The Bruker Xtreme II is part of the user facilities at the OncoRay Center at HZDR Dresden:

Functions:
- Bioluminescence Imaging (BLI)
- Multi-Spectral Fluorescence Imaging (MS FLI)
- Direct Radioistopic Imaging (DRITM)
- Cherenkov …

The Phoenix Nanotom® M is a nanofocus X-ray CT system for scientific and industrial computed tomography (microCT and nanoCT®) and 3D metrology. The system realizes a unique spatial and contrast resolution on a wide sample …

The Göttingen Instrument for Nano-Imaging with X-Rays (GINIX) is a dedicated endstation for coherent nano-diffraction and imaging at the Coherence Beamline P10. It is located in the second experimental hutch (EH2).

The Coherence Beamline P10 …

The High Energy Density (HED) scientific instrument, together with the HIBEF user consortium, is a new, unique platform for experiments combining hard X-ray FEL radiation and the capability to generate matter under extreme conditions of …

An industrial X-ray tube (ISOVOLT 450M1/25-55 from GE Sensing & Inspection Technologies GmbH) was used for the bubble visualization experiments (Fig. 3a). The high power ISOVOLT X-ray source operating with a maximum voltage of 320 …

The scope of the MID instrument are material science experiments using the unprecedented coherent properties of the X-ray laser beams of the European XFEL. The scientific applications reach from condensed matter physics, studying for example …

The solidification experiments are by an X-ray radiographic set-up delivering images with a spatial resolution of a few microns. A microfocus X-ray tube equipped with a tungsten target (phoenix X-ray XS225D-OEM) has been utilized. After …

The imaging beamline (IBL) is dedicated to micro- and nanotomography at energies between 5 keV and 50 keV. The flexible design of the experimental stations allows for the investigation of samples with diameters ranging seamlessly …

he second experimental hutch contains the micro tomography setup of P05. At a sample distance of 87 m from the source, the horizontal full width at half maximum of the beam is 5.6 mm which …

The nanotomography endstation in the experimental hutch 1, designed to allow 3D resolutions of below 100 nm, is currently under construction. As X-ray optics we will use compound refractive lenses (CRLs), made from SU-8 polymer …

The High Energy Materials Science Beamline HEMS at PETRA III satisfies high energy x-ray diffraction (XRD) and imaging techniques. It is tunable in the range 30 to 200 keV, and it is optimized for micrometer …

The Perkin Elmer RID1024 is an X-ray detector.

The Thales TH9438 9“ is an X-ray detector.

The measurement principle for both X-ray and neutron imaging is based on the material-dependent attenuation of the transmitted X-ray respectively neutron beam intensity. The output of all imaging experiments are grey-scale image sequences showing the …

Since late 2016, the Institute for Applied Materials (KIT) has an X-ray microscope (Xradia 520 Versa) with sub-μm resolution for 3D X-ray microscopy, which offers a spatial resolution below 0.7 µm with available voxel sizes …

NanoCT (Xradia Ultra 810 X-ray microscope) enables the non-destructive structural characterization of three-dimensional samples with resolution down to 50 nm. In this non-invasive X-ray microscopy technique, the sample is positioned in the focal spot of …