@phdthesis{Goetz2019, author = {G{\"o}tz, Sebastian Reinhold}, title = {Nonlinear spectroscopy at the diffraction limit: probing ultrafast dynamics with shaped few-cycle laser pulses}, doi = {10.25972/OPUS-19213}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-192138}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2019}, abstract = {An experimental setup for probing ultrafast dynamics at the diffraction limit was developed, characterized and demonstrated in the scope of the thesis, aiming for optical investigations while simultaneously approaching the physical limits on the length and timescale. An overview of this experimental setup was given in Chapter 2, as well as the considerations that led to the selection of the individual components. Broadband laser pulses with a length of 9.3 fs, close to the transform limit of 7.6 fs, were focused in a NA = 1.4 immersion oil objective, to the diffraction limit of below 300 nm (FWHM). The spatial focus shape was characterized with off-resonance gold nanorod scatterers scanned through the focal volume. For further insights into the functionality and limitations of the pulse shaper, its calibration procedure was reviewed. The deviations between designed and experimental pulse shapes were attributed to pulse-shaper artifacts, including voltage-dependent inter-layer as well as intra-layer LCD-pixel crosstalk, Fabry-P{\´e}rot-type reflections in the LCD layers, and space-time coupling. A pixel-dependent correction was experimentally carried out, which can be seen as an extension of the initial calibration to all possible voltage combinations of the two LCD layers. The capabilities of the experimental setup were demonstrated in two types of experiments, targeting the nonlinearity of gold (Chapter 3) as well as two-dimensional spectroscopy at micro-structured surfaces (Chapter 4). Investigating thin films, an upper bound for the absolute value for the imaginary part of the nonlinear refractive index of gold could be set to |n′′ 2 (Au)| < 0.6·10-16 m2/W, together with |n′ 2 (Au)| < 1.2·10-16 m2/W as an upper bound for the absolute value of the real part. Finite-difference time-domain simulations on y-shaped gold nanostructures indicated that a phase change of ∆Φ ≥ 0.07 rad between two plasmonic modes would induce a sufficient change in the spatial contrast of emission to the far-field to be visible in the experiment. As the latter could not be observed, this value of ∆Φ was determined as the upper bound for the experimentally induced phase change. An upper bound of 52 GW/cm2 was found for the damage threshold. In Chapter 4, a novel method for nonlinear spectroscopy on surfaces was presented. Termed coherent two-dimensional fluorescence micro-spectroscopy, it is capable of exploring ultrafast dynamics in nanostructures and molecular systems at the diffraction limit. Two-dimensional spectra of spatially isolated hotspots in structured thin films of fluorinated zinc phthalocyanine (F16ZnPc) dye were taken with a 27-step phase-cycling scheme. Observed artifacts in the 2D maps were identified as a consequence from deviations between the desired and the experimental pulse shapes. The optimization procedures described in Chapter 2 successfully suppressed the deviations to a level where the separation from the nonlinear sample response was feasible. The experimental setup and methods developed and presented in the scope of this thesis demonstrate its flexibility and capability to study microscopic systems on surfaces. The systems exemplarily shown are consisting of metal-organic dyes and metallic nanostructures, represent samples currently under research in the growing fields of organic semiconductors and plasmonics.}, subject = {Ultrakurzzeitspektroskopie}, language = {en} } @phdthesis{Schmitt2017, author = {Schmitt, Hans-Christian}, title = {Deaktivierungsprozesse in isolierten aromatischen Heterocyclen und Pyrenen}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-155445}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2017}, abstract = {In der vorliegenden Arbeit wurde erfolgreich eine neue Gasphasen-Apparatur f{\"u}r Photoelektronen-Imaging-Experimente simuliert, aufgebaut und in Verbindung mit einem ps-Lasersystem in Betrieb genommen. Neben dem Aufbau der Apparatur stand die Aufkl{\"a}rung der Dynamik angeregter Zust{\"a}nde von aromatischen Heterocyclen und Pyrenen im Fokus dieser Arbeit. Die untersuchten Molek{\"u}le wurden durch Resonanzverst{\"a}rkte Mehrphotonenionisation in einem Molekularstrahlexperiment sowohl zeit-, als auch frequenzaufgel{\"o}st untersucht.}, subject = {Laserspektroskopie}, language = {de} } @phdthesis{Kramer2017, author = {Kramer, Christian}, title = {Investigation of Nanostructure-Induced Localized Light Phenomena Using Ultrafast Laser Spectroscopy}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-150681}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2017}, abstract = {In recent years, the interaction of light with subwavelength structures, i.e., structures that are smaller than the optical wavelength, became more and more interesting to scientific research, since it provides the opportunity to manipulate light-induced dynamics below the optical diffraction limit. Specifically designed nanomaterials can be utilized to tailor the temporal evolution of electromagnetic fields at the nanoscale. For the investigation of strongly localized processes, it is essential to resolve both their spatial and their temporal behavior. The aim of this thesis was to study and/or control the temporal evolution of three nanostructure-induced localized light phenomena by using ultrafast laser spectroscopy with high spatial resolution. In Chapter 4, the absorption of near-infrared light in thin-film a-Si:H solar cells was investigated. Using nanotextured instead of smooth interfaces for such devices leads to an increase of absorption from < 20\% to more than 50\% in the near-infrared regime. Time-resolved experiments with femtosecond laser pulses were performed to clarify the reason for this enhancement. The coherent backscattered radiation from nanotextured solar cell devices was measured as a function of the sample position and evaluated via spectral interferometry. Spatially varying resonance peaks in the recorded spectra indicated the formation of localized photonic modes within the nanotextured absorber layers. In order to identify the modes separately from each other, coherent two-dimensional (2D) nanoscopy was utilized, providing a high spatial resolution < 40 nm. In a nanoscopy measurement on a modified device with an exposed nanotextured a-Si:H absorber layer, hot-spot electron emission was observed and confirmed the presence of localized modes. Fitting the local 2D nanospectra at the hot-spot positions enabled the determination of the resonance frequencies and coherence lifetimes of the modes. The obtained lifetime values varied between 50 fs and 130 fs. Using a thermionic emission model allowed the calculation of the locally absorbed energy density and, with this, an estimation of the localization length of the photonic modes (≈1 μm). The localization could be classified by means of the estimated localization length and additional data evaluation of the backscattered spectra as strong localization ─ the so-called Anderson localization. Based on the experimental results, it was concluded that the enhanced absorption of near-infrared light in thin-film silicon solar cells with nanotextured interfaces is caused by the formation of strongly localized photonic modes within the disordered absorber layers. The incoming near-infrared light is trapped in these long-living modes until absorption occurs. In Chapter 5, a novel hybridized plasmonic device was introduced and investigated in both theory and experiment. It consists of two widely separated whispering gallery mode (WGM) nanoantennas located in an elliptical plasmonic cavity. The goal was to realize a periodic long-range energy transfer between the nanoantennas. In finite-difference time-domain (FDTD) simulations, the device was first optimized with respect to strong coupling between the localized antenna modes and the spatially-extended cavity mode. The geometrical parameters of the antennas and the cavity were adjusted separately so that the m="0" antenna mode and the cavity mode were resonant at λ="800 nm" . A high spatial overlap of the modes was achieved by positioning the two antennas in the focal spots of the cavity, leading to a distance between the antenna centers of more than twice the resonant wavelength of the modes. The spectral response of the optimized device revealed an energy splitting of the antenna and the cavity mode into three separated hybridized eigenmodes within an energy range of about 90 meV due to strong coupling. It could be well reproduced by a simple model of three coupled Lorentzian oscillators. In the time domain, an oscillatory energy transfer between both antennas with a period of 86 fs and an energy transfer efficiency of about 7\% was observed for single-pulse excitation. For the experiments, devices with cavities and antennas of varying size were fabricated by means of focused-ion-beam (FIB) milling. Time-resolved correlation measurements were performed with high spatial and temporal resolution by using sequences of two femtosecond laser pulses for excitation and photoemission electron microscopy (PEEM) for detection. Local correlation traces at antennas in resonant devices, i.e., devices with enhanced electron emission at both antenna positions, were investigated and reconstructed by means of the coupled-oscillator model. The corresponding spectral response revealed separated peaks, confirming the formation of hybridized eigenmodes due to strong coupling. In a subsequent simulation for single-pulse excitation, one back-and-forth energy transfer between both antennas with an energy transfer efficiency of about 10\% was observed. Based on the theoretical and experimental results, it was demonstrated that in the presented plasmonic device a periodic long-range energy transfer between the two nanoantennas is possible. Furthermore, the coupled-oscillator model enables one to study in depth how specific device properties impact the temporal electric-field dynamics within the device. This can be exploited to further optimize energy transfer efficiency of the device. Future applications are envisioned in ultrafast plasmonic nanocircuitry. Moreover, the presented device can be employed to realize efficient SPP-mediated strong coupling between widely separated quantum emitters. In Chapter 6, it was investigated in theory how the local optical chirality enhancement in the near field of plasmonic nanostructures can be optimized by tuning the far-field polarization of the incident light. An analytic expression was derived that enables the calculation of the optimal far-field polarizations, i.e., the two far-field polarizations which lead to the highest positive and negative local optical chirality, for any given nanostructure geometry. The two optimal far-field polarizations depend on the local optical response of the respective nanostructure and thus are functions of both the frequency ω and the position r. Their ellipticities differ only in their sign, i.e., in their direction of rotation in the time domain, and the angle between their orientations, i.e., the angle between the principal axes of their ellipses, is ±π/"2" . The handedness of optimal local optical chirality can be switched by switching between the optimal far-field polarizations. In numerical simulations, it was exemplarily shown for two specific nanostructure assemblies that the optimal local optical chirality can significantly exceed the optical chirality values of circularly polarized light in free space ─ the highest possible values in free space. The corresponding optimal far-field polarizations were different from linear and circular and varied with frequency. Using femtosecond polarization pulse shaping provides the opportunity to coherently control local optical chirality over a continuous frequency range. Furthermore, symmetry properties of nanostructures can be exploited to determine which far-field polarization is optimal. The theoretical findings can have impact on future experimental studies about local optical chirality enhancement. Tuning the far-field polarization of the incident light offers a promising tool to enhance chirally specific interactions of local electromagnetic fields with molecular and other quantum systems in the vicinity of plasmonic nanostructures. The presented approach can be utilized for applications in chiral sensing of adsorbed molecules, time-resolved chirality-sensitive spectroscopy, and chiral quantum control. In conclusion, each of the localized light phenomena that were investigated in this thesis ─ the enhanced local absorption of near-infrared light due to the formation of localized photonic modes, the periodic long-range energy transfer between two nanoantennas within an elliptical plasmonic cavity, and the optimization of local optical chirality enhancement by tuning the far-field polarization of the incident light ─ can open up new perspectives for a variety of future applications. .}, subject = {Ultrakurzzeitspektroskopie}, language = {en} } @article{WohlgemuthMiyazakiTsukadaetal.2017, author = {Wohlgemuth, Matthias and Miyazaki, Mitsuhiko and Tsukada, Kohei and Weiler, Martin and Dopfer, Otto and Fujii, Masaaki and Mitrić, Roland}, title = {Deciphering environment effects in peptide bond solvation dynamics by experiment and theory}, series = {Physical Chemistry Chemical Physics}, volume = {19}, journal = {Physical Chemistry Chemical Physics}, number = {33}, doi = {10.1039/C7CP03992A}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159647}, pages = {22564-22572}, year = {2017}, abstract = {Most proteins work in aqueous solution and the interaction with water strongly affects their structure and function. However, experimentally the motion of a specific single water molecule is difficult to trace by conventional methods, because they average over the heterogeneous solvation structure of bulk water surrounding the protein. Here, we provide a detailed atomistic picture of the water rearrangement dynamics around the -CONH- peptide linkage in the two model systems formanilide and acetanilide, which simply differ by the presence of a methyl group at the peptide linkage. The combination of picosecond pump-probe time-resolved infrared spectroscopy and molecular dynamics simulations demonstrates that the solvation dynamics at the molecular level is strongly influenced by this small structural difference. The effective timescales for solvent migration triggered by ionization are mainly controlled by the efficiency of the kinetic energy redistribution rather than the shape of the potential energy surface. This approach provides a fundamental understanding of protein hydration and may help to design functional molecules in solution with tailored properties.}, language = {en} } @unpublished{HocheSchmittHumeniuketal.2017, author = {Hoche, Joscha and Schmitt, Hans-Christian and Humeniuk, Alexander and Fischer, Ingo and Mitrić, Roland and R{\"o}hr, Merle I. S.}, title = {The mechanism of excimer formation: an experimental and theoretical study on the pyrene dimer}, series = {Physical Chemistry Chemical Physics}, journal = {Physical Chemistry Chemical Physics}, doi = {10.1039/C7CP03990E}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159656}, year = {2017}, abstract = {The understanding of excimer formation in organic materials is of fundamental importance, since excimers profoundly influence their functional performance in applications such as light-harvesting, photovoltaics or organic electronics. We present a joint experimental and theoretical study of the ultrafast dynamics of excimer formation in the pyrene dimer in a supersonic jet, which is the archetype of an excimer forming system. We perform simulations of the nonadiabatic photodynamics in the frame of TDDFT that reveal two distinct excimer formation pathways in the gas-phase dimer. The first pathway involves local excited state relaxation close to the initial Franck-Condon geometry that is characterized by a strong excitation of the stacking coordinate exhibiting damped oscillations with a period of 350 fs that persist for several picoseconds. The second excimer forming pathway involves large amplitude oscillations along the parallel shift coordinate with a period of ≈900 fs that after intramolecular vibrational energy redistribution leads to the formation of a perfectly stacked dimer. The electronic relaxation within the excitonic manifold is mediated by the presence of intermolecular conical intersections formed between fully delocalized excitonic states. Such conical intersections may generally arise in stacked π-conjugated aggregates due to the interplay between the long-range and short-range electronic coupling. The simulations are supported by picosecond photoionization experiments in a supersonic jet that provide a time-constant for the excimer formation of around 6-7 ps, in good agreement with theory. Finally, in order to explore how the crystal environment influences the excimer formation dynamics we perform large scale QM/MM nonadiabatic dynamics simulations on a pyrene crystal in the framework of the long-range corrected tight-binding TDDFT. In contrast to the isolated dimer, the excimer formation in the crystal follows a single reaction pathway in which the initially excited parallel slip motion is strongly damped by the interaction with the surrounding molecules leading to the slow excimer stabilization on a picosecond time scale.}, language = {en} } @phdthesis{Albert2018, author = {Albert, Julian}, title = {Quantum Studies on Low-Dimensional Coupled Electron-Nuclear Dynamics}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-161512}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2018}, abstract = {In the context of quantum mechanical calculations, the properties of non-adiabatic coupling in a small system, the Shin-Metiu model, is investigated. The transition from adiabatic to non-adiabatic dynamics is elucidated in modifying the electron-nuclear interaction. This allows the comparison of weakly correlated electron-nuclear motion with the case where the strong correlations determine the dynamics. The studies of the model are extended to include spectroscopical transitions being present in two-dimensional and degenerate four-wave mixing spectroscopy. Furthermore, the quantum and classical time-evolution of the coupled motion in the complete electron-nuclear phase space is compared for the two coupling cases. Additionally, the numerically exact electron flux within the weak coupling case is compared to the Born-Oppenheimer treatment. In the last part of the thesis, the model is extended to two dimensions. The system then possesses potential energy surfaces which exhibit a typical 'Mexican hat'-like structure and a conical intersection in the adiabatic representation. Thus, it is possible to map properties of the system onto a vibronic coupling (Jahn-Teller) hamiltonian. Exact wave-packet propagations as well as nuclear wave-packet dynamics in the adiabatic and diabatic representation are performed.}, subject = {Theoretische Chemie}, language = {en} } @article{KnorrSokkarSchottetal.2016, author = {Knorr, Johannes and Sokkar, Pandian and Schott, Sebastian and Costa, Paolo and Thiel, Walter and Sander, Wolfram and Sanchez-Garcia, Elsa and Nuernberger, Patrick}, title = {Competitive solvent-molecule interactions govern primary processes of diphenylcarbene in solvent mixtures}, series = {Nature Communications}, volume = {7}, journal = {Nature Communications}, doi = {10.1038/ncomms12968}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-165954}, pages = {12968}, year = {2016}, abstract = {Photochemical reactions in solution often proceed via competing reaction pathways comprising intermediates that capture a solvent molecule. A disclosure of the underlying reaction mechanisms is challenging due to the rapid nature of these processes and the intricate identification of how many solvent molecules are involved. Here combining broadband femtosecond transient absorption and quantum mechanics/molecular mechanics simulations, we show for one of the most reactive species, diphenylcarbene, that the decision-maker is not the nearest solvent molecule but its neighbour. The hydrogen bonding dynamics determine which reaction channels are accessible in binary solvent mixtures at room temperature. In-depth analysis of the amount of nascent intermediates corroborates the importance of a hydrogen-bonded complex with a protic solvent molecule, in striking analogy to complexes found at cryogenic temperatures. Our results show that adjacent solvent molecules take the role of key abettors rather than bystanders for the fate of the reactive intermediate.}, language = {en} } @phdthesis{Roeder2017, author = {R{\"o}der, Anja M.}, title = {Excited-State Dynamics in Open-Shell Molecules}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-151738}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2017}, abstract = {In this thesis the excited-state dynamics of radicals and biradicals were characterized with femtosecond pump-probe spectroscopy. These open-shell molecules play important roles as combustion intermediates, in the formation of soot and polycyclic aromatic hydrocarbons, in atmospheric chemistry and in the formation of complex molecules in the interstellar medium and galactic clouds. In these processes molecules frequently occur in some excited state, excited either by thermal energy or radiation. Knowledge of the reactivity and dynamics of these excited states completes our understanding of these complex processes. These highly reactive molecules were produced via pyrolysis from suitable precursors and examined in a molecular beam under collision-free conditions. A first laser now excites the molecule, and a second laser ionizes it. Time-of-flight mass spectrometry allowed a first identification of the molecule, photoelectron spectroscopy a complete characterization of the molecule - under the condition that the mass spectrum was dominated by only one mass. The photoelectron spectrum was obtained via velocity-map imaging, providing an insight in the electronic states involved. Ion velocity map imaging allowed separation of signal from direct ionization of the radical in the molecular beam and dissociative photoionization of the precursor. During this thesis a modified pBasex algorithm was developed and implemented in python, providing an image inversion tool without interpolation of data points. Especially for noisy photoelectron images this new algorithm delivers better results. Some highlighted results: • The 2-methylallyl radical was excited in the ππ*-state with different internal energies using three different pump wavelengths (240.6 , 238.0 and 236.0 nm). Ionized with 800 nm multi-photon probe, the photoelectron spectra shows a s-Rydberg fingerprint spectrum, a highly positive photoelectron anisotropy of 1.5 and a bi-exponential decay ( τ1= 141\pm43 fs, τ2= 4.0\pm0.2 ps for 240.6 nm pump), where the second time-constant shortens for lower wavelengths. Field-induced surface hopping dynamics calculations confirm that the initially excited ππ*-state relaxes very fast to an s-Rydberg state (first experimentally observed time-constant), and then more slowly to the first excited state/ground state (second time-constant). With higher excitation energies the conical intersection between the s-Rydberg-state and the first excited state is reached faster, resulting in shorter life-times. • The benzyl radical was excited yith 265 nm and probed with two wavelengths, 798 nm and 398 nm. Probed with 798 nm it shows a bi-exponential decay (\tau_{1}=84\pm5 fs, \tau_{2}=1.55\pm0.12 ps), whereas with 398 nm probe only the first time-constant is observed (\tau_{1}=89\pm5 fs). The photoelectron spectra with 798 nm probe is comparable to the spectrum with 398 nm probe during the first 60 fs, at longer times an additional band appears. This band is due to a [1+3']-process, whereas with 398 nm only signal from a [1+1']-process can be observed. Non-adiabatic dynamic on the fly calculations show that the initially excited, nearly degenerate ππ/p-Rydberg-states relax very fast (first time-constant) to an s-Rydberg state. This s-Rydberg state can no longer be ionized with 398 nm, but with 798 nm ionization via intermediate resonances is still possible. The s-Rydberg state then decays to the first excited state (second time-constant), which is long-lived. • Para-xylylene, excited with 266 nm into the S2-state and probed with 800 nm, shows a bi-exponential decay (\tau_{1}=38\pm7 fs, \tau_{2}=407\pm9 fs). The initially excited S2-state decays quickly to S1-state, which shows dissociative photoionization. The population of the S1-state is directly visible in the masses of the dissociative photoionization products, benzene and the para-xylylene -H. • Ortho-benzyne, produced via pyrolysis from benzocyclobutendione, was excited with 266 nm in the S2 state and probed with 800 nm. In its time-resolved mass spectra the dynamic of the ortho-benzyne signal was superposed with the dynamics from dissociative photoionization of the precursor and of the ortho-benzyne-dimer. With time-resolved ion imaging gated on the ortho-benzyne these processes could be seperated, showing that the S2-state of ortho-benzyne relaxes within 50 fs to the S1-state.}, subject = {Radikal }, language = {en} } @unpublished{BoehnkeDellermannCeliketal.2018, author = {B{\"o}hnke, Julian and Dellermann, Theresa and Celik, Mehmet Ali and Krummenacher, Ivo and Dewhurst, Rian D. and Demeshko, Serhiy and Ewing, William C. and Hammond, Kai and Heß, Merlin and Bill, Eckhard and Welz, Eileen and R{\"o}hr, Merle I. S. and Mitric, Roland and Engels, Bernd and Meyer, Franc and Braunschweig, Holger}, title = {Isolation of diradical products of twisted double bonds}, series = {Nature Communications}, journal = {Nature Communications}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-160248}, year = {2018}, abstract = {Molecules containing multiple bonds between atoms—most often in the form of olefins—are ubiquitous in nature, commerce, and science, and as such have a huge impact on everyday life. Given their prominence, over the last few decades, frequent attempts have been made to perturb the structure and reactivity of multiply-bound species through bending and twisting. However, only modest success has been achieved in the quest to completely twist double bonds in order to homolytically cleave the associated π bond. Here, we present the isolation of double-bond-containing species based on boron, as well as their fully twisted diradical congeners, by the incorporation of attached groups with different electronic properties. The compounds comprise a structurally authenticated set of diamagnetic multiply-bound and diradical singly-bound congeners of the same class of compound.}, language = {en} } @article{LisinetskayaBraunProchetal.2016, author = {Lisinetskaya, Polina and Braun, Christian and Proch, Sebastian and Kim, Young Dok and Gantef{\"o}r, Gerd and Mitrić, Roland}, title = {Excited state nonadiabatic dynamics of bare and hydrated anionic gold clusters Au\(^-_3\)[H\(_2\)O]\(_n\) (n=0-2)}, series = {Physical Chemistry Chemical Physics}, volume = {18}, journal = {Physical Chemistry Chemical Physics}, number = {9}, issn = {1463-9076}, doi = {10.1039/c5cp04297f}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159176}, pages = {6411-6419}, year = {2016}, abstract = {We present a joint theoretical and experimental study of excited state dynamics in pure and hydrated anionic gold clusters Au\(^-_3\)[H\(_2\)O]\(_n\) (n = 0-2). We employ mixed quantum-classical dynamics combined with femtosecond time-resolved photoelectron spectroscopy in order to investigate the influence of hydration on excited state lifetimes and photo-dissociation dynamics. A gradual decrease of the excited state lifetime with the number of adsorbed water molecules as well as gold cluster fragmentation quenching by two or more water molecules are observed both in experiment and in simulations. Non-radiative relaxation and dissociation in excited states are found to be responsible for the excited state population depletion. Time constants of these two processes strongly depend on the number of water molecules leading to the possibility to modulate excited state dynamics and fragmentation of the anionic cluster by adsorption of water molecules.}, language = {en} } @article{LisinetskayaRoehrMitrić2016, author = {Lisinetskaya, Polina and R{\"o}hr, Merle I. S. and Mitrić, Roland}, title = {First-principles simulation of light propagation and exciton dynamics in metal cluster nanostructures}, series = {Applied Physics B}, volume = {122}, journal = {Applied Physics B}, number = {6}, issn = {0946-2171}, doi = {10.1007/s00340-016-6436-6}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159193}, pages = {175}, year = {2016}, abstract = {We present a theoretical approach for the simulation of the electric field and exciton propagation in ordered arrays constructed of molecular-sized noble metal clusters bound to organic polymer templates. In order to describe the electronic coupling between individual constituents of the nanostructure we use the ab initio parameterized transition charge method which is more accurate than the usual dipole-dipole coupling. The electronic population dynamics in the nanostructure under an external laser pulse excitation is simulated by numerical integration of the time-dependent Schrodinger equation employing the fully coupled Hamiltonian. The solution of the TDSE gives rise to time-dependent partial point charges for each subunit of the nanostructure, and the spatio-temporal electric field distribution is evaluated by means of classical electrodynamics methods. The time-dependent partial charges are determined based on the stationary partial and transition charges obtained in the framework of the TDDFT. In order to treat large plasmonic nanostructures constructed of many constituents, the approximate self-consistent iterative approach presented in (Lisinetskaya and Mitric in Phys Rev B 89:035433, 2014) is modified to include the transition-charge-based interaction. The developed methods are used to study the optical response and exciton dynamics of Ag-3(+) and porphyrin-Ag-4 dimers. Subsequently, the spatio-temporal electric field distribution in a ring constructed of ten porphyrin-Ag-4 subunits under the action of circularly polarized laser pulse is simulated. The presented methodology provides a theoretical basis for the investigation of coupled light-exciton propagation in nanoarchitectures built from molecular size metal nanoclusters in which quantum confinement effects are important.}, language = {en} } @article{WohlgemuthMitric2016, author = {Wohlgemuth, Matthias and Mitric, Roland}, title = {Photochemical Chiral Symmetry Breaking in Alanine}, series = {Journal of Physical Chemistry A}, volume = {45}, journal = {Journal of Physical Chemistry A}, number = {120}, doi = {10.1021/acs.jpca.6b07611}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-158557}, pages = {8976-8982}, year = {2016}, abstract = {We introduce a general theoretical approach for the simulation of photochemical dynamics under the influence of circularly polarized light to explore the possibility of generating enantiomeric enrichment through polarized-light-selective photochemistry. The method is applied to the simulation of the photolysis of alanine, a prototype chiral amino acid. We show that a systematic enantiomeric enrichment can be obtained depending on the helicity of the circularly polarized light that induces the excited-state photochemistry of alanine. By analyzing the patterns of the photoinduced fragmentation of alanine we find an inducible enantiomeric enrichment up to 1.7\%, which is also in good correspondence to the experimental findings. Our method is generally applicable to complex systems and might serve to systematically explore the photochemical origin of homochirality.}, language = {en} } @unpublished{PetersenLindnerMitric2018, author = {Petersen, Jens and Lindner, Joachim O. and Mitric, Roland}, title = {Ultrafast Photodynamics of Glucose}, series = {Journal of Physical Chemistry B}, journal = {Journal of Physical Chemistry B}, doi = {10.1021/acs.jpcb.7b08602}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159155}, year = {2018}, abstract = {We have investigated the photodynamics of \(\beta\)-D-glucose employing our field-induced surface hopping method (FISH), which allows us to simulate the coupled electron-nuclear dynamics, including explicitly nonadiabatic effects and light-induced excitation. Our results reveal that from the initially populated S\(_{1}\) and S\(_{2}\) states, glucose returns nonradiatively to the ground state within about 200 fs. This takes place mainly via conical intersections (CIs) whose geometries in most cases involve the elongation of a single O-H bond, while in some instances ring-opening due to dissociation of a C-O bond is observed. Experimentally, excitation to a distinct excited electronic state is improbable due to the presence of a dense manifold of states bearing similar oscillator strengths. Our FISH simulations explicitly including a UV laser pulse of 6.43 eV photon energy reveals that after initial excitation the population is almost equally spread over several close-lying electronic states. This is followed by a fast nonradiative decay on the time scale of 100-200 fs, with the final return to the ground state proceeding via the S\(_{1}\) state through the same types of CIs as observed in the field-free simulations.}, language = {en} } @article{HocheSchmittHumeniuketal.2017, author = {Hoche, Joscha and Schmitt, Hans-Christian and Humeniuk, Alexander and Fischer, Ingo and Mitrić, Roland and R{\"o}hr, Merle I. S.}, title = {The mechanism of excimer formation: an experimental and theoretical study on the pyrene dimer}, series = {Physical Chemistry Chemical Physics}, volume = {19}, journal = {Physical Chemistry Chemical Physics}, number = {36}, doi = {10.1039/C7CP03990E}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159514}, pages = {25002-25015}, year = {2017}, abstract = {The understanding of excimer formation in organic materials is of fundamental importance, since excimers profoundly influence their functional performance in applications such as light-harvesting, photovoltaics or organic electronics. We present a joint experimental and theoretical study of the ultrafast dynamics of excimer formation in the pyrene dimer in a supersonic jet, which is the archetype of an excimer forming system. We perform simulations of the nonadiabatic photodynamics in the frame of TDDFT that reveal two distinct excimer formation pathways in the gas-phase dimer. The first pathway involves local excited state relaxation close to the initial Franck-Condon geometry that is characterized by a strong excitation of the stacking coordinate exhibiting damped oscillations with a period of 350 fs that persist for several picoseconds. The second excimer forming pathway involves large amplitude oscillations along the parallel shift coordinate with a period of ≈900 fs that after intramolecular vibrational energy redistribution leads to the formation of a perfectly stacked dimer. The electronic relaxation within the excitonic manifold is mediated by the presence of intermolecular conical intersections formed between fully delocalized excitonic states. Such conical intersections may generally arise in stacked π-conjugated aggregates due to the interplay between the long-range and short-range electronic coupling. The simulations are supported by picosecond photoionization experiments in a supersonic jet that provide a time-constant for the excimer formation of around 6-7 ps, in good agreement with theory. Finally, in order to explore how the crystal environment influences the excimer formation dynamics we perform large scale QM/MM nonadiabatic dynamics simulations on a pyrene crystal in the framework of the long-range corrected tight-binding TDDFT. In contrast to the isolated dimer, the excimer formation in the crystal follows a single reaction pathway in which the initially excited parallel slip motion is strongly damped by the interaction with the surrounding molecules leading to the slow excimer stabilization on a picosecond time scale.}, language = {en} } @unpublished{LambertVoelkerKochetal.2015, author = {Lambert, Christoph and V{\"o}lker, Sebastian F. and Koch, Federico and Schmiedel, Alexander and Holzapfel, Marco and Humeniuk, Alexander and R{\"o}hr, Merle I. S. and Mitric, Roland and Brixner, Tobias}, title = {Energy Transfer Between Squaraine Polymer Sections: From helix to zig-zag and All the Way Back}, series = {Journal of the American Chemical Society}, journal = {Journal of the American Chemical Society}, doi = {10.1021/jacs.5b03644}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159607}, year = {2015}, abstract = {Joint experimental and theoretical study of the absorption spectra of squaraine polymers in solution provide evidence that two different conformations are present in solution: a helix and a zig-zag structure. This unique situation allows investigating ultrafast energy transfer processes between different structural segments within a single polymer chain in solution. The understanding of the underlying dynamics is of fundamental importance for the development of novel materials for light-harvesting and optoelectronic applications. We combine here femtosecond transient absorption spectroscopy with time-resolved 2D electronic spectroscopy showing that ultrafast energy transfer within the squaraine polymer chains proceeds from initially excited helix segments to zig-zag segments or vice versa, depending on the solvent as well as on the excitation wavenumber. These observations contrast other conjugated polymers such as MEH-PPV where much slower intrachain energy transfer was reported. The reason for the very fast energy transfer in squaraine polymers is most likely a close matching of the density of states between donor and acceptor polymer segments because of very small reorganization energy in these cyanine-like chromophores.}, language = {en} } @article{RoehrLisinetskayaMitric2016, author = {R{\"o}hr, Merle I. S. and Lisinetskaya, Polina G. and Mitric, Roland}, title = {Excitonic Properties of Ordered Metal Nanocluster Arrays: 2D Silver Clusters at Multiporphyrin Templates}, series = {Journal of Physical Chemistry A}, volume = {120}, journal = {Journal of Physical Chemistry A}, number = {26}, doi = {10.1021/acs.jpca.6b04243}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159464}, pages = {4465-4472}, year = {2016}, abstract = {The design of ordered arrays of metal nanoclusters such as for example 2D cluster organic frameworks might open a new route towards the development of materials with tailored optical properties. Such systems could serve as plasmonically enhanced light-harvesting materials, sensors or catalysts. We present here a theoretical approach for the simulation of the optical properties of ordered arrays of metal clusters that is based on the ab initio parametrized Frenkel exciton model. We demonstrate that small atomically precise silver clusters can be assembled in one- and two-dimensional arrays on suitably designed porphyrin templates exhibiting remarkable optical properties. By employing explicit TDDFT calculations on smaller homologs, we show that the intrinsic optical properties of metal clusters are largely preserved but undergo J- and H-type excitonic coupling that results in controllable splitting of their excited states. Furthermore, ab initio parameterized Frenkel exciton model calculations allow us to predict an energetic splitting of up to 0.77 eV in extended two-dimensional square arrays and 0.79 eV in tilted square aggregates containing up to 25 cluster-porphyrin subunits.}, language = {en} } @unpublished{RoederHumeniukGiegerichetal.2017, author = {R{\"o}der, Anja and Humeniuk, Alexander and Giegerich, Jens and Fischer, Ingo and Poisson, Lionel and Mitric, Roland}, title = {Femtosecond Time-Resolved Photoelectron Spectroscopy of the Benzyl Radical}, series = {Physical Chemistry Chemical Physics}, journal = {Physical Chemistry Chemical Physics}, doi = {10.1039/C7CP01437F}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-159474}, year = {2017}, abstract = {We present a joint experimental and computational study of the nonradiative deactivation of the benzyl radical, C\(_7\)H\(_7\) after UV excitation. Femtosecond time-resolved photoelectron imaging was applied to investigate the photodynamics of the radical. The experiments were accompanied by excited state dynamics simulations using surface hopping. Benzyl has been excited at 265 nm into the D-band (\(\pi\pi^*\)) and the dynamics was probed using probe wavelengths of 398 nm or 798 nm. With 398 nm probe a single time constant of around 70-80 fs was observed. When the dynamics was probed at 798 nm, a second time constant \(\tau_2\)=1.5 ps was visible. It is assigned to further non-radiative deactivation to the lower-lying D\(_1\)/D\(_2\) states.}, language = {en} } @phdthesis{Hader2017, author = {Hader, Kilian}, title = {Lokalisierungsdynamik unter Ber{\"u}cksichtigung von Molek{\"u}l-Feld-Wechselwirkung, Kern-Elektron-Kopplung und Exziton-Exziton-Annihilierung}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-146735}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2017}, abstract = {Diese Arbeit befasst sich mit verschiedenen Aspekten der Dynamik von Kernen, Elektronen und gekoppelten Kern-Elektron-Systemen, wobei je nach System unterschiedliche Herangehensweisen gew{\"a}hlt wurden. Zentrale Punkte sind bei allen drei Kapiteln einerseits die Lokalisierung von Teilchen und Energie und andererseits eine hohe Sensitivit{\"a}t in Bezug auf die Wahl der Anfangsbedingungen. Im ersten Teil wurden von der Carrier-Envelope-Phase (CEP) abh{\"a}ngende, laser-induzierte Lokalisierungen betrachtet. Das zentrale Element ist dabei das entwickelte Doppelpulsschema, mit welchem eine CEP-Abh{\"a}ngigkeit in beobachtbaren Gr{\"o}ßen erzeugt wird. Als Beispielsysteme wurden die Fragmentation im D₂⁺-Modellsystem und eine Isomerisierung im Doppelminimumpotential (DMP) untersucht. Als Observable wird die Asymmetrie betrachtet Im DMP kann die Asymmetrie mit dem Entantiomeren/Isomeren{\"u}berschuss gleich gesetzt werden kann und im D₂⁺-Modellsystem mit der Lokalisierung des Elektrons auf einem der beiden dissoziierenden Kerne. Eine Phasenabh{\"a}ngigkeit der Asymmetrien besteht nur f{\"u}r die CEP des zweiten Pulses φ₂, f{\"u}r welchen keine Begrenzungen f{\"u}r die Anzahl an Laserzyklen auftreten. Im DMP wurde die CEP-Abh{\"a}ngigkeit der Asymmetrien auch bei unterschiedlichen Startkonfigurationen untersucht. F{\"u}r alle untersuchten Startkonfigurationen konnte ein Laserparametersatz gefunden werden, der f{\"u}r zumindest eine der beiden Asymmetrien eine CEP-Abh{\"a}ngigkeit liefert. Aufgrund der aufgehobenen energetischen Entartung der Paare gerader und ungerader Symmetrie ist die resultierende Lokalisierung zeitabh{\"a}ngig. Zur Messung der vorhergesagten Dynamiken ist z.B. die Aufnahme eines Photoelektronen-Spektrums denkbar. In n{\"a}chsten Kapitel wurden unterschiedliche Dynamiken innerhalb eines 4d Kern-Elektron-Modells in der N{\"a}he einer konischen Durchschneidung (CI) zweier Potentiale betrachtet. Hierbei ist hervorzuheben, dass eine solche gleichzeitige Untersuchung von Kern- und Elektron-Dynamik in Systemen mit CIs in der Literatur, nach Wissen des Autors, bisher nicht ver{\"o}ffentlicht ist. Das 4d-Potential wurde mit Hilfe des sogenannten Potfit-Algorithmus gefittet. Dieser Fit wurde anschließend verwendet, um die Dynamik des gekoppelten Systems mit Hilfe der "Multi-Configuration Time-Dependent Hartree"(MCTDH)-Methode zu berechnen. Aus der Analyse der gekoppelten Kern-Elektron-Wellenfunktion ergaben sich zwei grundlegend unterschiedliche Klassen von Dynamiken: • Diabatisch: Kern- und Elektrondynamik sind nahezu entkoppelt. Der Kern bewegt sich und das Elektron bleibt statisch. • Adiabatisch: Kern- und Elektrondynamik sind stark gekoppelt. Die Kerndynamik findet auf Kreisbahnen statt. Mit der Rotation der Kerndichte um den Winkel φ geht eine Rotation der Elektron-Dichte einher. Die diabatische Bewegung entspricht der Dynamik durch die konische Durchschneidung und die adiabatische Bewegung der Dynamik auf der unteren Potentialfl{\"a}che. Welche der beiden Dynamiken stattfindet, wird durch die Wahl der Anfangsbedingung bestimmt. Der wesentliche Unterschied zwischen den beiden Startzust{\"a}nden ist dabei die Lage des Knotens im elektronischen Anteil der Wellenfunktion. In den diabatischen Bewegungen bleibt z.B. der pₓ -artige Charakter der elektronischen Wellenfunktion konstant, wohingegen sich bei der adiabatischen Dynamik der Charakter mit der Kernbewegung {\"a}ndert. Die Zeitersparnis durch die Verwendung des MCTDH-Ansatzes im Vergleich zur Split-Operator-Methode liegt etwa bei einem Faktor 5. Das letzte Kapitel widmet sich der mikroskopischen Beschreibung von Exziton-Exziton- Annihilierung (EEA). Dabei werden numerische L{\"o}sungen der aus einem mikro- skopischen Modell hergeleiteten Ratengleichungen mit Messungen ( transienter Absorption) verglichen. Es wurden zwei Systeme untersucht: ein Squarain-basiertes Heteropolymer (SQA-SQB)ₙ und ein [2-methoxy-5-(2-ethylhexyloxy)-1,4-phenylenvinylen]-Polymer, auch bekannt als MEH-PPV. In beiden F{\"a}llen gelang die systematische Parameterbestimmung mit Hilfe einer Aufteilung in lokalisierte Subsysteme. Diese Subsysteme werden einzeln gewichtet und anschließend aufsummiert, wobei die Gewichte optimiert werden k{\"o}nnen. Aus den so erhaltenen Parametern ergibt sich f{\"u}r beide Systeme ein {\"a}hnliches Bild: • Durch ultraschnelle Lokalisierung der Anregung im fs-Bereich auf kleinere Aggregateinheiten bilden sich voneinander getrennte Subsysteme. • Die in den Subsystemen lokalisierten Exzitonen k{\"o}nnen sich nur innerhalb dieser Bereiche frei bewegen. Es ist ausreichend, direkt benachbarte Mono-, Bi-, Tri- und Tetra-Exzitonen in bis zu zwei Dimensionen zu ber{\"u}cksichtigen. • Auf einer fs-Zeitskala annihilieren direkt benachbarte Exzitonen. • Im MEH-PPV ergibt sich der Signalzerfall im fs-Bereich als Mittelwert aus einer schnellen (zwischen Ketten) und einer langsamen (innerhalb von Ketten) Annihilierung. • Im ps- bis ns-Bereich wird sowohl durch Diffusion vermittelte Annihilierung, also auch der Zerfall der ersten angeregten Zust{\"a}nde bedeutsam.}, subject = {Quantenmechanik}, language = {de} } @phdthesis{Brueckner2017, author = {Br{\"u}ckner, Charlotte}, title = {The Electronic Structure and Optoelectronic Processes at the Interfaces in Organic Solar Cells Composed of Small Organic Molecules - A Computational Analysis of Molecular, Intermolecular, and Aggregate Aspects}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-141652}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2017}, abstract = {Describing the light-to-energy conversion in OSCs requires a multiscale understanding of the involved optoelectronic processes, i.e., an understanding from the molecular, intermolecular, and aggregate perspective. This thesis presents such a multiscale description to provide insight into the processes in the vicinity of the organic::organic interface, which are crucial for the overall performance of OSCs. Light absorption, exciton diffusion, photoinduced charge transfer at the donor-acceptor interface, and charge separation are included. In order to establish structure-property relationships, a variety of different molecular p-type semiconductors are combined at the organic donor-acceptor heterojunction with fullerene C60, one of the most common acceptors in OSCs. Starting with a comprehensive analysis of the accuracy of diverse ab initio, DFT, and semiempiric methods for the properties of the individual molecules, the intermolecular, and aggregate/device stage are subsequently addressed. At all stages, both methodological concepts and physical aspects in OSCs are discussed to extend the microscopic understanding of the charge generation processes.}, subject = {Benchmark}, language = {en} } @phdthesis{Schwarz2015, author = {Schwarz, Christoph Benjamin}, title = {Full vector-field control of femtosecond laser pulses with an improved optical design}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-142948}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2015}, abstract = {The controlled shaping of ultrashort laser pulses is a powerful technology and applied in many laser laboratories today. Most of the used pulse shapers are only able to produce linearly polarized pulses shaped in amplitude and phase. Some devices are also capable of producing limited time-varying polarization profiles, but they are not able to control the amplitude. However, for some state-of-the-art non-linear time-resolved methods, such as polarization-enhanced two-dimensional spectroscopy, the possibility of controlling the amplitude and the polarization simultaneously is desirable. Over the last years, different concepts have been developed to overcome these restrictions and to manipulate the complete vector-field of an ultrashort laser pulse with independent control over all four degrees of freedom - phase, amplitude, orientation, and ellipticity. The aim of this work was to build such a vector-field shaper. While the basic concept used for our setup is based on previous designs reported in the literature, the goal was to develop an optimized optical design that minimizes artifacts, allowing for the generation of predefined polarization pulse sequences with the highest achievable accuracy. In Chapter 3, different approaches reported in the literature for extended and unrestricted vector-field control were examined and compared in detail. Based on this analysis, we decided to follow the approach of modulating the spectral phase and amplitude of two perpendicularly polarized pulses independently from each other in two arms of an interferometer and recombining them to a single laser pulse to gain control over the complete vector field. As described in Chapter 4, the setup consists of three functional groups: i) an optical component to generate and recombine the two polarized beams, ii) a 4f setup, and iii) a refracting telescope to direct the two beams under two different angles of incidence onto the grating of the 4f setup in a common-path geometry. This geometry was chosen to overcome potential phase instabilities of an interferometric vector-field shaper. Manipulating the two perpendicularly polarized pulses simultaneously within one 4f setup and using adjacent pixel groups of the same liquid-crystal spatial light modulator (LC SLM) for the two polarizations has the advantages that only a single dual-layer LC SLM is required and that a robust and compact setup was achieved. The shaping capabilities of the presented design were optimized by finding the best parameters for the setup through numerical calculations to adjust the frequency distributions for a broad spectrum of 740 - 880 nm. Instead of using a Wollaston prism as in previous designs, a thin-film polarizer (TFP) is utilized to generate and recombine the two orthogonally polarized beams. Artifacts such as angular dispersion and phase distortions along the beam profile which arise when a Wollaston prism is used were discussed. Furthermore, it was shown by ray-tracing simulations that in combination with a telescope and the 4f setup, a significant deformation of the beam profile would be present when using a Wollaston prism since a separation of the incoming and outgoing beam in height is needed. The ray-tracing simulations also showed that most optical aberrations of the setup are canceled out when the incoming and outgoing beams propagate in the exact same plane by inverting the beam paths. This was realized by employing a TFP in the so-called crossed-polarizer arrangement which has also the advantage that the polarization-dependent efficiencies of the TFP and the other optics are automatically compensated and that a high extinction ratio in the order of 15000:1 is reached. Chromatic aberrations are, however, not compensated by the crossed-polarizer arrangement. The ray-tracing simulations confirmed that these chromatic aberrations are mainly caused by the telescope and not by the cylindrical lens of the 4f setup. Nevertheless, in the experimentally used wavelength range of 780 - 816 nm, only minor distortions of the beam profile were observed, which were thus considered to be negligible in the presented setup. The software implementation of the pulse shaper was reviewed in Chapter 5 of this thesis. In order to perform various experiments, five different parameterizations, accounting for the extended shaping capabilities of a vector-field shaper, were developed. The Pixel Basis, the Spectral Basis, and the Spectral Taylor Basis can generally be used in combination with an optimization algorithm and are therefore well suited for quantum control experiments. For multidimensional spectroscopy, the Polarized Four-Pulse Basis was established. With this parameterization pulse sequences with up to four subpulses can be created. The polarization state of each subpulse can be specified and the relative intensity, phase, and temporal delay between consecutive subpulses can be controlled. In addition, different software programs were introduced in Chapter 5 which are required to perform the experiments conducted in this work. The experimental results were presented in Chapter 6. The frequency distribution across the LC SLM was measured proving that the optimal frequency distribution was realized experimentally. Furthermore, the excellent performance of the TFP was verified. In general, satellite pulses are emitted from the TFP due to multiple internal reflections. Various measurements demonstrated that these pulses are temporally separated by at least 4.05 ps from the main pulse and that they have vanishing intensity. The phase stability between the two arms of the presented common-path setup σ = 28.3 mrad (λ/222) over 60 minutes. To further improve this stability over very long measurement times, an on-the-fly phase reduction and stabilization (OPRAS) routine utilizing the pulse shaper itself was developed. This routine automatically produces a compressed pulse with a minimized relative phase between the two polarization components. A phase stability of σ = 31.9 mrad (λ/197) over nearly 24 hours was measured by employing OPRAS. Various pulse sequences exceeding the capabilities of conventional pulse shapers were generated and characterized. The experimental results proved that shaped pulses with arbitrary phase, amplitude, and polarization states can be created. In all cases very high agreement between the target parameters and the experimental data was achieved. For the future use of the setup also possible modifications were suggested. These are not strictly required, but all of them could further improve the performance and flexibility of the setup. Firstly, it was illustrated how a "dual-output" of the setup can be realized. With this modification it would be possible to use the main intensity of the shaped pulse for an experiment while using a small fraction to characterize the pulse or to perform OPRAS simultaneously. Secondly, the basic idea of replacing the telescope by focusing mirrors in order to eliminate the chromatic aberrations was presented. Regarding the different parameterizations for vector-field shaping, some modifications increasing the flexibility of the implemented bases and the realization of a von Neumann Basis for the presented setup were proposed. In future experiments, the vector-field shaper will be used in conjunction with a photoemission electron microscope (PEEM). This approach combines the temporal resolution provided by ultrashort laser pulses with the high spatial resolution gained by electron microscopy in order to perform two-dimensional spectroscopy and coherent control on nanostructures with polarization-shaped femtosecond laser pulses. In combination with other chiral-sensitive experimental setups implemented earlier in our group, the vector-field shaper opens up new perspectives for chiral femtochemistry and chiral control. The designed vector-field shaper meets all requirements to generate high-precision polarization-shaped multipulse sequences. These can be used to perform numerous polarization-sensitive experiments. Employing the OPRAS routine, a quasi-infinitely long phase stability is achieved and complex and elaborated long-term measurements can be carried out. The fact that OPRAS demands no additional hardware and that only a single dual-layer LC SLM and inexpensive optics are required allows the building of a vector-field shaper at comparatively low costs. We hope that with the detailed insights into the optical design process as well as into the software implementation given in this thesis, vector-field shaping will become a standard technique just as conventional pulse shaping in the upcoming years.}, subject = {Ultrakurzer Lichtimpuls}, language = {en} }