TY - JOUR T1 - Search for new high-mass phenomena in the dilepton final state using 36 fb\(^{−1}\) of proton-proton collision data at \(\sqrt{s}=13\) TeV with the ATLAS detector JF - Journal of High Energy Physics N2 - A search is conducted for new resonant and non-resonant high-mass phenomena in dielectron and dimuon final states. The search uses 36.1 fb\(^{−1}\) of proton-proton collision data, collected at \(\sqrt{s}=13\) TeV by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the Standard Model prediction is observed. Upper limits at 95% credibility level are set on the cross-section times branching ratio for resonances decaying into dileptons, which are converted to lower limits on the resonance mass, up to 4.1 TeV for the E\(_6\)-motivated \(Z^′_χ\). Lower limits on the \({qqℓℓ}\) contact interaction scale are set between 2.4 TeV and 40 TeV, depending on the model. KW - High energy physics KW - Beyond Standard Model KW - Hadron-Hadron scattering (experiments) Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-172462 VL - 2017 IS - 182 ER - TY - JOUR T1 - Measurement of the inclusive jet cross-sections in proton-proton collisions at \(\sqrt{s}=8\) TeV with the ATLAS detector JF - Journal of High Energy Physics N2 - Inclusive jet production cross-sections are measured in proton-proton collisions at a centre-of-mass energy of \(\sqrt{s} = 8\) TeV recorded by the ATLAS experiment at the Large Hadron Collider at CERN. The total integrated luminosity of the analysed data set amounts to 20.2 fb\(^{−1}\). Double-differential cross-sections are measured for jets defined by the anti-\(k_t\) jet clustering algorithm with radius parameters of \(R\) = 0.4 and \(R\) = 0.6 and are presented as a function of the jet transverse momentum, in the range between 70 GeV and 2.5 TeV and in six bins of the absolute jet rapidity, between 0 and 3.0. The measured cross-sections are compared to predictions of quantum chromodynamics, calculated at next-to-leading order in perturbation theory, and corrected for non-perturbative and electroweak effects. The level of agreement with predictions, using a selection of different parton distribution functions for the proton, is quantified. Tensions between the data and the theory predictions are observed. KW - High energy physics KW - Hadron-Hadron scattering (experiments) KW - Jet physics Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173123 VL - 2017 IS - 09 ER - TY - JOUR T1 - Search for direct top squark pair production in events with a Higgs or \(Z\) boson, and missing transverse momentum in \(\sqrt{s}\) = 13 TeV \(pp\) collisions with the ATLAS detector JF - Journal of High Energy Physics N2 - A search for direct top squark pair production resulting in events with either a same-flavour opposite-sign dilepton pair with invariant mass compatible with a \(Z\) boson or a pair of jets compatible with a Standard Model (SM) Higgs boson (\(h\)) is presented. Requirements on the missing transverse momentum, together with additional selections on leptons, jets, jets identified as originating from \(b\)-quarks are imposed to target the other decay products of the top squark pair. The analysis is performed using proton-proton collision data at \(\sqrt{s}\) = 13 TeV collected with the ATLAS detector at the LHC in 2015–2016, corresponding to an integrated luminosity of 36.1 fb\(^{-1}\). No excess is observed in the data with respect to the SM predictions. The results are interpreted in two sets of models. In the first set, direct production of pairs of lighter top squarks (\(\tilde{t}_1\)) with long decay chains involving \(Z\) or Higgs bosons is considered. The second set includes direct pair production of the heavier top squark pairs (\(\tilde{t}_2\)) decaying via \(\tilde{t}_2\) → \(Z\tilde{t}_1\) or \(\tilde{t}_2\) → \(h\tilde{t}_1\). The results exclude at 95% confidence level \(\tilde{t}_2\) and \(\tilde{t}_1\) masses up to about 800 GeV, extending the exclusion region of supersymmetric parameter space covered by previous LHC searches. KW - High energy physics KW - Beyond Standard Model KW - Hadron-Hadron scattering (experiments) KW - Higgs physics Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-173210 VL - 2017 IS - 08 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 - JOUR T1 - Measurement of inclusive and differential cross sections in the \(H\) → \({ZZ}^*\) → \(4{ℓ}\) decay channel in \({pp}\) collisions at \(\sqrt{s} = 13\) TeV with the ATLAS detector JF - Journal of High Energy Physics N2 - Inclusive and differential fiducial cross sections of Higgs boson production in proton-proton collisions are measured in the \(H\) → \({ZZ^*}\) → \(4{ℓ}\) decay channel. The proton-proton collision data were produced at the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector in 2015 and 2016, corresponding to an integrated luminosity of 36.1 fb\(^{−1}\). The inclusive fiducial cross section in the \(H\) → \({ZZ^*}\) → \(4{ℓ}\) decay channel is measured to be 3.62 ± 0.50(stat)\(^{+0.25}_{− 0.20}\) (sys) fb, in agreement with the Standard Model prediction of 2.91 ± 0.13 fb. The cross section is also extrapolated to the total phase space including all Standard Model Higgs boson decays. Several differential fiducial cross sections are measured for observables sensitive to the Higgs boson production and decay, including kinematic distributions of jets produced in association with the Higgs boson. Good agreement is found between data and Standard Model predictions. The results are used to put constraints on anomalous Higgs boson interactions with Standard Model particles, using the pseudo-observable extension to the kappa-framework. KW - High energy physics KW - Hadron-Hadron scattering (experiments) KW - Higgs physics Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-172724 VL - 2017 IS - 10 ER - TY - JOUR T1 - Search for top quark decays \(t → qH\), with \(H → γγ\), in \(\sqrt{s} = 13\) TeV \(pp\) collisions using the ATLAS detector JF - Journal of High Energy Physics N2 - This article presents a search for flavour-changing neutral currents in the decay of a top quark into an up-type (\({q = c, u}\)) quark and a Higgs boson, where the Higgs boson decays into two photons. The proton-proton collision data set analysed amounts to 36.1 fb\(^{−1}\) at \(\sqrt{s} = 13\) TeV collected by the ATLAS experiment at the LHC. Top quark pair events are searched for, where one top quark decays into \(qH\) and the other decays into \(bW\). Both the hadronic and leptonic decay modes of the \(W\) boson are used. No significant excess is observed and an upper limit is set on the \({t → cH}\) branching ratio of 2.2 × 10\(^{−3}\) at the 95% confidence level, while the expected limit in the absence of signal is 1.6 × 10\(^{−3}\). The corresponding limit on the \(tcH\) coupling is 0.090 at the 95% confidence level. The observed upper limit on the \({t → uH}\) branching ratio is 2.4 × 10\(^{−3}\). KW - High energy physics KW - Flavour changing neutral currents KW - Hadron-Hadron scattering (experiments) KW - Higgs physics KW - Top physics Y1 - 2017 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-172568 VL - 2017 IS - 10 ER - TY - JOUR T1 - Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at \(\sqrt{s}\) = 13 TeV with the ATLAS detector JF - Journal of High Energy Physics N2 - A search for pair production of a scalar partner of the top quark in events with four or more jets plus missing transverse momentum is presented. An analysis of 36.1 fb\(^{−1}\) of \(\sqrt{s}\) = 13 TeV proton-proton collisions collected using the ATLAS detector at the LHC yields no significant excess over the expected Standard Model background. To interpret the results a simplified supersymmetric model is used where the top squark is assumed to decay via \(\tilde{t}_1\) → \(t^{(∗)}\)\(\tilde{χ}^0_1\) and \(\tilde{t}_1\) → \(b\tilde{χ}^±_1\) → \({bW}^{(∗)}\tilde{χ}^0_1\), where \(\tilde{χ}^0_1\) (\(\tilde{χ}^±_1\)) denotes the lightest neutralino (chargino). Exclusion limits are placed in terms of the top-squark and neutralino masses. Assuming a branching ratio of 100% to \(t\tilde{χ}^0_1\), top-squark masses in the range 450–1000 GeV are excluded for \(\tilde{χ}^0_1\) masses below 160 GeV. In the case where \(m_{\tilde{t}_1}\) ∼ \(m_t\) + \(m_{\tilde{χ}^0_1}\), top-squark masses in the range 235–590 GeV are excluded. 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-172161 VL - 12 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 - 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 A1 - Glinz, Jonathan A1 - Šleichrt, Jan A1 - Kytýř, Daniel A1 - Ayalur-Karunakaran, Santhosh A1 - Zabler, Simon A1 - Kastner, Johann A1 - Senck, Sascha T1 - Phase-contrast and dark-field imaging for the inspection of resin-rich areas and fiber orientation in non-crimp vacuum infusion carbon-fiber-reinforced polymers JF - Journal of Materials Science N2 - In this work, we present a multimodal approach to three-dimensionally quantify and visualize fiber orientation and resin-rich areas in carbon-fiber-reinforced polymers manufactured by vacuum infusion. Three complementary image modalities were acquired by Talbot–Lau grating interferometer (TLGI) X-ray microcomputed tomography (XCT). Compared to absorption contrast (AC), TLGI-XCT provides enhanced contrast between polymer matrix and carbon fibers at lower spatial resolutions in the form of differential phase contrast (DPC) and dark-field contrast (DFC). Consequently, relatively thin layers of resin, effectively indiscernible from image noise in AC data, are distinguishable. In addition to the assessment of fiber orientation, the combination of DPC and DFC facilitates the quantification of resin-rich areas, e.g., in gaps between fiber layers or at binder yarn collimation sites. We found that resin-rich areas between fiber layers are predominantly developed in regions characterized by a pronounced curvature. In contrast, in-layer resin-rich areas are mainly caused by the collimation of fibers by binder yarn. Furthermore, void volume around two adjacent 90°-oriented fiber layers is increased by roughly 20% compared to a random distribution over the whole specimen. Y1 - 2021 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-351581 VL - 56 IS - 16 ER -