TY - THES A1 - Dietrich, Philipp T1 - Traveling Wave Magnetic Particle Imaging: Visuelle Stenosequantifizierung und Perkutane Transluminale Angioplastie im Gefäßmodell T1 - Traveling Wave Magnetic Particle Imaging: visual stenosis quantification and percutaneous transluminal angioplasty in a phantom model N2 - Magnetic Particle Imaging (MPI) ist ein innovatives tomographisches Bildgebungs­verfahren, mit dem Tracerpartikel äußerst sensitiv und schnell mehrdimensional abgebildet werden können. Die Methode basiert auf der nichtlinearen Magnetisierungs­antwort superparamagnetischer Eisenoxidnanopartikel (SPION) in einem Messpunkt, welcher ein Messvolumen rastert. In vorliegender Arbeit wurde das sog. Traveling Wave MPI (TWMPI) Verfahren eingesetzt, wodurch im Vergleich zu konventionellen MPI-Scannern ein größeres Field of View (FOV) und eine geringere Latenz bis zur Bildanzeige erreicht werden konnte. TWMPI weist einige für medizinische Zwecke vielversprechende Eigenschaften auf: Es liefert zwei- und dreidimensionale Bildrekonstruktionen in Echtzeit mit hoher zeitlicher und räumlicher Auflösung. Dabei ist die Bildgebung von Grund auf hintergrundfrei und erfordert keinerlei ionisierende Strahlung. Zudem ist die Technik äußerst sensitiv und kann SPION-Tracer noch in mikromolaren Konzentrationen detektieren. Ziel dieser Arbeit war es daher zu untersuchen, inwiefern es mittels TWMPI möglich ist, künstliche Stenosen im Gefäßmodell visuell in Echtzeit darzustellen und quantitativ zu beurteilen sowie überdies eine perkutane transluminale Angioplastie (PTA) im Gefäßmodell unter TWMPI-Echtzeit-Bildgebung durchzuführen. Alle Experimente wurden in einem speziell angefertigten TWMPI-Scanner durchgeführt (JMU Würzburg, Experimentelle Physik V (Biophysik), FOV: 65 x 29 x 29 mm³, Auflösung: ca. 1.5 - 2 mm). Die Lumen-Darstellungen erfolgten mittels des SPION-Tracers Ferucarbotran in einer Verdünnung von 1 : 50 (entspr. 10 mmol [Fe]/l). Das PTA-Instrumentarium wurde mit eigens hergestelltem ferucarbotran­haltigem Lack (100 mmol [Fe]/l) markiert. Für die verschiedenen Teilexperimente wurden den jeweiligen speziellen Anforderungen entsprechend mehrere Gefäßmodelle handgefertigt. Für die visuelle Stenosequantifizierung wurden fünf starre Stenosephantome unterschiedlicher Stenosierung (0%, 25%, 50%, 75%, 100%) aus Polyoxymethylen her­gestellt (l: 40 mm, ID: 8 mm). Die Gefäßmodelle wurden mehrfach zentral im FOV platz­iert und das stenosierte Lumen mittels sog. Slice-Scanning Modus (SSM, Einzel­aufnahme inkl. 10 Mittelungen: 200 ms, Bildfrequenz: 5 Bilder pro Sekunde, Latenz: ca. 100 ms) als zweidimensionale Quasi-Projektionen abgebildet. Diese Aufnahmen (n = 80, 16 je Phantom) wurden mit einer ein­heitlichen Grauskalierung versehen und anschließend entsprechend den NASCET-Kriterien visuell ausgewertet. Alle achtzig Aufnahmen waren unabhängig vom Stenosegrad aufgrund einheitlicher Fensterung sowie konstanter Scannerparameter untereinander gut vergleichbar. Niedrig­gradige Stenosen konnten insgesamt genauer abgebildet werden als höhergradige, was sich neben der subjektiven Bildqualität auch in geringeren Standardabweichungen zeigte (0%: 3.70 % ± 2.71, 25%: 18.64 % ± 1.84, 50%: 52.82 % ± 3.66, 75%: 77.84 % ± 14.77, 100%: 100 % ± 0). Mit zunehmendem Stenosegrad kam es vermehrt zu geometrischen Ver­zerrungen im Zentrum, sodass bei den 75%-Stenosen eine breitere Streuung der Messwerte mit einer höheren Standardabweichung von 14.77% einherging. Leichte, randständige Artefakte konnten bei allen Datensätzen beobachtet werden. Für die PTA wurden drei interaktive Gefäßmodelle aus Polyvinylchlorid (l: 100 mm, ID: 8 mm) mit zu- und abführendem Schlauchsystem entwickelt, welche mittels Kabelband von außen hochgradig eingeengt werden konnten. Analog zu einer konventionellen PTA mittels röntgenbasierter digitaler Subtraktionsangiographie (DSA), wurden alle erforder­lichen Arbeitsschritte (Gefäßdarstellung, Drahtpassage, Ballonplatzierung, Angioplastie, Erfolgskontrolle) unter (TW)MPI-Echtzeit-Bildgebung (Framerate: 2 - 4 FPS, Latenz: ca. 100 ms) abgebildet bzw. durchgeführt. Im Rahmen der PTA war eine Echtzeit-Visualisierung der Stenose im Gefäßmodell durch Tracer-Bolusgabe sowie die Führung des markierten Instrumentariums zum Zielort möglich. Die Markierung der Instrumente hielt der Beanspruchung während der Prozedur stand und ermöglichte eine genaue Platzierung des Ballonkatheters. Die Stenose konnte mittels Angioplastie-Ballons unter Echtzeit-Darstellung gesprengt werden und der Interventionserfolg im Anschluss durch erneute Visualisierung des Lumens validiert werden. Insgesamt zeigt sich MPI somit als adäquate Bildgebungstechnik für die beiden in der Fragestellung bzw. Zielsetzung definierten experimentellen Anwendungen. Stenosen im Gefäßmodell konnten erfolgreich in Echtzeit visualisiert und bildmorphologisch nach NASCET-Kriterien quantifiziert werden. Ebenso war eine PTA im Gefäßmodell unter TWMPI-Echtzeit-Bildgebung machbar. Diese Ergebnisse unter­streichen das grundlegende Potenzial von MPI für medizinische Zwecke. Um zu den bereits etablierten Bildgebungsmethoden aufzuschließen, ist jedoch weitere Forschung im Bereich der Scanner-Hard- und -Software sowie bezüglich SPION-Tracern nötig. N2 - Magnetic Particle Imaging (MPI) is an innovative tomographic imaging method with which tracer particles can be depicted multidimensionally quickly and extremely sensitively. The method is based on the nonlinear magnetization response of superparamagnetic iron oxide nanoparticles (SPION) in a measuring point that runs through a measurement volume. In the present work, the so-called Traveling Wave MPI (TWMPI) method was used, whereby a larger Field of View (FOV) and a lower latency from measurement to image display could be achieved compared to conventional MPI scanners. TWMPI has some promising properties for medical purposes: it delivers two- and three-dimensional image reconstructions in real time with high temporal and spatial resolution. The imaging is background-free by default and does not require any ionizing radiation. In addition, the technology is extremely sensitive and can detect SPION tracers in micromolar concentrations. The aim of this work was therefore to investigate to what extent it is possible to use TWMPI to graphically visualize and quantitatively assess artificial stenoses in a phantom model in real time and furthermore to perform a percutaneous transluminal angioplasty (PTA) in a phantom model under TWMPI real-time imaging. All experiments were carried out in a specially manufactured TWMPI scanner (JMU Würzburg, Experimental Physics V (Biophysics), FOV: 65 x 29 x 29 mm³, resolution: approx. 1.5 - 2 mm). Lumen visualization was achieved by use of the SPION tracer Ferucarbotran in a dilution of 1 : 50 (corresponding to 10 mmol [Fe] / l). The PTA instruments were marked with specially produced ferucarbotran-containing lacquer (100 mmol [Fe]/l). For the different sub-experiments, several vessel phantoms were custom-made according to the respective specific requirements. For visual stenosis quantification, five rigid stenosis phantoms of different grade of stenosis (0%, 25%, 50%, 75%, 100%) were built from polyoxymethylene (l: 40 mm, ID: 8 mm). The vessel phantoms were placed centrally in the FOV several times and the stenotic lumen was depicted as two-dimensional quasi-projections using a so-called slice scanning mode (SSM, single recording incl. averaging 10‑fold: 200 ms, frame rate: 5 frames per second, latency: approx. 100 ms). A uniform gray scaling was applied to these images (n = 80, 16 per phantom) before they were visually evaluated according to the NASCET criteria. Due to the uniform gray scaling, display settings and constant scanner parameters, all eighty images were well comparable with each other, regardless of the degree of stenosis. Overall, low-grade stenoses could be depicted more accurately than higher-grade ones, which, in addition to the subjective image quality, was also reflected in lower standard deviations (0%: 3.70 % ± 2.71, 25%: 18.64 % ± 1.84, 50%: 52.82 % ± 3.66, 75%: 77.84 % ± 14.77, 100%: 100 % ± 0). With increasing­ degree of stenosis, geometric distortions in the center increased, so that within the 75% stenoses a wider spread of the measured values led to a higher standard deviation of 14.77%. Faint, marginal artifacts could be observed over all data sets. For PTA, three interactive vessel phantoms made of polyvinyl chloride (l: 100 mm, ID: 8 mm) were developed with additional tubing to and from the phantom. These vessel phantoms could be highly constricted from the outside by use of cable ties. Analogous to a conventional PTA using X-ray-based digital subtraction angiography (DSA), all necessary steps (vascular visualization, wire passage, balloon placement, angioplasty, control imaging) were depicted by resp. carried out under (TW)MPI real-time imaging (frame rate: 2 – 4 FPS, latency: approx. 100 ms). During the PTA, real-time visualization of the stenosis in the vascular phantom by tracer bolus administration as well as guidance of the marked instruments to the destination was possible. The marking of the instruments withstood the stress during the procedure and allowed an accurate placement of the balloon catheter. The stenosis could be dilated with an angioplasty balloon under real-time imaging and the intervention success could then be validated by re-visualization of the lumen. Overall, MPI thus proves to be an adequate imaging technique in regard of the two experimental applications defined in the questions and aims of this study. Stenoses in a vascular phantom could be successfully visualized in real time and quantified visually according to NASCET criteria. Furthermore, a PTA in a vascular phantom guided by TWMPI real-time imaging was feasible. These findings underscore the fundamental potential of MPI for medical purposes. In order to catch up with the already established imaging methods, however, further research is needed in the field of scanner hard- and software as well as regarding SPION tracers. KW - Medizinische Radiologie KW - Magnetpartikelbildgebung KW - Interventionsradiologie KW - Experimentelle Bildgebung KW - Magnetic Particle Imaging KW - Traveling Wave Magnetic Particle Imaging KW - Interventionelle Radiologie KW - MPI KW - experimental imaging KW - magnetic particle imaging KW - traveling wave magnetic particle imaging KW - interventional radiology KW - Transluminale Angioplastie KW - MPI Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-352517 ER - TY - JOUR T1 - Measurement of dijet azimuthal decorrelations in \({pp}\) collisions at root s=8 TeV with the ATLAS detector and determination of the strong coupling JF - Physical Review D N2 - measurement of the rapidity and transverse momentum dependence of dijet azimuthal decorrelations is presented, using the quantity R-Delta phi. The quantity R-Delta phi specifies the fraction of the inclusive dijet events in which the azimuthal opening angle of the two jets with the highest transverse momenta is less than a given value of the parameter Delta phi(max). The quantity R-Delta phi is measured in proton-proton collisions at root s = 8 TeV as a function of the dijet rapidity interval, the event total scalar transverse momentum, and Delta phi(max). The measurement uses an event sample corresponding to an integrated luminosity of 20.2 fb(-1) collected with the ATLAS detector at the CERN Large Hadron Collider. Predictions of a perturbative QCD calculation at next-to-leading order in the strong coupling with corrections for nonperturbative effects are compared to the data. The theoretical predictions describe the data in the whole kinematic region. The data are used to determine the strong coupling alpha(S) and to study its running for momentum transfers from 260 GeV to above 1.6 TeV. Analysis that combines data at all momentum transfers results in alpha(S) (m(Z)) = 0.1127(- 0.0027) (+0.0063). KW - pp collisions Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-220665 VL - 98 IS - 9 ER - TY - JOUR T1 - Search for squarks and gluinos in final states with same-sign leptons and jets using 139 fb\(^{-1}\) of data collected with the ATLAS detector JF - Journal of High Energy Physics N2 - A search for supersymmetric partners of gluons and quarks is presented, involving signatures with jets and either two isolated leptons (electrons or muons) with the same electric charge, or at least three isolated leptons. A data sample of proton-proton collisions at root s = 13 TeV recorded with the ATLAS detector at the Large Hadron Collider between 2015 and 2018, corresponding to a total integrated luminosity of 139 fb(-1), is used for the search. No significant excess over the Standard Model expectation is observed. The results are interpreted in simplified supersymmetric models featuring both R-parity conservation and R-parity violation, raising the exclusion limits beyond those of previous ATLAS searches to 1600 GeV for gluino masses and 750 GeV for bottom and top squark masses in these scenarios. KW - Hadron-Hadron scattering (experiments) KW - Supersymmetry Y1 - 2020 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-277538 IS - 6 ER - TY - JOUR T1 - Search for triboson \({W^\pm}{W^\pm}{W^\mp}\) production in \(pp\) collisions at \(\sqrt{s}\) = 8 TeV with the ATLAS detector JF - European Physical Journal C N2 - This paper reports a search for triboson \({W^\pm}{W^\pm}{W^\mp}\) production in two decay channels (\({W^\pm}{W^\pm}{W^\mp}\) → \({ℓ^\pm}{νℓ^\pm}{νℓ^\mp}{ν}\) and \({W^\pm}{W^\pm}{W^\mp}\) → \({ℓ^\pm}{νℓ^\pm}{νjj}\) with \(ℓ=e,μ\)) in proton-proton collision data corresponding to an integrated luminosity of 20.3 fb\(^{−1}\) at a centre-of-mass energy of 8 TeV with the ATLAS detector at the Large Hadron Collider. Events with exactly three charged leptons, or two leptons with the same electric charge in association with two jets, are selected. The total number of events observed in data is consistent with the Standard Model (SM) predictions. The observed 95% confidence level upper limit on the SM \({W^\pm}{W^\pm}{W^\mp}\) production cross section is found to be 730 fb with an expected limit of 560 fb in the absence of SM \({W^\pm}{W^\pm}{W^\mp}\) production. Limits are also set on \(WWWW\) anomalous quartic gauge couplings. KW - high energy physics KW - triboson production KW - triple gauge couplings (TGCs) KW - quartic gauge couplings (QGCs) KW - decay channels Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173710 VL - 77 IS - 141 ER - TY - JOUR T1 - A measurement of the calorimeter response to single hadrons and determination of the jet energy scale uncertainty using LHC Run-1 \(pp\)-collision data with the ATLAS detector JF - European Physical Journal C N2 - A measurement of the calorimeter response to isolated charged hadrons in the ATLAS detector at the LHC is presented. This measurement is performed with 3.2 nb\(^{−1}\) of proton–proton collision data at \(\sqrt{s}\) = 7 TeV from 2010 and 0.1 nb\(^{−1}\) of data at \(\sqrt{s}\) = 8 TeV from 2012. A number of aspects of the calorimeter response to isolated hadrons are explored. After accounting for energy deposited by neutral particles, there is a 5% discrepancy in the modelling, using various sets of GEANT4 hadronic physics models, of the calorimeter response to isolated charged hadrons in the central calorimeter region. The description of the response to anti-protons at low momenta is found to be improved with respect to previous analyses. The electromagnetic and hadronic calorimeters are also examined separately, and the detector simulation is found to describe the response in the hadronic calorimeter well. The jet energy scale uncertainty and correlations in scale between jets of different momenta and pseudorapidity are derived based on these studies. The uncertainty is 2–5% for jets with transverse momenta above 2 TeV, where this method provides the jet energy scale uncertainty for ATLAS. KW - high energy physics KW - ATLAS detector KW - hadronic calorimeter KW - charged hadron response KW - identified particle response KW - hadronic physics Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173690 VL - 77 IS - 26 ER - TY - JOUR A1 - Aeschlimann, Martin A1 - Brixner, Tobias A1 - Cinchetti, Mirko A1 - Frisch, Benjamin A1 - Hecht, Bert A1 - Hensen, Matthias A1 - Huber, Bernhard A1 - Kramer, Christian A1 - Krauss, Enno A1 - Loeber, Thomas H. A1 - Pfeiffer, Walter A1 - Piecuch, Martin A1 - Thielen, Philip T1 - Cavity-assisted ultrafast long-range periodic energy transfer between plasmonic nanoantennas JF - Light: Science & Applications N2 - Radiationless energy transfer is at the core of diverse phenomena, such as light harvesting in photosynthesis\(^1\), energy-transfer-based microspectroscopies\(^2\), nanoscale quantum entanglement\(^3\) and photonic-mode hybridization\(^4\). Typically, the transfer is efficient only for separations that are much shorter than the diffraction limit. This hampers its application in optical communication and quantum information processing, which require spatially selective addressing. Here, we demonstrate highly efficient radiationless coherent energy transfer over a distance of twice the excitation wavelength by combining localized and delocalized\(^5\) plasmonic modes. Analogous to the Tavis-Cummings model, two whispering-gallery-mode antennas\(^6\) placed in the foci of an elliptical plasmonic cavity\(^7\) fabricated from single-crystal gold plates act as a pair of oscillators coupled to a common cavity mode. Time-resolved two-photon photoemission electron microscopy (TR 2P-PEEM) reveals an ultrafast long-range periodic energy transfer in accordance with the simulations. Our observations open perspectives for the optimization and tailoring of mesoscopic energy transfer and long-range quantum emitter coupling. KW - chemistry KW - nanocavities KW - nanophotonics and plasmonics KW - photonic devices Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173265 VL - 6 ER - TY - JOUR A1 - Ullherr, Maximilian A1 - Diez, Matthias A1 - Zabler, Simon T1 - Robust image reconstruction strategy for multiscalar holotomography JF - Journal of Imaging N2 - Holotomography is an extension of computed tomography where samples with low X-ray absorption can be investigated with higher contrast. In order to achieve this, the imaging system must yield an optical resolution of a few micrometers or less, which reduces the measurement area (field of view = FOV) to a few mm at most. If the sample size, however, exceeds the field of view (called local tomography or region of interest = ROI CT), filter problems arise during the CT reconstruction and phase retrieval in holotomography. In this paper, we will first investigate the practical impact of these filter problems and discuss approximate solutions. Secondly, we will investigate the effectiveness of a technique we call “multiscalar holotomography”, where, in addition to the ROI CT, a lower resolution non-ROI CT measurement is recorded. This is used to avoid the filter problems while simultaneously reconstructing a larger part of the sample, albeit with a lower resolution in the additional area. KW - reconstruction KW - region of interest KW - ROI KW - multiscalar holotomography KW - holotomography KW - computed tomography KW - CT KW - X-ray Y1 - 2022 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-262112 SN - 2313-433X VL - 8 IS - 2 ER - TY - RPRT A1 - Groß, Lennart T1 - Advices derived from troubleshooting a sensor-based adaptive optics direct stochastic optical reconstruction microscope T1 - Hinweise aus der Fehleranalyse eines Mikroskops mit direkter stochastischer optischer Rekonstruktion und sensorgestützter adaptiver Optik N2 - One rarely finds practical guidelines for the implementation of complex optical setups. Here, we aim to provide technical details on the decision making of building and revising a custom sensor-based adaptive optics (AO) direct stochastic optical reconstruction microscope (dSTORM) to provide practical assistance in setting up or troubleshooting similar devices. The foundation of this report is an instrument constructed as part of a master's thesis in 2021, which was built for deep tissue imaging. The setup is presented in the following way: (1) An optical and mechanical overview of the system at the beginning of this internship is given. (2) The optical components are described in detail in the order at which the light passes through, highlighting their working principle and implementation in the system. The optical component include (2A) a focus on even sample illumination, (2B) restoring telecentricity when working with commercial microscope bodies, (2C) the AO elements, namely the deformable mirror (DM) and the wavefront sensor, and their integration, and (2D) the separation of wavefront and image capture using fluorescent beads and a dichroic mirror. After addressing the limitations of the existing setup, modification options are derived. The modifications include the implementation of adjustment only light paths to improve system stability and revise the degrees of freedom of the components and changes in lens choices to meet the specifications of the AO components. Last, the capabilities of the modified setup are presented and discussed: (1) First, we enable epifluorescence imaging of bead samples through 180 µm unstained murine hippocampal tissue with wavefront error correction of ~ 90 %. Point spread function, wavefront shape and Zernike decomposition of bead samples are presented. (2) Second, we move from epifluorescent to dSTORM imaging of tubulin stained primary mouse hippocampal cells, which are imaged through up to 180 µm of unstained murine hippocampal tissue. We show that full width at half maximum (FWHM) of prominent features can be reduced in size by nearly a magnitude from uncorrected epiflourescence images to dSTORM images corrected by the adaptive optics. We present dSTORM localization count and FWHM of prominent features as as a function of imaging depth. N2 - Praktische Leitlinien für die Implementierung komplexer optischer Systeme sind selten zu finden. Hier wollen wir technische Details zur Entscheidungsfindung beim Bau und der Überarbeitung eines maßgefertigten Mikroskops mit sensorgestützter adaptiver Optik (AO) und direkter stochastischer optischer Rekonstruktion (dSTORM) bereitstellen, um praktische Hilfestellung bei der Einrichtung oder Fehlerbehebung ähnlicher Geräte zu geben. Grundlage dieses Berichts ist ein Instrument, das im Rahmen einer Masterarbeit im Jahr 2021 für die Abbildung von tiefem Gewebe gebaut wurde. Der Aufbau wird wie folgt dargestellt: (1) Es wird ein optischer und mechanischer Überblick über das System zu Beginn dieses Praktikums gegeben. (2) Die optischen Komponenten werden in der Reihenfolge, in der das Licht sie durchläuft, detailliert beschrieben und ihre Funktionsweise und Umsetzung im System hervorgehoben. Zu den optischen Komponenten gehören (2A) ein Fokus auf gleichmäßige Probenausleuchtung, (2B) die Wiederherstellung der Telezentrizität bei der Arbeit mit handelsüblichen Mikroskopkörpern, (2C) die AO-Elemente, nämlich der deformierbare Spiegel (DM) und der Wellenfrontsensor, und deren Integration, sowie (2D) die Trennung von Wellenfront- und Bilderfassung mittels fluoreszierender Beads und einem dichroitischen Spiegel. Nachdem die Einschränkungen des bestehenden Aufbaus angesprochen wurden, werden Modifikationsmöglichkeiten abgeleitet. Die Modifikationen umfassen die Implementierung von Justage-Lichtpfaden, um die Systemstabilität zu verbessern und die Freiheitsgrade der Komponenten zu überarbeiten, sowie Änderungen bei der Auswahl der Linsen, um die Spezifikationen der AO-Komponenten zu erfüllen. Abschließend werden die Ergebnisse des modifizierten Aufbaus vorgestellt und diskutiert: (1) Zunächst ermöglichen wir die Epifluoreszenz-Abbildung von Bead-Proben durch 180 µm ungefärbtes Hippocampus-Gewebe der Maus mit einer Wellenfront-Fehlerkorrektur von ~ 90 %. Es werden Punktspreizungsfunktion, Wellenfrontform und Zernike-Zerlegung von Bead-Proben vorgestellt. (2) Zweitens gehen wir von der Epifluoreszenz zur dSTORM-Bildgebung von Tubulin-gefärbten primären Hippocampuszellen der Maus über, die durch bis zu 180 µm ungefärbtes Hippocampusgewebe der Maus abgebildet werden. Wir zeigen, dass die Halbwertsbreite (Full Width at Half Maximum, FWHM) auffälliger Merkmale von unkorrigierten Epifloureszenz-Bildern zu dSTORM-Bildern, die durch die adaptive Optik korrigiert wurden, um fast eine Größenordnung reduziert werden kann. Wir präsentieren die Anzahl der dSTORM-Lokalisierungen und die FWHM auffälliger Merkmale als Funktion der Abbildungstiefe. KW - Einzelmolekülmikroskopie KW - Adaptive Optik KW - Adaptive Optics KW - Single Molecule Localization Microscopy KW - dSTORM Y1 - 2022 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-289951 ER - TY - JOUR T1 - Measurements of top-quark pair to \(Z\)-boson cross-section ratios at \(\sqrt{s}\) \(=13 , 8, 7\) TeV with the ATLAS detector JF - Journal of High Energy Physics N2 - Ratios of top-quark pair to \(Z\)-boson cross sections measured from proton-proton collisions at the LHC centre-of-mass energies of \(\sqrt{s}\) = 13 TeV, 8 TeV, and 7 TeV are presented by the ATLAS Collaboration. Single ratios, at a given \(\sqrt{s}\) for the two processes and at different \(\sqrt{s}\) for each process, as well as double ratios of the two processes at different \(\sqrt{s}\), are evaluated. The ratios are constructed using previously published ATLAS measurements of the \({t\overline{t}}\) and \(Z\)-boson production cross sections, corrected to a common phase space where required, and a new analysis of \(Z\) → ℓ\(^+\)ℓ\(^-\) where ℓ = \(e, µ\) at \(\sqrt{s}\) = 13 TeV performed with data collected in 2015 with an integrated luminosity of 3.2 fb\(^−1\). Correlations of systematic uncertainties are taken into account when evaluating the uncertainties in the ratios. The correlation model is also used to evaluate the combined cross section of the \(Z\) → \(e\)\(^+\)\(e\)\(^−\) and the \(Z\) → \(µ\)\(^+\)\(µ\)\(^−\) channels for each \(\sqrt{s}\) value. The results are compared to calculations performed at next-to-next-to-leading-order accuracy using recent sets of parton distribution functions. The data demonstrate significant power to constrain the gluon distribution function for the Bjorken-\(x\) values near 0.1 and the light-quark sea for \(x\) < 0.02. KW - High energy physics KW - Hadron-Hadron scattering (experiments) Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173544 VL - 2017 IS - 02 ER - TY - JOUR T1 - Measurements of charge and CP asymmetries in \(b\)-hadron decays using top-quark events collected by the ATLAS detector in \(pp\) collisions at \(\sqrt{s}\) = 8 TeV JF - Journal of High Energy Physics N2 - Same- and opposite-sign charge asymmetries are measured in lepton+jets \({t\overline{t}}\) events in which a \(b\)-hadron decays semileptonically to a soft muon, using data corresponding to an integrated luminosity of 20.3 fb\(^{−1}\) from proton-proton collisions at a centre-of-mass energy of \(\sqrt{s}\) = 8 TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. The charge asymmetries are based on the charge of the lepton from the top-quark decay and the charge of the soft muon from the semileptonic decay of a \(b\)-hadron and are measured in a fiducial region corresponding to the experimental acceptance. Four CP asymmetries (one mixing and three direct) are measured and are found to be compatible with zero and consistent with the Standard Model. KW - High energy physics KW - Hadron-Hadron scattering (experiments) Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173603 VL - 2017 IS - 02 ER -