Manuscript accepted on :July 11, 2017
Published online on: 
An Efficient Filtering Approach for Speckle Reduction in Ultrasound Images
Sumit Kushwaha
Electronics Engineering Department, Kamla Nehru Institute of Technology, Sultanpur, India.
Corresponding Author Email: sumit.kushwaha1@gmail.com
DOI : http://dx.doi.org/10.13005/bpj/1240
Abstract:
Ultrasound (US) imaging is a valuable imaging technique for clinical diagnosis. It is noninvasive in nature and imaging the internal structure of the body to identify the probabilistic diseases or, abnormalities in tissues behavior. However, inherent response of speckle noise in US images limit the fine and edge details which affect the contrast resolution. This makes clinical diagnosis more difficult.In this paper, we proposed a nonlinear anisotropic diffusion filtering for speckle reduction approach based on nonlinear progression partial differential equation (PDE). For analysis purpose, we have considered the set of eightreal clinical BMode US images of human liver from different patient. These real US images are used for quantitative analysis. We compare the performance of four speckle reduction filters as PeronaMalik Filter, LEE Filter, FROST Filter, ADMBSS Filter with our proposed filter in terms of peak signal to noise ratio (PSNR) value performance index under various noise variance selection Parmenter. Finally, we see that our proposed approach preserves the clinical details in US images and minimizing the noise level. Results for set of eight US images shows that our proposed filtering approach is more efficient for speckle noise reduction in comparison to other discussed filters in term of higher PSNR value (dB).
Keywords:
Ultrasound; Diffusion filter; PDE; PSNR; MATLAB;
Download this article as:Copy the following to cite this article: Kushwaha S. An Efficient Filtering Approach for Speckle Reduction in Ultrasound Images. Biomed Pharmacol J 2017;10(3). 
Copy the following to cite this URL: Kushwaha S. An Efficient Filtering Approach for Speckle Reduction in Ultrasound Images. Biomed Pharmacol J 2017;10(3). Available from: http://biomedpharmajournal.org/?p=16002 
Introduction
Medical Ultrasound (US) Imaging technique is a nonionizing radiations imaging modality that enables real time diagnosis treatment. This technique has noninvasive nature. It is widely used in medical field for diagnosis, patient routine checkups for good health, and more and more use in surgeries and intrusions as a supervision modality. This inferior image quality is a challenging issue in US imaging as compared to other imaging modalities. The degree of degradation in US image quality can be highly varying and it depends on patients to patients. Sometimes it is an important challenge to imaging desired structures in particular pose of a fatty patient [1], [2]. US images suffers from numerous acoustic imaging objects including resonance, deviations and effect of speckle noise. In this paper, we focused on minimization of speckle noise effect in US images. Speckle noise effect seems like a granular texture effect on the US image. It is an inherent response of the backscattered interfering signal from the desired interrogated medium [3]. In fact, an accurate description of the speckle noise pattern statistics is still an active research area which involves complex analytical modelling. Speckle noise behavior statistics may be characterized into different modules [4]. Speckle noise effect is spatially correlated with correlation length which is calculated by the autocorrelation of the point spread function (PSF). In various US imaging cases, need for depth of diffusion leads to important speckle correlation lengths.
Earlier speckle reduction LEE filter [5] and FROST filter [6] were believed that speckle noise has additive and multiplication noise component in it. These filters are suitable for speckle reduction by minimizing mean squared error (MSE). These filter statistics are based estimation in local windows. The limitations with these filters are that it smoothed the image near structured and edges region. Perona and Malik filter [7] is firstly adopted the anisotropic diffusion technique for speckle noise reduction in US Images. This filter avoids the unnecessary smoothing related with linear diffusion techniques, but not preserve edges details. A recent speckle reduction method ADMBSS filter [8] proposes a memory based on speckle statistics filtering. This simple technique aims to apply memory mechanism as delay differential equation (DDE) for the diffusion tensor. The behavior of this memory mechanism follows the statistics of the tissues and preserves the clinical details in US images.
Finally, the main challenges with US filtering techniques are preserving the relevant clinical details and avoiding over filtering problem. Keep in mind these limitations and challenges of stateoftheart filters, we proposed an efficient anisotropic diffusion filter for speckle reduction in US images. Our proposed filter gives better result for experiment with eight real US test images of different patients. This is the novelty of our proposed work.
Related Studies
Lee Filter For Speckle
The Lee filter reduces the speckle noise by applying a spatial filter to each pixel in an image, which filters the data based on local statistics calculated within a square window. The value of the center pixel is replaced by a value calculated using the neighboring pixels [4], [5]. This pointwise linear filter is based on the Minimum Mean Square Error (MMSE), and produced speckle noise free image based on the following equation (value of filtered pixel):
where,
and
and
K= weight function,
P_{c}—Center pixel value of kernel/window (Median value)
L_{m}—Local mean of filter window
L_{v}—Local variance of filter window
M—Multiplicative noise mean (Default value: 1)
MV—Multiplicative noise variance (Default value: 0.25)
N Looks—Number of looks (Specifies the number of looks of the image. This is used to calculate the Multiplicative noise variance and control the amount of smoothing applied to the image. Using a smaller value for the Number of Looks leads to more smoothing, and a larger value preserves more image features [9].)
The N Looks for a homogeneous region of an image is the ratio between the mean squared to the variance. The Looks is defined as follows:
The local mean L_{m }of filter window is defined as:
Similarly, the local variance L_{v} of the filter window is defined as:
From eq. (4), if value of L_{v }is negative, in that case we have a very homogeneous area, L_{v }should be set to zero. Then estimate
is given by the local mean L_{m }If value of L_{v }is very high, this indicates a very high contrast region (or, an edge presence) and
=f (x, y, z). These extreme cases are in accordance with the Bayesian approach that is adopted in this linear MMSE filter [5].
Frost Filter For Speckle
The FROST filter is used to design an adaptive filter algorithm to reduce speckle noise in spatial domain and computationally very efficient. This filter preserves the important features of image at the edges. It is a MMSE convolutional filter for speckle reduction. The Frost filter is an exponentially damped circularly symmetric filter that uses local statistics within individual filter windows. The pixel being filtered is replaced with a value calculated based on the distance from the filter center, the damping factor, and the local variance. The Frost filter requires a damping factor (define the extent of smoothing). The Damping Factor value defines the extent of exponential damping. The smaller the value is, the better the smoothing ability and filter performance. After application of the Frost filter, the denoised images show better sharpness at the edges [6], [10], [11].The algorithm used in the implementation of the Frost filter is as follows:
From eq. (1):
where,
K = e^{(B*S)},
where,
and
S—Absolute value of the pixel distance from the center pixel to its neighbors in the filter window,
D—Exponential damping factor (Default value:1)
The factor D is chosen such that when in a homogeneous region, B approaches zero, yielding the mean filter output; at an edge B becomes so large that filtering is inhibited completely [12].
Perona Malik Filter
Perona Malik filter is a classical diffusion filter technique for speckle reduction in US images. This diffusion filter is a linear and space invariant transformation of the original image. The resulting image in this filter obtained by convolution between the images and an isotropic Gaussian filter [13]. Perona and Malik [7] have given a name to their filter called anisotropic diffusion filter. This diffusion filter technique typically looks like the process that creates a scale space not a diffusion tensor, where an image generates a parameterized family of successively more and more blurred images based on a diffusion process.Diffusion is a physical process to create equilibrium concentration differences without destroying or, creating body mass. The Perona Malik filter is based on the equation:
with initial condition u_{o }(x, y, z) = u (x, y,z: t =0) which is noisy image/input image. u (x, y, z: t) is the output image. D (x, y, z: t) is diffusion coefficient, known as symmetric positive definite tensor. D (x, y, z: t) also controls the rate of the diffusion. D (x, y, z: t) depends on local structure of u (x, y,z: t) (if D is constant, then filter is isotropic diffusion filter and if D is not constant, then filter is anisotropic diffusion filter) and ∇. and ∇ denote the divergence operator and gradient operator, respectively, u_{o }(x, y, z) is the initial image, i.e. noisy image, t is temporal variable. Eq. (7), Linear Anisotropic Diffusion (LAD), is an elliptic Partial Differential Equation (PDE) [14].
By using finite difference method, eq. (7) given as:
which is expressed as
where “≈” shows that the R.H.S. part of the equation is the difference approximation of the L.H.S. part.
Similarly, we have
and,
All the values of eq. (8), eq. (9), and eq. (10) inserting in eq. (7) to obtain difference approximation of
Pu Δx = 1, Δy = 1, and Δz = 1we get:
So, obtaining discrete realization of anisotropic diffusion filter for u (x, y,z: t) image from eq. (11):
In eq. (12), we can see that the major problem is selection of diffusion coefficient D (x, y,z: t) in anisotropic diffusion filter.
Diffusion coefficient D (x, y,z: t) is calculated as [15]:
when diffusion occurs across the boundaries and applies it in homogeneous areas. and,
When diffusion occurs near the boundaries and applies it in homogeneous areas.
Where, kappa is the gradient modulus threshold that controls the diffusion coefficient. Also, kappa controls the sensitivity near the edges and chosen experimentally or as a function of the noise in the image (kappa > 0).
Anisotropic Diffusion for Memory Based on Speckle Statistics (ADMBSS) Filter
ADMBSS filter [8] is to eliminate the effect of gradient information due to the lack of contours and low contrast of US images with objective of preservation of relevant clinical details in interest region using probabilisticdriven selective memory mechanism filtering. This filter is adapted to the US medical imaging context [9]. For preserving clinical information in US images, G. RamosLlordénet. al. [8] consider two different methods for tissue classification. 1^{st} selective diffusion tensor method and 2^{nd} probability driven memory methods in region of interest for tissue classification
A selective filtering tensor operator 0 (x, y, z: t) used as transformation of the instantaneous diffusion tensor D (x, y, z: t) at location (x, y, z) into a null tensor for suitable tissue classification and preservation. In this context, p (x, y, z: t) = 1 – p (x, y,z: t) for the probability of the tissue regions and p (x, y, z: t) for the probability of the nontissue (meaningless) regions. For this selective behavior, the diffusion tensor D (x, y, z: t) is multiplied by its Eigenvalues by p (x, y, z: t). Memory mechanism used, to know the anisotropic diffusion direction satisfy the condition that p (x, y, z: t) → 0, so τ (x, y, z) p (x, y, z: t) → ∞ . Memory mechanism will be disable if p (x, y, z: t) → 1, so that τ (x, y, z) p (x, y, z: t) → 0. So the new reconstruct diffusion tensor by using expansion of outer product:
where
and,
Preserving pathway of the time dependent probability for getting more robust characterization than obtained from instantaneous probability, p (x, y, z: t), tensor operator O (x, y, z: t) is not directly applied to L (x, y, z: t). This p (x, y, z: t) provides more robust characterization than p (x, y, z: t).
Now, delay differential equation (DDE), with same initial and periodic condition as [10] and τ (x, y, z) is the spatial dependence of τ, will be:
Where, L (x, y, z: t) is the diffusion tensor matrix at point (x, y, z) and time t. Integrate eq. (52), we get:
To turn ON/OFF the memory mechanism, spatial dependence τ (x, y, z) should satisfied the minimum conditions that τ (x, y, z): [0,1] → (0, ∞). The anisotropic diffusion flux F (x, y, z: t) = L (x, y, z: t) ∇ u (x, y, z: t), then from eq. (18):
Where filtered diffusion tensor
and
Proposed NonLinear Anisotropic Diffusion Filter
Most of the diffusion filters are simply modifications of peronamalik filter [7] where D is constant (scalar coefficient based on gradient of the image D ∇ u (x, y, z: t) which avoids diffusion near the boundaries and applies it in homogeneous areas). Here, we propose an efficient nonlinear anisotropic diffusion for speckle reduction filtering approach based on nonlinear progression of PDE. This proposed filter selects finite power intensity image u_{o} (x, y, z) and having none zerovalued intensities over the image domain Ω. Here,
is a given field of symmetric positive definite diffusion tensors where Ω is an open region of ^{3} and ∂Ω is boundary of Ω. Eigenvectors { v_{1 , }v_{2 , }v_{3 ,}} of these tensors define preferential diffusion directions, and the Eigenvalues their corresponding coefficients. Evolution rule eq. (6) is complemented with an initial condition u (x, y, z; 0) = u_{o} (x, y, z) at time t = 0. If has pixels of vector type, then their components are treated independently [5], [16]. We get the output image u (x, y, z; t) by following PDE:
where ∂Ω denotes the boundary of
is the outer normal to the ∂Ω, and D (x, y, z) is coefficient of diffusion which is defined as a decreasing function of the instantaneous coefficient of variation.
or,
In eq. (23) and (24), q (x, y, z; t) is the instantaneous coefficient of variation serves as the edge detector in speckled imagery, q_{o }(t) is the speckle scale function and is estimation parameter related to the coefficient of variation of noise. q (x, y, z; t) is determined by:
In case of 2D, instantaneous coefficient of variation
Here, four stage iterative method can be used to solve mathematically. Let anisotropic diffusion time step ∇ t and spatial step h in x, y, z directions respectively, then the discretization of time and space coordinates as t = n Δ t; n = 0, 1, 2, 3, … … and x = ih, y = jh, z = kh; i = 0,1,2,3, … … ., M – 1, j =0,1,2,3, … , N – 1, k = 0,1,2,3, … … . , k – 1 respectively, where Mh x Nh x kh is support image size.For mathematical applications, we choose h = 1, and Δ t = 0.05. Let
then iterative method can be described as:
Here, we are using symmetric boundary conditions. So:
Experiment and Discussion
In this experiment, we have considered the set of eightreal clinical BMode US images of human liver from different patient [17], [18]. These real US images are used for quantitative analysis. The size of these real clinical BMode US images of human liver is 256 x 256 x 24 (in pixel unit) in x, y, and z directions respectively. This data set is fed into the MATLAB [19] platform for quantitative analysis. For measuring the all filters performance, we have used Peak Signal to Noise Ratio (PSNR) value (measured in dB) [20]. Higher PSNR value means higher level of image quality reconstruction. We have tested the performance of the filters (LEE Filter [5], FROST Filter [6], Perona Malik Filter [7], ADMBSS Filter [8], and Proposed Filter) for all US images under different noise variance as 0.01, 0.04, 0.07, 0.1, and 0.5. All quantitative analysis results are represented in table form from Table I to VIII, and also shown in graphical form in figure 2. The output image of all filters under different noise variances are shown sequentially from figure 3 to figure 7. Now, we have seen that our proposed filter gives higher PSNR value under different noise variances in comparison to other discussed filters. This shows that our proposed filter is work efficiently for speckle noise reduction in US images under different noise variances.
Figure 1: Experiment results obtain from these eight Bmode US images of human liver.

Figure 2: The graphs are plotted for PSNR result values for different filters. These graphs show that our proposed filter is more efficient for removing Speckle noise.

Figure 3: Noise Level Variance 0.01

Figure 4: Noise Level Variance 0.04

Figure 5: Noise Level Variance 0.07

Figure 6: Noise Level Variance 0.1

Figure 7: Noise Level Variance 0.5

Table 1: Performance Comparison of Different Filters for Image 1
PSNR(dB) RESULTS FOR THE IMAGE 1 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  33.5863  30.7646  27.9208  33.0753  59.9532 
0.04  26.8198  25.5545  24.1795  33.8953  52.0865 
0.07  24.2403  23.0597  22.0432  43.5523  43.3213 
0.1  22.8419  21.5929  20.7415  37.116  39.3994 
0.5  18.6482  15.4397  15.0582  34.3762  28.4605 
Table 2: Performance Comparison of Different Filters for Image 2
PSNR(dB) RESULTS FOR THE IMAGE 2 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  31.8765  29.6114  27.4193  38.7373  60.1176 
0.04  25.3038  24.1023  23.0549  37.0798  46.9497 
0.07  23.1179  21.8245  21.0142  54.1903  39.5293 
0.1  21.8242  20.3137  19.6463  47.3763  36.3813 
0.5  18.2999  14.5549  14.2363  42.1617  27.4346 
Table 3: Performance Comparison of Different Filters for Image 3
PSNR(dB) RESULTS FOR THE IMAGE 3 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  33.6423  30.7505  27.9583  31.5686  60.4925 
0.04  26.838  25.6038  24.1918  31.7607  51.1155 
0.07  24.3578  23.1577  22.1389  44.7001  43.5445 
0.1  22.8507  21.5427  20.7171  29.142  38.5877 
0.5  18.6508  15.4617  15.0717  39.746  28.6693 
Table 4: Performance Comparison of Different Filters for Image 4
PSNR(dB) RESULTS FOR THE IMAGE 4 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  31.8291  29.5409  27.3701  37.9569  61.7416 
0.04  25.2852  24.0751  23.0358  34.5986  45.9795 
0.07  23.1725  21.8448  21.0474  50.9217  39.4964 
0.1  21.8462  20.3749  19.6957  41.2622  36.0276 
0.5  18.2611  14.545  14.2376  43.3388  27.3917 
Table 5: Performance Comparison of Different Filters for Image 5
PSNR(dB) RESULTS FOR THE IMAGE 5 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  32.7224  29.9306  27.1693  45.0071  59.175 
0.04  27.2024  25.7441  24.1846  41.735  52.7133 
0.07  24.9565  23.6137  22.4323  38.3478  44.5785 
0.1  23.5763  22.1666  21.1989  40.7795  40.0525 
0.5  19.3568  16.1321  15.705  42.24  29.3316 
Table 6: Performance Comparison of Different Filters for Image 6
PSNR(dB) RESULTS FOR THE IMAGE 6 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  34.1398  31.1547  28.1883  32.4728  60.5218 
0.04  25.2852  26.0935  24.6419  28.4759  53.269 
0.07  24.9829  23.8935  22.6956  33.6521  44.4787 
0.1  23.474  22.2108  21.3055  32.4591  40.083 
0.5  18.9455  15.9552  15.5656  43.2921  29.074 
Table 7: Performance Comparison of Different Filters for Image 7
PSNR(dB) RESULTS FOR THE IMAGE 7 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  33.7113  30.9191  28.3638  36.439  60.8786 
0.04  27.2024  25.6571  24.4113  44.4852  49.149 
0.07  24.6137  23.355  22.4096  34.3248  41.7057 
0.1  23.2736  21.9426  21.1419  29.9298  38.9144 
0.5  19.0164  15.8372  15.4541  18.3136  29.0295 
Table 8: Performance Comparison of Different Filters for Image 8
PSNR(dB) RESULTS FOR THE IMAGE 8 EXPERIMENT  
Noise Level  Perona Malik Filter  LEE Filter  FROST Filter  ADMBSS Filter  Proposed Filter 
0.01  31.4013  28.6532  26.1152  38.0811  62.3628 
0.04  25.9988  24.4407  23.009  39.4908  49.7713 
0.07  24.7752  22.3701  21.2703  40.2364  41.8029 
0.1  22.447  20.9436  20.0514  26.1845  38.1168 
0.5  18.6631  15.1269  14.7353  20.7533  28.1388 
Conclusion
Speckle noise is inherent response in US images. Since it degraded the image quality and affecting fine and edge details. So, it is difficult task to see the clinical details in patient diagnosis. In this paper, we proposed a nonlinear anisotropic diffusion filtering based speckle reduction approach based on nonlinear progression PDE. This approach minimizes the speckle noise, preserves the clinical diagnosis details of patient. The experimental analysis tested on set of eightreal clinical BMode US images of human liver from different patientunder various noise variance selection Parmenter. We compare the performance of PeronaMalik Filter, LEE Filter, FROST Filter, ADMBSS Filter with our proposed nonlinear anisotropic diffusion based speckle reduction filter. We see that our proposed approach preserves the clinical details in US images and minimizing the noise level in term of higher PSNR value (dB). This is very helpful approach for radiologists/Doctors to accurate clinical diagnosis. Future works will include speckle reduction for more real time US images as well as in real time US imaging video.
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