None.
The embodiments described herein relate generally to a time-to-digital converter device and associated methodology for improved measurement accuracy and resolution.
A commercial gamma ray detector includes an array of scintillator crystals coupled to a transparent light guide, which distributes scintillation light over an array of photomultiplier tubes (PMTs) arranged over the transparent light guide. Signals from the PMTs in a same area are generally summed in the analog domain, and then timing is measured based on the leading edge of the summed signal, or event.
A Time-to-Digital-Converter (TDC) is often used to measure timing in a gamma ray detector. A TDC accurately converts the realization of an event into a number than can be related to the time the event occurred. Various methods exist to perform this task. Amongst others, counting a large number of very fast logic transitions between coarse clock cycles has been used to perform this task. In some cases, it may be desirable to indicate the occurrence of a series of events known to be generated sequentially. For instance, time marks a rising signal takes to reach a pre-determined set of threshold values can be very useful information.
Time-to-digital converters (TDCs) have also been implemented with a variety of architectures. A first conventional architecture is a classic delay chain having a single chain of identical delay elements connected in series. The classic delay chain also includes a set of single bit memory elements, each connected to an output of one of the delay elements. A start signal is supplied to the input of the chain of delay elements to indicate a beginning of the time period to be measured. The start signal propagates through the chain of delay elements. The end of the time period to be measured is indicated by a stop signal that is simultaneously provided to the clock inputs of all of the memory elements in order to capture the position of the propagated start signal within the chain of delay elements. The captured position is then thermometer-decoded to compute the delay between the start and stop signals, and this delay is used to compute the length of the time period to be measured as a multiple of the delay imparted by each of the delay elements.
Therefore, the resolution of the classic delay chain is limited to the time-delay of each delay element in the delay chain. For example, if each delay element in the chain imparts a delay of “tu”, then the resolution of the classic delay chain is “tu”. As such, in a physical implementation of the classic delay chain, such as in a semiconductor device, the minimum value of tu is limited by the physical properties of the semiconductor. As sampling is performed at the same point in time for each delay element in the classic delay chain, the physical limitations on the delay tu give rise to the limits of measurement resolution.
Another conventional delay chain is the Vernier delay chain. As in the classic delay chain, the Vernier delay chain includes a chain of identical delay elements connected in series and a set of single bit memory elements, each connected to the output of one of the delay elements. However, the Vernier delay chain also includes a second delay chain of identical delay elements connected in series. The output of each of the delay elements in the second delay chain is connected to a clock input of one of the memory elements. Further, the delays elements in the first delay chain each impart a delay of tu, and the delay elements of the second delay chain each impart a delay of tc, where tc<tu.
In operation, the start signal is supplied to the first delay chain of the Vernier delay chain, and the stop signal is supplied to the second delay chain. As the delay imparted by the elements of the second delay chain is less than that of the elements of the first delay chain, the stop signal will eventually overtake the start signal. When the stop signal overtakes the start signal, the propagation of the start signal in the first delay chain is captured by the memory elements and thermometer-decoded to determine the time interval between the start and stop signals. The time period to be measured is then calculated as a multiple of the difference between the delays of the first delay chain and the delays of the second delay chain, or tu−tc.
As with the classic delay chain, the delays in the Vernier delay chain are limited by the physical properties of the semiconductor device on which it is implemented. Therefore, there is a minimum delay difference (tu−tc) (i.e. resolution) that can be achieved using the Vernier delay chain. Thus, it is difficult to make precise time period measurements using the Vernier delay chain.
Accordingly, a need exists for an apparatus and associated methodology that improves upon the limitations of the classic and Vernier delay chains, and that achieves improved accuracy and resolution.
A more complete appreciation of the embodiments described herein, and many of the attendant advantages thereof will be readily obtained as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings, wherein
In general, time-to-digital converter device according to exemplary embodiments of the present advancements includes a first delay chain circuit that generates a first value corresponding to a time delay between a start signal and a stop signal. The time-to-digital converter device also includes at least one second delay chain circuits that generates a second value corresponding to a time delay between a delayed start signal and the stop signal. At least one delay element generates the delayed start signal by applying a predetermined delay to the start signal, and a combining circuit generates an output value based on the first and second values. In the time-to-digital converter according to the exemplary embodiments of the present advancements, the output value corresponds to the time delay between the start signal and the stop signal.
Referring now to the drawings, wherein like reference numerals designate identical or corresponding parts throughout the several views,
Further, in
As one of ordinary skill in the art would recognize, the time-to-digital converter device of
The time-to-digital converter device of
Though eight delay chain elements 203 . . . 210 are shown in
In operation, the start signal is provided to the terminal 201 of
As one of ordinary skill in the art will recognize, propagation of the start signal through the delay chain elements 203 . . . 210 is measured at the delay boundaries. In other words, the propagated start signal is sampled at the outputs of each of the delay chain elements 203 . . . 210. Thus, the start signal is captured after an integer number of delays tu imparted by the delay chain elements 203 . . . 210. Fractions of tu are not measured. As such the resolution of the delay chain in
In
In operation, the start signal is applied to delay chain elements 203 . . . 210 via terminal 201 at the beginning of the time period to be measured and the stop signal is applied to the terminal 202 at the end of the time to be measured. The start signal propagates through the delay chain elements 203 . . . 210, and the stop signal propagates through the delay chain elements 321 . . . 327. As the delay of delay elements 321 . . . 327 is less than the delay of delay chain elements 203 . . . 210, the stop signal will eventually overtake the start signal. When the propagation of the stop signal arrives at the output of delay element 327, the outputs of memory elements 211 . . . 218 are provided to the thermometer decoder 219, and a resulting output representative of the time period to be measured is provided to terminal 220. The delay chain of
As with
Next an exemplary implementation of the time-to-digital converter circuit will be described with reference to
In
Terminal 12 is directly connected to the clock inputs 42b and 43b of delay chains 42 and 43 respectively. The outputs of delay chains 42 and 43 are combined in combiner 41 and provided to output terminal 19.
Next, the operation of the time-to-digital conversion device of
At step S2 in
Next, the timing diagram of
At a predetermined time, a stop signal 60 is applied to stop terminal 12. The stop signal 60 is directly applied to both delay chains 42, 43 without delay. At time 65, the stop signal causes the delay chains to “capture” the current value of each of their respective delay chain elements b1 . . . b16. For example, at time 65 b1 . . . b4 are high and b5 . . . b8 are low in delay chain 42, while b9 . . . b11 are high and b12 . . . b16 are low in delay chain 43. Thus, the captured chain value for delay chain 42 is “11110000”, or four, and the captured value for delay chain 43 is “11100000” or three. The computed time difference is then the sum of these values divided by the delay imparted by delay element 40.
As can be appreciated, the delay chains 42, 43, start signals 61, 61b and stop signal 60 in
Next, a gamma ray detection system according to an exemplary embodiment of the present advancements is described with reference to
In
Each photomultiplier tube 110, 135, 140 and 195 is respectively connected to variable gain amplifiers, or VGA, 150, 152, 154, and 156. The VGAs 150, 152, 154 and 156 act as signal buffers and allow the acquisition system to be adjusted to accommodate variation in PMT gain, such as occurs naturally as part of the PMT manufacturing process and occurs due to aging of the PMTs. The signal output from each VGA 150, 152, 154 or 156 is split into two separate electronic paths.
One electronics path for is used for measuring the arrival time of the gamma ray. The signal for this path is typically formed by summing two or more signals from the same detector in a summing amplifier 184 or 186. The act of summing multiple signals from the same detector can improve the signal to noise ratio for the timing estimate and reduce the number of required electronic components. After summing, the signal is passed to a discriminator 187 or 188. The discriminator 187 or 188, which typically has an adjustable threshold, produces a precisely timed electronic pulse when the summed signal passes the threshold setting. The output of the discriminator triggers a time-to-digital converter, or TDC, 189 and 190. The TDC 189 or 190 produces a digital output which encodes the time of the discriminator pulse relative to a system clock (not shown). For a time-of-flight PET system, the TDC 189 or 190 typically produces a time stamp with an accuracy of 15 to 25 ps.
For each PMT 110, 135, 140 and 195 there is an independent electronics path which is used to measure the amplitude of the signal on each PMT 110, 135, 140 and 195. This path consists of a filter 160, 162, 164, 166 and an analog to digital converter, or ADC, 176, 177, 178, 179. The filter 160, 162, 164 or 166, typically a bandpass filter, is used to optimize the signal to noise ratio of the measurement and performs an anti-aliasing function prior to conversion to a digital signal by the ADC 176, 177, 178 or 179. The ADC 176, 177, 178 or 179 can be a free-running type, running at 100 MHz, for example, in which case the central processing unit, or CPU, 170, performs a digital integration, or the ADC can be a peak-sensing type. The ADC and TDC outputs are provided to a CPU, 170, for processing. The processing consists of estimating an energy and position from the ADC outputs and an arrival time from the TDC output for each event, and may include the application of a many correction steps, based on prior calibrations, to improve the accuracy of the energy, position, and time estimates.
As one of ordinary skill in the art would recognize, the CPU 170 can be implemented as discrete logic gates, as an Application Specific Integrated Circuit (ASIC), a Field Programmable Gate Array (FPGA) or other Complex Programmable Logic Device (CPLD). An FPGA or CPLD implementation may be coded in VHDL, Verilog or any other hardware description language and the code may be stored in an electronic memory directly within the FPGA or CPLD, or as a separate electronic memory. Further, the electronic memory may be non-volatile, such as ROM, EPROM, EEPROM or FLASH memory. The electronic memory may also be volatile, such as static or dynamic RAM, and a processor, such as a microcontroller or microprocessor, may be provided to manage the electronic memory as well as the interaction between the FPGA or CPLD and the electronic memory.
Alternatively, the CPU 170 may be implemented as a set of computer-readable instructions stored in any of the above-described electronic memories and/or a hard disk drive, CD, DVD, FLASH drive or any other known storage media. Further, the computer-readable instructions may be provided as a utility application, background daemon, or component of an operating system, or combination thereof, executing in conjunction with a processor, such as a Xenon processor from Intel of America or an Opteron processor from AMD of America and an operating system, such as Microsoft VISTA, UNIX, Solaris, LINUX, Apple, MAC-OS and other operating systems known to those skilled in the art.
Once processed by the CPU 170, the processed signals are stored in electronic storage 180, and/or displayed on display 145. As one of ordinary skill in the art would recognize, electronic storage 180 may be a hard disk drive, CD-ROM drive, DVD drive, FLASH drive, RAM, ROM or any other electronic storage known in the art. Display 145 may be implemented as an LCD display, CRT display, plasma display, OLED, LED or any other display known in the art. As such, the descriptions of the electronic storage 180 and the display 145 provided herein are merely exemplary and in no way limit the scope of the present advancements.
In the above descriptions, any processes, descriptions or blocks in flowcharts should be understood as representing modules, segments or portions of code which include one or more executable instructions for implementing specific logical functions or steps in the process, and alternate implementations are included within the scope of the exemplary embodiments of the present advancements in which functions may be executed out of order from that shown or discussed, including substantially concurrently or in reverse order, depending upon the functionality involved, as would be understood by those skilled in the art.
While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel methods, apparatuses and systems described herein may be embodied in a variety of other forms; furthermore, various omissions, substitutions and changes in the form of the methods, apparatuses and systems described herein may be made without departing from the spirit of the inventions. The accompanying claims and their equivalents are intended to cover such forms or modifications as would fall within the scope and spirit of the inventions.
Number | Name | Date | Kind |
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20080295603 | Shin et al. | Dec 2008 | A1 |
20100283653 | Dai et al. | Nov 2010 | A1 |
Number | Date | Country |
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2007-041007 | Feb 2007 | JP |
Number | Date | Country | |
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20120104259 A1 | May 2012 | US |