Apparatus and associated methodology for improving timing resolution in gamma ray detection
View Patent ↗An apparatus and associated method for gamma ray detection that improves the timing resolution is provided. A crystal of interaction in a scintillation crystal array emits scintillation light in response to interaction with a gamma ray. The scintillation light is detected by one or more photomultiplier tubes. Each photomultiplier tube that detects the scintillation light detects the light at a different time. The apparatus determines the location of the gamma ray interaction and uses the location of the interaction to generate correction times for each waveform generated by the photomultiplier tubes. The waveforms are corrected with the correction timings and combined to extract a time of arrival estimate for the gamma ray. Noise thresholding is also used to select waveforms having low noise for combination to extract the time of arrival estimate.
1. A method of improving timing resolution in a gamma ray detector, comprising:
sampling, using a plurality of samplers, each configured to convert an analog signal into a digital signal, waveforms from a plurality of photosensors arranged over at least one crystal element, the waveforms being generated by the photosensors based on scintillation light emitted from a scintillation event within the at least one crystal element in response to arrival of a gamma ray;
identifying a location of the scintillation event within the at least one crystal element;
determining a correction time for each of the waveforms based on the identified location of the scintillation event;
correcting each of the waveforms using the corresponding correction time; and
estimating a time of arrival of the gamma ray at the at least one crystal element based the corrected waveforms.
2. The method according to claim 1 , wherein the plurality of samplers acquire samples periodically at a rate of at least 1 GHz.
3. The method according to claim 1 , wherein the correction times are stored in a look-up table and the location of the scintillation event is used as an index to the look-up table.
4. The method according to claim 1 , wherein the correcting step comprises:
interpolating each of the waveforms after correction to synchronize the waveforms in time.
5. The method according to claim 1 , wherein the identifying step comprises:
identifying the location of the scintillation event based on relative arrival times at each of the plurality of photosensors.
6. The method according to claim 1 , wherein the correcting step comprises:
interpolating the waveforms based on the correction times.
7. The method according to claim 1 , wherein the correcting step comprises:
correcting each waveform with a different correction time corresponding to the location of the scintillation event.
8. The method according to claim 1 , further comprising:
determining a depth of interaction within the at least one crystal element based on at least one of relative timing among the waveforms and a detailed shape of the waveforms; and
reducing parallax error in a corresponding PET image using the determined depth of interaction.
9. The method according to claim 1 , wherein the photosensors are photomultiplier tubes.
10. The method according to claim 1 , wherein the photosensors are silicon photomultipliers.
11. The method according to claim 1 , further comprising:
dynamically selecting a subset of photosensors based on prospective information,
wherein in the estimating step, the time of arrival of the gamma ray at the at least one crystal element is estimated based on corrected waveforms from the dynamically selected subset of the plurality of photosensors.
12. The method according to claim 11 , wherein the prospective information includes a projected count rate, an exam protocol and an isotope used in the exam protocol.
13. The method according to claim 1 , further comprising:
dynamically selecting a subset of photosensors based on retrospective information,
wherein in the estimating step, the time of arrival of the gamma ray at the at least one crystal element is estimated based on corrected waveforms from the dynamically selected subset of the plurality of photosensors.
14. The method according to claim 13 , wherein the retrospective information includes waveform amplitudes corresponding to each of the plurality of photosensors, a time since the last gamma ray detection at each of the plurality of photosensors, and a measured noise level of each of the plurality of photosensors.
15. A gamma ray detector, comprising:
a plurality of samplers configured to sample waveforms from a plurality of photosensors arranged over at least one crystal element, the waveforms being generated by the photosensors based on scintillation light emitted from a scintillation event in the at least one crystal element in response to arrival of a gamma ray;
an electronic memory configured to store the waveforms after sampling; and
a data processor connected to the plurality of samplers and configured
to identify a location of the scintillation event within the at least one crystal element,
to determine a correction time for each of the waveforms based on the identified location of the scintillation event,
to correct each of the waveforms using the corresponding correction time, and
to estimate a time of arrival of the gamma ray at the crystal of interaction based on the corrected waveforms.
16. The gamma ray detector according to claim 15 , wherein the correction times are stored in a look-up table on the electronic memory, and the data processor determines each correction time using the location of the scintillation event as an index to the look-up table.
17. The gamma ray detector according to claim 15 , wherein the data processor time-shifts each waveform by an integer multiple of a sampling rate used by a corresponding one of the plurality of samplers, the integer multiple corresponding to the corresponding correction time.
18. The gamma ray detector according to claim 15 , wherein the data processor interpolates each waveform based on the corresponding correction time.
19. The gamma ray detector according to claim 15 , wherein the data processor is further configured to determine a depth of interaction of the gamma ray in the at least one crystal element based on at least one of relative timings among the waveforms and detailed shape of the waveforms, and to reduce parallax error in a corresponding PET image using the depth of interaction.
20. The method according to claim 15 , wherein the gamma ray detector is included in a positron emission tomography scanner.
21. The method according to claim 15 , wherein the gamma ray detector is included in a time-of-flight positron emission tomography scanner.
22. A gamma ray detector, comprising:
means for sampling a plurality of waveforms generated by a plurality of photosensors arranged over at least one crystal element, the waveforms being generated based on scintillation light emitted by a scintillation event in the at least one crystal element in response to arrival of a gamma ray;
a memory storing the sampled waveforms;
means for identifying a location of the scintillation event within the at least one crystal element;
means for determining a correction timing for each of the waveforms based on the identified location of the scintillation event;
means for correcting each of the waveforms using the corresponding correction timing; and
means for estimating a time of arrival of the gamma ray at the at least one scintillation crystal element based on the corrected waveforms.
23. The gamma ray detector according to claim 22 , further comprising:
means for interpolating the waveforms after correction to synchronize the waveforms in time.
24. The gamma ray detector according to claim 22 , further comprising:
means for storing predetermined correction times in a look-up table indexed by crystal locations, the location of the scintillation event being used as a look-up table index to determine the correction timing.
25. The gamma ray detector according to claim 22 , further comprising:
means for time-shifting the waveforms by integer multiples of a predetermined sampling rate used to sample the waveforms, the integer multiple corresponding to the correction timing.
26. The gamma ray detector according to claim 22 , further comprising:
means for interpolating the waveforms in accordance with the correction timing.
27. The gamma ray detector according to claim 22 , further comprising:
means for determining a depth of interaction of the gamma ray in the at least one crystal element based on at least one of relative timings among the waveforms and detailed shape of the waveforms; and
means for reducing parallax error in a corresponding PET image based on the depth of interaction.
28. A non-transitory computer-readable medium storing computer-readable instructions thereon, the computer-readable instructions, when executed by a computer, cause the computer to perform a method comprising:
sampling waveforms from a plurality of photosensors arranged over at least one crystal element, the waveforms being generated by the photosensors based on scintillation light emitted from a scintillation event in the at least one crystal element in response to arrival of a gamma ray;
identifying a location of the scintillation event within the at least one crystal element;
determining a correction time for each of the waveforms based on the identified location of the scintillation event;
correcting each of the waveforms using the corresponding correction time; and
estimating a time of arrival of the gamma ray at the at least one crystal element based on the corrected waveforms.