PRECISION AND RESOLUTION OF QUANTITATIVE IMAGING BY COMBINING SPECTRAL AND NON-SPECTRAL MATERIAL DECOMPOSITION
20190159741 ยท 2019-05-30
Assignee
Inventors
Cpc classification
G01T1/2985
PHYSICS
A61B6/5235
HUMAN NECESSITIES
A61B6/5205
HUMAN NECESSITIES
A61B6/4241
HUMAN NECESSITIES
International classification
A61B6/00
HUMAN NECESSITIES
Abstract
The invention proposes to combine spectral image data with non-spectral image data in order to overcome limitations of the different data taking methods. Results from the methods are preferably combined as functions of spatial frequency so that spectral image data provide high accuracy at low frequencies, whereas the non-spectral image data helps reducing the noise at high frequencies. The invention enables a range of applications in different fields of X-ray imaging such as improved tissue contrast and tissue characterization.
Claims
1. A calculation unit for processing quantitative image data, wherein the calculation unit comprises, a receiving unit; and a processing unit, wherein the receiving unit is configured for receiving spectral image data of an object of interest; wherein the receiving unit is configured for receiving non-spectral image data of the object of interest, wherein the processing unit is configured for calculating material properties as a function of position from the spectral image data; wherein the processing unit is configured for calculating material properties as a function of position from the non-spectral image data; wherein the processing unit is configured for combining the material properties calculated from the spectral and from the non-spectral image data as a function of spatial frequency by weighting the spectral and the non-spectral image data depending on the spatial frequencies in the image.
2. The calculation unit according to claim 1, wherein the processing unit is configured to give stronger weight to the low-spatial-frequency parts of the spectral image data as compared to the low-spatial-frequency parts of the non-spectral image data; and wherein the processing unit is configured to give stronger weight to the high-spatial-frequency parts of the non-spectral image data as compared to the high-spatial-frequency parts of the spectral image data.
3. The X-ray imaging system, comprising a calculation unit of claim 1, and an imaging unit, wherein the imaging unit is configured to provide spectral and non-spectral image data to the calculation unit.
4. The X-ray imaging system according to claim 3, wherein the spectral and/or the non-spectral image data are phase contrast image data, differential phase contrast image data, or dark field image data.
5. A method for quantitative image data processing, the method comprising the following steps: Acquiring spectral image data of an object of interest; Calculating material properties as a function of position from the spectral image data; Acquiring non-spectral image data of the object of interest; Calculating material properties as a function of position from the non-spectral image data; and Combining the material properties calculated from the spectral and from the non-spectral image data as a function of spatial frequency comprising the step of weighting the spectral and the non-spectral image data depending on the spatial frequencies of the image.
6. The method according to claim 5, wherein the spectral image data are spectral tomosynthesis data and/or the non-spectral image data are non-spectral tomosynthesis data.
7. The method according to claim 5, wherein the step of acquiring the non-spectral image comprises using additional a priori assumptions and/or additional data input.
8. The method according to claim 5, wherein the step of combining the material properties calculated from the spectral and from the non-spectral image data as a function of spatial frequency is at least partly carried out in the spatial-frequency domain.
9. The method according to claim 5, wherein the step of combining the material properties calculated from the spectral and from the non-spectral image data as a function of spatial frequency is at least partly carried out in the spatial domain and comprises the step of a convolution with a filter kernel and/or other means of low-pass, band-pass or high-pass filtering.
10. The method according to claim 5, wherein the step of weighting as a function of spatial frequency gives stronger weight to the low-spatial-frequency parts of the spectral image data as compared to the low-spatial-frequency parts of the non-spectral image data, and wherein the step of weighting as a function of spatial frequency gives stronger weight to the high-spatial-frequency parts of the non-spectral image data as compared to the high-spatial-frequency parts of the spectral image data.
11. The method according to claim 5, wherein the step of calculating material properties as a function of position from the spectral image data and from the non-spectral image data includes the step of identifying or characterizing at least one of the following: properties identifying a lesion, such as a cyst or a tumor or a microcalcification; properties identifying glandular and adipose breast tissue or skin; concentration of a contrast agent inside the object of interest.
12. A computer program element, which, when executed by a processor, is adapted to carry out the method steps according to claim 5.
13. A computer readable medium, comprising a computer program element according to claim 12.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0035] Exemplary embodiments of the invention will be described in the following with reference to the following drawings.
[0036]
[0037]
[0038]
[0039]
[0040]
DETAILED DESCRIPTION OF EMBODIMENTS
[0041]
[0042] The X-ray imaging system 1 further comprises data and supply connections 30. By means of these connections, raw image data acquired with the X-ray detector arrangement, in particular the imaging unit, can be provided to a calculation unit C, exemplarily comprised in a housing structure 32 in
[0043] The calculation unit C can be connected to a display unit D comprised in display housing structure 34, which is adjusted for visual representation of quantitative image data that have been processed by the calculation unit C. For instance, quantitative image data visualized by the display unit D can be maps of volumetric breast density, also referred to as glandularity maps, or maps of any other combination of materials, calculated from spectral and non-spectral image data, which have been acquired by the X-ray detector arrangement and which have been processed by the calculation unit C.
[0044] It is noted that the present invention is also related to other types of mammography X-ray imaging systems, for instance systems in which the patient is lying on a support structure with the face looking downwards, such as biopsy systems. Further, the X-ray imaging system may also comprise further movable structures to which the X-ray source and the X-ray detector arrangement can be mounted, for example the image may be acquired by scanning a narrow detector across the image field and/or the X-ray tube may be moved along an arc to obtain image data from multiple angles.
[0045] It is further noted that the present invention is not limited to mammography systems. The X-ray system can be any type of 2D or tomosynthesis X-ray imaging system that provides spectral and non-spectral image data.
[0046] The arrangement shown in
[0047]
[0048] In the following, basic steps of an exemplary method for processing quantitative image data are described with respect to
[0049] It should be noted that the spectral and/or the non-spectral image data may contain information on the phase of the X-rays that have passed through the object of interest instead of, or in addition to, information on the absorption of the X rays. Such phase-contrast information might be acquired as the differential of the phase with respect to position in the image. In the latter case it is referred to as differential phase contrast. It should be further noted that the spectral and/or the non-spectral image data may contain information on the small-angle X-ray scattering properties of the object instead of, or in addition to, information on the absorption of the X rays. Such information can be used to form dark-field images.
[0050] Acquisition of the spectral and non-spectral data may be in the reversed order or combined into a single step in which the non-spectral data is derived from the spectral data. In method step 118 the material properties calculated from the spectral and from the non-spectral image data are combined as a function of spatial frequency, where the spatial frequency in this sense represents structure size in the image; it is essentially a measure of how often sinusoidal components of the image repeat per unit of distance.
[0051] In optional method step 120, a visual representation of the material properties calculated from spectral and non-spectral image data is provided.
[0052] The spectral data acquired in step 110 can be acquired with a spectral photon-counting detector. In this case, the spectral detector generates, for example, low-energy (for instance lower half of spectrum) and high-energy (for instance upper half of spectrum) counts, thereby generating two image data sets in each image acquisition. The full-spectrum total (non-spectral) counts are simply the sum of the low- and high-energy counts. The low- and high-energy data sets each have a lower number of counts per pixel and therefore a higher quantum noise compared to the total-count data. The total-count data can then generate an image with maximal signal-to-noise ratio, whereas the low- and high-energy data each generate images with different average energies and a lower signal-to-noise ratio than the total-count image. The low- and high-energy count images can subsequently be combined to generate a spectral image. The spectral images obtained by this procedure will have increased noise compared to the total-count image because 1) the signal-to-noise ratio in each of the low- and high-energy count images is lower, and 2) the spectral processing is often equivalent to taking a difference between the two images, which is an operation that essentially adds the noise of the two images while the image signal is reduced.
[0053] According to an exemplary embodiment, the spectral data in method step 110 are acquired as spectral tomosynthesis data. Spectral tomosynthesis data can be acquired using a photon-counting detector, or, for instance sandwich detectors, kVp switching, filter switching, or multiple exposures.
[0054] The non-spectral data acquired in method step 114 can be data related to a non-spectral image acquired separately or the non-spectral image can be the total-count data acquired as part of the spectral image acquisition.
[0055] The exemplary method according to
[0056] According to one embodiment, the non-spectral data in step 114 can be tomosynthesis data. In tomosynthesis, differentiation between different tissue types can be accomplished in three dimensions (3D) by segmentation of the image pixel values on a slice-by-slice basis. Pixel-by-pixel two-dimensional (2D) tissue maps can be calculated by averaging in the depth direction. However, tomosynthesis provides only limited 3D information because the angular range of the acquisitions is limited and the in-plane resolution is generally much better than the depth resolution. Further, the depth resolution is better for structures with a small in-plane extent and is worse for large structures. Hence, the precision of the 3D segmentation will depend on the in-plane (2D) extension of the structure because of the asymmetric shape of the point-spread function. The segmentation will be good only for small structures, corresponding to high-spatial-frequencies. Large structures, corresponding to low-spatial-frequencies will be blurred in the depth direction and the contribution from these structures will be overestimated as they will occupy a larger number of slices than corresponding to their actual extent in the height direction. The limiting case is a structure that occupies the full in-plane field-of-view for which there will be no height information and which is not possible to segment in any of the slices.
[0057] The non-spectral image data acquired in step 114 can be tomosynthesis data acquired by a partial rotation with a C-arm CBCT (cone beam computed tomography) system. In this case, the spectral image data acquired in step 110 can be acquired, for instance, by multiple scans with alternating filters and/or kVp.
[0058] Material properties calculated from the spectral image data and material properties calculated from the non-spectral image data may include normal breast tissue, such as glandular and adipose breast tissue, and skin. Furthermore, material properties may include a contrast agent, such as iodine. In contrast-enhanced imaging the invention could, for instance, improve the measurement of iodine concentration by reducing noise. The invention could also improve visibility of iodine in the breast, enhancing the prevalence of iodine in blood vessels and smaller structures. In addition, or instead of the aforementioned material properties, material properties can include breast lesions, such as cysts, tumors, or micro calcifications.
[0059] A further exemplary embodiment of a method according to the invention is shown in
[0060] With reference to
[0061] With further reference to method step 118 in
I.sub.enhanced=.sup.1(w.sub.spectral(f)
(I.sub.spectral(x))+w.sub.non-spectral(f)
(I.sub.non-spectral(x)))
I.sub.enhanced denotes the enhanced quantitative image data obtained from combining the spectral and non-spectral image data. Further, I.sub.spectral denotes the spectral image data and I.sub.non-spectral the non-spectral image. The functions w.sub.spectral and w.sub.non-spectral denote spatial-frequency dependent weighting functions and and
.sup.1 are the Fourier and inverse Fourier transforms, respectively. A weighting according to the above equation is mathematically equivalent to the following calculation in the spatial domain:
I.sub.enhanced=v.sub.spectral(x)*I.sub.spectral(x)+v.sub.non-spectral(x)*I.sub.non-spectral(x)
[0062] In the latter case, v.sub.spectral(x)=.sup.1(w.sub.spectral(f)) and v.sub.non-spectral(x)=
.sup.1 (w.sub.non-spectral(f)) are filter kernels and * denotes the convolution operator. It is noted that the two aforementioned calculations are mathematically equivalent. Differences on the end result can be attributed to numerical precision and quality of the software implementation, and the choice of method might depend on practicalities such as speed of running the software. It should also be noted that other methods exist for processing images as a function of spatial frequency and structure size, for instance wavelet methods and Gaussian/Laplacian pyramid methods. The invention is not limited to any particular method of processing.
[0063]
[0064] While the present invention has been illustrated and described in detail in the drawings and foregoing description, such illustration and description are to be considered illustrative or exemplary and not restrictive. The invention is not limited to the disclosed embodiments. Other variations to the disclosed embodiments can be understood and effected by those skilled in the art in practicing a claimed invention, from a study of the drawings, the disclosure and the dependent claims.
[0065] In the claims, the word comprising does not exclude other elements or steps, and the indefinite article a or an does not exclude a plurality. A single processor or other unit may fulfill the functions of several items re-cited in the claims. Any reference sign in the claims should not be construed as limiting the scope.