UpadhyayaVivek1
SalimMohammad2
-
(Department of Electronics & Communication, Malaviya National Institute of Technology,
India 2018rec9028@mnit.ac.in)
-
(Department of Electronics & Communication, Malaviya National Institute of Technology,
India msalim.ece@mnit.ac.in )
Copyright © The Institute of Electronics and Information Engineers(IEIE)
Keywords
Compressive sensing (CS), Magnetic resonance imaging (MRI), Structural similarity index (SSIM), Feature similarity index measure (FSIM)
1. Introduction
Magnetic Resonance Imaging (MRI) is an imaging method that is very popular nowadays.
Imaging contrast of soft tissues is very high, and it is the prime reason for its
popularity. Our bodies are made up of a large amount of water and hydrogen atoms,
and they act like magnetic elements. If the body is placed in an external magnetic
field, then these little magnetic entities will align according to the external fields
[1]. These little magnetic entities also rotate with an angular frequency known as the
Larmor frequency. Further, if radiofrequency is also applied in this Larmor frequency
range, then the previously spinning protons will absorb some amount of RF energy and
move from lower to higher energy states. This is known as the condition of resonance.
When the external RF source is switched off, these protons are again switched to their
initial position, and the energy difference will surge the level of the magnetic resonance
signal. We know that the different body tissues release different amounts of energy
because of their chemical and physical composition, so the magnetic resonance signal
is also different at that level. The main problem associated with MRI is the rate
of the acquisition process as it is very slow. Therefore, in the next sub-section,
we discuss how the data acquisition process takes place in MRI.
1.2 Data Acquisition Strategy for MRI
The data which is acquired in a raw form is stored in the k-space or Fourier domain
as a matrix. Therefore, if we want to analyze it in the image, then we have to apply
a two-dimensional inverse Fourier transform. Two types of the gradients are used to
encode the k-space: one is horizontal, which is based on frequency, and the other
is vertical, which is based on the phase. They are named the Frequency Encode Gradient
(FEG) and Phase Encode Gradient (PEG).
1.3 Types of Weighted Images
If the contrast of a magnetic image is based on the longitudinal relaxation time,
then it is termed as a T1 weighted image. Both the repetition time and the echo time
are short for this type of weighting strategy. Similarly, T2 weighted images are images
that are based on the transverse relaxation time, and the value of repetition time
and the echo time are long in this case. The third category is based on the density
of hydrogen atoms in the body tissue for a particular volume. In this case, the value
of repetition time is large, and the echo time is very short. In the next section,
we elaborate on the work that has been done by various researchers in this domain.
2. Literature Review
One author proposed an approach that is based on the combination of objective-based
and deep learning-based compressive sensing reconstruction approaches [2]. Multi-layer based convolutional sparse coding with iterative thresholding is used
to recover the MRI based image. MR images of the knee and brain were used for the
experiment. PSNR and SSIM values were mentioned in the results. A method based on
enhanced Laplacian Scaled shrinkage and BM3D was proposed by the authors for MR image
reconstruction.
Brain, shoulder, chest, and head-based MRI images were considered for analysis [3]. A comparative study based on SSIM, PSNR values, sampling rate, and standard deviation
for various algorithms was mentioned. Yiling Liu et al. proposed an improvement for
a compressive sensing-based MRI scheme to overcome the structure loss [4]. In this paper, the authors presented the theoretical aspects of the normalized iterative
hard thresholding scheme. The contribution of the authors is a quantized framework
that can be employed for MRI as well as radio astronomy [5].
A mathematical model was proposed by the authors, which consists of a locally low-rank
MRI reconstruction technique. Knee and brain MR images were considered, and the normalized
RMSE value was mentioned in the results [6]. Yipeng Liu et al. talked about dynamic MRI. Further, they proposed a hybrid model
based on a compressive sensing approach for the highly efficient recovery of MRI images
[7]. Experimental justification for the high efficiency and low computational complexity
was also mentioned. The prime concern of all the authors was to improve the quality
of reconstruction of MRI, and the computational complexity should low. In the next
section of the paper, we move towards the mathematical framework for the compressive
sensing MRI strategy.
Fig. 1. Data Acquisition Strategy Flow Diagram.
Fig. 2. Signal Intensities for Different Weighted Images
3. Mathematical Framework for CS-MRI
Compressive sensing is a technique that can be used to acquire sparse signals by employing
a direct method, or the signal may be sparse in some domain [8]. We talk about the key parameters that are responsible for the success of the compressive
sensing approach. The first key aspect is that the signal must be sparse, or it may
be sparse in some random domains. The second one is the incoherence as we use under-sampling
in the compressive sensing, so we have to remove the aliasing problem. This is tackled
by using the incoherent representation basis.
3.1 Sparsity for Magnetic Resonance Imaging
It is a well-known concept that natural images are not sparse in their domain, but
they may be sparse in some other transform domain. We consider a dense n x n spatial-domain
image a, and it is compressible to some other domain ${\Psi}$ (DCT or wavelet). If
image a is reframed to n x 1 column vectors, then ${\Psi}$ can be considered as a
transform matrix.
3.2 Mutual Coherence
Our prime concern is the efficient recovery of an image from compressed data, so the
measurement matrix ${\Phi}$ must be incoherent in some sparse basis matrix ${\Psi}$
[9]. Let G$_{\mathrm{u}}$ be a measurement matrix and G$_{\mathrm{u}}$= ${\Phi}$ G, where
$\Phi \in R^{m\times n}$, in which each row has all zero values except one value.
If we want to analyze it mathematically, it is represented as below.
If Gu and ${\Phi}$ contain elements that are correlated, then incoherence is small.
Otherwise, it has a higher value.
Table 1. Various input images used for the experiment.
MR
Image
|
T-1
MR Image
|
T-2
MR Image
|
PD
MR Image
|
Brain
|
|
|
|
Pelvis
|
|
|
|
Feet
|
|
|
|
Thigh
|
|
|
|
Thorax
|
|
|
|
3.3 Proposed Approach
In this work, we want to find out a strategy that can easily indicate that the compressive
sensing approach is an effective framework that can be used to compress MR images
and then retrieve them. Therefore, for this purpose, we defined a basic approach that
is given in the flow diagram below. As per the literature, when under-sampling is
conducted in the k-space by periodic interleaving, it will violate the Nyquist theorem
and will produce aliasing in the recovered images. Therefore, the aliasing and incoherence
should be less visible in the recovered MR image.
As in the work proposed by Candes et al., fewer samples can also reconstruct images
without an aliasing effect. In MR, the signal has spatial redundancy, so in some transform
domains, few components have maximum information from the image. Therefore, the compressive
sensing approach can easily be applied and efficiently recover MR images with a few
samples.
As per the flow diagram, first of all, a raw input image is considered. Then, we convert
this image into a corresponding number of N discrete samples. After that, the sparsity
of the image is calculated by defining the basis and sensing matrices and generating
them. Then, we multiply the image with the basis and sensing matrix to represent it
in the basis domain.
The inverse function is applied to recover the original image by using the reconstruction
strategy. Lastly, we obtain the magnetic resonance image. To check the quality of
the recovered image, we use certain image-quality assurance indexes like SSIM, FSIM,
etc. In the next section, we discuss various image quality assessment parameters that
will clarify the efficiency of the reconstruction algorithm.
Fig. 3. Flow Diagram of Proposed Approach.>
4. Result and Analysis
The purpose of this work is to compress various types of MR images with the help of
compressive sensing and then to compare the reconstructed images with the original
image to calculate the efficiency of the proposed image. For this purpose, a set of
images was utilized: T-1, T2, and proton density-based images. Image quality assessment
was done by using the PSNR, MSE, SSIM, FSIM, and CVSS. Expressions for all the IQA
parameters are mentioned in the upcoming section.
4.1 Peak Signal-to-noise Ratio
The peak signal-to-noise ratio is an image quality assessment parameter that is used
to analyze the quality of a computed tomography-based image [10]. The calculation of PSNR is conducted using actual MR image samples and the reconstructed
MR image samples. A higher value of PSNR denotes better quality of the reconstructed
MR image.
F$_{\mathrm{i}}$ = MR based image’s actual signal, L$_{\mathrm{o}}$ = MR-based image’s
reconstructed signal, m = total number of components.
Fig. 4. Plot Representing C/R vs. PSNR for Brain.
Fig. 5. Plot Representing C/R vs. PSNR for Pelvis.
4.2 Compression Ratio (C/R)
The compression ratio is a defined parameter that indicates how many sample components
are considered in the reconstruction process out of the total number of components
present in that signal or MR image [11]. It is the ratio between the sample utilized in reconstruction and the total number
of samples in the MR image.
m= samples used for reconstruction of MR image, n= actual number of samples in MR
image.
4.3 Structural Similarity Index Measure (SSIM)
The SSIM index is a mathematical model to find out the similarity between two images.
It can be considered as a quality measurement for one image compared to another image
that keeps the quality of the image in the main perspective. We can say it is a modified
structure of the universal image quality index [12].
4.4 Feature Similarity Index Measure (FSIM)
The basic function of FSIM is to map the similarity between two images. Phase congruency
and the gradient magnitude are the two key techniques to find out the value of FSIM
[13].
Here, PC$_{\mathrm{m}}$is the maximum value of phase congruency of both images. ${\Omega}$
represents that the image is in the spatial domain.
4.5 Contrast and Visual Salient Similarity (CVSS)
CVSS is also an image quality assessment parameter that is used to find out the quality
of a reconstructed image [14]. In this approach, we find out a score value that represents how close the recovered
image is to the actual image. The quality score parameter is defined below.
Here, w$_{1}$ and w$_{2}$ are the weights of the local contrast similarity and visual
saliency, respectively.
4.6 Mean Square Error (MSE)
MSE is used to calculate the relation of the original and recovered MR images.
Here, U represents the original MR image, V represents the recovered MR image, and
n shows the total number of samples. Diagrams that show the value of compression ratio
vs. PSNR and SSIM values are shown below. We can easily find out the variation between
the three types of weighted images. In the images, plots are given for the compression
ratio vs. peak signal-to-noise ratio and structural similarity index measures. Now,
we elaborate on various tables consisting of the compression Ratio vs. FSIM, CVSS,
and MSE.
To present the efficiency of the proposed algorithm, we compare our work with the
work proposed by Tariq Tashan et al. [15]. They presented multilevel MR imaging. As a result of comparison, we found that our
proposed approach has significantly enhanced values of image quality assurance matrices.
Fig. 6. Plot Representing C/R vs. PSNR for Feet.
Fig. 7. Plot Representing C/R vs. PSNR for Thigh.
Fig. 8. Plot Representing C/R vs. PSNR for Thorax.
Fig. 9. Plot Representing C/R vs. SSIM for Brain.
Fig. 10. Plot Representing C/R vs. SSIM for Pelvis.
Fig. 11. Plot Representing C/R vs. SSIM for Feet.
Fig. 12. Plot Representing C/R vs. SSIM for Thigh.
Fig. 13. Plot Representing C/R vs. SSIM for Thor\#ax.
Table 1. Table for C/R vs. FSIM for T1 MR Images.
C/R
|
FSIM Values for T1 Weighted Image
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
0.5760
|
0.6821
|
0.5872
|
0.5981
|
0.6928
|
1000/4096
|
0.6391
|
0.7348
|
0.6190
|
0.6888
|
0.7410
|
1500/4096
|
0.6918
|
0.7894
|
0.7038
|
0.7491
|
0.8029
|
2000/4096
|
0.7268
|
0.8427
|
0.7331
|
0.7927
|
0.8484
|
2500/4096
|
0.8023
|
0.8810
|
0.8082
|
0.8506
|
0.8897
|
3000/4096
|
0.8354
|
0.9237
|
0.8531
|
0.8971
|
0.9235
|
3500/4096
|
0.9075
|
0.9542
|
0.9090
|
0.9534
|
0.9587
|
Table 2. Table for C/R vs. FSIM for T2 MR Images.
C/R
|
FSIM Values for T2 Weighted Image
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
0.6221
|
0.7471
|
0.6747
|
0.7031
|
0.7590
|
1000/4096
|
0.6858
|
0.7913
|
0.7468
|
0.7786
|
0.8111
|
1500/4096
|
0.7197
|
0.8365
|
0.7728
|
0.8505
|
0.8534
|
2000/4096
|
0.7673
|
0.8702
|
0.8394
|
0.8904
|
0.8807
|
2500/4096
|
0.8174
|
0.9099
|
0.8869
|
0.9371
|
0.9198
|
3000/4096
|
0.8672
|
0.9372
|
0.9260
|
0.9611
|
0.9437
|
3500/4096
|
0.9052
|
0.9656
|
0.9634
|
0.9775
|
0.9675
|
Table 3. Table for C/R vs. FSIM for PD MR Images.
C/R
|
FSIM Values for Proton Density Weighted Image
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
0.5365
|
0.7086
|
0.5669
|
0.6001
|
0.6804
|
1000/4096
|
0.5876
|
0.7538
|
0.6197
|
0.6945
|
0.7290
|
1500/4096
|
0.6312
|
0.8070
|
0.6722
|
0.7560
|
0.7830
|
2000/4096
|
0.6856
|
0.8364
|
0.7262
|
0.7988
|
0.8271
|
2500/4096
|
0.7387
|
0.8735
|
0.7848
|
0.8477
|
0.8614
|
3000/4096
|
0.7816
|
0.9186
|
0.8302
|
0.8992
|
0.8905
|
3500/4096
|
0.8428
|
0.9481
|
0.8942
|
0.9489
|
0.9380
|
Table 4. Table for C/R vs. CVSS for T1 MR Images.
C/R
|
CVSS Values for T1 Weighted Image
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
0.0908
|
0.0614
|
0.1024
|
0.0994
|
0.0659
|
1000/4096
|
0.0790
|
0.0466
|
0.0907
|
0.0776
|
0.0575
|
1500/4096
|
0.0672
|
0.0411
|
0.0746
|
0.0647
|
0.0388
|
2000/4096
|
0.0442
|
0.0295
|
0.0650
|
0.0508
|
0.0296
|
2500/4096
|
0.0430
|
0.0203
|
0.0455
|
0.0360
|
0.0203
|
3000/4096
|
0.0316
|
0.0121
|
0.0351
|
0.0231
|
0.0131
|
3500/4096
|
0.0168
|
0.0069
|
0.0195
|
0.0091
|
0.0065
|
Table 5. Table for C/R vs. CVSS for T2 MR Images.
C/R
|
CVSS Values for T2 Weighted Image
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
0.0826
|
0.0434
|
0.0614
|
0.0512
|
0.0429
|
1000/4096
|
0.0805
|
0.0315
|
0.0403
|
0.0374
|
0.0259
|
1500/4096
|
0.0609
|
0.0237
|
0.0343
|
0.0250
|
0.0208
|
2000/4096
|
0.0512
|
0.0178
|
0.0249
|
0.0176
|
0.0152
|
2500/4096
|
0.0397
|
0.0119
|
0.0158
|
0.0095
|
0.0112
|
3000/4096
|
0.0299
|
0.0069
|
0.0107
|
0.0054
|
0.0070
|
3500/4096
|
0.0184
|
0.0039
|
0.0051
|
0.0029
|
0.0035
|
Table 6. Table for C/R vs. CVSS for PD MR Images.
C/R
|
CVSS Values for Proton Density Weighted Image
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
0.1333
|
0.0692
|
0.1159
|
0.1122
|
0.0847
|
1000/4096
|
0.1253
|
0.0497
|
0.1019
|
0.0860
|
0.0664
|
1500/4096
|
0.1171
|
0.0412
|
0.0898
|
0.0659
|
0.0479
|
2000/4096
|
0.1003
|
0.0290
|
0.0733
|
0.0491
|
0.0378
|
2500/4096
|
0.0871
|
0.0251
|
0.0582
|
0.0320
|
0.0275
|
3000/4096
|
0.0635
|
0.0138
|
0.0430
|
0.0201
|
0.0207
|
3500/4096
|
0.0436
|
0.0081
|
0.0239
|
0.0084
|
0.0099
|
Table 7. Table for C/R vs. MSE for T1 MR Images.
C/R
|
MSE Values for T1 Weighted Image (*10^2)
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
8.37
|
7.58
|
9.96
|
1.11
|
5.02
|
1000/4096
|
6.08
|
5.59
|
6.54
|
6.97
|
3.40
|
1500/4096
|
4.07
|
5.59
|
4.54
|
4.16
|
2.34
|
2000/4096
|
2.87
|
2.84
|
3.07
|
2.5
|
1.58
|
2500/4096
|
1.90
|
1.82
|
2.05
|
1.55
|
1.09
|
3000/4096
|
1.24
|
1.18
|
1.15
|
0.83
|
0.74
|
3500/4096
|
.63
|
0.60
|
0.53
|
0.37
|
0.36
|
Table 8. Table for C/R vs. MSE for T2 MR Images.
C/R
|
MSE Values for T2 Weighted Image (*10^2)
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
7.39
|
2.63
|
2.92
|
2.91
|
2.50
|
1000/4096
|
5.01
|
1.83
|
1.86
|
1.70
|
1.50
|
1500/4096
|
3.97
|
1.42
|
1.44
|
1.14
|
1.12
|
2000/4096
|
2.80
|
1.04
|
0.855
|
0.715
|
0.772
|
2500/4096
|
2.03
|
0.717
|
0.555
|
0.442
|
0.509
|
3000/4096
|
1.24
|
0.437
|
0.349
|
0.235
|
0.363
|
3500/4096
|
0.660
|
0.243
|
0.157
|
0.107
|
0.177
|
Table 9. Table for C/R vs. MSE for PD MR Images.
C/R
|
MSE Values for Proton Density Weighted Image (*10^2)
|
Brain
|
Pelvis
|
Feet
|
Thigh
|
Thorax
|
500/4096
|
26.3
|
9.40
|
14.2
|
12.3
|
8.56
|
1000/4096
|
16.0
|
7.20
|
10.5
|
8.16
|
4.96
|
1500/4096
|
10.9
|
5.40
|
6.38
|
4.52
|
3.83
|
2000/4096
|
8.36
|
3.79
|
4.26
|
2.69
|
2.61
|
2500/4096
|
5.33
|
2.58
|
2.69
|
1.56
|
1.82
|
3000/4096
|
3.00
|
1.55
|
1.67
|
0.859
|
1.12
|
3500/4096
|
1.61
|
0.846
|
0.744
|
0.381
|
0.583
|
Table 10. Comparison with Work Shown by Tariq et al..
C/R
|
PSNR Values (dB)
|
For Proposed algorithm
|
For algorithm mention in [15]
|
0.12
|
38.3
|
37.1
|
0.24
|
40.1
|
39.2
|
0.36
|
43.6
|
42.1
|
0.48
|
45.2
|
44.2
|
0.61
|
46.4
|
45.5
|
0.73
|
47.9
|
46.7
|
0.85
|
48.2
|
47.3
|
5. Conclusion
Compressive sensing is a technique that can efficiently reduce the number of samples
required for a good reconstruction process. This technique was used, and we can see
that it was very effective in this work. As MR imaging is a slow and time-consuming
process, the patient has to wait for a long time (20-30 minutes) for the imaging process.
Spending this much time under a huge magnetic field can also harm the patient’s body
and some tissues. Therefore, reducing the number of samples in the k-space for the
recovery process can also reduce the required time.
In this work, we analyzed various numbers of image quality assessment matrices, which
indicated that even if we reduce the number of samples in the reconstruction process,
the quality of the image at a significant value of compression ratio is up to the
mark and can easily represent all the information in the MR image. Signal intensities
for T1, T2, and proton density-weighted MR images are different, so they will directly
affect the reconstruction process too. At the same compression ratio (e.g., 3000/4096),
the values of FSIM, SSIM, PSNR, MSE, and CVSS are different for similar body-part
images in different weighted images.
As we can see, if the number of samples that are required to reconstruct an image
is large enough, then the time required to reconstruct the image is also large. Therefore,
if the number of samples is reduced to a certain level, then the time required in
the MRI process can also be reduced to a certain level. Table 10 shows a significant comparison of our work with other work [15]. Here, we can check that the PSNR values for our proposed algorithm are sufficiently
large compared to the other PSNR values.
ACKNOWLEDGMENTS
This research was supported by the Visvesvaraya Ph.D. Scheme, MeitY, Govt. of India,
with unique awardee number “MEITY-PHD-2946”. Name of Grant Recipient: Vivek Upadhyaya.
Conflict of Interest
Vivek Upadhyaya received a research grant from the Visvesvaraya Ph.D. Scheme, MeitY,
Govt. of India, with unique awardee number “MEITY-PHD-2946”. Dr. Mohammad Salim declares
that he has no conflict of interest.
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Author
Vivek Upadhyaya graduated with his “Bachelor of Engineering” in Electro-nics and Communication
Engineering from Rajasthan University, Rajasthan, India in 2009. He has done M. Tech
in Electronics and Communication from Malaviya National Institute of Technology, Jaipur,
in the year 2016 and a Ph.D. (Pursuing) from Malaviya National Institute of technology.
He has been the recipient of the Visvesvaraya scholarship given by the Ministry of
Electronics & I.T. (Govt. of India) during his Ph.D. His research work is focused
on Medical Image and Data Compression. He has been carrying out his research on Compressive
Sensing for Medical Imaging.
Mohammad Salim has more than 35 years of teaching experience and is presently serving
as a professor in the Department of Electronics & Communication, Malaviya National
Institute of Technology, Jaipur, India. He has guided more than 50 M.Tech. theses,
45 undergraduate projects, and 5 Ph.D. thesis. He has been to Sheffield Hallam University,
Sheffield, U.K., for eight months under the U.K.-India REC project. He has been a
nominated member in the Rajasthan High Court Committee for monitoring mobile tower
radiation. His research interests include error control codes, wireless communications,
signal and image processing analysis, mobile communication, optical properties of
metal nanoparticles, optical communication, optoelectronics and photonics, RF and
microwaves, EMI/EMC, solar cells, electromagnetic radiation hazards, RF power harvesting,
etc.