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  1. NTU Theses and Dissertations Repository
  2. 電機資訊學院
  3. 光電工程學研究所
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/56699
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor曾雪峰(Snow H. Tseng)
dc.contributor.authorShuai-Hsun Leeen
dc.contributor.author李帥勳zh_TW
dc.date.accessioned2021-06-16T05:42:57Z-
dc.date.available2014-08-17
dc.date.copyright2014-08-17
dc.date.issued2014
dc.date.submitted2014-08-11
dc.identifier.citation[1] Yee, K.S., 'Numerical solution of initial boundary value problems involving Maxwell's equations in isotropic media,' IEEE Transaction on Antennas and Propagation. AP 14: p. 302.
[2] Berenger, J.P., 'A perfectly matched layer for the absorption of electromagnetic waves,' J. Computational Physics. 114: p. 185-200, 1996.
[3] Engquist, B. and A. Majda, 'Absorbing boundary conditions for the numerical simulation of waves,' Mathematics of Computation. 311: p. 629-651, 1997.
[4] Mur, G., 'Absorbing boundary conditions for the finite-difference approximation of the time-domain electromagnetic field equations,' IEEE Trans. Electromagn. Compat. 23: p. 377-382, 1981.
[5] Berenger, J.P., 'Improved PML for the FDTD solution of wave-structure interaction problems,' IEEE Trans. Antennas Propagat. 45: p. 466-473, 1997.
[6] Sullivan, D.M., 'A simplified PML for use with the FDTD method,' IEEE Microwave Guided Wave Lett. 6(97-99, 1996).
[7] Sacks, Z.S., et al., 'A perfectly matched anisotropic absorber for use as an absorbing boundary condition,' IEEE Trans. Antennas Propagat. 43: p. 1460-1463, 1995.
[8] Gedney, S.D., 'An anisotropic PML absorbing media for FDTD simulation of fields in lossy dispersive media,' Electromagnetics. 16: p. 399-415, 1996.
[9] Mberloose, D., J., and M.A. Stuchley, 'Reflection analysis of PML ABC's for low-frequency applications,' IEEE Microwave Guided Wave Lett. 6: p. 177-179, 1996.
[10] Berenger, J.P., 'Numerical reflection of evanescent waves from perfectly matched layers,' IEEE Antennas Propagat. 3: p. 1888-1891, 1997.
[11] Roden, J.A., 'Convolutional PML (CPML): An efficient FDTD implementation of the CFS-PMLs,' Microwave Optical Tech. Lett. 27: p. 334-339, 2000.
[12] Teixeira, F.L., et al., 'Perfectly matched layer and piecewise-linear recursive convolution for the FDTD solution of the 3D dispersive half-space problem,' IEEE Trans. Magnetics. 34: p. 2747-2750, 1998.
[13] Berenger, J.P., 'Numerical reflection from FDTD PMLs: A comparison of the split PML with unsplit and CFS PMLs,' IEEE Trans. Antennas Propagat. 50: p. 258-265, 2002.
[14] Zhao, A.P., 'Generalized-material -independent PML absorbers used for the FDTD simulation of electromagnetic waves in 3D arbitrary anisotorpic and magnetic media,' IEEE Trans. Microwave Theory Tech. 46: p. 1511-1513, 1998.
[15] Chew, W.C. and W.H. Weedon, 'A 3D perfectly matched medium from modified Maxwell's equations with stretched coordinates,' IEEE Microwave Guided Wave Lett. 7: p. 599-604, 1994.
[16] Lau, Y.C., M.S. Leong, and P.S. Kooi, 'Extension of Berenger's PML boundary condition in matching lossy medium and evanescent waves,' Electronics Lett. 32: p. 974-976, 1996.
[17] Fang, J. and Z. Wu, 'Generalized perfectly matched layer for the absorption of propagating and evanescent waves in lossless and lossy media,' IEEE Trans. Microwave Theory Tech. 14: p. 2216-2222, 1996.
[18] Taflove, A. and S.C. Hagness, 'Computational electrodynamics the Finite-Difference Time-Domain Method,' Boston:ARTECH HOUSE, 2005.
[19] Namiki, T. and K. Ito, 'Investigation of numerical errors of the two-dimensional ADI-FDTD method,' IEEE Trans. Microwave Theory Tech. 48: p. 1950-1956, 2000.
[20] Taflove, A. and M.E. Brodwin, 'Numerical-solution of steady-state electromagnetic scattering problems using time-domain Maxwell's equations,' IEEE Transaction on Microwave Theory and Techniques. 23: p. 623-630.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/56699-
dc.description.abstract吸收邊界條件最初廣泛的應用在模擬邊界的吸收以避免誤差來自邊界的反射,本篇論文中,利用有限差分時域法(FDTD),以摺積完美匹配層(CPML)的基本概念去創造出圓形的光學靶,並且分析其解析度對應所造成的誤差及不同頻率對應的吸收效率,光源將使用高斯光束、環形高斯分佈場來分析其吸收效率,最後的結果得出吸收效率與解析度有關,但和頻率無關。
由於電磁波在如生物組織等強散射介質中,造成電磁波從四面八方而來,利用圓形光學吸收體的特性,能夠有效的吸收各方向的入射光,以應用在模擬光學現象在生物組織中的情形。
zh_TW
dc.description.abstractAbsorbing boundary conditions (ABCs) are widely used for boundary absorbing which can reduce the error from the boundary reflection in simulation space. In the thesis, we explore and analyze the absorption of a convolutional perfectly matched layer (CPML) optical target under the condition of different resolutions, and different frequencies Gaussian beam source in the Finite-Difference Time-Domain (FDTD) simulations. We show the performance of CPML optical target that eliminates the impinging wave and analyze the absorption efficiency of CPML optical target with different resolutions and the influence by different frequencies source. Specific simulation results show that the absorption of the CPML optical target is dependent upon its resolution, but independent upon the source frequency. In turbid media such as biological tissue, electromagnetic (EM) wave would be scattered strongly so that makes the light come from any direction possibly. By using the optical target to absorb the impinging wave from arbitrary direction, we can model light propagation through biological tissue to a specific target posistion.en
dc.description.provenanceMade available in DSpace on 2021-06-16T05:42:57Z (GMT). No. of bitstreams: 1
ntu-103-R01941076-1.pdf: 2745976 bytes, checksum: 55b99b8b6d147a58fc9381ae47147814 (MD5)
Previous issue date: 2014
en
dc.description.tableofcontents誌謝 I
中文摘要 III
Abstract IV
CONTENTS V
LIST OF FIGURES VII
Chapter 1. Introduction of optical absorber 1
1.1 FDTD simulation of optical target 1
1.2 Application of optical target 2
1.3 Outline 3
Chapter 2. Introduction of the FDTD Method 5
2.1 Central difference scheme 5
2.2 FDTD algorithm 8
2.3 Numerical dispersion and Stability 16
2.4 Error analysis 20
Chapter 3. Introduction of the components used in the simulation 27
3.1 Hard-source, soft-source and the total-field/scattered-field (TF/SF) technique 27
3.2 Perfectly matched layer (PML) absorbing boundary conditions 37
Chapter 4. Simulation structure 45
4.1 Simulation structure of creating source 45
4.2 Simulation structure of CPML optical target 50
Chapter 5 Simulation results 53
5.1 Validation of Gaussian beam 53
5.2 Validation of CPML optical target 57
Chapter 6 Conclusion and future prospects 71
6.1 Conclusion 71
6.2 Future prospects 72
REFERENCE 74
dc.language.isoen
dc.subject光學吸收體zh_TW
dc.subject摺積完美吸收邊界zh_TW
dc.subject有限時域差分法zh_TW
dc.subjectoptical targeten
dc.subjectCPMLen
dc.subjectFDTDen
dc.title使用有限差分時域法模擬分析光學吸收體zh_TW
dc.titleFDTD simulation analysis of the CPML optical targeten
dc.typeThesis
dc.date.schoolyear102-2
dc.description.degree碩士
dc.contributor.oralexamcommittee江衍偉(Yean-Woei Kiang),張世慧(Shih-Hui Chang)
dc.subject.keyword光學吸收體,摺積完美吸收邊界,有限時域差分法,zh_TW
dc.subject.keywordoptical target,CPML,FDTD,en
dc.relation.page75
dc.rights.note有償授權
dc.date.accepted2014-08-12
dc.contributor.author-college電機資訊學院zh_TW
dc.contributor.author-dept光電工程學研究所zh_TW
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