(160kV) 3D X-ray Nano-Scale Computed Tomography-FPD
The (160kV) 3D X-ray Nano-Scale Computed Tomography with Flat Panel Detector (FPD) is an advanced imaging system designed for extremely detailed examination of objects at the nano-scale. Using a powerful 160kV X-ray source, this technology captures detailed 2D X-ray projections as the object rotates. The inclusion of a Flat Panel Detector ensures efficient detection of transmitted X-rays, converting them into electronic signals for digital processing.
Through smart algorithms, a 3D volumetric dataset is carefully reconstructed from the 2D images, offering unprecedented resolution. This innovative approach allows for nano-scale imaging, providing researchers and professionals with detailed insights into the internal structure, composition, and morphology of various materials. The (160kV) 3D X-ray Nano-Scale Computed Tomography-FPD system is at the forefront of cutting-edge imaging technology, with applications ranging from materials science to biological research and industrial analysis.
In the video, a battery sample was recorded using our self-developed nano-CT system at 100 fps and played at 2x speed.
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 |