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采用时域微波断层成像技术进行早期乳腺癌检测能够准确地获得乳房的电参数分布, 具有明确的物理解释和医学诊断价值. 临床应用讲究即时性, 为了提高检测的速度, 本文将交替隐式有限差分法应用到乳腺癌检测中, 基于正反演时间步进成像算法进行成像分析, 结果显示在保证精度的前提下, 采用交替隐式有限差分法的成像时间可缩短为传统时域有限差分法的23%, 提高了微波断层成像技术的临床可应用性.
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关键词:
- 微波断层成像 /
- 交替隐式时域有限差分法 /
- 乳腺癌
In microwave tomography (MWT), electric-parameter distributions of the breast can be reconstructed to detect the early-breast-cancer, which has a specific physical explanation and medical diagnostic value. In time-domain, the finite-difference time-domain (FDTD) method is usually applied to these problems. However, due to the constraint of Courant-Friedrich-Levy (CFL) stability condition, the time step should be small enough to well match the small fine cells, which begets an increasing computational cost, such as the central processing unit (CPU) time. For real-time clinical, it is very important and essential to look for efficient methods to improve the computational efficiency. The alternating-direction implicit finite-difference time-domain (ADI-FDTD) method, on the other hand, provides a larger time step than that the CFL stability condition limitation could set. In order to shorten the time of imaging and improve the detection efficiency, the ADI-FDTD method is first used for the early-breast-cancer detection in this paper. MWT for breast cancer detection requires solving nonlinear inverse scattering problems. Most nonlinear inversion algorithms require solving a number of forward scattering problems followed by an optimization procedure. Therefore, we turn the inverse scattering problem into an optimization question according to the least squares criterion. The optimization procedure aims at minimizing the error between measured scattered fields and estimated scattered fields by the forward solver. Nonlinear reconstruction algorithm is used to solve an update for the scattering object properties used in our breast model. This iteration process is repeated until the convergence between the measured and estimated data is obtained. The specific process of the iteration method is divided into two steps: the forward step, which is to solve a forward problem for a scattering object with estimated electrical properties, and the backward step, which is to solve adjoint fields by introducing the Lagrange multiplier penalty function. Both the forward and backward calculations are conducted by using the ADI-FDTD method. The algorithm is evaluated for a two-dimensional (2D) semicircle breast model with tumors. We compare the imaging results obtained by the ADI-FDTD method for various time steps with the results obtained by the conventional FDTD method and the real distribution. The results agree well, the simulation results prove that the imaging time by using this ADI-FDTD method can be reduced to 23% that by the conventional FDTD method. In addition, the simulation results suggest that the ADI-FDTD method can be more efficient if higher resolution is required, thus further enhancing the clinical applicability of MWT.-
Keywords:
- microwave tomography /
- alternating direction implicit finite-difference time-domain /
- breast cancer
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[10] Miyakawa M, Ishida T, Watanabe M 2004 26th annual International Conference of the IEEE Engineering in Medicine and Biology Society San Francisco, California, September 1-5, 2004 p1427
[11] Andreas F, Parham H, Mikael P 2006 IEEE Trans. Biomed. Eng. 53 1594
[12] Johnson J E, Takashi T, Toshiyuki T 2008 IEEE Trans. Biomed. Eng. 55 1941
[13] Gustafsson M, He S 1999 Math. Comput. Simulat. Math. 50 541
[14] Gustafsson M, He S 2000 Radio Sci. 35 525
[15] Gustafsson M 2000 Ph. D. Dissertation (Sweden Lund: Lund University)
[16] Takenaka T, Tanaka T, Harada H, He S 1998 Microw. Opt. Techn. Lett. 16 292
[17] Takenaka T, Jia H, Tanaka T 2000 J. Electromagnet. Wave. 14 1609
[18] Takenaka T, Zhou H, Tanaka T 2003 J. Opt. Soc. Am. A 20 1867
[19] Rekanos I T, RIsNen A 2003 IEEE Trans. Magn. 39 1381
[20] Rekanos I T 2003 J. Electromagnet. Wave. 17 271
[21] Liu G D, Zhang Y R 2010 Acta Phys. Sin. 59 6969 (in Chinese) [刘广东, 张业荣 2010 59 6969]
[22] Liu G D, Zhang Y R 2010 Chin. J. Radio 25 1175 (in Chinese) [刘广东, 张业荣 2010 电波科学学报 25 1175]
[23] Namiki T 1999 IEEE Trans. Microwave. Theory Techn. 47 2003
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[1] Siegel R, Ma J, Zou Z H, Jemal A 2014 Ca-Cancer J. Clin. 64 9
[2] Ahmedin J, Rebecca S, Xu J, Elizabeth W 2010 Ca-Cancer J. Clin. 60 277
[3] Smith-Bindman R, Chu P, Miglioretti D L, Quale C, Rosenberg R D, Cutter G, Geller B, Bacchetti P, Sickles E A, Kerlikowske K 2005 J. Natl. Cancer I. 97 358
[4] Guo B 2007 Ph. D. Dissertation (USA Florida: Florida University)
[5] Hagness S C, Taflove A, Bridges J E 1998 IEEE Trans. Biomed. Eng. 45 1470
[6] Fear E C, Stuchly M A 1999 IEEE Microwave. Guided Wave Lett. 9 470
[7] Rubaek T, Meaney P, Meincke P, Paulsen K D 2007 IEEE Trans. Antennas Propag. 55 2320
[8] Meaney P M, Fanning M W, Li D, Poplack S P 2000 IEEE Trans. Microwave Theory Techn. 48 1841
[9] Bindu G N, Abraham S J, Lonappan A, Thomas V, Aanandan C K, Mathew K T 2006 Prog. Electromagn. Res. 58 149
[10] Miyakawa M, Ishida T, Watanabe M 2004 26th annual International Conference of the IEEE Engineering in Medicine and Biology Society San Francisco, California, September 1-5, 2004 p1427
[11] Andreas F, Parham H, Mikael P 2006 IEEE Trans. Biomed. Eng. 53 1594
[12] Johnson J E, Takashi T, Toshiyuki T 2008 IEEE Trans. Biomed. Eng. 55 1941
[13] Gustafsson M, He S 1999 Math. Comput. Simulat. Math. 50 541
[14] Gustafsson M, He S 2000 Radio Sci. 35 525
[15] Gustafsson M 2000 Ph. D. Dissertation (Sweden Lund: Lund University)
[16] Takenaka T, Tanaka T, Harada H, He S 1998 Microw. Opt. Techn. Lett. 16 292
[17] Takenaka T, Jia H, Tanaka T 2000 J. Electromagnet. Wave. 14 1609
[18] Takenaka T, Zhou H, Tanaka T 2003 J. Opt. Soc. Am. A 20 1867
[19] Rekanos I T, RIsNen A 2003 IEEE Trans. Magn. 39 1381
[20] Rekanos I T 2003 J. Electromagnet. Wave. 17 271
[21] Liu G D, Zhang Y R 2010 Acta Phys. Sin. 59 6969 (in Chinese) [刘广东, 张业荣 2010 59 6969]
[22] Liu G D, Zhang Y R 2010 Chin. J. Radio 25 1175 (in Chinese) [刘广东, 张业荣 2010 电波科学学报 25 1175]
[23] Namiki T 1999 IEEE Trans. Microwave. Theory Techn. 47 2003
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