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- Compound refractive lens (2)
- Color X-ray camera (1)
- Elemental distribution (1)
- Full field micro-XRF (1)
- Micro-XAS (1)
- Nematode (1)
- Silicon impurities (1)
- Solar cell (1)
- TXRF (1)
- X-ray absorption near edge structure (XANES) (1)
A study regarding the possibility to use compound refractive lenses (CRLs) for X-ray absorption spectroscopy (XAS) was conducted. For XAS measurements the energy of the monochromatic incident beam has to be tuned over an energy range which is broader than the energy bandwidth of a CRL. To prove that µ-XAS with compound refractive lenses is possible, it had to be investigated how changes in the energy influence the beam parameters. This was done by tuning the energy around the nominal energy of the lens and recording images with a high resolution X-ray imaging setup. To investigate the changes in the spot size the scintillator was placed at the nominal focal distance and scans along the beam axis were performed. The effect on the photon flux of the incident beam due to absorption in the lens was investigated by performing XANES measurement on different reference materials with and without CRL. The results of these measurements using a CRL designed for 9 keV are shown and discussed.
We report on the trace analysis of copper and iron impurities in multicrystalline silicon wafers with the microbeam X-ray fluorescence (µ-XRF) technique. The efficiency of solar cells, which are based on multicrystalline silicon wafers, is strongly influenced by minor contamination with metals such as copper and iron. Application of compound refractive lenses (CRLs) in µ-XRF allows versatile two-dimensional mapping of relevant contaminations and localization of their sites of deposition. In this context, the measured bulk average limit of detection (LOD) was one picogram of iron and copper per gram of silicon. We suggest that µ-XRF is a valuable tool for non-destructive spatial (3D) quantification of metal impurities in a wide range of materials and devices whose functioning could be critically affected by impurities.
The distribution and speciation of zinc were studied in the body of female specimens of the soil-inhabiting, plant-feeding nematode, Xiphinema vuittenezi treated with nano-ZnO and its bulk counterpart. Lyophilized nematodes were studied by X-ray absorption near edge structure spectrometry (XANES) in order to characterize the zinc speciation. Furthermore, in the cross-sections prepared by focused ion beam technique, elemental maps were obtained using the electron probe microanalysis (EPMA) technique. XANES spectra were collected from three different regions (head, midbody and tail region) of nematodes in case of two different treatments (50 mg/L bulk and nano-ZnO suspension, 24 h long treatment). The sample spectra were fitted by the spectra of several reference compounds, the main components of the fitted spectra are the following in all cases: bulk/nano-ZnO; ZnHis and Zn3(PO4)2 * xH2O. Consequently, partial biotransformation takes place for both treatments, histidine- and phosphate-rich ligands play dominant role in the binding of zinc. According to the result of the EPMA analysis, it can be established that the distribution of zinc correlates with the calcium and phosphorus distribution for both treatments. Considering the results of the investigations performed by the two microanalytical techniques, it is likely that calcium phosphate granules were formed in order to bind zinc and hereby to take part in zinc detoxification. Apparent difference in the behavior of bulk and nano-sized ZnO in the body of the investigated nematodes was not found.
Absorption effects and the impact of specimen shape on TXRF analysis has been discussed intensively. Model calculations indicated that ring shaped specimens should give better results in terms of higher counts per mass signals than filled rectangle or circle shaped specimens. One major reason for the difference in signal is shading effects. Full field micro-XRF with a color X-ray camera (CXC) was used to investigate shading, which occurs when working with small angles of excitation as in TXRF. The device allows monitoring the illuminated parts of the sample and the shaded parts at the same time. It is expected that sample material hit first by the primary beam shade material behind it. Using the CXC shading could be directly visualized for the high concentration specimens.
In order to compare the experimental results with calculation of the shading effect the generation of controlled specimens is crucial. This was achieved by 'drop on demand' technology. It allows generating uniform, microscopic deposits of elements. The experimentally measured shadings match well with those expected from calculation.