Production of antihydrogen via double charge exchange

Spectroscopy of the 1S-2S transition of antihydrogen confined in a neutral atom trap and comparison with the equivalent spectral line in hydrogen will provide an accurate test of CPT symmetry and the first one in a mixed baryon-lepton system. Also, with neutral antihydrogen atoms, the gravitational interaction between matter and antimatter can be tested unperturbed by the much stronger Coulomb forces.rnAntihydrogen is regularly produced at CERN's Antiproton Decelerator by three-body-recombination (TBR) of one antiproton and two positrons. The method requires injecting antiprotons into a cloud of positrons, which raises the average temperature of the antihydrogen atoms produced way above the typical 0.5 K trap depths of neutral atom traps. Therefore only very few antihydrogen atoms can be confined at a time. Precision measurements, like laser spectroscopy, will greatly benefit from larger numbers of simultaneously trapped antihydrogen atoms.rnTherefore, the ATRAP collaboration developed a different production method that has the potential to create much larger numbers of cold, trappable antihydrogen atoms. Positrons and antiprotons are stored and cooled in a Penning trap in close proximity. Laser excited cesium atoms collide with the positrons, forming Rydberg positronium, a bound state of an electron and a positron. The positronium atoms are no longer confined by the electric potentials of the Penning trap and some drift into the neighboring cloud of antiprotons where, in a second charge exchange collision, they form antihydrogen. The antiprotons remain at rest during the entire process, so much larger numbers of trappable antihydrogen atoms can be produced. Laser excitation is necessary to increase the efficiency of the process since the cross sections for charge-exchange collisions scale with the fourth power of the principal quantum number n.rnThis method, named double charge-exchange, was demonstrated by ATRAP in 2004. Since then, ATRAP constructed a new combined Penning Ioffe trap and a new laser system. The goal of this thesis was to implement the double charge-exchange method in this new apparatus and increase the number of antihydrogen atoms produced.rnCompared to our previous experiment, we could raise the numbers of positronium and antihydrogen atoms produced by two orders of magnitude. Most of this gain is due to the larger positron and antiproton plasmas available by now, but we could also achieve significant improvements in the efficiencies of the individual steps. We therefore showed that the double charge-exchange can produce comparable numbers of antihydrogen as the TBR method, but the fraction of cold, trappable atoms is expected to be much higher. Therefore this work is an important step towards precision measurements with trapped antihydrogen atoms.

Halogen-Kupfer-Austausch mit Kupferhypersilanid und Organylhalogeniden

Die Reaktion von Kupfertris(trimathylsilyl)silan (= Hypersilylkupfer, CuHyp) mit Iodoorganylverbindungen sollte analog zum Ullmann-Protokoll zum Halogen-Nukleophil-Austausch führen. Tatsächlich beobachteten wir zumeist die Bildung von Cuprio-Organylen, isolierbar in Form von mehrkernigen Neutralkomplexen aus dem Produkt und weiteren Äquivalenten von Hypersilylkupfer. Nach Zugabe von (weichen) Basen wie Trimethylphosphan kam es zur Auflösung dieser Komplexe und zur Bildung der erwarteten Silylorganyle. Von der systematischen Variation der eingesetzten Arene, Alkene und Alkine sowie ihrer Liganden versprachen wir uns tiefere Einsicht in die mechanistischen Zusammenhänge. Neben dem üblichen Halogen-Kupfer-Autausch konnten wir bei orthosubstituierten, bzw. zusätzlich tetramethylsubstituierten Diiodarenen einen einfachen Iod-Siyl-Autausch beobachten (vermutlich über Arinzwischenstufen), für Alkinedukte sogar eine doppelte Silylierung. Tatsächlich zeigen quantenchemische Berechnungen für CuHyp-Iodoorganyl-Systeme eine klare Präferenz von ullmannartigen Verläufen; andererseits führte Basenzugabe erst nachträglich zur Bildung von Ullmann-Produkten über die Auflösung der primären Komplexe. Innerhalb der üblicherweise gebildeten mehrkernigen Komplexe kommen Bindungen durch die Wechselwirkung unbesetzter σ*-Molekülorbitalee am Kupferzentrum von CuHyp und elektronenreichen bindenden Orbitalen in den Kupferorganyleinheiten zustande. Freie Elektronenpaare am Phosphor bei PMe3 könnten analog die Auflösung der Neutralkomplexe und die Bildung von vierkernigen Kupfer(III)-Intermediaten zwischen den Kupferorganyleinheiten und Iodsilan in der Lösung bewirken, die aufgrund ihrer strukturellen und energetischen Besonderheiten zu den erwarteten Ullmann-Produkten weiterreagieren würden. Die beobachteten Primärreaktionen verliefen dann offensichtlich über vergleichbare, aber unterschiedlich strukturierte Intermediate, vermutlich aufgrund der Tatsache, dass das eingesetzte CuHyp als Trimer vorliegt. Diese Annahme wird durch die direkte Silylierung von Iodalkinen gestützt, deren Dreifachbindungen möglicherweise als interne Base die trimeren in monomere CuHyp-Einheiten überführen. In eine ähnliche Richtung wäre die jüngst berichtete direkte Silylierung von Allylen bei Anwesenheit von elektronenreichen CN-Gruppen zu deuten.

Development, characterization, and application of flowing atmospheric-pressure afterglow ionization for mass spectrometric analysis of ambient organic aerosols

Addressing current limitations of state-of-the-art instrumentation in aerosol research, the aim of this work was to explore and assess the applicability of a novel soft ionization technique, namely flowing atmospheric-pressure afterglow (FAPA), for the mass spectrometric analysis of airborne particulate organic matter. Among other soft ionization methods, the FAPA ionization technique was developed in the last decade during the advent of ambient desorption/ionization mass spectrometry (ADI–MS). Based on a helium glow discharge plasma at atmospheric-pressure, excited helium species and primary reagent ions are generated which exit the discharge region through a capillary electrode, forming the so-called afterglow region where desorption and ionization of the analytes occurs. Commonly, fragmentation of the analytes during ionization is reported to occur only to a minimum extent, predominantly resulting in the formation of quasimolecular ions, i.e. [M+H]+ and [M–H]– in the positive and the negative ion mode, respectively. Thus, identification and detection of signals and their corresponding compounds is facilitated in the acquired mass spectra. The focus of the first part of this study lies on the application, characterization and assessment of FAPA–MS in the offline mode, i.e. desorption and ionization of the analytes from surfaces. Experiments in both positive and negative ion mode revealed ionization patterns for a variety of compound classes comprising alkanes, alcohols, aldehydes, ketones, carboxylic acids, organic peroxides, and alkaloids. Besides the always emphasized detection of quasimolecular ions, a broad range of signals for adducts and losses was found. Additionally, the capabilities and limitations of the technique were studied in three proof-of-principle applications. In general, the method showed to be best suited for polar analytes with high volatilities and low molecular weights, ideally containing nitrogen- and/or oxygen functionalities. However, for compounds with low vapor pressures, containing long carbon chains and/or high molecular weights, desorption and ionization is in direct competition with oxidation of the analytes, leading to the formation of adducts and oxidation products which impede a clear signal assignment in the acquired mass spectra. Nonetheless, FAPA–MS showed to be capable of detecting and identifying common limonene oxidation products in secondary OA (SOA) particles on a filter sample and, thus, is considered a suitable method for offline analysis of OA particles. In the second as well as the subsequent parts, FAPA–MS was applied online, i.e. for real time analysis of OA particles suspended in air. Therefore, the acronym AeroFAPA–MS (i.e. Aerosol FAPA–MS) was chosen to refer to this method. After optimization and characterization, the method was used to measure a range of model compounds and to evaluate typical ionization patterns in the positive and the negative ion mode. In addition, results from laboratory studies as well as from a field campaign in Central Europe (F–BEACh 2014) are presented and discussed. During the F–BEACh campaign AeroFAPA–MS was used in combination with complementary MS techniques, giving a comprehensive characterization of the sampled OA particles. For example, several common SOA marker compounds were identified in real time by MSn experiments, indicating that photochemically aged SOA particles were present during the campaign period. Moreover, AeroFAPA–MS was capable of detecting highly oxidized sulfur-containing compounds in the particle phase, presenting the first real-time measurements of this compound class. Further comparisons with data from other aerosol and gas-phase measurements suggest that both particulate sulfate as well as highly oxidized peroxyradicals in the gas phase might play a role during formation of these species. Besides applying AeroFAPA–MS for the analysis of aerosol particles, desorption processes of particles in the afterglow region were investigated in order to gain a more detailed understanding of the method. While during the previous measurements aerosol particles were pre-evaporated prior to AeroFAPA–MS analysis, in this part no external heat source was applied. Particle size distribution measurements before and after the AeroFAPA source revealed that only an interfacial layer of OA particles is desorbed and, thus, chemically characterized. For particles with initial diameters of 112 nm, desorption radii of 2.5–36.6 nm were found at discharge currents of 15–55 mA from these measurements. In addition, the method was applied for the analysis of laboratory-generated core-shell particles in a proof-of-principle study. As expected, predominantly compounds residing in the shell of the particles were desorbed and ionized with increasing probing depths, suggesting that AeroFAPA–MS might represent a promising technique for depth profiling of OA particles in future studies.