X-ray 2D Radiography (Transmission Image)-FPD
X-ray 2D Radiography (Transmission Image) - FPD is a cutting-edge imaging technique utilized for capturing high-resolution images of objects or materials in two dimensions. This method employs a Flat Panel Detector (FPD) to detect X-ray photons transmitted through the sample, producing detailed transmission images.
The mechanism of X-ray 2D radiography involves passing X-ray radiation through the object or material being examined. The FPD, composed of a scintillator layer and an array of photodiodes, converts the X-ray photons into visible light photons upon interaction. These light photons are then detected and converted into electrical signals, which are processed to generate transmission images with exceptional clarity and resolution.
By analyzing the intensity and spatial distribution of transmitted X-rays, X-ray 2D Radiography provides valuable insights into the internal structure, density variations, and defects within the sample. This non-destructive imaging technique finds wide-ranging applications in fields such as industrial inspection, medical diagnostics, and materials science, facilitating accurate characterization and quality assessment of diverse materials and components.
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 |