藉由多重表面電漿共振效應之高分子電光調變器

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邱進忠(Jin-Jung Chyou) 查詢紙本館藏

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機械工程學系

論文名稱

藉由多重表面電漿共振效應之高分子電光調變器
(Electro-optic polymer light modulators based on multiple surface plasmon resonance effects)

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摘要(中)

電光調變器效率的提昇，可藉由調變機制設計及適當選擇電光材料來達成。在論文中，提出兩種利用非線性電光有機高分子材料設計與製作的高效率電光調變器，分別利用耦合波導表面電漿波原理所設計的耦合波導表面電漿子電光調變器及利用最佳化波導層厚度提高兩個表面電漿波耦合程度，所設計的雙表面電漿共振電光調變器。這兩種高分子電光調變器，係利用經過電場極化後的非線性電光高分子材料特有之波克效應及膜層厚度最佳化，藉由稜鏡耦合入射光至高分子波導層，以產生耦合波導表面電漿共振或雙表面電漿共振，並透過外加電壓來動態調變電光高分子的折射率，以改變共振耦合程度，來調變反射光強。耦合波導表面電漿電光調變器之基本架構，係由高折射率稜鏡、金屬薄膜層、電光高分子層及薄金屬電極層所構成。在最佳化高分子膜層厚度，由菲比-泊若干涉效應產生之波導共振模態與薄金屬電極層與空氣層介面之表面電漿波相互耦合，產生一個較佳的調變效率。透過設計，我們發現此新型電光調變器可以利用較低的調變電壓操作，以達到高效率的目的。雙表面電漿共振耦合電光調變器之基本架構，係由高折射率稜鏡、金屬薄膜層、電光高分子層、薄金屬電極層及電光高分子緩衝層所構成。在電光高分子膜層厚度最佳化下，入射光在衰逝全反射架構下，於適當共振角下，將使上金屬薄膜層介面之短距離表面電漿共振與下金屬電極層介面之長距離表面電漿共振相互耦合，以提高反射光場調變效率。由於光源在表面電漿共振型電光調變器內交互作用長度遠低於其他調變器，所以具有低損耗傳輸的優點。
本論文逐一討論電光調變器的基本組成、多層膜色散關係、高分子電光調變器之表面電漿共振應用原理、理論推導及模擬分析光調變器效率與電光高分子層厚度的關係。另製造表面電漿共振型電光調變器所必須量測之多層膜各膜層光學特性，可以直接藉由表面電漿共振角度探測技術及使用我們發展出來的改良式資料分析方法，快速決定各種膜層之折射係數與厚度。採用表面電漿共振角度探測技術，除了可以量測決定多層膜各膜層光學特性外，亦具有量測電光係數及調變效率的能力，故大幅簡化實驗程序。由於電光高分子層的製程簡單及相容於積體化電路的優點，故本文採用兩種電光高分子材料：一種為實驗室自行組合DANS-PMMA 電光高分子及另一種為之側鏈型發色團基之電光高分子。我們也應用前述原理，完成兩種有機高分子材料之耦合波導表面電漿共振的實驗。

摘要(英)

The improvement on the efficiency of electro-optic (EO) light modulator can be achieved by the optimal design of EO modulating mechanism and the proper selection of EO materials. In this dissertation, two novel high efficiency EO modulators based on multiple surface plasmon resonance (SPR) effects are presented. One of the proposed EO polymeric modulators is based on a novel design in which the degree of coupling of the collimating monochromatic beam into the coupled waveguide-surface plasmon resonance (CWSPR) is electrically varied in order to enhance the modulation efficiency of the device. The other is so called double surface plasmon resonance (DSPR) and based on increasing coupling effect between two surface plasmon resonances via the optimization of the waveguide layer thickness. Both of EO modulators employed the Pockels effect possessed by the poled nonlinear optical organic polymer (NLOP) and the optimization of the thickness of EO thin film. By applying voltage across EO polymer film to vary the refractive index of the EO polymer, the degree of coupling of CWSPR and DSPR is altered and the reflectivity is modulated. The CWSPR EO modulator consists of a high refractive index prism, a thin metal film, a poled polymer layer, and metal electrode. By optimizing the thickness of the EO polymer, the coupling effect of the SPR and the waveguide coupled resonance (WCR) which induced by the Fabry-Perot (F-P) interference within EO polymer can be enhanced. As a result, the CWSPR EO modulator is able to operate with less modulation voltage and achieves better modulation efficiency. The DSPR EO modulator consists of a high refractive index prism, a thin metal film, a poled polymer layer, thin metal electrode, and EO film. In the same way, by optimizing the EO polymer thickness, the coupling effect of the short-range surface plasmon resonance induced at top metal interface and the long-range surface plasmon resonance induced at bottom metal interface will be enhanced and the modulator then yields a better efficiency. The EO polymer light modulator based on SPR-related principles offer the advantage of less insertion loss due to its shorter interaction length.
This dissertation sequentially introduce the principles of SPR, the dispersion relation of multilayer system, the fundamentals of the modulator, the theoretical study and simulation concerning the relationship between the efficiency of modulator and the thickness of EO film. The determination of the refractive indexes and thicknesses for the various films, which is required for the fabrication of EO polymer modulator possessed with multilayer structure, can be achieved by employing the home-made SPR sensing technique and an improved data analysis method. In the similar approach, the SPR sensing technique is also capable of measuring the EO properties of the poled polymer film. This will greatly simplify experimental procedure. Since the NLOPs offer the advantages of having large EO constants, low dielectric constants, the simplicity to be fabricated, low cost, the diversity of synthesis and being compatible with integrated circuits, they are considered to be the most promising materials for the development of EO light modulator. Due to the aforementioned strengths offered by EO polymer, the EO polymers used in this project include two NLOP materials, one nonlinear optical organic polymer is a polymethyl methacrylate polymer (PMMA) side-chained with DANS (4, 4’-aminnonitroazobenzene) chromophore (DANS-PMMA) which synthesized and fabricated by our lab and the other is a side-chained EO polyimide with 2-(N-ethyl-4-(tricyanovinyl)anilino)ethanol chromophore. Based on using the foregoing principles, we have implemented two CWSPR EO modulators with these two NLOP materials. The modulators are characterized, and their performance is tested, in terms of the optical properties of the polymer thin film, the EO coefficient, the insertion loss, and the modulation index. Additionally, the dynamic response of the EO light modulator is also investigated and discussed.

關鍵字(中)

★ 生物分子交互作用分析(BIA)
★ 生物感測器
★ 電光調變器
★ 電光高分子
★ 耦合波導表面電漿共振(CWSPR)
★ 波導耦合共振（WCR）
★ 表面電漿共振(SPR)
★ 衰逝全反射(ATR)
★ 分子轉印高分子(MIP）
★ 多次實驗數據分析法

關鍵字(英)

★ Coupled waveguide-surface plasmon resonance (CWS
★ Waveguide coupled resonance (WCR)
★ Electro-optic polymer
★ Electro-optic modulator
★ Molecular imprinting polymer (MIP)
★ Biosensor
★ Biomolecular interaction analysis (BIA)
★ Multi-experiment data analysis
★ Surface p

論文目次

Abstract I
摘要 IV
Acknowledgements VI
Table of Contents VIII
List of Figures XI
List of Tables XX
Chapter 1 Introduction 1
1.1 General background 1
1.2 Motivation 3
1.3 Outline 8
Chapter 2 Principles 10
2.1 Surface plasmon resonance 10
2.1.1 Dispersion relation of a two-layer structure 16
2.1.2 Dispersion relation of a three-layer structure 25
2.1.3 Dispersion relation of a four-layer structure 30
2.2 Coupled waveguide-surface plasmon resonance 34
2.2.1 Waveguide theory 37
2.2.2 Coupled waveguide-surface plasmon resonance 40
2.3 Double surface plasmon resonance 45
2.4 Nonlinear optical susceptibility 49
2.4.1 EO nonlinearity 52
2.4.2 Non-centrosymmetric structure of nonlinear optical medium 54
2.4.3 EO effect 54
2.4.4 Anisotropic EO waveguide layer 56
2.5 Operation principles of EO light modulators 59
2.5.1 Performance index for EO light modulator 62
2.5.2 Optimal design for EO light modulator 62
2.6 Organic nonlinear optical polymer 70
Chapter 3 Fabrication 73
3.1 Fabrication of EO polymers 73
3.1.1 Guest-host type EO polyimide 73
3.1.2 EO polyimide with side-chain nonlinear optical moiety. 78
3.2 Poling 81
Chapter 4 Optical Properties of Thin Film 86
4.1 Improved analytic solution 88
4.2 Multi-experiment data analysis 92
4.3 Refractive index change for a N2-Ar exchange SPR experiment. 100
4.4 Optical properties of molecular imprinting polymer film 103
Chapter 5 Optical Metrology 106
5.1 Optical setup 106
5.2 EO modulation of the CWSPR modulator for guest-host system with gold electrode and DANS/PMMA polymer 108
5.3 EO modulation of the CWSPR modulator with gold electrode and side-chained polymer 110
5.3.1 Optical constants of EO polymer film 110
5.3.2 EO coefficient 111
5.3.3 Dynamic response 112
5.4 EO modulation of the CWSPR modulator with silver electrode and side-chained polymer 115
5.4.1 EO polymer thin-film fabrication 116
5.4.2 Poling process 117
5.4.3 Metrology 117
5.4.4 EO coefficient 118
5.4.5 Dynamic response 126
5.5 EO modulation of the DSPR modulator with silver electrode and side-chained polymer 128
5.5.1 EO polymer thin-film fabrication 129
5.5.2 Poling process 130
5.5.3 Metrology 130
Chapter 6 Conclusions 140
References 143
Publication List of Jin-Jung Chyou（邱進忠） 150
Vita Jin-Jung Chyou 152
Index 153

參考文獻

[1] J. M. Senior, Optical fiber communications: principles and practices, second ed., Prentice Hall: New York, 1992.
[2] K.-I. Suto, H. Yoshinaga, T. Kokubun, K. Kikushima, and E. Yoneda, “Intermodulation distortion in 48 TV channel FM-FDM optical transmission,” IEEE Photon. Technol. Lett. 3(9), 844-846 (1991).
[3] A. Billings, Optics optoelectronics and photonics engineering principles and applications, Prentice Hall: New York, 1993.
[4] R. G. Hunsperger, Photonic devices and systems, Marcel Dekker: New York, 1994.
[5] E. Uiga, Optoelectronics, Prentice Hall: Upper Saddle River, N.J., 270, 1995.
[6] C. C. Teng, “Traveling-wave polymeric optical intensity modulator with more than 40 GHz of 3-dB electrical bandwidth,” Appl. Phys. Lett. 60(13), 1538-1540 (1992).
[7] G. L. Li, and P. K. L. Yu, “Optical intensity modulators for digital and analog applications,” J. of Lightwave Technol. 21(9), 2010-2030 (2003).
[8] W. Wang, Y. Shi, D. J. Olson, W. Lin, and J. H Bechtel, “Push-pull poled polymer Mach-Zehnder modulators with a single microstrip line electrode,” IEEE Photon. Technol. Lett. 11(1), 51-53 (1999).
[9] J. Yang, Q. Zhou, X. Jiang, M. Wang, and R. T. Chen, “Polymer-based electrooptical circular-polarization modulator,” IEEE Photon. Technol. Lett. 16(1), 96-98 (2004).
[10] H. Raether, Surface plasmons on smooth and rough surfaces and on gratings, Springer-Verlag, Berlin, 4-13, 1988.
[11] G. T. Sincerbox and J. C. Gordon II, “Small fast large-aperture light modulator using attenuated total reflection,” Appl. Opt. 20(8), 1491-1494 (1981)
[12] O. Solgaard, F. Ho, J. I. Thackara, and D. M. Bloom, “High frequency attenuated total internal reflection light modulator,” Appl. Phys. Lett. 61(21), 2500-2502 (1992).
[13] D. Sarid, “Long-range surface-plasma waves on very thin metal films,” Phys. Rev. Lett. 47(26), 1927-1930 (1981).
[14] L. Wendler and R. Haupt, “Long-range surface plasmon-polaritons in asymmetric layer structures,” J. Appl. Phys. 59(9), 3289-3291 (1986).
[15] D. Sarid, R. T. Deck, A. E. Craig, R. K. Hickernell, R. S. Jameson, and J. J. Fasano, “Optical field enhancement by long-range surface plasma waves,” Appl. Opt. 21(22), 3993-3995 (1982)
[16] J. S. Schildkraut, “Long-range surface plasmon electrooptic modulator,” Appl. Opt. 27(21), 4587-4590 (1988).
[17] C. Jung, S. Yee, and K. Kuhn, “Electro-optic polymer light modulator based on surface plasmon resonance,” Appl. Opt. 34(6), 946-949 (1995).
[18] Y. Jiang, Z. Cao, G. Chen, X. Dou, and Y. Chen, “Low voltage electro-optic polymer light modulator using attenuated total internal reflection,” Opt. Laser Technol. 33, 417-420 (2001).
[19] S.-S. Sun, S. Maaref, E. Alam, Y. Wang, Z. Fan, M. Bahoura, P. Higgins, and C. E. Bonner, “Recent development of crosslinked NLO polymers for large bandwidth electro-optical modulations,” Proc. SPIE 4580, 297-308 (2001).
[20] J.-J. Chyou, C.-S. Chu, Z.-H. Shih, C.-Y. Lin, K.-T. Huang, S.-J. Chen, and S.-F. Shu, “High efficiency electro-optic polymer light modulator based on waveguide-coupled surface plasmon resonance,” Proc. SPIE 5221, 197-206 (2003).
[21] J. Davies, Surface analytical techniques for probing biomaterial processes, CRC press: Boca Raton, Chap. 3, 67-87, 1996.
[22] T.-A. Chen, Alex K.-Y, Jen, and Y. Cai, “Facile approach to nonlinear optical side-chain aromatic polymides with large second-order nonlinearity and thermal stability,” J. Am. Chem. Soc. 117, 7295-7296 (1995).
[23] T.-A. Chen, Alex K.–Y, Jen, and Y. Cai, “Two-step synthesis of side-chain aromatic polyimides for second-order nonlinear optics,” Macromolec. 29, 535-539 (1996).
[24] G. Khanarian, J. Sounik, D. Allen, S. F. Shu, C. Walton, H. Goldberg, and J. B. Stamatoff, “Electro-optic characterization of nonlinear-optical guest-host films and polymers,” J. Opt. Soc. Am. B 13(9), 1927-1934 (1996).
[25] R. F. Wallis and G. I. Stegeman, Electromagnetic Surface Excitations, Springer-Verlag: Berlin, 2-7, 1985.
[26] F. L. Pedrotti and L. S. Pedrotti, Introduction to Optics, Prentice-Hall: Englewood Cliffs, New Jersey, Chap. 23, 472-488, 1987.
[27] R. D. Guenther, Modern Optics, John Wiley and Sons: New York, 67-73, 1990.
[28] J. Homola, S. S. Yee, and G. Gauglitz, “Surface plasmon resonance sensors: review,” Sens. Actuators B 54, 3-15 (1999).
[29] H. Raether, “Surface plasma oscillations and their applications,” in Physics of Thin Films 9, Academic: New York, 145, 1977.
[30] K. Welford, “The method of attenuated total reflection,” in Surface plasmon-polaritations, IOP short meeting series 9, 25-99 (1988).
[31] E. N. Economou, “Surface plasmons in thin films,” Phy. Rev. 182(2), 539-554 (1969).
[32] J.-J. Chyou, S.-J. Chen, C.-S. Chu, Z.-H. Shih, C.-Y. Lin, and C.-F. Shu, “Fabrication and metrology of EO polymer light modulator based on waveguide-coupled surface plasmon resonance,” Opt. Eng. 44(3), 034001-1-034001-7 (2005).
[33] P. Yeh, Introduction to photorefractive nonlinear optics, John Wiley and Sons: New York, Chap. 12, 389, 1993.
[34] W. H. G. Horsthuis and G. J. M. Krijnen, “Simple measuring method for electro-optic coefficients in poled polymer waveguides” Appl. Phys. Lett., 55(7), 616-618 (1989).
[35] Y. Jiang, Z. Cao, Q. Shen, X. Dou, Y. Chen, “Improved attenuated-total-reflection technique for measuring the electro-optic coefficients of nonlinear optical polymers,” J. Opt. Soc. Am. B. 17(5), 805-808 (2000).
[36] D. Haas, H. Yoon, H.-T. Man, G. Cross, S. Mann, N. Parsons, “Polymeric electro-optic waveguide modulator; materials and fabrication,” Proc. SPIE 1147, 222-232 (1989).
[37] W. H. Steier, A. Chen, S.-S. Lee, S. Garner, H. Zhang, V. Chuyanov, L. R. Dalton, F. Wang, A. S. Ren, C. Zhang, G. Todorova, A. Harper, H. R. Fetterman, D. Chen, A. Udupa, D. Bhattacharya, and B. Tsap, “Polymer electro-optic devices for integrated optics,” Chem. Phys. 245, 487-506 (1999).
[38] V. Dentan, Y. Levy, M. Dumont, P. Robin and E. Chastaing, “Electrooptic properties of a ferroelectric polymer studied by attenuated total reflection,” Opt. Commun. 69(5,6), 379-383 (1989).
[39] C. C. Teng and H. T. Man, “Simple reflection technique for measuring the electro-optic coefficient of poled polymers,” Appl. Phys. Lett. 56(18), 1734-1736 (1990).
[40] S. Ducharme, J. Feinberg, and R. Neurgaonkar, “Electrooptic and piezoelectric measurements in photorefractive barium titanate and strontium barium niobate”, IEEE J. Quantum Electron. 23(12), 2116-2120 (1987).
[41] B. E. A, Saleh and M. C. Teich, Fundamentals of photonics, John Wiley and Sons: New York, Chap. 18, 699, 1991.
[42] E. V. Tomme, P. V. Daele, R. G. Baets, and P. E. Lagasse, “Integrated optic devices based on nonlinear optical polymers”, IEEE J. Quantum Electron. 27(3), 778-787 (1991).
[43] E. Kretschman and H. Raether, Z. Naturforsch., A: Phys. Sci. 23a, 2135-2136 (1968).
[44] Otto, Z. Phys. 216, 398-410(1968).
[45] A. Driessen, H. M. M. Klein Koerkamp, and Th. J. A. Popma, “Novel integrated optic intensity modulator based on mode coupling,” Fiber Integr. Opt. 13, 445-461 (1994).
[46] L. A. Hornak, Polymer for lightwave and Integrated optics: technology and appllications, Marcel-Dekker: New York, 280, 1992.
[47] D. M. Burland, R. D. Miller, and C. A. Walsh, “Second-order nonlinearity in poled-polymer system,” Chem. Rev. 94, 31-75 (1994).
[48] T. C. Kowalczyk, T. Z. Kosc, K. D. Singer, A. J. Beuhler, D. A. Wargowski, P. A. Cahill, C.H.Seager, M. B. Meinhardt, and S. Ermer, “Crosslinked polyimide electro-optic meaterials,” J. Appl. Phys. 78(10), 5876-5883 (1995).
[49] S.-S. Lee, S. M. Garner, V. Chuyanov, H. Zhang, W. H. Steier, F. Wang, L. R. Dalton, A. H. Udupa, and H. R. Fetterman, “Optical intensity modulator based on a novel electrooptic polymer incorporating a high chromophore,” IEEE J. Quantum Electron. 36(5), 527-532 (2000).
[50] Y. Shi, C. Zhang, H. Zhang, J. H. Bechtel, L. R. Dalton, B. H. Robinson, and W. H. Steier, “Low (sub-1-volt) halfwave voltage polymeric electro-optic modulators achieved by controlling chromophore shape,” Science 288, 119-122 (2000).
[51] X. Zhang, X. Lu, L. Wu, and R. T. Chen, “Contact poling of the nonlinear optical film for polymer-based electro-optic modulator,” Proc. SPIE 4653, 87-95 (2002).
[52] J. A. Giacometti, S. Fedosov, and M. M. Costa, “Corona charging of polymers: recent advances on constant current charging,” Brazilian Journal of Physics 29(2), 269-279 (1999).
[53] B. Liedberg, C. Nylander, and I. Lundstrom, “Surface plasmon resonance for gas detection and biosensing,” Sens. Actuators B 4, 299-304 (1983).
[54] J. M. Phelps and D. M. Taylor, “Determining the relative permittivity and thickness of a lossless dielectric overlayer on a metal film using optically excited surface plasmon polaritons,” J. Phys. D: Appl. Phys. 29, 1080-1087 (1996).
[55] H. E. de Bruijn, B. S. F. Altenburg, R. P. H. Kooyman, and J. Greve, “Determination of thickness and dielectric constant of thin transparent dielectric layers using surface plasmon resonance,” Opt. Commun. 82(5,6), 425-432 (1991).
[56] K. A. Peterlinz and R. Georgiadis, “Two-color approach for determination thickness and dielectric constant of thin films using surface plasmon resonance spectroscopy,” Opt. Commun. 130, 260-266 (1996).
[57] K. S. Johnston, S. R. Karlsen, C. C. Jung, and S. S. Yee, “New analytical technique for characterization of thin films using surface plasmon resonance,” Mater. Chem. Phys. 42, 242-246 (1995).
[58] T. M. Chinowsky and S. S. Yee, “Quantifying the information content of surface plasmon resonance reflection spectra,” Sens. Actuators, B 51, 321-330 (1998).
[59] T. M. Chinowsky, L. S. Jung, and S. S. Yee, “Optimal linear data analysis for surface plasmon resonance biosensors,” Sens. Actuators, B 54, 89-97 (1999).
[60] W. P. Chen and J. M. Chen, “Use of surface plasma waves for determination of the thickness and optical constants of thin metallic films,” J. Opt. Soc. Am. 71(2), 189-191 (1981).
[61] J.-J. Chyou, S.-J. Chen, C.-S. Chu, C.-H. Tsai, F.-C. Chien, G.-Y. Lin, K.-T. Huang, W.-C. Ku, S.-K. Chiu, and C.-M. Tzeng, “Multi-experiment linear data analysis for ATR biosensors,” Proc. SPIE 4819, 175-184 (2002).
[62] P. Yeh, Optical waves in layered media, John Wiley and Sons: New York, Chap. 5, 102-110, 1988.
[63] R. H. Myers and J. S. Milton, A first course in the theory of linear statistical models, PWS-KENT Publications: Boston, Chap. 3, 83-87, 1991.
[64] U. Schroder, “The Influence of thin metallic coatings on the dispersion of surface plasma-oscillations in gold-silver film systems,” Surf. Sci. 102(1), 118-130 (1981)
[65] K. Taniwaki, A. Hyakutake, T. Aoki, M. Yoshikawa, M. D. Guiver, and G. P. Robertson, “Evaluation of the recognition ability of molecularly imprinted materials by surface plasmon resonance (SPR) spectroscopy,” Anal. Chim. Acta 489, 191-198 (2003)
[66] J.-N. Yih, F.-C. Chien, C.-Y. Lin, H.-F. Yau, and S.-J. Chen, “An angular-interrogation attenuated-total-reflection metrology system for plasmonic sensors,” Appl. Opt. 44(29), 6155-6162, (2005).
[67] E. Bennett, R. L. Peck, D. K. Burge, and J. M. Bennett, “Formation and growth of tarnish on evaporated silver films,” J. Appl. Phys. 40, 3351-3360 (1969).
[68] N. Mehan and A. Mansingh, “Study of tarnished films formed on silver by exposure to H2S with the surface-plasmon resonance technique,” Appl. Opt. 39(28), 5214-5220 (2000).

指導教授

葉則亮、陳顯禎
(Tse-Liang Yeh、Shean-Jen Chen)

審核日期

2006-3-28

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