Altapova V.R., Ershov A., Rolo T.d.S., Reznikova E., Mohr J., Pivovarov Y.L., Pichugin V.F., Baumbach G.T.

in Journal of Surface Investigation, 6 (2012) 394-397. DOI:10.1134/S1027451012050035

Abstract

The imaging methods used at the ANKA Synchrotron Light Source (Institute for Synchrotron Radiation, Karlsruhe Institute of Technology) are briefly reviewed. Examples of recent applications of the phase-contrast imaging method using a grating interferometer and fast radiography with optic flow data analysis to study static and moving biological objects are presented. © 2012 Pleiades Publishing, Ltd.

Alaribe L., Disch C., Fauler A., Engels R., Keller E., Cecilia A., Rolo T.D.S., Hamann E., Fiederle M.

in IEEE Nuclear Science Symposium Conference Record (2012) 1567-1571, 6154633. DOI:10.1109/NSSMIC.2011.6154633

Abstract

Currently, there is a great interest in the research and development of SrI 2:Eu 2+ scintillating crystals. The high light yield, high density (4.6 g/cm 3) and high effective atomic number (49.4) make the Eu 2+-activated SrI 2 suitable for use as x-ray and gamma ray detector. SrI 2:Eu 2+-single crystals were grown with the vertical Bridgman technique in silica ampoules to prevent melt hydration and oxygen contamination during the crystal growth. For measurements, crystals were hermetically encapsulated in aluminum containers with quartz glass optical windows. The radioluminescence spectra of the SrI 2:Eu 2+-samples show maximum at 431 nm and 432 nm for the 5% and 6% dopant concentrations respectively. The light yield of the bulk samples was up to 80 000 photons/MeV and up to 119 000 photons/MeV for a 360 μm sample integrated in an x-ray imaging setup. © 2011 IEEE.

Alaribe L., Disch C., Fauler A., Engels R., Keller E., Cecilia A., Dos Santos Rolo T., Fiederle M.

in Materials Research Society Symposium Proceedings, 1341 (2012) 21-26. DOI:10.1557/opl.2011.1275

Abstract

Eu 2+- activated strontium iodide is a promising material for x-ray and gamma ray detector. A lot of difficulties are though encountered growing strontium iodide crystals due to the high oxygen-sensitivity, hygroscopic property and high impurity concentration. Single crystals of Srl 2:Eu were grown from zone refined starting materials in silica ampoules. The crystals showed good optical qualities. The light yield of two samples cut from the same ingot was determined to be 53 000 photons/MeV and 119±22 photons/keV for a 0.4 cm 3 sample and a 360 μm sample respectively, indicating some level of light trapping in the bulk sample. Keywords: scintillator, Bridgman growth method, energy resolution. © 2011 Materials Research Society.

Haas D., Mexner W., Spangenberg T., Cecilia A., Vagovic P., Kopmann A., Balzer M., Vogelgesang M., Pasic H., Chilingaryan S.

in PCaPAC 2012 – 9th International Workshop on Personal Computers and Particle Accelerator Controls (2012) 103-105.

Abstract

X-ray imaging permits to spatially resolve the 2D and 3D structure in materials and organisms, which is crucial for the understanding of their properties. Additional temporal resolution of structure evolution gives access to dynamics of processes and allows to understand functionality of devices and organisms with the goal to optimize technological processes. Such time-resolved dynamic analysis of micro-sized structures is now possible by aid of ultrafast tomography, as being developed at the TopoTomo beamline of the synchrotron light source ANKA. At TopoTomo, the whole experimental workflow has been significantly improved in order to decrease the total duration of a tomography experiment down to the range of minutes. To meet these requirements, detectors and the computing infrastructure have been optimized, comprising a Tango-based control system for ultra fast tomography with a data throughput of several 100 MB/s. Multi-GPU based computing allows for high speed data processing by using a special reconstruction scheme. Furthermore the data management infrastructure will allow for a life cycle management of data sets accumulating several TByte/day. The final concept will also be part of the IMAGE beamline, which is going to be installed in 2013. © 2012 by the respective authors.