High energy X-ray imaging technology

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The HEXITEC Collaboration HEXITEC Collaboration Logo.png
The HEXITEC Collaboration

High energy X-ray imaging technology (HEXITEC) is a family of spectroscopic, single photon counting, pixel detectors developed for high energy X-ray and gamma ray spectroscopy applications. [1] [2]

Contents

The HEXITEC consortium was formed in 2006 funded by the Engineering and Physical Sciences Research Council, UK. [3] [4] The consortium is led by the University of Manchester; other members include the Science and Technology Facilities Council, the University of Surrey, Durham University and University of London, Birkbeck. In 2010 the consortium expanded to include the Royal Surrey County Hospital and the University College London. The vision of the consortium was to "develop a UK-based capability in high energy X-ray imaging technology". It is now available commercially through Quantum Detectors.

High energy X-ray imaging technology

X-ray spectroscopy is a powerful experimental technique that provides qualitative information about the elemental composition and internal stresses and strain within a specimen. High energy X-rays have the ability to penetrate deeply into materials allowing the examination of dense objects such as welds in steel, geological core sections bearing oil or gas or for the internal observation of chemical reactions inside heavy plant or machinery. Different experimental techniques such as X-ray fluorescence imaging and X-Ray diffraction imaging require X-ray detectors that are sensitive over a broad range of energies. Established semiconductor detector technology based on silicon and germanium have excellent energy resolution at X-ray energies under 30 keV but above this, due to a reduction in the material mass attenuation coefficient, the detection efficiency is dramatically reduced. To detect high energy X-rays, detectors produced from higher density materials are required.

High density, compound semiconductors such as cadmium telluride (CdTe), cadmium zinc telluride (CdZnTe), gallium arsenide (GaAs), mercuric iodide or thallium bromide have been the subject of extensive research for use in high energy X-ray detection. The favorable charge transport properties and high electrical resistivity of CdTe and CdZnTe have made them ideally suited to applications requiring spectroscopy at higher X-ray energies. Imaging applications, such as SPECT, require detectors with a pixelated electrode that allow objects to be imaged in 2D and 3D. Each pixel of the detector requires its own chain of readout electronics and for a highly pixelated detector this requires the use of a high sensitivity application-specific integrated circuit.

The HEXITEC ASIC

The HEXITEC application specific integrated circuit (ASIC) was developed for the consortium by the Science and Technology Facilities Council Rutherford Appleton Laboratory. The initial prototype consisted of an array of 20 x 20 pixels on a 250μm pitch fabricated using a 0.35μm CMOS process; [5] the second generation of the ASIC expanded the array size to 80 x 80 pixels (4 cm2). Each ASIC pixel contains a charge amplifier, a CR-RC shaping amplifier and a peak track-and-hold circuit. The ASIC records the position and total charge deposited for each X-ray event detected.

The PIXIE ASIC

A typical X-ray / gamma-ray spectrum collected with the HEXITEC detector Am241 spectra HEXITEC.png
A typical X-ray / gamma-ray spectrum collected with the HEXITEC detector

The PIXIE ASIC is a research and development ASIC developed by the Science and Technology Facilities Council Rutherford Appleton Laboratory for the consortium. The ASIC is being used to investigate charge induction and the small pixel effect in semiconductor detectors as described by the Shockley–Ramo theorem. [6] The ASIC consists of three separate arrays of 3 x 3 pixels on a 250μm pitch and a single array of 3 x 3 pixels on a 500μm pitch. Each pixel contains a charge amplifier and output buffer allowing the induced charge pulses of each pixel to be recorded.

The HEXITEC-MHz ASIC

The original HEXITEC ASIC was delivered in the early 2010's and operated at a maximum frame rate of 10kHz. At this speed the detector system was able to deliver per pixel X-ray spectroscopy with an energy resolution of <1keV but was limited to fluxes of 104 photons s-1 mm-2. With the development of Diffraction-limited storage ring synchrotrons, the intensity of X-rays produced in typical experiments increased by >×100. In order to continue to provide a spectroscopic X-ray imaging capability at these facilities, a new generation of the HEXITEC ASIC had to be developed. The development of the HEXITEC-MHz ASIC began in 2018 with the aim of increasing the frame rate of the camera system to 1MHz to allow spectroscopic imaging at photon fluxes in excess of 106 photons s-1 mm-2 while maintaining the same spectroscopic performance. The first ASICs were delivered in 2022 and are currently undergoing testing at the Science and Technology Facilities Council Rutherford Appleton Laboratory and Diamond Light Source. [7]

HEXITEC detectors

HEXITEC ASICs are flip-chip bonded to a direct conversion semiconductor detector using a low temperature (~100 °C) curing silver epoxy and gold stud technique in a hybrid detector arrangement. The X-ray detector layer is a semiconductor, typically cadmium telluride (CdTe) or cadmium zinc telluride (CdZnTe), between 1 – 3 mm thick. The detectors consist of a planar cathode and a pixelated anode and are operated under a negative bias voltage. X-rays and gamma rays interacting within the detector layer form charge clouds of electron-hole pairs which drift from the cathode to the anode pixels. The charge drifting across the detectors induce charge on the ASIC pixels as described by the Shockley–Ramo theorem which form the detected signal. The detectors are capable of measuring a photo-peak FWHM of the order 1 keV in the energy range 3 - 200 keV. [8]

Applications

HEXITEC detectors are in use in a number of different application areas including: materials science, [9] medical imaging, [10] [11] illicit material detection, [12] and X-ray astronomy. [13]

Related Research Articles

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References

  1. ↑ "3-D Color X-ray Spots Corrosion, Cancer and Contraband". Photonics.com. 2013-01-09.
  2. ↑ "Camera takes 3D colour X-ray photographs in near real time". theengineer.co.uk. 2013-01-07.
  3. ↑ "New Materials for High Energy Colour X-ray Imaging". EPSRC. 2006-06-01.
  4. ↑ "HEXITEC Translation grant. The application of colour X-ray imaging". EPSRC. 2011-01-04.
  5. ↑ Jones, Lawrence; Seller, Paul; Wilson, Matthew; Hardie, Alec (June 2009). "HEXITEC ASIC—a pixellated readout chip for CZT detectors". Nuclear Instruments and Methods in Physics Research Section A. 604 (1–2): 34–37. Bibcode:2009NIMPA.604...34J. doi:10.1016/j.nima.2009.01.046.
  6. ↑ Veale, Matthew; Bell, Steven J.; Jones, Lawrence L.; Seller, Paul; Wilson, Matthew D.; Allwork, Christopher; Kitou, Dimitris; Sellin, Paul J.; et al. (October 2011). "An ASIC for the Study of Charge Sharing Effects in Small Pixel CdZnTe X-Ray Detectors". IEEE Transactions on Nuclear Science. 58 (5): 2357. Bibcode:2011ITNS...58.2357V. doi:10.1109/TNS.2011.2162746. S2CID   23658071.
  7. ↑ Cline, Ben (September 2023). "HEXITECMHz - A 1 MHz continuous frame rate spectroscopic X-ray imaging detector system". Nuclear Instruments and Methods in Physics Research Section A: 168718. doi:10.1016/j.nima.2023.168718.
  8. ↑ Seller, Paul; Bell, S; Cernik, R J; Christodoulou, C; Egan, C K; Gaskin, J A; Jacques, S; Pani, S; et al. (December 2011). "Pixellated Cd(Zn)Te high-energy X-ray instrument". Journal of Instrumentation. 6 (12): C12009. Bibcode:2011JInst...6C2009S. doi:10.1088/1748-0221/6/12/C12009. PMC   3378031 . PMID   22737179.
  9. ↑ Jacques, Simon; Egan, Christopher K.; Wilson, Matthew D.; Veale, Matthew C.; Seller, Paul; Cernik, Robert J. (November 2012). "A laboratory system for element specific hyperspectral X-ray imaging". Analyst. 138 (3): 755–9. doi:10.1039/c2an36157d. PMID   23145429.
  10. ↑ Scuffham, James; Wilson, M D; Seller, P; Veale, M C; Sellin, P J; Jacques, S D M; Cernik, R J (August 2012). "A CdTe detector for hyperspectral SPECT imaging". Journal of Instrumentation. 7 (8): P08027. doi:10.1088/1748-0221/7/08/P08027. S2CID   250665467.
  11. ↑ Alkhateeb, Shyma; Abdelkader, Mohamed H.; Bradley, David A.; Seller, Paul; Veale, Matthew C.; Wilson, Matt D.; Pani, Silvia (February 2013). Nishikawa, Robert M; Whiting, Bruce R (eds.). "Energy dispersive X-ray diffraction computed tomography of breast-simulating phantoms and a tissue sample" (PDF). SPIE Medical Imaging. Medical Imaging 2013: Physics of Medical Imaging. 8668: 86684G. doi:10.1117/12.2007710. S2CID   120523203.
  12. ↑ O'Flynn, Daniel; Desai, Hemant; Reid, Caroline B; Christodoulou, Christiana; Wilson, Matthew D; Veale, Matthew C; Seller, Paul; Hills, Daniel; Wong, Ben; Speller, Robert D (July 2013). "Identification of simulants for explosives using pixellated X-ray diffraction". Crime Science. 2: 4. doi: 10.1186/2193-7680-2-4 .
  13. ↑ "High-Energy Replicated Optics - HERO". NASA. Archived from the original on 16 November 2005. Retrieved 19 July 2013.
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