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Combination Compress Sensing and Digital Wireless Transmission for the MRI signal Tan Due Tran , Tuyen Ta Due, and Tung Thanh Bui IMEMS and Microsystems Department, UET-VNU Hanoi, VIETN

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Combination Compress Sensing and Digital Wireless Transmission for the MRI

signal

Tan Due Tran , Tuyen Ta Due, and Tung Thanh Bui

IMEMS and Microsystems Department, UET-VNU Hanoi, VIETNAM 2Research Organization for Science and Engineering, Ritsumeikan University, JAPAN

XuanThuy Street, Hanoi, +844

Vietnam

Abstract:

Rapid image acquisition in magnetic resonance imaging

(MRI) offers a number of potential benefits, such as

avoiding physiological effects or scanning time on

patients, overcoming physical constraints inherent

within the MRI scanner, or meeting timing requirements

when imaging dynamic structures and processes In this

paper, the combination of compressed sensing and

parallel magnetic resonance imaging techniques was

proposed in order to increase the data acquisition speed

of MRI However, each coil arrangement is connected to

the reception circuit via a coaxial cable which leads to

several limitations To reduce this disadvantage, we also

propose a design of digital wireless transmission system

based on 802.11b standard for MRI application

1 INTRODUCTION

Magnetic resonance imaging (MRI), an imaging technique,

is widely used in medical diagnosis in order to acquire

images of the inside of the human body Previously,

techniques for rapid imaging include parallel MRI (PMRl) in

which the simultaneous use of multiple coils is deployed

Two typical parallel imaging techniques are simultaneous

acquisition of spatial harmonics (SMASH) and sensitivity

encoding (SENSE) [1, 2] In pMRI, a coaxial cable is need

for connecting each coil to the corresponding received

circuit The number of the cables and so on the required

connectors is need as high as possible but limited due to

constraint space and cross-talk among these coils Wireless

transmission can be a good candidate to replace cable

connections of the coil arrays to reduce these disadvantages

Recently, compressed sensing (CS) is a breakthrough

research field, which finds ways to sample signals at much

lower rate than the Nyquist one The condition is that the

sensing signal is sparse in some domain of representation

(Fourier transforms, for example) However, most of

developments in CS are based on the use of a single

channel/coil

In this paper, we combined compress sensing and digital

wireless transmission for the rapid MRI The organization of

this paper is as follows Section II describes operation

principle of our proposed wireless multi-channel compressed

sensing for MRI based on two conventional methods:

compressed sensing, parallel imaging, and digital wireless

transmission Section III presents our simulation results

Conclusions are drawn in the last section

2 OPERATION PRINCIPLES 2.1 Compressed sensing

Compressed sensing (CS) is a type of random under-sampling which allows for rapid acquisition of spare

or compressible signals, at a frequency significantly lower than the usual Nyquist frequency [3] To consider a I x N discrete time signal x and assume that x is a k-space in the N-dimensional space:

where 'P is N x N sparsitying matrix, s is the N x I transform vector containing K non-zero coefficients, K «

N When used in MRI, 'P is a Fourier matrix

In CS, x is linearly acquired by under-determined system which is represented by a measurement matrix <1>

y= <1>x (2) where y is M - dimensional measurement vector obtained incomplete measurements (M<N)

The reconstruction can be done using various spare approximation techniques such as II-optimization based Basic Pursuit or Orthogonal Matching Pursuit (aMP) [4] The condition of aMP is that the matrix <1> is coherence with 'P This condition is met by having <1> as a random matrix with Gaussian i.i.d elements

Fig I illustrates a MRI acquisition with a single coil in which Cartesian sampling is applied in k-space Note that the reconstruction can be easy performed by utilizing the inverse fast Fourier transform (IFFT)

ky

I

kx

Figure I Cartesian trajectory (a) and MRI undersampling in k-space [5] 2.2 Parallel Imaging

To receiver the MRI data, several array coils are used concurrently (Fig 2) Consequently, each coil would have

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individual values of image's intensity The k-space signal

obtained from the l-th coil:

xY

Where:

p(x,y) is the image function to be recover

Clx,y) is the sensitivity function for the l-th coil

(x,y) are spatial domain coordinate

(kx, ky) are samples in k-space

Figure 2 Illustration of using multi-coils for pMRl [5)

It's certain that Equ (3) is the Fourier transform of the

sensitivity-weighed images: C](x,y) p(x,y) The sensitivity

functions Clx,y) are often not known and the l-th image S]

could be expressed as the ideal image modulated by

sensitivity functions as:

In pMRI, only a smaller of data is acquired to reduce the

acquisition time The number of excitations, consequently,

the number of phase-encoding steps determine for the total

acquisition time By skipping phase-encoding steps, the

sensed size of the imaged area is also reduced The spatial

resolution is not change but the aliasing artifact is appeared

The pMRI reconstruction algorithm has a role to estimate the

coil sensitivities C] then use these coil sensitivities to remove

the aliasing and reconstruct the ideal image The quality of

the reconstruction can be expressed as the absolute

difference between the reconstructed image and the ideal

image

There are two very basic methods for parallel MRI

reconstruction: Sensitivity encoding for fast MRI (SENSE)

[1] and Simultaneous acquisition of spatial harmonics

(SMASH) [2]

SENSE works in the image domain that using the un-aliasing

method to the reduce field of view (FOY) images In this

method, the inversion of the aliasing transformation for each pixel is calculated individually The important process is that estimation of the map of the coil sensitivities:

It can be seen that we have a calibration procedure with the reference images (without aliasing artifact and noise) In practice, we can smooth and extrapolate the coil sensitivities

to obtain a acceptable sensitivity map However, it is obvious that this map can only be estimated by using no-aliasing reference images

However, the SENSE can work only in a Cartesian grid but not in arbitrary sequence An effective method which is able

to overcome this problem is called conjugate gradient SENSE (CG-SENSE) [6] However, the CG-SENSE also requires the information of the sensitivity map In present, the SENSE method is modified in order to work in auto-calibration mode One of these versions is mSENSE [7] In CG-SENSE, MRI reconstruction from the k-space samples is performed by Nonlinear Conjugate Gradient (NCG) [8]

2.3 Digital Wireless Transmission

In this paper, the system schematic of digital wireless transmission for MRI signal is shown in Fig 3 The budget for transmission is calculated based on the MR image pixel size 128 x 128 x number of coils, accommodate framing, overhead, and checksum, etc Therefore, the 801.11 b standard is chosen due to its capable to provide the bit rate requirement at 11 Mbps

MRI signal

Channel

Figure 3 The system model of a single coil

For MRI application, high bit error rate (BER) performance

in communication is also required Fig 4 is the simulated result of BER performance versus signal to noise ratio (SNR)

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Figure 4 BER peformance of the 801.11b standard communication

2.4 Proposed System Descriptions

Our scheme can be summarized as following steps:

• Generate (kx, ky) that are Gaussian random sequences

The number of (kx, ky) based on pre-defined

compression ratio r = MIN For each channel, determine

coordinates in k-space based on (kx, ky) and store as a

mask

• For each channel, under-sample and acquire digital data

in k-space based on the mask and store them in a vector

y

• Synthesis and send the processed data to wireless

transmitter

• Receive the data at the computer

• Estimate sensitivity maps using polynomial fitting

• Perform SENSE reconstruction using conjugated

gradient method

3 RESULTS AND PERFORMANCE

The data source utilizing in this work is human MPRAGE

from [9] The BER condition of 10-9 is set in communication

setting The original image from 8 coils was shown in Fig 5

Figure 5 The original image from 8 channels

Fig 6 shows the k-space under-sampling points in this

scenario

Figure 6 The k-space sampling point (white points) for the compression

ratio r=0.2

Using the zero padding, the combined analysed images were displayed in Fig 7

Figure 7 The combined aliased image from 8 channels for the

compression ratio r=0.2

The image in Fig 8 was obtained by CG-SENSE reconstructing method The result can be also compared to the desired result (Fig 9) We can obtain this best reconstructed image by using the sampled ratio of 1.0

Figure 8 The SENSE reconstructed image for the compression ratio r=0.2

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1.8

1.6

1.4

Figure 9 The reconstructed image with full-sampling, r=1.0

For each compression ratio, the error in the reconstructed

image as compared to the original image Suppose that I is a

NxM original image and] is the reconstructed image The

error between them can be defined by:

1 N M I � I

Fig 10 shows the reconstructed performance obtained by

Monte-Carlo method

0.12

0.1

w

(IJ 0.08

0.06

0 04

ratio

Figure 10 Reconstructed performance by random approach

4 CONCLUSION

We have successful in combining the random based

compressed sensing, parallel MRI, and digital wireless

transmission in order to improve the scanning time for MR

image acquisition The simulation on phantom image shows

that the system can be brought to practice economic system

ACKNOWLEDGMENT

This work is partly supported from the College of Technology, Vietnam National University, Hanoi

REFERENCES

[1] Daniel K Sodickson and W Manning, "Simultaneous acquisition of spatial harmonics (SMASH): fast imaging with radio frequency coil arrays", Magnetic Resonance in Medicine, pp 591-603,1997

[2] Klass P Pruessmann, Markus Weiger, Markus B Sheidegger, and Peter Boesiger, "SENSE: Sensitivity Encoding for Fast MRI", Magnetic Resonance in Medicine, pp 952-956, 1999

[3] E 1 Candes and T Tao, "Reflections on compressed sensing", IEEE Iriformation Theory Society Newsletter,

58(4), pp 20-23, 2008

[4] J Tropp and A Gilbert, "Signal recovery from random measurements via orthogonal matching pursuit," IEEE Transactions on Iriformation Theory, vol 53, pp 4655 -4666,2007

[5] Michael Lustig, David L Donoho, Juan M Santos, and John M Pauly, "Compressed Sensing MRI: A look at how CS can improve on current imaging techniques",

IEEE signal processing magazine, pp 72-82,2008 [6] Pruessmann KP, Weiger M, Bornert P, Boesiger P,

"Advances in Sensitivity Encoding With Arbitrary k-Space Trajectories", Magnetic Resonance in Medicine,

Volume 46, Issue 4, pp 638-651, 2001

[7] Herbert Kostler, Jorn 1.W Sandstede, Claudia Lipke, Wilfried Land-schutz, Mein-rad Beer, and Dietbert Hahn, "Auto-sense perfusion im-aging of the whole human heart", Journal of Magnetic Resonance Imaging,

pp 702-708,2003

[8] M Lustig, D Donoho, and 1 M Pauly, "Sparse MRI: The application of compressed sensing for rapid MR imaging," Magnetic Resonance in Medicine, vol 58, pp 1182-1195,2007

[9] "SENSE: sensitivity-encoding MRI Matlab tools." [Online] Available: http://www.nmr.mgh.harvard.edur tblinltool sense.htm

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