Surgical guidance system using hand-held probe with accompanying positron coincidence detector
09784852 · 2017-10-10
Assignee
Inventors
Cpc classification
G01T1/161
PHYSICS
G01T1/2008
PHYSICS
G01T1/1642
PHYSICS
A61B6/4258
HUMAN NECESSITIES
A61B6/4405
HUMAN NECESSITIES
A61B6/4266
HUMAN NECESSITIES
G01T1/1603
PHYSICS
International classification
A61B6/00
HUMAN NECESSITIES
G01T1/161
PHYSICS
Abstract
A surgical guidance system offering different levels of imaging capability while maintaining the same hand-held convenient small size of light-weight intra-operative probes. The surgical guidance system includes a second detector, typically an imager, located behind the area of surgical interest to form a coincidence guidance system with the hand-held probe. This approach is focused on the detection of positron emitting biomarkers with gamma rays accompanying positron emissions from the radiolabeled nuclei.
Claims
1. A surgical guidance system for detecting areas of increased uptake of biomarker within a region of interest (ROI) on a patient treated with a beta-emitting bio-marker comprising: a) a hand-held detection probe including 1) a first scintillator layer for converting incident beta radiation to light, said first scintillator layer producing a first pulse shape; 2) a second scintillator layer for converting incident beta radiation to light, said second scintillator layer in optical contact with said first scintillator layer and producing a second pulse shape; 3) a gamma scintillator layer in optical contact with said second scintillator layer to detect one of a pair of 511 keV annihilation gamma rays from said ROI and producing a third pulse shape; and 4) a photodetector in optical contact with said gamma scintillator layer; b) a coincidence detector for detecting gamma rays from the ROI, said coincidence detector including a second gamma scintillator layer to detect the other of the pair of 511 keV annihilation gamma rays from said ROI and producing a fourth pulse shape; c) a hardware processor for separating the pulse shapes on the basis of their different time decay and amplitude characteristics; and d) a coincidence imager for displaying a formed coincident image of the ROI from the pulse shapes of the hand-held detection probe and the coincidence detector, said surgical guidance system producing an intensified image at said areas of increased uptake of biomarker.
2. The surgical guidance system of claim 1 wherein said first scintillator layer is selected from the group consisting of plastic scintillator, YAP crystal scintillator, and CaF(Eu) scintillator material.
3. The surgical guidance system of claim 1 wherein said second scintillator layer is selected from the group consisting of silicon, CsI(Tl), CaF(EU), YAG, and CsF.
4. The surgical guidance system of claim 1 wherein said gamma scintillator layer of said hand-held probe is selected from the group consisting of BGO, LSO, LYSO, GSO, and LGSO.
Description
DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
(9) Referring now to accompanying
(10) In the case of several hot spots 18, 20 and 22 (see
(11) In the surgical guidance system of the present invention 10, the geometry of a small size probe sensor 12 and a large imaging detector 14 on the opposite side of the organ 16A or patient body 16, sensitivity of the system (defined by number of coincidences) decreases quickly with distance from the probe sensor. This effect limits substantially the signal due to radiation background from radiation distributed in tissue behind the cancer tissue.
(12) In the example represented in
(13) As depicted in
(14) As described more fully below and depicted schematically in
(15) Coincidence imager 14, can be of differing sizes, varying from about 1 cm.sup.2 to a 1 m.sup.2 size. In special cases, it can be also a non-imaging type and usually larger than probe detector that operates in coincidence with the probe, and is placed on the opposite side of the organ, extremity or patient torso 16 as shown in
(16) Coincidence detector 14 may comprise any of a long list of conventional materials including: solid state material, such as CdZnTe, CdTe, Si, etc.; scintillator materials such as high stopping power crystal scintillators (BGO, LSO, LYSO, GSO, LGSO, etc.) other inorganic scintillators such as NaI(Tl), CsI(Tl), CsI(Na), LaBr3, etc.; scintillating glasses; hybrid heavy converters (lead, tungsten, etc) with a gaseous electron amplification medium; hybrid with heavy converters (lead, tungsten, etc) with a plastic scintillator; hybrid with heavy converter (lead, tungsten, etc) and a liquid scintillator; hybrid with heavy converter (lead, tungsten, etc) and a high pressure gas scintillator; and liquid xenon or mixtures of xenon with krypton and other additives.
(17) The active gamma sensitive element of the coincidence detector can be either a continuous material, forexample a plate of NaI(Tl) scintillator, or pixellated for example, an array of BGO pixels.
(18) Probe 12 can be provided with increased functionally to detect betas (positrons) and gammas to enhance its positron detection capabilities (as described by Yamamoto et al., Annals of Nuclear Medicine Vol. 19, No. 1, 23-28, 2005). Two or even three types of materials can be used in such a dual-mode probe. The role of a thin entry detection element is to directly detect positrons (beta particles) emitted from radiolabel used in the applied biomarker. The beta detection element can be composed of a single layer or can be a set of two consecutive layers, operating in coincidence. In the latter case the beta sensor is highly selective for beta particles, a fraction of which will traverse the first layer and deposit another energy signal in the second layer. Gamma interactions will not produce simultaneous (coincident) signals from these two layers for the same events. By this signal differentiation, beta signals can be separated from the gamma background signals.
(19) An example of a practical and preferred three element beta/gamma sensor is: 0.25 mm thick plastic scintillator (element 32 in
(20) Positron (beta) only probes have also been devised (for example those described by Raylman et al., U.S. Pat. No. 6,456,869. Sep. 24, 2002) to avoid signal interference from scattered gamma background, but their sensitivity is limited to only very shallow (<2-5 mm) tissue layers due to limited range of positrons in tissue. Therefore, while providing a clear signal from the exposed cancer tissue (providing that positron labeled biomarker is uptaken by the lesion/cancer) the beta only probe cannot detect emissions from deeper layers.
(21) Compact hand-held gamma probes with directional guidance were designed (f.e. Majewski et al., U.S. Pat. No. 6,643,538, Nov. 4, 2003) but their guidance capability is limited to lower energy gamma rays (˜140 keV) and positrons, i.e. they do not provide good directional guidance in detecting higher energy 511 keV gamma rays from the positron decays.
(22) In the case of multilayer beta/gamma sensors comprising scintillation materials, the materials are preferably selected to have different pulse shapes so that a single photodetector can be used and the beta and gamma contributions are separated on the basis of this pulse shape. This so-called phoswitch structure can be built of a large variety of materials. Two simple examples are thin plastic scintillators or YAP crystal scintillators as used as beta sensors and optically attached to a gamma sensor such as GSO.
(23) At another level of functionality, the probe sensors can be built from an array of sub-sensors, to provide additional more accurate spatial resolution (i.e. more precise surgical guidance) while maintaining or increasing probe sensitivity.
(24) In the case of solid state probes, each sub-element is read separately by multi-channel readout electronics placed in probe 12. In the case of scintillation probes, multi-element photo-detectors are used either incorporated in probe 12, or placed at the end of multi-fiber light guide in optical contact with probe 12.
(25) The gamma radiation sensor 34 in probe 12 can be made of, for example: a solid state material, such as CdZnTe, CdTe, etc, or a scintillator material such as high stopping power crystal scintillators (BGO, LSO, LYSO, GSO, LGSO, etc). The additional positron sensitive material can be also made of a thin solid state material such as silicon, or a thin bright scintillator such as plastic scintillator, CsI(Tl), CaF(Eu), YAP, YAG, CsF, etc.
(26) Scintillation light from the scintillator sensor can be detected by a directly coupled or via a light guide coupled photosensor. Several types of photodetectors can be used: photomultipliers, silicon photodiodes, avalanche photodiodes, silicon photomultipliers, and hybrid photomultipliers (with silicon element)
(27) Two major variants or configurations of the system can be utilized: a flexible version when used during biopsy or surgery primarily involving organs such as breast, head, neck, extremities, in this case a smaller and also compact coincidence imager is used attached to, for example, an articulated arm for easy manipulation around the organ(s) in the surgery field; and a more static version with a larger field of view coincidence imager 14, for example, placed under or directly embedded in the patient bed 13 (see
(28) During surgery the feedback information provided to the probe operator/surgeon has to be prompt, provided with minimal delay. Therefore, while the in-depth analysis of the collected and/or available data from the probe and coincident imager 14 is important, fast feedback to the operator/surgeon is of prime value.
(29) Different aspects of the formed coincident image in coincidence imager 14 can be used to provide precise information to the probe operator as to the existence and position of the uptake region (lesion etc): average position (center of gravity of the count distribution); size and shape of the projected distribution, providing information about the extent and size of the uptake, for example isolated hot spots vs larger area/volume; information about the depth of the uptake (in the case of simpler point-like uptake regions).
(30) In the special implementation of the concept for prostate cancer depicted in
EXAMPLES
Example 1
(31) A probe comprising an about 1 cm cube LSO crystal attached to a 1.4 cm diameter R647 Hamamatsu PMT; and an imaging detector comprising a 20×15 cm LYSO array of 2×2×15 mm LYSO pixels (pitch 2.1 mm) optically attached to a 4×3 array of Hamamatsu flat panel H8500 PSPMTs is used to image a “point” microCi: Na22 source 50 embedded in acrylic 52 representing a lesion in a housing 54 (see
(32) Geometry:
(33) In this example, the “lesion” is about 2 cm from the probe sensor center. The lesion-to-imaging detector distance is about 13 cm.
Example 2
(34) A smaller probe comprising a 3×3×10 mm BGO crystal is attached to a R1635 Hamamatsu PMT. Count rate curves are measured while moving (scanning) the probe close to the source. Both single mode and coincidence mode are used. The results of using these two systems are shown in Table 1.
(35) TABLE-US-00001 TABLE 1 Image ROI (2 min Position (mm) Single Rate (Hz) Coinc. Rate (Hz) counts) 0 1310 665 1633 2.5 1650 815 1625 5.0 1990 985 3255 7.5 2295 1120 4079 10 2380 1125 2496 12.5 2220 1065 1859 15 1840 875 1795 17.5 1530 620 Random 1400
(36) The above data are represented graphically in
(37) The observed sharper position definition is due to a coincidence effect between the probe and the region in the imager. This demonstrates much better guidance capabilities of the system, as compared to a simple gamma/beta probe.
(38) As the invention has been described, it will be apparent to those skilled in the art that the same may be varied in many ways without departing from the spirit and scope of the invention. Any and all such modifications are intended to be included within the scope of the appended claims.