METHOD AND APPARATUS FOR DETERMINING TIME OF FLIGHT AND DEPTH OF INTERACTION USING A POSITRON EMISSION TOMOGRAPHY SYSTEM
A PET apparatus includes a detector block including a miniblock including detector crystals, a first detector crystal and a second detector crystal being separated by an inner reflector, the inner reflector having a depth-dependent transparency, a first photosensor configured to detect light from a gamma ray detection event, and a second photosensor configured to detect the light from the gamma ray detection event, a first intensity and a second intensity of the light detected by the first and second photosensor being dependent on the depth-dependent transparency of the inner reflector; and processing circuitry configured to determine, based on the detected first intensity, a first energy, determine, based on the detected second intensity, a second energy, and determine, based on the first energy and the second energy, a depth of interaction (DOI) of the gamma ray detection event.
1 . A positron emission tomography (PET) apparatus, comprising:
a detector block including
a miniblock including a plurality of detector crystals, a first detector crystal and a second detector crystal of the plurality of detector crystals being separated by an inner reflector, the inner reflector having a depth-dependent transparency,
a first photosensor configured to detect light from a gamma ray detection event, a first intensity of the light detected by the first photosensor being dependent on the depth-dependent transparency of the inner reflector, and
a second photosensor configured to detect the light from the gamma ray detection event, a second intensity of the light detected by the second photosensor being dependent on the depth-dependent transparency of the inner reflector; and
processing circuitry configured to
determine, based on the detected first intensity, a first energy,
determine, based on the detected second intensity, a second energy, and
determine, based on the first energy and the second energy, a depth of interaction (DOI) of the gamma ray detection event.
2 . The apparatus of claim 1 , wherein the inner reflector includes a plurality of openings, the depth-dependent transparency of the inner reflector being determined by the plurality of openings.
3 . The apparatus of claim 2 , wherein the plurality of openings is divided into at least two sections along the inner reflector, a first section of the at least two sections having a different density of the plurality of openings compared to a second section of the at least two sections.
4 . The apparatus of claim 3 , wherein the first section of the at least two sections is disposed towards a top of the inner reflector, the top of the inner reflector being disposed opposite a bottom of the inner reflector, the bottom of the inner reflector being disposed proximal to the first photosensor or the second photosensor, the density of the plurality of openings of the first section of the at least two sections being higher than the density of the plurality of openings of the second section of the at least two sections.
5 . The apparatus of claim 4 , wherein an opening size for each opening of the plurality of openings is identical.
6 . The apparatus of claim 2 , wherein the plurality of openings is divided into at least two sections along the inner reflector, a first section of the at least two sections having a different opening size for each opening of the plurality of openings compared to a second section of the at least two sections.
7 . The apparatus of claim 6 , wherein the opening size for the each opening of the plurality of openings in the first section of the at least two sections is greater than the opening size for the each opening of the plurality of openings in the second section of the at least two sections.
8 . The apparatus of claim 7 , wherein a number of the plurality of openings in the first section of the at least two sections is identical to a number of the plurality of openings in the second section of the at least two sections.
9 . The apparatus of claim 1 , wherein the inner reflector includes a first section having a first uniform transparency and a second section having a second uniform transparency.
10 . The apparatus of claim 9 , wherein the first uniform transparency is determined by a film applied to the first section of the inner reflector and the second uniform transparency is based on a second film applied to the second section of the inner reflector.
11 . The apparatus of claim 10 , wherein the first section is disposed towards a top of the inner reflector, the top of the inner reflector being disposed opposite a bottom of the inner reflector, the second section being disposed towards the bottom of the inner reflector, the bottom of the inner reflector being disposed proximal to the first photosensor or the second photosensor, the first uniform transparency being higher than the second uniform transparency.
12 . The apparatus of claim 9 , wherein the first uniform transparency is determined by a thickness of the first section of the inner reflector and the second uniform transparency is determined by a thickness of the second section of the inner reflector.
13 . The apparatus of claim 1 , wherein
the inner reflector includes a top and a bottom, the top of the inner reflector being disposed opposite the bottom of the inner reflector, the bottom of the inner reflector being disposed proximal to the first photosensor or the second photosensor, and
a thickness of the inner reflector increases from the top of the inner reflector to the bottom of the inner reflector, the depth-dependent transparency being determined by the thickness of the inner reflector.
14 . The apparatus of claim 1 , wherein the processing circuitry is further configured to determine the DOI based on a ratio of the first energy to the second energy.
15 . The apparatus of claim 1 , wherein the processing circuitry is further configured to:
determine, based on the light detected by the first photosensor, a first time of flight (TOF) value;
determine, based on the light detected by the second photosensor, a second TOF value; and
determine, based on the first TOF value and the second TOF value, a miniblock TOF value.
16 . The apparatus of claim 1 , wherein the miniblock includes an outer reflector surrounding the miniblock along sides of the miniblock.
17 . The apparatus of claim 1 , wherein a number of the plurality of the detector crystals is identical to a number of the photosensors.
18 . A method, comprising:
detecting, via a first photosensor in a detector block including a miniblock having a plurality of detector crystals including a first detector crystal and a second detector crystal separated by an inner reflector having a depth-dependent transparency, a first intensity of light from a gamma ray detection event incident on the first detector crystal;
detecting, via a second photosensor in the detector block, a second intensity of the light from the gamma ray detection event incident on the second detector crystal;
determining, based on the detected first intensity of the light, a first energy;
determining, based on the detected second intensity of the light, a second energy; and
determining, based on the first energy and the second energy, a depth of interaction (DOI) of the gamma ray detection event.
19 . The method of claim 18 , further comprising:
determining, based on the light detected by the first photosensor, a first time of flight (TOF) value;
determining, based on the light detected by the second photosensor, a second TOF value; and
determining, based on the first TOF value and the second TOF value, a miniblock TOF value.
20 . The method of claim 18 , wherein the step of determining the DOI further comprises determining the DOI based on a ratio of the first energy to the second energy.