Gamma camera for PET and SPECT studies

• US 6,072,177 A
• Filed: 09/14/1998
• Issued: 06/06/2000
• Est. Priority Date: 01/08/1997
• Status: Expired due to Fees

• Current Assignee: SMV America Incorporated
• Original Assignee: SMV America Incorporated
• Inventors: McCroskey, William K., Vickers, David S., Heipp, Christ H.
• Primary Examiner(s): Westin, Edward P.
• Assistant Examiner(s): HANIG, RICHARD E
• Application Number:
  US09/152,117
• Time in Patent Office: 631 Days
• Field of Search: 250/252.1, 250/363.03, 250/363.04, 250/363.09
• US Class Current: 250/252.1
• CPC Class Codes: A61B 6/037 Emission tomography
• CPC Class Codes: A61B 6/4258 for detecting non x-ray radiation, e.g. gamma radiation A61B6/037 takes precedence
• CPC Class Codes: G01T 1/1642 using a scintillation crystal and position sensing photodetector arrays, e.g. ANGER cameras
• CPC Class Codes: G01T 1/172 with coincidence circuit arrangements G01T1/178 takes precedence ; combination of detectors, see G01T1/1603, G01T1/30, G01T1/361

Abstract

A gamma camera is modified to perform PET studies as well as SPECT studies by utilization of the camera'"'"'s SPECT electronics to likewise generate triggering pulse signals for photons indicative of a positron annihilation event which are corrected, on a bundled basis, for position, linearity and uniformity by the same digital processors used by the camera for SPECT studies. In addition the triggering pulse signals generate analog timing signals passed through a coarse coincidence circuit to establish matched pairs of timing signals which are digitally time stamped and processed along with the bundled set of pulse signals that the timing signals originated from. The timing signals in turn are corrected from a mapped detector head look up table on the basis of the corrected position of the triggering pulse signal and the time lag between each matched timing signal pair passed through a fine coincidence window processor thus insuring that the line of response passing through the corrected, precisely established positions of scintillations that produced the triggering pulse signals occurred within a time period clearly indicative of a positron annihilation event. By counting only true LORs images having high resolution can be constructed even though the camera'"'"'s detecting heads cover a limited solid angle of event detections. The timing correction table is generated from an improved calibration technique which factors out those inherent time delays, including signal noise and jitter, which are specific to that gamma camera.

Claims

1. A process for calibrating the coincidence timing of a nuclear camera used to perform PET studies in which coincident pair photons are detected by opposing PMTs and matched as a coincident pair if the PMT signals for any given PMT occurs within a set time of an opposing PMT signal, said process including the steps of

a) placing a positron producing radiation point source adjacent the center of one PMT to produce a uniform flood of radiation over an initial group of opposing PMTs;

b) generating timing trigger signals for the point source PMT and the opposing initial group of PMTs;

c) delaying by a set short time the timing trigger signals from either the point source PMT or the opposing group of PMTs;

d) matching any given timing trigger signal from said point source with any given timing trigger signal from any given PMT in said group occurring within said short time to establish a matched pair;

e) determining the time lag between the timing triggering signals of each matched pair;

f) building a time lag histogram for each PMT in said initial group; and

,

g) sampling each histogram to determine a mean time delay for correcting timing signals developed by said camera during PET imaging.

2. The process of claim 1 further including the steps of

h) placing said positron producing radiation source adjacent the center of a PMT in said initial group for producing a uniform flood of radiation over a second group of PMTs, said second group including the PMT which was adjacent to said point source in step (a);

i) repeating steps (b)-(f) for said second group to develop means delay times for each PMT in each second group.

3. The process of claim 2 further including the steps of

j) determining the difference in mean time lag from the mean time lags established in step (g) for that PMT in said initial group which became the point source PMT in step (i) and that PMT in said other group which was the initial point source PMT in step (a);

and

k) adjusting the delay of the timing triggering signals when the camera operates by said difference in mean time lag time.

4. The process of claim 3 wherein said camera is a gamma camera having at least two, opposed detecting heads spanning an area, each containing a plurality of PMTs, said initial group of PMTs comprising all the PMTs on one detector head and the remaining group comprising all the PMTs in the opposite detector head.

5. A method for calibrating the timing signals developed by a gamma camera performing PET studies, said camera including first and second detector heads between which a patient is placed, each detector head containing a plurality of PMTs extending over a head area;

a triggering timing circuit for generating from each PMT'"'"'s pulse signals triggering timing signals;

a coincident circuit for matching and time stamping matched pairs of triggering timing signals originating from opposing heads within a first set time period;

digital signal processors for correcting said timed stamp signals and determining if each matched corrected pair occurred within a second, shorter set time period, said method comprising the steps of

a) placing a positron producing radiation point source adjacent the center of a given PMT in one detector head for uniformly flooding all the PMTs in the opposite detector head with positron producing radiation;

b) delaying the triggering timing signals from one of said detector heads an initial time shorter than said first time period;

c) generating by said coincidence circuit time stamped signals indicative of the time lag between matched triggering signals from said PMT adjacent said point source and any given flooded PMT on the opposite detector head;

d) storing for each flooded PMT the time stamp signals in a multichannel analyzer associated with each flooded PMT until channels of all the multichannel analyzers for all the flooded PMTs are filled to a set limit;

e) sampling each multichannel analyzer to arrive at a mean delay time for correcting said time stamp signals in said digital signal processors.

6. The method of claim 5 further including the steps of

f) after completing step (f) moving said point source radiation adjacent the center of a given PMT in the previously flooded detector head for uniformly flooding the PMTs with radiation in the detector head which previously contained said point source;

g) repeating steps (b), (c) and (d) for the other detector head whereby both detector heads have for all of their PMTs mean delay time signals.

7. The method of claim 6 wherein said given PMT adjacent said point source radiation is the centermost PMT in said detector head.

8. The method of claim 7 further including the steps of comparing the mean lag times for the two common LORs extending between the alternating point source PMTs to obtain a time difference and

adjusting the time delay in said coincident circuit by said difference time whereby inherent electronic delays in triggering the timing signals are accounted for.

9. The method of claim 7 further including the step of mapping the entire area of each detection head on a pixel scale with the mean delay times produced for all the PMTs in step (e).

10. The method of claim 8 wherein said gamma camera further includes a variable delay for each detector head in said detector circuit and applying said difference time to the slower detector'"'"'s variable delay to increase the delay time of said variable delay by said difference time.