30.00.00 ATOMIC AND MOLECULAR PHYSICS
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- protein hydration (2)
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- time-resolved photoelectron spectroscopy (2)
- time-resolved spectroscopy (2)
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- amino-acids (1)
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Institute
Sonstige beteiligte Institutionen
- Institut für Optik und Atomare Physik, Technische Universität Berlin, 10623 Berlin, Germany (2)
- Laboratory for Chemistry and Life Science, Institute of Innovative Research, Tokyo Institute of Technology, Yokohama 226-8503, Japan (2)
- Center for Nanosystems Chemistry (CNC), Universität Würzburg, Am Hubland, 97074 Würzburg, Germany (1)
- LIDYL, CEA, CNRS, Université Paris-Saclay, CEA Saclay 91191 Gif-sur-Yvette France (1)
- Université de Paris-Saclay (1)
ResearcherID
- M-1240-2017 (1)
The mechanism of excimer formation: an experimental and theoretical study on the pyrene dimer
(2017)
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.
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.
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.
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.
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.
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.
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.
In der vorliegenden Arbeit wurde erfolgreich eine neue Gasphasen-Apparatur für
Photoelektronen-Imaging-Experimente simuliert, aufgebaut und in Verbindung mit einem ps-Lasersystem in Betrieb genommen.
Neben dem Aufbau der Apparatur stand die Aufklärung der Dynamik angeregter Zustände von aromatischen Heterocyclen und Pyrenen im Fokus dieser Arbeit. Die untersuchten Moleküle wurden durch Resonanzverstärkte Mehrphotonenionisation in einem Molekularstrahlexperiment sowohl zeit-, als auch frequenzaufgelöst untersucht.
Diffusionsgewichtete MR-Bilder sind ein wichtiger Bestandteil für die klinische Diagnostik
verschiedener Pathologien, wie z.B. bei Schlaganfall oder Tumoren. Meistens
wird ein mono-exponentielles Diffusionsmodell verwendet und über verschiedene
Raumrichtungen gemittelt. Der Einfluss von Fluss auf das diffusionsgewichtete
Signal und eine mögliche Richtungsabhängigkeit werden dabei vernachlässigt. Dabei
machen Diffusionsmodelle, die mehr Eigenschaften des Signals abbilden, unter
Umständen eine genauere Diagnostik möglich. Mit DTI wird die Richtungsabhängigkeit
der Diffusion erfasst und bei IVIM wird der Beitrag von Fluss zum Signal
berücksichtigt. Die Niere ist ein stark strukturiertes Organ und weist Anisotropie
in der Diffusion auf. Außerdem ist die Niere ein sehr gut durchblutetes Organ. DTI
und IVIM beschreiben also unabhängig voneinander zwei wichtige Aspekte des diffusionsgewichteten
Signals in der Niere, ohne dass der Vorteil des jeweils anderen
Modells Beachtung findet.
In dieser Arbeit wurde das Modell IVOF zur umfassenden Beschreibung von Diffusionssignal
vorgestellt, bei dem sowohl die Richtungsabhängigkeit der Diffusion,
als auch das Signal der fließenden Spins und deren Richtungsabhängigkeit abgebildet
wird. Die Vorteile von DTI und IVIM werden also in IVOF vereint und darüber
hinaus auch die mögliche Anisotropie die Flusssignals berücksichtigt. Es konnte gezeigt
werden, dass dieses Modell das diffusionsgewichtete Signal in der menschlichen
Niere besser beschreibt als die herkömmlichen Modelle (DTI und IVIM) und auch
besser als eine Kombination von DTI und IVIM, bei der ein isotroper Flussanteil
des Signals angenommen wird.
Es wurde weiterhin gezeigt, dass selbst wenn der Flussanteil im verwendeten Diffusionsmodell
berücksichtigt wird, der tatsächlich gemessene Flussanteil in der Niere
von der Art der Messung, d.h. Bewegungsempfindlichkeit des Gradientenschemas
abhängt. Das bedeutet, dass der mikroskopische Fluss in der Niere nicht, wie häufig
angenommen, komplett zeitlich inkohärent ist. Bei Vergleichen von IVIM Studien
an der Niere ist es deshalb notwendig, die Bewegungsempfindlichkeit der jeweiligen
Gradientenschemata zu berücksichtigen. Wie groß das absolute Verhältnis von kohärent zu inkohärent fließendem Signal ist, konnte nicht festgestellt werden. Ebenso
wenig konnte die absolute Flussgeschwindigkeit bzw. die Art des Flusses (Laminare
Strömung, Pfropfenströmung, oder andere) ermittelt werden.
TSE hat sich als vielversprechendes, artefaktfreies Verfahren für die Aufnahme
diffusionsgewichteter Bilder der Niere gezeigt. Im Vergleich mit dem Standardverfahren EPI wurden ähnliche Werte der Parameter von DTI und IVIM gefunden.
Abweichungen zwischen EPI und TSE sind vor allem durch die Unschärfe der TSE
Bilder aufgrund von T2-Zerfall zu erklären. Bis zur klinischen Anwendbarkeit diffusionsgewichteter
TSE Bilder bzw. Parameterkarten sind noch einige Weiterentwicklungen
der Methode nötig. Vor allem sind schärfere TSE Bilder erstrebenswert und
es sollten mehrere Schichten in einer klinisch vertretbaren Zeitspanne aufgenommen
werden, ohne dass dabei die zulässigen SAR Grenzwerte überschritten werden.
Bei allen Untersuchungen in dieser Arbeit handelt es sich um Machbarkeitsstudien.
Daher wurden alle Messungen nur an erwachsenen, gesunden Probanden durchgeführt, um zu zeigen, dass das jeweilige vorgeschlagene Modell zu den Daten passt
bzw. dass die vorgeschlagene Methode prinzipiell funktioniert. Bei welchen Pathologien
die hier vorgeschlagenen Methoden und Modelle einen diagnostischen Nutzen
haben, muss in zukünftigen Studien erforscht werden. Außerdem wurden keine b-
Werte zwischen 0 und 200 s/mm2 aufgenommen, bei denen fließende Spins noch
signifikant zum Signal beitragen. Betrachtet man die Ergebnisse der Diffusionsbildgebung
mit verschiedenen m1 in dieser Arbeit, dann ist neben dem b-Wert auch die
Bewegungsempfindlichkeit m1 nötig, um das Signal in diesem Bereich korrekt zu
beschreiben.
Alles in allem sollte der Beitrag von Fluss zum diffusionsgewichteten MR-Signal
in der Niere immer berücksichtigt werden. Die vielfältigen Einflüsse, die unterschiedliche
Parameter auf das Signal von Mikrofluss haben, wurden in dieser Arbeit untersucht
und präsentieren weiterhin ein spannendes Feld für kommende Studien.
Diffusionsgewichtete TSE Sequenzen sind auch für die klinische Diagnostik eine potentielle
Alternative zu Artefakt-anfälligen EPI Sequenzen. Bis dahin sollten jedoch
die Bildschärfe und Abdeckung der diffusionsgewichteten TSE Sequenz weiter verbessert
werden.
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.