a ovel technique for finding the boundary between the ... · 1 introduction magnetic resonance...
TRANSCRIPT
A �ovel Technique for Finding the Boundary between
the Cerebral Hemispheres from MR Axial Head Scans
K. Somasundaram
1 and T. Kalaiselvi
1
1 Department of Computer Science and Applications,
Gandhigram Rural University,
Gandhigram, Tamilnadu, India.
Abstract. We present a robust technique to detect a linear boundary
between the cerebral hemisphere using the knowledge of brain features
and magnetic resonance imaging (MRI) characteristics. We use two
approaches to extract the brain from T1 and T2 MR axial head scans to
find the brain contour. From the brain contour, we detect the boundary
between the hemispheres by joining the edges of the two portions of cleft
that corresponds to inter-hemispheric fissure present in the contour. The
detected boundary is used to separate the cerebrum into two hemispheres.
We tested our method over several scans collected from MRI centre and
authorized brain image web sites. The performance was validated with
medical experts using both normal and abnormal scans. The predictive
accuracy gives the quantitative measure calculated between the hand-
stripped and our result and is 99% in normal cases and lowered for
abnormal slices.
Keywords: cerebral hemispheres, inter-hemispheric fissure, mid-sagittal
plane, brain extraction algorithm, brain contour, knowledge system, slice
transformation
1 Introduction
Magnetic Resonance Imaging (MRI) is a diagnostic tool used to visualize the
body’s soft tissues. It is noninvasive and does not require ionizing radiation (X-
rays) or radioactive tracers. It uses magnetization and radio waves to produce
high quality three- or two-dimensional cross sectional images in any direction
from top to bottom (axial orientation), side to side (sagittal orientation), or front
to back (coronal orientation). Hydrogen imaging is the most widely used MRI
procedure. The intensity characteristic of a given tissue depends on the proton
density (PD) of the tissue. The higher the PD, the stronger the response signals.
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MR image contrast also depends on two other tissue-specific parameters: the
longitudinal relaxation time T1 and the transverse relaxation time T2. T1 images
are typically used for anatomic information whereas T2 images offer high
sensitivity to most pathologic processes. The rich anatomy information provided
by MRI has made it an indispensable tool for medical diagnosis especially human
brain analysis in recent years.
A human brain has three main components cerebrum, cerebellum and brain
stem. Cerebrum is the largest part of the brain and performs the higher level
functions of the brain. It contains two hemispheres known as left cerebral
hemisphere (LCH) and right cerebral hemisphere (RCH). These cerebral
hemispheres are divided by a deep cleft in lengthwise along the body’s median
plane and is known as longitudinal fissure as shown in Fig.1. The cleft is also
referred to as the inter-hemispheric fissure (IHF). The cleft between the two
cerebral hemispheres contains cerebro spinal fluid (CSF) and the falx cerebri, the
fold of dura matter that separates the cerebral hemispheres.
Fig. 1. Longitudinal Fissure or Inter-Hemispheric Fissure in human brain.
Edge 1 on upper
portion of cleft
Edge 2 on lower
portion of cleft
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The human body’s median plane is referred as mid-sagittal plane (MSP) by
the medical imaging modalities like computed tomography (CT), MRI, positron
emission tomography (PET) and single photon emission computed tomography
(SPECT) techniques due to its relative alignment with the sagittal plane of the
human body. MSP is defined as a planar surface which bisects the cerebrum into
two cerebral hemispheres at their point of bilateral symmetry and alternatively
defined as the plane that passes through the IHF [1] [2] [3]. The standard 3D
space for brain imaging proposed by Talairach [4] fixed the ideal MSP along the
vertical central line of each 2-D axial or coronal slice. But in real time imaging
space of patients, the partitioning plane between the hemispheres does not
coincide with the vertical central line, the ideal MSP, due to the tilt of patient’s
head in the device or the selection of different scanning angles during the image
acquisition phase. Hence the detection of translation and angle of rotation of the
partitioning plane i.e., patient MSP about the ideal MSP is useful for further
processing like image registration, anatomical standardization and spatial
normalization. This is also useful in brain diagnostic process to verify the
position of IHF whether it fits with or deviated from MSP. Usually a normal
brain exhibits symmetry about the IHF. The estimation of MSP is useful for
recognizing non healthy regions of brain and diagnosing several brain diseases
like schizophrenias [5], Creutzfeldt-Jakob disease in T2-weighted MR images
[6], Epilepsy [7] and Alzheimer [8].
Several methods have been developed for MSP extraction. They are
classified into two categories: feature based and image similarity based methods
[1]. Feature based methods define the MSP as the plane that best fits the
longitudinal fissure [3] [9] [10] [11]. Image similarity based methods mostly
depend upon symmetry measure like cross-correlation about a point or line or
block to produce the optimal MSP [1] [2] [12] [13] [14] [15]. Cross correlation is
an expensive operation in general [1]. So we prefer for the feature based methods.
The existing feature based methods have their own limitations. They require
either human intervention or complex functions for optimizing the result. But we
propose a fully automatic intelligent system that solely depends on the brain
anatomy and image intensity information.
In a 2D slice, MSP is a line, mid-sagittal line (MSL) that passes through the
IHF. In this paper, we present a knowledge based method to detect MSL in a
MRI scan. Our method aims to generate the MSL by joining the edges of upper
and lower portions of cleft as shown in Fig.1. These cleft portions are visible
clearly only after removing the surrounding non-brain regions from the MR axial
head scans. So we employ brain extraction algorithms as a preprocessing tool for
our approach. The proposed scheme is simpler than the existing methods and is
based on image intensity and brain features.
The paper is organized as follows. First, we present our method. Then, the
materials used in our experiments are given. The experimental results and
discussions are given finally.
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2 Method
Our method comprise of three stages as shown in Fig 2. In stage-1, the brain
portion is extracted from MR Head scans by eliminating the non-brain portions
like scalp, eyes, fat, muscle, background clutter that are superimposed on the slice
in the form of acquisition parameters and patient’s data. In stage-2, the contour of
extracted brain is utilized to generate the boundary between the cerebral
hemispheres. This boundary corresponds to MSL. Finally in stage-3 the image is
transformed to fix the detected MSL to middle vertical line, the world coordinate
of brain space.
Input: MR axial Head scan
Stage-1: Brain Portion Extraction
Fig. 2. Flowchart of our proposed method
Output: Mid-Sagittal Line (MSL)
Stage-2: Detection of Boundary line
between Hemispheres
Stage-3: Slice transformation to
Standard Space
START
STOP
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2.1 Stage-1: Brain Extraction
In this stage the brain portion is separated from the surrounding non-brain
regions. We have developed two Brain Extraction Algorithms (BEA) for T1 and
T2 scans respectively [16] [17] [18] referred as T1-BEA and T2-BEA hereafter.
The T2-BEA makes use of the combined effect of anisotropic diffusion
process [19], optimal thresholding and morphological processes [20] to separate
the brain from non-brain portions. The diffusion process is used to highlight the
brain from T2 head scan followed by optimal thresholding technique to generate
a rough binary brain portion. The morphological operations, erosion and dilation,
and connected component analysis are used to produce the brain mask by
removing the weakly connected non-brain regions like eyes, neck and etc. Finally
the brain mask is used to extract the brain from T2 scans. The results of T2-BEA
at different stages for a sample slice are given in Fig.3a-3e.
Fig. 3. The results of T2-BEA (a) Original Image (b) Diffused Image (c) Binary form of
rough brain (d) Brain mask produced by morphological operations: erosion and dilation,
and connected component analysis (e) Extracted Brain
The T1-BEA initially detects three main features of human head scalp, skull
and brain using spatial and intensity information of T1 scans and produce a 3-
labeled image as shown in Fig.4b with label 0 for background, label 1 for scalp
and brain and label 2 for skull and other non-brain tissues. Then using run length
identification scheme for labeling [20], it either discards the scalp or extracts the
brain portion to select the rough portion of brain region from T1 scans. The rough
brain region is shown in Fig.4c. Finally the morphological operations and
connected component analysis are employed to produce brain mask as given in
Fig.4d. The brain mask is used to extract the fine brain (Fig.4e) from the original
image (Fig.4a).
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Fig. 4. The results of T1-BEA (a) Original image (b) 3-labeled gray image with
background (label 0) as black, scalp and brain (label 1) as white and skull (label 2) as gray.
(c) Rough brain portion (d) Brain mask produced by morphological operations: erosion
and dilation, and connected component analysis (e) Extracted brain
2.2 Stage-2: Generation of Boundary between LCH and RCH
The aim of this stage is to identify a boundary between the cerebral
hemispheres. The boundary surface between the hemispheres lies in IHF. The
following expert knowledge are used to trace the boundary surface between
cerebral hemispheres.
1. Intensity information of CSF: The IHF is filled with CSF and CSF
voxels should therefore be good candidates to form boundary surfaces.
2. Spatial information: The IHF, known as longitudinal fissure, divides
the brain in the middle in lengthwise and approximately appears as a
line between the hemispheres
Since each CSF voxel lies between two GM surfaces (falx cerebri) in the IHF
the boundary is strongly affected by partial volume effect (PVE). So the
boundary surface may not be correctly determined using the CSF intensity
information. Hence the shape of boundary is treated as a line and our algorithm is
aimed to generate this line that corresponds to MSL.
A knowledge system is proposed to detect the edges of the IHF present in the
extracted brain. In each 2D axial slice, a mark, MU is made at the nadir of the
upper portion of cleft and another mark ML is fixed at the zenith of the lower
portion of cleft as shown in Fig.5. Then a line, MSL is generated by joining these
two marks MU and ML.
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Fig. 5. Brain with ideal MSL and Proposed MSL
Table 1. The description and general assumption of proposed knowledge system used to
detect the edges of IHF.
�o. Description General
Assumption
For upper edge
(MU)
For lower edge
(ML)
1 Search /
State Space
Within the bounded
rectangle of the
extracted brain
where W is the width
and H is the height
of the rectangle
x∈ [1, H/4]
y∈ [4W/10,6W/10]
x ∈ [3H/4, H]
y∈ [4W/10, 6W/10]
2 Initial /
Start
State
The intersection
point of the initial
MSL (central
vertical line of
bounded rectangle)
and the brain contour
Upper point of
intersection
Lower point of
intersection
3 Goal
State
Two end points of
IHF
nadir of the upper
portion of cleft
zenith of the lower
portion of cleft
4 Rule Consider Cx, Px and
Nx are the x-
coordinates of the
current pixel,
previous pixel and
next pixel
IF
(Px≤Cx & Nx≥Cx)
then
Store the pixel as a
representative pixel
IF
(Px≥Cx & Nx≤Cx)
then
Store the pixel as a
representative pixel
Ideal MSL
MU on upper portion of cleft
Line that connects the marks MU
and ML of the cleft
(Proposed MSL)
ML on lower portion of cleft
Brain contour
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Fig. 6. The general assumption of knowledge system to detect the marks MU and ML of
cleft
The descriptions and assumptions of the proposed knowledge system are
given in Table 1 and in Fig.6. The proposed algorithm for the knowledge system
is as follows:
Steps of Searching Algorithm
1) Start the process from initial state (Table 1)
2) Do the search in the state space along the brain contour
3) For each pixel apply the rule and detect the representative pixels
4) Constructs a separate list of representative pixels of each edge,
i.e., MU-list and ML-list respectively
5) Sort the lists based on x-values of pixels in a descending order
for MU-list and ascending order for ML-list
6) Take the top most pixels as edge points (MU and ML) in each sorted list
respectively.
Special Case: If successive pixels are present at the beginning of the
sorted list then the median pixel will be taken as the edge pixel.
7) Stop the process
The line that connects the MU and ML is corresponding to the boundary line
as shown in Fig.5.
Initial state for MU
Search space for MU Brain Contour
Vertical Central Line of Bounded Rectangle
Bounded rectangle of brain
Initial state for ML
Search space for ML
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2.3 Stage-3: Slice Transformation to standard space
The detected MSL is used to transform the MRI scans to the ideal world co-
ordinates system. For the slice, shown in Fig.3a, the detected MSL (white) and
the 2D world co-ordinate system with slice centre as origin (light gray) are shown
in Fig.5. The detected MSL can be used to compute the required transformation
that maps the MSL to the ideal MSP. The mapping procedure (M) to move from
the imaging coordinates (IC) to world coordinates (WC) is given by:
MWC, IC = R(90-θ) . T(d) (1)
where T is the translation matrix to map the origin of two coordinate systems, R
is the rotation matrix that align the MSL with ideal MSP, d is the distance along
the horizontal axis and θ, the angle of deviation of MSL about the horizontal axis.
The value (90-θ) gives the required rotation angle to fix the MSL with the vertical
axis (ref. Fig.7). The angle θ is calculated as:
θ = tan -1
(m) (2)
where m is the slope of MSL. Fig.7b shows the transformed image shown in of
Fig.7a that makes the MSL to perfectly coincide with the ideal MSP. This is the
required preprocessing step for image registration and spatial normalization
processes in brain imaging pipelines.
Fig. 7. (a) MR scan with detected MSL (in bright color) and world coordinate (in light
gray color) (b) Transformed image with coordinates θ and d
The transformation to world co-ordinate system made to the sample image
(Fig.3a) is shown in Fig.8. The rotated image given in Fig.8c is the final
d
θ 90-θ
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transformed image to standard space that makes the detected MSL coincides with
the ideal MSL.
Fig. 8. (a) Sample image given in Fig.3a with standard space (gray lines) and detected
MSL (white line) (b) Translated image along the horizontal axis (c) Rotated about the
vertical axis
The brain portions appearing on both sides of central line of transformed
image correspond to the two cerebral hemispheres. Using the ideal MSL
generated by the above procedure, the cerebral hemispheres are separated and are
shown in Fig.9.
Fig. 9. Cerebral Hemispheres separated by MSL. (a) Hemisphere at the left side (b)
Hemisphere at the right side
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2.4 Evaluation parameters
Both qualitative and quantitative validations are considered for the
performance evaluation. The qualitative evaluation is simply the visual inspection
of the result done by four experts of the field. The quantitative evaluation based
on sensitivity (S), specificity (Sp) and predictive accuracy (PA) as given in
equations (3)-(5), are performed between hand-drawn brain regions, hemispheres
by the experts and the respective portions produced by our proposed methods.
These parameters are used to measure the performance of the algorithm against
the manual extraction. The sensitivity (S) is the percentage of region of interest
(ROI) voxels recognized by the algorithm and specificity (Sp) is the percentage
of non-ROI voxels recognized by the algorithm using the True Positive (TP),
False Positive (FP), True Negative (TN) and False Negative (FN) values
extracted by an algorithm. Here ROI is either brain or cerebral hemispheres. The
predictive accuracy (PA) is the percentage of both ROI and non-ROI regions
recognized by the proposed method. TP and FP are the total number of pixels
correctly and incorrectly classified as ROI by the automated algorithm. TN and
FN are defined as the total pixels correctly and incorrectly classified as non-ROI
tissue by the automated algorithm.
S = F"TP
TP
+
, (3)
Sp = FPT"
T"
+
, (4)
PA = 100 × F"FPT"TP
T"TP
+++
+ . (5)
3 Materials
We used 40 real MRI volumes of both normal and abnormal subjects for our
experiments. These 3D volumes with anisotropic nature of voxel dimension are
available as a stack of 2D slices. Low contrast and intensity inhomogenity scans
were present with some volumes. Few volumes were affected either by wrap
around artifact or by zipper artifact.
Fifteen subjects of MRI head scans were collected from KGS Advanced MR
and CT Scans, Madurai, Tamilnadu, India. For each subject, scans were taken in
the entire three orientations using1.5T Siemens machine.
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Another fifteen T1 test volumes were obtained from Brain Extraction
Evaluation (BEE) web service maintained by the International Neuroimaging
Consortium (INC), University of Minnesota (ftp://neurovia.umn.edu/pub/BEE).
These T1 subjects were acquired on a Siemens 1.5T scanner using 3D FLASH
with FOV 165×220 mm, matrix 192×256 and voxel dimensions
0.86×0.86×1.0 mm.
Ten datasets of normal and abnormal subjects including brain tumor
(Neoplastic disease) and multiple sclerosis taken from ‘The Whole Brain Atlas’
provided by the Department of Radiology and Neurology at Brigham and
Women’s Hospital, Harvard Medical School, The Library of Medicine and the
American Academy of Neurology
(http://www.med.harvard.edu/AANLIB/home.html). The dimension of each of
volume is 256×256 pixels and slice thickness varying from 2-5mm with 260mm
field of view. So the pixel dimension is fitted to 1×1 mm.
4 Results and Discussions
Our segmentation method was initially tested on few 2D normal and
abnormal axial slices that were chosen from real brain volumes collected from
MRI scan centres and websites. Both qualitative and quantitative evaluations are
done for validating our method. The results obtained are given in Fig.10. They
were inspected and appreciated by medical experts. Our method not only
separates the cerebral hemispheres but also removes the unwanted non brain
regions appearing around the hemispheres. Therefore our method will be useful
for further processing like tissue segmentation, image compression, registration
and bilaterally symmetry analysis procedures.
Ten sample slices are selected from our material pool for the quantitative
evaluation. The Reason for selecting these slices is that these slices have different
characteristics like type, size, contrast, location, position and pathology. The
parameter values in addition to clinical and other descriptions about the ten
chosen slices are given in Table 2. In case of sensitivity and specificity, the
values greater than 98% shows that our method produces the acceptable results
and even comparable to manual segmentation. The predictive accuracy is 99% in
normal cases and lowered for abnormal slices. This algorithm was applied on
more than 100 slices including some normal and abnormal brain volumes. The
results are almost the same on normal slices (ref. slice number 1 in Table 2)
whereas in some abnormal slices the hand-drawn IHF is deviated from our mid-
sagittal line. This variation is also noticeable from the result of slice number 5
and 8 of Table 2 that are lower than other values. The visual effect of the slice 5
and 8 is given in column 3 and 6 of Fig. 10. The single mass effect in the right
side pushes the IHF towards the left side and hence the IHF has a curve effect and
deviated from the MSL.
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Fig. 10. Sample scans selected from MR T1 and T2 brain volumes are given in row 1, the
brain extraction results and separated hemispheres of respective scans are shown in
column wise in row 2, row 3 and row 4.
Our method worked successfully on several normal and abnormal 2D slices.
The success of our algorithm depends on two factors. The primary one is related
to the accuracy of BEA. If the BEA failed to extract the brain portion clearly,
especially with the clefts, then the proposed procedure failed. But this will
happen only for very low contrast images and images with severe artifacts. Both
of our BEAs are developed for 2-D and 3-D spaces and produces acceptable
results for all orientations. Our BEAs successfully removed all the non-brain
regions including the imaging clutters automatically as shown in column 3 and
column 6 of Fig.10. This is considered to be one of the important merits of our
BEA algorithms. The second factor is concerned with the search space for the
MSL edges. It is actually approximated near the middle vertical line at each slice.
If the head is tilted much during the scanning time then the cleft portions will be
far away from the middle vertical line and it will not be captured correctly. Hence
we have to either increase the search space or use some other scheme to select the
initial line other than middle vertical line. But the broad head tilting occurs only
for patients who are not fit for MRI screening.
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Table 2. Quantitative evaluation of ten sample slices made between hand-drawn portions
done by an expert and portions produced by the proposed method
Slice
�o.
Type
Size
Clinical
and other
Description
Region
Sensitivity
(S)
Specificity
(Sp)
Predictive
Accuracy
(PA)
1 t2
scan 256x256 Normal
Brain 0.9880 0.9976 99.47
LCH 0.9930 0.9957 99.53
RCH 0.9614 0.9998 99.38
2 t2
scan 256x256
Glioma –
grade IV
astrocytoma
Brain 0.9738 0.9885 98.37
LCH 0.9601 0.9940 98.80
RCH 0.9656 0.9955 99.02
3 t2
scan 256x256
Glioma –
anaplastic
astrocytoma
Brain 0.9906 0.9920 99.16
LCH 0.9843 0.9942 99.28
RCH 0.9770 0.9987 99.56
4 t2
scan 256x256 Sarcoma
Brain 0.9923 0.9913 99.17
LCH 0.9812 0.9948 99.23
RCH 0.9840 0.9974 99.47
5 t2
scan 256x256
Mass effect
and
background
clutter
Brain 0.9859 0.9916 98.96
LCH 0.9313 0.9947 98.39
RCH 0.9767 0.9885 98.63
6 t1
scan 256x256 Mass effect
Brain 0.9819 0.9998 99.53
LCH 0.9838 0.9992 99.72
RCH 0.9590 1 99.49
7 t1
scan 256x256
Glioma –
gadolium
contrasted
Brain 0.9915 0.9937 99.31
LCH 0.9903 0.9926 99.23
RCH 0.9496 0.9976 99.06
8 t1
scan 512x512
Mass effect
and
background
clutter
Brain 0.9906 0.9961 99.40
LCH 0.9317 0.9984 98.56
RCH 0.9937 0.9871 98.84
9 t1
scan 500x383 Mass effect
Brain 0.9892 0.9935 99.13
LCH 0.9834 0.9869 98.60
RCH 0.9588 0.9978 98.70
10 t1
scan 148x127
Mass effect
and
low
contrast
image
Brain 0.9903 0.9414 96.31
LCH 0.9887 0.9763 97.91
RCH 0.9713 0.9817 97.94
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This method could be extended to 3D brain volumes. The proposed method
produces the MSL with the help of edges of cleft presents with the 2D slices. The
clefts at each 2D slices are more visible with the upper portions of 3D volume.
Hence the MSLs produced by upper slices could be useful for producing MSP of
any 3D brain volume. We can obtain more accurate results for 3D volume by
comparing the results of BEA and edges of MSL between adjacent slices. In
some abnormal volume the IHF is deviated from MSP due to swelling of
hemisphere. To overcome such situations, MSL could be used as initial line for
energy minimization procedure like active contour methods, to trace the shape of
inter-hemispheral membrane. Studies are underway extending this 2D approach
to generate MSP and to extract the shape of IHF for 3D brain volumes.
Acknowledgments
The authors wish to thank Dr. K.G. Srinivasan M.D., R.D., Consultant
Radiologist, KGS Advanced MR & CT Scan, Madurai, Tamilnadu, India and Dr.
N. Karunakaran DMRD., DNB., Consultant – Radiodiagnosis and Dr. S. P.
Salome Pritha, Department of Radiology, Meenakshi Mission Hospital and
Research Centre, Madurai, Tamilnadu, India for providing the MR Head scans
and for obtaining the qualitative as well as quantitative validation. The authors
would also wish to thank Dr. K. Selvamuthukumaran M.Ch. (Neuro), Sr.
Consultant, Department of Neuro Surgery, Meenakshi Mission Hospital and
Research Centre, Madurai, Tamilnadu, India and
Dr.S.P.Balachandran,M.D.,D.M.,(Neuro), Neurologist, Dindigul Neuro Centre,
Dindigul District, Tamilnadu, India for their help in verifying the results.
This work is catalysed and funded by Science and Society Divisions,
Department of Science and Technology, Government of India, Grant number:
SP/YO/011/2007.
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