Entwicklung einer online-Chromatographie für Element 106 (Seaborgium)

Das Studium chemischer Eigenschaften der schwersten Elemente, der Transactiniden, erfordert immer leistungsfähigere Apparaturen. Wegen ihrer kurzen Halbwertszeiten müssen diese Elemente schnell von der Targetkammer mittels Gasjet zur Apparatur transportiert und dort in die wässrige Phase überführt werden. Das sollte zur Vermeidung von Verlusten durch vorzeitigen Zerfall möglichst online betrieben werden, d.h. die in der Kernreaktion gebildeten Atome werden kontinuierlich aus der Targetkammer ausgespült und in der Apparatur in die wässrige Phase überführt. Dabei stellt sich das Problem, die kleinen Aerosol-Partikel (100-200 nm und etwa 1010 Teilchen pro Liter) bei einem Gasfluss von 2 bis 3 Liter Jet-Gas pro min in eine mit 1 bis 2 mL/min fließende wässrige Lösung zu überführen. Hierzu wurden zwei verschiedene Systeme am TRIGA-Reaktor Mainz entwickelt und in Experimenten an den Schwerionenbeschleunigern am PSI und der GSI erfolgreich eingesetzt. Da die diskontinuierlich arbeitende Chemieapparatur ARCA, mit der bisher chemische Eigenschaften der Elemente 101, 103, 104, 105 und 106 bestimmt wurden, wegen niedriger Produktionsraten bei Element 106 an ihre technologischen Grenzen stößt, bestand eine weitere Aufgabe der vorliegenden Arbeit darin, ein kontinuierlich arbeitendes Chromatographiesystem aufzubauen, mit dem Verteilungskoeffizienten des Elements 106 gemessen werden können. Bei der in dieser Arbeit entwickelten und in Versuchen mit kurzlebigen Hafnium-, Wolfram- und Rutherfordium-Isotopen getesten, kontinuierlich arbeitenden Mehrsäulentechnik wird der direkte Nachweis des Transactinids aufgegeben, und die Retentionszeit in dem chromatographischen System über die Menge der während der Retention zerfallenen Atome bestimmt. Neben der apparativen Entwicklung dieser Technik, die geringste Totvolumina im System erfordert, mussten bei der Auswahl des geeigneten chemischen Systems die engen Grenzen dieser Methode beachtet werden, was umfangreiche Kenntnisse zur trägerfreien Chemie der homologen Elemente erfordert. Neben Batchexperimenten mit trägerfrei produzierten Nukliden wurde für offline-Experimente auch ARCA erfolgreich eingesetzt. Der Vergleich von Kd-Werten, die in Batchexperimenten, mit ARCA und mit der prinzipiell neuen Methode der Mehrsäulentechnik bestimmt wurden, zeigten dabei gute Übereinstimmungen. Für die Anwendbarkeit der Mehrsäulentechnik sind aber auch geeignete radioaktive Zerfallsketten notwendig, die in einem langlebigen Isotop enden sollten, welches über lange Experimentierzeiten akkumuliert werden kann. Dabei ist die Diskriminierung von einzelnen Atomen langlebiger Actiniden als Endglieder der Zerfallskette der Transactiniden gegen den natürlichen und elektronischen Untergrund sehr anspruchsvoll und möglicherweise der limitierende Faktor dieser Technik. Neben Beiträgen zur Fluoridkomplexierung von Elementen der 4. Nebengruppe (inklusive Rutherfordium) und der 6. Nebengruppe, wurde die Hydrolyse von Elementen der 6. Nebengruppe untersucht. Hier zeigen sich bei Verwendung von trägerfreien Aktivitäten abweichende Resultate gegenüber der Literatur.Auf der Grundlage dieser Daten wurde ein Mehrsäulenexperiment für 7,4-s 265Sg (Element 106) vorbereitet, für dessen Einsatz sowohl ein drehendes Targetradsystem für eine erhöhte Produktionsrate getestet wurde, als auch der Einsatz von speziell funktionalisierten Ionenaustauscherharzen.

Optical resonances of sphere-on-plane geometries

The optical resonances of metallic nanoparticles placed at nanometer distances from a metal plane were investigated. At certain wavelengths, these “sphere-on-plane” systems become resonant with the incident electromagnetic field and huge enhancements of the field are predicted localized in the small gaps created between the nanoparticle and the plane. An experimental architecture to fabricate sphere-on-plane systems was successfully achieved in which in addition to the commonly used alkanethiols, polyphenylene dendrimers were used as molecular spacers to separate the metallic nanoparticles from the metal planes. They allow for a defined nanoparticle-plane separation and some often are functionalized with a chromophore core which is therefore positioned exactly in the gap. The metal planes used in the system architecture consisted of evaporated thin films of gold or silver. Evaporated gold or silver films have a smooth interface with their substrate and a rougher top surface. To investigate the influence of surface roughness on the optical response of such a film, two gold films were prepared with a smooth and a rough side which were as similar as possible. Surface plasmons were excited in Kretschmann configuration both on the rough and on the smooth side. Their reflectivity could be well modeled by a single gold film for each individual measurement. The film has to be modeled as two layers with significantly different optical constants. The smooth side, although polycrystalline, had an optical response that was very similar to a monocrystalline surface while for the rough side the standard response of evaporated gold is retrieved. For investigations on thin non-absorbing dielectric films though, this heterogeneity introduces only a negligible error. To determine the resonant wavelength of the sphere-on-plane systems a strategy was developed which is based on multi-wavelength surface plasmon spectroscopy experiments in Kretschmann-configuration. The resonant behavior of the system lead to characteristic changes in the surface plasmon dispersion. A quantitative analysis was performed by calculating the polarisability per unit area /A treating the sphere-on-plane systems as an effective layer. This approach completely avoids the ambiguity in the determination of thickness and optical response of thin films in surface plasmon spectroscopy. Equal area densities of polarisable units yielded identical response irrespective of the thickness of the layer they are distributed in. The parameter range where the evaluation of surface plasmon data in terms of /A is applicable was determined for a typical experimental situation. It was shown that this analysis yields reasonable quantitative agreement with a simple theoretical model of the sphere-on-plane resonators and reproduces the results from standard extinction experiments having a higher information content and significantly increased signal-to-noise ratio. With the objective to acquire a better quantitative understanding of the dependence of the resonance wavelength on the geometry of the sphere-on-plane systems, different systems were fabricated in which the gold nanoparticle size, type of spacer and ambient medium were varied and the resonance wavelength of the system was determined. The gold nanoparticle radius was varied in the range from 10 nm to 80 nm. It could be shown that the polyphenylene dendrimers can be used as molecular spacers to fabricate systems which support gap resonances. The resonance wavelength of the systems could be tuned in the optical region between 550 nm and 800 nm. Based on a simple analytical model, a quantitative analysis was developed to relate the systems’ geometry with the resonant wavelength and surprisingly good agreement of this simple model with the experiment without any adjustable parameters was found. The key feature ascribed to sphere-on-plane systems is a very large electromagnetic field localized in volumes in the nanometer range. Experiments towards a quantitative understanding of the field enhancements taking place in the gap of the sphere-on-plane systems were done by monitoring the increase in fluorescence of a metal-supported monolayer of a dye-loaded dendrimer upon decoration of the surface with nanoparticles. The metal used (gold and silver), the colloid mean size and the surface roughness were varied. Large silver crystallites on evaporated silver surfaces lead to the most pronounced fluorescence enhancements in the order of 104. They constitute a very promising sample architecture for the study of field enhancements.

Laboratory study on the optical properties of absorbing atmospheric aerosols and field applications

The interaction between aerosols and sun light plays an important role in the radiative balance of Earth’s atmosphere. This interaction is obtained by measuring the removal (extinction), redistribution (scattering), and transformation into heat (absorption) of light by the aerosols; i.e. their optical properties. Knowledge of these properties is crucial for our understanding of the atmospheric system. rn Light absorption by aerosols is a major contributor to the direct and indirect effects on our climate system, and an accurate and sensitive measurement method is crucial to further our understanding. A homebuilt photoacoustic sensor (PAS), measuring at a 532nm wavelength, was fully characterized and its functionality validated for measurements of absorbing aerosols. The optical absorption cross-sections of absorbing polystyrene latex spheres, to be used as a standard for aerosol absorption measurements, were measured and compared to literature values. Additionally, a calibration method using absorbing aerosol of known complex refractive index was presented.rn A new approach to retrieve the effective broadband refractive indices (mbroad,eff) of aerosol particles by a white light aerosol spectrometer (WELAS) optical particle counter (OPC) was achieved. Using a tandem differential mobility analyzer (DMA)-OPC system, the nbroad,eff are obtained for both laboratory and field applications. This method was tested in the laboratory using substances with a wide range of optical properties and it was used in ambient measurements to retrieve the nbroad,eff of biomass burning aerosols in a nationwide burning event in Israel. The retrieved effective broadband refractive indices for laboratory generated scattering aerosols were: ammonium sulfate (AS), glutaric acid (GA), and sodium chloride, all within 4% of literature values. For absorbing substances, nigrosine and various mixtures of nigrosine with AS and GA were measured, as well as a lightly absorbing substance, Suwannee river fulvic acid (SRFA). For the ambient measurements, the calibration curves generated from this method were to follow the optical evolution of biomass burning (BB) aerosols. A decrease in the overall aerosol absorption and scattering for aged aerosols during the day after the fires compared to the smoldering phase of the fires was found. rn The connection between light extinction of aerosols, their chemical composition and hygroscopicity for particles with different degrees of absorption was studied. The extinction cross-section (σext) at 532nm for different mobility diameters was measured at 80% and 90% relative humidity (RH), and at an RH<10%. The ratio of the humidified aerosols to the dry ones, fRHext(%RH,Dry), is presented. For purely scattering aerosols, fRHext(%RH,Dry) is inversely proportional with size; this dependence was suppressed for lightly absorbing ones. In addition, the validity of the mixing rules for water soluble absorbing aerosols is explored. The difference between the derived and calculated real parts of the complex RIs were less than 5.3% for all substances, wavelengths, and RHs. The obtained imaginary parts for the retrieved and calculated RIs were in good agreement with each other, and well within the measurement errors of retrieval from pulsed CRD spectroscopy measurements. Finally, a core-shell structure model is also used to explore the differences between the models, for substances with low growth factors, under these hydration conditions. It was found that at 80% RH and for size parameters less than 2.5, there is less than a 5 % difference between the extinction efficiencies calculated with both models. This difference is within measurement errors; hence, there is no significant difference between the models in this case. However, for greater size parameters the difference can be up to 10%. For 90% RH the differences below a size parameter of 2.5 were up to 7%.rn Finally, the fully characterized PAS together with a cavity ring down spectrometer (CRD), were used to study the optical properties of soot and secondary organic aerosol (SOA) during the SOOT-11 project in the AIDA chamber in Karlsruhe, Germany. The fresh fractal-like soot particles were allowed to coagulate for 28 hours before stepwise coating them with SOA. The single scattering albedo for fresh fractal-like soot was measured to be 0.2 (±0.03), and after allowing the soot to coagulate for 28 hours and coating it with SOA, it increased to 0.71(±0.01). An absorption enhancement of the coated soot of up to 1.71 (±0.03) times from the non-coated coagulated soot was directly measured with the PAS. Monodisperse measurements of SOA and soot coated with SOA were performed to derive the complex refractive index (m) of both aerosols. A complex refractive index of m = 1.471(±0.008) + i0.0(±0.002) for the SOA-αO3 was retrieved. For the compact coagulated soot a preliminary complex refractive index of m = 2.04(+0.21/-0.14) + i0.34(+0.18/-0.06) with 10nm(+4/-6) coating thickness was retrieved.rn These detail properties can be use by modelers to decrease uncertainties in assessing climatic impacts of the different species and to improve weather forecasting.rn