DocumentCode :
1510259
Title :
Digital Signal Processing Techniques to Improve Time Resolution in Positron Emission Tomography
Author :
Monzo, J.M. ; Esteve, R. ; Lerche, C.W. ; Ferrando, N. ; Toledo, J. ; Aliaga, R.J. ; Herrero, V. ; Mora, F.J.
Author_Institution :
i3M (Inst. de Instrumentacion para Imagen Mol.), Univ. Politec. de Valencia, Valencia, Spain
Volume :
58
Issue :
4
fYear :
2011
Firstpage :
1613
Lastpage :
1620
Abstract :
Coincidence time resolution is one of the most important issues in PET detectors. Improving this resolution is required to increase the noise equivalent count rate (NECR) that reduces the noise in the reconstructed images. The aim of this work is to evaluate the behavior and time resolution of different proposed time pick-off algorithms in order to select the best configuration for our PET system. The experimental setup used for this research is composed by two monolithic LSO crystals+PSPMT detectors and an FPGA based PET data acquisition system (DAQ). The acquired signals are sampled using a 12-bit 70 MHz analog to digital converter (ADC) per channel. The setup has no centralized electronics for trigger and event time extraction. Consequently, events for each detector head are processed independently and all the signals are acquired in the same way. Time resolution in this kind of systems can be improved by means of digital processing techniques and using different shapings for the last dynode signals. Four digital algorithms extracting time information from the acquired pulses have been evaluated: (1) Amplitude bipolar digital constant fraction discriminator (BCFD), (2) charge BCFD, (3) interpolated amplitude BCFD and (4) interpolated charge BCFD. Two different architectures for the interpolation algorithm have been used (one-sample and two-sample interpolation), which allow us to work with two different FPGA internal sampling frequencies: 140 MHz and 210 MHz. The results show the importance of selecting the right algorithm and parameters. Time coincidence resolution in our hardware system can be improved by up to 6.9 ns FWHM depending on the chosen digital algorithm programmed on the FPGA. The measurements with our setup reveal that charge based algorithms are less sensitive to signal noise and generate better results than amplitude algorithms. The best configuration achieves a FWHM resolution close to 1.8 ns.
Keywords :
data acquisition; field programmable gate arrays; image reconstruction; medical image processing; positron emission tomography; signal processing; FPGA internal sampling frequencies; FWHM resolution; LSO crystals; PET detectors; PSPMT detectors; analog-to-digital converter; bipolar digital constant fraction discriminator; centralized electronics; coincidence time resolution; data acquisition system; digital signal processing; event time extraction; field-programmable gate array; frequency 140 MHz; frequency 210 MHz; interpolation algorithm; noise equivalent count rate; pick-off algorithms; positron emission tomography; signal noise; time resolution; timing algorithms; Data acquisition; Detectors; Field programmable gate arrays; Interpolation; Positron emission tomography; Signal processing algorithms; Signal resolution; Constant fraction discriminator; digital signal processing; field-programmable gate array (FPGA); positron emission tomography (PET); time resolution; timing algorithms;
fLanguage :
English
Journal_Title :
Nuclear Science, IEEE Transactions on
Publisher :
ieee
ISSN :
0018-9499
Type :
jour
DOI :
10.1109/TNS.2011.2140382
Filename :
5763735
Link To Document :
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