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International
OPEN ACCESS Journal
Of Modern Engineering Research (IJMER)
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 56|
Performance of MMSE Denoise Signal Using LS-MMSE
Technique
U. Rama Krishna1
, A.Vanaja2
1
Department of ECE, Student, S.R.K institute of Technology, Vijayawada, India
2
Asst .professor, Department of ECE S.R.K institute of Technology, Vijayawada, India
I. Introduction
Wavelet regularization [1] has been shown to be particularly effective in reducing noise, while
preserving important signal features. The performance of the method can be further improved at little
computational cost, by using the technique known as cycle spinning [2]-[4]. Cycle spinning compensates for the
lack of shift-invariance of the wavelet basis by considering different shifts of the signal. Total variation (TV) [5]
regularization is another widely used Denoising method, which penalizes random oscillations in the signal,
while allowing the discontinuities. Interestingly, for 1-D signals, Haar-wavelet shrinkage with cycle spinning
has been shown to closely related to TV regularization [6]. In this paper, we exploit the link between the two
estimation methods to derive a new wavelet- based method for efficiently solving TV type denoising problems
in 1or2-D. The key observation is that TV-regularized least squares minimization can be reformulated as a
constrained optimization problem in the wavelet domain. We use the augmented-Lagrangian method [7] to cast
the problem as a sequence of unconstrained problems that can be solved by simple soft- thresholding. By
replacing the soft-thresholding function by another scalar function or by a precompiled lookup table, we can
efficiently extend our algorithm beyond traditional l1 regularizes to general, possibly non-convex, potential
functions. The rest of this paper is organized as follows. In section 2, we describe the CCS-MMSE. Section3
explain the LS-MMSE. Section4 GIVES some experimental results. Finally, a conclusion will be presented in
section V.
II. CCS-MMSE
The CCS-MMSE technique follows two steps. They are wavelet denoise (Haar wavelet) and consistent
cycle spinning explained in section-2a and 2-b. The algorithm of CCS-MMSE is given by
1. Initialize parameters
2. For snr = 1:20
3. For iteration 1:2000
4. X=Generate random signal
5. X1=convert serial to parallel
6. B=2*X-1%convert binary signal
7. Pilot=[bit(1:m) pilot symbol bit (m+1:end)]%insert pilot signal
8. Wavelet = dwt2(pilot, „haar wavelet‟)%add wave let
9. G=insert interval
10. W=HG+n %output signal
11. 𝝓 𝑴𝑴𝑺𝑬 𝒘 −
𝟏
𝟐
𝜼 𝑴𝑴𝑺𝑬
−𝟏
𝒘 − 𝒘
𝟐
− 𝐥𝐨𝐠 𝒑 𝒖
𝜼 𝑴𝑴𝑺𝑬
−𝟏
𝒘 %|(CCS-MMSE)
12. Error=error+(|X-∅mmse)
13. End iteration
14. End snr
Abstract: This paper presents performance of mmse denoises signal using consistent cycle spinning
(ccs) and least square (LS) techniques. In the past decade, TV denoise technique is used to reduced the
noisy signal. The main drawback is the low quality signal and high MMSE signal. Presently, we
proposed the CCS-MMSE and LS-MMSE technique .The CCS-MMSE technique consists of two steps.
They are wavelet based denoise and consistent cycle spinning. The wavelet denoise is powerful
decorrelating effect on many signal domains. The consistent cycle spinning is used to estimation the
MMSE in the signal domain. The LS-MMSE is better estimation of MMSE signal domain compare to
CCS-MMSE.The experimental result shows the average MMSE reduction using various techniques.
Key words: CCS-MMSE, LS-MMSE, MMSE estimation, Total Variation Denoising, Wavelet Denoising.
Performance of MMSE Denoise Signal Using LS-MMSE Technique
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 57|
2.1 Haar Wavelet Denoise
The wavelet denoise is power is powerful decorrelating effect on many signal domains. The problem of
estimation of wavelet denoise is given by
𝐖 = 𝐟(𝐖 ) (𝐮) = 𝐚𝐫𝐠𝐦𝐢𝐧{
𝟏
𝟐
𝐰 − 𝐮 𝟐
𝟐
+ ∅ (𝐰) } --------------- (1)
∅W is non-smooth convex function using wavelet soft threshold and is given by
∅ 𝒘 𝒘 − 𝝀 𝟐 𝒘 𝒅
------------ (2)
μ is the vector of lag range multipliers.
The soft thresholding function η is applied to component-wise on the detail wavelet coefficients. The
detail coefficients derived from haar-wavelet transform.
Improving the signal quality using haar wavelet denoise is used. It is removing noisy signal domain. These are
the advantages of wavelet denoise technique. A major drawback of haar wavelet denoise is to estimate the
MMSE estimation is not in general equivalent to MMSE estimation in the signal domain. It is happen only on
wavelet transform is orthogonal.
2.2 Consistent Cycle Spinning
The CCS method is used to estimate the MMSE in the different signal domain. In cycle spinning
technique is used to expanding the signal in a wavelet frame. It has fast convergence. It is fast and minimizing
the signal noise, the cost function decreases monotonically until the algorithm reaches a fixed point. Cycle
spinning implies a reduant representation. Thus, not every set of wavelet-domain coefficients can be perfectly
inverted back to the signal domain. When the estimated coefficients violate the invertibility condition a problem
will arise. It can be resolved through consistency. The algorithm of cycle spinning as shown below
Input: y, s0ЄRN, τ, ЄR0
Set: k=0, λ0=0, u=Ay;
Repeat
𝒁 𝒌+𝟏
= 𝒑𝒓𝒐𝑿∅
𝟏
𝟏 + 𝝁
𝒖 + 𝝁𝑨𝒔 𝒌
+ 𝝀 𝒌
;
𝝉
𝟏 + 𝝁
𝑺 𝒌+𝟏
= 𝑨†
𝒁 𝒌−𝟏
−
𝟏
𝝁
𝝀 𝒌
𝝀 𝒌+𝟏
= 𝝀 𝒌
− 𝝁 𝒛 𝒌+𝟏
− 𝑨𝒔 𝒌−𝟏
k=k+1
Until stopping criterion
Return S=Sk
The characterize of iterative MMSE shrinkage in CCS-MMSE IS given by
𝝓 𝑴𝑴𝑺𝑬 𝒘 = −
𝟏
𝟐
𝜼 𝑴𝑴𝑺𝑬
−𝟏
𝒘 − 𝒘
𝟐
− 𝐥𝐨𝐠 𝒑 𝒖
𝜼 𝑴𝑴𝑺𝑬
−𝟏
𝒘 ------- (3)
It is minimizing the cost function and better performance technique compare to TV denoise technique.
The objective function with the new penalty function is given by
𝓛 𝑾, 𝑿 = 𝓙 𝒖, 𝒘 +
𝝉
𝟐
𝒘 − 𝑾 𝑿 𝟐
𝟐
− 𝝁 𝚻
𝒘 − 𝑾 𝑿 ----------- (4)
Where r>0 is the penalty parameter and 𝜇 is the vector of lag range multipliers.
2.3 Discrete Fourier Transform
The DFT is used to compute the Fourier transform of discrete data. The Wavelet performance is better
than DFT because wavelet can localized in both frequency and time. The DFT maps a discrete signal into the
frequency domain. In the DFT we use sine and cosine waves, it commonly called as DFT basis functions.
The DFT basis generating functions are
Ck[i] =cos (2πki/N),
Sk[i] = sin (2πki/N)
Where
ck[i] is the cosine wave for the amplitude held in real part
sk[i] is the cosine wave for the amplitude held in imaginary part.
The DFT can be calculated in three different waves. Such as
1) Set of simultaneous equations
2) Correlation
3) FFT [Fast Fourier Transform]
Performance of MMSE Denoise Signal Using LS-MMSE Technique
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 58|
In this paper we are using the Fast Fourier Transform. Fast Fourier Transform is ingenious algorithm it
decomposes a DFT with N points. The Fast Fourier Transform is 100 times faster than the Set of simultaneous
equations, Correlation. Here we notice that, DFT has less than 32 points than we used correlation method
otherwise we go for the Fast Fourier Transform.
III. LS-MMSE
The method of least squares-mmse is estimating the mmse by minimizing the squared discrepancies
between observed data and their expected signal values. We will study the method in the context of regression
problem, where the variation in one variable, called the response variable Y, multiple linear regression co-
variables x. The prediction of Y is given by
Y=f(X) +noise……. (5)
Where
f= egression function. It is used to estimate the co-variables and their responses.
The block diagram of LS-MMSE is given by
Fig.3.1 block diagram of LS-MMSE technique
The least squares criterion is a computationally better compare to CCS-MMSE. It corresponds to
maximum likelihood estimation when the noise is normally distributed with equal variances. Other measures of
fit are sometimes used, for example, least absolute derivations, which is more robust against outliers.
The least squares estimator, denoted by β, is that value of b that minimizes
𝒚𝒊 − 𝒇 𝒃 𝒙𝒊
𝟐𝒏
𝒊=𝟏 ----------- (6)
The covariance matrix of estimator β is equal to
𝑋′
𝑋 𝜎2
Where σ2 is the variance of the noise. As an estimator of σ2
, we consider
𝛔 𝟐
=
𝟏
𝐧−𝐩
𝐲 − 𝐗𝛃
𝟐
=
𝟏
𝐧−𝐩
𝐞 𝐢
𝟐𝐧
𝐢=𝟏 ----------- (7)
The algorithm of LS-MMSE is given by
1. Initialize parameters
2. For snr = 1:20
3. For iteration 1:2000
4. X=Generate random signal
5. X1=convert serial to parallel
6. B=2*X-1%convert binary signal
7. Pilot=[bit(1:m) pilot symbol bit(m+1:end)]%insert pilot signal
8. Wavelet = dwt2(pilot, „haar wavelet‟)%add wave let
9. G=insert interval
10. W=HG+n %output signal
11. 𝛔 𝟐
=
𝟏
𝐧−𝐩
𝐲 − 𝐗𝛃
𝟐
=
𝟏
𝐧−𝐩
𝐞 𝐢
𝟐𝐧
𝐢=𝟏
12. Error=error+(|X-∅mmse)
13. End iteration
14. End snr
Performance of MMSE Denoise Signal Using LS-MMSE Technique
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 59|
Improving the signal quality, removing noisy signal domain and minimum MMSE denoise signal are
the advantages of LS-MMSE technique.
IV. Experiment Results
We have used MATLAB to perform simulations of the CCS-MMSE and LS-MMSE are discussed in
section II, III. As can be seen in Fig 2,3 and 4, both CCS-MMSE and LS-MMSE result in the best MSE
reduction for all signals and noise levels. The performance of LMMSE and TV methods heavily depends on the
type of signal.
Fig4.1 the average MSE reduction is plotted against AWGN variance with Gaussian noise
Fig4.2.the average MSE reduction is plotted against AWGN variance with Laplace noise
Fig4.3.the average MSE reduction is plotted against AWGN variance with Cauchy noise
Performance of MMSE Denoise Signal Using LS-MMSE Technique
| IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 60|
V. Conclusion& Future Scope
We present the performance of average MSE reduction using various Bayesian methods. The LS-MSE
technique is better performance to existing methods in terms of mmse reduction. Although, the results presented
here focus on 1D signal, the extensions to 2D OR 3D data can be achived by using higher-dimensional Haar-
transforms in CCS-MMSE technique.
REFERENCES
[1] Abbas Kazerouni, Ulugbek S.Kamilov, “Bayesian Denoising: from MAP to MMSE Using Consistent Cycle
Spinning”, IEEE Tran .Signal Processing, vol20, no.3, pp. 249-252, March 2013.
[2] D.L. Donoho and I.M. John stone, “Ideal spatial adaption by wavelet shrinkage”, Biometrika, vol. 8.1, no.3, pp.425-
455, 1994
[3] R.R.Coifmanand D.L.Donoho, “Springer Lecture Notes in Statistics”. New York: Springer-Verlag, 1995, pp. 125–
150, ch. Translation-invariant de-noising.
[4] M.A.T. Figueiredo and R. D. Nowak, “An EM algorithm for wavelet-based image restoration,” IEEE Trans. Image
Process., vol. 12, no. 8, pp. 906–916, 2003.
[5] M. Guerquin-Kern, M. Häberlin, K. P. Prüssmann, and M. Unser, “A fast wavelet-based reconstruction method for
magnetic resonance imaging,” IEEE Trans. Med. Image., vol. 30, no. 9, pp. 1649–1660, 2011.
[7] L.I.Rudin,S.Osher,andE.Fatemi, “Nonlinear total variation based noise removal algorithms,” Physica D, vol. 60, pp.
259–268, 1992.
[8] G. Steidl, J.Weickert, T. Brox, P.Mrazek, and M.Welk, “On the equivalence of soft wavelet shrinkage, total variation
diffusion, total variation regularization, and SIDEs,” SIAM J. Numer. Anal., vol.42, no.2, pp. 686–713, 2004.
[9] J.Nocedal and S.J.Wright, “Numerical Optimization”, 2nd ed. New York: Springer, 2006.

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Performance of MMSE Denoise Signal Using LS-MMSE Technique

  • 1. International OPEN ACCESS Journal Of Modern Engineering Research (IJMER) | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 56| Performance of MMSE Denoise Signal Using LS-MMSE Technique U. Rama Krishna1 , A.Vanaja2 1 Department of ECE, Student, S.R.K institute of Technology, Vijayawada, India 2 Asst .professor, Department of ECE S.R.K institute of Technology, Vijayawada, India I. Introduction Wavelet regularization [1] has been shown to be particularly effective in reducing noise, while preserving important signal features. The performance of the method can be further improved at little computational cost, by using the technique known as cycle spinning [2]-[4]. Cycle spinning compensates for the lack of shift-invariance of the wavelet basis by considering different shifts of the signal. Total variation (TV) [5] regularization is another widely used Denoising method, which penalizes random oscillations in the signal, while allowing the discontinuities. Interestingly, for 1-D signals, Haar-wavelet shrinkage with cycle spinning has been shown to closely related to TV regularization [6]. In this paper, we exploit the link between the two estimation methods to derive a new wavelet- based method for efficiently solving TV type denoising problems in 1or2-D. The key observation is that TV-regularized least squares minimization can be reformulated as a constrained optimization problem in the wavelet domain. We use the augmented-Lagrangian method [7] to cast the problem as a sequence of unconstrained problems that can be solved by simple soft- thresholding. By replacing the soft-thresholding function by another scalar function or by a precompiled lookup table, we can efficiently extend our algorithm beyond traditional l1 regularizes to general, possibly non-convex, potential functions. The rest of this paper is organized as follows. In section 2, we describe the CCS-MMSE. Section3 explain the LS-MMSE. Section4 GIVES some experimental results. Finally, a conclusion will be presented in section V. II. CCS-MMSE The CCS-MMSE technique follows two steps. They are wavelet denoise (Haar wavelet) and consistent cycle spinning explained in section-2a and 2-b. The algorithm of CCS-MMSE is given by 1. Initialize parameters 2. For snr = 1:20 3. For iteration 1:2000 4. X=Generate random signal 5. X1=convert serial to parallel 6. B=2*X-1%convert binary signal 7. Pilot=[bit(1:m) pilot symbol bit (m+1:end)]%insert pilot signal 8. Wavelet = dwt2(pilot, „haar wavelet‟)%add wave let 9. G=insert interval 10. W=HG+n %output signal 11. 𝝓 𝑴𝑴𝑺𝑬 𝒘 − 𝟏 𝟐 𝜼 𝑴𝑴𝑺𝑬 −𝟏 𝒘 − 𝒘 𝟐 − 𝐥𝐨𝐠 𝒑 𝒖 𝜼 𝑴𝑴𝑺𝑬 −𝟏 𝒘 %|(CCS-MMSE) 12. Error=error+(|X-∅mmse) 13. End iteration 14. End snr Abstract: This paper presents performance of mmse denoises signal using consistent cycle spinning (ccs) and least square (LS) techniques. In the past decade, TV denoise technique is used to reduced the noisy signal. The main drawback is the low quality signal and high MMSE signal. Presently, we proposed the CCS-MMSE and LS-MMSE technique .The CCS-MMSE technique consists of two steps. They are wavelet based denoise and consistent cycle spinning. The wavelet denoise is powerful decorrelating effect on many signal domains. The consistent cycle spinning is used to estimation the MMSE in the signal domain. The LS-MMSE is better estimation of MMSE signal domain compare to CCS-MMSE.The experimental result shows the average MMSE reduction using various techniques. Key words: CCS-MMSE, LS-MMSE, MMSE estimation, Total Variation Denoising, Wavelet Denoising.
  • 2. Performance of MMSE Denoise Signal Using LS-MMSE Technique | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 57| 2.1 Haar Wavelet Denoise The wavelet denoise is power is powerful decorrelating effect on many signal domains. The problem of estimation of wavelet denoise is given by 𝐖 = 𝐟(𝐖 ) (𝐮) = 𝐚𝐫𝐠𝐦𝐢𝐧{ 𝟏 𝟐 𝐰 − 𝐮 𝟐 𝟐 + ∅ (𝐰) } --------------- (1) ∅W is non-smooth convex function using wavelet soft threshold and is given by ∅ 𝒘 𝒘 − 𝝀 𝟐 𝒘 𝒅 ------------ (2) μ is the vector of lag range multipliers. The soft thresholding function η is applied to component-wise on the detail wavelet coefficients. The detail coefficients derived from haar-wavelet transform. Improving the signal quality using haar wavelet denoise is used. It is removing noisy signal domain. These are the advantages of wavelet denoise technique. A major drawback of haar wavelet denoise is to estimate the MMSE estimation is not in general equivalent to MMSE estimation in the signal domain. It is happen only on wavelet transform is orthogonal. 2.2 Consistent Cycle Spinning The CCS method is used to estimate the MMSE in the different signal domain. In cycle spinning technique is used to expanding the signal in a wavelet frame. It has fast convergence. It is fast and minimizing the signal noise, the cost function decreases monotonically until the algorithm reaches a fixed point. Cycle spinning implies a reduant representation. Thus, not every set of wavelet-domain coefficients can be perfectly inverted back to the signal domain. When the estimated coefficients violate the invertibility condition a problem will arise. It can be resolved through consistency. The algorithm of cycle spinning as shown below Input: y, s0ЄRN, τ, ЄR0 Set: k=0, λ0=0, u=Ay; Repeat 𝒁 𝒌+𝟏 = 𝒑𝒓𝒐𝑿∅ 𝟏 𝟏 + 𝝁 𝒖 + 𝝁𝑨𝒔 𝒌 + 𝝀 𝒌 ; 𝝉 𝟏 + 𝝁 𝑺 𝒌+𝟏 = 𝑨† 𝒁 𝒌−𝟏 − 𝟏 𝝁 𝝀 𝒌 𝝀 𝒌+𝟏 = 𝝀 𝒌 − 𝝁 𝒛 𝒌+𝟏 − 𝑨𝒔 𝒌−𝟏 k=k+1 Until stopping criterion Return S=Sk The characterize of iterative MMSE shrinkage in CCS-MMSE IS given by 𝝓 𝑴𝑴𝑺𝑬 𝒘 = − 𝟏 𝟐 𝜼 𝑴𝑴𝑺𝑬 −𝟏 𝒘 − 𝒘 𝟐 − 𝐥𝐨𝐠 𝒑 𝒖 𝜼 𝑴𝑴𝑺𝑬 −𝟏 𝒘 ------- (3) It is minimizing the cost function and better performance technique compare to TV denoise technique. The objective function with the new penalty function is given by 𝓛 𝑾, 𝑿 = 𝓙 𝒖, 𝒘 + 𝝉 𝟐 𝒘 − 𝑾 𝑿 𝟐 𝟐 − 𝝁 𝚻 𝒘 − 𝑾 𝑿 ----------- (4) Where r>0 is the penalty parameter and 𝜇 is the vector of lag range multipliers. 2.3 Discrete Fourier Transform The DFT is used to compute the Fourier transform of discrete data. The Wavelet performance is better than DFT because wavelet can localized in both frequency and time. The DFT maps a discrete signal into the frequency domain. In the DFT we use sine and cosine waves, it commonly called as DFT basis functions. The DFT basis generating functions are Ck[i] =cos (2πki/N), Sk[i] = sin (2πki/N) Where ck[i] is the cosine wave for the amplitude held in real part sk[i] is the cosine wave for the amplitude held in imaginary part. The DFT can be calculated in three different waves. Such as 1) Set of simultaneous equations 2) Correlation 3) FFT [Fast Fourier Transform]
  • 3. Performance of MMSE Denoise Signal Using LS-MMSE Technique | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 58| In this paper we are using the Fast Fourier Transform. Fast Fourier Transform is ingenious algorithm it decomposes a DFT with N points. The Fast Fourier Transform is 100 times faster than the Set of simultaneous equations, Correlation. Here we notice that, DFT has less than 32 points than we used correlation method otherwise we go for the Fast Fourier Transform. III. LS-MMSE The method of least squares-mmse is estimating the mmse by minimizing the squared discrepancies between observed data and their expected signal values. We will study the method in the context of regression problem, where the variation in one variable, called the response variable Y, multiple linear regression co- variables x. The prediction of Y is given by Y=f(X) +noise……. (5) Where f= egression function. It is used to estimate the co-variables and their responses. The block diagram of LS-MMSE is given by Fig.3.1 block diagram of LS-MMSE technique The least squares criterion is a computationally better compare to CCS-MMSE. It corresponds to maximum likelihood estimation when the noise is normally distributed with equal variances. Other measures of fit are sometimes used, for example, least absolute derivations, which is more robust against outliers. The least squares estimator, denoted by β, is that value of b that minimizes 𝒚𝒊 − 𝒇 𝒃 𝒙𝒊 𝟐𝒏 𝒊=𝟏 ----------- (6) The covariance matrix of estimator β is equal to 𝑋′ 𝑋 𝜎2 Where σ2 is the variance of the noise. As an estimator of σ2 , we consider 𝛔 𝟐 = 𝟏 𝐧−𝐩 𝐲 − 𝐗𝛃 𝟐 = 𝟏 𝐧−𝐩 𝐞 𝐢 𝟐𝐧 𝐢=𝟏 ----------- (7) The algorithm of LS-MMSE is given by 1. Initialize parameters 2. For snr = 1:20 3. For iteration 1:2000 4. X=Generate random signal 5. X1=convert serial to parallel 6. B=2*X-1%convert binary signal 7. Pilot=[bit(1:m) pilot symbol bit(m+1:end)]%insert pilot signal 8. Wavelet = dwt2(pilot, „haar wavelet‟)%add wave let 9. G=insert interval 10. W=HG+n %output signal 11. 𝛔 𝟐 = 𝟏 𝐧−𝐩 𝐲 − 𝐗𝛃 𝟐 = 𝟏 𝐧−𝐩 𝐞 𝐢 𝟐𝐧 𝐢=𝟏 12. Error=error+(|X-∅mmse) 13. End iteration 14. End snr
  • 4. Performance of MMSE Denoise Signal Using LS-MMSE Technique | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 59| Improving the signal quality, removing noisy signal domain and minimum MMSE denoise signal are the advantages of LS-MMSE technique. IV. Experiment Results We have used MATLAB to perform simulations of the CCS-MMSE and LS-MMSE are discussed in section II, III. As can be seen in Fig 2,3 and 4, both CCS-MMSE and LS-MMSE result in the best MSE reduction for all signals and noise levels. The performance of LMMSE and TV methods heavily depends on the type of signal. Fig4.1 the average MSE reduction is plotted against AWGN variance with Gaussian noise Fig4.2.the average MSE reduction is plotted against AWGN variance with Laplace noise Fig4.3.the average MSE reduction is plotted against AWGN variance with Cauchy noise
  • 5. Performance of MMSE Denoise Signal Using LS-MMSE Technique | IJMER | ISSN: 2249–6645 | www.ijmer.com | Vol. 4 | Iss.10| Oct. 2014 | 60| V. Conclusion& Future Scope We present the performance of average MSE reduction using various Bayesian methods. The LS-MSE technique is better performance to existing methods in terms of mmse reduction. Although, the results presented here focus on 1D signal, the extensions to 2D OR 3D data can be achived by using higher-dimensional Haar- transforms in CCS-MMSE technique. REFERENCES [1] Abbas Kazerouni, Ulugbek S.Kamilov, “Bayesian Denoising: from MAP to MMSE Using Consistent Cycle Spinning”, IEEE Tran .Signal Processing, vol20, no.3, pp. 249-252, March 2013. [2] D.L. Donoho and I.M. John stone, “Ideal spatial adaption by wavelet shrinkage”, Biometrika, vol. 8.1, no.3, pp.425- 455, 1994 [3] R.R.Coifmanand D.L.Donoho, “Springer Lecture Notes in Statistics”. New York: Springer-Verlag, 1995, pp. 125– 150, ch. Translation-invariant de-noising. [4] M.A.T. Figueiredo and R. D. Nowak, “An EM algorithm for wavelet-based image restoration,” IEEE Trans. Image Process., vol. 12, no. 8, pp. 906–916, 2003. [5] M. Guerquin-Kern, M. Häberlin, K. P. Prüssmann, and M. Unser, “A fast wavelet-based reconstruction method for magnetic resonance imaging,” IEEE Trans. Med. Image., vol. 30, no. 9, pp. 1649–1660, 2011. [7] L.I.Rudin,S.Osher,andE.Fatemi, “Nonlinear total variation based noise removal algorithms,” Physica D, vol. 60, pp. 259–268, 1992. [8] G. Steidl, J.Weickert, T. Brox, P.Mrazek, and M.Welk, “On the equivalence of soft wavelet shrinkage, total variation diffusion, total variation regularization, and SIDEs,” SIAM J. Numer. Anal., vol.42, no.2, pp. 686–713, 2004. [9] J.Nocedal and S.J.Wright, “Numerical Optimization”, 2nd ed. New York: Springer, 2006.