A multi-threshold sampling method for TOF-PET signal processing
Creators
- 1. Department of Radiology, University of Chicago, Chicago, IL 60637 (United States)
- 2. Enrico Fermi Institute, University of Chicago, Chicago, IL 60637 (United States)
- 3. Lawrence Berkeley National Laboratory, Berkeley, CA 94720 (United States)
Description
As an approach to realizing all-digital data acquisition for positron emission tomography (PET), we have previously proposed and studied a multi-threshold sampling method to generate samples of a PET event waveform with respect to a few user-defined amplitudes. In this sampling scheme, one can extract both the energy and timing information for an event. In this paper, we report our prototype implementation of this sampling method and the performance results obtained with this prototype. The prototype consists of two multi-threshold discriminator boards and a time-to-digital converter (TDC) board. Each of the multi-threshold discriminator boards takes one input and provides up to eight threshold levels, which can be defined by users, for sampling the input signal. The TDC board employs the CERN HPTDC chip that determines the digitized times of the leading and falling edges of the discriminator output pulses. We connect our prototype electronics to the outputs of two Hamamatsu R9800 photomultiplier tubes (PMTs) that are individually coupled to a 6.25x6.25x25mm3 LSO crystal. By analyzing waveform samples generated by using four thresholds, we obtain a coincidence timing resolution of about 340 ps and an ∼18% energy resolution at 511 keV. We are also able to estimate the decay-time constant from the resulting samples and obtain a mean value of 44 ns with an ∼9ns FWHM. In comparison, using digitized waveforms obtained at a 20 GSps sampling rate for the same LSO/PMT modules we obtain ∼300ps coincidence timing resolution, ∼14% energy resolution at 511 keV, and ∼5ns FWHM for the estimated decay-time constant. Details of the results on the timing and energy resolutions by using the multi-threshold method indicate that it is a promising approach for implementing digital PET data acquisition.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.nima.2009.01.100Additional details
Identifiers
- DOI
- 10.1016/j.nima.2009.01.100;
- PII
- S0168-9002(09)00070-9;
Publishing Information
- Journal Title
- Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment
- Journal Volume
- 602
- Journal Issue
- 2
- Journal Page Range
- p. 618-621
- ISSN
- 0168-9002
- CODEN
- NIMAER
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 41031447
- Subject category
- S46: INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY;
- Descriptors DEI
- AMPLITUDES; CERN; COMPARATIVE EVALUATIONS; CRYSTALS; DATA ACQUISITION; DECAY; ENERGY RESOLUTION; IMPLEMENTATION; KEV RANGE 100-1000; PERFORMANCE; POSITRON COMPUTED TOMOGRAPHY; PROCESSING; SAMPLING; SIGNALS; TIME RESOLUTION; WAVE FORMS
- Descriptors DEC
- COMPUTERIZED TOMOGRAPHY; DIAGNOSTIC TECHNIQUES; EMISSION COMPUTED TOMOGRAPHY; ENERGY RANGE; EVALUATION; INTERNATIONAL ORGANIZATIONS; KEV RANGE; RESOLUTION; TIMING PROPERTIES; TOMOGRAPHY
Optional Information
- Copyright
- Copyright (c) 2009 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.