This invention relates to a novel technique, which is able to enhance an indistinct or noisy digital image, that has been acquired from medical imaging scanners as Computed Tomography (CT) and Magnetic Resonance Imaging (MRI).
It may be remarked that earlier investigators have proposed procedures for upgradation of medical image to some extent, such techniques encompassing histogram equalization, adaptive filtering, or filtering approaches using multiple subimage schemata. However, the procedures are generally not adaptable to variable tissue intensities, and hence cannot give optimal enhancement. Moreover, none of the existing image enhancement technique is able to enhance different kinds of image modalities. Recently wavelet-based approach has been used to explore the possibility of selective image improvement, but here there are many more variables involved. In the latter case, the problem is that one has to tune, in advance, to some arbitrary scale-specific or scale-dependent parameters of the wavelets, which may be suboptimal.
The drawbacks and limitations on the existing techniques are that there is usually loss of information as basically a filtering operation is used on the image to filter out energy power residing in the stochastic noise component of the image. These filters lose some content of the image or may cause artifacts, both of which may hamper the diagnosis.
Furthermore, the majority of the above procedures are not tissue-selective nor tissue-adaptive, since, in general, the various structures in the image are enhanced evenly and monotonously together, as mentioned earlier. The existing techniques do not produce variegated contrast level among different regions, however such variegation is much desirable for proper perception of images.
There is actually a topical need of a proper medical image enhancement technique that can operate adaptively on the variegated texture of heterogeneous tissue image. With this desirability in mind, it may be mentioned that the principal of Stochastic Resonance (SR) has been studied by scientists for various applications to physical or biological systems, such as enhancement of sound detection or optical scattering. However, there in no literature available on SR application for medical image enhancement. Of course, the proposed methodology is the first application of SR for diagnostic medical imaging system.
The proposed SR technique has proven effective and overcomes certain limitations in the existing techniques as information loss and unwanted artifacts due to filtering. The SR procedure administers extra quality to the contrast of an image through the added stochastic fluctuations, and there is minimal power dissipation or information loss in the image.
The proposed technique is also lesion specific as the image processing operation, namely the stochastic integral transform (SIT), can be adapted locally to enhance the suspicious regions of tissue. The nature of the pixel-adaptive SIT mapping is such that it provides varying contrast in different regions, so that the entire image is neither enhanced equally nor monotonously. Further, the methodology can enhance different kinds of image modalities and has been tested on various lesions and tumours, under different imaging modalities as CT, MRI, etc. The proposed procedure imparts an excellent opportunity to clinicians and radiologists to enhance and diagnose the unclear or latent lesions in an image.
Although some procedures for image upgradation have been proposed, none of the existing techniques promises enhancement without information loss. The proposed method enhances the edges of the lesion, delineates the edema segments more clearly, and demarcates the latent structural brain lesions, along with aiding more efficient discrimination of the different zones of the lesion. Furthermore, the proposed method is also useful in broad-ranging image processing applications of a general nature.
This invention relates to a novel Stochastic Resonance technique of medical image enhancement device based on Integral Transform of the image, comprising of the following step-wise elements. Image Transform component for generating specific types of Integral transforms like Radon transform for PCT, Fourier transform for MRI. Perturbator component for preparing the stochastic perturbation waveform. Stochastic Resonator component for performing the stochastic resonance on the image transform. Performance monitoring component for characterizing the image enhancement factor of the SR-processed image. Control component for adjusting and controlling the bistability parameters of the double-well system that induces tochastic resonance. Matrix Display component for arranging the provisional display of the array matrix of the SR-enhanced images, as the bistability parameters are varied. Final Image display component for display of the maximally enhanced final output image.
The initial image P is obtained in the CT or MRI scanner [Schema (A)]; then the initial image P is subject to Image Transform Operation with Stochastic Resonance Induction [Schema (B)] so as to obtain the Final Enhanced image Q.
The invented technique is able to enhance a digital image acquired from scanners, as CT and MRI. The novelty is to add optimized noise to an already noisy or indistinct image, so as to enhance the contrast in the image. The addition of small amount of noise to a noisy image induces enhancement of the digital signal and this phenomenon is known as Stochastic Resonance (SR). The inventors administer the SR to the 2D-Radon domain for CT images and Fourier domain for MRI images, and the Inventors perform the image upgradation process by inventing a quantitative formulation that the inventors refer to as ‘Stochastic Integral Transform’ (SIT) (
This invention reports for the first time the proof-of-principle that the nonlinear dynamics-based principle of stochastic resonance is a useful procedure for image enhancement in CT, MR etc. Ever since the initiation of digital imaging technology about sixty years ago, image processing methodologies have been dominated by communication-based techniques, such as by using various filter which filters the image and reduces the total power in the image. On the other hand, the Inventors have developed a new image enhancement approach using the newer physics-based yet biologically-oriented development in nonlinear dynamics methodology discovered in their laboratory. The procedure improve the quality of an image by administering to the image a zero-mean white Gaussian noise thermodynamically by means of stochastic fluctuation. The invention uses our novel proposition of Stochastic Integral Transform (SIT), which has not been suggested by anyone earlier, and this transformation can be used strategically for improving the accession of imaging signals of the pathophysiolocial system, thereby aiding in improved diagnosis and treatment.
The feasibility and proof-of-principle has been shown as follows. The quantitative procedure with computational algorithms for image enhancement of CT and MR images has been developed and the procedure has been validated using tested images. Testing has been done for several kinds of lesions as parasitic, infective and malignant, like cysticercosis, glioma, meningioma, tuberculoma, astrocytoma, etc. The Inventors estimated the quality of the upgraded image using the Image Upgradation Index parameter whose concept and measurement that they have developed. The mean upgradation index of over all the tested CT images is about 165% and that of MR images 125%. Intended for use by a wide community of users in medical imaging, physicians, radiologists, biomedical engineers, neuroscientists and others, our image processing procedures has been coded using Matlab language, and the same can be extended to stand-alone executable platform independent of Matlab, for the end users. The package is convertible to a directly user-friendly procedure, for use by concerned scientists, clinicians and engineers in the field of imaging, diagnostics, therapeutics and image processing.
Stochastic resonance is a novel concept, whereby the addition of optimal stochastic fluctuation or noise-based perturbation, to a signal-operated system, enhances the signal and the system response. One of the well-known examples of a physical or computational system that undergoes stochastic resonance is that a particle in a double-well potential. Motivated by statistical physics, the inventors consider an over-damped motion of a Brownian particle system in the presence of noise and an external periodic force, with the system having a bistable potential P(x), where P(x) is given by:
P(x)=(m/2)·x2+(n/4)·x4
here m and n are the bistability parameters which jointly determine the double well's height and width, that is, the activation threshold and separation between the minima, respectively. Here, we model the image pixel under stochastic fluctuation, by means of a particle under thermodynamic fluctuation noise (Brownian motion). This fluctuation noise enables the particle (or pixel) to transit from one state to the other, i.e. from weak-signal state to strong-signal state. We assume here that the noise is zero-mean Gaussian white noise. The stochastic resonator (SR) of the noise-induced transition of the signal can be taken as:
x′(t)=dx/td=−P′(x)+A+N [1]
where A is the amplitude of the signal, N is a zero-mean input (the stochastic noise with variance s2), and P′(x) is the differential of P(x) with respect to x and is given by [mx+nx3]. Note that x′(t) implies differentiation of x(t) with respect to its variable t, while P′(x) indicates differentiation of P(x) with respect to the latter's variable x. The simulation is discretized in temporal steps of τ using Maruyama-Euler stochastic equation, given by:
x
v
=x
u+δτ(mxu−nx3u+A+N)
where xu is the value of x at nth time-step, xv is the value of x at (n+1)th time-step, while δτ is the time interval between the temporal steps. The x′(t) parameter of eq. [1] forms the stochastic resonator (SR) of the system. Note that the initial condition is x0=x (0), i.e the value of x at time t=0. After the above, we now apply the stochastic resonator to the image to be enhanced. First, the gray level of given 2-D image I(x, y) is transformed to a zero-mean input, namely to a derived image I*(x, y) where:
I*(x,y)=I(x,y)−I0(x,y)
Where I0(x, y) is the spatial average value of the original 2-D image I(x, y) which is the MRI or CT image that we wish to enhance. Now, we administer the stochastic resonator (SR) to the respective integral transform domain, namely the 2-D Fourier transform domain of the derived image I*(x, y) in case of the MRI scan, or the 2-D Radon transform domain of the derived image I*(x, y) in case of the CT scan, where the Fourier Transform TF and Radon Transforms TR are respectively defined by:
Where kx and ky are the Fourier wave vectors in k-space, and ρ and θ are the polar coordinates, while δD is the Dirac Delta Function selecting the plane of projection (i.e., δD=1 if x=0, whereas δD=0 if x≠0). The Radon or Fourier transform can be generalized as an Integral Transform. Hence the administration of the Stochastic Resonator to the Integral Transform, can be taken to be a noise-activated transform TN, that we name as the Stochastic Integral Transform (SIT), which is given in terms of a double integral over the 2-D plane of the image:
Where SR is the stochastic resonance operator [see eq. (1)], and I*(x, y) is the derived image, while TG is the Generalized Integral Transform, such as 2D Fourier transform TF [given in eq. (2)] or the 2D Radon transform TR [given in eq. (3)]. The stochastic integral transform of the image TN of eq. (4) is then subject to discrete Fourier transform and then backprojection algorithm is applied to obtain the enhanced image.
The step-wise elements of the proposed image enhancement system are (
The inventors present some results obtained using the proposed approach. The values of the parameters ‘m’ and ‘n’ were varied to furnish a matrix of different stochastically activated images. The maximally enhanced image was chosen from the matrix using the characteristic of the perceptual contrast discriminability in the image, namely the just-noticeable-difference in intensity (JND). The proposed algorithm produces adequate contrast in the output image, and results in almost no ringing artifacts even around sharp transition regions, which are a disadvantage in typical conventional contrast enhancement techniques. Some of our experimental results on CT and MRI modalities are shown below.
The proposed method was able to enhance the edges of lesion in CT images.
The enhanced image is also able to better outline the sulcal-gyri architecture in the cortex, and well delineates the two zone sof the oedema region of the white matter, namely the umbral and penumbral zones of edema shown in
a) shows a T1-weighted MR image of a lesion in which the ROI is marked in the figure and one cannot distinguish the gray from white matter, while the lesion margin cannot be discerned. In the SR enhanced image in
Number | Date | Country | Kind |
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1216/DEL/08 | May 2008 | IN | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IN09/00096 | 2/10/2009 | WO | 00 | 2/1/2011 |