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http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/34659完整後設資料紀錄
| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 王維新 | |
| dc.contributor.author | Wen-Hao Hsu | en |
| dc.contributor.author | 徐文浩 | zh_TW |
| dc.date.accessioned | 2021-06-13T06:20:58Z | - |
| dc.date.available | 2009-02-06 | |
| dc.date.copyright | 2006-02-06 | |
| dc.date.issued | 2006 | |
| dc.date.submitted | 2006-01-24 | |
| dc.identifier.citation | [1] R. G. Hunsperger, Integrated Optics: Theory and Technology 5th Ed., Springer, 2002.
[2] R. V. Schmidt and I. P. Kaminow, “Metal-diffused optical waveguides in LiNbO3,” Appl. Phys. Lett., vol. 25, no. 8, pp. 458-460, Oct. 1974. [3] M. N. Armenise, “Fabrication techniques of lithium niobate waveguides,” IEE Proc., vol. 135, no. 2, pp. 85-91, Apr. 1988. [4] S. Fouchet, A. Carenco, C. Daguet, R. Guglielmi, and L. Riviere, “Wavelength dispersion of Ti induced refractive index change in LiNbO3 as a function of diffusion parameters,” J. Lightwave Technol., vol. 5, no. 5, pp. 700-708, May 1987. [5] M. Fukuma and J. Noda, “Optical properties of titanium-diffused LiNbO3 strip waveguides and their coupling-to-fiber characteristics,” Appl. Opt., vol. 19, no. 4, pp. 591-597, Feb. 1980. [6] M. Minakata, S. Saito, M. Shibata, and S. Miyazawa, “Precise determination of refractive-index changes in Ti-diffused LiNbO3 optical waveguides,” J. Appl. Phys., vol. 49, no. 9, pp. 4677-4682, Sep. 1978. [7] J. R. Carruthers, I. P. Kaminow, and L. W. Stulz, “Diffusion kinetics and optical waveguiding properties of outdiffused layers in lithium niobate and lithium tantalite,” Appl. Opt., vol. 13, no. 10, pp. 2333-2342, Oct. 1974. [8] Y. P. Liao, D. J. Chen, R. C. Lu, and W. S. Wang, “Nickel-diffused lithium niobate optical waveguide with process-dependent polarization,” IEEE Photon. Technol. Lett., vol. 8, no. 4, pp. 548-550, Apr. 1996. [9] W. M. Young, R. S. Feigelson, M. M. Fejer, M. J. F. Digonnet, and H. J. Shaw, “Photorefractive damage resistant Zn-diffused waveguides in MgO:LiNbO3,” Opt. Lett., vol. 16, pp. 995-997, 1991. [10] Y. P. Liao and R. C. Lu, “TE-pass polarizers with NI-NIPE-NI structure in Z-cut LiNbO3,” Electron. Lett., vol. 35, no. 17, pp. 1465-1467, Aug. 1999. [11] W. M. Young, M. M. Fejer, M. J. F. Digonnet, A. F. Marshall, and R. S. Feigelson, “Fabrication, characterization and index profile modeling of high-damage resistance Zn-diffused waveguides in congruent and MgO:lithium niobate,” J. Lightwave Technol., vol. 10, no. 9, pp. 1238-1246, Sep. 1992. [12] 涂瑞清,「長波長鋅擴散式鈮酸鋰光波導元件之研製」,國立台灣大學光電工程學研究所博士論文,2000年。 [13] M. E. Glicksman, Diffusion in Solids: Field Theory, Solid-State Principles, and Aapplications, Wiley, 2000. [14] W. H. Process, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numertical Recipes in C, Cambridge University Press, 1999. [15] J. M. White and P. F. Heidrich, “Optical waveguide refractive index profiles determined from measurement of mode indices: a simple analysis,” Appl. Opt., vol. 15, no. 1, pp. 151-155, 1976. [16] K. S. Chiang, “Construction of refractive-index profiles of planar dielectric waveguides from the distribution of effective indexes,” J. Lightwave Technol., vol. 3, no. 2, pp. 385-391, Apr. 1985. [17] D. Marcuse, “Electrostatic field of coplanar lines computed with the point matching method,” IEEE J. Quantum Electron., vol. 25, no. 5, pp. 939-947, May 1989. [18] A. Yariv, “Coupled-mode theory for guided-wave optics,” IEEE J. Quantum Electron., vol. 9, no. 9, pp. 919-933, Sep. 1973. [19] J. Chilwell and I. Hodgkinson, “Thin-films field-transfer matrix theory of planar multilayer waveguides and reflection from prism-loaded waveguides,” J. Opt. Soc. Am. A, vol. 1, no. 7, pp. 742-753, Jul. 1984. [20] A. K. Ghatak, K. Thyagarajan, and M. R. Shenoy, “Numerical analysis of planar optical waveguides using matrix approach,” J. Lightwave Technol., vol. 5, no. 5, pp. 660-667, May 1987. [21] J. Čtyroký, J. Homola, and M. Skalský, “Modelling of surface plasmon resonance waveguide sensor by complex mode expansion and propagation method,” Optical and Quantum Electron., vol. 29, pp. 301-311, 1997. [22] 蘇俊陽,「光波導之數值模擬」,國立台灣大學電機工程學研究所博士論文,1995年。 [23] K. Kawana and T. Kitoh, Introduction to Optical Waveguide Analysis, Wiley, 2001. [24] G. B. Hocker and W. K. Burns, “Modes in diffused optical waveguides of arbitrary index profile,” IEEE J. Quantum Electron., vol. 11, no. 6, pp. 270-276, Jun. 1975. [25] W. S. Wang, Y. P. Liao, and C. H. Yang, “Nickel-indiffusion waveguide for TE-TM mode splitter in lithium niobate,” Int. J. High Speed Electronics and System, vol. 8, no. 4, pp. 621-642, 1997. [26] 廖裕評,「金屬擴散式極化分離器之研製」,國立台灣大學電機工程學研究所博士論文,1995年。 [27] 陳卓彥,「藍光鋅鎳擴散式馬赫任德電光調變器之研製」,國立台灣大學光電工程學研究所碩士論文,2005年。 [28] 陳松良,「鈮酸鋰藍光方向耦合器之研製」,國立台灣大學光電工程學研究所碩士論文,2005年。 [29] W. S. Wang, M. C. Lee, S. L. Chen, W. H. Hsu, “Titanium-indiffused lithium niobate blue-laser waveguides,” in Proc. CLEO/Pacific Rim, 2005, paper CTuK1-4. [30] Y. Kokubun and S. Asakawa, “ARROW-type polarizer utilizing from birefringence in multilayer first cladding,” IEEE Photon. Technol. Lett., vol. 5, no. 12, pp. 1418-1420, Dec. 1993. [31] A. Morand, C. Sanchez-Pèrez, P. Benech, S. Tedjini, D. Bose, “Integrated optical waveguide polarizer on glass with a birefringent polymer overlay,” IEEE Photon. Technol. Lett., vol. 10, no. 11, pp. 1599-1601, Nov. 1993. [32] C. H. Chen and L. Wang, “Design of finite-length metal-clad optical waveguide polarizer,” IEEE J. Quantum Electron., vol. 34, no. 7, pp. 1089-1097, Jul. 1998. [33] P. G. Suchoski, T. K. Findakly, and F. J. Leonberger, “Low-loss high-extinction polarizers fabricated in LiNbO3 by proton exchange,“ Opt. Lett., vol. 13, no. 2, pp. 172-174, 1988. [34] Y. P. Liao and R. C. Lu, “TE-pass polarisers with NI-NIPE-NI structure in Z-cut LiNbO3,” Electron. Lett., vol. 35, no. 17, pp. 1465-1467, Aug. 1999. [35] P. Jiang, F. Zhou, P. J. R. Laybourn, and R. M. De La Rue, “Buried optical waveguide polarizer by titanium indiffusion and proton-exchange in LiNbO3,” IEEE Photon. Technol. Lett., vol. 4, no. 8, pp. 881-883, Aug. 1992. [36] C. C. Huang and C. C. Huang, “Novel multisectional bending polymeric waveguide polarizer,” in Proc. CLEO, vol. 2, 2004, pp. 3. [37] R. C. Twu, C. C. Huang, and W. S. Wang, “Zn indiffusion waveguide polarizer on a Y-cut LiNbO3 at 1.32-um wavelength,” IEEE Photon. Technol. Lett., vol. 12, no. 2, pp. 161-163, Feb. 2000. [38] 陳瑞鑫,「利用濕式蝕刻法研製之脊型鈮酸鋰光波導元件」,國立台灣大學電機工程學研究所博士論文,1995年。 [39] G. Stock, “Realisation of integrated optical polarizers for Ti:LiNbO3 with Au, Al, and Ti metal cladding,” Electron. Lett., vol. 24, no. 14, pp. 899-901, Jul. 1988. [40] J. Čtyroký and H. J. Henning, “Thin-film polarizer for Ti:LiNbO3 waevguides at lamda=1.3um,” Electron. Lett., vol. 22, no. 14, pp. 756-758, Jul. 1986. [41] R. A. Becker and R. C. Williamson, “Photorefractive effects in LiNbO3 channel waveguides: model and experimental verification,” Appl. Phys. Lett., vol. 47, no. 10, pp. 1024-1026, Nov. 1985. [42] W. H. Hsu, K. C. Lin, J. Y. Lin, Y. S. Wu, and W. S. Wang, “Polarization splitter with variable TE-TM mode converter using Zn and Ni codiffused LiNbO3 waveguides,” IEEE J. Select. Topic Quantum Electron., vol. 11. no. 1, pp. 271-277, Jan/Feb 2005. [43] W. H. Hsu, K. C. Lin, and W. S. Wang, “A homogeneous Y-branch type polarization splitter with electrically-tunable output powers on lithium niobate,” in Proc. CLEO/Europe, 2003, pp. 654. [44] K. C. Lin, W. H. Hsu, and W. S. Wang, “Novel optical polarization splitter in lithium niobate,” in Proc. Sixth Chinese Optoelectronics Symposium, 2003, pp. 288-291. [45] B. Glance, “Polarization independent coherent optical receiver,” J. Lightwave Technol., vol. 5, no. 2, pp. 274-276, Feb. 1987. [46] W. J. Minford, R. Depaula, and G. A. Bogert, “Interferometric fiber optical gyroscope using a novel 3x3 integrated optic polarizer/splitter,” in Dig. Conf. Optical Fiber Sensors, 1988, pp. 385-392. [47] M. Kobayashi, H. Terui, and K. Egashira, “An optical TE-TM mode splitter,” Appl. Phys. Lett., vol. 32, no. 5, pp. 300-302, 1978. [48] D. Yap, L. M. Johnson, and G. W. Pratt. Jr., “Passive Ti:LiNbO3 channel waveguide TE-TM mode splitter,” Appl. Phys. Lett., vol. 44, no. 6, pp. 583-585, 1984. [49] R. C. Twu, C. C. Huang, and W. S. Wang, “TE-TM mode splitter with heterogeneously coupled Ti-diffused and Ni-diffused waveguides on Z-cut lithium niobate,” Electron. Lett., vol. 36, no. 3, pp. 220-221, Feb. 2000. [50] H. Yajima, “Dielectric thin-film optical branching waveguide,” Appl. Phys. Lett., vol. 22, no. 12, pp. 647-649, 1973. [51] W. K. Burns and A. F. Milton, “Mode conversion in planar-dielectric separating waveguides,” IEEE J. Quantum Electron., vol. 11, no. 1, pp. 32-39, Jan. 1975. [52] M. Masuda and G. L. Yip, “An optical TE/TM mode splitter using a LiNbO3 branching waveguide,” Appl. Phys. Lett., vol. 37, no. 1, pp. 20-22, 1980. [53] J. J. G. M. van der Tol and J. H. Laarhuis, “A polarization splitter on LiNbO3 using only titanium diffusion,” J. Lightwave Technol., vol. 9, no. 7, pp. 879-886, July 1991. [54] N. Goto and G. L. Yip, “A TE-TM mode splitter in LiNbO3 by proton exchange and Ti diffusion,” J. Lightwave Technol., vol. 7, no. 10, pp. 1567-1574, Oct. 1989. [55] P. K. Wei and W. S. Wang, “Novel TE-TM mode splitter on lithium niobate using nickel indiffusion and proton exchange techniques,” Electron. Lett., vol. 30, no. 1, pp. 35-37, Jan. 1994. [56] J. Hankey, J. Urquhart, A. J. Moseley, C. Edge, M. J. Wale, M. Owen, and S. J. Pike, “Balanced polarisation diversity receiver using hybrid assembly techniques for optical coherent multichannel systems,” Electron. Lett., vol. 27, no. 21, pp. 1935-1937, Oct. 1991. [57] R. C. Alferness, “Efficient waveguide electro-optic TE/TM mode converter/wavelength filter,” Appl. Phys. Lett., vol. 36, no. 7, pp. 513-515, 1980. [58] R. S. Cheng, W. L. Chen, and W. S. Wang, “Mach-Zehnder modulators with lithium niobate ridge waveguides fabricated by proton-exchange wet etch and nickel indiffusion,” IEEE Photon. Technol. Lett., vol. 7, no. 11, pp. 1282-1284, 1995. [59] S. J. Chang, C. L. Tsai, Y. B. Lin, J. F. Liu, and W. S. Wang, “Improved electro-optic modulator with ridge structure in x-cut LiNbO3,” J. Lightwave Technol., vol. 17, no. 5, pp. 843-847, 1999. [60] Ed L. Wooten, K. M. Kissa, A. Yi-Yan, E. J. Murphy, D. A. Lafaw, P. F. Hallemeier, D. Maack, D. V. Attanasio, D. J. Fritz, G. J. McBrien, and D. E. Bossi, “A review of lithium niobate modulators for fiber-optic communication systems, ” IEEE J. Select. Topics Quantum Electron., vol. 6, no. 1, pp. 69-82, Jan. 2000. [61] K. C. Lin, W. H. Hsu, and W. S. Wang, “Tunable ridged lithium niobate polarization splitter,” in Proc. Optics and Photonics Taiwan, 2002. [62] Y. P. Liao and R. C. Lu, “Design and fabrication of wide-angle TE-TM mode splitter in lithium niobate,” IEEE J. Select. Topics Quantum Electron., vol. 6, no. 1, pp. 88-93, Jan. 2000. [63] C. W. Lin, C. L. Chen, W. H. Hsu, and W. S. Wang, “Polarization splitter with simplified coherent coupling structure,” in Proc. Optics and Photonics Taiwan, 2005, paper PA-FR1-103. [64] J. Y. Li, W. H. Hsu, and W. S. Wang, “A TE-TM mode splitter using annealed proton exchanged and zinc/nickel co-diffusion waveguide,” in Tech. Dig. CLEO/Pacific Rim, vol. 1, 2001, pp. 94-95. [65] S. R. Park and B. O, “Novel design concept of waveguide mode adapter for low-loss mode conversion,” IEEE Photon. Technol. Lett., vol. 13, no. 7, pp. 675-677, July 2001. [66] F. Laurell, J. Webjorn, G. Arviddson, and J. Holmberg, “Wet etching of proton-exchanged lithium niobate – a novel processing technique,” J. Lightwave Technol., vol. 10, no. 11, pp. 1606-1609, Nov. 1992. [67] J. L. Jackel, C. E. Rice, and J. J. Veselka, “Proton exchange for high-index waveguides in LiNbO3,” Appl. Phys. Lett., vol. 41, no. 7, pp. 607-608, 1982. [68] N. A. Sanford, J. M. Connors, and W. A. Dyes, “Simplified z-propagating DC bias stable TE-TM mode converter fabricated in y-cut lithium niobate,” J. Lightwave Technol., vol. 6, no. 6, pp. 898-902, June 1988. [69] 吳翊魁,「改良式脊型電光調變器之研究」,國立台灣大學光電工程學研究所碩士論文,2005年。 [70] W. Y. Hwang, M. C. Oh, H. Park, J. H. Ahn, S. G. Han, and H. G. Kim, “Polarization stabilizer using a polarization splitter and a thermooptic polymer waveguide device,” IEEE Photon. Technol. Lett., vol. 10, no. 12, pp. 1736-1738, Dec. 1998. [71] F. Caccavale, F. Segato, I. Mansour, and M. Gianesin, “A finite differences method for the reconstruction of refractive index profiles from near-field measurements,” J. Lightwave Technol., vol. 16, no. 7, pp. 1348-1353, Jul. 1998. [72] D. Brooks, and S. Ruschin, “Improved near-field method for refractive index measurement of optical waveguides,” IEEE Photon. Technol. Lett., vol. 8, no. 2, pp. 254-256, Apr. 1996. [73] W. H. Hsu, C. C. Hsin, T. L. Ting, and W. S. Wang, “Refractive index modeling of diffused lithium niobate waveguides using genetic algorithm,” in Proc. Optics and Photonics Taiwan, 2003, paper FC2. [74] W. S. Tsai, W. H. Hsu, and Way-Seen Wang, “The effect of noise on the reconstruction of waveguide index profile by the near-field method,” in Proc. Optics and Photonics Taiwan, 2005, paper B-FR-IV 4-6. [75] W. H. Hsu, Y. S. Chu, L. Y. Chen, C. W. Lin, and W. S. Wang, “Investigations of the silica-waveguide-based surface plasmon resonance sensor over wide analyte detection range,” in Proc. Optics and Photonics Taiwan, 2005, paper B-SA-IV 8-1. [76] W. H. Hsu, Y. S. Chu, T. L. Ting, L. Y. Chen, and W. S. Wang, “A study of surface plasmon resonance sensors using proton exchanged waveguides on lithium niobate,” in Proc. Optics and Photonics Taiwan, 2004, paper B-SA-VII2. (Student Paper Award) [77] C. F. Klingshirn, Semiconductor optics, Springer, 1995. [78] D. Sarid, “Long-range surface-plasma waves on very thin metal films,” Phys. Rev. Lett., vol. 47, no. 26, pp. 1927-1930, Dec. 1981. [79] J. J. Burke, G. I. Stegeman, and T. Tamir, “Surface-polariton-like waves guided by thin, lossy, metal films,” Phys. Rev. B, vol. 33, no. 8, pp. 5186-5201, Apr. 1986. [80] J. Homola, S. S. Yee, and G. Gauglitz, “Surface plasmon resonance sensors: review,” Sens. Actuators B, Chem., vol. 54, pp. 3-15, 1999. [81] J. R. Sambles, G. W. Bradbery, and F. Yang, “Optical excitation of surface plasmons: an introduction,” Contemporary Phys., vol. 32, no. 3, pp. 173-183, 1991. [82] R.D. Harris and J.S. Wilkinson, “Waveguide surface plasmon resonance sensors,” Sens. Actuators B, Chem., vol.29, pp. 261-267, 1995. [83] J. Čtyroký, J. Homola, P. V. Lambeck, S, Musa, H. J. W. M. Hoekstra, R. D. Harris, J. S. Wilkinson, B. Usievich, N. M. Lyndin, “Theory and modeling of optical waveguide sensors utilizing surface plasmon resonance,“ Sen. Actuator B, Chem., vol. 54, pp. 66-73, 1999. [84] R. A. Innes and J. R. Sambles, “Optical characterization of gold using surface plasmon-polaritons,” J. Phys. F: Met. Phys., vol. 17, pp. 277-287, 1987. [85] C. R. Lavers and J. S. Wilkinson, “A waveguide-coupled surface-plasmon sensor for an aqueous environment,” Sen. Actuator B, Chem., vol. 22, pp. 75-81, 1994. [86] M.N. Weiss, R. Srivastava, and H. Groger, “Experimental investigation of a surface plasmon-based integrated-optic humidity sensor,” Electron. Lett., vol. 32, no. 9, pp. 842-843, 1996. [87] J. Dostálek, J. Čtyroký, J. Homola, E. Brynda, M. Skalský, P. Nekvindová, J. Špirková, J. Škvor, and J. Schröfel, “Surface plasmon resonance biosensor based on integrated optical waveguide,” Sens. Actuators B, Chem., vol. 76, pp. 8-12, 2001. [88] J. Homola, I. Koudela, and S. S. Yee, “Surface plasmon resonance sensors based on diffraction gratings and prism couplers: sensitivity comparison,” Sens. Actuators B, Chem., vol. 54, pp. 16-24, 1999. [89] 朱怡欣,「光波導式表面電漿子共振感測元件之研製」,國立台灣大學電子工程學研究所碩士論文,2005年。 [90] M. N. Weiss, R. Srivastava, H. Groger, Peter Lo, and S. F. Luo, “A theoretical investigation of environment monitoring using surface plasmon resonance waveguide sensors,” Sens. Actuators A, Phys., vol. 51, pp. 211-217, 1996. [91] J. Čtyroký, J. Homola, and M. Skalský, “Tuning of spectral operation range of a waveguide surface plasmon resonance sensor,” Electron. Lett., vol. 33, no. 14, pp. 1246-1247, 1997. [92] R.C. Jorgenson and S.S. Yee, “A fiber-optic chemical sensor based on surface plasmon resonance,” Sens. Actuators B, Chem., vol. 12, pp. 213-220, 1993. [93] M. J. Weber, Handbook of Optical Material, CRC Press, 2003. [94] D. M. Gill, D. Jacobson, C. A. White, C. C. W. Jones, Y. Shi, W. J. Minford, and A Harris, “Ridged LiNbO3 modulators fabricated by a novel oxygen-ion implant/wet-etch technique,” J. Lightwave Technol., vol. 22, no. 3, pp. 887-894, Mar. 2004. [95] T. L. Ting, L. Y. Chen, and W. S. Wang, “A novel wet-etching method using joint proton source in LiNbO3,” to be published in IEEE Photon. Technol. Lett. [96] T. J. Wang, C. F. Huang, W. S. Wang, and P. K. Wei, “A novel wet-etching method using electric-field-assisted proton exchange in LiNbO3,” J. Lightwave Technol., vol. 22, no. 7, pp. 1764-1771, Jul. 2004. | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/34659 | - |
| dc.description.abstract | 本論文探討在Z切鈮酸鋰基板上以鋅鎳共同擴散的方式設計製作光波導及元件,並首次針對其製程特性、定量擴散行為、折射率模型、以及相關的應用與優勢,作深入的系統性研究與分析。
在製程特性方面,有鎳金屬作為附著層,解決了原本鋅金屬對於鈮酸鋰基板附著力不佳的問題,使得製程成功率大為提升。在擴散過程中,高溫不超過攝氏950度,因此沒有鋰離子外擴散的問題,並使用兩段式升溫,增加鋅金屬氧化的程度,以提升製程穩定性。在擴散行為分析方面,採用二次離子質譜儀縱深分析,配合電子微探儀表面測定,考慮升降溫的效應,分別建立鎳、鋅單獨擴散,以及鋅鎳共同擴散的定量擴散模型,並討論共同擴散與單獨擴散之間的差異。 根據所得之定量擴散模型,結合稜鏡耦合系統對於光波導等效折射率的量測,並進一步利用逆WKB法重建折射率分佈,可以計算出各個擴散源的折射率模型。實驗結果顯示單位濃度鎳所造成的折射率變化量高於鋅,而由於不同極化方向上的折射率變化趨勢不同,因此造成了製程相依極化特性。在鋅鎳共同擴散的情況下,其折射率分佈可成功地由相關的擴散與折射率模型計算出,並且由於鋅的擴散速度較慢,可以改善原本鎳擴散式光波導光場侷限性不佳的問題。 在元件的應用上,本研究首先將鋅鎳共同擴散式光波導應用於波導極化器,實驗結果顯示非普極化方向的極化訊熄比為24dB,普極化方向可達29dB,且不需要任何額外的結構設計。其次,本研究也結合製程相依極化特性以及鈮酸鋰晶體的電光效應,設計及實作出一可調式極化分離器,極化分離訊熄比在非普極化與普極化方向分別為18dB與23dB,極化轉換率可達60%以上。這樣的元件提供了極化分離器一個調整輸出光功率比例的機制,在光通訊元件或光感測器上,均有一定的實用性。 | zh_TW |
| dc.description.abstract | In this dissertation, optical waveguides and devices made by Zn and Ni co-diffusion on Z-cut lithium niobate (ZNI:LiNbO3) are systematically investigated from their fabrication characteristics, (co-)diffusion behaviors, refractive index models, to unique applications for the first time.
In the waveguide fabrication process, the required diffusion temperature is no higher than 950 Celsius degree, and thus free of lithium out-diffusion problem. The adhesion of deposited Zn layer to substrate is significantly improved by the presence of Ni. A two-step thermal cycle is programmed in the diffusion process to enhance oxidation of Zn and yield stable waveguide conditions. To study the diffusion behaviors, secondary ion mass spectrometer (SIMS) and electron probe x-ray microanalyzer (EPMA), along with a FDTD-based diffusion simulator, are used to build and verify quantitative diffusion models for Ni, Zn, and ZNI. The diffusion parameters are successfully retrieved, and major effects of co-diffusion are also discussed. With the quantitative diffusion models, prism-coupler measurement and IWKB methods are combined to construct refractive index models for related diffusants. Experimental results show that index change induced by unit concentration of Ni is higher than that of Zn. Different polarizations exhibit different trends in refractive index models so that the fabrication-dependent polarizations can be achieved. The index profiles of ZNI:LiNbO3 waveguides can be derived by co-diffusion model and refractive index models of individual diffusants. It is also found that the optical confinement of ZNI waveguides is better than Ni-indiffused ones because the diffusivity of Zn is lower than that of Ni. For practical applications, ZNI:LiNbO3 waveguides supporting single polarization are used as waveguide polarizers with polarization extinction ratios of 24dB and 29dB for extraordinary and ordinary waves, respectively, without any special design of buffer layer or waveguide structure. In addition, tunable polarization splitters, in which the output power ratio between two polarization components can be electrically tuned, are proposed and demonstrated with ZNI:LiNbO3 waveguides, leveraging both the fabrication-dependent polarization property and EO effect. Experiment results show polarization splitting ratio of 18dB and 23dB for extraordinary and ordinary waves, respectively, with mode conversion efficiency up to 60%. Advantages of applying ZNI:LiNbO3 waveguides to integrated optical applications are also addressed in this dissertation. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-13T06:20:58Z (GMT). No. of bitstreams: 1 ntu-95-D91941003-1.pdf: 2992902 bytes, checksum: 24fdafe31999f6b6b7340fed798afb40 (MD5) Previous issue date: 2006 | en |
| dc.description.tableofcontents | 第一章 緒論 1
1-1 研究背景 1 1-2 研究動機 2 1-3 內容簡介 3 第二章 研究方法 4 2-1 研究目標與架構 4 2-2 擴散行為分析 6 2-3 光波導特性量測 7 2-4 光波導分析模擬 10 第三章 波導製程與擴散模型 17 3-1 製程步驟與特性 17 3-2 鎳金屬擴散模型 21 3-3 鋅金屬擴散模型 28 3-4 鋅鎳共同擴散模型 33 3-5 共同擴散行為之討論 39 第四章 折射率模型與製程相依極化特性 43 4-1 鎳擴散式光波導折射率模型 43 4-2 鋅擴散式光波導折射率模型 48 4-3 鋅鎳共同擴散式光波導折射率模型 52 4-4 折射率模型討論與製程相依極化特性 58 4-5 鋅鎳共同擴散式光波導的特色 60 第五章 波導極化器 61 5-1 波導極化器簡介 61 5-2 鋅鎳共同擴散式波導極化器 62 5-3 通道式光波導製程條件 64 5-4 波導極化器實驗結果 66 第六章 可調式極化分離器 68 6-1 極化分離器簡介 68 6-2 元件設計與操作原理 69 6-3 製程步驟與條件 71 6-4 實驗結果與討論 74 6-5 可調式極化分離器之應用 77 第七章 結論 80 附錄A 多模態二氧化矽光波導式表面電漿子共振感測器之分析 83 附錄B 以濕式蝕刻法製作深脊型結構之實驗結果 90 參考文獻 97 中英文名詞對照表 107 | |
| dc.language.iso | zh-TW | |
| dc.subject | 積體光學 | zh_TW |
| dc.subject | 光波導 | zh_TW |
| dc.subject | 金屬擴散 | zh_TW |
| dc.subject | 鈮酸鋰 | zh_TW |
| dc.subject | metal indiffusion | en |
| dc.subject | optical waveguides | en |
| dc.subject | integrated optics | en |
| dc.subject | lithium niobate | en |
| dc.title | 鋅鎳共同擴散式鈮酸鋰光波導元件之特性與應用 | zh_TW |
| dc.title | Characterizations and Applications of Zinc and Nickel Co-Diffused Optical Waveguides on Lithium Niobate | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 94-1 | |
| dc.description.degree | 博士 | |
| dc.contributor.oralexamcommittee | 李清庭,張宏鈞,胡振國,涂元光,黃遠東,彭隆瀚 | |
| dc.subject.keyword | 積體光學,鈮酸鋰,金屬擴散,光波導, | zh_TW |
| dc.subject.keyword | integrated optics,lithium niobate,metal indiffusion,optical waveguides, | en |
| dc.relation.page | 110 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2006-01-25 | |
| 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 |
| 顯示於系所單位: | 光電工程學研究所 | |
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