Comparing Image Quality in Phase Contrast subμ\mu X-Ray Tomography -- A Round-Robin Study

How to evaluate and compare image quality from different sub-micrometer (sub$\mu$) CT scans? A simple test phantom made of polymer microbeads is used for recording projection images as well as 13 CT scans in a number of commercial and non-commercial scanners. From the resulting CT images, signal and noise power spectra are modeled for estimating volume signal-to-noise ratios (3D SNR spectra). Using the same CT images, a time- and shape-independent transfer function (MTF) is computed for each scan, including phase contrast effects and image blur ($\mathrm{MTF_{blur}}$). The SNR spectra and MTF of the CT scans are compared to 2D SNR spectra of the projection images. In contrary to 2D SNR, volume SNR can be normalized with respect to the object's power spectrum, yielding detection effectiveness (DE) a new measure which reveals how technical differences as well as operator-choices strongly influence scan quality for a given measurement time. Using DE, both source-based and detector-based sub$\mu$ CT scanners can be studied and their scan quality can be compared. Future application of this work requires a particular scan acquisition scheme which will allow for measuring 3D signal-to-noise ratios, making the model fit for 3D noise power spectra obsolete

Microwave spectroscopy on heavy-fermion systems: probing the dynamics of charges and magnetic moments

Investigating solids with light gives direct access to charge dynamics, electronic and magnetic excitations. For heavy fermions, one has to adjust the frequency of the probing light to the small characteristic energy scales, leading to spectroscopy with microwaves. We review general concepts of the frequency-dependent conductivity of heavy fermions, including the slow Drude relaxation and the transition to a superconducting state, which we also demonstrate with experimental data taken on UPd2Al3. We discuss the optical response of a Fermi liquid and how it might be observed in heavy fermions. Microwave studies with focus on quantum criticality in heavy fermions concern the charge response, but also the magnetic moments can be addressed via electron spin resonance (ESR). We discuss the case of YbRh2Si2, the open questions concerning ESR of heavy fermions, and how these might be addressed in the future. This includes an overview of the presently available experimental techniques for microwave studies on heavy fermions, with a focus on broadband studies using the Corbino approach and on planar superconducting resonators.Comment: 11 pages, 6 figures, proceedings of QCnP 201

Multi-Lens Array Full-Field X-ray Microscopy

X-ray full-field microscopy at laboratory sources for photon energies above 10 keV suffers from either long exposure times or low resolution. The photon flux is mainly limited by the objectives used, having a limited numerical aperture NA. We show that this can be overcome by making use of the cone-beam illumination of laboratory sources by imaging the same field of view (FoV) several times under slightly different angles using an array of X-ray lenses. Using this technique, the exposure time can be reduced drastically without any loss in terms of resolution. A proof-of-principle is given using an existing laboratory metal-jet source at the 9.25 keV Ga Kα-line and compared to a ray-tracing simulation of the setup

Elucidating the Sectioning Fragmentation Mechanism in Silica-Supported Olefin Polymerization Catalysts with Laboratory-Based X-Ray and Electron Microscopy

Strict morphological control over growing polymer particles is an indispensable requirement in many catalytic olefin polymerization processes. In catalysts with mechanically stronger supports, e. g., polymerization-grade silicas, the emergence of extensive cracks via the sectioning fragmentation mechanism requires severe stress build-up in the polymerizing catalyst particle. Here, we report on three factors that influence the degree of sectioning in silica-supported olefin polymerization catalysts. Laboratory-based X-ray nano-computed tomography (nanoCT) and focused ion beam-scanning electron microscopy (FIB-SEM) were employed to study catalyst particle morphology and crack propagation in two showcase catalyst systems, i.e., a zirconocene-based catalyst (i.e., Zr/MAO/SiO2, with Zr=2,2’-biphenylene-bis-2-indenyl zirconium dichloride and MAO=methylaluminoxane) and a Ziegler-Natta catalyst (i.e., TiCl4/MgCl2/SiO2), during slurry-phase ethylene polymerization. The absence of extensive macropores in some of the catalysts’ larger constituent silica granulates, a sufficient accessibility of the catalyst particle interior at reaction onset, and a high initial polymerization rate were found to favor the occurrence of the sectioning pathway at different length scales. While sectioning is beneficial for reducing diffusion limitations, its appearance in mechanically stronger catalyst supports can indicate a suboptimal support structure or unfavourable reaction conditions

Solid-phase-assisted synthesis of targeting peptide-PEG-oligo(ethane amino)amides for receptor-mediated gene delivery.

In the forthcoming era of cancer gene therapy, efforts will be devoted to the development of new efficient and non-toxic gene delivery vectors. In this regard, the use of Fmoc/Boc-protected oligo(ethane amino)acids as building blocks for solid-phase-supported assembly represents a novel promising approach towards fully controlled syntheses of effective gene vectors. Here we report on the synthesis of defined polymers containing the following: (i) a plasmid DNA (pDNA) binding domain of eight succinoyl-tetraethylenpentamine (Stp) units and two terminal cysteine residues; (ii) a central polyethylene glycol (PEG) chain (with twenty-four oxyethylene units) for shielding; and (iii) specific peptides for targeting towards cancer cells. Peptides B6 and c(RGDfK), which bind transferrin receptor and αvβ3 integrin, respectively, were chosen because of the high expression of these receptors in many tumoral cells. This study shows the feasibility of designing these kinds of fully controlled vectors and their success for targeted pDNA-based gene transfer

Hochauflösende Röntgenbildgebung auf Basis einer Flüssigmetall-Anoden-Quelle mit und ohne Röntgenoptiken

With increasing miniaturization in industry and medical technology, non-destructive testing techniques are an area of everincreasing importance. In this framework, X-ray microscopy offers an efficient tool for the analysis, understanding and quality assurance of microscopic species, in particular as it allows reconstructing three-dimensional data sets of the whole sample’s volumevia computed tomography (CT). The following thesis describes the conceptualization, design, construction and characterization of a compact laboratory-based X-ray microscope in the hard X-ray regime around 9 keV, corresponding to a wavelength of 0.134 nm. Hereby, the main focus is on the optimization of resolution and contrast at relatively short exposure times. For this, a novel liquid-metal-jet anode source is the basis. Such only recently commercially available X-ray source reaches a higher brightness than other conventional laboratory sources, i.e. the number of emitted photons (X-ray quanta) per area and solid angle is exceptionally high. This is important in order to reach low exposure times. The reason for such high brightness is the usage of the rapidly renewing anode out of liquid metal which enables an effective dissipation of heat, normally limiting the creation of high intensities on a small area. In order to cover a broad range of different samples, the microscope can be operated in two modes. In the “micro-CT mode”, small pixels are realized with a crystal-scintillator and an optical microscope via shadow projection geometry. Therefore, the resolution is limited by the emitted wavelength of the scintillator, as well as the blurring of the screen. However, samples in the millimeter range can be scanned routinely with low exposure times. Additionally, this mode is optimized with respect to in-line phase contrast, where edges of an object are enhanced and thus better visible. In the second “nano-CT mode”, a higher resolution can be reached via X-ray lenses. However, their production process is due to the physical properties of the hard X-ray range - namely high absorption and low diffraction - extremely difficult, leading typically to low performances. In combination with a low brightness, this leads to long exposure times and high requirements in terms of stability, which is one of the key problems of laboratory-based X-ray microscopy. With the here-developed setup and the high brightness of its source, structures down to 150 nm are resolved at moderate exposure times (several minutes per image) and nano-CTs can be obtained.Mit zunehmender Miniaturisierung in Industrie und Medizintechnik werden zerstörungsfreie Prüfverfahren immer wichtiger. In diesem Umfeld bietet Röntgenmikroskopie ein effizientes Instrument zu Analyse, Verständnis und Qualitätssicherung mikroskopischer Proben, insbesondere da sie im Rahmen der Computer-Tomografie (CT) die Aufnahme dreidimensionaler Datensätze des gesamten Probenvolumens ermöglicht. Die vorliegende Arbeit befasst sich mit Konzeption, Design, Aufbau und Charakterisierung eines kompakten Labor-Röntgenmikroskops im harten Röntgenbereich bei 9 keV, bzw. einer Wellenlänge von 0.134 nm. Im Fokus liegt dabei die Optimierung von Auflösung und Kontrast bei möglichst kurzen Belichtungszeiten. Hier für bildet die Basis eine neuartige Flüssig-Metall- Anoden Röntgenquelle. Solche erst seit kurzem kommerziell verfügbare Quellen erreichen eine höhere Brillianz als konventionelle Laborquellen, d.h. dass die Anzahl der emittierten Photonen (Röntgenquanten) pro Fläche und Raumwinkel außergewöhnlich hoch ist. Dies ist ein entscheidender Faktor, um nötige Belichtungszeiten zu verringern. Der Grund für die hohe Brillianz ist die Verwendung einer sich sehr schnell erneuernden Anode aus flüssigem Metall. Diese ermöglicht die effektive Abfuhr von Wärme, welche normalerweise die Erzeugung von höheren Intensitäten auf kleinerer Fläche limitiert. Um ein möglichst großes Spektrum an Proben abzubilden, kann das Mikroskop in zwei Modi betrieben werden. Im ”Mikro-CT Modus“ werden kleine Pixel mit Hilfe eines Kristall-Leuchtschirms und einem Lichtmikroskop über das Schattenwurfprinzip erreicht, weswegen dessen Auflösung durch die Wellenlänge des emittierten Lichts und die Unschärfe des Schirms beschränkt ist. Dafür können Proben im Millimeterbereich bei geringen Belichtungszeiten standardmäßig aufgenommen werden. Zudem wurde dieser Modus auf inline Phasen-Kontrast optimiert, bei welchem die Kanten eines Objekts durch Interferenz überhöht dargestellt werden und somit besser sichtbar sind. Im zweiten ”Nano-CT Modus“ kann eine erhöhte Auflösung mit Hilfe von Röntgenlinsen erreicht werden. Deren Herstellung ist aber aufgrund der physikalische Eigenschaften im harten Röntgenbereichs - nämlich starke Absorption und schwache Brechung - technisch extrem schwierig und meist mit einer sehr geringe optischen “Leistung” verbunden. Dies führt in Kombination mit einer geringen Brillianz zu sehr langen Belichtungszeiten und hohen Anforderungen an die Stabilität, was ein Kernproblem der auf Laborquellen basierenden Röntgenmikroskope darstellt. Mit der hier entwickelten Anlage können durch die hohe Brillianz der verwendeten Quelle bei moderaten Belichtungszeiten (wenige Minuten pro Bild) Strukturen der Größe 150 nm voneinander getrennt, sowie Nano-CTs aufgenommen werden

Laboratory-Based Nano-Computed Tomography and Examples of Its Application in the Field of Materials Research

In a comprehensive study, we demonstrate the performance and typical application scenarios for laboratory-based nano-computed tomography in materials research on various samples. Specifically, we focus on a projection magnification system with a nano focus source. The imaging resolution is quantified with common 2D test structures and validated in 3D applications by means of the Fourier Shell Correlation. As representative application examples from nowadays material research, we show metallization processes in multilayer integrated circuits, aging in lithium battery electrodes, and volumetric of metallic sub-micrometer fillers of composites. Thus, the laboratory system provides the unique possibility to image non-destructively structures in the range of 170–190 nanometers, even for high-density materials