Purpose: To propose a transition region extraction algorithm for two point fat-water separation.
Methods:In the proposed method, fat-water transition region is first extracted as initial information. Remaining pixels are determined based on transition region in units of sub-region instead of pixels to improve calculation efficiency and avoid the vulnerability to the growing path.
Results:Fat-water separation were successfully achieved by the proposed method in the datasets tested.
Conclusion: A method based on fat-water transition region extraction is proposed for two point fat-water separation.
The analytical phasor solutions could be obtained in two point fat-water imaging [1]. Fat-water separation problem can be then translated into a binary choice problem between the two candidate solutions [2]. Resolving the ambiguity is possible when the fat ratio in a pixel approximates 50% as long as the echo time difference (ΔTE) induced fat-water phase difference is not kπ [3]. Traditional region growing methods usually starts from identifying these “seed pixels”, and solves the rest pixels by region-growing method [3] [4].
In our implementation, we made two major modifications to the traditional region-growing methods. First, the algorithm starts with a fat-water transition region extraction instead of seed pixels. Fat-water transition region is defined as where the water-dominant and fat-dominant pixels are neighbors. The extraction procedure is explained as follows:
The two candidate phasor solutions for each pixel are categorized into two groups: $$$P_w$$$ and $$$P_f$$$ . The solution corresponding to water-dominant result are grouped in $$$P_w$$$ , while fat-dominant in $$$P_f$$$ . Supposing water-dominant pixel 1 and fat-dominant pixel 2 are neighbors with the identical phasor $$$P_t$$$ . For pixel 1, the aliased phasor solution $$$P_a=P_t v^{*}$$$ , while for pixel 2 $$$P_a=P_t v$$$ , where $$$v =e^{i 2\pi f_{F}\Delta TE}$$$ . Once the angle of $$$v$$$ is unequal to $$$k \pi$$$ ( $$$k$$$ is an arbitrary integer), the true solution pair is the smoothest among all four possible combinations (Figure 1). For this kind of pixel pair, there exists a sudden phasor change ( $$$\angle v$$$ ) in both $$$P_w$$$ and $$$P_f$$$ . In order to identify these pixels, the local phasor change for pixel r is defined as:
$$$D_{i}(r)=\max_k{|angle[P_{i}(r)\cdot P_i^*(r_k)]|}$$$ $$$i = w,f$$$ (1)
where K denotes the index of 8-neighborhood in 2D image, $$$(.)^{*}$$$ is the conjugate operator. As long as $$$D_w$$$ or $$$D_f$$$ is larger than $$$\alpha*\angle v$$$, this pixel would be identified as transition region pixel.
Second, the remaining pixels are determined in units of sub-regions after the extraction of these transition regions. Solutions of pixel in one sub-region are either all from $$$P_w$$$ or all from $$$P_f$$$. The determination is based on the cost function defined as:
$$$c_{i}=\sum_J{|\angle(P_{i}(s_j)\cdot P_i^*(t_j))|}$$$ $$$i = w,f$$$ (2)
where $$$J$$$ denotes all neighboring pixel pairs between current sub-region $$$S$$$ and the neighboring solved transition region $$$T$$$ . $$$s_j\in S$$$ and $$$t_j\in T$$$ . The solution resulting in smaller cost function is considered as true solution for the sub-region.
Flowchart of proposed method is illustrated in Fig.2. $$$P_w$$$ and $$$P_f$$$ (Fig.2B) are calculated using the equations given in ref.[1]. The fat-water transition region (Fig.2C) is extracted from the image and the rest pixels (Fig.2D) are divided into several sub-regions. The cost function of each sub-regions are calculated according to Eq.(2). Having determined the phasor solutions of all sub-regions (Fig.2E), the transition region pixels, along with other undermined pixels, are updated with region growing schemes[5] (Fig.2F). Once the phasor solutions of the whole image are decided, fat and water component could be determined accordingly (Fig.2G).
Proposed method is tested on datasets acquired from a 3T system (uMR 770, Shanghai United Imaging Healthcare, Shanghai, China) in various anatomies. Acquisition parameters are as following: flip angle $$$10^{。}$$$, slice thickness 3 mm, bandwidth 1100 Hz/pixel, TE = 2.3/3.16 ms corresponding to 0 and $$$3\pi/4$$$ fat-water phase difference at 3T, TR = 9.35 ms.
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