TY - JOUR A1 - Heil, Hannah S. A1 - Schreiber, Benjamin A1 - Götz, Ralph A1 - Emmerling, Monika A1 - Dabauvalle, Marie-Christine A1 - Krohne, Georg A1 - Höfling, Sven A1 - Kamp, Martin A1 - Sauer, Markus A1 - Heinze, Katrin G. T1 - Sharpening emitter localization in front of a tuned mirror JF - Light: Science & Applications N2 - Single-molecule localization microscopy (SMLM) aims for maximized precision and a high signal-to-noise ratio1. Both features can be provided by placing the emitter in front of a metal-dielectric nanocoating that acts as a tuned mirror2,3,4. Here, we demonstrate that a higher photon yield at a lower background on biocompatible metal-dielectric nanocoatings substantially improves SMLM performance and increases the localization precision by up to a factor of two. The resolution improvement relies solely on easy-to-fabricate nanocoatings on standard glass coverslips and is spectrally and spatially tunable by the layer design and wavelength, as experimentally demonstrated for dual-color SMLM in cells. KW - imaging and sensing KW - super-resolution microscopy Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-228080 VL - 7 ER - TY - JOUR A1 - He, Jiangang A1 - Di Sante, Domenico A1 - Li, Ronghan A1 - Chen, Xing-Qiu A1 - Rondinelli, James M. A1 - Franchini, Cesare T1 - Tunable metal-insulator transition, Rashba effect and Weyl Fermions in a relativistic charge-ordered ferroelectric oxide JF - Nature Communications N2 - Controllable metal–insulator transitions (MIT), Rashba–Dresselhaus (RD) spin splitting, and Weyl semimetals are promising schemes for realizing processing devices. Complex oxides are a desirable materials platform for such devices, as they host delicate and tunable charge, spin, orbital, and lattice degrees of freedoms. Here, using first-principles calculations and symmetry analysis, we identify an electric-field tunable MIT, RD effect, and Weyl semimetal in a known, charge-ordered, and polar relativistic oxide Ag2BiO3 at room temperature. Remarkably, a centrosymmetric BiO6 octahedral-breathing distortion induces a sizable spontaneous ferroelectric polarization through Bi3+/Bi5+ charge disproportionation, which stabilizes simultaneously the insulating phase. The continuous attenuation of the Bi3+/Bi5+ disproportionation obtained by applying an external electric field reduces the band gap and RD spin splitting and drives the phase transition from a ferroelectric RD insulator to a paraelectric Dirac semimetal, through a topological Weyl semimetal intermediate state. These findings suggest that Ag2BiO3 is a promising material for spin-orbitonic applications. KW - electronic properties and materials KW - ferroelectrics and multiferroics KW - topological matter Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-227946 VL - 9 ER - TY - THES A1 - Zhao, Suting T1 - Symmetry Resolution of Entanglement in Holography T1 - Symmetrieaufgelöste Verschränkung in Holographie N2 - This thesis investigates the charged moments and the symmetry-resolved entanglement entropy in the context of the AdS3/CFT2 duality. In the first part, I focus on the holographic U(1) Chern-Simons-Einstein gravity, a toy model of AdS3/CFT2 with U(1) Kac-Moody symmetry. I start with the vacuum background with a single entangling interval. I show that, apart from a partition function in the grand canonical ensemble, the charged moments can also be interpreted as the two-point function of vertex operators on the replica surface. For the holographic description, I propose a duality between the bulk U(1) Wilson line and the boundary vertex operators. I verify this duality by deriving the effective action for the Chern-Simons fields and comparing the result with the vertex correlator. In the twist field approach, I show that the charged moments are given by the correlation function of the charged twist operators and the additional background operators. To solve the correlation functions involved, I prove the factorization of the U(1) extended conformal block into a U(1) block and a Virasoro block. The general expression for the U(1) block is derived by directly summing over the current descendant states, and the result shows that it takes an identical form as the vertex correlators. This leads to the conclusion that the disjoint Wilson lines compute the neutral U(1) block. The final result for the symmetry-resolved entanglement entropy shows that it is always charge-independent in this model. In the second part, I study charged moments in higher spin holography, where the boundary theory is a CFT with W3 symmetry. I define the notion of the higher spin charged moments by introducing a spin-3 modular charge operator. Restricting to the vacuum background with a single entangling interval, I employ the grand canonical ensemble interpretation and calculate the charged moments via the known higher spin black hole solution. On the CFT side, I perform a perturbative expansion for the higher spin charged moments in terms of the connected correlation functions of the spin-3 modular charge operators. Using the recursion relation for the correlation functions of the W3 currents, I evaluate the charged moments up to the quartic order of the chemical potential. The final expression matches with the holographic result. My results both for U(1) Chern-Simons Einstein gravity and W3 higher spin gravity constitute novel checks of the AdS3/CFT2 correspondence. N2 - Diese Arbeit untersucht die Symmetrie-aufgelöste Verschränkungsentropie im Kontext der AdS3/CFT2-Dualität. Im ersten Teil konzentriere ich mich auf die holographische U(1) Chern-Simons-Einstein- Gravitations-Theorie, welches ein Spielzeugmodell für AdS3/CFT2 mit U(1) Kac-Moody-Symmetrie ist. Ich beginne mit dem Vakuumhintergrund mit einem einzigen Verschränkungsintervall. Ich zeige, dass neben einer Partitionsfunktion im großen kanonischen Ensemble die geladenen Momente auch als Zweipunktfunktion von Vertex-Operatoren auf der Replikationsoberfläche interpretiert werden können. Für deren holographische Beschreibung wähle ich eine Dualität zwischen der Bulk U(1) Wilson-Linie und den Randvertexoperatoren. Diese Dualität verifiziere ich, indem ich die effektive Wirkung für die Chern-Simons-Felder herleite und das Ergebnis mit dem Vertex-Korrelator vergleiche. Im Twist-Field-Ansatz zeige ich, dass die geladenen Momente durch die Korrelationsfunktion der geladenen Twist-Operatoren und der zusätzlichen Hintergrundoperatoren gegeben sind. Um die beteiligten Korrelationsfunktionen zu lösen, beweise ich die Faktorisierung des U(1) erweiterten konformen Blocks in einen U(1)-Block und einen Virasoro- Block. Der allgemeine Ausdruck für den U(1) Block wird direkt durch die Summierung über alle Absteigerzustände hergeleitet. Das erzielte Ergebnis hat tatsächlich die gleiche Form wie die Vertex-Korrelatoren hat. Dies führt zur Schlussfolgerung, dass die getrennten Wilson-Linien den neutralen U(1) Block berechnen. Das Endergebnis für die Symmetrieaufgelöste Verschränkungsentropie zeigt, dass sie in diesem Modell immer ladungsunabhängig ist. Im zweiten Teil untersuche ich geladene Momente in der Holographie höherer Spins, wobei die Randtheorie eine CFT mit W3 Symmetrie ist. Ich definiere das Konzept der geladenen Momente höheren Spins, indem ich einen Spin-3-modularen Ladungsoperator einführe.Wenn ich mich auf den Vakuum-Hintergrund mit einem einzelnen Verschränkungsintervall beschränke, nutze ich die Interpretation des großkanonischen Ensembles und berechne die geladenen Momente mithilfe der bekannten Lösung für das schwarze Loch höheren Spins. Auf der CFT-Seite führe ich eine perturbative Expansion für die höheren spingeladenen Momente in Bezug auf die verbundenen Korrelationsfunktionen der modularen Spin-3-Ladungsoperatoren durch. Unter Verwendung der Rekursionsrelationen für die Korrelationsfunktionen der W3-Ströme werte ich die geladenen Momente bis zur quartischen Ordnung des chemischen Potenzials aus. Das endgültige Ergebnis stimmt mit dem holographischen Ergebnis überein. Meine Ergebnisse für U(1) Chern-Simons-Einstein-Gravitation und W3 höhere Spingravitation stellen neuartige Überprüfungen des AdS3/CFT2 dar Korrespondenz. KW - AdS-CFT-Korrespondenz KW - Gauge/Gravity Duality KW - Symmetry Resolution KW - Quantum Information Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-363854 ER - TY - THES A1 - Kappes, Alexander T1 - High-Redshift Blazars Observed by the International LOFAR Telescope T1 - Mit dem internationalen LOFAR-Teleskop beobachtete Blazare mit hoher Rotverschiebung N2 - This work presents the first ILT observations of high redshift blazars and their study in terms of jet evolution, morphology, and interaction with the surrounding medium. Each of these represents a highly topical area of astronomywith a large number of open questions. To better understand Active Galactic Nuclei (AGN) and their fundamental inner workings, new techniques are needed to exploit the full potential of the next generation of radio interferometers. Some of these tools are presented here and applied to one of the latest generation of software radio telescopes. A major focus of the studies presented is on the unification model, where the observed blazars are discussed for their properties to be rotated counterparts of Fanaroff-Riley Class II (FR-II) radio galaxies, when classified as Flat Spectrum Radio Quasars (FSRQs). In addition, multiwavelength information has been included in the analysis. Both studies are feasibility studies that will serve as a basis for future similar studies. The characteristics discussed and their interpretation do not allow conclusions to be drawn for their respective populations. However, by applying them to a larger number of targets, population studies will be possible. The first chapters introduce the necessary topics, AGN, principles of radio observations and ILT, in the necessary depth to provide the reader with a solid knowledge base. They are particularly important for understanding the current limits and influences of uncertainties in the observation, calibration and imaging process. But they also shed light on realistic future improvements. A particular focus is on the development and evolution of the LOw-Frequency ARray (LOFAR)-Very Long Baseline Interferometry (VLBI) pipeline. With the tools at hand, the first study addresses the high redshift blazar S5 0836+710 $(z=2.218)$, which has been observed at various wavelengths and resolutions. It has a disrupted one-sided jet with an associated extended region further out. Despite the excellent wavelength coverage, only the additional ILT observations provided a complete picture of the source. With the data, the extended region could be classified as a hotspot moving at slightly relativistic speeds.. With the ILT data it was also possible to extract the flux of the core region of the AGN, and in projection to reveal the mixed counter-hotspot behind it. This also allowed constraints on jet parameters and environmental properties to be modelled, which were previously inconclusive. Technically, this study shows that the ILT can be used as an effective VLBI array for compact sources with small angular scales. However, the detection of faint components beyond redshifts of $z=2$ may require the capabilities of the Square Kilometre Array (SKA) to provide a significant number of detections to enable statistical conclusions. The second study uses a much improved calibration pipeline to analyse the high redshift blazar GB1508+5714 $(z=4.30)$. The ILT data revealed a previously unseen component in the eastern direction. A spectral index map was generated from the Karl G. Jansky Very Large Array (VLA) data, showing spectral index values of $-1.2_{-0.2}^{+0.4}$ for the western component, steeper than $-1.1$ for the eastern region, and $0.023 \pm 0.007$ for the core. Using the information provided by the ILT observation, as well as multi-wavelength information from other observations ranging from the long radio wavelengths to the $\gamma$ regime, four models were developed to interpret the observed flux with different emission origins. This also allowed to test a proposed interaction channel of the electrons provided by the jet, to cool off via inverse compton scattering with the Cosmic Microwave Background (CMB) photons, rather than by the usual synchrotron emission. This is referred to as cmb quenching in the literature, which could be shown in the study, to be necessary in any case. Finally, one of the four models was considered in which the hotspots in the detected components are unresolved and mixed by the lobe emission, with the X-ray emission coming from the lobes and partially mixed by the bright core region. The results of this preferred model are consistent with hotspots in a state of equipartition and lobes almost so. The study shows that high redshift blazars can be studied with the ILT, and expanding the sample of high redshift blazars resolved at multiple frequencies will allow a statistical study of the population. Finally, this work successfully demonstrates the powerful capabilities of the ILT to address questions that were previously inaccessible. The current state of the LOFAR-VLBI pipeline, when properly executed, allows work on the most challenging objects and will only improve in the future. In particular, this gives a glimpse of the possibilities that SKA will bring to astronomy. N2 - In dieser Arbeit werden die ersten Beobachtungen von Blazaren mit hoher Rotverschiebung, sowie ihre Untersuchung im Hinblick auf die Jet-Entwicklung, die Morphologie und die Wechselwirkung mit dem umgebenden Medium vorgestellt. Jeder dieser Bereiche stellt ein hochaktuelles Gebiet der Astronomie, mit einer großen Anzahl offener Fragen, dar. Um Active Galactic Nuclei (AGN) und ihr fundamentales Innenleben besser zu verstehen, sind neue Techniken erforderlich, um das volle Potenzial der nächsten Generation von Radiointerferometern auszuschöpfen. Einige dieser Werkzeuge werden hier vorgestellt und auf ein Teleskop der neuesten Generation von Software-Radioteleskopen angewandt. Ein Hauptaugenmerk der vorgestellten Studien liegt auf dem "Unification Model", bei dem die beobachteten Blazare auf ihre Eigenschaften als rotierte Gegenstücke von Fanaroff-Riley Class II (FR-II)-Radiogalaxien untersucht werden, wenn sie als Flat Spectrum Radio Quasars (FSRQs) klassifiziert werden. Darüber hinaus wurden Informationen über mehrere Wellenlängen in die Analyse einbezogen. Bei beiden Studien handelt es sich um Machbarkeitsstudien, die als Grundlage für künftige ähnliche Studien dienen werden. Die erörterten Merkmale und ihre Interpretation lassen keine Schlussfolgerungen für die jeweiligen Populationen zu. Erst durch die Anwendung auf eine größere Anzahl von Objekten werden Populationsstudien möglich sein. Die ersten Kapitel führen in die notwendigen Themen, AGN, Prinzipien der Radiobeobachtung und das International LOFAR Telescope (ILT), in der notwendigen Tiefe ein, um dem Leser eine solide Wissensbasis zu vermitteln. Sie sind besonders wichtig, um die aktuellen Grenzen und Einflüsse von Unsicherheiten im Beobachtungs-, Kalibrierungs- und Abbildungsprozess zu verstehen. Sie geben aber auch Aufschluss über realistische zukünftige Verbesserungen. Ein besonderer Schwerpunkt liegt auf der Entwicklung und Weiterentwicklung der LOw-Frequency ARray (LOFAR)-Very Long Baseline Interferometry (VLBI)-Pipeline. Mit den zur Verfügung stehenden Werkzeugen befasst sich die erste Studie mit dem hochrotverschobenen Blazar S5 0836+710 (z=2.218), der bei verschiedenen Wellenlängen und Auflösungen beobachtet wurde. Er hat einen unterbrochenen einseitigen Jet mit einer damit verbundenen ausgedehnten Region weiter außen. Trotz der hervorragenden Wellenlängenabdeckung ermöglichten erst die zusätzlichen Beobachtungen durch das ILT ein vollständiges Bild der Quelle. Mit den Daten konnte die ausgedehnte Region als Hotspot klassifiziert werden, der sich mit leicht relativistischen Geschwindigkeiten bewegt. Mit den ILT-Daten war es auch möglich, den Fluss der Kernregion des AGN zu extrahieren und in der Projektion den Hotspot des gegenläufigen Jets dahinter aufzudecken. Dies ermöglichte auch die Modellierung von Jet-Parametern und Umgebungseigenschaften, die zuvor nicht zugänglich waren. Technisch gesehen zeigt diese Studie insbesondere, dass das ILT als VLBI-Array für kompakte Quellen mit kleinen Winkelskalen effektiv verwendet werden kann. Die Entdeckung schwacher Komponenten jenseits von Rotverschiebungen von $z=2$ könnte jedoch das SquareKilometre Array (SKA) erfordern, um eine signifikante Anzahl von Entdeckungen zu liefern, welche statistische Schlussfolgerungen zulassen. Die zweite Studie verwendet eine stark verbesserte Kalibrierungspipeline, um den hoch rotverschobenen Blazar GB 1508+5714 (z=4.30) zu analysieren. Die ILT-Daten enthüllten eine bisher nicht gesehene Komponente in östlicher Richtung. Mit den Karl G. Jansky Very Large Array (VLA)-Daten wurde eine Spektralindexkarte erstellt, die Spektralindexwerte von $-1,2^{+0,4}_{-0,2}$ für die westliche Komponente, steiler als $-1,1$ für die östliche Region und $0,023 \pm 0,007$ für den Kern zeigt. Anhand der von der ILT-Beobachtung gelieferten Informationen sowie von Multi-Wellenlängen-Informationen aus anderen Beobachtungen, die von den langen Radiowellenlängen bis zum $\gamma$-Bereich reichen, wurden vier Modelle entwickelt, um den beobachteten Fluss mit unterschiedlichen Emissionsquellen zu interpretieren. Dies ermöglichte es auch, einen vorgeschlagenen Wechselwirkungskanal der Elektronen, welche durch den Jet bereitgestellt werden, zu testen, um sich durch inverse Compton-Streuung mit den Photonen der kosmischen Hintergrundstrahlung abzukühlen, anstatt durch die übliche Synchrotronemission. Dies wird in der Literatur als "CMB-Quenching" bezeichnet, welches in der Studie, als in jedem Fall notwendig, nachgewiesen werden konnte. Schließlich wurde eines der vier Modelle in Betracht gezogen, bei dem die Hotspots in den nachgewiesenen Komponenten unaufgelöst sind und durch die Lobe-Emission vermischt werden, wobei die Röntgenemission von den Lobes stammt und teilweise durch die helle Kernregion vermischt wird. Die Ergebnisse dieses bevorzugten Modells zeigen, dass sich die Hot Spots und Lobes nahezu in einem Zustand der Äquipartition befinden. Die Studie zeigt somit, dass Blazare mit hoher Rotverschiebung mit dem ILT untersucht werden können, und die Hinzunahme von weiteren Blazaren mit hoher Rotverschiebung, die mit mehreren Frequenzen aufgelöst wurden, eine statistische Untersuchung der Population ermöglichen werden. Schließlich demonstriert diese Arbeit erfolgreich die leistungsstarken Fähigkeiten des ILT, um Fragen anzugehen, die zuvor unzugänglich waren. Der derzeitige Stand der LOFAR-VLBI-Pipeline ermöglicht bei ordnungsgemäßer Ausführung die Arbeit an den anspruchsvollsten Objekten und wird sich in Zukunft noch weiter verbessern. Dies gibt insbesondere einen Einblick in die Möglichkeiten, die das SKA der Astronomie bieten wird. KW - Blazar KW - Kosmologie KW - Radioastronomie KW - Astrophysik KW - Cosmology KW - Radioastronomy KW - Astrophysics KW - LOFAR KW - International LOFAR Telescope Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-361444 ER - TY - THES A1 - Wagner, Tim Matthias T1 - Characterization of 2D antimony lattices T1 - Charakterisierung 2D Antimon Atomgitter N2 - Two-dimensional lattices are in the focus of research in modern solid state physics due to their novel and exotic electronic properties with tremendous potential for seminal future applications. Of particular interest within this research field are quantum spin Hall insulators which are characterized by an insulating bulk with symmetry-protected metallic edge states. For electrons within these one-dimensional conducting channels, spin-momentum locking enables dissipationless transport - a property which promises nothing short of a revolution for electronic devices. So far, however, quantum spin Hall materials require enormous efforts to be realized such as cryogenic temperatures or ultra-high vacuum. A potential candidate to overcome these shortcomings are two-dimensional lattices of the topological semi-metal antimony due to their potential to host the quantum spin Hall effect while offering improved resilience against oxidation. In this work, two-dimensional lattices of antimony on different substrates, namely Ag(111), InSb(111) and SiC(0001), are investigated regarding their atomic structure and electronic properties with complimentary surface sensitive techniques. In addition, a systematic oxidation study compares the stability of Sb-SiC(0001) with that of the two-dimensional topological insulators bismuthene-SiC(0001) and indenene-SiC(0001). A comprehensive experimental analysis of the \((\sqrt{3}\times\sqrt{3})R30^\circ\) Sb-Ag(111) surface, including X-ray standing wave measurements, disproves the proclaimed formation of a buckled antimonene lattice in literature. The surface lattice can instead be identified as a metallic Ag\(_2\)Sb surface alloy. Antimony on InSb(111) shows an unstrained Volmer-Weber island growth due to its large lattice mismatch to the substrate. The concomitant moir\'{e} situation at the interface imprints mainly in a periodic height corrugation of the antimony islands which as observed with scanning tunneling microscopy. On islands with various thicknesses, quasiparticle interference patterns allow to trace the topological surface state of antimony down to the few-layer limit. On SiC(0001), two different two-dimensional antimony surface reconstructions are identified. Firstly, a metallic triangular $1\times1$ lattice which constitutes the antimony analogue to the topological insulator indenene. Secondly, an insulating asymmetric kagome lattice which represents the very first realized atomic surface kagome lattice. A comparative, systematic oxidation study of elemental (sub-)monolayer materials on SiC(0001) reveals a high sensitivity of indenene and bismuthene to small dosages of oxygen. An improved resilience is found for Sb-SiC(0001) which, however, oxidizes nevertheless if exposed to oxygen. These surface lattices are therefore not suitable for future applications without additional protective measures. N2 - Zweidimensionale Kristallgitter sind aufgrund ihrer neuartigen, exotischen elektronischen Eigenschaften ein hochaktuelles Thema der modernen Festkörperphysik mit enormen Potential für bahnbrechende zukünftige Anwendungen. Die Klasse der Quanten-Spin-Hall-Isolatoren erfährt in diesem Zusammenhang besondere Aufmerksamkeit in der aktuellen Forschung aufgrund ihrer durch Symmetrie geschützten, metallischen Randkanäle. In diesen ermöglicht das sogenannte "spin-momentum locking" der Elektronen einen verlustfreien Ladungstransport - eine Eigenschaft, die nichts weniger als eine Revolution auf dem Gebiet der Elektronik verspricht. Bisher konnten Quanten-Spin-Hall-Isolatoren allerdings nur unter enormem Aufwand bei kryogenen Temperaturen oder im Ultrahochvakuum realisiert werden. Eine Materialkandidat welcher es ermöglichen könnte diese Unzulänglichkeit-en zu überwinden, sind zweidimensionale Gitter des topologischen Halbmetalls Antimon. Diese zeigen zum einen eine erhöhte Widerstandsfähigkeit gegen Oxidation und gelten zum anderen als potentielle Kandidaten für die Realisierung eben jenes Quanten-Spin-Hall-Effekts. Im Rahmen dieser Arbeit werden zweidimensionale Antimongitter auf unterschiedlichen Substraten, nämlich Ag(111), InSb(111) und SiC(0001), mit komplementären oberflächensensitiven Messmethoden hinsichtlich ihrer atomaren Struktur und elektronischen Eigenschaften untersucht. Zusätzlich wird mittels einer systematischen Oxydationsstudie die Stabilität von Sb-SiC(0001) mit derjenigen der topologischen Isolatoren Bismuthene-SiC(0001) und Indenene-SiC(0001) verglichen. Eine umfängliche experimentelle Analyse der \((\sqrt{3}\times\sqrt{3})R30^\circ\) Sb-Ag(111) Oberfläche, inklusive stehenden Röntgenwellenfeldern, widerlegt die in der Literatur beschriebene Ausbildung eines gefalteten Antimonene-Gitters. Die Oberflächenstruktur kann stattdessen als metallische Ag\(_2\)Sb Oberflächenlegierung identifiziert werden. Auf InSb(111) zeigt Antimon, bedingt durch den großen Unterschied in der Gitterkonstante, ein unverzerrtes Volmer-Weber Inselwachstum. Die damit einhergehende Moir\'{e} Situation an der Grenzfläche spiegelt sich dabei in einer periodischen Wellung der Oberfläche wieder. Auf Antimon-Inseln unterschiedlicher Dicke kann der topologische Oberflächenzustand mittels Quasi-Teilchen-Interferenzmustern bis hinab auf Schichtdicken von wenigen Atomlagen beobachtet werden. Auf SiC(0001) können zwei unterschiedliche zweidimensionale Oberflächenrekonstruktionen von Antimon identifiziert werden. Zum einen ein metallisches $1\times1$ Dreiecksgitter, dem Antimon-Analogon zum topologischen Isolator Indenene. Zum anderen ein isolierendes asymme-trisches Antimon Kagomegitter - das Erste jemals hergestellte atomare Oberflächengitter mit Kagome-Struktur. Eine vergleichende systematische Oxydationsstudie von elementaren (Sub-)Monolagen-materialien auf SiC(0001) zeigt eine hohe Anfälligkeit von Indenene und Bismuthene gegen-über selbst kleinen Dosen an Sauerstoff. Sb-SiC(0001) zeigt eine deutlich stärkere Oxidationsresistenz, oxidiert aber ebenfalls in Kontakt mit Sauerstoff. Die untersuchten Oberflächengitter sind somit ohne zusätzliche Schutzmaßnahmen nicht für zukünftige Anwendungen nutzbar. KW - Antimon KW - experimental physics KW - condensed matter KW - 2D KW - antimony KW - ultra high vacuum KW - scanning tunneling microscopy KW - angle resolved photoemission spectroscopy KW - epitaxial growth KW - topological insulator KW - kagome lattice KW - Atomgitter Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-363292 ER - TY - JOUR T1 - Combination of inclusive and differential t(t)over-bar charge asymmetry measurements using ATLAS and CMS data at root S=7 and 8 TeV JF - Journal of High Energy Physics N2 - This paper presents combinations of inclusive and differential measurements of the charge asymmetry (A(C)) in top quark pair (t(t)over-bar) events with a lepton+jets signature by the ATLAS and CMS Collaborations, using data from LHC proton-proton collisions at centre-of-mass energies of 7 and 8 TeV. The data correspond to integrated luminosities of about 5 and 20 fb(-1) for each experiment, respectively. The resulting combined LHC measurements of the inclusive charge asymmetry are A(C)(LHC7) = 0.005 +/- 0.007 (stat) +/- 0.006 (syst) at 7 TeV and A(C)(LHC8) = 0.0055 +/- 0.0023 (stat) +/- 0.0025 (syst) at 8 TeV. These values, as well as the combination of A(C) measurements as a function of the invariant mass of the t(t)over-bar system at 8 TeV, are consistent with the respective standard model predictions. KW - Hadron-Hadron scattering (experiments) KW - Patron distributions KW - Top physics KW - PP Collisions Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-312669 VL - 33 IS - 4 ER - TY - JOUR A1 - Kreinberg, Sören A1 - Porte, Xavier A1 - Schicke, David A1 - Lingnau, Benjamin A1 - Schneider, Christian A1 - Höfling, Sven A1 - Kanter, Ido A1 - Lüdge, Kathy A1 - Reitzenstein, Stephan T1 - Mutual coupling and synchronization of optically coupled quantum-dot micropillar lasers at ultra-low light levels JF - Nature Communications N2 - Synchronization of coupled oscillators at the transition between classical physics and quantum physics has become an emerging research topic at the crossroads of nonlinear dynamics and nanophotonics. We study this unexplored field by using quantum dot microlasers as optical oscillators. Operating in the regime of cavity quantum electrodynamics (cQED) with an intracavity photon number on the order of 10 and output powers in the 100 nW range, these devices have high β-factors associated with enhanced spontaneous emission noise. We identify synchronization of mutually coupled microlasers via frequency locking associated with a sub-gigahertz locking range. A theoretical analysis of the coupling behavior reveals striking differences from optical synchronization in the classical domain with negligible spontaneous emission noise. Beyond that, additional self-feedback leads to zero-lag synchronization of coupled microlasers at ultra-low light levels. Our work has high potential to pave the way for future experiments in the quantum regime of synchronization. KW - nanoscale devices KW - quantum optics KW - semiconductor lasers Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-229811 VL - 10 ER - TY - JOUR A1 - Kremer, Mark A1 - Biesenthal, Tobias A1 - Maczewsky, Lukas J. A1 - Heinrich, Matthias A1 - Thomale, Ronny A1 - Szameit, Alexander T1 - Demonstration of a two-dimensional PT-symmetric crystal JF - Nature Communications N2 - With the discovery of PT-symmetric quantum mechanics, it was shown that even non-Hermitian systems may exhibit entirely real eigenvalue spectra. This finding did not only change the perception of quantum mechanics itself, it also significantly influenced the field of photonics. By appropriately designing one-dimensional distributions of gain and loss, it was possible to experimentally verify some of the hallmark features of PT-symmetry using electromagnetic waves. Nevertheless, an experimental platform to study the impact of PT-symmetry in two spatial dimensions has so far remained elusive. We break new grounds by devising a two-dimensional PT-symmetric system based on photonic waveguide lattices with judiciously designed refractive index landscape and alternating loss. With this system at hand, we demonstrate a non-Hermitian two-dimensional topological phase transition that is closely linked to the emergence of topological mid-gap edge states. KW - micro-optics KW - optical materials and structures KW - topological matter Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-230132 VL - 10 ER - TY - JOUR A1 - Schneider, Christian A1 - Glazov, Mikhail M. A1 - Korn, Tobias A1 - Höfling, Sven A1 - Urbaszek, Bernhard T1 - Two-dimensional semiconductors in the regime of strong light-matter coupling JF - Nature Communications N2 - The optical properties of transition metal dichalcogenide monolayers are widely dominated by excitons, Coulomb-bound electron–hole pairs. These quasi-particles exhibit giant oscillator strength and give rise to narrow-band, well-pronounced optical transitions, which can be brought into resonance with electromagnetic fields in microcavities and plasmonic nanostructures. Due to the atomic thinness and robustness of the monolayers, their integration in van der Waals heterostructures provides unique opportunities for engineering strong light-matter coupling. We review first results in this emerging field and outline future opportunities and challenges. KW - optical physics KW - two-dimensional materials Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-231295 VL - 9 ER - TY - JOUR A1 - Schmitt, Martin A1 - Moras, Paolo A1 - Bihlmayer, Gustav A1 - Cotsakis, Ryan A1 - Vogt, Matthias A1 - Kemmer, Jeannette A1 - Belabbes, Abderrezak A1 - Sheverdyaeva, Polina M. A1 - Kundu, Asish K. A1 - Carbone, Carlo A1 - Blügel, Stefan A1 - Bode, Matthias T1 - Indirect chiral magnetic exchange through Dzyaloshinskii–Moriya-enhanced RKKY interactions in manganese oxide chains on Ir(100) JF - Nature Communications N2 - Localized electron spins can couple magnetically via the Ruderman–Kittel–Kasuya–Yosida interaction even if their wave functions lack direct overlap. Theory predicts that spin–orbit scattering leads to a Dzyaloshinskii–Moriya type enhancement of this indirect exchange interaction, giving rise to chiral exchange terms. Here we present a combined spin-polarized scanning tunneling microscopy, angle-resolved photoemission, and density functional theory study of MnO2 chains on Ir(100). Whereas we find antiferromagnetic Mn–Mn coupling along the chain, the inter-chain coupling across the non-magnetic Ir substrate turns out to be chiral with a 120° rotation between adjacent MnO2 chains. Calculations reveal that the Dzyaloshinskii–Moriya interaction results in spin spirals with a periodicity in agreement with experiment. Our findings confirm the existence of indirect chiral magnetic exchange, potentially giving rise to exotic phenomena, such as chiral spin-liquid states in spin ice systems or the emergence of new quasiparticles. KW - magnetic properties and materials KW - surfaces, interfaces and thin films Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-230986 VL - 10 ER - TY - JOUR A1 - China, Swarup A1 - Burrows, Susannah M. A1 - Wang, Bingbing A1 - Harder, Tristan H. A1 - Weis, Johannes A1 - Tanarhte, Meryem A1 - Rizzo, Luciana V. A1 - Brito, Joel A1 - Cirino, Glauber G. A1 - Ma, Po-Lun A1 - Cliff, John A1 - Artaxo, Paulo A1 - Gilles, Mary K. A1 - Laskin, Alexander T1 - Fungal spores as a source of sodium salt particles in the Amazon basin JF - Nature Communications N2 - In the Amazon basin, particles containing mixed sodium salts are routinely observed and are attributed to marine aerosols transported from the Atlantic Ocean. Using chemical imaging analysis, we show that, during the wet season, fungal spores emitted by the forest biosphere contribute at least 30% (by number) to sodium salt particles in the central Amazon basin. Hydration experiments indicate that sodium content in fungal spores governs their growth factors. Modeling results suggest that fungal spores account for ~69% (31–95%) of the total sodium mass during the wet season and that their fractional contribution increases during nighttime. Contrary to common assumptions that sodium-containing aerosols originate primarily from marine sources, our results suggest that locally-emitted fungal spores contribute substantially to the number and mass of coarse particles containing sodium. Hence, their role in cloud formation and contribution to salt cycles and the terrestrial ecosystem in the Amazon basin warrant further consideration. KW - atmospheric chemistry KW - biogeochemistry KW - environmental sciences Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-222492 VL - 9 ER - TY - JOUR A1 - Ciuchi, Sergio A1 - Di Sante, Domenico A1 - Dobrosavljević, Vladimir A1 - Fratini, Simone T1 - The origin of Mooij correlations in disordered metals JF - npj Quantum Materials N2 - Sufficiently disordered metals display systematic deviations from the behavior predicted by semi-classical Boltzmann transport theory. Here the scattering events from impurities or thermal excitations can no longer be considered as additive-independent processes, as asserted by Matthiessen’s rule following from this picture. In the intermediate region between the regime of good conduction and that of insulation, one typically finds a change of sign of the temperature coefficient of resistivity, even at elevated temperature spanning ambient conditions, a phenomenology that was first identified by Mooij in 1973. Traditional weak coupling approaches to identify relevant corrections to the Boltzmann picture focused on long-distance interference effects such as “weak localization”, which are especially important in low dimensions (1D and 2D) and close to the zero-temperature limit. Here we formulate a strong-coupling approach to tackle the interplay of strong disorder and lattice deformations (phonons) in bulk three-dimensional metals at high temperatures. We identify a polaronic mechanism of strong disorder renormalization, which describes how a lattice locally responds to the relevant impurity potential. This mechanism, which quantitatively captures the Mooij regime, is physically distinct and unrelated to Anderson localization, but realizes early seminal ideas of Anderson himself, concerning the interplay of disorder and lattice deformations. KW - electronic properties and materials KW - phase transitions and critical phenomena KW - theory and computation Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-223148 VL - 3 ER - TY - JOUR A1 - Kreinberg, Sören A1 - Grbešić, Tomislav A1 - Strauß, Max A1 - Carmele, Alexander A1 - Emmerling, Monika A1 - Schneider, Christian A1 - Höfling, Sven A1 - Porte, Xavier A1 - Reitzenstein, Stephan T1 - Quantum-optical spectroscopy of a two-level system using an electrically driven micropillar laser as a resonant excitation source JF - Light: Science & Applications N2 - Two-level emitters are the main building blocks of photonic quantum technologies and are model systems for the exploration of quantum optics in the solid state. Most interesting is the strict resonant excitation of such emitters to control their occupation coherently and to generate close to ideal quantum light, which is of utmost importance for applications in photonic quantum technology. To date, the approaches and experiments in this field have been performed exclusively using bulky lasers, which hinders the application of resonantly driven two-level emitters in compact photonic quantum systems. Here we address this issue and present a concept for a compact resonantly driven single-photon source by performing quantum-optical spectroscopy of a two-level system using a compact high-β microlaser as the excitation source. The two-level system is based on a semiconductor quantum dot (QD), which is excited resonantly by a fiber-coupled electrically driven micropillar laser. We dress the excitonic state of the QD under continuous wave excitation, and trigger the emission of single photons with strong multi-photon suppression (g\(^{(2)}\)(0)=0.02) and high photon indistinguishability (V = 57±9%) via pulsed resonant excitation at 156 MHz. These results clearly demonstrate the high potential of our resonant excitation scheme, which can pave the way for compact electrically driven quantum light sources with excellent quantum properties to enable the implementation of advanced quantum communication protocols. KW - near-infrared spectroscopy KW - photonic devices KW - semiconductor lasers KW - single photons and quantum effects Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-229802 VL - 7 ER - TY - JOUR A1 - Lee, Ching Hua A1 - Imhof, Stefan A1 - Berger, Christian A1 - Bayer, Florian A1 - Brehm, Johannes A1 - Molenkamp, Laurens W. A1 - Kiessling, Tobias A1 - Thomale, Ronny T1 - Topolectrical Circuits JF - Communications Physics N2 - Invented by Alessandro Volta and Félix Savary in the early 19th century, circuits consisting of resistor, inductor and capacitor (RLC) components are omnipresent in modern technology. The behavior of an RLC circuit is governed by its circuit Laplacian, which is analogous to the Hamiltonian describing the energetics of a physical system. Here we show that topological insulating and semimetallic states can be realized in a periodic RLC circuit. Topological boundary resonances (TBRs) appear in the impedance read-out of a topolectrical circuit, providing a robust signal for the presence of topological admittance bands. For experimental illustration, we build the Su-Schrieffer–Heeger circuit, where our impedance measurement detects the TBR midgap state. Topolectrical circuits establish a bridge between electrical engineering and topological states of matter, where the accessibility, scalability, and operability of electronics synergizes with the intricate boundary properties of topological phases. KW - electronics, photonics and device physics KW - topological insulators Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-236422 VL - 1 ER - TY - JOUR A1 - Kügel, Jens A1 - Karolak, Michael A1 - Krönlein, Andreas A1 - Serrate, David A1 - Bode, Matthias A1 - Sangiovanni, Giorgio T1 - Reversible magnetic switching of high-spin molecules on a giant Rashba surface JF - npj Quantum Materials N2 - The quantum mechanical screening of a spin via conduction electrons depends sensitively on the environment seen by the magnetic impurity. A high degree of responsiveness can be obtained with metal complexes, as the embedding of a metal ion into an organic molecule prevents intercalation or alloying and allows for a good control by an appropriate choice of the ligands. There are therefore hopes to reach an “on demand” control of the spin state of single molecules adsorbed on substrates. Hitherto one route was to rely on “switchable” molecules with intrinsic bistabilities triggered by external stimuli, such as temperature or light, or on the controlled dosing of chemicals to form reversible bonds. However, these methods constrain the functionality to switchable molecules or depend on access to atoms or molecules. Here, we present a way to induce bistability also in a planar molecule by making use of the environment. We found that the particular “habitat” offered by an antiphase boundary of the Rashba system BiAg2 stabilizes a second structure for manganese phthalocyanine molecules, in which the central Mn ion moves out of the molecular plane. This corresponds to the formation of a large magnetic moment and a concomitant change of the ground state with respect to the conventional adsorption site. The reversible spin switch found here shows how we can not only rearrange electronic levels or lift orbital degeneracies via the substrate, but even sway the effects of many-body interactions in single molecules by acting on their surrounding. KW - electronic structure of atoms and molecules KW - magnetic properties and materials KW - surfaces, interfaces and thin films Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-230866 VL - 3 ER - TY - JOUR A1 - Liu, Yuhai A1 - Wang, Zhenjiu A1 - Sato, Toshihiro A1 - Hohenadler, Martin A1 - Wang, Chong A1 - Guo, Wenan A1 - Assaad, Fakher F. T1 - Superconductivity from the condensation of topological defects in a quantum spin-Hall insulator JF - Nature Communications N2 - The discovery of quantum spin-Hall (QSH) insulators has brought topology to the forefront of condensed matter physics. While a QSH state from spin-orbit coupling can be fully understood in terms of band theory, fascinating many-body effects are expected if it instead results from spontaneous symmetry breaking. Here, we introduce a model of interacting Dirac fermions where a QSH state is dynamically generated. Our tuning parameter further allows us to destabilize the QSH state in favour of a superconducting state through proliferation of charge-2e topological defects. This route to superconductivity put forward by Grover and Senthil is an instance of a deconfined quantum critical point (DQCP). Our model offers the possibility to study DQCPs without a second length scale associated with the reduced symmetry between field theory and lattice realization and, by construction, is amenable to large-scale fermion quantum Monte Carlo simulations. KW - computational science KW - phase transitions and critical phenomena KW - topological insulators Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-237024 VL - 10 ER - TY - JOUR A1 - Soltamov, V. A. A1 - Kasper, C. A1 - Poshakinskiy, A. V. A1 - Anisimov, A. N. A1 - Mokhov, E. N. A1 - Sperlich, A. A1 - Tarasenko, S. A. A1 - Baranov, P. G. A1 - Astakhov, G. V. A1 - Dyakonov, V. T1 - Excitation and coherent control of spin qudit modes in silicon carbide at room temperature JF - Nature Communications N2 - One of the challenges in the field of quantum sensing and information processing is to selectively address and coherently manipulate highly homogeneous qubits subject to external perturbations. Here, we present room-temperature coherent control of high-dimensional quantum bits, the so-called qudits, associated with vacancy-related spins in silicon carbide enriched with nuclear spin-free isotopes. In addition to the excitation of a spectrally narrow qudit mode at the pump frequency, several other modes are excited in the electron spin resonance spectra whose relative positions depend on the external magnetic field. We develop a theory of multipole spin dynamics and demonstrate selective quantum control of homogeneous spin packets with sub-MHz spectral resolution. Furthermore, we perform two-frequency Ramsey interferometry to demonstrate absolute dc magnetometry, which is immune to thermal noise and strain inhomogeneity. KW - quantum information KW - qubits Y1 - 2019 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-239149 VL - 10 ER - TY - JOUR A1 - Tan, Z. B. A1 - Elo, T. A1 - Puska, A. A1 - Sarkar, J. A1 - Lähteenmäki, P. A1 - Duerr, F. A1 - Gould, C. A1 - Molenkamp, L. W. A1 - Nagaev, K. E. A1 - Hakonen, P. J. T1 - Hanbury-Brown and Twiss exchange and non-equilibrium-induced correlations in disordered, four-terminal graphene-ribbon conductor JF - Scientific Reports N2 - We have investigated current-current correlations in a cross-shaped conductor made of graphene. The mean free path of charge carriers is on the order of the ribbon width which leads to a hybrid conductor where there is diffusive transport in the device arms while the central connection region displays near ballistic transport. Our data on auto and cross correlations deviate from the predictions of Landauer-Büttiker theory, and agreement can be obtained only by taking into account contributions from non-thermal electron distributions at the inlets to the semiballistic center, in which the partition noise becomes strongly modified. The experimental results display distinct Hanbury – Brown and Twiss (HBT) exchange correlations, the strength of which is boosted by the non-equilibrium occupation-number fluctuations internal to this hybrid conductor. Our work demonstrates that variation in electron coherence along atomically-thin, two-dimensional conductors has significant implications on their noise and cross correlation properties. KW - conductive hybrid KW - partition noise KW - occupation number fluctuations KW - current-current correlation KW - device arm Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-240348 VL - 8 ER - TY - JOUR A1 - Waldherr, Max A1 - Lundt, Nils A1 - Klaas, Martin A1 - Betzold, Simon A1 - Wurdack, Matthias A1 - Baumann, Vasilij A1 - Estrecho, Eliezer A1 - Nalitov, Anton A1 - Cherotchenko, Evgenia A1 - Cai, Hui A1 - Ostrovskaya, Elena A. A1 - Kavokin, Alexey V. A1 - Tongay, Sefaattin A1 - Klembt, Sebastian A1 - Höfling, Sven A1 - Schneider, Christian T1 - Observation of bosonic condensation in a hybrid monolayer MoSe2-GaAs microcavity JF - Nature Communications N2 - Bosonic condensation belongs to the most intriguing phenomena in physics, and was mostly reserved for experiments with ultra-cold quantum gases. More recently, it became accessible in exciton-based solid-state systems at elevated temperatures. Here, we demonstrate bosonic condensation driven by excitons hosted in an atomically thin layer of MoSe2, strongly coupled to light in a solid-state resonator. The structure is operated in the regime of collective strong coupling between a Tamm-plasmon resonance, GaAs quantum well excitons, and two-dimensional excitons confined in the monolayer crystal. Polariton condensation in a monolayer crystal manifests by a superlinear increase of emission intensity from the hybrid polariton mode, its density-dependent blueshift, and a dramatic collapse of the emission linewidth, a hallmark of temporal coherence. Importantly, we observe a significant spin-polarization in the injected polariton condensate, a fingerprint for spin-valley locking in monolayer excitons. Our results pave the way towards highly nonlinear, coherent valleytronic devices and light sources. KW - polaritons KW - two-dimensional materials Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-233280 VL - 9 ER - TY - THES A1 - Franken, Robert T1 - Precision Predictions for \(\mathrm W^+ \mathrm W^-\) Scattering at the LHC T1 - Präzisionsvorhersagen für \(\mathrm W^+ \mathrm W^-\) -Streuung am LHC N2 - In this thesis we examine the vector boson scattering (VBS) process \(\mathrm p \mathrm p \to \mathrm e^+ \nu_\mathrm e\mu^-\bar\nu_\mu\mathrm j\mathrm j +X\) (short: \(\mathrm W^+\mathrm W^-\) scattering) at NLO accuracy in two experimental setups by performing a Monte Carlo analysis of a \(13\,\mathrm{TeV}\) LHC run. \(\mathrm W^+\mathrm W^-\) scattering shows similarities and differences compared to the scattering of other vector bosons. We present a detailed description of the types of appearing subprocesses and background processes. We give insight into our code which solves the problems we are faced within \(\mathrm W^+\mathrm W^-\) scattering. This is especially the presence of the Higgs-boson resonance in the fiducial phase-space region. Particular attention is dedicated to the permutation of resonances. The integrated signal cross section at LO \(\mathcal O(\alpha^6)\) amounts to \(2.6988(3)\,\mathrm{fb}\) and \(1.5322(2)\,\mathrm{fb}\), respectively, in the two experimental setups. The LO QCD-induced background of \(\mathcal O(\alpha_\mathrm s^2\alpha^4)\) amounts to \(6.9115(9)\,\mathrm{fb}\) and \(1.6923(3)\,\mathrm{fb}\). The EW corrections to the signal are \(-11.4\%\) and \(-6.7\%\), the QCD corrections amount to \(-5.2\%\) and \(-23.0\%\). The EW corrections to the background are \(-8.3\%\) and \(-5.3\%\), the QCD corrections amount to \(-30.3\%\) and \(-77.6\%\). Our results for the QCD corrections and the QCD-induced background include a large uncertainty from varying the renormalisation and factorisation scale, and we discuss improvements for future calculations. We show the differential cross sections with unique features of \(\mathrm W^+\mathrm W^-\) scattering compared to other VBS processes and investigate in particular the subprocess of Higgs-boson production by using a modified version of our setups. N2 - In dieser Arbeit untersuchen wir den Vektorboson-Streuprozess (VBS-Prozess) \(\mathrm p\mathrm p \to \mathrm e^+\nu_\mathrm e\mu^-\bar\nu_\mu\mathrm j\mathrm j + X\) (kurz: \(\mathrm W^+\mathrm W^-\)-Streuung) auf nächstführender Ordnung in zwei Versuchsanordnungen, indem wir eine Monte-Carlo-Analyse des LHC-Betriebs bei \(13\,\mathrm{TeV}\) durchführen. \(\mathrm W^+\mathrm W^-\)-Streuung zeigt Gemeinsamkeiten mit der und Unterschiede zur Streuung anderer Vektorbosonen. Wir stellen eine detaillierte Beschreibung der Arten auftauchender Subprozesse und Hintergrundprozesse vor und geben Einsicht in unseren Code, der die Probleme löst, vor die wir im Rahmen der \(\mathrm W^+\mathrm W^-\)-Streuung gestellt wurden. Dies ist insbesondere die Präsenz der Higgs-Boson-Resonanz im Bezugsphasenraum. Besonderes Augenmerk wird auf die Permutation der Resonanzen gelegt. Wir präsentieren den integrierten Wirkungsquerschnitt. Der integrierte Wirkungsquerschnitt des Signals beträgt \(2{,}6988(3)\,\mathrm{fb}\) beziehungsweise \(1{,}5322(2)\,\mathrm{fb}\) auf führender Ordnung \(\mathcal O(\alpha^6)\) in den beiden experimentellen Setups. Der QCD-Hintergrund auf führender Ordnung \(\mathcal O(\alpha_\mathrm s^2\alpha^4)\) beträgt \(6{,}9115(9)\,\mathrm{fb}\) bzw. \(1{,}6923(3)\,\mathrm{fb}\). Die elektroschwachen Korrekturen zum Signal belaufen sich auf \(-11{,}4\%\) bzw. \(-6{,}7\%\), die QCD-Korrekturen auf \(-5{,}2\%\) bzw. \(-23{,}0\%\). Die elektroschwachen Korrekturen zum Hintergrund sind \(-8{,}3\%\) bzw. \(-5{,}3\%\), die QCD-Korrekturen \(-30{,}3\%\) bzw. \(-77{,}6\%\). Unsere Ergebnisse für die QCD-Korrekturen und den QCD-induzierten Hintergrund enthalten eine große Unsicherheit durch die Variation der Renormierungs- und Faktorisierungsskala und wir diskutieren Verbesserungen für zukünftige Rechnungen. Wir zeigen die differentiellen Wirkungsquerschnitte mit Eigenheiten von \(\mathrm W^+\mathrm W^-\)-Streuung verglichen mit anderen VBS-Prozessen und betrachten insbesondere den Subprozess der Higgs-Boson-Produktion, indem wir eine modifizierte Version unserer Versuchsanordnungen verwenden. KW - W-Boson KW - Streuquerschnitt KW - LHC KW - Präzisionsvorhersage Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-369445 ER - TY - THES A1 - Baumann, Johannes T1 - Induced Superconductivity in HgTe Quantum Point Contacts T1 - Induzierte Supraleitung in Quecksilbertellurid Quantenpunktkontakten N2 - In this thesis, the Josephson effect in mercury telluride based superconducting quantum point contacts (SQPCs) is studied. Implementing such confined structures into topological superconductors has been proposed as a means to detect and braid Majorana fermions. For the successful realization of such experiments though, coherent transport across the constriction is essential. By demonstrating the Josephson effect in a confined topological system, the presented experiments lay the foundation for future quantum devices that can be used for quantum computation. In addition, the experiments also provide valuable insights into the behavior of the Josephson effect in the low-channel limit (N<20). Due to the confinement of the weak link, we can also study the Josephson effect in a topological insulator, where the edge modes interact. In conclusion, this thesis discusses the fabrication of, and low-temperature measurements on mercury telluride quantum point contacts embedded within Josephson junctions. We find that the merging of the currently used fabrication methods for mercury telluride quantum point contacts and Josephson junctions does not yield a good enough device quality to resolve subbands of the quantum point contact as quantization effects in the transport properties. As we attribute this to the long dry etching time that is necessary for a top-contact, the fabrication process was adapted to reduce the defect density at the superconductor-semiconductor interface. Employing a technique that involves side contacting the mercury telluride quantum well and reducing the size of the mercury telluride mesa to sub-micrometer dimensions yields a quantized supercurrent across the junction. The observed supercurrent per mode is in good agreement with theoretical predictions for ballistic, one-dimensional modes that are longer than the Josephson penetration depth. Moreover, we find that oscillatory features superimpose the plateaus of the supercurrent and the conductance. The strength of these oscillatory features are sample-dependent and complicate the identification of plateaus. We suggest that the oscillatory features originate mainly from local defects and the short gate electrode. Additionally, resonances are promoted within the weak link if the transparency of the superconductor-HgTe interface differs from one. Furthermore, the research explores the regimes of the quantum spin Hall effect and the 0.5 anomaly. Notably, a small yet finite supercurrent is detected in the QSH regime. In samples fabricated from thick mercury telluride quantum wells, the supercurrent appears to vanish when the quantum point contact is tuned into the regime of the 0.5 anomaly. For samples fabricated from thin mercury telluride quantum wells, the conductance as well as the supercurrent vanish for strong depopulation. In these samples though, the supercurrent remains detectable even for conductance values significantly below 2 e²/h. Numerical calculation reproduce the transport behavior of the superconducting quantum point contacts. Additionally, the topological nature of the weak link is thoroughly investigated using the supercurrent diffraction pattern and the absorption of radio frequency photons. The diffraction pattern reveals a gate independent, monotonous decay of $I_\text{sw}(B)$, which is associated with the quantum interference of Andreev bound states funneled through the quantum point contact. Interestingly, the current distribution in the weak link appears unaffected as the quantum point contact is depleted. In the RF measurements, indications of a 4π periodic supercurrent are observed as a suppression of odd Shapiro steps. The ratio of the 4π periodic current to the 2π periodic current appears to decrease for smaller supercurrents, as odd Shapiro steps are exclusively suppressed for large supercurrents. Additionally, considering the observation that the supercurrent is small when the bulk modes in the quantum point contact are fully depleted, we suggest that the re-emerging of odd Shapiro steps is a consequence of the group velocity of the edge modes being significantly suppressed when the bulk modes are absent. Consequently, the topological nature of the superconducting quantum point contact is only noticeable in the transport properties when bulk modes are transmitted through the superconducting quantum point contact. The shown experiments are the first demonstration of mercury telluride superconducting quantum point contacts that exhibit signatures of quantization effects in the conductance as well as the supercurrent. Moreover, the experiments suggest that the regime of interacting topological edge channels is also accessible in mercury telluride superconducting quantum point contacts. This is potentially relevant for the realization of Majorana fermions and their application in the field of quantum computation. N2 - Gegenstand dieser Arbeit ist der Josephson-Effekt in supraleitenden Quantenpunktkontakten (SQPCs) aus Quecksilbertellurid. Grundsätzlich wurde postuliert, dass räumlich eingeschränkte topologische Supraleitung in Quantenpunktkontakten verwendet werden kann, um Majorana-Fermionen zu realisieren und zu manipulieren. Dafür ist allerdings kohärente Supraleitung durch die Verjüngung des Quantenpunktkontaktes unerlässlich. Dies wird durch die Beobachtung des Josephson-Effektes durch den Quecksilbertellurid-Quantenpunktkontakt demonstriert. Somit legen die präsentierten Experimente den Grundstein für zukünftige Quanten-Bauelemente mit Anwendung im Bereich des Quantencomputings. Darüber hinaus liefern die Experimente auch einen Einblick in das Verhalten eines Josephson-Kontaktes, wenn dessen Verbindungsstück nur eine kleinen Anzahl an Transportmoden befördern kann (N<20). Durch die räumliche Nähe der Randkanäle des zwei-dimensionalen topologischen Isolators in der Verjüngung wird außerdem untersucht, wie sich der Josephson-Effekt unter Interaktion der helikalen Randkanäle verhält. Grundsätzlich behandelt diese Arbeit die Herstellung und Vermessung von supraleitenden Quecksilbertellurid-Quantenpunktkontakten, welche in einen Josephson-Kontakt eingebettet sind. Zunächst wird gezeigt, dass bei dem Versuch einen supraleitenden Quecksilbertellurid-Quantenpunktkontakt durch Anwenden der bekannten Fabrikationsprozesse von Quecksilbertellurid-Quantenpunktkontakten und Josephson-Kontakten herzustellen, die Qualität der Probe nicht gut genug ist, um quantisierten Transport durch einzelne Subbänder des Quantenpunktkontaktes aufzuweisen. Dies wird auf das lange Trockenätzen zurückgeführt, welche für einen Kontakt von oben notwendig ist. Daher wurde der Strukturierungsprozess angepasst, um die Defektdichte an dem Supraleiter-Halbleiter-Kontakt zu verringern. Durch das seitliche Kontaktieren des Quecksilbertellurid-Quantentroges und die Verkleinerung der Mesa auf submikrometer Größe, wird ein quantisierter Suprastrom durch den Josepshon-Kontakt beobachtet. Hierbei stimmt der von den Transportmoden getragene Suptrastrom gut mit den theoretischen Vorhersagen für ballistische, eindimensionale Moden überein, wenn deren Modenlänge größer als die Josephson-Eindringtiefe ist. Darüber hinaus wird beobachtet, dass die Stufen im Suprastrom und im Leitwert von Oszillationen überlagert werden. Die Stärke der Oszillationen ist hierbei probenabhängig, was die Identifikation einzelner Stufen erschwert. Die Oszillationen sind auf lokale Defekte und die kurze Gateelektrode zurückzuführen. Zusätzlich entstehen Resonanzen im Verbindungsstück des Josephson-Kontaktes, wenn die Transparenz der Supraleiter-HgTe-Kontaktes von eins abweicht. Des Weiteren werden die Bereiche des Quanten-Spin-Hall-Effektes und der 0.5-Anomalie untersucht. Bemerkenswerterweise wird im Quanten-Spin-Hall-Regime ein kleiner, aber endlicher Suprastrom detektiert. In Proben aus dicken Quecksilbertellurid-Quantentrögen verschwindet der Suprastrom, wenn der Quantenpunktkontakt in das Regime der 0.5-Anomalie gebracht wird. Bei dünnen Quecksilbertellurid-Quantentrögen verschwinden sowohl Leitwert als auch Suprastrom, wenn die Ladungsträgerdichte über das Quanten-Spin-Hall-Regime hinaus verringert wird. In diesen Proben bleibt allerdings der Suprastrom selbst für Leitwerte, die deutlich unter G=2 e²/h liegen, eindeutig erhalten. Das Transportverhalten der supraleitenden Quantenpunktkontakte wird durch numerische Simulationen reproduziert. Letztendlich werden die topologischen Eigenschaften des Verbindungsstückes auch durch das Beugungsbild des Suprastromes und durch die Absorption von RF-Photonen untersucht. Das Beugungsbild des Suprastromes zeigt einen monotonen Abfall von ebendiesem bei ansteigendem Magnetfeld, welcher unabhängig von der angelegten Gatespannung ist. Dieses Verhalten basiert auf Interferenzeffekten von gebundenen Andreev-Zuständen, welche die Verjüngung passieren. Interessanterweise scheint die Stromverteilung in dem Verbindungsstück unverändert zu bleiben, wenn der Quantenpunktkontakt entleert wird. In den RF-Messungen wird mit der Unterdrückung von ungeraden Shapiro-Stufen ein Anzeichen für einen 4\π-periodischen Suprastroms beobachtet. Das Verhältnis des 4π-periodischen Anteils des Suprastroms zum 2π-periodischen Anteil des Suprastroms wird kleiner, wenn der gesamte Suprastrom verringert wird. Demnach sind ungerade Shapiro-Stufen nur für große Supraströme unterdrückt. Wenn man darüber hinaus berücksichtigt, dass der Suprastrom klein ist, wenn die Volumenzustände im Quantenpunktkontakt entleert sind, liegt es nahe, dass das Wiederauftreten der ungeraden Shapiro-Stufen eine Konsequenz daraus ist, dass die Gruppengeschwindigkeit der helikalen Randkanäle unter Abwesenheit von Volumenzuständen deutlich verringert ist. Demzufolge sind die topologischen Eigenschaften des Verbindungsstückes nur bemerkbar, wenn auch Volumenzustände die Verjüngung passieren. Die gezeigten Experimente sind der erste Nachweis von supraleitenden Quantenpunktkontakten im zwei-dimensionalen topologischen Isolator Quecksilbertellurid, welche Kennzeichen von Quantisierungseffekte sowohl im Leitwert als auch im Suprastrom aufzeigen. Darüber hinaus implizieren die Experimente, dass der Bereich von interagierenden topologischen Randkanälen auch in supraleitenden Quecksilbertellurid-Quantenpunktkontakten zugänglich ist. Dies hat potenziell Relevanz für die Realisierung von Majorana-Fermionen in vergleichbaren Systemen und deren Anwendung im Bereich des Quantencomputing. KW - Topologischer Isolator KW - Supraleitung KW - Quecksilbertellurid KW - Niederdimensionaler Halbleiter KW - Topologische Supraleitung KW - Topological superconductivity KW - HgTe Y1 - 2024 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-369405 ER - TY - JOUR T1 - Search for new phenomena in events with same-charge leptons and b-jets in pp collisions at √\(s\) = 13 TeV with the ATLAS detector JF - Journal of High Energy Physics N2 - A search for new phenomena in events with two same- charge leptons or three leptons and jets identi fi ed as originating from b - quarks in a data sample of 36.1 fb of pp collisions at ps = 13TeV recorded by the ATLAS detector at the Large Hadron Collider is reported. No signi fi cant excess is found and limits are set on vector- like quark, fourtop- quark, and same- sign top- quark pair production. The observed ( expected) 95% CL mass limits for a vector- like T - and B - quark singlet are mT > 0 : 98 ( 0 : 99) TeV and mB > 1 : 00 ( 1 : 01) TeV respectively. Limits on the production of the vector- like T5=3 - quark are also derived considering both pair and single production; in the former case the lower limit on the mass of the T5=3 - quark is ( expected to be) 1.19 ( 1.21) TeV. The Standard Model fourtop- quark production cross- section upper limit is ( expected to be) 69 ( 29) fb. Constraints are also set on exotic four- top- quark production models. Finally, limits are set on samesign top- quark pair production. The upper limit on uu ! tt production is ( expected to be) 89 ( 59) fb for a mediator mass of 1TeV, and a dark- matter interpretation is also derived, excluding a mediator of 3TeV with a dark- sector coupling of 1.0 and a coupling to ordinary matter above 0.31. KW - Hadron-Hadron scattering (experiments) KW - SUSHI Y1 - 2018 U6 - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-312681 VL - 12 IS - 39 ER -