Article
Development of an FPGA-Based Data Acquisition Module for Small Animal PET
Inst. of Nucl. Res., Hungarian Acad. of Sci., Debrecen
IEEE Transactions on Nuclear Science (impact factor:
1.45).
11/2006;
DOI:10.1109/TNS.2006.876004
pp.2698 - 2703
Source: IEEE Xplore
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Conference Proceeding: MicroPET: a high resolution PET scanner for imaging small animals
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ABSTRACT: MicroPET is a high resolution positron emission tomography (PET) scanner designed for imaging small laboratory animals. It consists of a ring of 30 position-sensitive scintillation detectors, each with an 8×8 array of small lutetium oxyonhosilicate (LSO) crystals coupled via optical fibers to a multi-channel photomultiplier tube. The detectors have an intrinsic resolution averaging 1.68 mm, an energy resolution between 15 and 25% and 2.4 ns timing resolution at 511 keV. The detector ring diameter of microPET is 17.2 cm with an imaging field of view of 112 mm transaxially by 18 mm axially. The scanner has no septa and operates exclusively in 3D mode. Reconstructed image resolution 1 cm from the center of the scanner is 2.0 mm and virtually isotropic, yielding a volume resolution of 8 mm<sup>3</sup> For comparison, the volume resolution of state-of-the-art clinical PET systems is in the range of 50-75 mm<sup>3</sup>. Initial images of phantoms have been acquired and are reported. A computer controlled bed is under construction and will incorporate a small wobble motion to improve spatial sampling. This is projected to further enhance spatial resolution. MicroPET is the first PET scanner to incorporate the new scintillator LSO and to our knowledge is the highest resolution multi-ring PET scanner currently in existenceNuclear Science Symposium, 1996. Conference Record., 1996 IEEE; 12/1996 -
Article: Collection of scintillation light from small BGO crystals
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ABSTRACT: We propose to develop a high resolution positron emission tomography (PET) detector designed for animal imaging. The detector consists of a 2-D array of small bismuth germanate (BGO) crystals coupled via optical fibers to a multi-channel photomultiplier tube (MC-PMT). Though this approach offers several advantages over the conventional BGO block design, it does require that a sufficient number of scintillation photons be transported from the crystal, down the fiber and into the PMT. In this study we use simulations and experimental data to determine how to maximize the signal reaching the PMT. This involves investigating factors such as crystal geometry, crystal surface treatment, the use of reflectors, choice of optical fiber, coupling of crystal to the optical fiber and optical fiber properties. Our results indicate that using 2×2×10 mm BGO crystals coupled to 30 cm of clad optical fiber, roughly 50 photoelectrons are produced at the PMT photocathode for a 511 keV interaction. This is sufficient to clearly visualize the photopeak and provide adequate timing resolution for PET. Based on these encouraging results, a prototype detector will now be constructedIEEE Transactions on Nuclear Science 09/1995; · 1.45 Impact Factor -
Article: Detector development for a novel Positron Emission Mammography scanner based on YAP:Ce crystals
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ABSTRACT: A prototype for positron emission mammography is under development within a collaboration of the Departments of Physics of Pisa and Ferrara. The device will be composed of two opposing detectors (parallel plane geometry). The active part of the detector head is constituted by a matrix of scintillators with a small pixel size (2×2 mm2). We have evaluated the possibility to use an array of Position Sensitive PhotoMultiplier Tube (PSPMT mod R8520-C12 from Hamamatsu) for the readout of the scintillation matrix. Two different crystal-PMT coupling techniques have been explored: the results for each method are reported in this work. The overall performance, in terms of efficiency and pixel identification of the final prototype of the detector head are also presented. For future applications the new H8500 (also called the ‘flat panel’ PMT) has been studied and compared to the R8520 in terms of the imaging performance and other considerations such as cost and geometry. The imaging performance of these tubes is characterized in terms of the pixel image resolution and the peak-to-valley ratio.Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment.
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Keywords
2 ns FWHM
analog signal conditioning circuits
built-in hardware limitation
communication module
data acquisition
developed DAQ module
digital CFD algorithm
digital signal processing
field programmable gate array
FPGA
hardware coincidence detection
identical DAQ modules
LSO scintillator crystal block
maximum number
position sensitive PMT
postprocessing
precise time
real detector signals
small animal PET camera
time resolution