uniform precision us imaging

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0885–3010/$25.00 ©  2009 IEEE 2420 IEEE TRANSACTIONS ON ULTRASONICS, FERROELECTRICS, AND FREQUENCY CONTROL, . 56, . 11, NOVEMBER 2009 Abstract—Ultrasound strain imaging is becoming increas- ingly popular as a way to measure stiness variation in soft tissue. Almost all techniques involve the estimation of a eld of relative displacements between measurements of tissue un- dergoing dierent deformations. These estimates are often high resolution, but some form of smoothing is required to in- crease the precision, either by direct ltering or as part of the gradient estimation process. Such methods generate uniform resolution  images, but strain quality typical ly varies consider- ably within each image, hence a trade-ois necessary between increasing precision in the low-quality regions and reducing resolution in the high-quality regions. We introduce a smooth- ing technique, developed from the nonparametric regression literature, which can avoid this trade-oby generating uniform precision  images. In such an image, high resolution is retained in areas of high strain quality but sacriced for the sake of increased precision in low-quality areas. We contrast the algo- rithm with other methods on simulated, phantom, and clinical data, for both 2-D and 3-D strain imaging. We also show how the technique can be eciently implemen ted at real-time rates with realistic parameters on mo dest hardware. Uniform preci- sion nonparametric regression promises to be a useful tool in ultrasound strain imaging. I. I I seems likely that some form of ultrasonic strain imag- ing will be adopted into routine clinical practice, within a decade, to support a still unestablished set of diagnostic tasks, primarily within the broad category of soft tissue examinations. Applications discussed in the academic lit- erature have included detection of soft tissue tumors [1]– [3], discrimination without biopsy between complex cysts and malignant breast lesions [4], monitoring of atheroscle- rosis [5], [6], detection and grading of deep vein thrombo- sis [7], assessment of skin pathologies [8] and evaluation of myocardial tness [9]. Currently, a variety of techniques exist for generating strain images using ultrasound, and it is not yet clear which of these techniques will be most appropriate for each of these applications. However, the majority of tech- niques involv e the lo cal estimation of tissue displacement by comparing radio frequency (RF) ultrasound data ac- quired at diering tissue deformation states. The tissue deformation can be induced in a variety of ways. In the remainder of this paper, we will focus on quasistatic ul- trasound strain imaging, where the tissue is deformed by varying the contact pressure between the probe and the skin surface. However, the algorithms we develop apply equally to other strain-imaging techniques. Many meth- ods have been proposed for displacement estimati on, e.g., [10]–[22]. Such methods typically produce high-resolution displacement estimates, howeve r, the measurement quali- ty can vary enormously across a single image, for instance, due to variation in signal strength or decorrelation caused by nonaxial movement. In quasistatic strain imaging, displacement estimation is followed by gradient estimation in the axial direction. Simple dierencing of consecutive samples [23] amplies the high-frequency components of the measurement noise. Hence, dierencing is often achieved by more complex techniques such as piecewise-linear least squares regres- sion (PLLSR) [24], moving-a verage ltering [17] and stag- gered strain estimation [25]. All such linear techniques can be interpreted as simple dierencing followed by ltering with xed kernel coecients. Indeed, we have previously shown that, except in the case where the entire data set genuinely consists of noisy measurements from a single linear trend (in which case PLLSR is the optimal lter), simple dierencing followed by ltering with a Gaussian- shaped kernel can achieve lower estimation noise than these methods at the same resolution [26]. Because both the displacement tracking and ltering techniques make use of kernels with xed size, subsequent strain images have xed resolution but variable quality. However, this variation can be quantied, because it is straightforw ard to obtain a reasonable estimate of the pre- cision (inverse of measurement variance) of each measure- ment [27]. Strain images require some form of normaliza- tion to convert the strain into a displayable range and to reduce variation that is simply a result of variation in the applied stress [28]. The precision of the displayed strain value depends both on the displacement estimation preci- sion and on the normalization value used at each point in the image. Both of these factors can vary within each im- age, leading to large variations in precision that can make strain images hard to interpret. To prevent confusion due to the display of low-precision strain data, images are often suppressed once the over- all precision falls below a xed threshold [29]. However, strain images with low overall precision can still contain high precision regions, and this is exploited by techniques that combine multiple images, using local strain precision information to ensure that the best data in each image contribute more to the nal result. Such data still contain regions of low precision, but these can be masked by use of a suitable color wash [28]. Uniform Precision Ultrasound Strain Imaging Graham M. Treece, Joel E. Lindop, Andrew H. Gee, and Richard W. Prager Manuscript received March 9, 2009; accepted August 5, 2009. This work was partially supported by Research Grant EP/E030882/1 from the EPSRC. Much of this work was performed while Graham Treece was supported by a Research Fellowship from the Royal Academy of Engi- neering/EPSRC. He is now partly supported by the Evelyn Trust. G. M. Treece, A. H. Gee, and R. W. Prager are with the Depart- ment of Engineering, University of Cambridge, Cambridge, UK (e-mail: [email protected]). J. E. Lindop is with New Energy Finance Ltd., London, UK. Digital Obje ct Identier 10.1109/TUFFC.2009.133 0

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