Method for producing a high resolution detector array

This application claims the benefit of the filing date of Provisional Patent Application Serial No. 60/239,145, filed on Oct. 10, 2000.

Not Applicable

1. Field of Invention

This invention pertains to a method of producing a scintillator detector arrays that may be used in various applications, such as, but not limited to, a PET detector module or nuclear physics applications. More specifically, it relates to a method of producing a high resolution detector array that can be coupled to photodetectors. In certain applications, the photodetector provides an accurate timing pulse and initial energy discrimination, identification of the crystal interaction, which may include the depth of interaction (DOI).

2. Description of the Related Art

When constructing scintillator arrays, it is known to use block scintillator arrays with sawcut grooves packed with reflector powder. However, this method is not feasible for producing arrays of individual crystals. It is also known to use reflector molds made of a white compound. However, it is often desired to produce light output with a greater depth dependence than these type of reflectors are capable of producing.

Finally, it is also known to hand wrap “plumbers” Teflon® tape around individual detectors as a standard reflector choice for research PET cameras. However, plumbers Teflon® tape is not a realistic choice for large cameras and/or cameras that use very small crystals. Further, hand wrapping individual crystals is both time consuming and difficult to do consistently. Hand wrapping with Teflon® tape also limits the reduction of crystal size for future cameras. In addition, plumbers Teflon® tape, or thicker 8 mil Teflon® tape, is not an ideal reflector. It stretches and creeps, so it can be difficult to accurately cover only the surface of each crystal not coupled to a photodetector. The Teflon® tape also becomes transparent when squeezed, which occurs when making a compact scintillator crystal array, and when glue wicks through it. Moreover, it is difficult to wrap the individual crystals tightly with thicker 8 mil Teflon® tape resulting in inaccurate measures of depth dependence.

What is missing from the art is a method of disposing a reflector between each individual crystal of a high resolution detector array which can efficiently, consistently and accurately cover the desired surfaces of an individual crystal. Accordingly, it is an object of the present invention to provide a method of producing a high resolution detector array having a reflector disposed between individual crystals of the array.

It is a further object of the present invention is to provide a method for producing a high resolution detector array efficiently, consistently and accurately covers the desired surfaces of an individual crystal.

Yet another the object of the present invention is to provide a method for producing a high resolution detector array which will provide very high packing fraction i.e. the distance between scintillator elements will be minimized so the detector efficiency will be higher than is currently achievable.

Still another object of the present invention is to provide a method for producing a high resolution detector array which eliminates the need to hand wrap individual crystals.

In one embodiment of the present invention, the fabrication methodology is enhanced by handling LSO bars rather than single crystals when gluing on the Lumirror® as well as etching the LSO. Namely, an LSO boule is cut into bars of a selected dimension, for example 30 mm wide, which are then acid etched. A selected number, N, of these LSO bars can then be glued together with Lumirror® sheets between each bar (coating the LSO bars and Lumirror® sheets with Epotek 301-2). The glued bar block is then cut again into bars in a perpendicular direction, and these new LSO-Lumirror® bars are etched. Finally, a selected number, M, of these LSO-Lumirror® bars are glued together with Lumirror® sheets between each bar; thus creating an etched N×M LSO-Lumirror® array without having to handle individual LSO crystals or small Lumirror® pieces It will be appreciated by those skilled in the art that while M may be equal to N, M can also be greater than or less than N.

The above-mentioned features of the invention will become more clearly understood from the following detailed description of the invention read together with the drawings in which:

FIG. 1 is a perspective view of a detector array constructed in accordance with the prior art in which individual crystals are cut and adhered to a base material, such as a is light guide.

FIGS. 2 a , 2 b and 2 c are a perspective view of the first steps of the method of the present invention utilizing a single scintillator material.

FIGS. 3 a , 3 b and 3 c are a perspective view of the final steps of the method illustrated in FIGS. 2 a , 2 b and 2 c and the detector array produced by such method.

FIGS. 4 a , 4 b and 4 c are a perspective view of the fist steps of an alternate embodiment of the method of the present invention utilizing two different scintillator materials.

FIGS. 5 a , 5 b and 5 c are a perspective view of the final steps of the method illustrated in FIGS. 4 a , 4 b and 4 c and the detector array produced by such method.

FIGS. 6 a , 6 b and 6 c are a perspective view of the first steps of an additional alternate embodiment of the method of the present invention starting with a stacked scintillator material having a first decay time A 1 and a second decay time A 2 .

FIGS. 7 a , 7 b and 7 c are a perspective view of the final steps of the method illustrated in FIGS. 6 a , 6 b and 6 c and the detector array produced by such method.

FIGS. 8 a , 8 b and 8 c are a perspective view of the first steps of a further alternate embodiment of the method of the present invention utilizing a first stacked scintillator material having a first decay time A 1 and a second decay time A 2 and a second stacked scintillator material having a first decay time B 1 and a second decay time B 2 .

FIGS. 9 a , 9 b and 9 c are a perspective view of the final steps of the method illustrated in FIGS. 8 a , 8 b and 8 c and the detector array produced by such method.

The detector designs produced by the method disclosed herein, along with its alternate embodiments, will enable finer spatial resolution than is achievable with current state of the art detector fabrication methodologies. The method can be utilized to produce a detector array comprised of a single scintillator material, or as described herein, can employ the use of two or more scintillator materials of different decay times. The decay times are used as one of the parameters in determining the scintillator elements loci in position space. Most current detector designs use the decay time for depth of interaction encoding (DOI). Variants of the new design would also be capable of providing this feature.

In general, the detector fabrication method will provide very high packing fraction i.e. the distance between scintillator elements will be minimized so the detector efficiency will be higher than is currently achievable. Another important feature of the design is that four times as many detector elements will be able to be resolved in position space with no increase in the number of optical detectors; the result will be that the intrinsic spatial resolution will be half of the current designs i.e. we will be able to spatially resolve smaller objects.

According to one embodiment of the present invention, the method of the present invention entails the following steps. By way of example, it will be recognized that a prior art, standard block detector having dimensions of 52 mm wide×52 mm long×20 mm thick which is segmented into a 12×12 array has a crystal pitch of 4.3 mm and crystal size of 4.0 mm, as seen in FIG. 1 is constructed by arranging discrete cut scintillator crystal elements upon a substrate, resulting in large interstitial spaces which are typically packed with reflector powder. In contrast, according to the method of the present invention, a selected number, N, of bars of scintillator material are cut to a selected dimension, in one embodiment 52 mm long×2 mm wide×20 mm thick. In FIGS. 2 and 3, by way of example, the selected number of bars is twelve. It will be appreciated that while a 12×12 array is depicted in the figures, the method of the present invention could also be utilized to produce an 8×8 array, a 24×24 array, a 4×4 array etc. It will also be appreciated that the method could also be utilized to produce N×M arrays where M≠N. While the present method could be utilized to produce an N×M, (it being understood that M may or may not equal N), detector array of a single scintillator material (as illustrated in FIGS. 2 a , 2 b , 2 c , 3 a , 3 b and 3 c ), in other embodiments, the method of the present embodiment could be utilized to produce detector arrays utilizing two different scintillator materials, (see FIGS. 4 a , 4 b , 4 c , 5 a , 5 b and 5 c ), utilizing a stacked scintillator material having a first decay time A 1 and a second decay time A 2 , (see FIGS. 6 a , 6 b , 6 c , 7 a , 7 b and 7 c ) or utilizing two different scintillator materials in which the first scintillator material is a stacked scintillator material having a first decay time A 1 and a second decay time A 2 and the second scintillator material is a stacked scintillator material having a first decay time B 1 and a second decay time B 2 , (see FIGS. 8 a , 8 b , 8 c , 9 a , 9 b and 9 c ).

As illustrated in FIGS. 2-3, when producing a scintillation detector array from a single scintillator material, N bars 20 are cut from a block 10 of a selected scintillator material. The bars 20 in FIG. 2 b would then be etched. It will be understood that the etching can be accomplished by either a chemically etch process (inexpensive approach) or a mechanical polishing process (expensive approach); either choice can be made. The etched bars are then coated with an epoxy of selected index of refraction, preferably Epotek 301-2 or Sylgard 186, a thin (50-200 micron) polyester film 40 loaded with a reflective material such as CaCO 3 or TiO 2 etc. is then bonded to the scintillator bar using the selected epoxy. The preferred embodiment film is Lumirror® by Toray Corporation. The scintillator bars are then laminated together. The pattern would be a layer of scintillator 20 followed by a layer of epoxy and thin reflector film 40 , followed by a layer of scintillator 20 . This process is repeated until all N layers are laminated together, See FIG. 2 c . The assembly is then allowed to cure. Once fully cured the laminated block is subjected to a second sawing operation in which the laminated block is then cut into M bars 50 of a selected thickness by cutting across the laminated bars, see FIG. 3 a . As stated above, M may or may not be equal to N. This results in m bars 50 of a selected dimensions, for example 2 mm wide×52 mm long×20 mm thick. Note though that in this case each bar contains N scintillator elements 20 ′. These N bars 50 are then etched. The etched bars are then coated with an epoxy of selected index of refraction and reflector film 40 is then bonded to the scintillator bar 50 using the selected epoxy, see FIG. 3 b . The scintillator layers are then laminated together using the process described above, see FIG. 3 c . The process results in an N×M scintillator element array. As stated above, the figures illustrate and exemplary 12×12 detector array. However, as has been stated, it will be appreciated that other array sizes, could be produced in accordance with the method of the present invention, and that M may or may not equal N.

In another embodiment, illustrated in FIGS. 4-5, a detector array utilizing two different scintillator materials is produced. In this embodiment ½ N bars 20 are cut from a block 10 of a first selected scintillator material of a first selected decay time while ½ N bars are cut from block 15 of a second selected scintillator material of a second selected decay time. The bars 20 and 30 respectively in FIG. 4 b would then be etched. The etched bars are then coated with an epoxy of selected index of refraction, preferably Epotek 301-2 or Sylgard 186, a thin (50-200 micron) polyester film 40 loaded with a reflective material such as CaCO 3 or TiO 2 etc. is then bonded to the scintillator bar using the selected epoxy. The preferred embodiment film is Lumirror® by Toray Corporation. The scintillator bars are then laminated together. The pattern would be a layer of scintillator 20 , of decay time x, followed by a layer of epoxy and thin reflector film 40 , followed by a layer of scintillator 30 of decay time y, followed by a layer of epoxy and thin reflector film 40 followed by a layer of scintillator 20 of decay time x. This process is repeated until all N layers are laminated together, See FIG. 4 c . It being understood that the composite of the layer of scintillator 20 and the reflector film 40 is epoxied to the adjoining composite of scintillator 30 and reflector film 40 and so on. The assembly is then allowed to cure. Once fully cured the laminated block is subjected to a second sawing operation in which the laminated block is then cut into a selected number M bars 50 of a selected thickness by cutting across the laminated bars, see FIG. 5 a . This results in M bars 50 of a selected dimension, for example 2 mm wide×52 mm long×20 mm thick. Note though that in this case each bar contains ½ N scintillator elements 20 ′ and ½ N scintillator elements 30 ′. These M bars 50 are then etched. The etched bars are then coated with an epoxy of selected index of refraction and reflector film 40 is then bonded to the scintillator bar 50 using the selected epoxy, see FIG. 5 b . The scintillator bars 50 are then laminated together using the process described above except that every other layer is rotated 180 degrees. This rotation results in a checkerboard pattern of alternating scintillation crystals of different decay times, see FIG. 5 c . The process results in an N×M scintillator element array in which M may or may not equal N. Further, it will be appreciated that a detector array produced in accordance with the method of the present invention can be utilized in conjunction with light guides which may be either “active” or “inactive”, segmented or continuous, and if segmented then either “inverted” or “non-inverted”.

It will be recognized by those skilled in the art that the decay times of certain scintillator materials, Lutetium Oxyorthosilicate and Gadolinium Oxyorthosilicate to name a couple, are tuneable, such that a block of detector material could be constructed of a first block of a selected scintillator material having a selected decay time A 1 optically bonded to a second block of the same selected scintillator material having a decay time A 2 . See FIG. 6 a . As illustrated in FIGS. 6-7, when producing a scintillation detector array from a single scintillator material, N bars 20 are cut from a block 10 ′ of a selected scintillator material. The block 10 ′ is constructed of a first layer 12 of the selected scintillator material having decay time A 1 which is optically bonded to a second layer 14 of the selected scintillator material having decay time A 2 . The bars 20 in FIG. 6 b would then be etched. The etched bars are then coated with an epoxy of selected index of refraction, preferably Epotek 301-2 or Sylgard 186, a thin (50-200 micron) polyester film 40 loaded with a reflective material such as CaCO 3 or TiO 2 etc. is then bonded to the scintillator bar using the selected epoxy. The preferred embodiment film is Lumirror® by Toray Corporation. The scintillator bars are then laminated together, taking care not to invert the orientation of the layers with respect to decay time. The pattern would be a layer of scintillator bar 20 followed by a layer of epoxy and thin reflector film 40 , followed by a layer of scintillator bar 20 . This process is repeated until all N layers are laminated together, See FIG. 6 c . The assembly is then allowed to cure. Once fully cured the laminated block is subjected to a second sawing operation in which the laminated block is then cut into M bars 50 of a selected thickness by cutting across the laminated bars, see FIG. 6 a . As stated above, M may or may not be equal to N. This results in m bars 50 of a selected dimensions, for example 2 mm wide×52 mm long×20 mm thick. Note though that in this case each bar contains N scintillator elements 20 ′. These N bars 50 are then etched. The etched bars are then coated with an epoxy of selected index of refraction and reflector film 40 is then bonded to the scintillator bar 50 using the selected epoxy, see FIG. 6 b . The scintillator layers are then laminated together using the process described above, see FIG. 6 c . The process results in an N×M scintillator element array. As stated above, the figures illustrate and exemplary 12×12 detector array. However, as has been stated, it will be appreciated that other array sizes, could be produced in accordance with the method of the present invention, and that M may or may not equal N.

Further, as illustrated in FIGS. 8-9 a detector array utilizing two different scintillator materials in which the first scintillator material consists of a first block 12 of a selected scintillator material having a selected decay time A 1 optically bonded to a second block 14 of the same selected scintillator material having a decay time A 2 , and the second scintillator material consists of a first block 17 of a selected scintillator material having a selected decay time B 1 optically bonded to a second block 19 of the same selected scintillator material having a decay time B 2 . See FIG. 8 a . In this embodiment ½ N bars 20 are cut from block 10 ′ and ½ N bars 30 are cut from block 15 ′. The bars 20 and 30 respectively in FIG. 8 b are then etched. The etched bars are then coated with an epoxy of selected index of refraction, preferably Epotek 301-2 or Sylgard 186, a thin (50-200 micron) polyester film 40 loaded with a reflective material such as CaCO 3 or TiO 2 etc. is then bonded to the scintillator bar using the selected epoxy. The preferred embodiment film is Lumirror® by Toray Corporation. The scintillator bars are then laminated together, again taking care not to invert the bars with respect to decay times. The pattern would be a layer of scintillator bar 20 , followed by a layer of epoxy and thin reflector film 40 , followed by a layer of scintillator bar 30 , followed by a layer of epoxy and thin reflector film 40 followed by a layer of scintillator bar 20 . This process is repeated until all N layers are laminated together, See FIG. 4 c . It being understood that the composite of the layer of scintillator 20 and the reflector film 40 is epoxied to the adjoining composite of scintillator 30 and reflector film 40 and so on. The assembly is then allowed to cure. Once fully cured the laminated block is subjected to a second sawing operation in which the laminated block is then cut into a selected number M bars 50 of a selected thickness by cutting across the laminated bars, see FIG. 5 a . This results in M bars 50 of a selected dimension, for example 2 mm wide×52 mm long×20 mm thick. Note though that in this case each bar contains ½ N scintillator elements 20 ′ (of decay time A 1 and A 2 ) and ½ N scintillator elements 30 ′ (of decay time B 1 and B 2 ) in alternating fashion. These M bars 50 are then etched. The etched bars are then coated with an epoxy of selected index of refraction and reflector film 40 is then bonded to the scintillator bar 50 using the selected epoxy, see FIG. 3 b . The scintillator bars 50 are then laminated together using the process described above except that every other layer is rotated 180 degrees, again taking care that the bars are not inverted with respect to decay time. This rotation results in a checkerboard pattern of alternating scintillation crystals of different decay times, see FIG. 5 c . The process results in an N×M scintillator element array in which M may or may not equal N.

From the foregoing description, it will be recognized by those skilled in the art that a method of disposing a reflector between each individual crystal of a high resolution detector array which can efficiently, consistently and accurately cover each of four sides of an individual crystal has been provided. In this regard, the present invention provides a method of producing a high resolution detector array having a reflector disposed between individual crystals of the array. Further, the present invention provides a method for producing a high resolution detector array which will provide very high packing fraction i.e. the distance between scintillator elements will be minimized so the detector efficiency will be higher than is currently achievable and which eliminates the need to hand wrap individual crystals.

While the present invention has been illustrated by description of several embodiments and while the illustrative embodiments have been described in considerable detail, it is not the intention of the applicant to restrict or in any way limit the scope of the appended claims to such detail. Additional advantages and modifications will readily appear to those skilled in the art. The invention in its broader aspects is therefore not limited to the specific details, representative apparatus and methods, and illustrative examples shown and described. Accordingly, departures may be made from such details without departing from the spirit or scope of applicant's general inventive concept.