@phdthesis{Franke2019,
  author    = {Franke, Christian},
  title     = {Advancing Single-Molecule Localization Microscopy: Quantitative Analyses and Photometric Three-Dimensional Imaging},
  doi       = {10.25972/OPUS-15635},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-156355},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2019},
  abstract  = {Since its first experimental implementation in 2005, single-molecule localization microscopy (SMLM) emerged as a versatile and powerful imaging tool for biological structures with nanometer resolution. By now, SMLM has compiled an extensive track-record of novel insights in sub- and inter- cellular organization.\\ Moreover, since all SMLM techniques rely on the analysis of emission patterns from isolated fluorophores, they inherently allocate molecular information \$per\$ \$definitionem\$.\\ Consequently, SMLM transitioned from its origin as pure high-resolution imaging instrument towards quantitative microscopy, where the key information medium is no longer the highly resolved image itself, but the raw localization data set.\\ The work presented in this thesis is part of the ongoing effort to translate those \$per\$ \$se\$ molecular information gained by SMLM imaging to insights into the structural organization of the targeted protein or even beyond. Although largely consistent in their objectives, the general distinction between global or segmentation clustering approaches on one side and particle averaging or meta-analyses techniques on the other is usually made.\\ During the course of my thesis, I designed, implemented and employed numerous quantitative approaches with varying degrees of complexity and fields of application.\\ \\ In my first major project, I analyzed the localization distribution of the integral protein gp210 of the nuclear pore complex (NPC) with an iterative \textit{k}-means algorithm. Relating the distinct localization statistics of separated gp210 domains to isolated fluorescent signals led, among others, to the conclusion that the anchoring ring of the NPC consists of 8 homo-dimers of gp210.\\ This is of particular significance, both because it answered a decades long standing question about the nature of the gp210 ring and it showcased the possibility to gain structural information well beyond the resolution capabilities of SMLM by crafty quantification approaches.\\ \\ The second major project reported comprises an extensive study of the synaptonemal complex (SNC) and linked cohesin complexes. Here, I employed a multi-level meta-analysis of the localization sets of various SNC proteins to facilitate the compilation of a novel model of the molecular organization of the major SNC components with so far unmatched extend and detail with isotropic three-dimensional resolution.\\ In a second venture, the two murine cohesin components SMC3 and STAG3 connected to the SNC were analyzed. Applying an adapted algorithm, considering the disperse nature of cohesins, led to the realization that there is an apparent polarization of those cohesin complexes in the SNC, as well as a possible sub-structure of STAG3 beyond the resolution capabilities of SMLM.\\ \\ Other minor projects connected to localization quantification included the study of plasma membrane glycans regarding their overall localization distribution and particular homogeneity as well as the investigation of two flotillin proteins in the membrane of bacteria, forming clusters of distinct shapes and sizes.\\ \\ Finally, a novel approach to three-dimensional SMLM is presented, employing the precise quantification of single molecule emitter intensities. This method, named TRABI, relies on the principles of aperture photometry which were improved for SMLM.\\ With TRABI it was shown, that widely used Gaussian fitting based localization software underestimates photon counts significantly. This mismatch was utilized as a \$z\$-dependent parameter, enabling the conversion of 2D SMLM data to a virtual 3D space. Furthermore it was demonstrated, that TRABI can be combined beneficially with a multi-plane detection scheme, resulting in superior performance regarding axial localization precision and resolution.\\ Additionally, TRABI has been subsequently employed to photometrically characterize a novel dye for SMLM, revealing superior photo-physical properties at the single-molecule level.\\ Following the conclusion of this thesis, the TRABI method and its applications remains subject of diverse ongoing research.},
  subject      = {Einzelmolek{\"u}lmikroskopie},
  language  = {en}
}
@phdthesis{Brendel2017,
  author    = {Brendel, Michael},
  title     = {Correlation between Interface Energetics of Molecular Semiconductors and Opto-Electronic Properties of Planar Organic Solar Cells},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-155094},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {It was the scope of this work to gain a deeper understanding of the correlation between Interface energetics of molecular semiconductors in planar organic solar cells and the corresponding optoelectronic characteristics. For this aim, different approaches were followed. At first, a direct variation of donor/acceptor (D/A) interface energetics of bilayer cells was achieved by utilizing systematically modified donor compounds. This change could be correlated to the macroscopic device performance. At second, the impact of interface energetics was illustrated, employing a more extended device architecture. By introducing a thin interlayer between a planar D/A heterojunction, an energetic staircase was established. Exciton dissociation in such devices could be linked to the cascade energy level alignment of the photo-active materials. Finally, two different fullerene molecules C60 and C70 were employed in co-evaporated acceptor phases. The expected discrepancy in their electronic structure was related to the transport properties of the corresponding organic photovoltaic cells (OPVCs). The fullerenes are created simultaneously in common synthesis procedures. Next to the photo-physical relevance, the study was carried-out to judge on the necessity of separating the components from each other by purification which constitutes the cost-determining step in the total production costs.},
  subject      = {Organische Solarzelle},
  language  = {en}
}
@article{BechtleCamargoMolinaDeschetal.2016,
  author    = {Bechtle, Philip and Camargo-Molina, Jos{\´e} Eliel and Desch, Klaus and Dreiner, Herbert K. and Hamer, Matthias and Kr{\"a}mer, Michael and O'Leary, Ben and Porod, Werner and Sarrazin, Bj{\"o}rn and Stefaniak, Tim and Uhlenbrock, Mathias and Wienemann, Peter},
  title     = {Killing the cMSSM softly},
  series = {The European Physical Journal C},
  volume    = {76},
  journal   = {The European Physical Journal C},
  number    = {96},
  doi       = {10.1140/epjc/s10052-015-3864-0},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-165045},
  year      = {2016},
  abstract  = {We investigate the constrained Minimal Supersymmetric Standard Model (cMSSM) in the light of constraining experimental and observational data from precision measurements, astrophysics, direct supersymmetry searches at the LHC and measurements of the properties of the Higgs boson, by means of a global fit using the program Fittino. As in previous studies, we find rather poor agreement of the best fit point with the global data. We also investigate the stability of the electro-weak vacuum in the preferred region of parameter space around the best fit point. We find that the vacuum is metastable, with a lifetime significantly longer than the age of the Universe. For the first time in a global fit of supersymmetry, we employ a consistent methodology to evaluate the goodness-of-fit of the cMSSM in a frequentist approach by deriving p values from large sets of toy experiments. We analyse analytically and quantitatively the impact of the choice of the observable set on the p value, and in particular its dilution when confronting the model with a large number of barely constraining measurements. Finally, for the preferred sets of observables, we obtain p values for the cMSSM below 10 \%, i.e. we exclude the cMSSM as a model at the 90 \% confidence level.},
  language  = {en}
}
@phdthesis{Unsleber2016,
  author    = {Unsleber, Sebastian Philipp},
  title     = {Festk{\"o}rperbasierte Einzelphotonenquellen als Grundbausteine der Quanteninformationstechnologie},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-147322},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2016},
  abstract  = {Die vorliegende Arbeit hatte das Ziel basierend auf Halbleiternanostrukturen eine effiziente und skalierbare Quelle einzelner und ununterscheidbarer Photonen zu entwickeln. Dies ist eine Basiskomponente von zuk{\"u}nftigen quantenphysikalischen Anwendungen wie der Quantenkommunikation oder dem Quantencomputer. Diese Konzepte nutzen gezielt quantenmechanische Systeme um einerseits Kommunikation absolut abh{\"o}rsicher zu machen oder um neuartige Computer zu konstruieren, die bestimmte Aufgaben - wie die Produktzerlegung großer Zahlen - effizienter l{\"o}sen als heutige Systeme. Ein m{\"o}gliche Realisierung der Quantenkommunikation ist beispielsweise die Schl{\"u}sselverteilung zwischen zwei Parteien durch Verwendung des BB84-Protokolls. Dazu wird eine Lichtquelle ben{\"o}tigt, welche die physikalisch kleinstm{\"o}gliche Lichtmenge - ein einzelnes Photon - aussendet. Der Kommunikationskanal wird dann {\"u}ber verschiedene Polarisationszust{\"a}nde dieser Photonen gegen ein Abh{\"o}ren nach außen hin abgesichert. Da die maximale Kommunikationsdistanz aufgrund von Verlusten im Quantenkanal beschr{\"a}nkt ist, muss das Signal f{\"u}r gr{\"o}ßere Distanzen mit Hilfe eines sog. Quantenrepeaters aufbereitet werden. Ein solcher kann ebenfalls unter Verwendung von Einzelphotonenquellen realisiert werden. Das Konzept des Quantenverst{\"a}rkers stellt aber die zus{\"a}tzliche Anforderung an die Einzelphotonenquelle, dass die ausgesendeten Lichtteilchen in der Summe ihrer Eigenschaften wie Energie und Polarisation immer gleich und somit ununterscheidbar sein m{\"u}ssen. Auf Basis solcher ununterscheidbarer Photonen gibt es zudem mit dem linear optischen Quantenrechner auch m{\"o}gliche theoretische Ans{\"a}tze zur Realisierung eines Quantencomputers. Dabei kann {\"u}ber die Quanteninterferenz von ununterscheidbaren Photonen an optischen Bauteilen wie Strahlteilern ein Quanten-NOT-Gatter zur Berechnung spezieller Algorithmen realisiert werden. Als vielversprechende Kandidaten f{\"u}r eine solche Lichtquelle einzelner Photonen haben sich in den letzten Jahren Halbleiter-Quantenpunkte herauskristallisiert. Dank des festk{\"o}rperbasierten Ansatzes k{\"o}nnen diese Strukturen in komplexe photonische Umgebungen zur Erh{\"o}hung der Photonen-Extraktionseffizienz und -Emissionsrate eingebettet werden. Ziel dieser Arbeit war somit eine effiziente Quelle einzelner ununterscheidbarer Photonen zu realisieren. Im Hinblick auf die sp{\"a}tere Anwendbarkeit wurde der Fokus zudem auf die skalierbare bzw. deterministische Fabrikation der Quantenpunkt-Strukturen gelegt und zwei technologische Ans{\"a}tze - die kryogene in-situ-Lithographie und das positionierte Wachstum von Quantenpunkten - untersucht. Im ersten experimentellen Kapitel dieser Arbeit wird ein neuartiges Materialsystem vorgestellt, welches sich zur Generation einzelner Photonen eignet. Es k{\"o}nnen spektral scharfe Emissionslinien mit Linienbreiten bis knapp {\"u}ber 50 µeV aus Al\$_{0,48}\$In\$_{0,52}\$As Volumenmaterial beobachtet werden, wenn diese Schicht auf InP(111) Substraten abgeschieden wird. In Querschnitt-Rastertunnelmikroskopie-Messungen wurden ca. 16 nm große Cluster, welche eine um ungef{\"a}hr 7 \% h{\"o}here Indiumkonzentration im Vergleich zur nominellen Zusammensetzung des Volumenmaterials besitzen, gefunden. {\"U}ber die Simulation dieser Strukturen konnten diese als Quelle der spektral scharfen Emissionslinien identifiziert werden. Zudem wurde mittels Auto- und Kreuzkorrelationsmessungen nachgewiesen, dass diese Nanocluster einzelne Photonen emittieren und verschieden geladene exzitonische und biexzitonische Ladungstr{\"a}gerkomplexe binden k{\"o}nnen. Anschließend wurde der Fokus auf InGaAs-Quantenpunkte gelegt und zun{\"a}chst im Rahmen einer experimentellen und theoretischen Gemeinschaftsarbeit die Koh{\"a}renzeigenschaften eines gekoppelten Quantenpunkt-Mikrokavit{\"a}t-Systems untersucht. {\"U}ber temperaturabh{\"a}ngige Zwei-Photonen Interferenz Messungen und dem Vergleich mit einem mikroskopischen Modell des Systems konnten gezielt die Bestandteile der Quantenpunkt-Dephasierung extrahiert werden. Auf diesen Ergebnissen aufbauend wurde die gepulste, strikt resonante Anregung von Quantenpunkten als experimentelle Schl{\"u}sseltechnik etabliert. Damit konnten bei tiefen Temperaturen nahezu vollst{\"a}ndig ununterscheidbare Photonen durch eine Zwei-Photonen Interferenz Visibilit{\"a}t von {\"u}ber 98 \% nachgewiesen werden. F{\"u}r ein skalierbares und deterministisches Quantenpunkt-Bauelement ist entweder die Kontrolle {\"u}ber die Position an welcher der Quantenpunkt gewachsen wird n{\"o}tig, oder die Position an der eine Mikrokavit{\"a}t ge{\"a}tzt wird muss auf die Position eines selbstorganisiert gewachsenen Quantenpunktes abgestimmt werden. Im weiteren Verlauf werden Untersuchungen an beiden technologischen Ans{\"a}tzen durchgef{\"u}hrt. Zun{\"a}chst wurde der Fokus auf positionierte Quantenpunkte gelegt. Mittels in das Substrat ge{\"a}tzter Nanol{\"o}cher wird der Ort der Quantenpunkt-Nukleation festgelegt. Durch die ge{\"a}tzten Grenzfl{\"a}chen in Quantenpunkt-N{\"a}he entstehen jedoch auch Defektzust{\"a}nde, die negativen Einfluss auf die Koh{\"a}renz der Quantenpunkt-Emission nehmen. Deshalb wurde an diesem Typus von Quantenpunkten die strikt resonante Anregung etabliert und zum ersten Mal die koh{\"a}rente Kopplung des Exzitons an ein resonantes Lichtfeld demonstriert. Zudem konnte die deterministische Kontrolle der Exzitonbesetzung {\"u}ber den Nachweis einer Rabi-Oszillation gezeigt werden. Abschließend wird das Konzept der kryogenen in-situ-Lithographie vorgestellt. Diese erlaubt die laterale Ausrichtung der Mikrokavit{\"a}t an die Position eines selbstorganisiert gewachsenen Quantenpunktes. Damit konnte gezielt die Emission eines zuvor ausgew{\"a}hlten, spektral schmalen Quantenpunktes mit nahezu 75 \% Gesamteffizienz eingesammelt werden. Die Ununterscheidbarkeit der Quantenpunkt-Photonen war dabei mit einer Zwei-Photonen Interferenz Visibilit{\"a}t von bis zu \$\nu=(88\pm3)~\\%\$ sehr hoch. Damit wurde im Rahmen dieser Arbeit eine Einzelphotonenquelle realisiert, aus der sich sehr effizient koh{\"a}rente Photonen auskoppeln lassen, was einen wichtigen Schritt hin zur deterministischen Fabrikation von Lichtquellen f{\"u}r quantenphysikalischen Anwendungen darstellt.},
  subject      = {Quantenpunkt},
  language  = {de}
}
@phdthesis{Seibel2016,
  author    = {Seibel, Christoph},
  title     = {Elektronische Struktur von Halbleiteroberfl{\"a}chen mit starker Spin-Bahn-Wechselwirkung: Topologie, Spinpolarisation und Robustheit},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-140418},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2016},
  abstract  = {Neue Erkenntnisse {\"u}ber elektronische Eigenschaften von Festk{\"o}rpern legen den Grundstein f{\"u}r innovative Anwendungen der Zukunft. Von zentraler Bedeutung sind insbesondere die Eigenschaften der Elektronenspins. Um diese besser zu verstehen, befasst sich die vorliegende Arbeit mit der experimentellen Analyse der elektronischen Struktur von topologischen Isolatoren (Sb\$_2\$Te\$_3\$ , Bi\$_2\$Se\$_x\$Te\$_{3-x}\$, Bi\$_{1.5}\$Sb\$_{0.5}\$Te\$_{1.8}\$Se\$_{1.2} und Bi\$_{1.4}\$Sb\$_{1.1}\$Te\$_{2.2}\$S\$_{0.3}\$) und Kristallen mit starker Spin-Bahn-Wechselwirkung (BiTeI) mittels Photoelektronenspektroskopie. Zu Beginn werden die zum Verst{\"a}ndnis dieser Arbeit ben{\"o}tigten Grundlagen erkl{\"a}rt sowie die unterschiedlichen zum Einsatz kommenden Techniken eingef{\"u}hrt. Der Hauptteil der Arbeit teilt sich in drei Forschungsschwerpunkte. Der erste Teil befasst sich mit den elektronischen Eigenschaften der Valenzbandstruktur von Sb2Te3 und den auftretenden Oberfl{\"a}chenzust{\"a}nden. Durch gezielte Variation der Energie der anregenden Strahlung wird der Charakter der Wellenfunktion des topologischen Oberfl{\"a}chenzustands und dessen Wechselwirkung mit Valenzzust{\"a}nden erforscht. Dabei spielt die Topologie der Volumenbandstruktur eine grundlegende Rolle. Der zus{\"a}tzliche Vergleich zu Photoemissionsrechnungen erm{\"o}glicht detaillierte Einblicke in die Wechselwirkung zwischen Oberfl{\"a}chen- und Volumenzust{\"a}nden und gibt Aufschluss dar{\"u}ber, wie diese vermittelt werden. Im zweiten Abschnitt wird durch die Analyse des gemessenen Photoelektronenspins das Zusammenspiel der Spintextur des Grundzustands und Endzust{\"a}nden in Bi2Te3 untersucht. Dabei treten, im Gegensatz zu Grundzustandsrechnungen, Radialkomponenten des Polarisationsvektors in nichtsymmetrischer Messgeometrie auf. Sowohl deren Energieabh{\"a}ngigkeit als auch deren Auftreten in Photoemissionsrechnungen (1-Schritt-Modell) deutet darauf hin, dass diese ihren Ursprung in {\"U}bergangsmatrixelementen des Photoemissionsprozesses haben. Dieses Ergebnis wird mit Spinpolarisationsmessungen am Oberfl{\"a}chenzustand des nicht-topologischen Schichtsystems BiTeI verglichen. Im dritten Teil werden Auswirkungen unterschiedlicher Manipulationen der untersuchten Materialien auf deren elektronische Eigenschaften beschrieben. Die Adsorption von Bruchteilen einer monoatomaren Lage des Alkalimetalls Caesium auf die Oberfl{\"a}che des topologischen Isolators Sb2Te3 wird systematisch untersucht. Dadurch kann dessen intrinsische p-Dotierung teilweise abgebaut werden, wobei die Valenzbandstruktur trotz der Reaktivit{\"a}t des Adsorbats intakt bleibt. Des Weiteren werden Auswirkungen von {\"A}nderungen der Kristallst{\"o}chiometrie durch Volumendotierung vergleichend diskutiert. Ausblickend befasst sich das Kapitel mit dem Verhalten geringer Mengen ferromagnetischer Materialen (Fe, Ni) auf den Oberfl{\"a}chen der topologischen Isolatoren. F{\"u}r die verschiedenen Adsorbate werden Trends aufgezeigt, die von Temperatur und Zusammensetzung des Substratkristalls abh{\"a}ngen.},
  subject      = {Elektronenstruktur},
  language  = {de}
}
@article{KasprzakSivalertpornAlbertetal.2013,
  author    = {Kasprzak, J. and Sivalertporn, K. and Albert, F. and Schneider, C. and H{\"o}fling, S. and Kamp, M. and Forchel, A. and Muljarov, E. A. and Langbein, W.},
  title     = {Coherence dynamics and quantum-to-classical crossover in an exciton-cavity system in the quantum strong coupling regime},
  series = {New Journal of Physics},
  volume    = {15},
  journal   = {New Journal of Physics},
  number    = {045013},
  issn      = {1367-2630},
  doi       = {10.1088/1367-2630/15/4/045013},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-123005},
  year      = {2013},
  abstract  = {Interaction between light and matter generates optical nonlinearities, which are particularly pronounced in the quantum strong coupling regime. When a single bosonic mode couples to a single fermionic mode, a Jaynes-Cummings (JC) ladder is formed, which we realize here using cavity photons and quantum dot excitons. We measure and model the coherent anharmonic response of this strongly coupled exciton-cavity system at resonance. Injecting two photons into the cavity, we demonstrate a \(\sqrt 2\) larger polariton splitting with respect to the vacuum Rabi splitting. This is achieved using coherent nonlinear spectroscopy, specifically four-wave mixing, where the coherence between the ground state and the first (second) rung of the JC ladder can be interrogated for positive (negative) delays. With increasing excitation intensity and thus rising average number of injected photons, we observe spectral signatures of the quantum-to-classical crossover of the strong coupling regime.},
  language  = {en}
}
@article{HopfmannAlbertSchneideretal.2013,
  author    = {Hopfmann, C. and Albert, F. and Schneider, C. and H{\"o}fling, S. and Kamp, M. and Forchel, A. and Kanter, I. and Reizenstein, S.},
  title     = {Nonlinear emission characteristics of quantum dot-micropillar lasers in the presence of polarized optical feedback},
  series = {New Journal of Physics},
  volume    = {15},
  journal   = {New Journal of Physics},
  number    = {025030},
  issn      = {1367-2630},
  doi       = {10.1088/1367-2630/15/2/025030},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-123127},
  year      = {2013},
  abstract  = {We report on electrically pumped quantum dot-microlasers in the presence of polarized self-feedback. The high-\(\beta\) microlasers show two orthogonal, linearly polarized emission modes which are coupled via the common gain medium. This coupling is explained in terms of gain competition between the two lasing modes and leads to distinct differences in their input-output characteristics. By applying polarized self-feedback via an external mirror, we are able to control the laser characteristics of the emission modes in terms of the output power, the coherence time and the photon statistics. We find that linearly polarized self-feedback stabilizes the lasing of a given mode, while cross-polarized feedback between the two modes reduces strongly the intensity of the other emission mode showing particular high-intensity fluctuations and even super-thermal values of the photon autocorrelation function \(g^{(2)} (\tau)\) at zero delay. Measurements of \(g^{(2)} (\tau)\) under external feedback also allow us to detect revival peaks associated with the round trip time of the external cavity. Analyzing the damping and shape of the \(g^{(2)} (\tau)\) revival peaks by a phenomenological model provides us insight into the underlying physics such as the effective exciton lifetime and gain characteristics of the quantum dots in the active region of these microlasers.},
  language  = {en}
}
@article{VottelerCarvajalBerrioPudlasetal.2012,
  author    = {Votteler, Miriam and Carvajal Berrio, Daniel A. and Pudlas, Marieke and Walles, Heike and Schenke-Layland, Katja},
  title     = {Non-contact, Label-free Monitoring of Cells and Extracellular Matrix using Raman Spectroscopy},
  series = {Journal of Visual Expression},
  volume    = {63},
  journal   = {Journal of Visual Expression},
  number    = {e3977},
  doi       = {10.3791/3977},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-124569},
  year      = {2012},
  abstract  = {Non-destructive, non-contact and label-free technologies to monitor cell and tissue cultures are needed in the field of biomedical research.1-5 However, currently available routine methods require processing steps and alter sample integrity. Raman spectroscopy is a fast method that enables the measurement of biological samples without the need for further processing steps. This laser-based technology detects the inelastic scattering of monochromatic light.6 As every chemical vibration is assigned to a specific Raman band (wavenumber in cm-1), each biological sample features a typical spectral pattern due to their inherent biochemical composition.7-9 Within Raman spectra, the peak intensities correlate with the amount of the present molecular bonds.1 Similarities and differences of the spectral data sets can be detected by employing a multivariate analysis (e.g. principal component analysis (PCA)).10 Here, we perform Raman spectroscopy of living cells and native tissues. Cells are either seeded on glass bottom dishes or kept in suspension under normal cell culture conditions (37 °C, 5\% CO2) before measurement. Native tissues are dissected and stored in phosphate buffered saline (PBS) at 4 °C prior measurements. Depending on our experimental set up, we then either focused on the cell nucleus or extracellular matrix (ECM) proteins such as elastin and collagen. For all studies, a minimum of 30 cells or 30 random points of interest within the ECM are measured. Data processing steps included background subtraction and normalization.},
  language  = {en}
}
@phdthesis{Zipf2021,
  author    = {Zipf, Matthias},
  title     = {Ber{\"u}hrungslose Temperaturmessung an Gasen und keramisch beschichteten Oberfl{\"a}chen bei hohen Temperaturen},
  doi       = {10.25972/OPUS-24024},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-240248},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2021},
  abstract  = {Station{\"a}re Gasturbinen k{\"o}nnen von großer Bedeutung f{\"u}r die Verlangsamung des Klima-wandels und bei der Bew{\"a}ltigung der Energiewende sein. F{\"u}r die Weiterentwicklung von Gasturbinen zu h{\"o}heren Betriebstemperaturen und damit einhergehend zu h{\"o}heren Wirkungs-graden werden ber{\"u}hrungslose Messverfahren zur Ermittlung der Oberfl{\"a}chentemperatur von Turbinenschaufeln und der Gastemperatur der heißen Verbrennungsgase w{\"a}hrend des Be-triebs ben{\"o}tigt. Im Rahmen dieser Arbeit werden daher Methoden der ber{\"u}hrungslosen Tem-peraturmessung unter Verwendung von Infrarotstrahlung untersucht. Die ber{\"u}hrungslose Messung der Oberfl{\"a}chentemperatur moderner Turbinenschaufeln muss aufgrund derer infrarot-optischer Oberfl{\"a}cheneigenschaften im Wellenl{\"a}ngenbereich des mitt-leren Infrarots durchgef{\"u}hrt werden, in welchem die Turbinenbrenngase starke Absorptions-banden aufweisen. Zur Entwicklung eines ad{\"a}quaten Strahlungsthermometers f{\"u}r diesen Zweck wurden im Rahmen dieser Arbeit daher durch Ermittlung von Transmissionsspektren von Kohlenstoffdioxid und Wasserdampf bei hohen Temperaturen und Dr{\"u}cken in einer ei-gens hierf{\"u}r konstruierten Heißgas-Messzelle zun{\"a}chst Wellenl{\"a}ngenbereiche identifiziert, in welchen die geplanten Messungen m{\"o}glich sind. Anschließend wurde der Prototyp eines ent-sprechend konfigurierten Strahlungsthermometers im Zuge des Testlaufes einer vollskaligen Gasturbine erfolgreich erprobt. Weiterhin wurden im Rahmen dieser Arbeit zwei m{\"o}gliche Verfahren zur ber{\"u}hrungslosen Gastemperaturmessung untersucht. Das erste untersuchte Verfahren setzt ebenfalls auf Strah-lungsthermometrie. Dieses Verfahren sieht vor, aufgrund der Temperaturabh{\"a}ngigkeit des spektralen Transmissionsgrades in den Randbereichen von ges{\"a}ttigten Absorptionsbanden von Gasen aus der in diesen Bereichen transmittierten spektralen Strahldichte auf die Gastempera-tur zu schließen. Im Rahmen dieser Arbeit wurden Voruntersuchungen f{\"u}r dieses Tempera-turmessverfahren durchgef{\"u}hrt. So konnten auf der Grundlage von experimentell ermittelten Transmissionsspektren von Kohlenstoffdioxid bei Dr{\"u}cken zwischen 5 kPa und 600 kPa und Gastemperaturen zwischen Raumtemperatur und 1073 K f{\"u}r das geplante Verfahren nutzbare Wellenl{\"a}ngenintervalle insbesondere im Bereich der Kohlenstoffdioxid-Bande bei 4,26 µm identifiziert werden. Das zweite im Rahmen dieser Arbeit untersuchte Verfahren zur ber{\"u}hrungslosen Gastem-peraturmessung basiert auf der Temperaturabh{\"a}ngigkeit der Wellenl{\"a}ngenposition der Trans-missionsminima der Absorptionsbanden von infrarot-aktiven Gasen. Im Hinblick darauf wur-de dieses Ph{\"a}nomen anhand von experimentell bestimmten hochaufgel{\"o}sten Transmissions-spektren von Kohlenstoffdioxid {\"u}berpr{\"u}ft. Weiterhin wurden m{\"o}gliche Wellenl{\"a}ngenbereiche identifiziert und hinsichtlich ihrer Eignung f{\"u}r das geplante Verfahren charakterisiert. Als am vielversprechendsten erwiesen sich hierbei Teilbanden in den Bereichen um 2,7 µm und um 9,2 µm. Unter Beimischung von Stickstoff mit Partialdr{\"u}cken von bis zu 390 kPa erwies sich zudem auch die Bande bei 4,26 µm als geeignet. Die im Rahmen dieser Arbeit experimentell ermittelten Transmissionsspektren konnten dar-{\"u}ber hinaus schließlich durch Vergleich mit entsprechenden HITRAN-Simulationen verifiziert werden.},
  subject      = {Pyrometrie},
  language  = {de}
}
@article{MotykaSękRyczkoetal.2015,
  author    = {Motyka, Marcin and Sęk, Grzegorz and Ryczko, Krzysztof and Dyksik, Mateusz and Weih, Robert and Patriarche, Gilles and Misiewicz, Jan and Kamp, Martin and H{\"o}fling, Sven},
  title     = {Interface Intermixing in Type II InAs/GaInAsSb Quantum Wells Designed for Active Regions of Mid-Infrared-Emitting Interband Cascade Lasers},
  series = {Nanoscale Research Letters},
  volume    = {10},
  journal   = {Nanoscale Research Letters},
  number    = {471},
  doi       = {10.1186/s11671-015-1183-x},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-136386},
  year      = {2015},
  abstract  = {The effect of interface intermixing in W-design GaSb/AlSb/InAs/Ga\(_{0.665}\)In\(_{0.335}\)As\(_x\)Sb\(_{1-x}\)/InAs/AlSb/GaSb quantum wells (QWs) has been investigated by means of optical spectroscopy supported by structural data and by band structure calculations. The fundamental optical transition has been detected at room temperature through photoluminescence and photoreflectance measurements and appeared to be blueshifted with increasing As content of the GaInAsSb layer, in contrast to the energy-gap-driven shifts calculated for an ideally rectangular QW profile. The arsenic incorporation into the hole-confining layer affects the material and optical structure also altering the InAs/GaInAsSb interfaces and their degree of intermixing. Based on the analysis of cross-sectional transmission electron microscopy images and energy-dispersive X-ray spectroscopy, we could deduce the composition distribution across the QW layers and hence simulate more realistic confinement potential profiles. For such smoothed interfaces that indicate As-enhanced intermixing, the energy level calculations have been able to reproduce the experimentally obtained trend.},
  language  = {en}
}
@article{DyksikMotykaSęketal.2015,
  author    = {Dyksik, Mateusz and Motyka, Marcin and Sęk, Grzegorz and Misiewicz, Jan and Dallner, Matthias and Weih, Robert and Kamp, Martin and H{\"o}fling, Sven},
  title     = {Submonolayer Uniformity of Type II InAs/GaInSb W-shaped Quantum Wells Probed by Full-Wafer Photoluminescence Mapping in the Mid-infrared Spectral Range},
  series = {Nanoscale Research Letters},
  volume    = {10},
  journal   = {Nanoscale Research Letters},
  number    = {402},
  doi       = {10.1186/s11671-015-1104-z},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-139733},
  year      = {2015},
  abstract  = {The spatial uniformity of GaSb- and InAs substrate-based structures containing type II quantum wells was probed by means of large-scale photoluminescence (PL) mapping realized utilizing a Fourier transform infrared spectrometer. The active region was designed and grown in a form of a W-shaped structure with InAs and GaInSb layers for confinement of electrons and holes, respectively. The PL spectra were recorded over the entire 2-in. wafers, and the parameters extracted from each spectrum, such as PL peak energy position, its linewidth and integrated intensity, were collected in a form of two-dimensional spatial maps. Throughout the analysis of these maps, the wafers' homogeneity and precision of the growth procedure were investigated. A very small variation of PL peak energy over the wafer indicates InAs quantum well width fluctuation of only a fraction of a monolayer and hence extraordinary thickness accuracy, a conclusion further supported by high uniformity of both the emission intensity and PL linewidth.},
  language  = {en}
}
@phdthesis{Renziehausen2014,
  author    = {Renziehausen, Klaus},
  title     = {Wechselwirkung von Molek{\"u}len mit Laserpulsen: Untersuchungen zur numerischen Implementierung zeitabh{\"a}ngiger St{\"o}rungstheorie und zu Effekten der absoluten Phase von Laserpulsen beliebiger L{\"a}nge},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-100850},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2014},
  abstract  = {In dieser Dissertation wurden zwei Aspekte der Wechselwirkung von Laserpulsen mit Molek{\"u}len betrachtet: Erstens wurden numerische Algorithmen, die auf der zeitabh{\"a}ngigen St{\"o}rungstheorie basieren, zur Berechnung von quantenmechanischen Wellenfunktionen analysiert. Zweitens wurden Effekte der absoluten Phase (Carrier envelope phase = CEP) von Laserpulsen bei der Laseranregung molekularer Systeme analysiert. In den Analysen zum ersten Aspekt wurden zwei verschiedene Algorithmen - in dieser Arbeit als simple und improved algorithm bezeichnet - verwendet, und die Normabweichung von mit diesen Algorithmen berechneten Wellenfunktionen untersucht. Es konnte gezeigt werden, dass diese Normabweichung f{\"u}r beide Algorithmen in zwei unterschiedliche Beitr{\"a}ge zerlegt werden kann. Der erste Normabweichungsbeitrag tritt aufgrund der numerischen Diskretisierung der Zeit auf und verschwindet, wenn der Zeitschritt, der die Dauer der Intervalle f{\"u}r diese Diskretisierung angibt, gegen Null geht. Man kann den ersten Normabweichungsbeitrag mit exzellenter Genauigkeit berechnen und seine Eigenschaften, die sich f{\"u}r die beiden Algorithmen erheblich unterschieden, eingehend analysieren. Der zweite Normabweichungsbeitrag tritt dadurch auf, dass die zeitabh{\"a}ngige St{\"o}rungstheorie nicht normerhaltend ist, und geht daher gegen Null, wenn die St{\"o}rungsordnung gegen unendlich geht. Dieser zweite Beitrag ist außerdem in guter N{\"a}herung unabh{\"a}ngig vom Zeitschritt und f{\"u}r beide Algorithmen n{\"a}herungsweise gleich. Des Weiteren kann man das Verhalten des zweiten Normabweichungsbeitrags im Gegensatz zum ersten Beitrag nur qualitativ beschreiben. F{\"u}r die Analyse zum zweiten Themengebiet dieser Arbeit, den CEP-Effekten, wurde betrachtet, ob CEP-Effekte auch f{\"u}r Laserpulse beliebiger L{\"a}nge auftreten k{\"o}nnen. {\"U}ber eine analytische Betrachtung erkennt man, dass dies f{\"u}r ein Zweiniveausystem nur dann der Fall ist, wenn beide Zust{\"a}nde vor Beginn der Wechselwirkung des Systems mit dem Laserpuls besetzt sind. Man kann aus diesem Ergebnis folgern, dass f{\"u}r einen Laserpuls, der zwei elektronische Zust{\"a}nde eines Molek{\"u}ls {\"u}ber Einphotonen{\"u}berg{\"a}nge koppelt, in der Regel kein CEP-Effekt f{\"u}r beliebige L{\"a}ngen dieses Pulses auftritt. Der Grund daf{\"u}r ist, dass vor der Wechselwirkung eines molekularen Systems mit einem Laserpuls f{\"u}r dieses {\"u}blicherweise nur der elektronische Grundzustand besetzt ist. In dieser Arbeit wird gezeigt, dass dieses Problem durch ein spezielles Zweipulsschema f{\"u}r die Anregung eines molekularen Systems gel{\"o}st werden kann. F{\"u}r dieses Pulsschema wird ein erster Puls verwendet, der zeitlich so kurz ist, dass Wellenpakete in mehreren elektronischen Zust{\"a}nden angeregt werden. Der nachfolgende zweite Laserpuls ist spektral schmal, und seine zeitliche L{\"a}nge kann beliebig groß gew{\"a}hlt werden. Man erh{\"a}lt f{\"u}r dieses Pulsschema Observablen, die von der CEP des zweiten Pulses, aber nicht von der CEP des ersten Pulses abh{\"a}ngen; somit ist ein CEP-Effekt nachweisbar. Derartige Observablen sind geometrische Asymmetrien f{\"u}r Zerfallsprodukte von Photodissoziationsreaktionen. Insbesondere unterscheidet sich das hier vorgestellte Pulsschema von anderen Zweipulsschemata, f{\"u}r welche Observablen von der Differenz der CEPs beider Pulse abh{\"a}ngen, aber nicht von der CEP einer der beiden Pulse allein.},
  subject      = {St{\"o}rungstheorie},
  language  = {de}
}
@phdthesis{Wolter2014,
  author    = {Wolter, Steve},
  title     = {Single-molecule localization algorithms in super-resolution microscopy},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-109370},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2014},
  abstract  = {Lokalisationsmikroskopie ist eine Methodenklasse der superaufl{\"o}senden Fluoreszenzmikroskopie, deren Methoden sich durch stochastische zeitliche Isolation der Fluoreszenzemission auszeichnen. Das Blinkverhalten von Fluorophoren wird so ver{\"a}ndert, dass gleichzeitige Aktivierung von einander nahen Fluorophoren unwahrscheinlich ist. Bekannte okalisationsmikroskopische Methoden umfassen dSTORM, STORM, PALM, FPALM, oder GSDIM. Lokalisationsmikroskopie ist von hohem biologischem Interesse, weil sie die Aufl{\"o}sung des Fluoreszenzmikroskops bei minimalem technischem Aufwand um eine Gr{\"o}ßenordnung verbessert. Der verbundene Rechenaufwand ist allerdings erheblich, da Millionen von Fluoreszenzemissionen einzeln mit Nanometergenauigkeit lokalisiert werden m{\"u}ssen. Der Rechen- und Implementationsaufwand dieser Auswertung hat die Verbreitung der superaufl{\"o}senden Mikroskopie lange verz{\"o}gert. Diese Arbeit beschreibt meine algorithmische Grundstruktur f{\"u}r die Auswertung lokalisationsmikroskopischer Daten. Die Echtzeitf{\"a}higkeit, d.h. eine Auswertegeschwindigkeit oberhalb der Datenaufnahmegeschwindigkeit an normalen Messaufbauten, meines neuartigen und quelloffenen Programms wird demonstriert. Die Geschwindigkeit wird auf verbrauchermarktg{\"a}ngigen Prozessoren erreicht und dadurch spezialisierte Rechenzentren oder der Einsatz von Grafikkarten vermieden. Die Berechnung wird mit dem allgemein anerkannten Gaussschen Punktantwortmodell und einem Rauschmodell auf Basis der gr{\"o}ßten Poissonschen Wahrscheinlichkeit durchgef{\"u}hrt. Die algorithmische Grundstruktur wird erweitert, um robuste und optimale Zweifarbenauswertung zu realisieren und damit korrelative Mikroskopie zwischen verschiedenen Proteinen und Strukturen zu erm{\"o}glichen. Durch den Einsatz von kubischen Basissplines wird die Auswertung von dreidimensionalen Proben vereinfacht und stabilisiert, um pr{\"a}zisem Abbilden von mikrometerdicken Proben n{\"a}her zu kommen. Das Grenzverhalten von Lokalisationsalgorithmen bei hohen Emissionsdichten wird untersucht. Abschließend werden Algorithmen f{\"u}r die Anwendung der Lokalisationsmikroskopie auf verbreitete Probleme der Biologie aufgezeigt. Zellul{\"a}re Bewegung und Motilit{\"a}t werden anhand der in vitro Bewegung von Myosin-Aktin-Filamenten studiert. Lebendzellbildgebung mit hellen und stabilen organischen Fluorophoren wird mittels SNAP-tag-Fusionsproteinen realisiert. Die Analyse des Aufbaus von Proteinklumpen zeigt, wie Lokalisationsmikroskopie neue quantitative Ans{\"a}tze jenseits reiner Bildgebung bietet.},
  subject      = {Fluoreszenzmikroskopie},
  language  = {en}
}
@phdthesis{Niehoerster2022,
  author    = {Nieh{\"o}rster, Thomas},
  title     = {Spektral aufgel{\"o}ste Fluoreszenzlebensdauer-Mikroskopie mit vielen Farben},
  doi       = {10.25972/OPUS-29657},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-296573},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2022},
  abstract  = {Die Fluoreszenzmikroskopie ist eine vielseitig einsetzbare Untersuchungsmethode f{\"u}r biologische Proben, bei der Biomolek{\"u}le selektiv mit Fluoreszenzfarbstoffen markiert werden, um sie dann mit sehr gutem Kontrast abzubilden. Dies ist auch mit mehreren verschiedenartigen Zielmolek{\"u}len gleichzeitig m{\"o}glich, wobei {\"u}blicherweise verschiedene Farbstoffe eingesetzt werden, die {\"u}ber ihre Spektren unterschieden werden k{\"o}nnen. Um die Anzahl gleichzeitig verwendbarer F{\"a}rbungen zu maximieren, wird in dieser Arbeit zus{\"a}tzlich zur spektralen Information auch das zeitliche Abklingverhalten der Fluoreszenzfarbstoffe mittels spektral aufgel{\"o}ster Fluoreszenzlebensdauer-Mikroskopie (spectrally resolved fluorescence lifetime imaging microscopy, sFLIM) vermessen. Dazu wird die Probe in einem Konfokalmikroskop von drei abwechselnd gepulsten Lasern mit Wellenl{\"a}ngen von 485 nm, 532nm und 640nm angeregt. Die Detektion des Fluoreszenzlichtes erfolgt mit einer hohen spektralen Aufl{\"o}sung von 32 Kan{\"a}len und gleichzeitig mit sehr hoher zeitlicher Aufl{\"o}sung von einigen Picosekunden. Damit wird zu jedem detektierten Fluoreszenzphoton der Anregungslaser, der spektrale Kanal und die Ankunftszeit registriert. Diese detaillierte multidimensionale Information wird von einem Pattern-Matching-Algorithmus ausgewertet, der das Fluoreszenzsignal mit zuvor erstellten Referenzpattern der einzelnen Farbstoffe vergleicht. Der Algorithmus bestimmt so f{\"u}r jedes Pixel die Beitr{\"a}ge der einzelnen Farbstoffe. Mit dieser Technik konnten pro Anregungslaser f{\"u}nf verschiedene F{\"a}rbungen gleichzeitig dargestellt werden, also theoretisch insgesamt 15 F{\"a}rbungen. In der Praxis konnten mit allen drei Lasern zusammen insgesamt neun F{\"a}rbungen abgebildet werden, wobei die Anzahl der Farben vor allem durch die anspruchsvolle Probenvorbereitung limitiert war. In anderen Versuchen konnte die sehr hohe Sensitivit{\"a}t des sFLIM-Systems genutzt werden, um verschiedene Zielmolek{\"u}le voneinander zu unterscheiden, obwohl sie alle mit demselben Farbstoff markiert waren. Dies war m{\"o}glich, weil sich die Fluoreszenzeigenschaften eines Farbstoffmolek{\"u}ls geringf{\"u}gig in Abh{\"a}ngigkeit von seiner Umgebung {\"a}ndern. Weiterhin konnte die sFLIM-Technik mit der hochaufl{\"o}senden STED-Mikroskopie (STED: stimulated emission depletion) kombiniert werden, um so hochaufgel{\"o}ste zweifarbige Bilder zu erzeugen, wobei nur ein einziger gemeinsamer STED-Laser ben{\"o}tigt wurde. Die gleichzeitige Erfassung von mehreren photophysikalischen Messgr{\"o}ßen sowie deren Auswertung durch den Pattern-Matching-Algorithmus erm{\"o}glichten somit die Entwicklung von neuen Methoden der Fluoreszenzmikroskopie f{\"u}r Mehrfachf{\"a}rbungen.},
  subject      = {Fluoreszenzmikroskopie},
  language  = {de}
}
@phdthesis{Mueller2023,
  author    = {M{\"u}ller, Dominik Dennis},
  title     = {Laborbasierte Nano-Computertomographie mit hoher Energie f{\"u}r die Materialcharakterisierung und Halbleiterpr{\"u}fung in Simulation und Anwendung},
  doi       = {10.25972/OPUS-31338},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-313380},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2023},
  abstract  = {Verschiedene Konzepte der R{\"o}ntgenmikroskopie haben sich mittlerweile im Labor etabliert und erm{\"o}glichen heute aufschlussreiche Einblicke in eine Vielzahl von Probensystemen. Der „Labormaßstab" bezieht sich dabei auf Analysemethoden, die in Form von einem eigenst{\"a}ndigen Ger{\"a}t betrieben werden k{\"o}nnen. Insbesondere sind sie unabh{\"a}ngig von der Strahlerzeugung an einer Synchrotron-Großforschungseinrichtung und einem sonst kilometergroßen Elektronen-speicherring. Viele der technischen Innovationen im Labor sind dabei ein Transfer der am Synchrotron entwickelten Techniken. Andere wiederum basieren auf der konsequenten Weiterentwicklung etablierter Konzepte. Die Aufl{\"o}sung allein ist dabei nicht entscheidend f{\"u}r die spezifische Eignung eines Mikroskopiesystems im Ganzen. Ebenfalls sollte das zur Abbildung eingesetzte Energiespektrum auf das Probensystem abgestimmt sein. Zudem muss eine Tomographieanalage zus{\"a}tzlich in der Lage sein, die Abbildungsleistung bei 3D-Aufnahmen zu konservieren. Nach einem {\"U}berblick {\"u}ber verschiedene Techniken der R{\"o}ntgenmikroskopie konzentriert sich die vorliegende Arbeit auf quellbasierte Nano-CT in Projektionsvergr{\"o}ßerung als vielversprechende Technologie zur Materialanalyse. Hier k{\"o}nnen h{\"o}here Photonenenergien als bei konkurrierenden Ans{\"a}tzen genutzt werden, wie sie von st{\"a}rker absorbierenden Proben, z. B. mit einem hohen Anteil von Metallen, zur Untersuchung ben{\"o}tigt werden. Das bei einem ansonsten idealen CT-Ger{\"a}t aufl{\"o}sungs- und leistungsbegrenzende Bauteil ist die verwendete R{\"o}ntgen-quelle. Durch konstruktive Innovationen sind hier die gr{\"o}ßten Leistungsspr{\"u}nge zu erwarten. In diesem Zuge wird er{\"o}rtert, ob die Brillanz ein geeignetes Maß ist, um die Leistungsf{\"a}higkeit von R{\"o}ntgenquellen zu evaluieren, welchen Schwierigkeiten die praktische Messung unterliegt und wie das die Vergleichbarkeit der Werte beeinflusst. Anhand von Monte-Carlo-Simulationen wird gezeigt, wie die Brillanz verschiedener Konstruktionen an R{\"o}ntgenquellen theoretisch bestimmt und miteinander verglichen werden kann. Dies wird am Beispiel von drei modernen Konzepten von R{\"o}ntgenquellen demonstriert, welche zur Mikroskopie eingesetzt werden k{\"o}nnen. Im Weiteren besch{\"a}ftigt sich diese Arbeit mit den Grenzen der Leistungsf{\"a}higkeit von Transmissionsr{\"o}ntgenquellen. Anhand der verzahnten Simulation einer Nanofokus-R{\"o}ntgenquelle auf Basis von Monte-Carlo und FEM-Methoden wird untersucht, ob etablierte Literatur¬modelle auf die modernen Quell-konstruktionen noch anwendbar sind. Aus den Simulationen wird dann ein neuer Weg abgeleitet, wie die Leistungsgrenzen f{\"u}r Nanofokus-R{\"o}ntgenquellen bestimmt werden k{\"o}nnen und welchen Vorteil moderne strukturierte Targets dabei bieten. Schließlich wird die Konstruktion eines neuen Nano-CT-Ger{\"a}tes im Labor-maßstab auf Basis der zuvor theoretisch besprochenen Nanofokus-R{\"o}ntgenquelle und Projektionsvergr{\"o}ßerung gezeigt, sowie auf ihre Leistungsf{\"a}higkeit validiert. Es ist spezifisch darauf konzipiert, hochaufl{\"o}sende Messungen an Materialsystemen in 3D zu erm{\"o}glichen, welche mit bisherigen Methoden limitiert durch mangelnde Aufl{\"o}sung oder Energie nicht umsetzbar waren. Daher wird die praktische Leistung des Ger{\"a}tes an realen Proben und Fragestellungen aus der Material¬wissenschaft und Halbleiterpr{\"u}fung validiert. Speziell die gezeigten Messungen von Fehlern in Mikrochips aus dem Automobilbereich waren in dieser Art zuvor nicht m{\"o}glich.},
  subject      = {Computertomografie},
  language  = {de}
}
@article{HeIffLundtetal.2016,
  author    = {He, Yu-Ming and Iff, Oliver and Lundt, Nils and Baumann, Vasilij and Davanco, Marcelo and Srinivasan, Kartik and H{\"o}fling, Sven and Schneider, Christian},
  title     = {Cascaded emission of single photons from the biexciton in monolayered WSe\(_{2}\)},
  series = {Nature Communications},
  volume    = {7},
  journal   = {Nature Communications},
  doi       = {10.1038/ncomms13409},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-169363},
  year      = {2016},
  abstract  = {Monolayers of transition metal dichalcogenide materials emerged as a new material class to study excitonic effects in solid state, as they benefit from enormous Coulomb correlations between electrons and holes. Especially in WSe\(_{2}\), sharp emission features have been observed at cryogenic temperatures, which act as single photon sources. Tight exciton localization has been assumed to induce an anharmonic excitation spectrum; however, the evidence of the hypothesis, namely the demonstration of a localized biexciton, is elusive. Here we unambiguously demonstrate the existence of a localized biexciton in a monolayer of WSe\(_{2}\), which triggers an emission cascade of single photons. The biexciton is identified by its time-resolved photoluminescence, superlinearity and distinct polarization in micro-photoluminescence experiments. We evidence the cascaded nature of the emission process in a cross-correlation experiment, which yields a strong bunching behaviour. Our work paves the way to a new generation of quantum optics experiments with two-dimensional semiconductors.},
  language  = {en}
}
@phdthesis{Kastner2020,
  author    = {Kastner, Matthias J.},
  title     = {Spectroscopic investigation of molecular adsorption and desorption from individual single-wall carbon nanotubes},
  doi       = {10.25972/OPUS-21175},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-211755},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2020},
  abstract  = {Nanoelectronics is an essential technology for down-scaling beyond the limit of silicon-based electronics. Single-Wall Carbon Nanotubes (SWNT) are semiconducting components that exhibit a large variety of properties that make them usable for sensing, telecommunication, or computational tasks. Due to their high surface to volume ratio, carbon nanotubes are strongly affected by molecular adsorptions, and almost all properties depend on surface adsorption. SWNT with smaller diameters (0.7-0.9nm) show a stronger sensitivity to surface effects. An optimized synthesis route was developed to produce these nanotubes directly. They were produced with a clean surface, high quality, and large lengths of 2 μ m. The results complement previous studies on larger diameters (0.9-1.4nm). They allow performing statistically significant assumptions for a perfect nanotube, which is selected from a subset of nanotubes with good emission intensity, and high mechanical durability. The adsorption of molecules on the surface of carbon nanotubes influences the motion and binding strength of chargeseparated states in this system. To gain insight into the adsorption processes on the surface with a minimum of concurrent overlapping effects, a microscopic setup, and a measurement technique were developed. The system was estimated to exhibit excellent properties like long exciton diffusion lengths (>350nm), and big exciton sizes (8.5(5)nm), which was substantiated by a simulation. We studied the adsorption processes at the surface of Single-Wall Carbon Nanotubes for molecules in the gas phase, solvent molecules, and surfactant molecules. The experiments were all carried out on suspended individualized carbon nanotubes on a silicon wafer substrate. The experiments in the gas-phase showed that the excitonic emission energy and intensity experiences a rapid blue shift during observation. This shift was associated with the spontaneous desorption of large clusters of gaseous molecules caused by laser heat up. The measurement of this desorption was essential for creating a reference to an initially clean surface and allows us to perform a comparison with previous measurements on this topic. Furthermore, the adsorption of hydrogen on the nanotube surface at high temperatures was investigated. It was found that a new emission mode arises slightly red-shifted to the excitonic emission in these systems. The new signal is almost equally strong as the main excitonic peak and was associated with the brightening of dark excitons at sp3-defects through a K-phonon assisted pathway. The finding is useful for the direct synthesis of spintronic devices as these systems are known to act as single-photon emitters. The suspended nanotubes were further studied to estimate the effect of solvent adsorption on the excitonic states during nanotube dispersion for each nanotube individually. A significant quantum yield loss is observable for hexane and acetonitrile, while the emission intensity was found to be the strongest in toluene. The reference to a clean surface allowed us to estimate the exact influence of the dielectric environment of adsorbing solvents on the excitonic emission energy. Solvent adsorption was found to lead to an energy shift that is almost twice as high as suggested in previous studies. The amount of this energy shift, however, was comparably similar for all solvents, which suggests that the influence of the distinct dielectric constant in the outer environment less significantly influences the energy shift than previously thought. An interesting phenomenon was found when using acetonitrile as a solvent, which leads to greatly enhanced emission properties. The emission is more than twice as high as in the same air-suspended nanotubes, which suggests a process that depends on the laser intensity. In this study, it was reasonably explained how an energy down-conversion is possible through the coupling of the excitonic states with solvent vibrations. The strength of this coupling, however, also suggests adsorptions to the inside of the tubular nanotube structure leading to a coupled vibration of linear acetonitrile molecules that are adsorbed to the inner surface. The findings are important for the field of nanofluidics and provide an excellent system for efficient energy down-conversion in the transmission window of biological tissue. Having separated the pure effect of solvent adsorption allowed us to study the undisturbed molecular adsorption of polymers in these systems. The addition of polyfluorene polymer leads to a slow but stepwise intensity increase. The intensity increase is overlapping with a concurrent process that leads to an intensity decrease. Unfortunately, observing the stepwise process has a low spacial resolution of only 100-250nm, which is in the range of the exciton diffusion length in these systems and hinders detailed analysis. The two competing and overlapping processes processes are considered to originate from slow π-stacking and fast side-chain binding. Insights into this process are essential for selecting suitably formed polymers. However, the findings also emphasize the importance of solvent selection during nanotube dispersion since solvent effects were proven to be far more critical on the quantum yield in these systems. These measurements can shed light on the ongoing debate on polymers adsorption during nanotube individualization and allow us to direct the discussion more towards the selection of suitable solvents. This work provides fundamental insights into the adsorption of various molecules on the surface of individually observed suspended Single-Wall Carbon Nanotubes. It allows observing the adsorption of individual molecules below the optical limit in the solid, liquid, and gas phases. Nanotubes are able to act as sensing material for detecting changes in their direct surrounding. These fundamental findings are also crucial for increasing the quantum yield of solvent-dispersed nanotubes. They can provide better light-harvesting systems for microscopy in biological tissue and set the base for a more efficient telecommunication infrastructure with nano-scale spintronics devices and lasing components. The newly discovered solvent alignment in the nanotube surrounding can potentially also be used for supercapacitors that are needed for caching the calculation results in computational devices that use polymer wrapped nanotubes as transistors. Although fundamental, these studies develop a strategy to enlighten this room that is barely only visible at the bottom of the nano-scale.},
  subject      = {Kohlenstoff-Nanor{\"o}hre},
  language  = {en}
}
@phdthesis{Grimm2023,
  author    = {Grimm, Philipp Martin},
  title     = {Locally driven complex plasmonic nanoantenna systems},
  doi       = {10.25972/OPUS-30315},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-303152},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2023},
  abstract  = {Metallic nanostructures possess the ability to support resonances in the visible wavelength regime which are related to localized surface plasmons. These create highly enhanced electric fields in the immediate vicinity of metal surfaces. Nanoparticles with dipolar resonance also radiate efficiently into the far-field and hence serve as antennas for light. Such optical antennas have been explored during the last two decades, however, mainly as standalone units illuminated by external laser beams and more recently as electrically driven point sources, yet merely with basic antenna properties. This work advances the state of the art of locally driven optical antenna systems. As a first instance, the electric driving scheme including inelastic electron tunneling over a nanometer gap is merged with Yagi-Uda theory. The resulting antenna system consists of a suitably wired feed antenna, incorporating a tunnel junction, as well as several nearby parasitic elements whose geometry is optimized using analytical and numerical methods. Experimental evidence of unprecedented directionality of light emission from a nanoantenna is provided. Parallels in the performance between radiofrequency and optical Yagi-Uda arrays are drawn. Secondly, a pair of electrically connected antennas with dissimilar resonances is harnessed as electrodes in an organic light emitting nanodiode prototype. The organic material zinc phthalocyanine, exhibiting asymmetric injection barriers for electrons and holes, in conjunction with the electrode resonances, allows switching and controlling the emitted peak wavelength and directionality as the polarity of the applied voltage is inverted. In a final study, the near-field based transmission-line driving of rod antenna systems is thoroughly explored. Perfect impedance matching, corresponding to zero back-reflection, is achieved when the antenna acts as a generalized coherent perfect absorber at a specific frequency. It thus collects all guided, surface-plasmon mediated input power and transduces it to other nonradiative and radiative dissipation channels. The coherent interplay of losses and interference effects turns out to be of paramount importance for this delicate scenario, which is systematically obtained for various antenna resonances. By means of the here developed semi-analytical toolbox, even more complex nanorod chains, supporting topologically nontrivial localized edge states, are studied. The results presented in this work facilitate the design of complex locally driven antenna systems for optical wireless on-chip communication, subwavelength pixels, and loss-compensated integrated plasmonic nanocircuitry which extends to the realm of topological plasmonics.},
  subject      = {Plasmonik},
  language  = {en}
}
@phdthesis{Heinrich2022,
  author    = {Heinrich, Robert},
  title     = {Multi-species gas detection based on an external-cavity quantum cascade laser spectrometer in the mid-infrared fingerprint region},
  doi       = {10.25972/OPUS-26864},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-268640},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2022},
  abstract  = {Laser spectroscopic gas sensing has been applied for decades for several applications as atmospheric monitoring, industrial combustion gas analysis or fundamental research. The availability of new laser sources in the mid-infrared opens the spectral fingerprint range to the technology where multiple molecules possess their fundamental ro-vibrational absorption features that allow very sensitive detection and accurate discrimination of the species. The increasing maturity of quantum cascade lasers that cover this highly interesting spectral range motivated this research to gain fundamental knowledge about the spectra of hydrocarbon gases in pure composition and in complex mixtures as they occur in the petro-chemical industry. The long-term target of developing accurate and fast hydrocarbon gas analyzers, capable of real-time operation while enabling feedback-loops, would lead to a paradigm change in this industry. This thesis aims to contribute to a higher accuracy and more comprehensive understanding of the sensing of hydrocarbon gas mixtures. This includes the acquisition of yet unavailable high resolution and high accuracy reference spectra of the respective gases, the investigation of their spectral behavior in mixtures due to collisional broadening of their transitions and the verification of the feasibility to quantitatively discriminate the spectra when several overlapping species are simultaneously measured in gas mixtures. To achieve this knowledge a new laboratory environment was planned and built up to allow for the supply of the individual gases and their arbitrary mixing. The main element was the development of a broadly tunable external-cavity quantum cascade laser based spectrometer to record the required spectra. This also included the development of a new measurement method to obtain highly resolved and nearly gap-less spectral coverage as well as a sophisticated signal post-processing that was crucial to achieve the high accuracy of the measurements. The spectroscopic setup was used for a thorough investigation of the spectra of the first seven alkanes as of their mixtures. Measurements were realized that achieved a spectral resolution of 0.001 cm-1 in the range of 6-11 µm while ensuring an accuracy of 0.001 cm-1 of the spectra and attaining a transmission sensitivity of 2.5 x 10-4 for long-time averaging of the acquired spectra. These spectral measurements accomplish a quality that compares to state-of-the art spectral databases and revealed so far undocumented details of several of the investigated gases that have not been measured with this high resolution before at the chosen measurement conditions. The results demonstrate the first laser spectroscopic discrimination of a seven component gas mixture with absolute accuracies below 0.5 vol.\% in the mid-infrared provided that a sufficiently broad spectral range is covered in the measurements. Remaining challenges for obtaining improved spectral models of the gases and limitations of the measurement accuracy and technology are discussed.},
  subject      = {Quantenkaskadenlaser},
  language  = {en}
}
@phdthesis{Ochs2022,
  author    = {Ochs, Maximilian Thomas},
  title     = {Electrically Connected Nano-Optical Systems: From Refined Nanoscale Geometries to Selective Molecular Assembly},
  doi       = {10.25972/OPUS-29114},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-291140},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2022},
  abstract  = {Metallic nano-optical systems allow to confine and guide light at the nanoscale, a fascinating ability which has motivated a wide range of fundamental as well as applied research over the last two decades. While optical antennas provide a link between visible radiation and localized energy, plasmonic waveguides route light in predefined pathways. So far, however, most experimental demonstrations are limited to purely optical excitations, i.e. isolated structures are illuminated by external lasers. Driving such systems electrically and generating light at the nanoscale, would greatly reduce the device footprint and pave the road for integrated optical nanocircuitry. Yet, the light emission mechanism as well as connecting delicate nanostructures to external electrodes pose key challenges and require sophisticated fabrication techniques. This work presents various electrically connected nano-optical systems and outlines a comprehensive production line, thus significantly advancing the state of the art. Importantly, the electrical connection is not just used to generate light, but also offers new strategies for device assembly. In a first example, nanoelectrodes are selectively functionalized with self-assembled monolayers by charging a specific electrode. This allows to tailor the surface properties of nanoscale objects, introducing an additional degree of freedom to the development of metal-organic nanodevices. In addition, the electrical connection enables the bottom-up fabrication of tunnel junctions by feedback-controlled dielectrophoresis. The resulting tunnel barriers are then used to generate light in different nano-optical systems via inelastic electron tunneling. Two structures are discussed in particular: optical Yagi-Uda antennas and plasmonic waveguides. Their refined geometries, accurately fabricated via focused ion beam milling of single-crystalline gold platelets, determine the properties of the emitted light. It is shown experimentally, that Yagi-Uda antennas radiate light in a specific direction with unprecedented directionality, while plasmonic waveguides allow to switch between the excitation of two propagating modes with orthogonal near-field symmetry. The presented devices nicely demonstrate the potential of electrically connected nano-optical systems, and the fabrication scheme including dielectrophoresis as well as site-selective functionalization will inspire more research in the field of nano-optoelectronics. In this context, different future experiments are discussed, ranging from the control of molecular machinery to optical antenna communication.},
  subject      = {Nanooptik},
  language  = {en}
}
@article{SuchomelBrodbeckLiewetal.2017,
  author    = {Suchomel, H. and Brodbeck, S. and Liew, T. C. H. and Amthor, M. and Klaas, M. and Klembt, S. and Kamp, M. and H{\"o}fling, S. and Schneider, C.},
  title     = {Prototype of a bistable polariton field-effect transistor switch},
  series = {Scientific Reports},
  volume    = {7},
  journal   = {Scientific Reports},
  number    = {5114},
  doi       = {10.1038/s41598-017-05277-1},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-158323},
  year      = {2017},
  abstract  = {Microcavity exciton polaritons are promising candidates to build a new generation of highly nonlinear and integrated optoelectronic devices. Such devices range from novel coherent light emitters to reconfigurable potential landscapes for electro-optical polariton-lattice based quantum simulators as well as building blocks of optical logic architectures. Especially for the latter, the strongly interacting nature of the light-matter hybrid particles has been used to facilitate fast and efficient switching of light by light, something which is very hard to achieve with weakly interacting photons. We demonstrate here that polariton transistor switches can be fully integrated in electro-optical schemes by implementing a one-dimensional polariton channel which is operated by an electrical gate rather than by a control laser beam. The operation of the device, which is the polariton equivalent to a field-effect transistor, relies on combining electro-optical potential landscape engineering with local exciton ionization to control the scattering dynamics underneath the gate. We furthermore demonstrate that our device has a region of negative differential resistance and features a completely new way to create bistable behavior.},
  language  = {en}
}
@phdthesis{Genheimer2023,
  author    = {Genheimer, Ulrich},
  title     = {The Photophysics of Small Organic Molecules for Novel Light Emitting Devices},
  doi       = {10.25972/OPUS-32031},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-320313},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2023},
  abstract  = {This PhD thesis addresses the photophysics of selected small organic molecules with the purpose of using them for efficient and even novel light sources. In particular, the studies presented focused on revealing the underlying exciton dynamics and determining the transition rates between different molecular states. It was shown how the specific properties and mechanisms of light emission in fluorescent molecules, molecules with phosphorescence or thermally activated delayed fluorescence (TADF), biradicals, and multichromophores can be utilized to build novel light-emitting devices. The main tool employed here was the analysis of the emitters' photon statistics, i.e. the analysis of the temporal distribution of emitted photons, during electrical or optical excitation. In the introduction of this work, the working principle of an organic light-emitting diode (OLED) was introduced, while Chapter 2 provided the physical background of the relevant properties of organic molecules and their interaction with light. In particular, the occurrence of discrete energy levels in organic semiconductors and the process of spontaneous light emission were discussed. Furthermore, in this chapter a mathematical formalism was elaborated with the goal to find out what kind of information about the studied molecule can be obtained by analyzing its photon statistics. It was deduced that the intensity correlation function g (2)(t) contains information about the first two factorial moments of the photon statistics and that higher order factorial moments do not contain any additional information about the system under study if the system is always in the same state after the emission of a photon. To conclude the introductory part, Chapter 3 introduced the utilized characterization methods including confocal microscopy of single molecules, time correlated single photon counting and temperature dependent photoluminescence measurements. To provide the background necessary for an understanding of for the following result chapters, in Section 4.1 a closer look was taken at the phenomenon of blinking and photobleaching of individual molecules. For a squaraine-based fluorescent emitter rapid switching between a bright and dark state was observed during photoexcitation. Using literature transition rates between the molecular states, a consistent model was developed that is able to explain the distribution of the residence times of the molecule in the bright and dark states. In particular, an exponential and a power-law probability distribution was measured for the time the molecule resides in tis bright and dark state, respectively. This behavior as well as the change in photoluminescence intensity between the two states was conclusively explained by diffusion of residual oxygen within the sample, which had been prepared in a nitrogen-filled glovebox. For subsequent samples of this work, thin strips of atomic aluminum were deposited on the matrices to serve as oxygen getter material. This not only suppressed the efficiency of photobleaching, but also noticeably prolonged the time prior to photobleaching, which made many of the following investigations possible in the first place. For emitters used in displays, emission properties such as narrow-band luminescence and short fluorescence lifetimes are desired. These properties can be influenced not only by the emitter molecule itself, but also by the interaction with the chosen environment. Therefore, before focusing on the photophysics of individual small organic molecules, Section 4.2 highlighted the interaction of a perylene bisimide-based molecular species with its local environment in a disordered polymethyl methacrylate matrix. In a statistical approach, individual photophysical properties were measured for 32 single molecules and correlations in the variation of the properties were analyzed. This revealed how the local polarity of the molecules' environment influences their photophysics. In particular, it was shown how an increase in local polarity leads to a red-shifted emission, narrower emission lines, broader vibronic splitting between different emission lines in combination with a smaller Huang-Rhys parameter, and a longer fluorescence lifetime. In the future, these results may help to embed individual chromophores into larger macromolecules to provide the chromophore with the optimal local environment to exhibit the desired emission properties. The next two sections focused on a novel and promising class of chromophores, namely linear coordinated copper complexes, synthesized in the group of Dr. Andreas Steffen at the Institute of Inorganic Chemistry at the University of W{\"u}rzburg. In copper atoms, the d-orbitals are fully occupied, which prevents undesirable metal-centered d-d⋆ states, which tend to lie low in energy and recombine non-radiatively. Simultaneously, the copper atom provides a flexible coordination geometry, while complexes in their linear form are expected to exhibit the least amount of excited state distortions. Depending on the chosen ligands, these copper complexes can exhibit phosphorescence as well as temperature activated delayed fluorescence. In Section 4.3, a phosphorescent copper complex with a chlorine atom and a 1-(2,6-diisopropylphenyl)-3,3,5,5-tetramethyl-2-pyrrolidine-ylidene- ligand was tested for its suitability as an optically active material in an OLED. For this purpose, an OLED with a polyspirobifluorene-based copolymer matrix and the dopant at a concentration of 20 wt\% was electrically excited. Deconvolution of the emission spectrum in contributions from the matrix and the dopant revealed that 60 \% of the OLEDs emission was due to the copper complex. It was also shown that the shape of the emission spectrum of the copper complex remains unchanged upon incorporation into the OLED, but is red-shifted by about 233 meV. In Section 4.4, a second copper complex exhibiting thermally activated delayed fluorescence was analyzed. This complex comprised a carbazolate as well as a 2-(2,6- diisopropyl)-phenyl-1,1-diphenyl-isoindol-2-ium-3-ide ligand and was examined in the solid state and at the single-molecule level, where single photon emission was recorded up to an intensity of 78'000 counts per second. The evaluation of the second-order autocorrelation function of the emitted light proved an efficient transition between singlet and triplet excited states on the picosecond time scale. In the solid state, the temperature- dependent fluorescence decay of the complex was analyzed after pulsed photoexcitation in the temperature range between 300 K and 5 K. From these measurements, a small singlet-triplet energy gap of only 65 meV and a triplet sublevel splitting of 3.0 meV were derived. The transition rates between molecular states could also be determined. Here, the fast singlet decay time of τS1 = 9.8ns proved the efficient thermally activated delayed fluorescence process, which was demonstrated for the first time for this new class of copper(I) complexes thus. While the use of thermally activated delayed fluorescence is a potential way to harness otherwise long-living dark triplet states, radicals completely avoid dark triplet states. However, this usually comes with the huge drawback of the molecules being chemically unstable. Therefore, two chemically stable biradical species were synthesized in the framework of the DFG research training school GRK 2112 on Molecular biradicals: structure, properties and reactivity, by Yohei Hattori in the group of Prof. Dr. Christoph Lambert and Rodger Rausch in the group of Prof. Dr. Frank W{\"u}rthner at the Institute of Organic Chemistry at the University of W{\"u}rzburg, respectively. In Section 4.5, it was investigated how these molecules can be used in OLEDs. In the first isoindigo based biradical (6,6'-bis(3,5-di-tert-butyl-4-phenoxyl)-1,1'-bis(2- ethylhexyl)-[3,3'-biindolinyl-idene]-2,2'-dione) two tert-butyl moieties kinetically block chemical reactions at the place of the lone electrons and an electron-withdrawing core shifts the electron density into the center of the chromophore. With these properties, it was possible to realize a poly(p-phenylene vinylene) copolymer based OLED doped with the biradical and to observe luminescence during optical as well as electrical excitation. Analyzing shapes of the photo- and electroluminescence spectra at different doping concentrations, F{\"o}rster resonance energy transfer was determined to be the dominant transition mechanism for excitons from the matrix to the biradical dopants. Likewise, OLEDs could be realized with the second diphenylmethylpyridine based birad- ical (4-(5-(bis(2,4,6-trichlorophenyl)methyl)-4,6-dichloropyridin-2-yl)-N-(4-(5-(bis(2,4,6- -trichlorophenyl)methyl)-4,6-dichloropyridin-2-yl)phenyl)-N-(4-methoxyphenyl)aniline) as dopant. In this biradical, chlorinated diphenylmethyl groups protect the two unpaired electrons. Photo- and electroluminescence spectra showed an emission in the near in- frared spectral range between 750 nm and 1000 nm. Also, F{\"o}rster resonance energy trans- fer was the dominant energy transfer mechanism with an transfer efficiency close to 100 \% even at doping concentrations of only 5 wt\%. In addition to demonstrating the working OLEDs based in biradicals, the detection of luminescence of the two biradical species in devices also constitutes an important step toward making use of experimental techniques such as optically detected electron spin resonance, which could provide information about the electronic states of the emitter and their spin manifold during OLED operation. Another class of emitters studied are molecules in which several chromophores are co- valently linked to form a macrocyclic system. The properties of these multichromophores were highlighted in Section 4.6. Here, it was analyzed how the photophysical behavior of the molecules is affected by the covalent linking, which determines the interaction be- tween the chromophores. The first multichromophore, 2,2'-ditetracene, was synthesized by Lena Ross in the group of Prof. Dr. Anke Kr{\"u}ger at the Institute of Organic Chemistry at the University of W{\"u}rzburg and was analyzed in this work both at the single-molecule level and in its aggregated crystalline form. While the single crystals were purified and grown in a vertical sublimation oven, the samples for the single molecule studies were prepared in matrices of amorphous polymethyl methacrylate and crystalline anthracene. Tetracene was analyzed concurrently to evaluate the effects of covalent linking. In samples where the distance between two molecules is sufficiently large, tetracene and 2,2'-ditracene show matching emission profiles with the only difference in the Franck-Condon factors and a de- creased photoluminescence decay time constant from 14 ns for tetracene to 5 ns for 2,2'- ditracene, which can be attributed to the increased density of the vibrational modes in 2,2'-ditracene. Evaluation of the photon statistics of individual 2,2'-ditracene molecules however showed that the system does not behave as two individual chromophores but as a collective state, preserving the spectral properties of the two tetracene chromophores. Complementary calculations performed by Marian Deutsch in the group of Prof. Dr. Bernd Engels at the Institute of Physical and Theoretical Chemistry at the University of W{\"u}rzburg helped to understand the processes in the materials and could show that the electronic and vibronic modes of 2,2'-ditracene are superpositions of the modes occurring in tetracene. In contrast, single-crystalline 2,2'-ditetracene behaves significantly different than tetracene, namely exhibiting a red shift in photoluminescence of 150 meV, caused by an altered crys- talline packing that lowers the S1-state energy level. Temperature-dependent photolu- minescence measurements revealed a rich emission pattern from 2,2'-ditetracene single crystals. The mechanisms behind this were unraveled using photoluminescence lifetime density analysis in different spectral regions of the emission spectrum and at different tem- peratures. An excimer state was identified that is located about 5 meV below the S1-state, separated by a 1 meV barrier, and which can decay to the ground state with a time constant of 9 ns. Also, as the S1-state energy level is lowered below the E(S1) ≥ 2 ×E(T1) threshold, singlet fission is suppressed in 2,2'-ditetracene in contrast to tetracene. Therefore, at low temperatures, photoluminescence is enhanced by a factor of 46, which could make 2,2'- ditetracene a useful material for future applications in devices such as OLEDs or lasers. The second multichromophore species, para-xylylene bridged perylene bisimide macrocycles, were synthesized by Peter Spenst in the group of Prof. Dr. Frank W{\"u}rthner at the Institute of Organic Chemistry at the University of W{\"u}rzburg, by linking three and four perylene bisimides, respectively. To reveal the exciton dynamics in these macrocycles, highly diluted monomers as well as trimers and tetramers were doped into matrices of polymethyl methacrylate to create thin films in which individual macrocycles could be analyzed. The emission spectra of the macrocycles remained identical to those of the monomers, indicating weak coupling between the chromophores. Single photon emission could be verified for monomers as well as macrocycles, as exciton-exciton annihilation processes suppress the simultaneous emission of two photons from one macrocycle. Nevertheless, the proof of the occurrence of a doubly excited state was obtained by excitation power dependent photon statistics measurements. The formalism developed in the theory part of this thesis for calculating the photon statistics of multichromophore systems was used here to find a theoretical model that matches the experimental results. The main features of this model are a doubly excited state, fast singlet-singlet annihilation, and an efficient transition from the doubly excited state to a dark triplet state. The occurrence of triplet-triplet annihilation was demonstrated in a subsequent experiment in which the macrocycles were excited at a laser intensity well above the saturation intensity of the monomer species. In contrast to the monomers, the trimers and tetramers exhibited neither a complete dark state nor saturation of photoluminescence. Both processes, efficient singlet-singlet and triplet-triplet annihilation make perylene bisimide macrocycles exceptionally bright single photon emitters. These advantages were utilized to realize a room temperature electrically driven fluorescent single photon source. For this purpose, OLEDs were fabricated using polyvinylcarbazole and 2-tert-butylphenyl-5-biphenyl-1,3,4-oxadiazol blends as a host material for perylene bisimide trimers. Photon antibunching could be observed in both optically and electrically driven devices, representing the first demonstration of electrically driven single photon sources using fluorescent emitters at room temperature. As expected from the previous optical experiments, the electroluminescence of the molecules was exceptionally bright, emitting about 105 photons per second, which could be seen even by eye under the microscope. Finally, in the last section 4.7 of this thesis, two additional measurement schemes were proposed as an alternative to the measurement of the second-order correlation function g (2)(t) of single molecules, which only provides information about the first two factorial moments of the molecules' photon statistics. In the first scheme, the g (3)(t) function was measured with three photodiodes, which is a consequential extension of the Hanbury Brown and Twiss measurement with two photodiodes. It was demonstrated how measuring the g (3)(t) function is able to identify interfering emitters with non-Poisson statistics in the experiment. The second setup was designed with an electro-optic modulator that repeatedly gen- erates photoexcitation in the form of a step function. The recording of luminescence transients for different excitation intensities yields the same results as the correspond- ing g (2)-functions measured on single emitters, both in their shape and in their depen- dence on excitation power. To demonstrate this concept, the TADF emitter TXO-TPA (2- [4-(diphenylamino)phenyl]-10,10-dioxide-9H-thioxanthen-9-one) was doped at a concen- tration of 10-4 wt\% in a mCP (1,3-Bis(N-carbazolyl)benzene) matrix. This concentration was low enough that TXO-TPA molecules did not interact with each other, but an ensem- ble of molecules was still present in the detection volume. The intramolecular transition rates between singlet and triplet states of TXO-TPA could be derived with an error of at most 5 \%. Other experimental techniques designed to obtain this information require ei- ther lengthy measurements on single molecules, where sample preparation is also often a challenge, or temperature-dependent fluorescence lifetime measurements, which require a cryostat, which in turn places constraints on the sample design used. In future, this ap- proach could establish a powerful method to study external factors influencing molecular transition rates. Overall, this thesis has introduced new molecular materials, revealed their photophys- ical properties, and demonstrated how they can be used to fabricate efficient and even novel light sources.},
  subject      = {Fotophysik},
  language  = {en}
}
@article{LiShanRupprechtetal.2022,
  author    = {Li, Donghai and Shan, Hangyong and Rupprecht, Christoph and Knopf, Heiko and Watanabe, Kenji and Taniguchi, Takashi and Qin, Ying and Tongay, Sefaattin and Nuß, Matthias and Schr{\"o}der, Sven and Eilenberger, Falk and H{\"o}fling, Sven and Schneider, Christian and Brixner, Tobias},
  title     = {Hybridized exciton-photon-phonon states in a transition-metal-dichalcogenide van-der-Waals heterostructure microcavity},
  series = {Physical Review Letters},
  journal   = {Physical Review Letters},
  edition   = {accepted version},
  issn      = {1079-7114},
  doi       = {10.1103/PhysRevLett.128.087401},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-351303},
  year      = {2022},
  abstract  = {Excitons in atomically thin transition-metal dichalcogenides (TMDs) have been established as an attractive platform to explore polaritonic physics, owing to their enormous binding energies and giant oscillator strength. Basic spectral features of exciton polaritons in TMD microcavities, thus far, were conventionally explained via two-coupled-oscillator models. This ignores, however, the impact of phonons on the polariton energy structure. Here we establish and quantify the threefold coupling between excitons, cavity photons, and phonons. For this purpose, we employ energy-momentum-resolved photoluminescence and spatially resolved coherent two-dimensional spectroscopy to investigate the spectral properties of a high-quality-factor microcavity with an embedded WSe\(_2\) van-der-Waals heterostructure at room temperature. Our approach reveals a rich multi-branch structure which thus far has not been captured in previous experiments. Simulation of the data reveals hybridized exciton-photon-phonon states, providing new physical insight into the exciton polariton system based on layered TMDs.},
  language  = {en}
}