The invention relates generally to apparatus and methods for imaging for differentiating material characteristics, and more specifically to differentiating material characteristics using a hybrid imaging system.
In X-ray computed tomography (CT), cross-sectional images are generated of a scanned object. The values in the images represent the linear attenuation coefficient of the underlying tissue. As will be appreciated, the linear attenuation coefficient may be defined as a product of mass attenuation coefficient and density of the underlying tissue. Additional information may be obtained by not only reconstructing the degree of attenuation, but also the energy dependence of the attenuation. This type of information is much more material specific, and allows a user to distinguish between different materials with similar linear attenuation coefficients (i.e., the product of mass attenuation coefficient and density is comparable for both materials). In order to reduce the number of degrees of freedom, the energy-dependent attenuation is decomposed into a limited number of basis functions (typically Compton effect and photon-electric effect; or material 1 and material 2, etc.).
Previously conceived techniques employed dual or multiple energy techniques to facilitate material decomposition, which was achieved by acquiring projection data sets at two or more X-ray source voltages and/or different filtration. A more advanced technique is to use energy discrimination detectors, such as photon-counting detectors with multiple energy bins. However, the use of photon counting detectors suffers from limitations such as limited count rate capability (e.g., a few MHz/detector pixel), which limits the total X-ray flux rate, and hence the image quality, that may be obtained within a limited acquisition time interval. Additionally, the decomposition into different basis functions typically results in noise amplification in the images. Furthermore, the presence of scatter may cause error in the decomposition results.
There is therefore a need for an imaging system capable of energy discrimination and energy integration. In particular, there is a significant need for a design of a hybrid detector capable of energy discrimination and energy integration.
Briefly, in accordance with aspects of the present technique, a system is presented. The system includes a plurality of energy integrating detector elements configured to acquire energy integrating data. Further, the system includes a plurality of energy discriminating detector elements configured to acquire energy discriminating data, where the plurality of energy integrating detector elements and the plurality of energy discriminating detector elements are arranged in a spatial relationship to form a hybrid detector, and where the plurality of energy integrating detector elements and the plurality of energy discriminating detector elements are configured to obtain respective sets of energy integrating data and energy discriminating data for use in generating an image.
In accordance with another aspect of the present technique, a detector module is presented. The detector module includes a plurality of detector assemblies disposed on an interconnection substrate.
In accordance with yet another aspect of the present technique, a detector module is presented. The detector module includes a first layer comprising a plurality of energy integrating detector elements disposed on a first substrate, where the plurality of energy integrating detector elements is configured to acquire energy integrating data. The detector module also includes a second layer comprising a filtering element disposed adjacent the first layer, where the filtering element is configured to attenuate X-ray spectra. Furthermore, the detector module includes a third layer comprising a plurality of energy discriminating detector elements disposed adjacent the second layer and disposed on a second substrate, where the plurality of energy discriminating detector elements is configured to acquire energy discriminating data.
In accordance with further aspects of the present technique, a method of imaging is presented. The method includes obtaining energy integrating image data from a plurality of energy integrating detector elements. Additionally, the method includes obtaining energy discriminating image data from a plurality of energy discriminating detector elements. The method also includes combining the energy integrating image data and the energy discriminating image data to form combined image data, where the plurality of energy integrating detector elements and the plurality of energy discriminating detector elements are arranged in a spatial relationship to form a hybrid detector, and where the plurality of energy integrating detector elements and the plurality of energy discriminating detector elements are configured to obtain respective sets of energy integrating data and energy discriminating data for use in generating an image.
In accordance with another aspect of the present technique, an imaging system is presented. The imaging system includes one or more sources of radiation configured to emit a stream of radiation toward a patient to be scanned. Furthermore, the imaging system includes a computer configured to generate images with enhanced image quality and to provide tissue composition information. The imaging system also includes a detector assembly configured to detect the stream of radiation and to generate one or more signals responsive to the stream of radiation, where the detector assembly includes a plurality of energy integrating detector elements configured to acquire energy integrating data and a plurality of energy discriminating detector elements configured to acquire energy discriminating data, where the plurality of energy integrating detector elements and the plurality of energy discriminating detector elements are arranged in a spatial relationship to form a hybrid detector, and where the plurality of energy integrating detector elements and the plurality of energy discriminating detector elements are configured to obtain respective sets of energy integrating data and energy discriminating data for use in generating an image. In addition, the imaging system includes a system controller configured to control the rotation of the one or more sources of radiation and the detector assembly and to control the acquisition of one or more sets of projection data from the detector assembly via a data acquisition system. The imaging system also includes a computer system operationally coupled to the one or more sources of radiation and the detector assembly, where the computer system is configured to receive the one or more sets of projection data.
These and other features, aspects, and advantages of the present invention will become better understood when the following detailed description is read with reference to the accompanying drawings in which like characters represent like parts throughout the drawings, wherein:
Conventional CT detectors typically produce an electronic signal I that is proportional to a total amount of absorbed X-ray energy in each view. The electronic signal I may be given by:
where NK is representative of the number of detected X-ray photons with energy EK.
Consequently, the signal I does not contain any information regarding energy distribution of the individual photons. This mode of detection is generally referred to as “energy integrating” detection and detectors configured for such operation are generally referred to as energy integrating detectors with proportional energy weighting.
Further, a different type of detector, called a photon counting detector without energy discrimination, may be configured to measure a value proportional to the total number of photons N absorbed in each view. It may be noted that in this type of detector, the photons are uniformly weighted irrespective of energies before summation. The electronic signal I may be given by:
Such a detector is generally referred to as an energy integrating detector with equal energy weighting. The signal I in such a detector does not contain any information regarding energy distribution of the individual photons. It may be noted that energy integrating (EI) detectors with proportional or equal energy weighting may be considered as one class of detectors. This class of energy integrating detectors does not provide energy discrimination information.
Alternately, a detector may be configured to preferentially weight the number of photons within two or more energy intervals. This mode of detection is generally referred to as “energy discriminating” detection. Energy discriminating (ED) detectors may be implemented in different ways including the use of photon counting detectors with multiple energy bins.
Energy discriminating detectors provide some information regarding the energy distribution of the detected photons. These detectors may produce two or more signals corresponding to two or more energy intervals. The energy intervals may include a high energy signal and a low energy signal, for example. Accordingly, for a detector with two energy bins and energy weighting factors LK and HK the corresponding low energy and high energy signals may be given most generally by:
where NK is representative of the number of detected X-ray photons with energy EK.
Furthermore, for a photon counting energy discriminating detector having a plurality of energy bins, the weight factors may be chosen to be identical for all energies. Accordingly, the signal I may be represented by:
where each bin corresponds to a different energy interval.
Such photon counting energy discriminating detectors may saturate at high photon count rate and therefore operate correctly only within a limited dynamic range of X-ray flux rate. This additional information regarding the energy may be employed to advantageously reduce beam-hardening artifacts and more importantly to obtain more material-specific information.
Furthermore, conventional CT produces a CT number for each voxel. The CT number is typically the linear attenuation coefficient μre-scaled relative to the linear attenuation coefficients of vacuum and water. However, as will be appreciated, the linear attenuation coefficient is also a function of energy μ(E). Therefore, each reconstructed value may be representative of an effective linear attenuation coefficient μeff which is a weighted average of μ(E) over the used X-ray energy range. However, employing this approximation results in beam-hardening artifacts and eliminates the capability to identify two materials having similar average attenuation characteristics. Energy discriminating detectors may be employed to overcome the shortcomings discussed hereinabove. The energy discriminating detectors facilitate obtaining measurements over multiple energy intervals that provide extra information that may be necessary to reconstruct any extra unknowns.
A hybrid detector is a detector that advantageously includes energy integrating detector elements and energy discriminating detector elements. The energy integrating detector elements facilitate detecting a large number of photons, while the energy discriminating detector elements facilitate capturing additional information based on the energy-dependency of the attenuation. As will be described in detail hereinafter, a hybrid detector in accordance with exemplary aspects of the present technique is presented. As will be appreciated by one skilled in the art, the figures are for illustrative purposes and are not drawn to scale. Additionally, although, the exemplary embodiments illustrated hereinafter are described in the context of X-ray CT, it will be appreciated that use of the exemplary embodiments in emission tomography, such as Positron Emission Tomography (PET) and Single Photon Emission Computed Tomography (SPECT) are also contemplated in conjunction with the present technique. Furthermore, although, the exemplary embodiments illustrated hereinafter are described in the context of a medical imaging system, it will be appreciated that use of the exemplary embodiments in industrial applications, such as, but not limited to, explosive detection systems, luggage scanning systems and non-destructive evaluation systems are also contemplated in conjunction with the present technique.
The source of radiation 12 may be positioned near a collimator 14, which may be configured to shape a stream of radiation 16 that is emitted by the source of radiation 12. The stream of radiation 16 passes into the imaging volume containing the subject to be imaged, such as a human patient 18. The stream of radiation 16 may be generally fan-shaped or cone-shaped, depending on the configuration of the detector array, discussed below, as well as the desired method of data acquisition. A portion 20 of radiation passes through or around the subject and impacts a detector array, represented generally at reference numeral 22. Detector elements of the array produce electrical signals that represent the intensity of the incident X-ray beam. These signals are acquired and processed to reconstruct an image of the features within the subject.
The radiation source 12 is controlled by a system controller 24, which furnishes both power, and control signals for CT examination sequences. Moreover, the detector 22 is coupled to the system controller 24, which commands acquisition of the signals generated in the detector 22. The system controller 24 may also execute various signal processing and filtration functions, such as for initial adjustment of dynamic ranges, interleaving of digital image data, and so forth. In general, system controller 24 commands operation of the imaging system to execute examination protocols and to process acquired data. In the present context, system controller 24 also includes signal processing circuitry, typically based upon a general purpose or application-specific digital computer, associated memory circuitry for storing programs and routines executed by the computer, as well as configuration parameters and image data, interface circuits, and so forth.
In the embodiment illustrated in
Additionally, as will be appreciated by those skilled in the art, the source of radiation 12 may be controlled by an X-ray controller 30 disposed within the system controller 24. Particularly, the X-ray controller 30 is configured to provide power and timing signals to the X-ray source 12.
Further, the system controller 24 is also illustrated comprising a data acquisition system 34. In this exemplary embodiment, the detector 22 is coupled to the system controller 24, and more particularly to the data acquisition system 34. The data acquisition system 34 receives data collected by readout electronics of the detector 22. The data acquisition system 34 typically receives sampled analog signals from the detector 22 and converts the data to digital signals for subsequent processing by a computer 36.
The computer 36 typically is coupled to or incorporates the system controller 24. The data collected by the data acquisition system 34 may be transmitted to the computer 36 for subsequent processing and reconstruction, or stored directly to memory 38. The computer 36 may comprise or communicate with a memory 38 that can store data processed by the computer 36 or data to be processed by the computer 36. It should be understood that any type of memory configured to store a large amount of data might be utilized by such an exemplary system 10. Moreover, the memory 38 may be located at the acquisition system or may include remote components, such as network accessible memory media, for storing data, processing parameters, and/or routines for implementing the techniques described below.
The computer 36 may also be adapted to control features such as scanning operations and data acquisition that may be enabled by the system controller 24. Furthermore, the computer 36 may be configured to receive commands and scanning parameters from an operator via an operator workstation 40, which is typically equipped with a keyboard and other input devices (not shown). An operator may thereby control the system 10 via the input devices. Thus, the operator may observe the reconstructed image and other data relevant to the system from computer 36, initiate imaging, and so forth.
A display 42 coupled to the operator workstation 40 may be utilized to observe the reconstructed images. Additionally, the scanned image may also be printed by a printer 44, which may be coupled to the operator workstation 40. The display 42 and printer 44 may also be connected to the computer 36, either directly or via the operator workstation 40. The operator workstation 40 may also be coupled to a picture archiving and communications system (PACS) 46. It should be noted that PACS 46 might be coupled to a remote system 48, such as radiology department information system (RIS), hospital information system (HIS) or to an internal or external network, so that others at different locations may gain access to the image data.
It should be further noted that the computer 36 and operator workstation 40 may be coupled to other output devices, which may include standard or special purpose computers and associated processing circuitry. One or more operator workstations 40 may be further linked in the system for outputting system parameters, requesting examinations, viewing images, and so forth. In general, displays, printers, workstations, and similar devices supplied within the system may be local to the data acquisition components, or may be remote from these components, such as elsewhere within an institution or hospital, or in an entirely different location, linked to the image acquisition system via one or more configurable networks, such as the Internet, a virtual private network or the like.
As noted above, an exemplary imaging system utilized in a present embodiment may be a CT scanning system 50, as depicted in greater detail in
In typical operation, the X-ray source 12 projects an X-ray beam 64 from the focal point and toward detector array 22. The collimator 14 (see
Thus, as the X-ray source 12 and the detector 22 rotate, the detector 22 collects data related to attenuated X-ray beams 66. Data collected from the detector 22 then undergoes pre-processing and calibration to condition the data to represent the line integrals of the attenuation coefficients of the scanned objects. The processed data, commonly called projections, may then be filtered and backprojected to generate an image of the scanned area. An image may be reconstructed, in certain modes, using projection data for less or more than 360 degrees of rotation of the gantry 52.
In accordance with aspects of the present technique, various exemplary embodiments of a hybrid detector are presented. As used herein, a “hybrid” detector is a detector that includes a plurality of energy integrating detector elements and a plurality of energy discriminating detector elements arranged in a predetermined pattern. Also, the hybrid detector may include a planar detector, a ring-shaped detector, an arc-shaped detector, or combinations thereof. The various shapes of the hybrid detector, and the numerous arrangements of the energy integrating and energy discriminating detector elements will be described in greater detail with reference to
Turning now to
By implementing the detector arc 72 as described hereinabove, patient scan data acquired at zero degrees may be rescanned at 180 degrees incorporating full 360 degrees scanning and fan-to-parallel rebinning. However, as the tube and the detector assembly are rotated around the patient, the energy integrating detector elements 74 and the energy discriminating detector elements 73 swap sides relative to the patient. Using this opposing view geometry of the detector arc 72, energy integrating data may always be available to correct for possible saturated data from the energy discriminating detector elements 73 in every view of the scan. As will be appreciated, in cone-beam geometries of the detectors, direct rays and conjugate rays may be located at different positions. It may be noted that the arrangement of the energy integrating detector elements and energy discriminating detector elements described hereinabove may also be adapted for use in the cone-beam geometries.
Alternatively, a select part of the detector arc 78 may be configured to include a plurality of energy discriminating detector elements and a plurality of energy integrating detector elements arranged in a “comb like” pattern. In certain embodiments, every Nth energy discriminating detector element may be replaced with an energy integrating detector element. For example, in one embodiment, the detector arc 78 may include a plurality of energy discriminating detector elements disposed in a row, where every 5th energy discriminating detector element is replaced with an energy integrating detector element (not shown). Furthermore, in certain other embodiments, every Nth energy discriminating detector element may be “shielded” by an energy integrating detector element, as illustrated in
By implementing the detector arc 78 as described hereinabove, measurements detected from the sparsely distributed energy integrating detector elements 81 may be utilized to correct measurements obtained from the neighboring saturated energy discriminating detector elements 80. Additionally, self-absorption of these energy integrating detector elements 81 facilitates reduction in flux to the underlying energy discriminating detector elements 80 thereby ensuring that the energy discriminating detector elements 80 are substantially precluded from reaching saturation. These “shielded” measurements from the energy discriminating detector elements 80 provide a more precise correction for their neighboring “unshielded” energy discriminating detector elements 80.
It may be noted that, in certain embodiments, the roles of the energy integrating detector elements 81 and the energy discriminating detector elements 80 may be reversed depending on the size of the features to be evaluated in the object. In other words, the energy discriminating detector elements 80 may be disposed on the top while the energy integrating detector elements 81 may be disposed below the energy discriminating detector elements 80. Furthermore, detector parameters, such as thickness of direct conversion material, may be adjusted in the energy discriminating detector elements 80 to facilitate prevention of saturation of the energy discriminating detector elements 80.
Referring now to
In accordance with exemplary aspects of the present technique, two outer portions of the X-ray beam may be measured by the plurality of energy integrating detector elements, while a central portion of the X-ray beam may be measured by the plurality of energy discriminating detector elements. Accordingly, as depicted in the illustrated embodiment 92, the two outer portions of the X-ray beam 101 generated by the first source of radiation 93 may be measured by the plurality of energy integrating detector elements in the first and second side wings 96, 97. Moreover, the central portion of the X-ray beam 102 generated by the first source of radiation 93 may be measured by the plurality of energy discriminating detector elements in the central portion 98 of the detector arc 95.
Similarly, the two outer portions of the X-ray beam 103 generated by the second source of radiation 94 may be measured by the plurality of energy integrating detector elements in the first and second side wings 96, 97. Furthermore, the central portion of the X-ray beam 104 generated by the second source of radiation 94 may be measured by the plurality of energy discriminating detector elements in the central portion 98 of the detector arc 95.
By implementing the detector arc 95 as described hereinabove, a center portion of the region of interest, such as a relatively smaller region of interest 100, may be reconstructed with energy information, where as a relatively larger region of interest 99 may be used to support the reconstruction by providing attenuation information outside the relatively smaller region of interest 100. In other words, sufficient data is available to reconstruct the relatively larger region of interest 99 without energy information. Additionally, sufficient data is available to reconstruct the relatively smaller region of interest 100 with energy information.
As illustrated in
It may be noted the detector modules illustrated in
Optionally, some of the detector elements, such as the energy discriminating detector elements may also be offset in height. This arrangement greatly facilitates reduction in sensitivity of the detector elements to scatter as the detector elements positioned a little deeper are less sensitive to scatter. Additionally, regions in the scintillator of the energy integrating detector elements may be selectively configured to be less absorptive by reducing scintillator thickness or by reducing material doping, thereby allowing flexibility in positioning of the energy discriminating detector elements behind the energy integrating detector elements. Moreover, behind the less absorptive regions of the scintillator in the energy integrating detector elements, collimating plates may be employed to reduce residual scatter in measurements from the energy discriminating detector elements, thereby enabling improved material composition estimates.
Referring now to
Furthermore, the area detector 152 may be constructed employing high resolution and/or energy discriminating detector elements, whereas the fan detector 153 may be constructed using low resolution and/or energy integrating detector elements. Accordingly, the cross-shaped configuration is an arrangement whereby a region of an object at the center of the field of view is projected to a wide detector coverage detector, whereas the peripheral region of the object is projected to a narrow coverage. Such an arrangement allows leveraging the fact that the object attenuation is greatest in the center. As a result, the energy discriminating detector elements in the area detector 152 will not be saturated. In addition, a central portion of the detector, such as the area detector 152, has a larger coverage of the object. Accordingly, this larger coverage may be leveraged for cardiac imaging. In conventional geometries, cardiac imaging requires a strongly reduced table speed. However, if the central portion of the detector, such as the area detector 152, which corresponds to the heart region, is wider, the table speed may be increased again.
In addition, this exemplary arrangement 140 may also include a first outer source 141, a second outer source 143 and a central source 142. The sources of radiation 141, 142, 143 may be configured to separately illuminate the area detector 152 and the fan detector 153 or the fan detector 153 and a central portion of the area detector 152. The central source 142 may be configured to illuminate the area detector 152 and the fan detector 153, or a central portion of the area detector 152 and the fan detector 153. Also, the additional sources 141 and 143 may be configured to illuminate only the area detector 152. For example, the additional sources 141 and 143 allow may be configured to facilitate reduced cone-beam artifacts in the relatively small region of interest 150, particularly in axial acquisition modes.
A source collimator is represented by reference numeral 144, while a source gating and collimating control is represented by reference numeral 146. As illustrated in
Turning now to
It may be noted that, it is also contemplated that the detector 166 may include one or more rings. In one embodiment, a plurality of energy integrating detector elements 168 may be disposed on a first ring-shaped detector, while a plurality of energy discriminating detector elements 170 may be disposed on a second ring-shaped detector. The detector 166 may also include alternating rings of energy integrating detector elements and energy discriminating detector elements. Additionally, a plurality of energy integrating detector elements 168 and a plurality of energy discriminating detector elements 170 may be arranged on the one or more ring-shaped detectors in a checkerboard pattern. Moreover, the energy integrating detector elements 168 and energy discriminating detector elements 170 may be arranged in a plurality of configurations on the one or more ring-shaped detectors. For example, the energy integrating detector elements 168 and energy discriminating detector elements 170 may be disposed on the one or more ring-shaped detectors arranged based on the numerous arrangements of energy integrating detector elements and energy discriminating detector elements illustrated in
The detector module 188 may also include an interconnection substrate 194. The interconnection substrate 194 may include readout electronics and may be configured to facilitate coupling the plurality of energy integrating detector elements 178 and the plurality of energy discriminating detector elements 182 to associated readout electronics. It may be noted that the readout electronics may be configured to facilitate reading out signals from each of the plurality of energy integrating detector elements 178 and each of the plurality of energy discriminating detector elements 182. In certain embodiments, the interconnection substrate 194 may include a printed circuit board (PCB) or a ceramic electrical wiring board substrate, for example. Furthermore, in certain embodiments, the interconnection substrate 194 may include electronics disposed thereon, where the electronics may be configured to transmit and receiver data and/or power to the detector module 190.
Furthermore, the interconnection substrate 194 may include one or more interconnect pads 196 that may be configured to facilitate coupling the plurality of energy discriminating detector elements 182 to respective readout electronics. In certain embodiments, the interconnection substrate 194 may include a plurality of strips of interconnect pads to facilitate coupling a plurality of back-connected energy discriminating detector elements 182 to associated readout electronics. However, in certain other embodiments, the interconnection substrate 194 may include a full array of interconnect pads configured to facilitate coupling the plurality of back-connected energy discriminating detector elements 182 to respective readout electronics.
Moreover, the interconnection substrate 194 may also include wire bond pads 198. The plurality of energy integrating detector elements 178 may be coupled to the interconnection substrate 194 by operatively coupling the wire bonds 180 to the wire bond pads 198. It may be noted that use of backlit diodes does not call for use of wire bond pads 198. However, the wire bond pads 198 may be included for front-lit diodes employed in the substrate 176. Additionally, reference numeral 200 is representative of readout electronics associated with the plurality of energy integrating detector elements 178. Similarly, reference numeral 202 represents readout electronics associated with the plurality of energy discriminating detector elements 182. In certain embodiments, the readout electronics 200 and 202 may include application specific integrated circuits (ASICs). Furthermore, reference numeral 204 is representative of a direction of operatively coupling the detector assembly 190 to the interconnection substrate 194. In one embodiment, the detector assembly 190 may be electrically bonded to the interconnection substrate 194.
Turning now to
Referring now to
Turning now to
As previously noted with reference to
Turning now to
An assembly including the plurality of energy integrating detector elements 302, the plurality of energy discriminating detector elements 304 and the substrate 306 including the through-via interposer therein may be disposed on a first side of the interconnection substrate 308. Also, the flex circuit 310 having the energy integrating ASICs 312 and the energy discriminating ASICs 314 may be disposed on a second side of the interconnection substrate 308, where the second side is opposingly disposed from the first side of the interconnection substrate 308. The plurality of energy integrating detector elements 302 and the plurality of energy discriminating detector elements 304 may be operatively coupled to the corresponding readout electronics, such as the energy integrating ASICs 312 and the energy discriminating ASICs 314, via the interposer included with substrate 306.
The detector module 330 may include a first layer 332, a second layer 334, a third layer 336 and a fourth layer 338. The first layer 332 may include a plurality of energy integrating detector elements 340 arranged with X-ray transparent kerfs between the energy integrating detector elements on a first substrate 342, where the substrate 342 may include one or more wire bonds 344. In certain embodiments, the first substrate may include a scintillator sensor, for example. Additionally, the first layer 332 may also include a first interconnection substrate 346 that may be configured to facilitate coupling the plurality of energy integrating detector elements 340 to corresponding readout electronics. Accordingly, the first interconnection substrate 346 may include one or more wire bond pads 348 disposed thereon. The wire bonds 344 disposed on the substrate 342 may be coupled to the wire bond pads 348 via wires 350. Furthermore, the first interconnection substrate 346 may also include one or more energy integrating ASICs 352 disposed thereon. Also, the plurality of energy integrating detector elements 340 may be operatively coupled to corresponding readout electronics, such as energy integrating ASICs 352, via wires 350.
The second layer 334 may include a filtering element 354. In one embodiment, the filter 354 may be a movable filter, while in other embodiments the filtering element 354 may include a fixed filter. In certain embodiments, the filtering element may be adapted to attenuate relatively low energy X-ray spectra. In addition, the third layer 336 may include a plurality of energy discriminating detector elements 356 which receives the signal transmitted through the kerfs of the first layer 332. It may be noted that the plurality of energy discriminating detector elements 356 may be disposed on a second substrate (not shown). The second substrate may include a ceramic substrate, for example. Moreover, the fourth layer 338 may include a second interconnection substrate 358 configured to facilitate operatively coupling the plurality of energy discriminating detector elements 356 in the third layer 336 to corresponding readout electronics, such as energy discriminating ASICs 362 that may be disposed on the second interconnection substrate 358. The second interconnection substrate 358 may also include one or more interconnect pads 360 that may be configured to facilitate coupling the plurality of energy discriminating detector elements 356 to the second interconnection substrate 358. The plurality of energy discriminating detector elements 356 may be operatively coupled to the energy discriminating ASICs 362 via the second interconnection substrate 360. It may be noted that even though as illustrated in
The various embodiments of the apparatus for hybrid CT imaging and methods for hybrid CT imaging discussed hereinabove facilitate arranging a plurality of energy integrating detector elements and a plurality of energy discriminating detector elements in a one-dimensional or a two-dimensional detector array.
Furthermore, the use of energy discriminating detector elements of relatively small size advantageously facilitates reduction in the count rate. Additionally, as the plurality of energy discriminating detector elements are pre-attenuated, reduction in the count rate may be obtained. Also, the flux rate to the energy discriminating detector elements disposed beneath the energy integrating detector elements may be advantageously controlled via selective doping of the scintillator material or selectively controlling the thickness of the scintillator material. Furthermore, collimation of the energy discriminating detector elements cells beneath the energy integrating detector elements facilitates scatter reduction in the measurements obtained from the energy discriminating detector elements, thereby improving material composition estimates.
While only certain features of the invention have been illustrated and described herein, many modifications and changes will occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all such modifications and changes as fall within the true spirit of the invention.