PIXIS-XF Fiber Optic Input X-ray Cameras from Princeton Instruments
Applications: X-ray micro tomography • X-ray phase contrast imaging • Protein Crystallography • TEM
 

  • Front and Back-illuminated CCD's supported
  • X-ray photon counting capability
  • Proprietary Fiber Bonding Process *
  • Custom fiber taper configurations available
  • Removable phosphor screen and Be window option
  • Files are compatible with FIT2D software from ESRF
  • Easy to synchronizing with external UNIBLITZ PlIr blade x-ray shutter (up to 30Kev)

 

 

The PIXIS-XF is an advanced cooled digital x-ray camera system designed for lens-less direct imaging of phosphor screens and other Lambertian sources. When used with the optional removable x-ray scintillator screen and the software-programmable, high-capacity or high-sensitivity amplifier, this system can effectively provide x-ray photon counting capability with up to 16-bit dynamic range. Phosphors screens are available for 8 and 17 keV at a emission wavelength of 550 nm.

If Flexibility Counts
The cameras are designed to detect x-ray photons for scientific research needs to be flexible. X-ray scattering from complex crystals such as proteins requires high dynamic range and low-noise readout, whereas scattering from materials like polymers, fibers, and powders requires deep cooling and rapid imaging to capture phase or morphological changes during thermal or mechanical processing.

Phosphors Screen Options

(1) Gadolinium Oxy-Sulfide (with Terbium) powder phosphor – Gd2O2S:Tb
Princeton Instruments has developed two phosphors for 8 keV and 17 keV X-ray energies based on Gd2O2S:Tb powder. To provide highest possible resolution, small grain material is used on a mirrored Mylar. When large image area, high efficiency and lower costs are the considerations these phosphors are recommended. The Gd2O2S:Tb is recommended for x-ray energies < 33 keV as it has higher absorption efficiency and the CsI:Tl is recommended for x-ray energies > 33keV.

(2) Cesium Iodide (with Thallium) crystalline phosphor
For the application where highest possible resolution is a must Princeton Instruments has developed phosphors based on CsI:Tl crystalline structure for 8 keV, 25 keV and 60 keV X-ray energies. The crystalline needle structure of CsI:Tl has a few advantages over the powder phosphors (though it has lower absorption at x-ray energies < 33 keV). The needle structure of CsI:Tl acts as a light guide to transmit visible light generated from the absorbed X-ray photons and provides higher resolution than powder phosphor and preserves resolution when x-ray energy changes a little from experiment to experiment, and  provides more uniform light output. A special coating over the needle structure developed to preserve the high resolution also protects it from the moisture in the atmosphere.

Gd2O2S:Tb (8 and 17 keV)

Gd2O2S:Tb 8 keV

Gd2O2S:Tb 17 keV

CsI (8 and 80 keV)

CsI 8 keV

CsI 80 keV

 

Model imaging array (pixels) pixel size (µm)
Energy Rande

Quantum Efficiency

Sensor Type

PIXIS-XF 1024F

1024 x 1024

13 x 13

<3.5 kev - >150 kev.

32% at550 nm

front-illuminated

PIXIS-XF 1024B

1024 x 1024

13 x 13

<3.5 kev - >150 kev.

97% at 550 nm

back-illuminated

PIXIS-XF 2048F

1340 x 1300

20 x 20

<3.5 kev - >150 kev.

32% at 550 nm20

front-illuminated

PIXIS-XF 2048B

1340 x 1300

20 x 20

<3.5 kev - >150 kev.

97% at 550 nm

back-illuminated

Download the new X-ray Camera brochure (26 MB)- completely revised

Micro Computer Tomography (µCT) 

 

Computer tomography (CT) has been used as one of the most versatile techniques in the medical field since 1973 for non-invasive investigations. Though CT has been used in many other fields such as industry, archaeology, life and geosciences, it is limited in spatial resolution. The best spatial resolution achievable by conventional CT instruments is ~ 0.5 mm. Unfortunately, to examine the internal structure of extremely small objects at a sub-millimeter scale, this technique is insufficient.

Micro computer tomography (µCT)overcomes this limitation with the availability of high-resolution, high-dynamic range CCD cameras, high-resolution scintillators, micro-focus X-ray tubes with an optical focal spot of < 1 µm (or synchrotron X-ray source), and software algorithms to reconstruct 3D images. A typical system consists of an X-ray source, a rotating table with a sample holder and a CCD camera with a computer. Depending on the X-ray source, i.e., a micro-focus X-ray tube or a synchrotron X-ray source, a fiberoptic- or optical lens -coupled system is used to project an image onto a CCD camera. The best resolution delivered by these instruments is around 4 µm.

Dessert Lizard
Tomogram: 10243 voxels, @ 4 µm per voxel

Tissue engineered bone from a pig orbit reconstruction
Note:X-ray CT Images: Courtesy of ANU-XCT