1. Field of the Invention
The present invention relates to digital radiation imaging. In particular, the invention relates to the effective construction of optimized imaging areas of various size and shape by combining separate semiconductor pixel detectors side by side in a mosaic like manner so that the shape of the active area of the sensor is made to match as exactly as possible the X-ray beam shape (or shapes) of a specific application.
2. Description of Related Art
A major problem in constructing digital X-ray imaging devices is the manufacturing of large sensor areas. Commercial state of the art large area devices generally rely on flat panel technology. Sensors based on other technologies such as scintillator-CCD sensors or especially semiconductor-CMOS sensors produce higher image quality but suffer from a more limited active imaging area possible to manufacture.
The maximum continuous active area of single detector chip CCD and CMOS based sensors is typically a few square centimeters (cm2). These single detector chips may be combined by mounting them side by side in a mosaic like manner to form larger areas. Such mosaic constructions have been successfully applied in scanning systems in which the active imaging area has a slot shape to form a linear array of imaging elements. Rectangular shape imaging areas of a few tens of cm2 have also been successfully manufactured. Larger rectangular areas of CCD and CMOS based sensors are limited by the fact that one side of the single CCD and CMOS chips is always required for external electrical connections and prevents side by side mounting at that one side. Benefits of constructing imaging areas from separate small detector elements include flexibility to form areas of irregular shape and cost effective production. Prior art sensors, however, have not been able to address these needs.
Some applications may demand different sensor areas for different imaging modes. For example in modern digital dental extraoral X-ray imaging the same imaging system should be able to perform both fan beam panoramic scan acquisition and cone beam three dimensional (3D) imaging. In the scan mode a vertical relatively long slot like imaging area is preferred in order to match the sensor area with the X-ray fan beam shape and to optimize readout speed. In the 3D mode a vertically shorter but horizontally wider sensor area is optimal in providing appropriate cone beam coverage.
In the prior art, to match these partially contradicting sensor area requirements manufacturers of modern dental extraoral X-ray systems either have to use two separate available state of the art digital sensors or one large sensor (typically flat panel) with a sufficient area of rectangular shape to cover both the fan and the cone beam shapes. Both of these options introduce disadvantages in terms of cost, compactness and effective use. The present invention deals with this issue by introducing a novel digital X-ray sensor with a unique irregular shape of active area optimized for both of the imaging modes mentioned above. Dental extraoral X-ray imaging is here given as an example only. The invention can be used for benefit in any other X-ray imaging application with similar requirements of imaging area. The invention can be realized especially well with semiconductor-CMOS detector technology but may also be realized with other technologies such as the scintillator-CCD technology.
Several ideas and methods of constructing larger mosaic type active imaging areas of single detector elements have been introduced and patented [U.S. Pat. No. 6,207,744, U.S. Pat. No. 5,812,191, EP0421869, WO9708751, EP0138647]. The aim of such methods is generally to realize a large enough regular imaging area of either rectangular or slot shape. Most of the presented methods teach techniques to minimize the unavoidable dead space or blind region between the separate detector elements. The minimum gap between the active areas of adjacent detector elements is obviously achieved by mounting the elements in physical contact with each other. While eliminating or minimizing the inter-element dead space of multi element sensors is the ideal for acquiring uniform X-ray images it may not be feasible from the manufacturing point of view to assemble the separate detector elements physically touching each other. In addition to the optimal irregular shape of active area mentioned above the present invention introduces an effective manufacturing technique for multi element sensors. This technique is especially applicable to sensors based on semiconductor-CMOS technology and has specific relevance to CdTe-CMOS pixel detectors.
The present invention provides an X-ray imaging sensor with a unique irregular shape of active area differing from a rectangular shape, the shape being optimized to the requirements of the application of the sensor. As illustrated in
An important aspect of the invention is that the shape of the active area of the sensor is made to match as exactly as possible the X-ray beam shape (or shapes) of a specific application. If the X-ray beam shape differs significantly from a cone or a fan beam shape or if the application requires the use of two or more X-ray beams with different shapes no conventional sensor of linear or rectangular shape will match effectively the X-ray beam shapes. For example, in an application using a fan beam and a rectangular cone beam for different imaging modes a sensor with irregular shape of active area provides much more efficient beam coverage than a conventional sensor with a large rectangular active area. The benefits of an optimized sensor area include savings in material costs, faster data readout and the possibility to use one sensor instead of many for different beam shapes.
Another aspect of the invention is the method of manufacturing the mosaic like sensor structure by leaving a finite physical gap between adjacent detector elements. This structure is a departure from the prior art teachings of eliminating dead space between individual detector chips. This inventive manufacturing method of not providing minimum dead space within the active imaging area brings definite advantages in terms of production yield and long term endurance of the sensor. Since solid state semiconductors are generally fragile crystals, mounting them in physical contact increases greatly the risk of damaging the crystal edges with cracks or fractures during production. It also leaves the detector elements much more vulnerable to damage caused by thermal expansion or mechanical shock compared to the method of mounting the elements with an intermediate physical gap. Moreover, physical contact between the semiconductor detector crystals can lead to distortions in the signal collecting electric field applied to the crystals. The gap between the detector elements may be simply empty space or the gap may be created by placing some material such a mylar film in between the detector elements. The size of the gap is preferably but not necessary equal to or a multiple of the pixel size of the detector elements.
Still another aspect of the invention is the effective method of manufacturing several different mosaic type sensors with active areas of dissimilar irregular shape on identical sensor substrates the substrate being generally a printed circuit board (PCB). Since the control and signal readout schemes of the separate detector elements are identical it is possible to design one PCB to accommodate different combinations of detector elements. Thus with one type of a PCB and one (or more) type of a detector element, sensors with various shapes of active area for different applications can be produced easily and without the need of any costly and time consuming design changes of the substrate. Alternatively, a desired shape of the active sensor area can be constructed by combining side by side two or more separate either identical or non-identical sensor substrates each substrate populated with one or more detector elements of either similar or dissimilar size or shape.
The invention especially applies to X-ray imaging sensors made of CdTe-CMOS pixel detectors but it is not limited to this technology and also finds relevance in other technologies as well such as in the scintillator-CCD technology.
The invention is to be used in particular in dental extraoral X-ray imaging but is beneficial in other application as well.
A inventive radiation imaging device includes plural individual detectors defining an irregular rectangular active area responsive to x-rays and with different widths along a length of the active area. The individual detectors may be of different rectangular shapes and mounted on a motherboard. The motherboard may be formed of a first module mounting a first of two individual detectors and a second module detachable connected to the first module and mounting a second of two individual detectors.
A preferred shape 5 of the active area of the invented X-ray sensor is shown in
As illustrated by
The invention finds particular application with different kinds of tiled imaging devices comprising a scintillator or a phosphor on a CCD or CMOS sensor, or a combination os a CCD or CMOS imaging device(s) with a flat panel.
The term “pixel” in the context of this invention usually has the meaning of the physical pixel size on the imaging device or on the detector. However, “pixel” also has the meaning and includes the final image pixel size as displayed in a viewing means. For example, the size of the final image pixel in the image as is displayed on a computer monitor.
In certain cases the user may choose to combine (or bin) the detector (or imaging device) physical pixels in order to be able to increase the x-ray photon statistics on the finally displayed image and/or to be able to process faster the resulting image. Thus, the image as displayed may have a final image pixel size that differs from the detector physical pixel size. For example the invention allows for a 2×2 binning, a 3×3 binning, etc. The displayed image may also have asymmetric binning, for example 1×2 or 2×1 etc.
For the purposes of this invention, reference to the width of the gap being preferably less than 400% of the pixel size, means that the physical pixel size of the detector or the final image pixel size of the final image as displayed, as the case might be. For example, if the detector pixel size is 0.1 mm and there is a 2×2 binning, then the final image as displayed will have a pixel size of 0.2×0.2 mm**2 and the gap between the individual detector elements should be less than 400% of the 0.2 mm, i.e., less than 0.8 mm. Thus, the gap between the detector elements is in relation to the pixel size as perceived by a viewer of the image and the higher the resolution of the final image, the smaller the gap should be.
In one embodiment, the inventive radiation imaging device is made of individual detectors Cd(Zn)Te detectors juxtaposed next to each other with an average physical gap of at least 0.005 mm between the edges of the Cd(Zn)Te detectors, a physical average gap of between 0.005 mm-0.4 mm between the edges being preferred. This gap can be provided by a film, e.g., by a mylar thick 0.005 mm-0.4 mm thick or alternatively by accurately placing the Cd(Zn)Te detectors using a microscope having an average gap in the above range.
The data is acquired at a predefined rate as image frames each frame corresponding to a certain position of the X-ray source and sensor along the rotational path of the scan. The data is sent to a computer 31 for image reconstruction and display. A full panoramic layer or a local part of a panoramic layer as well as a transverse slice or a 3D image corresponding to a local part of a panoramic layer can be reconstructed from the data frames.
The system of
Thus, the system provides an x-ray imaging device adapted for producing multiple frames from a single x-ray imaging device during at least part of the exposure. The x-ray imaging device comprises a plurality of individual semiconductor pixel detectors in an array defining an active area responsive to x-rays. The active area having a rectangular shape with length y and a width x, with the width x having at least two different values for corresponding ranges along the length y.
Each detector is composed of pixels. An average physical gap is defined between each set of adjacent edges of adjacent ones of the individual detectors, each of the average physical gaps of all of the plural individual detectors is up to 400% of a pixel size of the pixels of the image produced by the radiation imaging as displayed for viewing.
The computer 31, a processor, processes the frames of a single exposure to compose selectively at least two of a group of elements, the elements comprising (a) a predetermined dental panoramic layer image, (b) a local part of a non-predetermined dental panoramic layer image, (c) a transverse slice to a local part of a dental panoramic layer image; and (d) 3-D reconstruction of a volume corresponding to some local part of a dental panoramic layer.
Further, at least two preselected programs may be provided for exposure for executing corresponding exposure profiles to compose selectively at least two of a group of elements, the elements comprising (a) a panoramic image, (b) a cephalometric image, (c) a transverse slice to a local part of a dental panoramic layer image; and (d) a 3-D reconstruction of a volume of interest.
The present application is a continuation of copending application Ser. No. 12/772,251 filed on May 3, 2010; which claims the benefit of prior filed U.S. patent application Ser. No. 11/819,018 filed on Jun. 25, 2001; which claims the benefit of prior filed U.S. patent application Ser. No. 11/673,583 filed on Feb. 11, 2007; which claims the benefit of prior filed U.S. patent application Ser. No. 11/277,530 filed on Mar. 27, 2006; which claims the benefit of prior filed U.S. provisional application Ser. No. 60/677,020 filed on May 2, 2005. The entire contents of each of the above-identified applications are hereby incorporated by reference.
Number | Name | Date | Kind |
---|---|---|---|
4188537 | Franke | Feb 1980 | A |
4823369 | Guenther et al. | Apr 1989 | A |
4878234 | Pfeiffer et al. | Oct 1989 | A |
4995062 | Schulze-ganzlin et al. | Feb 1991 | A |
5195114 | Sairenji et al. | Mar 1993 | A |
5383097 | Delucia et al. | Jan 1995 | A |
5784429 | Arai | Jul 1998 | A |
6049584 | Pfeiffer | Apr 2000 | A |
6118842 | Arai et al. | Sep 2000 | A |
6448544 | Stanton et al. | Sep 2002 | B1 |
6466641 | Virta et al. | Oct 2002 | B1 |
6496557 | Wilson et al. | Dec 2002 | B2 |
7016461 | Rotondo et al. | Mar 2006 | B2 |
7136452 | Spartiotis et al. | Nov 2006 | B2 |
7336763 | Spartiotis et al. | Feb 2008 | B2 |
7340032 | Besson | Mar 2008 | B2 |
7426260 | Cantu et al. | Sep 2008 | B2 |
7515678 | Hsieh et al. | Apr 2009 | B2 |
7676022 | Pantsar et al. | Mar 2010 | B2 |
7742560 | Spartiotis et al. | Jun 2010 | B2 |
7916833 | Pantsar et al. | Mar 2011 | B2 |
8295432 | Spartiotis et al. | Oct 2012 | B2 |
8532254 | Pantsar et al. | Sep 2013 | B2 |
8693624 | Spartiotis et al. | Apr 2014 | B2 |
20010048732 | Wilson et al. | Dec 2001 | A1 |
20040000630 | Spartiotis et al. | Jan 2004 | A1 |
20040133095 | Dunki-Jacobs et al. | Jul 2004 | A1 |
20040190678 | Rotondo et al. | Sep 2004 | A1 |
20050249331 | Wear et al. | Nov 2005 | A1 |
20060011852 | El-Hanany et al. | Jan 2006 | A1 |
20060126781 | Hartung et al. | Jun 2006 | A1 |
20060233301 | Erhardt et al. | Oct 2006 | A1 |
Number | Date | Country |
---|---|---|
0 138 647 | Apr 1985 | EP |
0 421 869 | Apr 1991 | EP |
0 673 623 | Sep 1995 | EP |
2 228 765 | Dec 1994 | GB |
07-275240 | Oct 1995 | JP |
09-122118 | May 1997 | JP |
10-225455 | Aug 1998 | JP |
2002-017718 | Jan 2002 | JP |
02052505 | Jul 2002 | WO |
03077319 | Sep 2003 | WO |
2004055550 | Jul 2004 | WO |
2004084728 | Oct 2004 | WO |
WO 2004084728 | Oct 2004 | WO |
2006109806 | Dec 2006 | WO |
Entry |
---|
PCT International Search Report mailed Feb. 1, 2010, in PCT Application No. PCT/IB2008001608. |
Certified Translation of PCT/DE04/00620. |
Number | Date | Country | |
---|---|---|---|
20130003921 A1 | Jan 2013 | US |
Number | Date | Country | |
---|---|---|---|
60677020 | May 2005 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 11277530 | Mar 2006 | US |
Child | 11673583 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12772251 | May 2010 | US |
Child | 13609672 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 11819018 | Jun 2007 | US |
Child | 12772251 | US | |
Parent | 11673583 | Feb 2007 | US |
Child | 11819018 | US |