preprint-to be submitted Imrpoving Strain Estimation in Breast Ultrasound Images Using Novel 1.5D Approach Simulation

2025-04-26 0 0 5.37MB 6 页 10玖币
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preprint-to be submitted
Imrpoving Strain Estimation in Breast Ultrasound
Images Using Novel 1.5D Approach (Simulation
and In-vivo results)
Irteza Enan Kabir
Electrical and Computer Engineering
University of Rochester
NY, United States
irtezaenan@gmail.com
Abstract—Ultrasound elastography is the method to image the
elasticity of compliant tissues due to a mechanical compression
applied to it. In elastography, the local strain of explored tissue
is estimated by analyzing the echo signals. This is accomplished
by a sonographer who uses ultrasound transducer to apply
pressure on the tissue area causing displacement of the tissue.
A set of data is obtained before and after the compression. This
stress along the axial direction not only causes deformation in
that direction but it can also cause lateral deformation in the
tissue. This relative deformation is later calculated using tracking
algorithms. Finally, estimating the elasticity, images are formed.
In this paper, we introduce a novel strain estimator. The proposed
1.5D strain estimator uses 1D windows for swift computations
and searches the lateral direction for taking the non-axial
movement into account. We have investigated the performance
of our estimator using simulated and in-vivo data of breast
tissue. The performance of our method is verified by comparing
with different methods up to 16% applied strain. The proposed
estimator has exhibited a superior performance compared to the
conventional methods. The image quality significantly improves,
especially in the presence of higher applied strain, when the non-
axial motion is significant.
Keywords—Correlation, Elastography, Elasticity Adaptive
stretching, Maximum-correlation, Stress, Strain, Breast, Pros-
trate, Ultrasound
I. INTRODUCTION
Ultrasound imaging has emerged with tremendous potential
as an imaging modality for the distinction of pathological
changes in tissue. Numerous applications have been explored
since it was first proposed for cancer imaging more than two
decades ago. It is emerging due to the fact that breast cancer
is the second most fatal cancer among women worldwide [1].
An estimation indicates that, in USA, around 246,660 cases
of breast cancer was found in 2016, which accounts for 29%
of all the new cancer diagnoses [2]. Another estimation states
that 40,610 death cases were found in 2017 alone [3].
The needs of efficiently diagnosing cancer yields the ne-
cessity of elastography algorithms. Imaging tissue elasticity
parameters has rapidly drawn attention for its capability to
produce new noninvasive and in vivo information. The idea
of examining the mechanical properties of tissue is not new.
Clinicians have been using palpation for detecting lumps since
400 BC. But due to rapid improvement of medical imag-
ing technologies, high resolution imaging is now available,
which has triggered clinical trials in many areas. Currently
ultrasound imaging is widely utilized for prostrate, breast,
liver, thyroid applications, etc. [4], [5]. Existence prediction
and visualization of the behavior of tissue when subjected to
mechanical force is performed in the form of elastography [6].
Elastograms usually contain information not present in sono-
grams, which mainly gives information on acoustic scattering
properties. In elasticity imaging, echo signals are acquired
before and after the external pressure applied to the surface
by an operator using ultrasound transducer. Strain is calculated
from this pre and post compression echoes by using different
algorithms. The algorithms may calculate strain directly [7] or
it may be gradient based strain estimation [8]. Gradient based
estimators calculate strain from the gradient of displacement.
It relies on computing the displacement from the time delays
between gated pre and post-compression echo segments [9].
The location of the maximum peak of the cross-correlation
gives the estimation of time shift. Gradient based techniques
are vulnerable to noise. As a result of tissue compression,
decorrelation noise is present as a major source of estimation
error. Post-compression signals are not exact delayed versions
of the pre-compression signals. Thus, decorrelation noise
occurs which increases with higher applied strains. Noises
of high frequencies are generally amplified by the gradient
based estimators due to the fact the original signals are also
of high frequencies [10]. Direct strain estimators on the
other hand calculate strain directly from the echo segments of
pre and post-compression in time domain [11] or frequency
domain [12]. The techniques are based on stretching the post-
compression signal to correlate with the pre-compression or
shifting the pre-compression signal before the computation of
cross-correlation. Strain images with higher SNR compared to
gradient based approach can be found by these methods. As
no gradient operation is involved in the process, these methods
don’t suffer from noise amplification problems associated with
gradient based methods.
978-1-6654-9106–8/22/$31.00 © 2022 IEEE
arXiv:2210.06677v1 [eess.IV] 13 Oct 2022
Fig. 1: Lateral shift due pressure applied in the axial direction.
II. METHOD
The proposed 1.5D strain estimation method was applied
on the conventional strain estimator, which calculates gradient
of estimated displacements (no stretching) and on the adaptive
stretching estimator that uses the stretch factor as an estimator
of the strain. The method consists of two main steps:
a. Finding the lateral shift of the post-compression signal
segments and the strain map.
b. Finding the strain values to compute the strain map.
A. Finding the lateral shift of the post-compression signal
segments
Pre-compression echo signals are segmented into overlap-
ping 1D windows, in a single column. This segment from pre-
compression signal is correlated with several neighboring post-
compression data segments. For example, a segment from pre-
compression ith data stream is correlated with the correspond-
ing segments of (i-n) th to (i+n) th post-compression columns
or data streams (Value of n can be varied. We have chosen n=6
for our computation). For each post-compression segment, the
maximum correlation is calculated yielding (2n+1) correlation
values. We then calculate which among the (2n+1) values is
the highest. If the ith pre-compression data line segment has
the highest correlation with the (i+j) th post-compression data
segment, it means that the tissue deformation took place in
such a way that the corresponding post-compression segment
has shifted +j columns. This lateral movement found for one
segment is also used for the following segments to predict
lateral movement adaptively which makes the algorithm com-
putation efficient
Fig. 2: Lateral motion estimation using correlation analysis of
a gated pre-compression data segment with several neighbor-
ing post-compression data segments.
While doing correlation analysis for finding lateral move-
ment, a slightly different approach is exercised. For the
correlation between a pre and a post window, the windows
are further divided into sub windows. Sub-windows from pre
are correlated with corresponding sub windows of post, each
time providing a maximum correlation value. When all the sub
window analysis is complete for a pair of windows, the median
value among the maximums provided by the small segments
is taken. This helps to avoid getting a false correlation peak.
Even if one sub window provides a false peak, the chance of
getting the true peak is high due to the approach.
B. Finding the strain values to compute the strain map
Fig. 3: Finding out appropriate stretch factor from Correlation
Coefficient peaks.
In gradient based estimator, strain is calculated from the
difference of displacements between two consecutive signal
segments. In time domain, the lags between segment of pre
and corresponding segment from post give the displacement.
By sliding the pre and post-compression windows, the dis-
placement map is computed for each of the pre-compression
window we considered earlier. The strain is then calculated
from the gradient of these displacements. Significant amount
of noise is associated with the gradient method. The selection
of window size and overlap between windows can affect the
amount of noise introduced [13]. Small window size and large
overlap introduces more noise in the strain estimation. But
overlap around 90% can give strain images with high axial
resolution [14]. Keeping this trade-off in mind, we have used
a 3mm data window size and a window shift of 0.5mm.
In adaptive stretching method, stretch factor itself gives
an estimation of strain. Post-compression signal segment is
stretched for matching best with the pre-compression coun-
terpart signal segment. For different stretching factor αi ,
similarity measure is calculated by means of cross-correlation
(CC). Suppose, in figure 3, for three different stretch factors,
we get three different peaks and “Peak 2” is maximum among
all three peaks. Then strain will be calculated from α2 as
follows,
Strain = 1- α2
摘要:

preprint-tobesubmittedImrpovingStrainEstimationinBreastUltrasoundImagesUsingNovel1.5DApproach(SimulationandIn-vivoresults)IrtezaEnanKabirElectricalandComputerEngineeringUniversityofRochesterNY,UnitedStatesirtezaenan@gmail.comAbstract—Ultrasoundelastographyisthemethodtoimagetheelasticityofcompliantti...

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