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PDE-BASED DENOISING TECHNIQUE IN MREIT



Byung Il Leea, Suk Ho Leeb, Tae-Seong Kima, Jin Keun Seob, Ohin Kwonc, and Eung Je Wooa

a

Kyung Hee University, Kyungki 449-701, Korea

b

Yonsei University, Seoul 120-749, Korea

c

Konkuk University, Seoul 143-701, Korea





In Magnetic Resonance Electrical Impedance Tomography (MREIT), we try to visualize cross-sectional

images of conductivity distributions inside an electrically conducting subject. Several conductivity image

reconstruction algorithms have been developed based on the measurement of only one component such as

Bz of the magnetic flux density B = (Bx, By, Bz) [1-2]. However, the measured data Bz in MREIT is usually

degraded in its accuracy due to the non-ideal data acquisition system of an MR scanner. Furthermore,

numerical computations of Bz or 2Bz in the developed conductivity reconstruction algorithms such as

the harmonic Bz algorithm [1] and the gradient Bz decomposition algorithm [2] tend to amplify the noise in

Bz. Hence, it is necessary to develop an efficient denoising technique that eliminates the random noise in

the Bz signal while preserving important features.



We have to change the problem into a form which is easier to handle. We use a kind of decomposition

technique which decomposes the original noisy Bz data into a smooth part and a noisy high-frequency part

as

Bz = Bzs + Bzn. (1)

After denoising each decomposed part independently using different denoising techniques, the noise-

removed parts are combined together to result in a noise-removed Bz data. Therefore, we propose a PDE-

based denoising technique which shuts the diffusion process off at the peaks. However, we have to judge

whether a peak indicates an edge or noise. In order to do this, we need to trace the location of the edges.

This can be done by using the information given by the corresponding MR magnitude image M. This can

be achieved by solving the following diffusion equation in the corresponding imaging slice  with its

boundary .

 u   1  

    g    u   0



in 

 t   M  

  (2)



 u ( x, y ,0)  Bz ( x, y ) on 

n





where g is an increasing function with g(0) = 0 and lims g (s)   .



Numerical results show that the reconstruction algorithm with the denoised Bz data successfully

reconstruct the conductivity image. The proposed denoising technique is based on a kind of harmonic

interpolator using its neighbouring noisy Bz data and concentrated on the noisy high-frequency part Bzn. In

a homogeneous medium, Bzn would be constant plus an added noisy.



Acknowledgements: This work was supported by the grant R11-2002-103 from Korea Science and

Engineering Foundation.



REFERENCES

1. S. H. Oh, B. I. Lee, E. J. Woo, S. Y. Lee, M. H. Cho, O. Kwon, and J. K. Seo, “Conductivity and current density

image reconstruction using harmonic Bz algorithm in magnetic resonance electrical impedance tomography,”

Phys. Med. Biol., vol. 48, pp. 3101-16, 2003.

2. C. Park, O. Kwon, E. J. Woo, and J. K. Seo, “Electrical conductivity imaging using gradient Bz decomposition

algorithm in magnetic resonance electrical impedance tomography (MREIT),” IEEE Trans. Med. Imag., vol. 23,

pp. 388-94, 2004.



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