the according surface data is reconstructed. These sampling schemes compose a set of images in form of a lookup table. This is similar to existing rendering techniques, which extract illumination information from a lookup. The size of the lookup table increases only with the number of samples or the image size used for creation as the images are of equal size. Thus, the quality of the saliency data is independent of the object’s geometrical complexity. The computation of a BSWDF can be performed either on a Central Processing Unit (CPU) or a GPU, and an implementation requires only a few instructions when using a shader program. If the surface features have been stored during a preprocess, a reprojection of the data is performed and combined with the current information of the object. Once the data is available, the computation of the saliency values is done using a specialized illumination model, and a priority for each primitive is extracted. If the GPU is used, the calculated data has to be transferred from the graphics card. We therefore use the “transform feedback” capabilities, which allow high transfer rates and preserve the order of processed primitives. So, an identification of regions of interest based on the currently used primitives is achieved. The TreeCut evaluation strategies are then able to optimize the representation in an perception-based manner.
As the adaptation utilizes information of the current scene, each change to an object can result in new visual salience information. So, a self-optimizing system is defined: the Feedback System. The output generated by this system converges towards a perception-optimized solution. To proof the saliency information to be useful, user tests have been performed with the results generated by the proposed Feedback System. We compared a saliency-enhanced object compression to a pure geometrical approach, common for LOD-generation. One result of the tests is that saliency information allows to increase compression even further as possible with the pure geometrical methods. The participants were not able to distinguish between objects even if the saliency-based compression had only 60% of the size of the geometrical reduced object. If the size ratio is greater, saliency-based compression is rated, on average, with higher score and these results have a high significance using statistical tests. The Feedback System extends an 3d object with the capability of self-optimization. Not only geometrical detail but also other properties can be limited and optimized using the TreeCut in combination with a BSWDF. We present a dynamic animation, which utilizes a Software Development Kit (SDK) for physical simulations. This was chosen, on the one hand, to show the universal applicability of the proposed system, and on the other hand, to focus on the connection between the TreeCut and the SDK. We adapt the existing framework, and include the SDK within our design. In this case, the TreeCut-operations not only alter geometrical but also simulation detail. This increases calculation performance because both the rendering and the SDK operate on less data after the reduction has been completed.
The selected simulation type is a soft-body simulation. Soft-bodies are deformable in a certain degree but retain their internal connection. An example is a piece of cloth that smoothly fits the underlying surface without tearing apart. Other types are rigid bodies, i.e. idealistic objects that cannot be deformed, and fluids or gaseous materials, which are well suited for point-based simulations. Any of these simulations scales with the number of simulation nodes used, and a reduction of detail increases performance significantly. We define a specialized BSWDF to evaluate simulation specific features, such as motion. The Feedback System then increases detail in highly salient regions, e.g. those with large motion, and saves computation time by reducing detail in static parts of the simulation. So, detail of the simulation is preserved while less nodes are simulated.
The incorporation of perception in real-time rendering is an important part of recent research. Today, the HVS is well understood, and valid computer models have been derived. These models are frequently used in commercial and free software, e.g. JPEG compression. Within this thesis, the Tree-Cut is presented to change the LOD of an object in a dynamic and continuous manner. No definition of the individual levels in advance is required, and the transitions are performed locally. Furthermore, in combination with an identification of important regions by the BSWDF, a perceptual evaluation of a 3d object is achieved. As opposed to existing methods, which approximate data from 2d images, the perceptual information is directly acquired from 3d data. Some of this data can be preprocessed if necessary, to defer additional computations during rendering. The Feedback System, created by the TreeCut and the BSWDF, optimizes the representation and is not limited to visual data alone. We have shown with our prototype that interactive frame rates can be achieved with modern hardware, and we have proven the validity of the reductions by performing several user tests. However, the presented system only focuses on specific aspects, and more research is required to capture even more capabilities that a perception-based rendering system can provide.
In diesem Bericht wurde das in [Pae02] eingeführte Verfahren "GenDurchschnitt" auf die symbolischen Daten zweier Datenbanken septischer Schock-Patienten angewendet. Es wurden jeweils Generalisierungsregeln generiert, die neben einer robusten Klassifikation der Patienten in die Klassen "überlebt" und "verstorben" auch eine Interpretation der Daten ermöglichten. Ein Vergleich mit den aktuellen Verfahren A-priori und FP-Baum haben die gute Verwendbarkeit des Algorithmus belegt. Die Heuristiken führten zu Laufzeitverbesserungen. Insbesondere die Möglichkeit, die Wichtigkeit von Variablen pro Klasse zu berechnen, führte zu einer Variablenreduktion im Eingaberaum und zu der Identifikation wichtiger Items. Einige Regelbeispiele wurden für jeden Datensatz genannt. Die Frühzeitigkeit von Regeln lieferte für die beiden Datenbanken ein unterschiedliches Ergebnis: Bei den ASK-Daten treten die Regeln für die Klasse "verstorben" früher als die der Klasse "überlebt" auf; bei den MEDAN-Klinikdaten ist es umgekehrt. Eine Erklärung hierfür könnte sein, dass es sich im Vergleich zu den MEDAN-Klinikdaten bei den ASK-Daten um ein Patientenkollektiv mit einer anderen, speziellen Patientencharakteristik handelt. Anhand der Ähnlichkeit der Regeln konnten für den Anwender eine überschaubare Anzahl zuverlässiger Regeln ausgegeben werden, die möglichst unähnlich zueinander sind und somit für einen Arzt in ihrer Gesamtheit interessant sind. Assoziationsregeln und FP-Baum-Regeln erzeugen zwar kürzere Regeln, die aber zu zahlreich und nicht hinreichend sind (vgl. [Pae02, Abschnitt 4]). Zusätzlich zu der Analyse der symbolischen Daten ist auch die Analyse der metrischen MEDAN-Klinikdaten der septischen Schock-Patienten interessant. Ebenfalls ist eine Kombination der Analysen der metrischen und symbolischen Daten sinnvoll. Solche Analysen wurden ebenfalls durchgeführt; die Ergebnisse dieser Analysen werden an anderer Stelle präsentiert werden. Weitere Anwendungen der Generalisierungsregeln sind denkbar. Auch eine Verbesserung des theoretischen Fundaments (vgl. [Pae02]) erscheint sinnvoll, da erst das Zusammenspiel theoretischer und praktischer Anstrengungen zum Ziel führt.
The pT-differential inclusive production cross section of the prompt charm-strange meson Ds+ in the rapidity range |y|<0.5 was measured in proton–proton collisions at s=7 TeV at the LHC using the ALICE detector. The analysis was performed on a data sample of 2.98×108 events collected with a minimum-bias trigger. The corresponding integrated luminosity is Lint=4.8 nb−1. Reconstructing the decay Ds+→ϕπ+, with ϕ→K−K+, and its charge conjugate, about 480 Ds± mesons were counted, after selection cuts, in the transverse momentum range 2<pT<12 GeV/c. The results are compared with predictions from models based on perturbative QCD. The ratios of the cross sections of four D meson species (namely D0, D+, D⁎+ and Ds+) were determined both as a function of pT and integrated over pT after extrapolating to full pT range, together with the strangeness suppression factor in charm fragmentation. The obtained values are found to be compatible within uncertainties with those measured by other experiments in e+e−, ep and pp interactions at various centre-of-mass energies.
Die vorliegende Arbeit befasst sich mit der Generierung virtueller Organismen respektive mit der dreidimensionalen Nachbildung anatomischer Strukturen von Pflanzen, Tieren, Menschen und imaginärer Wesen per Computer. Berücksichtigt werden dabei sowohl die verschiedenen Aspekte der Visualisierung, der Modellierung, der Animation sowie der Wachstums-, Deformations- und Bewegungssimulation. Dazu wird zuerst eine umfassende State-of-the-Art-Analyse konventioneller Methoden zur Organismengenerierung durchgeführt. Im Laufe dieser Analyse werden die Defizite herkömmlicher Verfahren aufgezeigt und damit eine gezielte Anforderungsanalyse für neue Verfahren erstellt. Mit Hilfe dieser Anforderungsanalyse wurde nach neuen Lösungsansätzen gesucht. Besonders hilfreich hat sich in diesem Zusammenhang die Frankfurter Organismus- und Evolutionstheorie erwiesen. Gemäß dieser Theorie stellen Organismen aus biomechanischer Sicht komplexe hydropneumatische Konstruktionen dar. Ihre Körperformen und Bewegungen werden weitgehend durch stabilisierende, kräfteerzeugende und kräfteübertragende Strukturen generiert, die den Gesetzen der klassischen Hydropneumatik folgen. So entstand die Idee, Organismen auf der anatomischen Ebene als eine komplexe Hierarchie unterschiedlicher hydropneumatischer Einheiten anzusehen, welche mechanisch miteinander interagieren. Diese Sichtweise liefert die Grundlage für ein neues biologisches Simulationsmodell. Es erlaubt der Computergraphik, sowohl die Form eines Organismus zu beschreiben als auch sein Verhalten bezüglich seiner Bewegungsabläufe, seiner evolutionären Formveränderungen, seiner Wachstumsprozesse und seiner Reaktion auf externe mechanische Krafteinwirkungen numerisch zu simulieren. Aufbauend auf diesem biologischen Simulationsmodell wurde ein neues Verfahren (Quaoaring) entwickelt und implementiert, das es erlaubt, beliebige organische Einheiten interaktiv in Echtzeit zu modellieren. Gleichzeitig ermöglicht dieses Verfahren die Animation von Bewegungen, Wachstumsprozessen und sogar evolutionären Entwicklungen. Die Animation verhält sich dabei im Wesentlichen biologisch stringent, z.B. wird das interne Volumen während komplexer Bewegungsabläufe konstant gehalten. Die größte Stärke der neuen Modellierungs- und Animationstechnik ist die holistische Verschmelzung des biologischen Simulationsmodells mit einem computergraphischen Geometriemodell. Dieses erlaubt dem Modellierer, biologische Konzepte für die Beschreibung der Form und anderer Attribute einer organischen Einheit zu verwenden. Darüber hinaus ermöglicht es die Animation des geometrischen Modells durch einfache Parameterspezifikation auf einer hohen Abstraktionsebene. Dazu wird ein utorenprozess beschrieben, wie Quaoaring für Modellierungs- und Animationszwecke verwendet werden kann. Es werden Aspekte der prototypischen Implementierung der Quaoaringtechnologie behandelt und über die Ergebnisse berichtet, die bei der Implementierung und der Anwendung dieses Softwareframeworks gewonnen wurden. Schließlich wird die Quaoaringtechnologie in ihrem technologischen Kontext beleuchtet, um ihr Zukunftspotential einzuschätzen.
Wir haben in dieser Arbeit einige Probleme auf Objekten betrachtet, deren Struktur wohlgeformten Klammerworten entspricht. Dies waren spezielle Routing-Probleme, das Umformen und Auswerten algebraischer Ausdrücke, sowie die Berechnung korrespondierender Symbole zweier Ausdrücke. Eine effiziente Lösung dieser Probleme gelang durch einen rekursiven Divide-and-Conquer Ansatz, der auf Grund der “natürlichen” rekursiven Definition der betrachteten Objekte auch nahe liegt. Im Divide-Schritt wurde das jeweilige Problem in viele wesentlich kleinere Teilprobleme zerlegt, so daß die gesamte Laufzeit des Algorithmus asymptotisch gleich der des Divide-Schrittes und des Conquer-Schrittes blieb. Das Zerlegen der Probleme erfolgte im wesentlichen unter Anwendung bekannter Routing-Algorithmen für monotone Routings und Bit-Permute-Complement Permutationen. Im Conquer-Schritt für das Klammerrouting und das Knotenkorrespondenzproblem wurden nur die Datenbewegungen des Divide-Schrittes rückwärts ausgeführt. Für das Tree-Contraction-Problem wurde dagegen im Conquer-Schritt die Hauptarbeit geleistet. Die Methode der Simulation eines PRAMAlgorithmus durch die Berechnung seiner Kommunikationsstruktur und eine entsprechende Umordnung der Datenelemente konnte sowohl für eine effiziente Implementierung des Tree-Contraction Conquer-Schrittes auf dem Hyperwürfel als auch für die Konstruktion eines einfachen NC1-Schaltkreises zum Auswerten Boolescher Formeln angewandt werden. In einer Implementierung eines Divide-and-Conquer Algorithmus auf einem Netzwerk müssen den generierten Teilproblemen für ihre weitere Bearbeitung Teile des Netzwerks zugeordnet werden. Um die weiteren Divide-Schritte nach der gleichen Methode ausführen zu können, sollte die Struktur dieser Teilnetzwerke analog zu der des gesamten Netzwerks sein. Wir haben das Teilnetzwerk-Zuweisungsproblem für den Hyperwürfel und einige hyperwürfelartige Netzwerke untersucht. Der Hyperwürfel und das Butterfly-Netzwerk können so in Teilnetzwerke vorgegebener Größen aufgeteilt werden, daß nur ein geringer Anteil der Prozessoren ungenutzt bleibt, und die Teilprobleme können schnell in die ihnen zugeordneten Teilnetzwerke gesendet werden. Unter Anwendung dieser Teilnetzwerk-Zuweisungs-Algorithmen haben wir optimale Implementierungen für eine große Klasse von Divide-and-Conquer Algorithmen auf dem Hyperwüfel und hyperwürfelartigen Netzwerken erhalten. Wir konnten garantieren, daß die Laufzeit der gesamten Implementierung des Divide-and-Conquer Algorithmus asymptotisch gleich der Laufzeit ist, die sich aus dem gegebenen Divide-Schritt und Conquer-Schritt ergibt, wenn man alle mit der Teilnetzwerk-Zuweisung verbundenen Probleme außer acht läßt. Wir haben die hier vorgestellte allgemeine Divide-and-Conquer Implementierung im optimalen Teilwürfel-Zuweisungs-Algorithmus, im Klammerrouting-Algorithmus, der selbst ein wesentlicher Teil des Tree-Contraction-Algorithmus ist, und im Algorithmus für das Knotenkorrespondenzproblem eingesetzt.
Die folgende Bachelorarbeit beschäftigt sich mit dem Thema des Displacement-Mappings unter Verwendung eines Tessellation-Shaders. Ziel dieser Arbeit ist es, ein Programm zu entwerfen, welches einen visuellen Einblick in die Tessellation und in das Displacement-Mapping bietet. Des Weiteren soll die Leistung der Tessellation mit der des Geometry-Shaders und einem QuadTree-Verfahren verglichen werden.
Dazu wird zuerst beschrieben, welche Umgebung zur Implementierung verwendet wurde. Anschließend werden zunächst einige geläufige Mappingverfahren betrachtet. Im nächsten Abschnitt wird dann auf die Tessellation und das Displacement-Mapping in Bezug auf Funktionsweise und Implementierung eingegangen. Es folgt ein Vergleich der Performance der unterschiedlichen Mapping-Verfahren untereinander. In einem weiteren Vergleich wird die Performance der Tessellation (mit Displacement-Mapping) mit einem Geometry-Shader und einem QuadTree-Verfahren anhand eines Terrains durchgeführt. Abschließend erfolgt die Beschreibung des Programms.
Direct photon production at mid-rapidity in Pb–Pb collisions at √sNN=2.76 TeV was studied in the transverse momentum range 0.9<pT<14 GeV/c. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the ALICE detector material with the e+e− pair reconstructed in the central tracking system. The results of the two methods were combined and direct photon spectra were measured for the 0–20%, 20–40%, and 40–80% centrality classes. For all three classes, agreement was found with perturbative QCD calculations for pT≳5 GeV/c. Direct photon spectra down to pT≈1 GeV/c could be extracted for the 20–40% and 0–20% centrality classes. The significance of the direct photon signal for 0.9<pT<2.1 GeV/c is 2.6σ for the 0–20% class. The spectrum in this pT range and centrality class can be described by an exponential with an inverse slope parameter of (297±12stat±41syst) MeV. State-of-the-art models for photon production in heavy-ion collisions agree with the data within uncertainties.
Direct photon production at mid-rapidity in Pb-Pb collisions at sNN−−−√=2.76 TeV was studied in the transverse momentum range 0.9<pT<14 GeV/c. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the ALICE detector material with the e+e− pair reconstructed in the central tracking system. The results of the two methods were combined and direct photon spectra were measured for the 0-20%, 20-40%, and 40-80% centrality classes. For all three classes, agreement was found with perturbative QCD calculations for pT≳5 GeV/c. Direct photon spectra down to pT≈1 GeV/c could be extracted for the 20-40% and 0-20% centrality classes. The significance of the direct photon signal for 0.9<pT<2.1 GeV/c is 2.6σ for the 0-20% class. The spectrum in this pT range and centrality class can be described by an exponential with an inverse slope parameter of (297±12stat±41syst) MeV. State-of-the-art models for photon production in heavy-ion collisions agree with the data within uncertainties.
Direct photon production at mid-rapidity in Pb-Pb collisions at sNN−−−√=2.76 TeV was studied in the transverse momentum range 0.9<pT<14 GeV/c. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the ALICE detector material with the e+e− pair reconstructed in the central tracking system. The results of the two methods were combined and direct photon spectra were measured for the 0-20%, 20-40%, and 40-80% centrality classes. For all three classes, agreement was found with perturbative QCD calculations for pT≳5 GeV/c. Direct photon spectra down to pT≈1 GeV/c could be extracted for the 20-40% and 0-20% centrality classes. The significance of the direct photon signal for 0.9<pT<2.1 GeV/c is 2.6σ for the 0-20% class. The spectrum in this pT range and centrality class can be described by an exponential with an inverse slope parameter of (297±12stat±41syst) MeV. State-of-the-art models for photon production in heavy-ion collisions agree with the data within uncertainties.
Measurements of inclusive and direct photon production at mid-rapidity in pp collisions at s√=2.76 and 8 TeV are presented by the ALICE experiment at the LHC. The results are reported in transverse momentum ranges of 0.4<pT<10 GeV/c and 0.3<pT<16 GeV/c, respectively. Photons are detected with the electromagnetic calorimeter~(EMCal) and via reconstruction of e+e− pairs from conversions in the ALICE detector material using the central tracking system. For the final measurement of the inclusive photon spectra the results are combined in the overlapping pT interval of both methods. Direct photon spectra, or their upper limits at 90% C.L. are extracted using the direct photon excess ratio Rγ, which quantifies the ratio of inclusive photons over decay photons generated with a decay-photon simulation. An additional hybrid method, combining photons reconstructed from conversions with those identified in the EMCal, is used for the combination of the direct photon excess ratio Rγ, as well as the extraction of direct photon spectra or their upper limits. While no significant signal of direct photons is seen over the full pT range, Rγ for pT>7 GeV/c is at least one σ above unity and consistent with expectations from next-to-leading order pQCD calculations.
Measurements of inclusive and direct photon production at mid-rapidity in pp collisions at s√=2.76 and 8 TeV are presented by the ALICE experiment at the LHC. The results are reported in transverse momentum ranges of 0.4<pT<10 GeV/c and 0.3<pT<16 GeV/c, respectively. Photons are detected with the electromagnetic calorimeter~(EMCal) and via reconstruction of e+e− pairs from conversions in the ALICE detector material using the central tracking system. For the final measurement of the inclusive photon spectra the results are combined in the overlapping pT interval of both methods. Direct photon spectra, or their upper limits at 90% C.L. are extracted using the direct photon excess ratio Rγ, which quantifies the ratio of inclusive photons over decay photons generated with a decay-photon simulation. An additional hybrid method, combining photons reconstructed from conversions with those identified in the EMCal, is used for the combination of the direct photon excess ratio Rγ, as well as the extraction of direct photon spectra or their upper limits. While no significant signal of direct photons is seen over the full pT range, Rγ for pT>7 GeV/c is at least one σ above unity and consistent with expectations from next-to-leading order pQCD calculations.
Measurements of inclusive and direct photon production at mid-rapidity in pp collisions at s√=2.76 and 8 TeV are presented by the ALICE experiment at the LHC. The results are reported in transverse momentum ranges of 0.4<pT<10 GeV/c and 0.3<pT<16 GeV/c, respectively. Photons are detected with the electromagnetic calorimeter~(EMCal) and via reconstruction of e+e− pairs from conversions in the ALICE detector material using the central tracking system. For the final measurement of the inclusive photon spectra the results are combined in the overlapping pT interval of both methods. Direct photon spectra, or their upper limits at 90% C.L. are extracted using the direct photon excess ratio Rγ, which quantifies the ratio of inclusive photons over decay photons generated with a decay-photon simulation. An additional hybrid method, combining photons reconstructed from conversions with those identified in the EMCal, is used for the combination of the direct photon excess ratio Rγ, as well as the extraction of direct photon spectra or their upper limits. While no significant signal of direct photons is seen over the full pT range, Rγ for pT>7 GeV/c is at least one σ above unity and consistent with expectations from next-to-leading order pQCD calculations.
The elliptic flow of inclusive and direct photons was measured at mid-rapidity in two centrality classes 0-20% and 20-40% in Pb-Pb collisions at sNN−−−√ = 2.76 TeV by ALICE. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the detector material with the e+e− pairs reconstructed in the central tracking system. The results of the two methods were combined and the direct photon elliptic flow was extracted in the transverse momentum range 0.9<pT<6.2 GeV/c. A comparison to RHIC data shows a similar magnitude of the measured direct-photon elliptic flow. Hydrodynamic and transport model calculations are systematically lower than the data, but are found to be compatible.
The elliptic flow of inclusive and direct photons was measured at mid-rapidity in two centrality classes 0-20% and 20-40% in Pb-Pb collisions at sNN−−−√ =2.76 TeV by ALICE. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the detector material with the e+e− pairs reconstructed in the central tracking system. The results of the two methods were combined and the direct photon elliptic flow was extracted in the transverse momentum range 0.9<pT<6.2 GeV/c. We test the hypothesis vγ,dir2≡0 for 0.9<pT<2.1 GeV/c and obtain a significance of 1.4σ for the 0-20% class and 1.0σ for the 20-40% class. A comparison to RHIC data shows a similar magnitude of the measured elliptic flow, while hydrodynamic and transport model calculations predict a smaller flow than observed.
In particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as described by the theory of quantum chromodynamics (QCD). These partons subsequently emit further partons in a process that can be described as a parton shower which culminates in the formation of detectable hadrons. Studying the pattern of the parton shower is one of the key experimental tools for testing QCD. This pattern is expected to depend on the mass of the initiating parton, through a phenomenon known as the dead-cone effect, which predicts a suppression of the gluon spectrum emitted by a heavy quark of mass mQ and energy E, within a cone of angular size mQ/E around the emitter. Previously, a direct observation of the dead-cone effect in QCD had not been possible, owing to the challenge of reconstructing the cascading quarks and gluons from the experimentally accessible hadrons. We report the direct observation of the QCD dead cone by using new iterative declustering techniques to reconstruct the parton shower of charm quarks. This result confirms a fundamental feature of QCD. Furthermore, the measurement of a dead-cone angle constitutes a direct experimental observation of the non-zero mass of the charm quark, which is a fundamental constant in the standard model of particle physics.
At particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as described by the theory of quantum chromodynamics (QCD). The vacuum is not transparent to the partons and induces gluon radiation and quark pair production in a process that can be described as a parton shower. Studying the pattern of the parton shower is one of the key experimental tools in understanding the properties of QCD. This pattern is expected to depend on the mass of the initiating parton, through a phenomenon known as the dead-cone effect, which predicts a suppression of the gluon spectrum emitted by a heavy quark of mass m and energy E, within a cone of angular size m/E around the emitter. A direct observation of the dead-cone effect in QCD has not been possible until now, due to the challenge of reconstructing the cascading quarks and gluons from the experimentally accessible bound hadronic states. We report the first direct observation of the QCD dead-cone by using new iterative declustering techniques to reconstruct the parton shower of charm quarks. This result confirms a fundamental feature of QCD, which is derived more generally from its origin as a gauge quantum field theory. Furthermore, the measurement of a dead-cone angle constitutes a direct experimental observation of the non-zero mass of the charm quark, which is a fundamental constant in the standard model of particle physics.
Diese Arbeit beschäftigt sich mit der konkreten Erzeugung von 2-3D Visualisierung. Im Fokus steht der notwendige Prozess zur Erzeugung von Computergrafik.
Da die Computergrafik heut zu Tage wichtiger Bestandteil vieler Aufgabengebiete ist, sollte deren Nutzung auch allen Menschen zugänglich sein. In den vergangen Jahren blieb dies meist nur Leuten aus den Fachgebieten vorbehalten, aufgrund der Komplexität und des notwendigen „Know-how“ über die Thematik. Mittlerweile gilt diese Tatsache als überholt. Viele Erneuerung im Bereich von Hardware und Software haben es ermöglicht, dass selbst ungeübte Anwender in der Lage sind, ansehnliche 3D Grafiken an ihren PCs bei der Arbeit oder zu Hause zu erzeugen. Dies soll ebenfalls das Ziel dieser Arbeit sein. Dazu wird in eine Applikation erstellt die die Visualisierung von graphischen Primitiven unter der Verwendug von Microsofts DirectX leicht und schnell ermöglichen soll. Als Basis dient ein Rendering-Framework, welches auf einheitliches Schnittstellenkonzept setzt, um die strikte Trennung zwischen Anwender- und Fachwissen zu vollziehen.
Weitere Schwerpunkte dieser Arbeit liegen im Bereich der Modellierung von graphischen Primtiven und der Nutzung von Shadern. Dazu wird in der Modellierung der Import von archivierten Modellen umgesetzt. Die Nutzung von Shadern soll soweit vereinfacht werden, dass Anwender auf Shader beleibig zugreifen können. Dies soll durch eine Verknüpfung zwischen Shadern und Modellen erfolgen, die ebenfalls im Bereich der Modellierung erfolgt.
Im Jahr 1993 schlug A. Shamir Protokolle zur Erstellung digitaler Unterschriften vor, die auf rationalen Funktionen kleinen Grades beruhen. D. Coppersmith, J. Stern und S. Vaudenay präsentierten die ersten Angriffe auf die Verfahren. Diese Angriffe können den geheimen Schlüssel nicht ermitteln. Für eine der von Shamir vorgeschlagenen Varianten zeigen wir, wie der geheime Schlüssel ermittelt werden kann. Das zweite Signaturschema von Shamir hängt von der Wahl einer algebraischen Basis ab. Eine besondere Bedeutung haben Basen, deren Elemente polynomiale Terme vom Grad 2 sind. Wir analysieren die Struktur der algebraischen Basen. Für den hervorgehobenen Spezialfall kann eine vollständige Klassifikation durchgeführt werden.
Digitale Kompetenzen von Hochschullehrenden messen : Validierungsstudie eines Kompetenzrasters
(2018)
Der Beitrag beschreibt die Entwicklung eines Kompetenzrasters zur Erfassung digitaler Kompetenzen von Hochschullehrenden und stellt Ergebnisse der Validierung des Rasters vor. Dazu werden die Ergebnisse eines Pre-Tests (N=90) unter Teilnehmenden eines E-LearningQualifizierungsangebots inferenzstatistisch ausgewertet. Zusätzlich werden zur äußeren Validierung des Kompetenzrasters Ergebnisse mit Aussagen der Befragungsteilnehmer*innen verglichen, die mit Hilfe qualitativer Methoden aus E-Portfolios gewonnen wurden. Die skalenanalytischen Befunde erbrachten für sechs der acht Subdimensionen digitaler Kompetenz eindeutige, einfaktorielle Lösungen mit guten Varianzaufklärungen. Die Subskalen verfügen über hohe interne Konsistenzen. Zwei Dimensionen trennen sich faktorenanalytisch in weitere Subtests auf, die sich im Test ebenfalls als reliabel erweisen. Zur Validität des Kompetenzrasters konnten durch Zusammenhänge mit Aussagen aus E-Portfolios positive Belege gesammelt werden.
The production of J/ψ and ψ(2S) was measured with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity (2.5<y<4) down to zero transverse momentum (pT) in the dimuon decay channel. Inclusive J/ψ yields were extracted in different centrality classes and the centrality dependence of the average pT is presented. The J/ψ suppression, quantified with the nuclear modification factor (RAA), was studied as a function of centrality, transverse momentum and rapidity. Comparisons with similar measurements at lower collision energy and theoretical models indicate that the J/ψ production is the result of an interplay between color screening and recombination mechanisms in a deconfined partonic medium, or at its hadronization. Results on the ψ(2S) suppression are provided via the ratio of ψ(2S) over J/ψ measured in pp and Pb-Pb collisions.
The production of J/ψ and ψ(2S) was measured with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity (2.5<y<4) down to zero transverse momentum (pT) in the dimuon decay channel. Inclusive J/ψ yields were extracted in different centrality classes and the centrality dependence of the average pT is presented. The J/ψ suppression, quantified with the nuclear modification factor (RAA), was studied as a function of centrality, transverse momentum and rapidity. Comparisons with similar measurements at lower collision energy and theoretical models indicate that the J/ψ production is the result of an interplay between color screening and recombination mechanisms in a deconfined partonic medium, or at its hadronization. Results on the ψ(2S) suppression are provided via the ratio of ψ(2S) over J/ψ measured in pp and Pb-Pb collisions.
The production of J/ψ and ψ(2S) was measured with the ALICE detector in Pb-Pb collisions at the LHC. The measurement was performed at forward rapidity (2.5<y<4) down to zero transverse momentum (pT) in the dimuon decay channel.
Inclusive J/ψ yields were extracted in different centrality classes and the centrality dependence of the average pT is presented. The J/ψ suppression, quantified with the nuclear modification factor (RAA), was studied as a function of centrality, transverse momentum and rapidity. Comparisons with similar measurements at lower collision energy and theoretical models indicate that the J/ψ production is the result of an interplay between color screening and recombination mechanisms in a deconfined partonic medium, or at its hadronization. Results on the ψ(2S) suppression are provided via the ratio of ψ(2S) over J/ψ measured in pp and Pb-Pb collisions.
Die Integration von Dienstgüte-Vorkehrungen in objektorientierte Verteilungsinfrastrukturen befähigt Anwendungsentwickler, den Verteilungs-induzierten Problemen verteilter Systeme zu begegnen. Im Rahmen dieser Arbeit wurde die generische Einbettung von Dienstgüte-Vorkehrungen in verteilte Objektsysteme untersucht und ein Lösungsansatz präsentiert. Zunächst wurde eine Analyse der für das Dienstgüte-Management notwendigen Aufgaben vorgestellt. Ausgehend von einem verteilten Objektmodell wurde untersucht, wie Dienstgüte-Vorkehrungen integriert werden können. Dienstgüte-Vorkehrungen stellen bei einem zugrundeliegenden Ob- jektmodell nicht-einkapselbare Verantwortlichkeiten dar. Die enge Bindung der Dienstgüte-Vorkehrungen an einen Dienst führt so zu Vermaschungen in den Strukturen der Implementierung. Damit ist die getrennte Wieder- verwendung beider erschwert. Zusätzlich werden unterschiedliche Abstrak- tionen vermischt. Die aspektorientierte Programmierung (AOP) behandelt solche Vermaschungen. Dienstgüte wurde bei der Integration in ein verteil- tes Objektmodell als ein Aspekt im Sinne der AOP klassifiziert. Ausgehend von den Anforderungen an das Dienstgüte-Management wur- de ein Rahmenwerk auf Basis eines verteilten Objektmodells entworfen. Der in dieser Arbeit dargestellte Schwerpunkt liegt auf der Spezifikation von Dienstgüte-Charakteristiken und deren Umsetzung in die Implementie- rungssprache der Anwendungsobjekte. Für die Unterstützung der Ende-zu- Ende-Dienstgüte-Erbringung ist der Einbezug von Dienstgüte-Vorkehrun- gen des Netzwerks, Betriebssystems oder spezieller Bibliotheken notwendig. Die resultierende Hierarchie von Dienstgüte-Mechanismen wird durch die vorgestellte Integration in eine Verteilungsinfrastruktur unterstützt. Durch die Integration der Dienstgüte-Spezifikation in die Schnittstel- lenbeschreibungssprache erlaubt das Rahmenwerk einen aspektorientierten Ansatz ohne die Einführung weiterer Sprachen zur Spezifikation oder Im- plementierung. Die Spezifikation von Dienstgüte-Charakteristiken in der erweiterten IDL wird in spezielle Entwurfsmuster in der Zielsprache umge- setzt. Diese Entwurfsmuster separieren die Anwendungsobjekte weitgehend von den Dienstgüte-Vorkehrungen. Die auf der Ebene der Anwendungsobjekte generierten Vorlagen für die Dienstgüte-Vorkehrungen können durch einen modifizierten bzw. schon da- für ausgelegten Verteilungsinfrastrukturkern in das System integriert wer- den. Eine einheitliche statische Schnittstelle erlaubt einen einfachen re- effektiven Ansatz. So ist der Zugriff auf Dienstgüte-Vorkehrungen tieferer Schichten wie auch die Integration anwendungsspezifischer Dienstgüte-Vor- kehrungen auf der Netzwerkschicht möglich. Das Rahmenwerk bietet somit eine klare Trennung der Verantwortlich- keiten, die sowohl Anwendungsentwickler wie auch Dienstgüte-Implemen- tierer unterstützt. Die aus der Schnittstellenbeschreibungssprache generier- ten Einheiten stellen für die Anwendungsobjekte eine Abstraktion dar, die sowohl die Verteilungsaspekte wie auch die Dienstgüte-Vorkehrungen ein- fach nutzbar anbietet und von der zugrundeliegenden Plattform isoliert. Eine sich aus dieser Arbeit ergebende Fragestellung besteht in der Er- weiterung und Verallgemeinerung des aspektorientierten Ansatzes. Die im Rahmen der Analyse betrachteten Dienstgüte-Charakteristiken sind aus dem systemnahen Bereich und insbesondere aus der Betrachtung typi- scher Probleme in verteilten Systemen und den daraus erwachsenen Anwen- dungsanforderungen gewonnen. Nicht-funktionale Aspekte der Dienster- bringung lassen sich weiter fassen. So kann ausgehend von den bereitge- stellten Abstraktionen untersucht werden, inwieweit auf Anwendungsebe- ne nicht-funktionale Eigenschaften in ähnlicher Weise einbettbar sind. Im Rahmen dieser Arbeit wurde beispielsweise eine Dienstgüte-Charakteristik zur Parallelisierung von Berechnungen realisiert. Eine anwendungsbezogene Dienstgüte-Charakteristik könnte numerische Optimierungen realisieren, die von den reinen mathematischen Operationen zu trennen ist. Andere Beispiele aus der Multimedia-Kategorie sind durch die Qualität einer Au- dio-Übertragung gegeben. So kann bei einer geringen Bandbreite durch die Kompression der Daten eine bessere Qualität der Audiowiedergabe ereicht werden, als durch Übertragung der Rohdaten. Die Kompressionsrate kann von der Anwendung isoliert und durch entsprechende Dienstgüte-Mecha- nismen realisiert werden. Qualitätsunterschiede ergeben sich durch mögli- che verlustbehaftete Kompression und de notwendigen Anforderungen an Hardware- oder Software-Unterstützung. Andere Kriterien für die Qualität lassen sich weniger leicht vor der Anwendung verbergen. Die Wiedergabe von Stereo- oder Mono-Audiodaten erfordert entsprechende Anwendungen und auch Ausstattungen der Endgeräte. Im Kontext dieser Arbeit wurde ein Objektmodell betrachtet, das eine starke Bindung zwischen Schnittstellen und Objekten besitzt. Insbeson- deren wurde bei der Umsetzung der Schnittstellenbeschreibungssprache in die Zielsprache eine Umsetzung gewählt, die Dienste als Objekte reprä- sentiert. Involviert die Diensterbringung verschiedene Objekte, kann nur ein Objekt als Stellvertreter all dieser Dienste den Service anbieten. Dieses Objekt ist für die Einhaltung von Dienstgüte-Vereinbarungen mit Klien- ten verantwortlich. Innerhalb der Objekte, die den Service realisieren, sind für die Dienstgüte-Erbringung dann ggf. weitere interne Dienstgüte-Vor- kehrungen zu etablieren. Komponentenmodelle versprechen hier einen all- gemeineren Ansatz, der die Integration von Dienstgüte-Vorkehrungen loh- nenswert erscheinen lässt. Zum einen unterstützen Komponentenmodelle definierte Schnittstellen zur Interaktion zwischen den beteiligten Objek- ten einer Komponente, und zum anderen bieten Komponenten eine über die Schnittstellenbeschreibungssprache hinausgehende Beschreibung ihrer Funktionalität in einer Komponentenspezifikation. Diese Komponentenspe- zifikation verspricht einen guten Ansatz, um Dienstgüte-Spezifikationen der Komponenten zu integrieren. Neben den beiden bislang beschriebenen Forschungsrichtungen, die je- weils ein Rahmenwerk für das Dienstgüte-Management voraussetzen und darauf aufbauen, existieren innerhalb des in der Arbeit vorgestellten Rah- menwerkes weitere offene Forschungsfragen. Die Ausgestaltung von Preisen bei der Vergabe von Ressourcen und die damit verbundenen Richtlinien für die Vergabe und auch den Entzug stellen noch kein abgeschlossenes Gebiet dar. Hier ist der Einbezug anderer Disziplinen vielversprechend. Preisrichtlinien für manche Ressourcen, die bei Nicht-Nutzung verfallen wie Netzwerkkapazität sind Gegenstand der Forschung in der Betriebs- wirtschaftslehre. Die Gestaltung von Vergaberichtlinien, insbesondere aber die Festlegung von Vergütungen bei Nichterbringung eines festgesetzten Dienstgüte-Niveaus oder Kompensationen bei dem Entzug von Ressourcen mit einer damit einhergehenden Verletzung der Dienstgüte-Vereinbarung, wirft rechtliche Fragen über die Gültigkeit solcher Richtlinien auf. Weitere, nicht-interdisziplinäre Fragestellungen, ergeben sich aus der Frage der Wiederverwendbarkeit und Dokumentation von Dienstgüte-Vor- kehrungen im Rahmenwerk. Die Erstellung eines Katalogs mit einem ein- heitlichen Aufbau wie es bei Entwurfsmustern üblich ist verspricht eine geeignete Dokumentationsform. Allerdings muss eine solche Dokumentati- on zwei Zielgruppen gerecht werden. Zum einen sind dies Anwendungsent- wickler, die eine gegebene Dienstgüte-Implementierung anwenden wollen und Informationen für die Nutzung und Anpassung der Anwendung benö- tigen und zum anderen Dienstgüte-Entwickler, die auf bereits existierende transportspezifische Dienstgüte-Mechanismen aufbauen. Für die hier skizzierten Forschungsrichtungen ist ein Rahmenwerk für das Dienstgüte-Management unerlässlich. Das in dieser Arbeit vorgestellte Rahmenwerk bietet eine gute Ausgangsbasis.
The first measurement of e+e− pair production at mid-rapidity (|ηe| < 0.8) in pp collisions at s√=7 TeV with ALICE at the LHC is presented. The dielectron production is studied as a function of the invariant mass (mee < 3.3 GeV/c2), the pair transverse momentum (pT,ee < 8 GeV/c), and the pair transverse impact parameter (DCAee), i.e., the average distance of closest approach of the reconstructed electron and positron tracks to the collision vertex, normalised to its resolution. The results are compared with the expectations from a cocktail of known hadronic sources and are well described when PYTHIA is used to generate the heavy-flavour contributions. In the low-mass region (0.14 < mee < 1.1 GeV/c2), prompt and non-prompt e+e− sources can be separated via the DCAee. In the intermediate-mass region (1.1 < mee < 2.7 GeV/c2), a double-differential fit to the data in mee and pT,ee and a fit of the DCAee distribution allow the total cc¯¯ and bb¯¯¯ cross sections to be extracted. Two different event generators, PYTHIA and POWHEG, can reproduce the shape of the two-dimensional mee and pT,ee spectra, as well as the shape of the DCAee distribution, reasonably well. However, differences in the cc¯¯ and bb¯¯¯ cross sections are observed when using the generators to extrapolate to full phase space. Finally, the ratio of inclusive to decay photons is studied via the measurement of virtual direct photons in the transverse-momentum range 1 < pT < 8 GeV/c. This is found to be unity within the statistical and systematic uncertainties and consistent with expectations from next-to-leading order perturbative quantum chromodynamic calculations.
The first measurement of e+e− pair production at mid-rapidity (|ηe| < 0.8) in pp collisions at s√=7 TeV with ALICE at the LHC is presented. The dielectron production is studied as a function of the invariant mass (mee < 3.3 GeV/c2), the pair transverse momentum (pT,ee < 8 GeV/c), and the pair transverse impact parameter (DCAee), i.e., the average distance of closest approach of the reconstructed electron and positron tracks to the collision vertex, normalised to its resolution. The results are compared with the expectations from a cocktail of known hadronic sources and are well described when PYTHIA is used to generate the heavy-flavour contributions. In the low-mass region (0.14 < mee < 1.1 GeV/c2), prompt and non-prompt e+e− sources can be separated via the DCAee. In the intermediate-mass region (1.1 < mee < 2.7 GeV/c2), a double-differential fit to the data in mee and pT,ee and a fit of the DCAee distribution allow the total cc¯¯ and bb¯¯¯ cross sections to be extracted. Two different event generators, PYTHIA and POWHEG, can reproduce the shape of the two-dimensional mee and pT,ee spectra, as well as the shape of the DCAee distribution, reasonably well. However, differences in the cc¯¯ and bb¯¯¯ cross sections are observed when using the generators to extrapolate to full phase space. Finally, the ratio of inclusive to decay photons is studied via the measurement of virtual direct photons in the transverse-momentum range 1 < pT < 8 GeV/c. This is found to be unity within the statistical and systematic uncertainties and consistent with expectations from next-to-leading order perturbative quantum chromodynamic calculations.
The first measurements of dielectron production at midrapidity (|ηc|<0.8) in proton-proton and proton-lead collisions at sNN−−−√ = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT,ee in the ranges mee < 3.5 GeV/c2 and pT,ee < 8.0 GeV/c2, in both collision systems. In proton-proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at s√ = 7 and 13 TeV. The slope of the s√ dependence of the three measurements is described by FONLL calculations. The dielectron cross section measured in proton-lead collisions is in agreement, within the current precision, with the expected dielectron production without any nuclear matter effects for e+e− pairs from open heavy-flavor hadron decays. For the first time at LHC energies, the dielectron production in proton-lead and proton-proton collisions are directly compared at the same sNN−−−√ via the dielectron nuclear modification factor RpPb. The measurements are compared to model calculations including cold nuclear matter effects, or additional sources of dielectrons from thermal radiation.
The first measurements of dielectron production at midrapidity (|ηc|<0.8) in proton-proton and proton-lead collisions at sNN−−−√ = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT,ee in the ranges mee < 3.5 GeV/c2 and pT,ee < 8.0 GeV/c2, in both collision systems. In proton-proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at s√ = 7 and 13 TeV. The slope of the s√ dependence of the three measurements is described by FONLL calculations. The dielectron cross section measured in proton-lead collisions is in agreement, within the current precision, with the expected dielectron production without any nuclear matter effects for e+e− pairs from open heavy-flavor hadron decays. For the first time at LHC energies, the dielectron production in proton-lead and proton-proton collisions are directly compared at the same sNN−−−√ via the dielectron nuclear modification factor RpPb. The measurements are compared to model calculations including cold nuclear matter effects, or additional sources of dielectrons from thermal radiation.
The first measurements of dielectron production at midrapidity (|ηc|<0.8) in proton-proton and proton-lead collisions at sNN−−−√ = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mT,ee and the pair transverse momentum pT,ee in the ranges mT,ee < 3.5 GeV/c2 and mT,ee < 8.0 GeV/c2, in both collision systems. In proton-proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at s√ = 7 and 13 TeV. The slope of the s√ dependence of the three measurements is described by FONLL calculations. The dielectron cross section measured in proton-lead collisions is in agreement, within the current precision, with the expected dielectron production without any nuclear matter effects for e+e− pairs from open heavy-flavor hadron decays. For the first time at LHC energies, the dielectron production in proton-lead and proton-proton collisions are directly compared at the same sNN−−−√ via the dielectron nuclear modification factor RpPb. The measurements are compared to model calculations including cold nuclear matter effects, or additional sources of dielectrons from thermal radiation.
The first measurement of e+e− pair production at mid-rapidity (|ηe| < 0.8) in pp collisions at s√=7 TeV with ALICE at the LHC is presented. The dielectron production is studied as a function of the invariant mass (mee < 3.3 GeV/c2), the pair transverse momentum (pT,ee < 8 GeV/c), and the pair transverse impact parameter (DCAee), i.e., the average distance of closest approach of the reconstructed electron and positron tracks to the collision vertex, normalised to its resolution. The results are compared with the expectations from a cocktail of known hadronic sources and are well described when PYTHIA is used to generate the heavy-flavour contributions. In the low-mass region (0.14 < mee < 1.1 GeV/c2), prompt and non-prompt e+e− sources can be separated via the DCAee. In the intermediate-mass region (1.1 < mee < 2.7 GeV/c2), a double-differential fit to the data in mee and pT,ee and a fit of the DCAee distribution allow the total cc¯¯ and bb¯¯¯ cross sections to be extracted. Two different event generators, PYTHIA and POWHEG, can reproduce the shape of the two-dimensional mee and pT,ee spectra, as well as the shape of the DCAee distribution, reasonably well. However, differences in the cc¯¯ and bb¯¯¯ cross sections are observed when using the generators to extrapolate to full phase space. Finally, the ratio of inclusive to decay photons is studied via the measurement of virtual direct photons in the transverse-momentum range 1 < pT < 8 GeV/c. This is found to be unity within the statistical and systematic uncertainties and consistent with expectations from next-to-leading order perturbative quantum chromodynamic calculations.
The first measurement of the e+e− pair production at midrapidity and low invariant mass in central Pb−Pb collisions at sNN−−−√=5.02 TeV at the LHC is presented. The yield of e+e− pairs is compared with a cocktail of expected hadronic decay contributions in the invariant mass (mee) and pair transverse momentum (pT,ee) ranges mee<3.5 GeV/c2 and pT,ee<8 GeV/c. For 0.18<mee<0.5 GeV/c2 the ratio of data to the cocktail of hadronic contributions without ρ mesons amounts to 1.42±0.12 (stat.)±0.17 (syst.)±0.12 (cocktail) and 1.44±0.12 (stat.)±0.17 (syst.)+0.17−0.21 (cocktail), including or not including medium effects in the estimation of the heavy-flavor background, respectively. It is consistent with predictions from two different models for an additional contribution of thermal e+e− pairs from the hadronic and partonic phases. In the intermediate-mass range (1.2<mee<2.6 GeV/c2), the pair transverse impact parameter of the e+e− pairs (DCAee) is used for the first time in Pb−Pb collisions to separate displaced dielectrons from heavy-flavor hadron decays from a possible (thermal) contribution produced at the interaction point. The data are consistent with a suppression of e+e− pairs from cc¯¯ and an additional prompt component. Finally, the first direct-photon measurement in the 10% most central Pb−Pb collisions at sNN−−−√=5.02 TeV is reported via the study of virtual direct photons in the transverse momentum range 1<pT<5 GeV/c. A model including prompt photons, as well as photons from the pre-equilibrium and fluid-dynamic phases, can reproduce the result, while being at the upper edge of the data uncertainties.
The first measurement of the e+e− pair production at low lepton pair transverse momentum (pT,ee) and low invariant mass (mee) in non-central Pb−Pb collisions at sNN−−−√=5.02 TeV at the LHC is presented. The dielectron production is studied with the ALICE detector at midrapidity (|ηe|<0.8) as a function of invariant mass (0.4≤mee<2.7 GeV/c2) in the 50−70% and 70−90% centrality classes for pT,ee<0.1 GeV/c, and as a function of pT,ee in three mee intervals in the most peripheral Pb−Pb collisions. Below a pT,ee of 0.1 GeV/c, a clear excess of e+e− pairs is found compared to the expectations from known hadronic sources and predictions of thermal radiation from the medium. The mee excess spectra are reproduced, within uncertainties, by different predictions of the photon−photon production of dielectrons, where the photons originate from the extremely strong electromagnetic fields generated by the highly Lorentz-contracted Pb nuclei. Lowest-order quantum electrodynamic (QED) calculations, as well as a model that takes into account the impact-parameter dependence of the average transverse momentum of the photons, also provide a good description of the pT,ee spectra. The measured ⟨p2T,ee⟩−−−−−√ of the excess pT,ee spectrum in peripheral Pb−Pb collisions is found to be comparable to the values observed previously at RHIC in a similar phase-space region.
The first measurement of the e+e− pair production at low lepton pair transverse momentum (pT,ee) and low invariant mass (mee) in non-central Pb−Pb collisions at sNN−−−√=5.02 TeV at the LHC is presented. The dielectron production is studied with the ALICE detector at midrapidity (|ηe|<0.8) as a function of invariant mass (0.4≤mee<2.7 GeV/c2) in the 50−70% and 70−90% centrality classes for pT,ee<0.1 GeV/c, and as a function of pT,ee in three mee intervals in the most peripheral Pb−Pb collisions. Below a pT,ee of 0.1 GeV/c, a clear excess of e+e− pairs is found compared to the expectations from known hadronic sources and predictions of thermal radiation from the medium. The mee excess spectra are reproduced, within uncertainties, by different predictions of the photon−photon production of dielectrons, where the photons originate from the extremely strong electromagnetic fields generated by the highly Lorentz-contracted Pb nuclei. Lowest-order quantum electrodynamic (QED) calculations, as well as a model that takes into account the impact-parameter dependence of the average transverse momentum of the photons, also provide a good description of the pT,ee spectra. The measured ⟨p2T,ee⟩−−−−−√ of the excess pT,ee spectrum in peripheral Pb−Pb collisions is found to be comparable to the values observed previously at RHIC in a similar phase-space region.
The first measurement of the e+e− pair production at low lepton pair transverse momentum (pT,ee) and low invariant mass (mee) in non-central Pb−Pb collisions at sNN−−−√=5.02 TeV at the LHC is presented. The dielectron production is studied with the ALICE detector at midrapidity (|ηe|<0.8) as a function of invariant mass (0.4≤mee<2.7 GeV/c2) in the 50−70% and 70−90% centrality classes for pT,ee<0.1 GeV/c, and as a function of pT,ee in three mee intervals in the most peripheral Pb−Pb collisions. Below a pT,ee of 0.1 GeV/c, a clear excess of e+e− pairs is found compared to the expectations from known hadronic sources and predictions of thermal radiation from the medium. The mee excess spectra are reproduced, within uncertainties, by different predictions of the photon−photon production of dielectrons, where the photons originate from the extremely strong electromagnetic fields generated by the highly Lorentz-contracted Pb nuclei. Lowest-order quantum electrodynamic (QED) calculations, as well as a model that takes into account the impact-parameter dependence of the average transverse momentum of the photons, also provide a good description of the pT,ee spectra. The measured ⟨p2T,ee⟩−−−−−√ of the excess pT,ee spectrum in peripheral Pb−Pb collisions is found to be comparable to the values observed previously at RHIC in a similar phase-space region.
The measurement of dielectron production is presented as a function of invariant mass and transverse momentum (pT) at midrapidity (|ye|<0.8) in proton-proton (pp) collisions at a centre-of-mass energy of s√=13 TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at s√=7 TeV or 13 TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσcc¯/dy|y=0=974±138(stat.)±140(syst.) μb and dσbb¯/dy|y=0=79±14(stat.)±11(syst.) μb using PYTHIA simulations and dσcc¯/dy|y=0=1417±184(stat.)±204(syst.) μb and dσbb¯/dy|y=0=48±14(stat.)±7(syst.) μb for POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various pT intervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of pT. Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations.
The measurement of dielectron production is presented as a function of invariant mass and transverse momentum (pT) at midrapidity (|ye|<0.8) in proton-proton (pp) collisions at a centre-of-mass energy of s√=13 TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at s√=7 TeV or 13 TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσcc¯/dy|y=0=974±138(stat.)±140(syst.) μb and dσbb¯/dy|y=0=79±14(stat.)±11(syst.) μb using PYTHIA simulations and dσcc¯/dy|y=0=1417±184(stat.)±204(syst.) μb and dσbb¯/dy|y=0=48±14(stat.)±7(syst.) μb for POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various pT intervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of pT. Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations.
Die wahrscheinlich beste Entscheidung : wie Online-Algorithmen mit der unsicheren Zukunft rechnen
(2018)
Lohnt es sich, als Skianfänger in einem schneeunsicheren Jahr Skier zu kaufen? Oder ist es günstiger, sie zu mieten? Oft müssen wir Entscheidungen treffen, ohne genügend Informationen über die Zukunft zu haben. Das gilt in noch größerem Maße für Rechnersysteme, die große Datenmengen verarbeiten und schnelle Entscheidungen treffen müssen. Damit sie trotz einer Vielzahl von Unsicherheiten erfolgreich arbeiten können, entwickeln Informatiker OnlineAlgorithmen.
Large language models have become widely available to the general public, especially due to ChatGPT's release. Consequently, the AI community has invested much effort into recreating language models of the same caliber as ChatGPT, since the latter is still a technical blackbox. This thesis aims to contribute to that cause by proposing R.O.B.E.R.T., a Robotic Operating Buddy for Efficiency, Research and Teaching. In doing so, it presents a first implementation of a lightweight environment which produces tailor-made, instruction-following language models with a heavy focus on conversational capabilities that instruct themselves into a given domain-context. Within this environment, the generation of datasets, the fine-tuning process and finally the inference of a unique R.O.B.E.R.T. instance are all carried out as part of an automated pipeline.
Interacting with the environment to process sensory information, generate perceptions, and shape behavior engages neural networks in brain areas with highly varied representations, ranging from unimodal sensory cortices to higher-order association areas. Recent work suggests a much greater degree of commonality across areas, with distributed and modular networks present in both sensory and non-sensory areas during early development. However, it is currently unknown whether this initially common modular structure undergoes an equally common developmental trajectory, or whether such a modular functional organization persists in some areas—such as primary visual cortex—but not others. Here we examine the development of network organization across diverse cortical regions in ferrets of both sexes using in vivo widefield calcium imaging of spontaneous activity. We find that all regions examined, including both primary sensory cortices (visual, auditory, and somatosensory—V1, A1, and S1, respectively) and higher order association areas (prefrontal and posterior parietal cortices) exhibit a largely similar pattern of changes over an approximately 3 week developmental period spanning eye opening and the transition to predominantly externally-driven sensory activity. We find that both a modular functional organization and millimeter-scale correlated networks remain present across all cortical areas examined. These networks weakened over development in most cortical areas, but strengthened in V1. Overall, the conserved maintenance of modular organization across different cortical areas suggests a common pathway of network refinement, and suggests that a modular organization—known to encode functional representations in visual areas—may be similarly engaged in highly diverse brain areas.
Significance Different areas of the mature brain encode vastly different representations of the world. This study shows that a modular functional organization where nearby neurons participate in similar functional networks is shared across different brain areas not only during early development, but also as the brain matures where it remains a shared feature that shapes neural activity. The largely conserved trajectory of developmental changes across brain areas suggests that similar circuit mechanisms may drive this maturation. This implies that the large literature on developing cortical circuits, which is largely focused on sensory areas, may also apply more broadly, and that perturbations during development that impinge on any such shared mechanisms may produce deficits that extend across multiple brain systems.
This thesis will first introduce in more detail the Bayesian theory and its use in integrating multiple information sources. I will briefly talk about models and their relation to the dynamics of an environment, and how to combine multiple alternative models. Following that I will discuss the experimental findings on multisensory integration in humans and animals. I start with psychophysical results on various forms of tasks and setups, that show that the brain uses and combines information from multiple cues. Specifically, the discussion will focus on the finding that humans integrate this information in a way that is close to the theoretical optimal performance. Special emphasis will be put on results about the developmental aspects of cue integration, highlighting experiments that could show that children do not perform similar to the Bayesian predictions. This section also includes a short summary of experiments on how subjects handle multiple alternative environmental dynamics. I will also talk about neurobiological findings of cells receiving input from multiple receptors both in dedicated brain areas but also primary sensory areas. I will proceed with an overview of existing theories and computational models of multisensory integration. This will be followed by a discussion on reinforcement learning (RL). First I will talk about the original theory including the two different main approaches model-free and model-based reinforcement learning. The important variables will be introduced as well as different algorithmic implementations. Secondly, a short review on the mapping of those theories onto brain and behaviour will be given. I mention the most in uential papers that showed correlations between the activity in certain brain regions with RL variables, most prominently between dopaminergic neurons and temporal difference errors. I will try to motivate, why I think that this theory can help to explain the development of near-optimal cue integration in humans. The next main chapter will introduce our model that learns to solve the task of audio-visual orienting. Many of the results in this section have been published in [Weisswange et al. 2009b,Weisswange et al. 2011]. The model agent starts without any knowledge of the environment and acts based on predictions of rewards, which will be adapted according to the reward signaling the quality of the performed action. I will show that after training this model performs similarly to the prediction of a Bayesian observer. The model can also deal with more complex environments in which it has to deal with multiple possible underlying generating models (perform causal inference). In these experiments I use di#erent formulations of Bayesian observers for comparison with our model, and find that it is most similar to the fully optimal observer doing model averaging. Additional experiments using various alterations to the environment show the ability of the model to react to changes in the input statistics without explicitly representing probability distributions. I will close the chapter with a discussion on the benefits and shortcomings of the model. The thesis continues whith a report on an application of the learning algorithm introduced before to two real world cue integration tasks on a robotic head. For these tasks our system outperforms a commonly used approximation to Bayesian inference, reliability weighted averaging. The approximation is handy because of its computational simplicity, because it relies on certain assumptions that are usually controlled for in a laboratory setting, but these are often not true for real world data. This chapter is based on the paper [Karaoguz et al. 2011]. Our second modeling approach tries to address the neuronal substrates of the learning process for cue integration. I again use a reward based training scheme, but this time implemented as a modulation of synaptic plasticity mechanisms in a recurrent network of binary threshold neurons. I start the chapter with an additional introduction section to discuss recurrent networks and especially the various forms of neuronal plasticity that I will use in the model. The performance on a task similar to that of chapter 3 will be presented together with an analysis of the in uence of different plasticity mechanisms on it. Again benefits and shortcomings and the general potential of the method will be discussed. I will close the thesis with a general conclusion and some ideas about possible future work.
Programmable hardware in the form of FPGAs found its place in various high energy physics experiments over the past few decades. These devices provide highly parallel and fully configurable data transport, data formatting, and data processing capabilities with custom interfaces, even in rigid or constrained environments. Additionally, FPGA functionalities and the number of their logic resources have grown exponentially in the last few years, making FPGAs more and more suitable for complex data processing tasks. ALICE is one of the four main experiments at the LHC and specialized in the study of heavy-ion collisions. The readout chain of the ALICE detectors makes use of FPGAs at various places. The Read-Out Receiver Cards (RORCs) are one example of FPGA-based readout hardware, building the interface between the custom detector electronics and the commercial server nodes in the data processing clusters of the Data Acquisition (DAQ) system as well as the High Level Trigger (HLT). These boards are implemented as server plug-in cards with serial optical links towards the detectors. Experimental data is received via more than 500 optical links, already partly pre-processed in the FPGAs, and pushed towards the host machines. Computer clusters consisting of a few hundred nodes collect, aggregate, compress, reconstruct, and prepare the experimental data for permanent storage and later analysis. With the end of the first LHC run period in 2012 and the start of Run 2 in 2015, the DAQ and HLT systems were renewed and several detector components were upgraded for higher data rates and event rates. Increased detector link rates and obsolete host interfaces rendered it impossible to reuse the previous RORCs in Run 2.
This thesis describes the development, integration, and maintenance of the next generation of RORCs for ALICE in Run 2. A custom hardware platform, initially developed as a joint effort between the ALICE DAQ and HLT groups in the course of this work, found its place in the Run 2 readout systems of the ALICE and ATLAS experiments. The hardware fulfills all experiment requirements, matches its target performance, and has been running stable in the production systems since the start of Run 2. Firmware and software developments for the hardware evaluation, the design of the board, the mass production hardware tests, as well as the operation of the final board in the HLT, were carried out as part of this work. 74 boards were integrated into the HLT hardware and software infrastructure, with various firmware and software developments, to provide the main experimental data input and output interface of the HLT for Run 2. The hardware cluster finder, an FPGA-based data pre-processing core from the previous generation of RORCs, was ported to the new hardware. It has been improved and extended to meet the experimental requirements throughout Run 2. The throughput of this firmware component could be doubled and the algorithm extended, providing an improved noise rejection and an increased overall mean data compression ratio compared to its previous implementation. The hardware cluster finder forms a crucial component in the HLT data reconstruction and compression scheme with a processing performance of one board equivalent to around ten server nodes for comparable processing steps in software.
The work on the firmware development, especially on the hardware cluster finder, once more demonstrated that developing and maintaining data processing algorithms with the common low-level hardware description methods is tedious and time-consuming. Therefore, a high-level synthesis (HLS) hardware description method applying dataflow computing at an algorithmic level to FPGAs was evaluated in this context. The hardware cluster finder served as an example of a typical data processing algorithm in a high energy physics readout application. The existing and highly optimized low-level implementation provided a reference for comparisons in terms of throughput and resource usage. The cluster finder algorithm could be implemented in the dataflow description with comparably little effort, providing fast development cycles, compact code and at, the same time, simplified extension and maintenance options. The performance results in terms of throughput and resource usage are comparable to the manual implementation. The dataflow environment proved to be highly valuable for design space explorations. An integration of the dataflow description into the HLT firmware and software infrastructure could be demonstrated as a proof of concept. A high-level hardware description could ease both the design space exploration, the initial development, the maintenance, and the extension of hardware algorithms for high energy physics readout applications.
Particle identification is an important feature of the ALICE detector at the LHC. In particular, for particle identification via the time-of-flight technique, the precise determination of the event collision time represents an important ingredient of the quality of the measurement. In this paper, the different methods used for such a measurement in ALICE by means of the T0 and the TOF detectors are reviewed. Efficiencies, resolution and the improvement of the particle identification separation power of the methods used are presented for the different LHC colliding systems (pp , p-Pb and Pb-Pb) during the first period of data taking of LHC (Run 1).
Particle identification is an important feature of the ALICE detector at the LHC. In particular, for particle identification via the time-of-flight technique, the precise determination of the event collision time represents an important ingredient of the quality of the measurement. In this paper, the different methods used for such a measurement in ALICE by means of the T0 and the TOF detectors are reviewed. Efficiencies, resolution and the improvement of the particle identification separation power of the methods used are presented for the different LHC colliding systems (pp , p-Pb and Pb-Pb) during the first period of data taking of LHC (Run 1).
Particle identification is an important feature of the ALICE detector at the LHC. In particular, for particle identification via the time-of-flight technique, the precise determination of the event collision time represents an important ingredient of the quality of the measurement. In this paper, the different methods used for such a measurement in ALICE by means of the T0 and the TOF detectors are reviewed. Efficiencies, resolution and the improvement of the particle identification separation power of the methods used are presented for the different LHC colliding systems (pp , p-Pb and Pb-Pb) during the first period of data taking of LHC (Run 1).
Future operation of the CBM detector requires ultra-fast analysis of the continuous stream of data from all subdetector systems. Determining the inter-system time shifts among individual detector systems in the existing prototype experiment mCBM is an essential step for data processing and in particular for stable data taking. Based on the input of raw measurements from all detector systems, the corresponding time correlations can be obtained at digital level by evaluating the differences in time stamps. If the relevant systems are stable during data taking and sufficient digital measurements are available, the distribution of time differences should display a clear peak. Up to now, the outcome of the processed time differences is stored in histograms and the maximum peak is considered, after the evaluation of all timeslices of a run leading to significant run times. The results presented here demonstrate the stability of the synchronicity of mCBM systems. Furthermore it is illustrated that relatively small amounts of raw measurements are sufficient to evaluate corresponding time correlations among individual mCBM detectors, thus enabling fast online monitoring of them in future online data processing.