Abstract:Let I : → be a given bounded image function, where is an open and bounded domain which belongs to n . Let us consider n = 2 for the purpose of illustration. Also, let S = {x i } i ∈ be a finite set of given points. We would like to find a contour ⊂ , such that is an object boundary interpolating the points from S. We combine the ideas of the geodesic active contour (cf. Caselles et al. [7,8]) and of interpolation of points (cf. Zhao et al. [40]) in a level set approach developed by Osher and Sethian [33]. We p… Show more
“…We addressed this problem by using the mean magnitude of the electric fields in the charged fluid system. The magnitude of E equ in (12) was modified as (18) where | · |is the magnitude of E equ , 〈 · 〉 is the mean magnitude of E equ on all fluid elements for each charged fluid, and max(·, ·) is the greater of the two values. Therefore, the electric strength of weak fluid elements was increased such that the magnitude of the overall electric field in the charged fluid systemwas uniform, which makes the CFM more robust in segmenting noisy images.…”
Section: Mean Electric Fieldmentioning
confidence: 99%
“…Recently, Xu et al [17] proposed a level-set-based segmentation method that uses an adaptive triangular mesh to achieve higher resolution at the interface. Gout et al [18] proposed a segmentation approach that combines the idea of the geodesic active contour and interpolation of points in the Osher-Sethian level set framework to find a boundary contour from a finite set of given points.…”
In this paper, we developed a new deformable model, the charged fluid model (CFM), that uses the simulation of a charged fluid to segment anatomic structures in magnetic resonance (MR) images of the brain. Conceptually, the charged fluid behaves like a liquid such that it flows through and around different obstacles. The simulation evolves in two steps governed by Poisson's equation. The first step distributes the elements of the charged fluid within the propagating interface until an electrostatic equilibrium is achieved. The second step advances the propagating front of the charged fluid such that it deforms into a new shape in response to the image gradient. This approach required no prior knowledge of anatomic structures, required the use of only one parameter, and provided subpixel precision in the region of interest. We demonstrated the performance of this new algorithm in the segmentation of anatomic structures on simulated and real brain MR images of different subjects. The CFM was compared to the levelset-based methods [Caselles et al. (1993) and Malladi et al. (1995)] in segmenting difficult objects in a variety of brain MR images. The experimental results in different types of MR images indicate that the CFM algorithm achieves good segmentation results and is of potential value in brain image processing applications.
“…We addressed this problem by using the mean magnitude of the electric fields in the charged fluid system. The magnitude of E equ in (12) was modified as (18) where | · |is the magnitude of E equ , 〈 · 〉 is the mean magnitude of E equ on all fluid elements for each charged fluid, and max(·, ·) is the greater of the two values. Therefore, the electric strength of weak fluid elements was increased such that the magnitude of the overall electric field in the charged fluid systemwas uniform, which makes the CFM more robust in segmenting noisy images.…”
Section: Mean Electric Fieldmentioning
confidence: 99%
“…Recently, Xu et al [17] proposed a level-set-based segmentation method that uses an adaptive triangular mesh to achieve higher resolution at the interface. Gout et al [18] proposed a segmentation approach that combines the idea of the geodesic active contour and interpolation of points in the Osher-Sethian level set framework to find a boundary contour from a finite set of given points.…”
In this paper, we developed a new deformable model, the charged fluid model (CFM), that uses the simulation of a charged fluid to segment anatomic structures in magnetic resonance (MR) images of the brain. Conceptually, the charged fluid behaves like a liquid such that it flows through and around different obstacles. The simulation evolves in two steps governed by Poisson's equation. The first step distributes the elements of the charged fluid within the propagating interface until an electrostatic equilibrium is achieved. The second step advances the propagating front of the charged fluid such that it deforms into a new shape in response to the image gradient. This approach required no prior knowledge of anatomic structures, required the use of only one parameter, and provided subpixel precision in the region of interest. We demonstrated the performance of this new algorithm in the segmentation of anatomic structures on simulated and real brain MR images of different subjects. The CFM was compared to the levelset-based methods [Caselles et al. (1993) and Malladi et al. (1995)] in segmenting difficult objects in a variety of brain MR images. The experimental results in different types of MR images indicate that the CFM algorithm achieves good segmentation results and is of potential value in brain image processing applications.
“…Figure 11͑a͒ shows that there is one CFM initialized in a free plane. The four fluid elements having equal charge 14 Experimental results in segmenting an object with sharp corners and cusps using  = −1.2 in a 256ϫ 256 phantom image. Note that the object has a wide intensity distribution that is similar to the background.…”
Section: Initialization and Front Propagationmentioning
confidence: 99%
“…This approach introduces another term into the partial differential equation to balance the speed functions such that the propagating interface can more flexibly evolve toward the desired position. Recently, Gout et al 14 proposed a segmentation approach that combines the idea of the geodesic active contour and interpolation of points in the Osher-Sethian level set framework to find a boundary contour from a finite set of given points. Guyader et al 15 used the Osher-Sethian level set to evolve an explicit function, while minimizing the energy.…”
“…It was adapted from the level set paradigm [9], and was proposed to segment contours "without edges" [1]. In [10], a solution combining the geodesic active contour approach and interpolation constraints is provided to improve the convergence of level sets in the case where the image is noisy and the contours are not well defined. The main weakness of this method is that the a priori knowledge of interpolation points is required, so that the method is not entirely blind.…”
In real-world conditions, contours are most often blurred in digital images because of acquisition conditions such as movement, light transmission environment, and defocus. Among image segmentation methods, Hough transform requires a computational load which increases with the number of noise pixels, level set methods also require a high computational load, and some other methods assume that the contours are one-pixel wide. For the first time, we retrieve the characteristics of multiple possibly concentric blurred circles. We face correlated noise environment, to get closer to real-world conditions. For this, we model a blurred circle by a few parameters-center coordinates, radius, and spread-which characterize its mean position and gray level variations. We derive the signal model which results from signal generation on circular antenna. Linear antennas provide the center coordinates. To retrieve the circle radii, we adapt the second-order statistics TLS-ESPRIT method for non-correlated noise environment, and propose a novel version of TLS-ESPRIT based on higher-order statistics for correlated noise environment. Then, we derive a least-squares criterion and propose an alternating least-squares algorithm to retrieve simultaneously all spread values of concentric circles. Experiments performed on hand-made and realworld images show that the proposed methods outperform the Hough transform and a level set method dedicated to blurred contours in terms of computational load. Moreover, the proposed model and optimization method provide the information of the contour grey level variations.
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