(160kV) 3D X-ray Nano-Scale Computed Tomography-HPC
The (160kV) 3D X-ray Nano-Scale Computed Tomography-High-Performance Computing (HPC) represents an advanced imaging technique that seamlessly integrates a high-energy X-ray source with sophisticated computational capabilities for detailed three-dimensional analysis of nanoscale structures . This cutting-edge approach is designed to unveil the intricate internal features of materials with unprecedented precision.
At its core, the method involves subjecting a sample to rotational scanning, where high-energy X-rays at 160 kilovolts penetrate through the material, capturing projections at multiple angles. These X-ray projections, showcasing the material's attenuation characteristics, form the basis of a comprehensive dataset. What sets this technique apart is the subsequent reconstruction process, empowered by High-Performance Computing. The computational prowess enables the rapid and intricate reconstruction of a high-resolution 3D volume from the acquired projections.
The (160kV) 3D X-ray Nano-Scale Computed Tomography-HPC approach provides researchers and scientists with an unparalleled tool for non-destructive exploration and analysis of nanoscale structures. From materials science to biology, the application of this technique opens new avenues for understanding and characterizing the internal morphology, distribution, and features of nanomaterials, contributing significantly to advancements in diverse scientific fields.
Excillum NanoTube N3 X-ray Source
The Excillum NanoTube N3 provides geometric-magnification X-ray imaging systems with industry-leading stability and resolution without the need for manual adjusting.
Advanced tungsten-diamond transmission target technology and sophisticated electron optics form the foundation of the Excillum NanoTube N3. Every time, the smallest, roundest spot is produced owing to the automatic e-beam focusing and astigmatism correction.
Moreover, the NanoTube N3 has the distinctive capability of monitoring and reporting the current spot size inside. Furthermore, cutting-edge cooling and thermal design produce extraordinary stability over lengthy exposures. This permits a real resolution of 150 nm lines and spaces.
Dectris EIGER2 R CdTe 500K Detector
Number of modules (WxH) |
1 x 1 = 1 |
Sensor | Cadmium Telluride (CdTe) |
Sensor material | Silicon (Si) |
Sensor thickness | 750 µm |
Pixel size (W x H) | 75 µm x 75 µm |
Pixel array format (W x H) | 1028 pixels x 512 pixels = 526 336 pixels |
Active area (W x H) | 77.1mm x 38.4mm = 2977.99mm 2 |
Intra-module gap | 2 pixels wide vertical gap in the center of each module |
Defective pixels | < 0.1% |
Image bit depth | 32 bit or 16 bit |
Readout bit depth | 16 bits |
Maximum count rate | 9.8 × 10 8 photons/s/mm 2 |
Adjustable threshold range | 4keV to 30keV |
Energy range | 8keV to 25keV |
Number of thresholds | two independent thresholds |
Readout time | continuous readout with 100 ns dead time |
Maximum frame rate | 100 Hz |
Point-spread function | 1 pixel (FWHM) |
Connection to detector control unit | 1 x LC/UPC duplex fiber optic connectors |
Power supply | External power supply unit |
Software interface | HTTP REST interface |
Dimensions (W x H x D) | 114mm x 92mm x 241.5mm |
Weight | 3.7kg |
Maximum operating altitude | 2000m asl |
Lab Motion Systems RT150ST
Bearing type | air bearing |
Max. speed | 725 RPM |
Max.axial load | 226N |
Radial error motion | < 100nm |
Axial error motion | <50nm |
Angular accuracy | ± 6.9 arcsec |
Nominal torque | 1.5Nm |
Peak torque | 2.5Nm |
Total mass | 6.2kg |
Lab Motion Systems XY150B-12
Bearing type | ball bearing |
Stroke | ±6mm |
Load capacity | 10kg |
Min. Incr. motion | 0.1 µm |
Repeatability | ±0.2 µm |
Speed | 0.22mm/s |
Total mass | 2.1kg |
Material | coated aluminum |
Optimal compatibility |
RT150 RT250 |