@phdthesis{Draeger2020, author = {Draeger, Simon}, title = {Rapid Two-Dimensional One-Quantum and Two-Quantum Fluorescence Spectroscopy}, doi = {10.25972/OPUS-19816}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-198164}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2020}, abstract = {In den letzten zwei Jahrzehnten hat sich die koh{\"a}rente mehrdimensionale Femtosekunden- Spektroskopie zu einem leistungsstarken und vielseitigen Instrument zur Untersuchung der chemischen Dynamik einer Vielzahl von Quantensystemen entwickelt. Die Kombination von transienten Informationen, die der Anrege-Abrage-Spektroskopie entsprechen, mit Informationen zur Kopplung zwischen energetischen Zust{\"a}nden und der Systemumgebung erm{\"o}glicht einen umfassenden Einblick in atomare und molekulare Eigenschaften. Viele experimentelle 2D-Aufbauten verwenden den koh{\"a}renzdetektierten Ansatz, bei dem nichtlineare Systemantworten als koh{\"a}rente elektrische Felder emittiert und r{\"a}umlich getrennt von den Anregungspulsen detektiert werden. Als Alternative zu diesem experimentell anspruchsvollen Ansatz wurde die populationsbasierte 2D-Spektroskopie etabliert. Hier wird die koh{\"a}rente Information in den Phasen einer kollinearen Anregungspulsfolge codiert und aus inkoh{\"a}renten Signalen wie Fluoreszenz {\"u}ber Phase Cycling extrahiert. Grunds{\"a}tzlich kann durch die Verwendung von Fluoreszenz als Observable eine Sensitivit{\"a}t bis zum Einzelmolek{\"u}lniveau erreicht werden. Ziel dieser Arbeit war die Realisierung eines pulsformergest{\"u}tzten vollst{\"a}ndig kollinearen fluoreszenzdetektierten 2D-Aufbaus und die Durchf{\"u}hrung von Proof-of- Principle-Experimenten in der Fl{\"u}ssigphase. Dieser inh{\"a}rent phasenstabile und kompakte Aufbau wurde in Kapitel 3 vorgestellt. Der verwendete Pulsformer erm{\"o}glicht eine Amplituden- und Phasenmodulation von Schuss zu Schuss. Zwei verschiedene Arten von Weißlichtquellen wurden angewendet und hinsichtlich ihrer jeweiligen Vorteile f{\"u}r die 2D-Fluoreszenzspektroskopie bewertet. Eine Vielzahl von Artefaktquellen, die mit dem vorliegenden Aufbau auftreten k{\"o}nnen, wurden diskutiert und Korrekturschemata und Anweisungen zur Vermeidung dieser Artefakte bereitgestellt. In Kapitel 4 wurde der Aufbau anhand einer Vierpulssequenz mit Cresylviolett in Ethanol demonstriert. Es wurde ein detailliertes Datenerfassungs- und Datenanalyseverfahren vorgestellt, bei dem Phase Cycling zur Extraktion der nichtlinearen Beitr{\"a}ge verwendet wird. Abh{\"a}ngig vom Phase Cycling-Schema ist es m{\"o}glich, alle nichtlinearen Beitr{\"a}ge in einer einzigen Messung aufzudecken. Literaturbekannte Oszillationen von Cresylviolett w{\"a}hrend der Populationszeit konnten reproduziert werden. Aufgrund der Messung in einer Umgebung im Rotating Frame und einer 1 kHz Schuss-zu-Schuss Pulsinkrementierung war es m{\"o}glich, ein 2D-Spektrum f{\"u}r eine Populationszeit in 6 s zu erhalten. Eine Fehlerevaluierung hat gezeigt, dass eine zehnfache Mittelwertbildung (1 min) ausreicht, um eine mittlere quadratische Abweichung von < 0:05 gegen� uber einer 400-fachen Mittelwertbildung zu erhalten, was beweist, dass das verwendete Messschema gut geeignet ist. Die Realisierung des ersten experimentellen fluoreszenzdetektierten 2Q-2D-Experiments und der erste experimentelle Zugang zum theoretisch vorhergesagten 1Q-2Q-Beitrag wurden in Kapitel 5 vorgestellt. Zu diesem Zweck wurde eine Dreipulssequenz auf Cresylviolett in Ethanol angewendet und die experimentellen Ergebnisse wurden mit Simulationen eines einfachen Sechs-Level-Systems verglichen. Im Gegensatz zur koh{\"a}renzdetektierten 2Q-2D-Spektroskopie sind bei dem vorgestellten Aufbau keine nichtresonanten L{\"o}sungsmittelsignale und Streuungsbeitr{\"a}ge sichtbar und es ist kein zus{\"a}tzliches Phasing-Verfahren erforderlich. Durch eine Kombination aus Experimenten und systematischen Simulationen wurden Informationen {\"u}ber die Relaxation der L{\"o}sungsmittelh{\"u}lle und die Korrelationsenergie gewonnen. Auf der Basis von Simulationen wurden Effekte der Pfadausl{\"o}schung diskutiert, die darauf schließen lassen, dass die 1Q-2Q-2D-Spektroskopie m{\"o}glicherweise die quantitative Analyse f{\"u}r molekulare Systeme erleichtert, die eine starke nichtstrahlende Relaxation aus h{\"o}heren elektronischen Zust{\"a}nden aufweisen. Zusammenfassend ist es mit der vorgestellten Methode m{\"o}glich, alle nichtlinearen Beitr{\"a}ge mit einer schnellen Datenaufnahme und einem einfach einzurichtenden Aufbau zu erfassen. Die gezeigten Proof-of-Principle-Experimente stellen eine Erweiterung der 2D-Spektroskopie-Werkzeugpalette dar und bieten eine fundierte Grundlage f{\"u}r zuk{\"u}nftige Anwendungen wie mehrdimensionale Spektroskopie, mehrfarbige 2D-Spektroskopie oder die Kombination von simultanen Fl{\"u}ssig- und Gasphasen-2D-Experimenten.}, subject = {Fluoreszenzspektroskopie}, language = {en} } @unpublished{MuellerDraegerMaetal.2018, author = {M{\"u}ller, Stefan and Draeger, Simon and Ma, Kiaonan and Hensen, Matthias and Kenneweg, Tristan and Pfeiffer, Walter and Brixner, Tobias}, title = {Fluorescence-Detected Two-Quantum and One-Quantum-Two-Quantum 2D Electronic Spectroscopy}, series = {Journal of Physical Chemistry Letters}, journal = {Journal of Physical Chemistry Letters}, doi = {10.1021/acs.jpclett.8b00541}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-173468}, year = {2018}, abstract = {We demonstrate two-quantum (2Q) coherent two-dimensional (2D)electronic spectroscopy using a shot-to-shot-modulated pulse shaper and fluorescence detection. Broadband collinear excitation is realized with the supercontinuum output of an argon-filled hollow-core fiber, enabling us to excite multiple transitions simultaneously in the visible range. The 2Q contribution is extracted via a three-pulse sequence with 16-fold phase cycling and simulated employing cresyl violet as a model system. Furthermore, we report the first experimental realization of one-quantum-two-quantum (1Q-2Q) 2D spectroscopy, offering less congested spectra as compared with the 2Q implementation. We avoid scattering artifacts and nonresonant solvent contributions by using fluorescence as the observable. This allows us to extract quantitative information about doubly excited states that agree with literature expectations. The high sensitivity and background-free nature of fluorescence detection allow for a general applicability of this method to many other systems.}, subject = {Fluoreszenz}, language = {en} } @phdthesis{Rewitz2014, author = {Rewitz, Christian}, title = {Far-Field Characterization and Control of Propagating Ultrashort Optical Near Fields}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-94887}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2014}, abstract = {In this work, femtosecond laser pulses are used to launch optical excitations on different nanostructures. The excitations are confined below the diffraction limit and propagate along the nanostructures. Fundamental properties of these ultrashort optical near fields are determined by characterizing the far-field emission after propagation with a setup developed for this task. Furthermore, control of the nanooptical excitations' spatial and temporal evolution is demonstrated for a designed nanostructure.}, subject = {Nahfeldoptik}, language = {en} } @phdthesis{Kullmann2013, author = {Kullmann, Martin Armin}, title = {Tracing Excited-State Photochemistry by Multidimensional Electronic Spectroscopy}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-81276}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2013}, abstract = {Light-induced excitation of matter proceeds within femtoseconds, resulting in excited states. Originating from these states chemical reaction mechanisms, like isomerization or bond formation, set in. Photophysical mechanisms like energy distribution and excitonic delocalization also occur. Thus, the reaction scheme has to be disentangled by assessing the importance of each process. Spectroscopic methods based on fs laser pulses have emerged as a versatile tool to study these reactions. Within this thesis time-resolved experiments with fs laser pulses on various molecular systems were performed. Novel photosystems, with possible applications ranging from ultrathin molecular wires to molecular switches, were extensively characterized. To resolve the complex kinetics of the investigated systems, time-resolved techniques had to be newly developed. By combining a visible excitation pulse pair with an additional pulse and a continuum probe electronic triggered-exchange two-dimensional spectroscopy (TE2D) was demonstrated for the first time. This goal was accomplished by combining a three-color transient-absorption setup with a pulse shaper. Hence, 2D spectroscopy with a continuum probe was also implemented. Using these methods two different molecular systems in solution were characterized in a comprehensive manner. (ZnTPP)2, a directly beta,beta'-linked Zn-metallated bisporphyrin, and a spiropyran-merocyanine photosystem, 6,8-dinitro BIPS, were characterized. (ZnTPP)2 is a homodimer, featuring strong excitonic effects. These manifest themselves in a twofold splitting of the Soret band (S2). 6,8-Dinitro BIPS exists in one of two possible conformations. The ring closed spiropyran absorbs only in the UV, while the ring open merocyanine also absorbs in the visible. For both molecular systems photodynamics upon illumination were monitored using transient-absorption. However, the obtained results were ambiguous, necessitating more complex methods. In the case of (ZnTPP)2 first the monomeric building block was characterized. There, population transfer from the S2 state into S1 within 2 ps was identified. Afterwards, intersystem crossing proceeds within 2 ns. For (ZnTPP)2 similar pathways were found, albeit the relaxation is faster. The intersystem crossing with 1.5 ns was not only indirectly deduced but directly measured by probing in the NIR spectral range. The excitonic influence of was investigated by coherent 2D spectroscopy in the Soret band. Population transfer within S2 was directly visualized on a time-scale of 100 fs. Calculation of the 2D spectra of a simple homodimer confirmed the results. After this analysis of the distinct excitonic character, this molecule may serve as a building block for larger porphyrin arrays with applications ranging from asymmetric catalysis over biomimicry of electron-transfer to organic optical devices. The second photosystem was the molecular switch 6,8-dinitro BIPS, existing in two conformations. Merocyanine is the more stable form in thermal equilibrium. Transient-absorption measurements uncovered that the sample consisted of a mixture of two merocyanine isomers, referred to as TTC and TTT. However, both isomers are capable of ring-closure forming spiropyran. The remaining excited molecules return to the ground state radiatively. Conducting 2D measurements utilizing a continuum probe the differing photochemistry of both isomers was examined in a single measurement. No isomerization between these conformations was detected. Therefore, 6,8-dinitro BIPS performs a concerted switching without long-living intermediates. This was confirmed by a pump-repump-probe scan. 6,8-DinitroBIPS can be closed by visible and opened by UV pulses using subsequent pulses and vice versa. These mechanisms via singlet pathways satisfy an important criterion for a unimolecular switching device. A second pump-repump-probe experiment showed that the sample is ionized, resulting in a merocyanine radical cation, when the first excited state is resonantly excited. Furthermore, by implementing TE2Dspectroscopy, it was elucidated that only TTC was ionized. Taking all this into account new techniques were developed and complex molecular systems were characterized within this thesis. Deeper insight into the photodynamics of (ZnTPP)2and 6,8-dinitro BIPS was gained by adapting transient absorption for the NIR spectral range, constructing a 2D setup in pump-probe geometry, and combining it with multipulse excitation to coherent TE2D. All techniques solved the questions for which they were constructed, but they are not limited to these cases. Especially TE2D opens new roads in photochemistry. By connecting reactant, product and the corresponding intermediates, a chemical reaction can be tracked through all stages, making unambiguous identification of the reactive states feasible. Thus, fundamental insight into the photochemistry of molecular compounds is gained.}, subject = {Femtosekundenspektroskopie}, language = {en} } @phdthesis{Quast2012, author = {Quast, Tatjana}, title = {Spectroscopic investigation of charge-transfer processes and polarisation pulse shaping in the visible spectral range}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-74265}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2012}, abstract = {The first part deals with the spectroscopic investigation of ultrafast light-induced charge-transfer processes in different molecular compounds. In the second part, the question of the generation and characterisation of broadband visible polarisation-shaped laser pulses is treated.}, subject = {Polarisiertes Licht}, language = {en} } @phdthesis{Tuchscherer2012, author = {Tuchscherer, Philip}, title = {A Route to Optical Spectroscopy on the Nanoscale}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-72228}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2012}, abstract = {Time-resolved optical spectroscopy has become an important tool to investigate the dynamics of quantum mechanical processes in matter. In typical applications, a first "pump" pulse excites the system under investigation from the thermal equilibrium to an excited state, and a second variable time-delayed "probe" pulse then maps the dynamics of the excited system. Although advanced nonlinear techniques have been developed to investigate, e.g., coherent quantum effects, all of these techniques are limited in their spatial resolution. The laser focus diameter has a lower bound given by Abbe's diffraction limit, which is roughly half the optical excitation wavelength—corresponding to about 400nm in the presented experiments. In the time-resolved experiments that have been suggested so far, averaging over the sample volume within this focus cannot be avoided. In this thesis, two approaches were developed to overcome the diffraction limit in optical spectroscopy and to enable the investigation of coherent processes on the nanoscale. In the first approach, analytic solutions were found to calculate optimal polarizationshaped laser pulses that provide optical near-field pump-probe pulse sequences in the vicinity of a nanostructure. These near-field pulse sequences were designed to allow excitation of a quantum system at one specific position at a certain time and probing at a different position at a later time. In the second approach, the concept of coherent two-dimensional (2D) spectroscopy, which has had great impact on the investigation of coherent quantum effects in recent years, was combined with photoemission electron microscopy, which yields a spatial resolution well below the optical diffraction limit. Using the analytic solutions, optical near fields were investigated in terms of spectroscopic applications. Near fields that are excited with polarization-shaped femtosecond laser pulses in the vicinity of appropriate nanostructures feature two properties that are especially interesting in the view of spectroscopic applications: On the one hand, control of the spatial distribution of the optical fields is achieved on the order of nanometers. On the other hand, the temporal evolution of these fields can be adjusted on the order of femtoseconds. In this thesis, solutions were found to calculate the optimal polarizationshaped laser pulses that control the near field in a general manner. The main idea to achieve this deterministic control was to disentangle the spatial and temporal near-field control. First, the spatial distribution of the optical near field was controlled by assigning the correct state of polarization for each frequency within the polarization-shaped laser pulse independently. The remaining total phase—not employed for spatial control—was then used for temporal near-field compression, which, in experimental applications, would lead to an enhancement of the nonlinear signal at the respective location. In contrast to the use of optical near fields, where pump-probe sequences themselves are localized below the diffraction limit and the detection does not have to provide the spatial resolution, a different approach was suggested in this thesis to gain spectroscopic information on the nanoscale. The new method was termed "Coherent two-dimensional (2D) nanoscopy" and transfers the concept of "conventional" coherent 2D spectroscopy to photoemission electron microscopy. The pulse sequences used for the investigation of quantum systems in this method are still limited by diffraction. However, the new key concept is to detect locally generated photoelectrons instead of optical signals. This yields a spatial resolution that is well below the optical diffraction limit. In "conventional" 2D spectroscopy a triple-pulse sequence initiates a four wave mixing process that creates a coherence. In a quantum mechanical process, this coherence is converted into a population by emission of an electric field, which is measured in the experiment. Contrarily, in the developed 2D nanoscopy, four-wave mixing is initiated by a quadruple-pulse sequence, which leaves the quantum system in an electronic population. This electronic population carries coherent information about the investigated quantum system and can be mapped with a spatial resolution down to a few nanometers given by the spatial resolution of the photoemission electron microscope. Hence, 2D nanoscopy can be considered a generalization of time-resolved photoemission experiments. In the future, it may be of similar beneficial value for the field of photoemission research as "conventional" 2D spectroscopy has proven to be for optical spectroscopy and nuclear magnetic resonance experiments. In a first experimental implementation of coherent 2D nanoscopy coherent processes on a corrugated silver surface were measured and unexpected long coherence lifetimes could be determined.}, subject = {Ultrakurzzeitspektroskopie}, language = {en} }