Time-of-flight two-photon photoemission spectromicroscopy with femtosecond laser radiation

Time-of-flight photoemission spectromicroscopy was used to measure and compare the two-photon photoemission (2PPE) spectra of Cu and Ag nanoparticles with linear dimensions ranging between 40 nm and several 100 nm, with those of the corresponding homogeneous surfaces. 2PPE was induced employing femtosecond laser radiation from a frequency-doubled Ti:sapphire laser in the spectral range between 375 nm and 425 nm with a pulse width of 200 fs and a repetition rate of 80 MHz. The use of a pulsed radiation source allowed us to use a high-resolution photoemission electron microscope as imaging time-of-flight spectrometer, and thus to obtain spectroscopic information about the laterally resolved electron signal. Ag nanoparticle films have been deposited on Si(111) by electron-beam evaporation, a technique leading to hemispherically-shaped Ag clusters. Isolated Cu nanoparticles have been generated by prolonged heating of a polycrystalline Cu sample. If compared to the spectra of the corresponding homogeneous surfaces, the Cu and Ag nanoparticle spectra are characterized by a strongly enhanced total 2PPE yield (enhancement factor up to 70), by a shift (about 0.1 eV) of the Fermi level onset towards lower final state energies, by a reduction of the work function (typically by 0.2 eV) and by a much steeper increase of the 2PPE yield towards lower final state energies. The shift of the Fermi level onset in the nanoparticle spectra has been explained by a positive unit charge (localized photohole) residing on the particle during the time-scale relevant for the 2PPE process (few femtoseconds). The total 2PPE yield enhancement and the different overall shape of the spectra have been explained by considering that the laser frequency was close to the localized surface plasmon resonance of the Cu and Ag nanoparticles. The synchronous oscillations induced by the laser in the metal electrons enhance the near-zone (NZ) field, defined as the linear superposition of the laser field and the field produced in the vicinity of the particles by the forced charge oscillations. From the present measurements it is clear that the NZ field behavior is responsible for the 2PPE enhancement and affects the 2PPE spatial and energy distribution and its dynamics. In particular, its strong spatial dependence allows indirect transitions through real intermediate states to take place in the metal clusters. Such transitions are forbidden by momentum conservation arguments and are thus experimentally much less probable on homogeneous surfaces. Further, we investigated specially tailored moon-shaped small metal nanostructures, whose NZ field was theoretically predicted, and compared the calculation with the laterally resolved 2PPE signal. We could show that the 2PPE signal gives a clear fingerprint of the theoretically predicted spatial dependence of the NZ field. This potential of our method is highly attractive in the novel field of plasmonics.

Modulation der Strahlen- und Chemosensitivität menschlicher Tumorzellen durch Interferon

Pankreaskarzinome und maligne Melanome weisen eine hohe Resistenz gegenüber Zytostatika und Bestrahlung in der Therapie auf. Die Behandlung eines metastasierenden Pankreaskarzinoms besteht aus einer Kombination aus 5-FU, CDDP und IR. Für die Behandlung des malignen Melanoms ist das methylierende Agenz DTIC das Mittel erster Wahl. Das ebenfalls methylierende Agenz TMZ, welches jedoch in Deutschland noch nicht für die Behandlung von malignen Melanomen zugelassen ist, erlangt immer größere Bedeutung. Die Ansprechrate der Tumore kann durch Kombination mit IFNs erhöht werden. In der vorliegenden Arbeit wurde an Pankreaskarzinom- bzw. Melanomzelllinien untersucht, ob IFNs einen radio- bzw. chemosensibilisierender Effekt ausüben und, wenn ja, welcher Mechanismus hierfür verantwortlich ist. Es wurden zehn Pankreaskarzinom-Zelllinien (Panc-1, Su8686, Capan-1, Capan-2, Bxpc-3, PA-TU 8988T, Aspc-1, HS 766T, Mia-PaCa-2 und PA-TU 8902) untersucht. Diese zeigten eine hohe Variabilität in ihrer intrinsischen Radiosensitivität sowie in ihrer Sensitivität gegenüber IFN-alpha und IFN-beta. IFN-beta erwies sich als toxischer im Vergleich zu IFN-alpha. Die radiosensibilisierende Wirkung der IFNs an Pankreaskarzinom-Zelllinien war moderat, wobei IFN-beta im Vergleich zu IFN-alpha effektiver war. Der radiosensibilisierende Effekt ging mit einer deutlichen Erhöhung der alpha-Komponente, der Überlebenskurven einher und kam durch eine IFN-beta vermittelte Verstärkung der IR-induzierten Apoptoserate zustande. Dies wurde sowohl durch SubG1 als auch durch Annexin V / PI Messungen gezeigt. Einen Einfluss von IFN-beta auf den Zellzyklus und die DSB-Reparatur konnte durch funktionelle Untersuchungen sowie durch PCR bzw. Western-Blot-Analysen als Grund für den sensibilisierdenen Effekt ausgeschlossen werden. Ein sensibilisierender Effekt von IFN-beta auf die durch TMZ-induzierte Zytotoxizität war für die Pankreaskarzinom-Zelllinien weder in MGMT-profizientem noch –depletiertem Zustand zu beobachten. Zur Untersuchung der sensibilisierenden Eigenschaften von IFNs gegenüber TMZ in malignen Melanomzelllinien wurden p53-Wildtyp (D05 und A375) und mutierte Zelllinien (D14 und RPMI 7951) untersucht. Gegenüber alleiniger TMZ-Behandlung reagierten die untersuchten p53-Wildtyp Melanomzelllinien nicht sensitiver auf eine Behandlung mit TMZ als p53-mutierte Zelllinien. Der Nachweis des Spaltprodukts der Caspase-9 lieferte einen Hinweis darauf, dass in den Melanomzelllinien unabhängig vom p53-Status nach alleiniger TMZ-Behandlung der mitochondriale Apoptoseweg aktiviert wird. Durch eine Vorbehandlung der Zellen mit IFN-alpha oder IFN-beta konnte die TMZ-induzierte Apoptoserate in malignen Melanomzellen deutlich gesteigert werden. In p53-Wildtyp Melanomzellen war der chemosensibilisierende Effekt der IFNs besonders ausgeprägt. IFN-beta erwies sich hierbei als effektiver, weshalb es für die folgenden Versuche verwendet wurde. Durch stabile Transfektion der Zelllinie D05 mit MGMT konnte das durch TMZ-induzierte Addukt O6MeG als für den sensibilisieredenen Effekt ausschlaggebende DNA-Schädigung charakterisiert werden. Western-Blot-Analysen und gamma-H2AX-Immunfluoreszenz Untersuchungen konnten einen Einfluss von IFN-beta auf die Prozessierung der Läsion O6MeG sowie einen Einfluss von IFN-beta auf die Induktion und Reparatur von TMZ verursachten DSBs ausschließen. Durch Experimente mit einem Fas-aktivierenden Antikörper und durch eine stabile Transfektion der Zelllinien D05 und A375 mit DN-FADD konnte gezeigt werden, dass p53-Wildtyp Melanomzellen nicht oder nur eingeschränkt in der Lage sind, nach TMZ-Behandlung über den Fas-Rezeptor Signalweg Apoptose zu induzieren. Ausschlaggebend hierfür ist die geringe Pro-Caspase-8 Expression dieser Zelllinien. Eine IFN-beta Vorbehandlung bewirkte eine Reaktivierung des Fas-Rezeptor Signalweges, was mit einer verstärkten Expression der Pro-Caspase-8 einherging. Durch Experimente mit Caspase-8 siRNA konnte diese IFN-beta induzierte Verstärkung der Pro-Caspase-8 Expression als entscheidender Faktor für den sensibilisierenden Effekt ausgemacht werden. Zum ersten Mal konnte damit in dieser Arbeit gezeigt werden, dass p53-Wildtyp Melanomzellen durch eine IFN-beta vermittelte Hochregulation der Pro-Caspase-8 ihre Fähigkeit wiedererlangen, nach TMZ-Behandlung über den Fas-Rezeptor Signalweg Apoptose auszulösen. Diese Arbeiten weisen einen Weg, auf welchem die hohe Resistenz von malignen Melanomzellen, welche zu 80 % das nicht mutierte p53 Gen beherbergen, über eine IFN-beta induzierte Reaktivierung der Fas-Rezeptor vermittelten Apoptosekaskade überwunden werden kann.

Radiation-induced defects in calcium fluoride and their influence on material properties under 193 nm laser irradiation

Calcium fluoride (CaF2) is one of the key lens materials in deep-ultraviolet microlithography because of its transparency at 193 nm and its nearly perfect optical isotropy. Its physical and chemical properties make it applicable for lens fabrication. The key feature of CaF2 is its extreme laser stability. rnAfter exposing CaF2 to 193 nm laser irradiation at high fluences, a loss in optical performance is observed, which is related to radiation-induced defect structures in the material. The initial rapid damage process is well understood as the formation of radiation-induced point defects, however, after a long irradiation time of up to 2 months, permanent damage of the crystals is observed. Based on experimental results, these permanent radiation-induced defect structures are identified as metallic Ca colloids.rnThe properties of point defects in CaF2 and their stabilization in the crystal bulk are calculated with density functional theory (DFT). Because the stabilization of the point defects and the formation of metallic Ca colloids are diffusion-driven processes, the diffusion coefficients for the vacancy (F center) and the interstitial (H center) in CaF2 are determined with the nudged elastic band method. The optical properties of Ca colloids in CaF2 are obtained from Mie-theory, and their formation energy is determined.rnBased on experimental observations and the theoretical description of radiation-induced point defects and defect structures, a diffusion-based model for laser-induced material damage in CaF2 is proposed, which also includes a mechanism for annealing of laser damage. rn

Measurement of the e + e - pi + pi - pi + pi - cross section using initial state radiation at BABAR

One of the most precisely measured quantities in particle physics is the magnetic moment of the muon, which describes its coupling to an external magnetic field. It is expressed in form of the anomalous magnetic moment of the muon a_mu=(g_mu-2)/2 and has been determined experimentally with a precision of 0.5 parts per million. The current direct measurement and the theoretical prediction of the standard model differ by more than 3.5 standard deviations. Concerning theory, the contribution of the QED and weak interaction to a_mu can be calculated with very high precision in a perturbative approach.rnAt low energies, however, perturbation theory cannot be used to determine the hadronic contribution a^had_mu. On the other hand, a^had_mu may be derived via a dispersion relation from the sum of measured cross sections of exclusive hadronic reactions. Decreasing the experimental uncertainty on these hadronic cross sections is of utmost importance for an improved standard model prediction of a_mu.rnrnIn addition to traditional energy scan experiments, the method of Initial State Radiation (ISR) is used to measure hadronic cross sections. This approach allows experiments at colliders running at a fixed centre-of-mass energy to access smaller effective energies by studying events which contain a high-energetic photon emitted from the initial electron or positron. Using the technique of ISR, the energy range from threshold up to 4.5GeV can be accessed at Babar.rnrnThe cross section e+e- -> pi+pi- contributes with approximately 70% to the hadronic part of the anomalous magnetic moment of the muon a_mu^had. This important channel has been measured with a precision of better than 1%. Therefore, the leading contribution to the uncertainty of a_mu^had at present stems from the invariant mass region between 1GeV and 2GeV. In this energy range, the channels e+e- -> pi+pi-pi+pi- and e+e- -> pi+pi-pi0pi0 dominate the inclusive hadronic cross section. The measurement of the process e+e- -> pi+pi-pi+pi- will be presented in this thesis. This channel has been previously measured by Babar based on 25% of the total dataset. The new analysis includes a more detailed study of the background contamination from other ISR and non-radiative background reactions. In addition, sophisticated studies of the track reconstruction as well as the photon efficiency difference between the data and the simulation of the Babar detector are performed. With these auxiliary studies, a reduction of the systematic uncertainty from 5.0% to 2.4% in the peak region was achieved.rnrnThe pi+pi-pi+pi- final state has a rich internal structure. Hints are seen for the intermediate states rho(770)^0 f_2(1270), rho(770)^0 f_0(980), as well as a_1(1260)pi. In addition, the branching ratios BR(jpsi -> pi+pi-pi+pi-) and BR(psitwos -> jpsi pi+pi-) are extracted.rn

Mechanistic study of cell death induction by O 6-methylating agents, focusing on the role of homologous recombination as a molecular target for sensitization of tumor cells to chemotherapeutic alkylating agents

Chemotherapeutic SN1‑methylating agents are important anticancer drugs. They induce several covalent modifications in the DNA, from which O6‑methylguanine (O6MeG) is the main toxic lesion. In this work, different hypotheses that have been proposed to explain the mechanism of O6MeG‑triggered cell death were tested. The results of this work support the abortive processing model, which states that abortive post‑replicative processing of O6MeG‑driven mispairs by the DNA mismatch repair (MMR) machinery results in single‑strand gaps in the DNA that, upon a 2nd round of DNA replication, leads to DNA double‑strand break (DSB) formation, checkpoint activation and cell death. In this work, it was shown that O6MeG induces an accumulation of cells in the 2nd G2/M‑phase after treatment. This was accompanied by an increase in DSB formation in the 2nd S/G2/M‑phase, and paralleled by activation of the checkpoint kinases ATR and CHK1. Apoptosis was activated in the 2nd cell cycle. A portion of cells continue proliferating past the 2nd cell cycle, and triggers apoptosis in the subsequent generations. An extension to the original model is proposed, where the persistence of O6MeG in the DNA causes new abortive MMR processing in the 2nd and subsequent generations, where new DSB are produced triggering cell death. Interestingly, removal of O6MeG beyond the 2nd generation lead to a significant, but not complete, reduction in apoptosis, pointing to the involvement of additional mechanisms as a cause of apoptosis. We therefore propose that an increase in genomic instability resulting from accumulation of mis‑repaired DNA damage plays a role in cell death induction. Given the central role of DSB formation in toxicity triggered by chemotherapeutic SN1‑alkylating agents, it was aimed in the second part of this thesis to determine whether inhibition of DSB repair by homologous recombination (HR) or non‑homologous end joining (NHEJ) is a reasonable strategy for sensitizing glioblastoma cells to these agents. The results of this work show that HR down‑regulation in glioblastoma cells impairs the repair of temozolomide (TMZ)‑induced DSB. HR down‑regulation greatly sensitizes cells to cell death following O6‑methylating (TMZ) or O6‑chlorethylating (nimustine) treatment, but not following ionizing radiation. The RNAi mediated inhibition in DSB repair and chemo‑sensitization was proportional to the knockdown of the HR protein RAD51. Chemo‑sensitization was demonstrated for several HR proteins, in glioma cell lines proficient and mutated in p53. Evidence is provided showing that O6MeG is the primary lesion responsible for the increased sensitivity of glioblastoma cells following TMZ treatment, and that inhibition of the resistance marker MGMT restores the chemo‑sensitization achieved by HR down‑regulation. Data are also provided to show that inhibition of DNA‑PK dependent NHEJ does not significantly sensitized glioblastoma cells to TMZ treatment. Finally, the data also show that PARP inhibition with olaparib additionally sensitized HR down‑regulated glioma cells to TMZ. Collectively, the data show that processing of O6MeG through two rounds of DNA replication is required for DSB formation, checkpoint activation and apoptosis induction, and that O6MeG‑triggered apoptosis is also executed in subsequent generations. Furthermore, the data provide proof of principle evidence that down‑regulation of HR is a reasonable strategy for sensitizing glioma cells to killing by O6‑alkylating chemotherapeutics.

Measurement of the e + e - pi + pi - cross section using initial state radiation at BESIII

The future goal of modern physics is the discovery of physics beyond the Standard Model. One of the most significant hints for New Physics can be seen in the anomalous magnetic moment of the muon - one of the most precise measured variables in modern physics and the main motivation of this work. This variable is associated with the coupling of the muon, an elementary particle, to an external electromagnetic field and is defined as a = (g - 2)/2, whereas g is the gyromagnetic factor of the muon. The muon anomaly has been measured with a relative accuracy of 0.5·10-6. However, a difference between the direct measurement and the Standard Model prediction of 3.6 standard deviations can be observed. This could be a hint for the existence of New Physics. Unfortunately, it is, yet, not significant enough to claim an observation and, thus, more precise measurements and calculations have to be performed.rnThe muon anomaly has three contributions, whereas the ones from quantum electrodynamics and weak interaction can be determined from perturbative calculations. This cannot be done in case of the hadronic contributions at low energies. The leading order contribution - the hadronic vacuum polarization - can be computed via a dispersion integral, which needs as input hadronic cross section measurements from electron-positron annihilations. Hence, it is essential for a precise prediction of the muon anomaly to measure these hadronic cross sections, σ(e+e-→hadrons), with high accuracy. With a contribution of more than 70%, the final state containing two charged pions is the most important one in this context.rnIn this thesis, a new measurement of the σ(e+e-→π+π-) cross section and the pion form factor is performed with an accuracy of 0.9% in the dominant ρ(770) resonance region between 600 and rn900 MeV at the BESIII experiment. The two-pion contribution to the leading-order (LO) hadronic vacuum polarization contribution to (g - 2) from the BESIII result, obtained in this work, is computed to be a(ππ,LO,600-900 MeV) = (368.2±2.5stat±3.3sys)·10-10. With the result presented in this thesis, we make an important contribution on the way to solve the (g - 2) puzzle.