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作者(中文):黃祥鴻
作者(外文):Huang, Hsiang-Hung
論文名稱(中文):螺旋超穎材料之負折射與旋光性之研究
論文名稱(外文):Study on the negative index and optical activity of helix metamaterials
指導教授(中文):洪毓玨
指導教授(外文):Hung, Yu-Cheuh
口試委員(中文):何榮銘
嚴大任
口試委員(外文):Ho, Rong-Ming
Yen, Ta-Jen
學位類別:碩士
校院名稱:國立清華大學
系所名稱:光電工程研究所
學號:101066525
出版年(民國):103
畢業學年度:102
語文別:英文
論文頁數:61
中文關鍵詞:超穎材料掌性介質負折射旋光性光二色性
外文關鍵詞:metamaterialchiral medianegative index materialoptical activitycircular dichroism
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Chiral metamaterials refer to metamaterials consisting of gyrotropic inclusions that do not
have a superposable mirror image. Because of the extraordinary optical activity (OA) and
circular dichroism (CD) phenomena, it has been suggested that chiral negative index meta-
materials (chiral NIMs) can provide a new route for constructing a superlens that goes
beyond the diffraction limit. The plasmonic-enhanced circular dichroism, on the other hand,
has also been evaluated as a crucial key in bio-chemistry to boost the sensitivity of CD-
spectroscopy to dissect complex biomolecules, such as proteins. In this regard, there has
been an increasing interest in studying chiral metamaterials. In this thesis, we investigated,
designed, and simulated the chiral metamaterials based on the intertwined gold helices, ded-
icating to construct negative index materials and high transmission and large rotary power
devices through finite-difference time domain (FDTD) method. By employing the effective
parameter retrieval technique, a four-intertwined helix combined with metallic wire griddings
that reached NIM was proposed. The NIM exhibited the maximum figure of merit (FOM,
−Re{n}/Im{n}) of 0.5 under normal incidence at 24.72 THz for the LCP wave. Incorporat-
ing the simulations with genetic algorithm (GA), we designed 4 polarization rotators with
maximum rotary power 105.24 (0/λ)and extremely high transmittance (average above 80%)
at the communication wavelength of 1.55 micrometer. These results show that helix-based devices
serve as potential candidates for future optoelectronic applications.
Chiral metamaterials refer to metamaterials consisting of gyrotropic inclusions that do not
have a superposable mirror image. Because of the extraordinary optical activity (OA) and
circular dichroism (CD) phenomena, it has been suggested that chiral negative index meta-
materials (chiral NIMs) can provide a new route for constructing a superlens that goes
beyond the diffraction limit. The plasmonic-enhanced circular dichroism, on the other hand,
has also been evaluated as a crucial key in bio-chemistry to boost the sensitivity of CD-
spectroscopy to dissect complex biomolecules, such as proteins. In this regard, there has
been an increasing interest in studying chiral metamaterials. In this thesis, we investigated,
designed, and simulated the chiral metamaterials based on the intertwined gold helices, ded-
icating to construct negative index materials and high transmission and large rotary power
devices through finite-difference time domain (FDTD) method. By employing the effective
parameter retrieval technique, a four-intertwined helix combined with metallic wire griddings
that reached NIM was proposed. The NIM exhibited the maximum figure of merit (FOM,
−Re{n}/Im{n}) of 0.5 under normal incidence at 24.72 THz for the LCP wave. Incorporat-
ing the simulations with genetic algorithm (GA), we designed 4 polarization rotators with
maximum rotary power 105.24 (0/λ)and extremely high transmittance (average above 80%)
at the communication wavelength of 1.55 micrometer. These results show that helix-based devices
serve as potential candidates for future optoelectronic applications.
Abstract

contents
1. Introduction
1.1 Development of Metamaterials
1.2 Chiral Metamaterials
1.3 Helix Metamaterials
1.4 Motivation

2. Fundamentals and Methods
2.1 Simulation Method and Material Model
2.1.1 Finite-Difference Time Domain method
2.1.2 Optical Properties of Materials
2.2 Negative Index Material
2.2.1 Negative Refractive Phenomenon
2.2.2 Diffraction Limit and NIM Perfect Lens
2.3 Genetic Algorithm
2.4 Bi-isotropic Media and Effective Medium Theory
2.4.1 Bi-isotropic Media
2.4.2 The Significance of Chirality Index κ
2.4.3 Effective Medium Theory
2.4.4 Validity of Effective Medium Theory
2.5 Optical Activity and Circular Dichroism for CMM
2.5.1 Born-Kuhn Model
2.5.2 One Electron Model

3 Parameter Retrieval and Negative Index Based on Helix Metamaterials
3.1 The 4-intertwined Helix and Method
3.2 Results and Discussion

4 Large Optical Activity and High Transmission Based on Helix Metamaterials
4.1 Method
4.2 Results
4.3 Discussion

5 Conclusions

Bibliography
[1] Y. Liu and X. Zhang, “Metamaterials: a new frontier of science and technology,” Chemical Society Reviews 40, 2494–2507 (2011).
[2] R. A. Shelby, D. R. Smith, and S. Schultz, “Experimental verification of a negative index of refraction,” Science 292, 77–79 (2001).
[3] D. Schurig, J. Mock, B. Justice, S. Cummer, J. Pendry, A. Starr, and D. Smith, “Metamaterial electromagnetic cloak at microwave frequencies,” Science 314, 977–980 (2006).
[4] S. Zhang, Y.-S. Park, J. Li, X. Lu, W. Zhang, and X. Zhang, “Negative refractive index in chiral metamaterials,” Physical review letters 102, 023901 (2009).
[5] M. Decker, R. Zhao, C. Soukoulis, S. Linden, and M. Wegener, “Twisted split-ring resonator photonic metamaterial with huge optical activity,” Optics letters 35, 1593–1595 (2010).
[6] J. K. Gansel, M. Wegener, S. Burger, and S. Linden, “Gold helix photonic metamaterials: a numerical parameter study,” Opt. Express 18, 1059–1069 (2010).
[7] J. K. Gansel, M. Thiel, M. S. Rill, M. Decker, K. Bade, V. Saile, G. von Freymann, S. Linden, and M. Wegener, “Gold helix photonic metamaterial as broadband circular polarizer,” Science 325, 1513–1515 (2009).
[8] K. Yee, “Numerical solution of initial boundary value problems involving maxwell’s equations in isotropic media,” Antennas and Propagation, IEEE Transactions on 14, 302–307 (1966).
[9] P. B. Johnson and R. W. Christy, “Optical constants of the noble metals,” Physical Review B 6, 4370 (1972).
[10] A. Vial, A.-S. Grimault, D. Mac´ ıas, D. Barchiesi, and M. L. de La Chapelle, “Improved
analytical fit of gold dispersion: Application to the modeling of extinction spectra with a finite-difference time-domain method,” Physical Review B 71, 85416 (2005).
[11] W. Cai and V. M.ˇSalaev, Optical metamaterials: fundamentals and applications (Springer, 2010).
[12] X. Zhang and Z. Liu, “Superlenses to overcome the diffraction limit,” Nature materials 7, 435–441 (2008).
[13] X. Yin, M. Schäferling, B. Metzger, and H. Giessen, “Interpreting chiral spectra: The plasmonic born-kuhn model,” Nano letters (2013).
[14] V. G. Veselago, “The electrodynamics of substances with simultaneously negative values of ϵ and µ,” Physics-Uspekhi 10, 509–514 (1968).
[15] G. Thompson, “Unusual waveguide characteristics associated with the apparent negative permeability obtainable in ferrites,” (1955).
[16] A. Hartstein, E. Burstein, A. Maradudin, R. Brewer, and R. Wallis, “Surface polaritons on semi-infinite gyromagnetic media,” Journal of Physics C: Solid State Physics 6, 1266 (1973).
[17] W. Rotman, “Plasma simulation by artificial dielectrics and parallel-plate media,” Antennas and Propagation, IRE Transactions on 10, 82–95 (1962).
[18] J. Pendry, A. Holden, D. Robbins, and W. Stewart, “Low frequency plasmons in thin-wire structures,” Journal of Physics: Condensed Matter 10, 4785 (1998).
[19] J. B. Pendry, A. J. Holden, D. Robbins, and W. Stewart, “Magnetism from conductors and enhanced nonlinear phenomena,” Microwave Theory and Techniques, IEEE Transactions on 47, 2075–2084 (1999).
[20] D. R. Smith, W. J. Padilla, D. Vier, S. C. Nemat-Nasser, and S. Schultz, “Composite medium with simultaneously negative permeability and permittivity,” Physical review letters 84, 4184 (2000).
[21] J. B. Pendry, D. Schurig, and D. R. Smith, “Controlling electromagnetic fields,” Science 312, 1780–1782 (2006).
[22] U. Leonhardt and T. G. Philbin, “General relativity in electrical engineering,” New Journal of Physics 8, 247 (2006).
[23] M. Wegener and S. Linden, “Shaping optical space with metamaterials,” Physics Today 63, 32 (2010).
[24] S. Tretyakov, I. Nefedov, A. Sihvola, S. Maslovski, and C. Simovski, “Waves and energy in chiral nihility,” Journal of electromagnetic waves and applications 17, 695–706 (2003).
[25] J. Pendry, “A chiral route to negative refraction,” Science 306, 1353–1355 (2004).
[26] I. V. Lindell, A. Sihvola, S. Tretyakov, and A. Viitanen, Electromagnetic waves in chiral and bi-isotropic media (Artech House, 1994).
[27] B. Wang, J. Zhou, T. Koschny, M. Kafesaki, and C. M. Soukoulis, “Chiral metamaterials: simulations and experiments,” Journal of Optics A: Pure and Applied Optics 11, 114003 (2009).
[28] Y. Tang and A. E. Cohen, “Enhanced enantioselectivity in excitation of chiral molecules by superchiral light,” Science 332, 333–336 (2011).
[29] Y. Tang, L. Sun, and A. E. Cohen, “Chiroptical hot spots in twisted nanowire plasmonic oscillators,” Applied Physics Letters 102, 043103–043103 (2013).
[30] M. Schäferling, D. Dregely, M. Hentschel, and H. Giessen, “Tailoring enhanced optical chirality: Design principles for chiral plasmonic nanostructures,” Physical Review X 2, 031010 (2012).
[31] E. Hendry, R. Mikhaylovskiy, L. Barron, M. Kadodwala, and T. Davis, “Chiral electro-magnetic fields generated by arrays of nanoslits,” Nano letters 12, 3640–3644 (2012).
[32] A. Garc´ ıa-Etxarri and J. A. Dionne, “Surface-enhanced circular dichroism spectroscopy mediated by nonchiral nanoantennas,” Physical Review B 87, 235409 (2013).
[33] L. D. Barron, Molecular light scattering and optical activity (Cambridge University Press, 2004).
[34] J. D. Kraus and R. J. Marhefka, Antennas: For All Applications (McGraw-Hill, 2003).
[35] Z. Yang, M. Zhao, and P. Lu, “How to improve the signal-to-noise ratio for circular polarizers consisting of helical metamaterials?” Opt. Express 19, 4255–4260 (2011).
[36] Z. Yang, M. Zhao, and P. Lu, “A numerical study on helix nanowire metamaterials as optical circular polarizers in the visible region,” Photonics Technology Letters, IEEE 22, 1303–1305 (2010).
[37] Z. Yang, M. Zhao, P. Lu, and Y. Lu, “Ultrabroadband optical circular polarizers consisting of double-helical nanowire structures,” Optics letters 35, 2588–2590 (2010).
[38] L. Wu, Z. Yang, M. Zhao, Y. Yu, S. Li, Q. Zhang, and X. Yuan, “Polarization characteristics of the metallic structure with elliptically helical metamaterials,” Optics express 19, 17539–17545 (2011).
[39] S. Li, Z. Yang, J. Wang, and M. Zhao, “Broadband terahertz circular polarizers with single-and double-helical array metamaterials,” JOSA A 28, 19–23 (2011).
[40] Y. Yu, Z. Yang, S. Li, and M. Zhao, “Higher extinction ratio circular polarizers with hetero-structured double-helical metamaterials,” Optics Express 19, 10886–10894 (2011).
[41] Y. Yu, Z. Yang, M. Zhao, and P. Lu, “Broadband optical circular polarizers in the terahertz region using helical metamaterials,” Journal of Optics 13, 055104 (2011).
[42] Z. Yang and M. Zhao, “How to improve the S/N ratio of the circular polarizer with single-helical metamaterials?” (2012).
[43] L. Wu, Z. Yang, M. Zhao, P. Zhang, Z. Lu, Y. Yu, S. Li, and X. Yuan, “What makes single-helical metamaterials generate pure circularly polarized light?” Optics Express 20, 1552–1560 (2012).
[44] Z. Zhao, D. Gao, C. Bao, X. Zhou, T. Lu, and L. Chen, “High extinction ratio circular polarizer with conical double-helical metamaterials,” Journal of Lightwave Technology 30, 2442–2446 (2012).
[45] J. K. Gansel, M. Latzel, A. Frolich, J. Kaschke, M. Thiel, and M. Wegener, “Tapered gold-helix metamaterials as improved circular polarizers,” Applied Physics Letters 100, 101109–101109 (2012).

[46] V. A. Fedotov, M. Rose, S. L. Prosvirnin, N. Papasimakis, and N. I. Zheludev, “Sharp trapped-mode resonances in planar metamaterials with a broken structural symmetry,” Phys. Rev. Lett. 99, 147401 (2007).
[47] C. K. Ullal, M. Maldovan, M. Wohlgemuth, E. L. Thomas, C. A. White, and S. Yang,“Triply periodic bicontinuous structures through interference lithography: a level-set approach,” JOSA A 20, 948–954 (2003).
[48] D. B. Burckel, J. R. Wendt, G. A. Ten Eyck, J. C. Ginn, A. R. Ellis, I. Brener, and M. B. Sinclair, “Micrometer-scale cubic unit cell 3d metamaterial layers,” Advanced Materials 22, 5053–5057 (2010).
[49] Lumerical Solutions, Inc. http://www.lumerical.com/tcadproducts/fdtd/.
[50] D. J. Griffiths and R. College, Introduction to electrodynamics, vol. 3 (prentice Hall Upper Saddle River, NJ, 1999).
[51] J. B. Pendry, “Negative refraction makes a perfect lens,” Physical review letters 85, 3966 (2000).
[52] J. W. Goodman, Introduction to Fourier optics (Roberts and Company Publishers, 2005).
[53] S. G. Lipson, Optical physics (Cambridge University Press, 1995).
[54] R. L. Haupt and D. H. Werner, Genetic Algorithms in Electromagnetics (Wiley, 2007).
[55] R. Zhao, T. Koschny, and C. M. Soukoulis, “Chiral metamaterials: retrieval of the effective parameters with and without substrate,” Optics Express 18, 14553–14567 (2010).
[56] S. Bassiri, C. Papas, and N. Engheta, “Electromagnetic wave propagation through a dielectric-chiral interface and through a chiral slab,” Journal of the Optical Society of America A 5, 1450–1459 (1988).
[57] C. A. Kyriazidou, H. Contopanagos, W. M. Merrill, and N. Alexpoulos, “Artificial versus
natural crystals: effective wave impedance of printed photonic bandgap materials,” Antennas and Propagation, IEEE Transactions on 48, 95–106 (2000).
[58] X. Chen, T. M. Grzegorczyk, B.-I. Wu, J. Pacheco Jr, and J. A. Kong, “Robust method to retrieve the constitutive effective parameters of metamaterials,” Physical Review E 70, 016608 (2004).
[59] T. Koschny, P. Markoˇ s, D. Smith, and C. Soukoulis, “Resonant and antiresonant frequency dependence of the effective parameters of metamaterials,” Physical Review E 68, 065602 (2003).
[60] H. Liu, Y. Liu, T. Li, S. Wang, S. Zhu, and X. Zhang, “Coupled magnetic plasmons in metamaterials,” Physica Status Solidi B 246, 1397–1406 (2009).
[61] Y. P. Svirko and N. Zheludev, Polarization of light in nonlinear optics (Wiley, 2000).
[62] J. A. Schellman, “Symmetry rules for optical rotation,” Accounts of chemical research 1, 144–151 (1968).
[63] S. A. Maier, Plasmonics: fundamentals and applications (Springer, 2007).
[64] N. Liu and H. Giessen, “Coupling effects in optical metamaterials,” Angewandte Chemie International Edition 49, 9838–9852 (2010).
[65] Y. Svirko, N. Zheludev, and M. Osipov, “Layered chiral metallic microstructures with inductive coupling,” Applied physics letters 78, 498–500 (2001).
[66] E. Condon, “Theories of optical rotatory power,” Reviews of modern physics 9, 432 (1937).
[67] J. Kaschke, J. K. Gansel, and M. Wegener, “On metamaterial circular polarizers based on metal n-helices,” Optics express 20, 26012–26020 (2012).
[68] C. Menzel, T. Paul, C. Rockstuhl, T. Pertsch, S. Tretyakov, and F. Lederer, “Validity of effective material parameters for optical fishnet metamaterials,” Physical Review B 81, 035320 (2010).
[69] Z. Li, K. B. Alici, H. Caglayan, M. Kafesaki, C. M. Soukoulis, and E. Ozbay, “Composite chiral metamaterials with negative refractive index and high values of the figure of merit,” Opt. Express 20, 6146–6156 (2012).
[70] C. Xu and J. Dong, “Negative refractive index in non-resonance spectrum area,” Chinese Optics Letters 8, 1067–1070 (2010).
[71] J. Valentine, S. Zhang, T. Zentgraf, E. Ulin-Avila, D. A. Genov, G. Bartal, and X. Zhang, “Three-dimensional optical metamaterial with a negative refractive index,” nature 455, 376–379 (2008).
[72] P. Tassin, L. Zhang, T. Koschny, E. Economou, and C. Soukoulis, “Low-loss metamaterials based on classical electromagnetically induced transparency,” Physical review letters 102, 053901 (2009).
[73] J. Aizpurua, G. W. Bryant, L. J. Richter, F. G. De Abajo, B. K. Kelley, and T. Mallouk, “Optical properties of coupled metallic nanorods for field-enhanced spectroscopy,” Physical Review B 71, 235420 (2005).
[74] A. Rogacheva, V. Fedotov, A. Schwanecke, and N. Zheludev, “Giant gyrotropy due to electromagnetic-field coupling in a bilayered chiral structure,” Physical review letters 97, 177401 (2006).
[75] E. Plum, J. Zhou, J. Dong, V. Fedotov, T. Koschny, C. Soukoulis, and N. Zheludev,“Metamaterial with negative index due to chirality,” Physical Review B 79, 035407 (2009).
[76] H. Liu, D. Genov, D. Wu, Y. Liu, Z. Liu, C. Sun, S. Zhu, and X. Zhang, “Magnetic plasmon hybridization and optical activity at optical frequencies in metallic nanostructures,” Physical review B 76, 073101 (2007).
[77] J. Zhou, D. R. Chowdhury, R. Zhao, A. K. Azad, H.-T. Chen, C. M. Soukoulis, A. J. Taylor, and J. F. OHara, “Terahertz chiral metamaterials with giant and dynamically tunable optical activity,” Phys. Rev. B 86, 035448 (2012).
[78] M. Decker, M. Ruther, C. Kriegler, J. Zhou, C. Soukoulis, S. Linden, and M. Wegener,“Strong optical activity from twisted-cross photonic metamaterials,” Optics letters 34, 2501–2503 (2009).
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