Gamma ray detector for positron emission tomography (pet) and single photon emisson computed tomography (spect)

• US 20050253073A1
• Filed: 07/17/2002
• Published: 11/17/2005
• Est. Priority Date: 07/17/2002
• Status: Abandoned Application

• Current Assignee: European Organization for Nuclear Research
• Original Assignee: European Organization for Nuclear Research
• Inventors: Weilhammer, Peter, Joram, Christian, Seguinot, Jaques
• Application Number:
  US10/521,221
• Publication Number:
  US 20050253073A1
• Time in Patent Office: Days
• US Class Current: 250/363.30
• CPC Class Codes: G01T 1/2985 In depth localisation, e.g. using positron emitters; Tomographic imaging (longitudinal and transverse section imaging; apparatus for radiation diagnosis sequentially in different planes, steroscopic radiation diagnosis); using external radiation sources A61B6/02

Abstract

The invention relates to a detector module (1) for a Positron Emission Tomograph (PET) and for Single Photon Emission Computed Tomography (SPECT) comprising a matrix (3) of scintillator crystals, said matrix having a first side and a second side opposite to said first side, each scintillator crystal having a first end (14) and a second end (15), said scintillator crystals (2) being oriented parallel to each other, whereby said first end (14) and said second end (15) of each of said scintillator crystals (2) coincide with said first side and said second side of said matrix (3), respectively; a first light sensitive detector (6) producing electrical signal proportional to the amount of light detected, being optically connected to said first side of said matrix (3), said first light sensitive detector (6) being position sensitive; and a second light sensitive detector (7) producing electrical signal proportional to the amount of light detected, said second light sensitive detector (7) being optically connected to said second side of said matrix (3), wherein said second light sensitive detector (7) is positioned sensitive. Using said detector module (1) a method to determine the 3D-coordinates of a point of interaction of a gamma quantum (γ1, γ2) with said detector module (1) is disclosed method. This allows to use signals from compton seattered γ'"'"'s to enhance the sensitivity of a Positron Emission Tomograph scanner provided being composed of said detection modules (1) without parallax errors.

Claims

1. Detector module for a Positron Emission Tomograph (PET) comprising

a matrix of scintillator crystals, said matrix having a first side and a second side opposite to said first side, each scintillator crystal having a first end and a second end, said scintillator crystals being oriented parallel to each other, whereby said first end and said second end of each of said scintillator crystals coincide with said first side and said second side of said matrix, respectively;

a first light sensitive detector producing an electrical signal proportional to the amount of light detected, being optically connected to said first side of said matrix, said first light sensitive detector (6) being position sensitive; and

a second light sensitive detector producing an electrical signal proportional to the amount of light detected, said second light sensitive detector being optically connected to said second side of said matrix, being position sensitive.

2. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said first light sensitive detector and said second light sensitive detector are segmented such that at least one segment in each of said light sensitive detectors corresponds to each of said scintillator crystals in said matrix.

3. Detector module for a Positron Emission Tomograph (PET) according to claim 2, wherein segmentation patterns of said light sensitive detectors match patterns of their respective matrix sides.

4. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said first light sensitive detector is a Hybrid Photo Diode (HPD) detector.

5. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said second light sensitive detector is a Hybrid Photo Diode (HPD) detector.

6. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said matrix has a rectangular pattern or a stonewall pattern with a first direction (y) parallel to one side of said rectangular pattern;

said scintillator crystals comprise a crystal material and an added crystal material length along said first direction (y) corresponds to about three times the absorption length of photons (γ

₁, γ

₂) with a primary photon energy to be detected in said crystal material.

7. Detector module for a Positron Emission Tomograph (PET) according to claim 6, wherein said matrix comprises 12×

18 scintillator crystals.

8. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said crystal material comprises Cerium doped Yttrium Aluminum Perovskite (YAP:

Ce).

9. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said crystal material comprises Cerium doped Lutetium Oxyortho-silicate (LSO:

Ce) or LuAP;

Ce.

10. Detector module for a Positron, Emission Tomograph (PET) according to claim 1, wherein said scintillator crystals have the dimensions of 3.2×

3.2×

100 mm³.

11. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said scintillator crystals are spaced in said matrix by wires strung between said scintillator crystals close to said first and said second side of said matrix.

12. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said wires have a diameter of 0.8 mm.

13. Detector module for a Positron Emission Tomograph (PET) according to claim 10, wherein said segments of said first and said second light detector have the dimensions of 4 mm×

4 mm.

14. Detector module for a Positron Emission Tomograph (PET) according to claim 1, wherein said scintillator crystals comprise crystal segments glued together with a glue having a matched refractive index as said crystal segments.

20. Single Photon Emission Computed Tomography detector comprising a photon detector characterized in that said photon detector is a detector module ( for a Positron Emission Tomograph according to any of the 1 to 14claim 1.

15. Positron Emission Tomograph (PET) scanner comprising a number of gamma detector modules characterized in that said gamma detector modules each comprise a detector module comprising

a matrix of scintillator crystals, each scintillator crystal having a first end and a second end, said scintillator crystals being oriented parallel to each other such that all mid points of said scintillator crystals lie in one plane;

a first light sensitive detector and a second light sensitive detector, each of said light sensitive detectors produces an output signal proportional to the amount of light detected and is position sensitive;

said number of gamma detector modules are regularly angularly spaced on a first and a second circle around an axis of said scanner and oriented such that all midpoints of said scintillator crystals of said detector modules lie in a symmetry plane perpendicular to said axis, whereby the spacing and distribution of said gamma detector modules on said first and said second circle is such that there is no line of sight in a direction perpendicular to said axis radial outward from the cross section of said axis with said symmetry plane, such that there is practically a full azimuthal coverage.

16. Positron Emission Tomograph (PET) scanner according to claim 15, wherein said angular spacing between a first one of said gamma detector modules being localized on said first circle to an adjacent second one of said gamma detector modules localized on said second circle is 15°

.

17. Method for detecting the point of interaction of a gamma ray (γ

₁, γ

₂) within a detector module comprising

a matrix of scintillator crystals, each scintillator crystal having a first end and a second end, said scintillator crystals being oriented parallel to each other such that all mid points of said scintillator crystals lie in a plane;

a first light sensitive detector and a second light sensitive detector, each of said light sensitive detectors produces an output signal proportional to the amount of light detected and is position sensitive;

said detector module having a coordinate system associated with, whereby two linear independent coordinate axes χ and

γ

span a χ

γ

-plane coinciding with said plane defined by said midpoints of said scintillator crystals and a third coordinate axis z is oriented perpendicular to said plane whereby an origin of said coordinate system lies in said Xy-plane and a positive direction of said coordinate axis z points to said first light sensitive detector (6), said method comprising the steps

determining the coordinates of said point of interaction in said Xy-plane by identifying a first scintillator crystal being hit and using the known coordinates of said first scintillator crystal being hit in said Xy-plane;

determining the coordinate of said point of interaction in said direction (z) perpendicular to said Xy-plane by determining the amount of charge Q1 detected in said first light sensitive detector and an amount of charge Q2 detected in said second light sensitive detector within a coincidence time interval, where the coordinate z is given by where L is the length of said first scintillator crystal.

18. Method for detecting the point of interaction of a gamma ray (γ

₁, γ

₂) within, a PET detector module according to claim 17, wherein said determined coordinate is considered to be valid, if the total amount of charge (Q L−

Q2) detected by said first and said second light sensitive detectors equals a reference charge corresponding to a predetermined photon energy.

19. Method for detecting the point of interaction of a gamma ray (γ

₁, γ

₂) within a PET detector module according to claim 17, where the determined coordinate is considered to be valid, if the total amount of charge (Q1+Q2) detected by said first and said second light sensitive detectors originating from said first scintillator crystal hit is lower than 60% of said reference charge, corresponding to said predetermined photon energy, and a second coordinate is determined according to the method of claim 18 in a same coincidence time interval, associated with a different scintillator crystal hit and the charges detected by said first light sensitive detector and said second light sensitive detector originating from said different scintillator crystal hit are Q3 and Q4, respectively, and the total amount of charges (Q1+Q2+Q3+Q4) detected by said first light sensitive detector and said second light sensitive detector originating from said first scintillator crystal hit and said different scintillator crystal hit is about equal to said reference charge and said coordinate is closer to the source emitting the gamma ray than said second coordinate.

21. Hybrid Photo Diodes (HPD) detector comprising

a vacuum containment, said vacuum containment having a flat entrance window at a top and a base at a bottom opposite to said top;

semi transparent visible light bialkali photocathode deposited inside said vacuum containment at said top parallel to said entrance window;

a semiconductor sensor mounted inside said vacuum containment on said base said semiconductor sensor comprising segments;

a self triggering electronic circuitry for reading out each of said segments separately, being mounted inside said vacuum containment at said base

an electron optic providing a imaging of photo electrons from said semi-transparent visible light bialkali photocathode onto said semiconductor sensor

22. Hybrid Photo Diodes (HPD) detector according to claim 21, wherein said base comprises a ceramic material.

23. Hybrid Photo Diodes (HPD) detector according to claim 21, wherein said semiconductor sensor is a silicon sensor.

24. Hybrid Photo Diodes (HPD) detector according to claim 21, wherein said self triggering circuitry comprises one channel for each segment of said semiconductor sensor;

a charge integrating preamplifier for each of said channels;

a shaper for each of said channels; and

a readout register for each of said channels.

25. Hybrid Photo Diodes (HPD) detector according to claim 24 wherein said shaper has a tunable shaping time.

26. Hybrid Photo Diodes (HPD) detector according to 25claim 21, further comprising a parallel fast shaper circuit for producing a trigger signal for a readout logic.

27. Hybrid Photo Diodes (HPD) detector according to 26claim 21, wherein said electron optics comprise any suitable number of ring electrode.

28. Hybrid Photo Diodes (HPD) detector according to claim 21, wherein said bialkali photocathode is directly deposited on the inside of said entrance window.

29. Hybrid Photo Diodes (HPD) detector according to claim 21, wherein said entrance window is comprising sapphire.