Das erste Ziel der vorliegenden Dissertation bestand darin, ein bereits bestehendes TOF-MS-Setup dahingehend zu erweitern, um damit Velocity Map Imaging-Experimente durchführen zu können. Dies erforderte zunächst die Konzipierung und Programmierung einiger für die Datenaufnahme, -verarbeitung und -analyse benötigter LabView-Anwendungen. Anschließend konnten erste Kalibrierexperimente an Methyliodid, in denen wichtige experimentelle Parameter identifiziert und optimiert wurden, durchgeführt werden. Außerdem gelang es dadurch, die Messgenauigkeit des Setups auf 0.7 % und dessen Auflösungsvermögen auf 4.4 % zu bestimmen, was im Bereich für VMI-Apparaturen typischer Werte liegt. Zur weiteren Überprüfung der Funktionstüchtigkeit des Setups wurde in ersten zeitaufgelösten Experimenten im Folgenden die Desaktivierung des S1-Zustands von Pyridin untersucht. Neben der Reproduktion einiger bereits literaturbekannter Resultate konnten dabei zusätzlich die im Multiphotonen-Ionisationsschritt populierten Rydberg-Zustände identifiziert werden. Anschließend wurde mit Experimenten an bisher weniger gut untersuchten organischen Aromaten und Heteroaromaten fortgefahren. Das Ziel dieser Studien lag in der Aufklärung der photoinduzierten Dynamiken der Verbindungen, wobei das zur Verfügung stehende ps-Lasersystem die Möglichkeit bot, die Desaktivierung elektronisch angeregter Zustände gezielt in Abhängigkeit von deren Schwingungsenergie zu untersuchen. Der darin bestehende Vorteil zeigte sich vor allem in Studien an Tolan und Phenanthridin, deren erste angeregte, optisch aktive Zustände am Origin Lebensdauern im ns-Bereich aufweisen, die sich mit zunehmender vibronischer Anregung jedoch auf bis zu 10 ps verringern. Als Grund dafür konnten nichtstrahlende Desaktivierungsprozesse, für deren Eintreten eine energetische Barriere überwunden werden muss, identifiziert werden. Während in Tolan nach Photoanregung ein Übergang in einen (πσ∗)-Zustand, der zur Ausbildung einer trans-bent-Struktur führt, erfolgt, ist im Falle von Phenanthridin vermutlich ein El-Sayed-erlaubter ISC-Übergang in einen 3(nπ∗)-Zustand für die drastische Verkürzung der S1-Lebensdauer verantwortlich. Ein solcher konnte weder im zu Phenanthridin isomerischen Benzo[h]quinolin, noch in dessen PAH-Muttermolekül Phenanthren beobachtet werden, was auf die höhere energetische Lage bzw. die Abwesenheit des mittels ISC populierten 3(nπ∗)-Zustands in diesen Molekülen zurückgeführt werden kann. In weiteren im Rahmen der vorliegenden Arbeit durchgeführten Experimente wurden zudem die aromatischen Moleküle Acenaphthylen und 4-(Dimethylamino)benzethin (DMABE) untersucht. Zeitaufgelöste Studien zeigten dabei, dass die Desaktivierung der S2-Zustände beider Moleküle auf der sub-ps-Zeitskala stattfindet und mit dem vorhandenen Lasersystem daher nicht aufgelöst werden kann. In Acenaphthylen erfolgt die S2-Relaxation größtenteils über einen sequentiellen IC-Mechanismus, innerhalb dem der S1-Zustand des Moleküls intermediär besetzt wird. Dessen Lebensdauer konnte am Origin auf 380 ps bestimmt werden, fällt mit steigender Schwingungsanregung jedoch auf bis zu 55 ps ab. Für die Desaktivierung des S2-Zustands von DMABE konnte hingegen ein paralleles Relaxationsmodell, in dem neben dem S1-Zustand ein weiterer elektronisch angeregter Zustand populiert wird, nachgewiesen werden. Bei diesem könnte es sich möglicherweise um einen (πσ∗)-Zustand, dessen Besetzung die Ausbildung einer trans-bent-Geometrie innerhalb der Acetylen-Einheit des Moleküls zur Folge hat, handeln. Einen weiteren großen Teil der vorliegenden Dissertation nahmen Experimente an van-der-Waals-gebundenen Clustersystemen ein. Im Fokus der Studien standen dabei Moleküle mit ausgedehnten aromatischen π-Systemen, da solche eine hohe Relevanz für verschiedene materialwissenschaftliche Forschungsgebiete besitzen. Ein Beispiel hierfür ist Tetracen, welches als Modellsystem für die Untersuchung von Singlet Fission-Prozessen angesehen wird. In Kombination mit nichtadiabatischen Surface-Hopping-Simulationen zeigten Experimente an Tetracen-Dimeren, dass nach deren S2-Anregung zunächst ein schneller S1←S2-Übergang (τ < 1 ps), gefolgt von der Ausbildung einer Excimerstruktur, stattfindet. Letztere erfolgt mit einer Zeitkonstante von 62 ps und führt zu einem Anstieg des transienten Ionensignals, wohingegen die Desaktivierung des Excimer-Zustands von einem abklingenden Signalbeitrag mit τ = 123 ps repräsentiert wird. Wenngleich über die weitere Relaxation der Excimerspezies zum gegenwärtigen Zeitpunkt keine Aussage getroffen werden kann, besteht damit die Möglichkeit, dass Excimer-Zustände als Zwischenstufe im SF-Mechanismus isolierter Tetracen-Dimere auftreten. In zeitaufgelösten Experimenten an Phenanthren-Dimeren konnte ebenfalls ein Anstieg des transienten Signals mit einer vergleichbaren Zeitkonstante von τ = 86 ps, der jedoch auf einem konstanten Signaloffset endet, gefunden werden. Dies deutet darauf hin, dass auch Phenanthren-Dimere in der Lage sind, Excimerstrukturen, die im Gegensatz zu denen des Tetracens jedoch deutlich langlebiger sind, auszubilden. Studien an den Dimerspezies der Azaphenanthrene Benzo[h]quinolin und Phenanthridin offenbarten hingegen etwas schnellere Relaxationen mit Zeitkonstanten von 15 bzw. 40 ps. Zudem zeigten beide Spezies eine stark ausgeprägte Fragmentation, sodass für deren Untersuchung auf die VMI-Detektionsmethode zurückgegriffen werden musste. Dadurch wurde deutlich, dass sich Photoionen-Imaging-Experimente hervorragend für Studien an schwach gebundenen Clustersystemen eignen, da diese die Separation verschiedener Signalbeiträge innerhalb eines betrachteten Massenkanals ermöglichen. / In the first part of this thesis an already existing TOF-MS setup was modified in order to enable Velocity Map Imaging experiments. Therefore, LabView programs for the aquisition, processing and evaluation of the experimental data had to be written. Afterwards, calibration experiments on methyl iodide were carried out to characterize and to optimize important experimental parameters. The experiments yielded values of 4.4 % and 0.7 % for the spectral resolution and the accuracy of the setup, respectively, in good agreement with reported values for typical VMI setups. In the next step, time-resolved experiments on the S1 state deactivation in pyridine were performed in order to further verify the functionality of the setup. In these experiments, several results from literature could be reproduced and additional information on the Rydberg states being populated during the multiphoton ionization of the molecules were obtained. Thus, the experiments proved the suitability of the setup and experiments on less well studied systems were carried out in the following. The goal of these studies was to elucidate the light-induced relaxation mechanisms of selected organic aromatics and heteroaromatics. Due to the spectral bandwidth of the available ps laser setup, dynamics of electronically excited states could be studied as a function of their vibronic energy. This advantage became obvious especially in studies on tolane and phenanthridine: In both molecules, the lifetime of the first excited bright state is in the ns range at its origin, but drops to around 10 ps at higher excitation energies. The reason therefore are nonradiative relaxation processes which can only take place when an energetic barrier is surmounted. In case of tolane, a transition to a (πσ∗) state, leading to the formation of a trans-bent structure, was found to occur at higher excitations. In contrast, an El-Sayed allowed ISC process to a (nπ∗) triplet state seems to be responsible for the drop of the S1 state lifetime in phenanthridine. Interestingly, neither in the isomeric azaphenanthrene benzo[h]quinoline, nor in the PAH parent molecule phenanthrene itself, such a behavior was observed. This is attributed to the higher energy of the first excited (nπ∗) triplet state in benzo[h]quinoline and its absence in phenanthrene, respectively. Further experiments presented in this thesis aimed to elucidate the excited-state dynamics of acenaphthylene and 4-(dimethylamino)benzethyne (DMABE). Time-resolved studies on both molecules revealed S2 state deactivations on the sub-picosecond timescale which thus can not be resolved with the available ps laser setup. In acenaphthylene, a subsequent IC relaxation back to the electronic ground state was found to occur upon S2 excitation and the lifetime of the intermediately populated S1 state was determined to 380 ps at its origin and to 55 ps at higher excitation energies. The S2 state of DMABE relaxes to the S1 state as well, but in addition, the population of another electronic state, which might possibly be a trans-bent (πσ∗) state, was observed. Another large part of the experimental work within this thesis was covered from studies on van der Waals clusters of different aromatic and heteroaromatic compounds. The investigations focused on molecules with extended π -systems, since those possess photophysical properties with high relevance for various applications in material science. As an example, tetracene dimers can be seen as a prototype for the singlet fission process and thus were studied in the scope of this work. In time-resolved experiments, a sequential relaxation with time constants of 62 and 123 ps was observed upon excitation of their S2 state. Based on non-adiabatic surface hopping simulations the time constants could be assigned to the formation and the following decay of an excimer species. Thus, the excimer state could act as an intermediate in the SF mechanism of isolated tetracene dimers, although no information on its further deactivation are available so far. Interestingly, the formation of the excimer state leads to a rise in the transient ion signal, whereas its deactivation correlates with a decaying contribution. A similar behavior was found in experiments on phenanthrene dimers, which relax to a long-lived electronic state with a rising time constant of 86 ps. This indicates that excimer structures are formed upon photoexcitation in phenanthrene dimers as well. However, since their deactivation was not observed on the timescale of the experiment, the phenanthrene excimers seem to possess a much longer lifetime than their tetracene analogues. Studies on the dimeric species of the phenanthrene aza-derivatives benzo[h]quinoline and phenanthridine revealed slightly faster deactivation processes with time constants of 15 and 40 ps, respectively. Furthermore, the multimers of both compounds showed strong fragmentations and thus had to be studied via VMI detection. Thereby it became obvious that photoion imaging experiments are an excellent tool for investigations on weakly bound van der Waals clusters, since they allow to distinguish between different signal contributions in a given mass channel.

Thesis advisor: Matthias M. Waegele / Studying the adsorption and reaction kinetics of surface-bound chemical species, on different metal catalysts or electrodes, is of paramount importance in the development of inhomogeneous catalytic methodology. Our study of the oxidation of CO on platinum was accomplished by designing a thin layer flow cell in an external reflection configuration. A charge-injection circuit was successfully implemented which decreased the time required to charge the double layer in the electrochemical cell. We were able to obtain a signal via Stark shift spectrum, of the adsorbed CO, using the thin layer cell configuration. Additionally, electrochemical impedance spectroscopy was used as a diagnostic tool to assess the effect of electrode geometry, on the voltage response, in the thin layer cell. The coupling of visible light-driven photoexciation with transition metal catalytic plat- forms is emerging as a synthetic strategy to achieve unique reactivity that has previously been inaccessible. One such example is the iridium/nickel-dipyridyl system discovered recently. Characterizing the interactions between the iridium and nickel catalysts, under reaction conditions, is important to develop a better understanding of the system. In order to apply infrared spectroscopic measurement techniques, in-situ, we made modifications to the synthetic scheme by changing the solvent and by utilizing different iridium catalysts for the synthesis of the desired methyl 4-(benzoyloxy)benzoate product. Using our trans- mission infrared setup we effectively demonstrated in-situ product detection of the aryl- ester coupled product. Additionally, after constructing a transient infrared pump-probe setup, we collected preliminary results of the triplet state lifetime of the iridium dye. The surface morphology of copper has been shown to affect the electrochemical reduction of CO2. Using surface-enhanced Raman spectroscopies, the reversible formation of nanoscale metal clusters on a copper electrode was revealed at sufficiently cathodic potentials where we observed the appearance of a new band at 2080 cm-1 corresponding to C≡O adsorbed to undercoordinated copper defect sites. The formation of new undercoordinated sites additionally resulted in the surface enhancement of the Raman scattering which amplified the intensity of the other spectral bands. / Thesis (MS) — Boston College, 2019. / Submitted to: Boston College. Graduate School of Arts and Sciences. / Discipline: Chemistry.

Das Ziel der vorliegenden Arbeit war die Umsetzung einer experimentellen Herangehensweise, welche die kohärente zweidimensionale (2D) Spektroskopie an Proben in unterschiedlichen Aggregatzuständen ermöglicht. Hierzu wurde zunächst ein Aufbau für flüssige Proben realisiert, in welchem die emittierte Fluoreszenz als Messsignal zur Aufnahme der 2D Spektren genutzt wird. Im Gegensatz zu dieser bereits etablierten Methode in der flüssigen Phase stellt die in dieser Arbeit außerdem vorgestellte 2D Spektroskopie an gasförmigen Proben in einem Molekularstrahl einen neuen Ansatz dar. Hierbei werden zum ersten Mal Kationen mittels eines Flugzeitmassenspektrometers als Signal verwendet und somit ionen-spezifische 2D Spektren isolierter Moleküle erhalten. Zusätzlich zu den experimentellen Entwicklungen wurde in dieser Arbeit ein neues Konzept zur Datenerfassung in der 2D Spektroskopie entworfen, welches mit Hilfe einer optimierten Signalabtastung und eines Compressed-Sensing Rekonstruktionsalgorithmus die Aufnahmezeit der Daten deutlich reduziert. Charakteristisch für die in dieser Arbeit eingesetzte Variante der 2D Spektroskopie ist die Verwendung einer phasenkohärenten Sequenz bestehend aus vier Laserimpulsen in einer kollinearen Laserstrahlgeometrie zur Anregung der Probe. Diese Impulssequenz wurde durch einen Laserimpulsformer erzeugt, der durch Änderung der relevanten Laserimpulsparameter mit der Wiederholrate des Lasers eine schnelle Datenerfassung ermöglicht. Die Antwort der Probe auf diese Anregung wurde durch inkohärente Observablen gemessen, welche proportional zur Population des angeregten Zustandes sind, wie zum Beispiel Fluoreszenz oder Ionen. Um aus diesem Signal während der Datenanalyse die gewünschten nichtlinearen Beiträge zu extrahieren, wurde die Messung mit verschiedenen Kombinationen der relativen Phase zwischen den Laserimpulsen wiederholt ("Phase Cycling"). Der Aufbau zur 2D Spektroskopie in flüssiger Phase mit Fluoreszenz-Detektion wurde an Hand von 2D Spektren des Laserfarbstoffes Cresyl Violett charakterisiert. Hierbei wurden Oszillationen in verschiedenen Bereichen des 2D Spektrums beobachtet, welche durch vibronische Kohärenzen hervorgerufen werden und mit früheren Beobachtungen in der Literatur übereinstimmen. Mit dem gleichen Datensatz wurde im nächsten Schritt das neue Konzept zur optimierten Datenerfassung demonstriert. Um ein optimiertes Schema für die Signalabtastung zu finden, wurde ein genetischer Algorithmus implementiert, wobei nur ein Viertel der eigentlichen Datenpunkte zur Messwerterfassung verwendet werden sollte. Dies reduziert die Zeitdauer der Datenerfassung auf ein Viertel der ursprünglichen Messzeit. Die Rekonstruktion des vollständigen Signales erfolgte mit Hilfe einer neuartigen, kompakten Darstellung von 2D Spektren basierend auf der von Neumann Basis. Diese Herangehensweise benötigte im Vergleich zur üblicherweise verwendeten Fourier Basis nur ein Sechstel der Koeffizienten um das Signal vollständig darzustellen und ermöglichte so die erfolgreiche Rekonstruktion der Oszillationen in Cresyl Violett aus einem reduzierten Datensatz. Mit Hilfe der neuartigen kohärenten 2D Spektroskopie an Molekularstrahlen wurden Übergänge von hoch angeregten Rydberg-Zuständen ins ionische Kontinuum in Stickstoffdioxid untersucht. Als dominierender Beitrag stellte sich hierbei der Übergang in auto-ionisierende Zustände heraus. Ein wesentlicher Vorteil der Datenerfassung über ein Flugzeitmassenspektrometer ist die Möglichkeit der gleichzeitigen Aufnahme von 2D Spektren der Edukte und Produkte einer chemischen Reaktion. Dies wurde in Experimenten zur Mehrphotonenionisation gezeigt, in denen deutliche Unterschiede in den 2D Spektren des Stickstoffdioxid-Kations und des Stickstoffmonoxid-Fragmentes sichtbar wurden, welche auf unterschiedliche Antwortfunktionen zurückzuführen sind. Die in dieser Arbeit entwickelten experimentellen Techniken ermöglichen die schnelle Aufnahme von 2D Spektren für Proben in unterschiedlichen Aggregatzuständen und erlauben einen zuverlässigen, direkten Vergleich der Ergebnisse. Sie sind deshalb ein Wegbereiter für zukünftige Untersuchungen der Eigenschaften quantenmechanischer Kohärenzen in photophysikalischen Prozessen oder während photochemischer Reaktionen in unterschiedlichen Aggregatzuständen. / The aim of the present work was to implement an experimental approach that enables coherent two-dimensional (2D) electronic spectroscopy of samples in various states of matter. For samples in the liquid phase, a setup was realized that utilizes the sample fluorescence for the acquisition of 2D spectra. Whereas the liquid-phase approach has been established before, coherent 2D spectroscopy on gaseous samples in a molecular beam as developed in this work is in fact a new method. It employs for the first time cations in a time-of-flight mass spectrometer for signal detection and was used to obtain the first ion-selective 2D spectra of a molecular-beam sample. Additionally, a new acquisition concept was developed in this thesis that significantly decreases measurement times in 2D spectroscopy using optimized sparse sampling and a compressed-sensing reconstruction algorithm. Characteristic for the variant of 2D spectroscopy presented in this work is the usage of a phase-coherent sequence of four laser pulses in a fully collinear geometry for sample excitation. The pulse sequence was generated by a custom-designed pulse shaper that is capable of rapid scanning by changing the pulse parameters such as time delays and phases with the repetition rate of the laser. The sample's response was detected by monitoring incoherent observables that arise from the final-state population, for instance fluorescence or cations. Phase cycling, i.e., signal acquisition with different combinations of the relative phases of the excitation pulses, was applied to extract nonlinear signal contributions from the full signal during data analysis. Liquid-phase 2D fluorescence spectroscopy was established with the laser dye cresyl violet as a sample molecule, confirming coherent oscillations previously observed in literature that are originating from vibronic coherences in specific regions of the 2D spectrum. The data set of this experiment was used subsequently to introduce optimized sparse sampling in 2D spectroscopy. An optimization algorithm was implemented in order to find the best sampling pattern while taking only one quarter of the regular time-domain sampling points, thereby reducing the acquisition time by a factor of four. Signal recovery was based on a new and compact representation of 2D spectra using the von Neumann basis, which required about six times less coefficients than the Fourier basis to retain the relevant information. Successful reconstruction was shown by recovering the coherent oscillations in cresyl violet from a reduced data set. Finally, molecular-beam coherent 2D spectroscopy was introduced with an investigation of ionization pathways in highly-excited nitrogen dioxide, revealing transitions to discrete auto-ionizing states as the dominant contribution to the ion signal. Furthermore, the advantage of the time-of-flight approach to obtain reactant and product 2D spectra simultaneously enabled the observation of distinct differences in the multiphoton-ionization response functions of the nitrogen dioxide cation and the nitrogen oxide ionic fragment. The developed experimental techniques of this work will facilitate fast acquisition of 2D spectra for samples in various states of matter and permit reliable direct comparison of results. Therefore, they pave the way to study the properties of quantum coherences during photophysical processes or photochemical reactions in different environments.

Three types of nonlinear optical spectroscopies, ultrafast two-dimensional infrared (2DIR) spectroscopy, transient infrared (IR) absorption/pump-probe spectroscopy, and sum-frequency generation (SFG) vibrational spectroscopy, are used to investigate molecular structure and dynamics in two distinct classes of materials. First, 2DIR and pump-probe spectroscopies are used to study ultrafast rotational and vibrational energy relaxation in dense gaseous and supercritical fluid solutions, special solvation effects near the critical point, and the evolution of cooperative, liquid-phase dynamics as a function of density for two different solvent systems. 2DIR’s demonstrated capabilities offer a unique tool for identifying co-existing free rotor and liquid-like populations within the same fluid sample, evaluating the adequacy of isolated binary collision (IBC) relaxation descriptions in dense gas and near-liquid density fluids, and learning about how solute-solvent intermolecular properties separately influence rotational and vibrational relaxation in these dynamic and heterogeneous environments. Analysis of the density-dependent 2DIR and pump-probe spectra of a quasi-free rotor (asymmetric stretch rovibrational band of N2O) in SF6 and Xe provides timescales for rotational energy relaxation rates (1 – 3 collisions), but much slower vibrational energy relaxation rates. A critical slowing effect on the rate of rotational relaxation is identified, and liquid-like solvation is observed in dense gaseous solutions at state points lower than the critical density. Solvent-dependent differences in energy relaxation and IBC model breakdown, as well as applications of this 2DIR methodology to other high density and supercritical solution dynamics and descriptions are discussed. In a second nonlinear spectroscopy project, SFG is used to study the role of substrate type, gold or silver, and surface roughness on the parity odd-even effect in n-alkanethiolate (n = 10 – 16) self-assembled monolayers (SAMs), materials of potential importance to molecular scale electronics. SFG methyl vibrational transition intensities, frequencies, and linewidths display parity and metal dependence attributable to the orientational differences of the interfacial ethyl group, which inverts for SAMs on Ag substrates relative to SAMs on Au. Substrate roughness, an often-underreported experimental parameter, is shown here to affect the extent of odd-even methyl orientation anisotropy, and this SFG analysis establishes a new roughness limit for the appearance of odd-even effects on Ag substrates.

This thesis is aimed at establishing modalities of time-resolved photoelectron spectroscopy (tr-PES) conducted at a free-electron laser (FEL) source and at a high harmonic generation (HHG) source for imaging the motion of atoms, charge and energy at photoexcited hybrid organic/inorganic interfaces. Transfer of charge and energy across interfaces lies at the heart of surface science and device physics and involves a complex interplay between the motion of electrons and atoms. At hybrid organic/inorganic interfaces involving planar molecules, such as pentacene and copper(II)-phthalocyanine (CuPc), atomic motions in out-of-plane direction are particularly apparent. Such hybrid interfaces are of importance to, e.g., next-generation functional devices, smart catalytic surfaces and molecular machines. In this work, two hybrid interfaces – pentacene atop Ag(110) and copper(II)-phthalocyanine (CuPc) atop titanium disulfide (1T-TiSe2) – are characterized by means of modalities of tr-PES. The experiments were conducted at a HHG source and at the FEL source FLASH at Deutsches Elektronen-Synchrotron DESY (Hamburg, Germany). Both sources provide photon pulses with temporal widths of ∼ 100 fs and thus allow for resolving the non-equilibrium dynamics at hybrid interfaces involving both electronic and atomic motion on their intrinsic time scales. While the photon energy at this HHG source is limited to the UV-range, photon energies can be tuned from the UV-range to the soft x-ray-range at FLASH. With this increased energy range, not only macroscopic electronic information can be accessed from the sample’s valence and conduction states, but also site-specific structural and chemical information encoded in the core-level signatures becomes accessible. Here, the combined information from the valence band and core-level dynamics is obtained by performing time- and angle-resolved photoelectron spectroscopy (tr-ARPES) in the UV-range and subsequently performing time-resolved x-ray photoelectron spectroscopy (tr-XPS) and time-resolved photoelectron diffraction (tr-XPD) in the soft x-ray regime in the same experimental setup. The sample’s bandstructure in energy-momentum space and time is captured by a time-of-flight momentum microscope with femtosecond temporal and sub-Ångström spatial resolutions. In the investigated systems, out-of-equilibrium dynamics are traced that are connected to the transfer of charge and energy across the hybrid interfaces. While energetic shifts and complementary population dynamics are observed for molecular and substrate states, the shapes of involved molecular orbitals change in energy-momentum space on a subpicosecond time scale. In combination with theory support, these changes are attributed to iiiatomic reorganizations at the interface and transient molecular structures are reconstructed with sub-Ångström precision. Unique to the material combination of CuPc/TiSe2, a structural rearrangement on the macroscopic scale is traced simultaneously: ∼ 60 % of the molecules undergo a concerted, unidirectional in-plane rotation. This surprising observation and its origin are detailed in this thesis and connected to a particularly efficient charge transfer across the CuPc/TiSe2 interface, resulting in a charging of ∼ 45 % of CuPc molecules. / Das Ziel der vorliegenden Doktorarbeit ist es, die Bewegung von Atomen, Ladungsträgern und Energie an organisch/anorganischen Grenzschichten fernab des thermischen Gleichgewichts zu visualisieren und deren Wechselwirkung zu entschlüsseln. Dies wird experimentell mittels zeitaufgelöster Photoemissionsexperimente an einer Freien-Elektronen-LaserQuelle und an einer Höher-Harmonischen-Quelle verwirklicht. Ladungs- und Energietransfer zwischen organisch/anorganischen Grenzschichten sind zentrale Komponenten für die Funktion Molekül-basierter Anwendungen, wie z.B. katalytische Oberflächen, elektronische Schalt- und Speichergeräte oder molekulare Maschinen. Sie stellen einen dynamischen Prozess dar, der sich in einem Wechselspiel aus der Bewegung von Elektronen zwischen beiden Schichten und atomaren Bewegungen innerhalb beider Schichten äußert. Planare Moleküle, wie Pentacen oder Kupfer(II)-Phthalocyanin (CuPc), eignen sich besonders um solche atomaren Bewegungen zu untersuchen, da diese aufgrund geringer Rückstellkräfte senkrecht zur Molekülebene besonders ausgeprägt sein können. In dieser Arbeit werden Ladungs- und Energietransferprozesse an zwei ausgewählten Grenzschichten untersucht: Pentacen auf Silber (Ag(110)) und CuPc auf Titan Diselenid (1T-TiSe2). Zeitaufgelöste Photoemissionsexperimente (tr-PES) wurden an einer HöherHarmonischen-Quelle und an dem Freien-Elektronen-Laser FLASH (Deutsches Elektronen-Synchrotron DESY, Hamburg, Deutschland) durchgeführt. Beide Lichtquellen liefern Photonenpulse mit einer Halbwertsbreite von etwa 100 fs und sind daher geeignet, um Nicht-Gleichgewichtsprozesse zeitlich aufzulösen, die auf der Bewegung von sowohl Elektronen als auch Atomen basieren. Die gewählte Höher-Harmonische-Quelle liefert Photonenenergien im UV-Bereich. Bei FLASH hingegen können die Photonenenergien variabel vom UV-Bereich bis hin zum Weichröntgenbereich erzeugt werden. Dieser erweiterte Energiebereich ermöglicht es, zusätzlich zur elektronischen Dynamik im Valenzbereich, auch Dynamiken kernnaher Zustände zu beobachten. Mithilfe dreier Modalitäten von zeitaufgelöster Photoemission – zeit- und winkelaufgelöste Photoelektronenspektroskopie (tr-ARPES), zeitaufgelöste Röntgenphotoelektronenspektroskopie (tr-XPS) und zeitaufgelöste Röntgenphotoelektronen-Diffraktion (tr-XPD) – werden sowohl die elektronischen als auch strukturellen Dynamiken der Grenzschicht rekonstruiert. Dabei dient tr-ARPES im UV-Bereich zur Charakterisierung der makroskopischen elektronischen Eigenschaften und tr-XPS und tr-XPD im Weichröntgenbereich dienen zur Analyse lokaler chemischer und struktureller Eigenschaften. Alle Messungen wurden unter denselben experimentellen Beidingungen durchgeführt und mithilfe eines Flugzeit-Impulsmikroskops konnte die transiente Bandstruktur mit einer Ortauflösung im Sub-Ångström-Bereich und einer Zeitauflö- sung im Femtosekunden-Bereich aufgenommen werden. In beiden untersuchten Systemen werden elektronische und strukturelle Prozesse an der Molekül–Substrat Grenzfläche beobachtet, die durch einen Ladungs- und Energietransfer in Folge optischer Anregung erklärt werden. Dieser Transfer äußert sich elektronisch durch ein Befüllen des Substrat-Leitungsbands und einem zeitgleichen Entleeren der MolekülValenzorbitale. Strukturelle Veränderungen, wie die Adsorptionshöhe oder intramolekulare Atompositionen, werden aus den sich zeitgleich verformenden Molekül-Valenzorbitalen rekonstruiert. Speziell für CuPc/TiSe2 wird ein effektiver Ladungstransfer beobachtet, wodurch 375 fs nach optischer Anregung ∼ 45 % der Moleküle einfach positiv geladen vorliegen. Diese Ladungstrennung zwischen den sich wie ein Schachbrett anordnenden positivgeladenen und neutralen Molekülen sowie dem Substrat führt zu einer Modulation des Oberflächenpotentials, welche eine energetische Verschiebung aller Grenzflächenzustände bedingt und intramolekulare Strukturveränderungen sowie eine makroskopische Reorganisation des Molekülfilms zur Folge hat: ∼ 60 % der Moleküle drehen sich innerhalb von ∼ 375 fs synchron auf dem Substrat und nehmen nach ∼ 1800 fs wieder ihre Ausgangsposition ein. Diese überraschende Beobachtung sowie die Ursache werden detaillierter in der vorliegenden Arbeit diskutiert und in den Kontext aktueller Forschung an "molekularen Schaltern" gebracht.

No description available.

In this PhD thesis, we study the interplay between symmetry-breaking order and quantum-disordered phases in the milieu of frustrated quantum magnets, and further show how the excitation process of long-wavelength (semi-)classical modes in spin-orbit coupled antiferromagnets crucially depends on the nature and interactions of the underlying quantum quasiparticles. First, we focus on Kitaev's exactly solvable model for a Z2 spin liquid as a building block for constructing novel phases of matter, utilizing Majorana mean-field theory (MMFT) to map out phase diagrams and study occurring phases. In the Kitaev Kondo lattice, conduction electrons couple via a Kondo interaction to the local moments in the Kitaev model. We find at small Kondo couplings a fractionalized Fermi liquid (FL*) phase, a stable non-Fermi liquid where conventional electronic quasiparticles coexist with the deconfined excitations of the spin liquid. The transition between FL* and a conventional Fermi liquid is masked by an exotic (confining) superconducting phase which exhibits nematic triplet pairing, which we argue to be mediated by the Majorana fermions in the Kitaev spin liquid. We moreover study bilayer Kitaev models, where two Kitaev honeycomb spin liquids are coupled via an antiferromagnetic Heisenberg interaction. Varying interlayer coupling and Kitaev coupling anisotropy, we find both direct transitions from the spin liquid to a trivial dimer paramagnet as well as intermediate 'macrospin' phases, which can be studied by mappings to effective transverse-field Ising models. Further, we find a novel interlayer coherent pi-flux phase. Second, we consider the stuffed honeycomb Heisenberg antiferromagnet, where recent numerical studies suggest the coexistence of collinear Néel order and a correlated paramagnet, dubbed 'partial quantum disorder'. We elucidate the mechanism which drives the disorder in this model by perturbatively integrating out magnons to derive an effective model for the disordered sublattice. This effective model is close to a transition between two competing ground states, and we conjecture that strong fluctuations associated with this transition lead to disorder. Third, we study the generation of coherent low-energy magnons using ultrafast laser pulses in the spin-orbit coupled antiferromagnet Sr2IrO4, inspired by recent pump-probe experiments. While the relaxation dynamics of the system at long time scales can be well described semi-classically, the ultrafast excitation process is inherently non-classical. Using symmetry analysis to write down the most general coupling between electric field and spin operators, we subsequently integrate out high-energy spin fluctuations to derive induced effective fields which act to excite the low-energy magnon, constituting a generalized 'inverse Faraday effect'. Our theory reveals a tight relationship between induced fields and the two-magnon density of states.:1 Introduction 1.1 Frustrated antiferromagnets 1.2 Quantum spin liquids 1.3 Fractionalization and topological order 1.4 Spin-orbit coupling 1.5 Outline I Novel phases by building on Kitaev’s honeycomb model 2 Kitaev honeycomb spin liquid 2.1 Microscopic spin model and constants of motion 2.2 Majorana representation of spin algebra 2.3 Exact solution 2.3.1 Ground state 2.3.2 Correlations and dynamics 2.3.3 Thermodynamic properties 2.4 Z2 gauge structure 2.5 Toric code 2.6 Topological order 2.6.1 Superselection sectors and ground-state degeneracy 2.6.2 Topological entanglement entropy 2.6.3 Symmetry-enriched and symmetry-protected topological phases 3 Mean-field theory 3.1 Generalized spin representations 3.1.1 Parton constructions 3.1.2 SO(4) Majorana representation 3.2 Projective symmetry groups 3.3 Mean-field solution of the Kitaevmodel 3.4 Comparisonwithexactsolution 3.4.1 Spectral properties 3.4.2 Correlation functions 3.4.3 Thermodynamic properties 3.5 Generalized decoupling 3.6 Comparison to previous Abrikosov fermion mean-field theories of the Kitaev model 3.7 Discussion 4 Fractionalized Fermi liquids and exotic superconductivity in the Kitaev Kondo lattice 4.1 Metals with frustration 4.2 Local-moment formation and Kondo effect 4.2.1 Single Kondo impurity 4.2.2 Kondo lattices and heavy Fermi liquids 4.3 Fractionalized Fermi liquids 4.4 Construction of the Kitaev Kondo lattice 4.4.1 Hamiltonian 4.4.2 Symmetries 4.5 Mean-field decoupling of Kondo interaction 4.5.1 Solution of self-consistency conditions 4.6 Overview of mean-field phases 4.7 Fractionalized Fermi liquid 4.7.1 Results from mean-field theory 4.7.2 Perturbation theory beyond mean-field theory 4.8 Heavy Fermi liquid 4.9 Superconducting phases 4.9.1 Spontaneously broken U(1) phase rotation symmetry 4.9.2 Excitation spectrum and nematicity 4.9.3 Topological triviality 4.9.4 Group-theoretical classification 4.9.5 Pairing glue 4.10 Comparison with a subsequent study 4.11 Discussion and outlook 5 Bilayer Kitaev models 5.1 Model and stacking geometries 5.1.1 Hamiltonian 5.1.2 Symmetries and conserved quantities 5.2 Previous results 5.3 Mean-field decoupling and phase diagrams 5.3.1 AA stacking 5.3.2 AB stacking 5.3.3 σAC stacking 5.3.4 σ ̄AC stacking 5.4 Quantum phase transition in the AA stacking 5.4.1 Perturbative analysis 5.5 Phase transition in the σAC stacking 5.6 Macro-spin phases 5.6.1 KSL-MAC transition: Effective model for Kitaev dimers 5.6.2 DIM-MAC transition: Effective theory for triplon condensation 5.6.3 Macro-spin interactions and series expansion results 5.6.4 Antiferromagnet in the AB stacking 5.7 Stability of KSL and the interlayer-coherent π-flux phase 5.7.1 Perturbative stability of the Kitaev spin liquid 5.7.2 Spontaneous interlayer coherence near the isotropic point 5.8 Summary and discussion II Partial quantum disorder in the stuffed honeycomb lattice 6 Partial quantum disorder in the stuffed honeycomb lattice 6.1 Definition of the stuffed honeycomb Heisenberg antiferromagnet 6.2 Previous numerical results 6.3 Derivation of an effective model 6.3.1 Spin-wave theory for the honeycomb magnons 6.3.2 Magnon-central spin vertices 6.3.3 Perturbation theory 6.3.4 Instantaneous approximation 6.3.5 Truncation of couplings 6.3.6 Single-ion anisotropy 6.3.7 Discussion of most dominant interactions 6.4 Analysis of effective model 6.4.1 Classical ground states 6.4.2 Stability of classical ground states in linear spin-wave theory 6.4.3 Minimal model for incommensurate phase 6.4.4 Discussion of frustration mechanism in the effective model 6.5 Partial quantum disorder beyond the effectivemodel 6.5.1 Competition between PD and the (semi-)classical canted state 6.5.2 Topological aspects 6.5.3 Experimental signatures 6.6 Discussion 6.6.1 Directions for further numerical studies 6.6.2 Experimental prospects III Optical excitation of coherent magnons 7 Ultrafast optical excitation of magnons in Sr2IrO4 7.1 Pump-probe experiments 7.2 Previous approaches to the inverse Faraday effect and theory goals 7.3 Sr2IrO4 as a spin-orbit driven Mott insulator 7.4 Spin model for basal planes in Sr2IrO4 7.4.1 Symmetry analysis 7.4.2 Classical ground state and linear spin-wave theory 7.4.3 Mechanism for in-plane anisotropy 7.5 Pump-induced dynamics 7.5.1 Coupling to the electric field: Symmetry analysis 7.5.2 Keldysh path integral 7.5.3 Low-energy dynamics 7.5.4 Driven low-energy dynamics 7.6 Derivation of the induced fields 7.6.1 Perturbation theory 7.6.2 Evaluation of loop diagram 7.6.3 Analytical momentum integration in the continuum limit 7.6.4 Numerical evaluation of effective fields 7.7 Analysis of induced fields 7.7.1 Polarization and angular dependence 7.7.2 Two-magnon spectral features 7.8 Applications to experiment 7.8.1 Predictions for experiment 7.8.2 Magnetoelectrical couplings 7.9 Discussion and outlook 8 Conclusion and outlook 8.1 Summary 8.2 Outlook IV Appendices A Path integral methods B Spin-wave theory B.1 Holstein-Primakoff bosons B.2 Linear spin-wave theory B.2.1 Diagonalization via Bogoliubov transformation B.2.2 Applicability of linear approximation B.3 Magnon-magnon interactions B.3.1 Dyson's equation and 1/S consistency B.3.2 Self-energy from quartic interactions in collinear states on bipartite lattices C Details on the SO(4) Majorana mean-field theory C.1 SO(4) Matrix representation of SU(2) subalgebras C.2 Generalized SO(4) Majorana mean-field theory for a Heisenberg dimer (Chapter 3) C.3 Dimerization of SO(4) Majorana mean-field for the Kitaev model (Chapter3) C.4 Mean-field Hamiltonian in the Kitaev Kondo lattice (Chapter 4) C.5 Example solutions in the superconducting phase for symmetry analysis (Chapter4) D Linear spin-wave theory for macrospin phase in the bilayer Kitaev model (Chapter 5) D.1 Spin-wave Hamiltonian and Bogoliubov rotation D.2 Results and discussion E Extrapolation of the effective couplings for the staggered field h -> 0 (Chapter 6) E.1 xy interaction E.1.1 Leadingorder ~ S0 E.1.2 Subleadingorder ~ S^(−1) E.2 z-Ising interaction F Light-induced fields by analytical integration (Chapter 7) F.1 Method F.2 Results Bibliography

Thesis (MSc (Physics))--University of Stellenbosch, 2009. / An ultrafast pump-probe spectroscopy experiment was developed in order to investigate the fast photoinduced isomerization reaction of the molecule resveratrol. Characteristics of the resveratrol molecule are discussed, including the photoisomerization reaction from trans- to cis-resveratrol. The experimental setup for the conventional spectroscopy measurement was developed and characterized in order to investigate and understand the conventional absorption and uorescence spectroscopy of resveratrol thoroughly. The absorption spectra for both trans- and cis-resveratrol, as well as the uorescence spectra were measured, discussed and explained. This therefore forms a foundation and serves as an initial step to develop a pump-probe spectroscopy experiment for resveratrol. A general overview of ultrafast pump-probe spectroscopy is presented, as well as an explanation of the nal developed experimental setup. The principles and characteristics of the chirped pulse ampli cation (CPA) femtosecond laser source and the tunable noncollinear optical parametric ampli er (NOPA) employed as the pump pulse are discussed. The process of white light continuum (WLC) generation was investigated to utilize as the ultrashort probe pulse. Two white light continuum generation experimental setups were developed and characterized for WLC generation in a transparent medium with the fundamental CPA laser light at 775 nm (in sapphire) and with the second harmonic (SH) of the CPA light at 387 nm (in quartz). A spectrometer was designed, built and characterized in conjuction with a line focus, for simultaneous measurement of the absorption in the pumped, unpumped and reference regions in the sample. In this way the photoisomerization of resveratrol could be measured with temporal resolution as a transient absorption signal. A 420 μg/ml resveratrol solution in ethanol was investigated in this pump-probe spectroscopy experiment and the results obtained are discussed accordingly.

Thesis (PhD (Physics))--University of Stellenbosch, 2010. / ENGLISH ABSTRACT: Silicon/silicon dioxide (Si/SiO2) interface is widely used in microelectronics as the gate between the drain and source of most metal oxide semiconductor field effect transistors (MOSFETs). The functionality, reliability and electrical properties of such transistors are strongly dependent on the quality of the Si/SiO2 structure forming the gate. Characterization of the Si/SiO2 interface is important in understanding device degradation therefore the Si/SiO2 interface is a subject of intensive investigation. Research studies of Si/SiO2 interfaces using optical methods have been reported by many groups around the world but to date many open questions still exist. The physics of photoinduced trap or defect generation processes and the subsequent trapping of charge carriers, the precise role of photoinduced interfacial electric field in altering optical properties of the Si/SiO2 interface and its role in affecting the second harmonic (SH) yield measurements are not well understood. In this work a commercial near infrared femtosecond (fs) laser source [1.55 eV, 75 ± 5 fs, 10 nJ, 80 MHz] is used to study native Si/SiO2 interfaces of free standing single crystalline Si membrane and bulk Si. Optical second harmonic (SH) generated at the Si/SiO2 interfaces of a Si membrane in reflection and for the first time in transmission is demonstrated as well as stationary, single colour, pump-probe reflectivity measurements from the Si/SiO2 interface of bulk n-type Si. The experimental setups for the second harmonic generation (SHG) and pump-probe techniques were designed and implemented, and measurements were recorded by a computer controlled data acquisition system. Free standing Si membrane samples were successfully produced at the Institut f¨ur Photonische Technologien (IPHT) in Jena, Germany from bulk Si using a chemical etching process and were characterised using the z-scan technique. The penetration depth of light with a photon energy of 1.55 eV in silicon allows transmission of the fundamental fs laser pulses through the Si membrane (∼ 10 μm in thickness) and this is exploited to generate a SH signal in transmission from the Si/SiO2 interfaces of the Si membrane. In the presence of sufficiently intense fs laser light defects are created at the interfaces and populated by multiphoton transfer of charges from Si to SiO2 where they are subsequently trapped. The transfer of charge establishes interfacial electric fields across the interfaces of the Si membrane and this enhances SHG. This phenomenon is called electric field induced second harmonic (EFISH) generation. To our knowledge, EFISH measurements from interfaces of Si membrane performed in transmission are demonstrated for the first time in the present study. The demonstration of EFISH in transmission revealed new results which allowed us to provide additional perspectives on the EFISH generation process at Si/SiO2 interfaces never reported before. The temporal response of SH signals from virgin spots were recorded at different incident laser powers for both reflection and transmission geometries. The SH responses measured in transmission were observed to be time dependent and show an increase during irradiation of the sample corresponding to EFISH process. A series of SH measurements were recorded at different laser powers to compare the magnitudes of SH yield in each detection geometry for a single Si/SiO2 interface. The magnitude of the SH yield measured in transmission was higher than expected and surpassed the SH yield measured in reflection. The expectation is based on the fact that the local intensity of the fundamental beam at the second interface where the SH in transmission is generated is low compared to the local intensity at the first interface where the SH in reflection originates. A physical model is developed to consistently interpret the experimental results obtained in this study. In this model we established the origin of EFISH signals in each detection geometry, explain the unexpected high SH signals measured in transmission and provide an analysis of the time constants extracted from SH response in transmission and reflection. In addition, we also report for the first time stationary pump-probe reflectivity measurements from bulk n-type Si(111) samples with native oxide. A strong pump beam was focused on the same spot as a weak probe beam from the same fs laser source. The change in reflectivity of the Si(111)/SiO2 system was recorded by monitoring the change in intensity of the weak reflected probe beam. The temporal evolutions of the reflectivity of the material were recorded at different pump powers. The reflectivity of the material increases over several minutes of irradiation and reaches steady-state after long time irradiation. The change in reflectivity of the material is attributed to a nonlinear process called Kerr effect, and the temporal response arises from the photoinduced interfacial electric field across the Si(111)/SiO2 interface caused by multiphoton charge transfer from bulk Si(111) to the SiO2 layer. The results reported in this study contribute to the understanding of the photoinduced interfacial electric field caused by charge carrier separation across buried solid-solid interfaces. They also reveal nonlinear optical processes such as the Kerr effect caused by charge dynamics across the interface in addition to the well known SHG process. / AFRIKAANSE OPSOMMING: Die silikon/silikon dioksied (Si/SiO2) skeidingsvlak word algemeen gebruik in mikro-elektronika as die hek tussen die put en die bron van die meeste metaaloksied halfgeleier veld-effek transistors (MOSFETs). Die werkverrigting, betroubaarheid en elektriese eienskappe van sulke transistors word grootliks bepaal deur die kwaliteit van die Si/SiO2 struktuur wat die hek vorm. Karakterisering van die Si/SiO2 skeidingsvlak is belangrik om die degradering van die transistor te verstaan en daarom is die Si/SiO2 skeidingsvlak die onderwerp van intensiewe ondersoek. Ondersoek van die Si/SiO2 skeidingsvlak deur van optiese metodes gebruik te maak is geraporteer deur verskeie internasionale groepe, maar daar bestaan tot vandag toe nog n groot aantal onbeantwoorde vrae. Die fisika van die fotogenduseerde generering van defekte en van posisies waarin ladings gevang kan word, asook die daaropvolgende vasvang van ladingsdraers, die presiese rol van die fotoge¨ınduseerde elektriese veld oor die skeidingsvlak in die verandering van die optiese eienskappe van die Si/SiO2 skeidingsvlak en die grootte van die tweede harmoniek (SH) sein word nog nie goed verstaan nie. In hierdie werk word n kommersile naby-infrarooi femtosekonde (fs) laserbron [1.55 eV, 75 ± 5 fs, 10 nJ, 80 MHz] gebruik om natuurlike Si/SiO2 skeidingsvlakke van vrystaande enkelkristallyne Si membrane en soliede Si te bestudeer. Optiese tweede harmoniek (SH) wat by die Si/SiO2 skeidingsvlakke van ’n Si membraan gegenereer word - in refleksie en vir die eerste keer in transmissie - is gedemonstreer, asook stasionˆere, een-golflengte pomp-toets refleksiemetings op die Si/SiO2 skeidingsvlak van soliede n-gedoteerde Si. Die eksperimentele opstellings vir die tweede harmoniek generering (SHG) en pomp-toets tegnieke is ontwerp en uitgevoer en metings is opgeneem deur ’n rekenaarbeheerde dataversamelingstelsel. Vrystaande Si membraan monsters is suksesvol by die Institut f¨ur Photonische Technologien (IPHT) in Jena, Duitsland vervaardig uit soliede Si deur ’n chemiese etsproses en is gekarakteriseer met behulp van die z-skanderingstegniek as deel van hierdie studie. Die diepte waartoe lig met ’n fotonenergie van 1.55 eV in silikon indring laat die transmissie van die fundamentele fs laserpulse deur die Si membraan (met ∼ 10 μm dikte) toe en dit word ontgin om ’n SH sein van die Si/SiO2 skeidingsvlakke van die Si membraan in transmissie te meet. In die teenwoordigheid van fs laserlig met voldoende intensiteit word defekte by die skeidingsvlakke geskep en bevolk deur meer-foton ladingsoordrag van die Si na die SiO2 waar die ladings daaropvolgens vasgevang word. Die oordrag van ladings skep elektriese velde oor die skeidingsvlakke van die Si membraan en dit versterk die SHG. Hierdie verskynsel word elektriese veld ge¨ınduseerde tweede harmoniek (EFISH) generering genoem. Sover ons kennis strek is die meting van EFISH seine van skeidingsvlakke van Si membrane in transmissie vir die eerste keer in hierdie studie gedemonstreer. Die demonstrasie van EFISH in transmissie het nuwe resultate opgelewer wat ons toegelaat het om bykomende perspektiewe op die EFISH genereringsproses by Si/SiO2 skeidingsvlakke te verskaf waaroor nog nooit vantevore verslag gedoen is nie. Die tydafhanklike gedrag van die SH seine van voorheen onbestraalde posisies is gemeet by verskillende drywings van die inkomende laserbundel vir beide die refleksie en transmissie geometrie¨e. Die gedrag van die SH sein in transmissie is waargeneem om tydafhanklik te wees en ’n toename te toon gedurende bestraling van die monster in ooreenstemming met EFISH prosesse. ’n Reeks van SH metings is opgeneem by verskillende laserdrywings om die groottes van die SH opbrengste in elke meetgeometrie vir ’n enkele Si/SiO2 skeidingsvlak te vergelyk. Die grootte van die SH opbrengs wat in transmissie gemeet is was ho¨er as verwag is en het die grootte van die SH opbrengs in refleksie oortref. Die verwagting is gebaseer op die feit dat die lokale intensiteit by die tweede skeidingsvlak waar SH in transmisie gegenereer word relatief laag is in vergelyking met die lokale intensiteit by die eerste skeidingsvlak waar SH in refleksie ontstaan. ’n Fisiese model is ontwikkel om die eksperimentele resultate wat in hierdie studie verkry is op ’n konsekwente wyse te interpreteer. In hierdie model het ons die oorsprong van EFISH seine in elke meetgeometrie vasgestel, die onverwagte ho¨e SH seine wat in transmissie gemeet is verklaar en ’n analise van die tydkonstantes wat uit die SH gedrag in transmissie en refleksie afgelei is gedoen. Verder rapporteer ons ook vir die eerste keer stasionˆere pomp-toets reflektiwiteitsmetings van soliede n-gedoteerde Si(111) monsters met ’n natuurlike oksied. ’n Sterk pompbundel is gefokus op dieselfde posisie as ’n swak toetsbundel van dieselfde laserbron. Die verandering in reflektiwiteit van die Si(111)/SiO2 stelsel is gemeet deur die verandering in die intensiteit van die swak weerkaatste toetsbundel te monitor. Die tydevolusie van die reflektiwiteit van die mate riaal is gemeet by verskillende pompdrywings. Die reflektiwiteit van die materiaal neem toe gedurende etlike minute van bestraling en bereik ’n stasionˆere toestand na ’n lang tyd van bestraling. Die verandering in reflektiwiteit van die materiaal word toegeskryf aan ’n nielini ˆere prosess, naamlik die Kerr effek, en die tydafhanklike gedrag ontstaan as gevolg van die fotoge¨ınduseerde elektriese veld oor die Si(111)/SiO2 skeidingsvlak wat veroorsaak word deur meer-foton ladingsoordrag van die soliede Si(111) na die SiO2 laag. Die resultate wat in hierdie studie gerapporteer word dra by tot die verstaan van die fotoge ¨ınduseerde elektriese veld oor die skeidingsvlak wat veroorsaak word deur die skeiding van ladingsdraers oor die bedekte kristal-kristal skeidingsvlak. Dit lˆe ook nie-liniˆere optiese prosesse soos die Kerr effek bloot wat veroorsaak word deur die dinamika van ladings oor die skeidingsvlak, bykomend tot die bekende SHG proses.

Since its inception a quarter of a century ago, Kelvin probe force microscopy (KPFM) has enabled studying contact potential differences (CPDs) on the nanometre scale. However, current KPFM investigations are limited by the bandwidth of its constituent electronic loops to the millisecond regime. To overcome this limitation, pump-probe-driven Kelvin probe force microscopy (pp-KPFM) is introduced that exploits the non-linear electric interaction between tip and sample. The time resolution surpasses the electronic bandwidth and is limited by the length of the probe pulse. In this work, probe pulse lengths as small as 4.5 ns have been realized. These probe pulses can be synchronized to any kind of pump pulses. The first system investigated with pp-KPFM is an electrically-driven organic field-effect transistor (OFET). Here, charge carrier propagation in the OFET channel upon switching the drain-source voltage is directly observed and compared to simulations based on a transmission line model. Varying the charge carrier density reveals the impeding influence of Schottky barriers on the maximum switching frequency. The second system is an optically-modulated silicon homojunction. Here, the speed of surface photovoltage (SPV) build-up is accessed and compared to timeaveraged results. Due to slow trap states, the time-averaged method is found to lack comprehensiveness. In contrast, pp-KPFM exposes two intensity-dependent recombination times on the same timescale — high-level Shockley-Read-Hall recombination in the bulk and heat-dominated recombination in the surface layer — and a delay of the SPV decay with rising frequency, which is attributed to charge carrier retention at nanocrystals. The third system is a DCV5T-Me:C60 bulk heterojunction. The SPV dynamics is probed and compared to measurements via open-circuit corrected transient charge carrier extraction by linearly increasing voltage. Both methods reveal an exponential onset of the band bending reduction that is attributed to the charge carrier diffusion time in DCV5T-Me, and a double exponential decay, hinting at different recombination paths in the studied organic solar cell. The above-mentioned experiments demonstrate that pp-KPFM surpasses conventional KPFM when it comes to extracting dynamic device parameters such as charge carrier retention and recombination times, and prove that pp-KPFM is a versatile and reliable tool for studying electrodynamics on nanosurfaces.