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http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/33749完整後設資料紀錄
| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 王維新 | |
| dc.contributor.author | Tien-Lun Ting | en |
| dc.contributor.author | 丁天倫 | zh_TW |
| dc.date.accessioned | 2021-06-13T05:45:30Z | - |
| dc.date.available | 2011-07-21 | |
| dc.date.copyright | 2006-07-21 | |
| dc.date.issued | 2006 | |
| dc.date.submitted | 2006-07-12 | |
| dc.identifier.citation | [1] E. Voges and A. Neyer, “Integrated-optic devices on LiNbO3 for optical communication,” J. Lightwave Tech., vol. 5, pp. 1129-1238, 1987.
[2] R. G. Hunsperger, Integrated Optics: Theory and Technology 5th Ed., Springer, 2002. [3] G. J. Griffiths and R. J. Esdaile, “Analysis of titanium diffused planar optical waveguides in lithium niobate,” IEEE J. Quantum Electron., vol. 20, pp. 149-159, 1984. [4] P. K. Wei and W. S. Wang, “Fabrication of lithium niobate optical channel waveguides by nickel indiffusion,” Microwave and Opt. Tech. Lett., vol. 7, pp. 219-221, 1994. [5] 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. Tech. Lett., vol. 8, pp. 548-550, 1996. [6] S. J. Chang, C. L. Tsai, Y. B. Lin, J. F. Liu, and W. S. Wang, “Improved electrooptic modulator with ridge structure in X-cut LiNbO3,” J. Lightwave Tech., vol. 17, pp. 843-847, 1999. [7] R. S. Cheng, T. J. Wang, and W. S. Wang, “Wet-etched ridge waveguides in y-cut lithium niobate,” J. Lightwave Tech., vol. 15, pp. 1880-1887, 1997. [8] W. H. Hsu, K. C. Lin, J. Y. Li, Y. S. Wu, and W. S. Wang, “Polarization splitter with variable TE-TM mode converter using Zn and Ni codiffused LiNbO3 waveguides,” IEEE J. Sel. Topics Quantum Electron., vol. 11, no. 1, pp. 271-277 Jan./Feb. 2005. [9] K. Nassau, H. J. Levinstein, and G. M. Loiacono, “The domain structure and etching of ferroelectric lithium niobate,” Appl. Phys. Lett., vol. 6, pp. 228-229, 1965 [10] C. L. Lee and C. L. Lu, “CF4 plasma etching on LiNbO3,” Appl. Phys. Lett., vol. 35, pp. 756-758, 1979. [11] Y. Ohmachi and J. Noda, “Electro-optic light modulator with branched ridge waveguide,” Appl. Phys. Lett., vol. 27, pp. 544-546, 1975. [12] I. P. Kaminow and V. Ramaswamy, “Lithium niobate ridge waveguide modulator,” Appl. Phys. Lett., vol. 24, pp. 622-624, 1974. [13] F. Laurell, J. Webjorn, G. Arvidsson, and J. Holmberg, “Wet etching of proton-exchanged lithium niobate-a novel processing technique,” J. Lightwave Tech., vol. 10, pp. 1606-1609, 1992. [14] V.M.N. Passaro, M.N. Armenise, D. Nesheva, I.T. Savatinova, and E.Y.B. Pun, “LiNbO3 optical waveguides formed in a new proton source,” J. Lightwave Tech., vol. 20, pp. 71-77, 2002. [15] J. Webjörn, “Structural influence of proton exchange on domain-inverted lithium niobate revealed by means of selective etching,” J. Lightwave Tech., vol. 11, pp. 589-594, 1993. [16] M. E. Glicksman, Diffusion in Solids: Field Theory, Solid-State Principles, and Applications, Wiley, 2000. [17] S. T. Vohra and A. R. Mickelson, “Diffusion characteristics and waveguiding properties of proton-exchanged and annealed LiNbO3 channel waveguides,” J. Appl. Phys., vol. 66, pp. 5161-5174, 1989. [18] W. H. Process, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes in C, Cambridge University Press, 1999. [19] K. Kawano and T. Kitoh, Introduction to Optical Waveguide Analysis, Wiley, 2001. [20] 陳瑞鑫,「利用溼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,1996年。 [21] T.-L. Ting, L.-Y. Chen, and W.-S. Wang, “A novel wet-etching method using joint proton source in LiNbO3,” IEEE Photon. Tech. Lett., vol. 18, pp. 568-570, 2006. [22] T.-L. Ting, L.-Y. Chen, and W.-S. Wang, “Wet Etching X-cut LiNbO3 using diluted joint proton source,” to be published in Microwave and Opt. Tech. Lett. [23] 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 Tech., vol. 22, pp. 1764-1771, 2004. [24] Y. N. Korkishko and V. A. Fedorov, “Structural phase diagram of HxLi1-xNbO3 waveguides: the correlation between optical and structural properties,” IEEE J. Sel. Topics Quantum Electron., vol. 2, no. 2, pp. 187-196, 1996. [25] M. D. Micheli, J. Botineau, P. Sibillot, D. B. Ostrowsky, and M. Papuchon, “Fabrication and characterization of titanium indiffused proton exchanged (TIPE) waveguides in lithium niobate,” Opt. Comm., vol. 42, pp.101-103, 1982. [26] M. D. Micheli, J. Botineau, S. Neveu, P. Sibillot, D. B. Ostrowsky, and M. Papuchon, “Extension of second-harmonic phase-matching range in lithium niobate guides,” Opt. Lett., vol. 8, pp. 116-118, 1983. [27] D. Y. Zang and C. S. Tsai, “Single-mode waveguide microlenses and microlens arrays fabrication in LiNbO3 using titanium indiffused proton exchange technique,” Appl. Phys. Lett., vol. 46, pp. 703-705, 1985. [28] 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. Tech. Lett., vol. 4, pp. 881-883, 1992. [29] S. A. Reid, M. Varasi, and S. Reynolds, “Double dilute melt proton exchange Fresnel lenses for LiNbO3 optical waveguides,” J. Opt. Comm., vol. 10, pp. 67-73, 1989. [30] C. Canali, A. Camera, G. Della Mea, P. Mazzoldi, S. M. Al Shukri, A. C. G. Nutt, and R. M. De La Rue, “Structural characterization of proton exchanged LiNbO3 optical waveguides,” J. Appl. Phys., vol. 59, pp. 2643-2649, 1986. [31] J. L. Jackel, C. E. Rice, and J. J. Veselka, “Proton exchange for high-index waveguides in LiNbO3,” Appl. Phys. Lett., vol. 41, pp. 607-608, 1982. [32] R. G. Wilson, S. W. Novak, J. M. Zavada, A. Loni, and R. M. De La Rue, “Secondary ion mass spectrometry depth profiling of proton-exchanged LiNbO3 waveguides,” J. Appl. Phys., vol. 66, pp. 6055-6058, 1989. [33] T. Veng and T. Skettrup, “Ion exchange model for α phase proton exchange waveguides in LiNbO3,” J. Lightwave Tech., vol. 16, pp. 646-649, 1998. [34] S. T. Vohra and A. R. Mickelson, “Diffusion characteristics and waveguiding properties of proton-exchanged and annealed LiNbO3 channel waveguides,” J. Appl. Phys., vol. 66, pp. 5161-5174, 1989. [35] W. Charczenko and A. R. Mickelson, “Modeling of proton-exchanged and annealed channel waveguides and directional couplers,” J. Appl. Phys., vol. 73, pp. 3139-3148, 1993. [36] D. F. Clark, A. C. G. Nutt, K. K. Wong, P. J. R. Laybourn, and R. M. De La Rue, “Characterization of proton-exchange slab optical waveguides in z-cut LiNbO3,” J. Appl. Phys., vol. 54, pp. 6218-6220, 1983. [37] J. Nikolopoulos and G. L. Yip, “Theoretical modeling and characterization of annealed proton-exchanged planar waveguide in z-cut LiNbO3,” J. Lightwave Tech., vol. L.T.-5, pp. 700-708, 1987. [38] F. Sauer and V. Freise, “Diffusion in binären Gemischen mit Volumenänderung,“ Z. Elektrochem. Angew. Phys. Chem., vol. 66, pp. 353–363, 1962. [39] D. Anderson and M. Lisak, “Approximate solutions of some nonlinear diffusion equations,” Phys. Rev., vol. A22, pp.2761-2768, 1980. [40] E. Y. B. Pun, K. K. Loi, and P. S. Chung, “Proton-exchanged optical waveguides in z-cut LiNbO3 using phosphoric acid,” IEEE Trans. Lightwave Tech., vol. 11, pp. 277-284, 1993. [41] T. Shiozawa, H. Miyamoto, H. Ohta, M. Yamaguchi, and T. Oki, “Determination of two-dimensional optical waveguide index distribution function parameters from effective indexes,” J. Lightwave Tech., vol. 8, pp. 497-505, 1990. [42] W. L. Chen, R. S. Cheng, J. H. Lee, and W. S. Wang, “Lithium niobate ridge waveguides by nickel diffusion and proton-exchanged wet-etching,” IEEE Photon. Tech. Lett., vol. 7, pp. 1318-1320, 1995. [43] M. S. Stern, “Rayleigh quotient solution of semivectorial field problems for waveguide with arbitrary index profiles,” IEE Proc. J., vol. 138, pp. 185-190, 1991. [44] G. R. Hadley, “Transparent boundary condition for beam propagation,” Opt. Lett., vol. 16, pp. 624-626, 1991. [45] G. R. Hadley, “Transparent boundary condition for the beam propagation method,” IEEE J. Quantum Electron., vol. 28, pp. 363-370, 1992. [46] S. Fouchet, A. Carenco, C. Daguet, R. Gugliemi, and L. Riviere, “Wavelength dispersion of Ti induced refractive index change in LiNbO3 as a function of diffusion parameters,” J. Lightwave Tech., vol. L.T.-5, pp. 700-708, 1987. [47] 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。 [48] R. Scarmozzino and R. M. Osgood, “Investigation of the Padé approximant-based wide-angle beam propagation method for accurate modeling of waveguide circuits,” J. Lightwave Tech., vol. 14, pp. 2813-2822, 1996. [49] L. B. Soldano and E. C. M. Pennings, “Optical multi-mode interference devices based on self-imaging: Principles and applications,” J. Lightwave Tech., vol. 13, pp. 615-627, 1995. [50] M. Bachmann, P. A. Besse, and H. Melchior, “General self-imaging properties in N×N multimode interfernece couplers including phase relations,” Appl. Opt. , vol. 33, pp. 3905-3911, 1994. [51] S. Safavi-Naeini, S. K. Chaudhuri, and A. Goss, “Design and analysis of novel multimode optical filters in dielectric waveguide,” J. Lightwave Tech., vol. 11, pp. 1970-1977, 1993. [52] Q. Wang, S. He, and L. Wang, “A low-loss Y-branch with a multimode waveguide transition section,” IEEE Photon. Tech. Lett., vol. 14, pp. 1124-1126, 2002. | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/33749 | - |
| dc.description.abstract | 本論文以混合苯甲酸和己二酸作為質子酸源,在鈮酸鋰基板上進行質子交換溼式蝕刻法製作脊形光波導及元件。並針對其製程特性、蝕刻行為、質子交換氫離子擴散模型、以及相關的應用與優勢,進行深入而有系統的研究與分析。
在製程特性方面,於Z切晶片上,混合酸與傳統純苯甲酸的製程幾乎完全相同;主要差別在X切晶片的質子交換過程,本研究以碳酸鋰取代苯甲酸鋰來稀釋質子酸源,以求兩種酸酸度的下降比較平均。由蝕刻結果可以發現,在特定的己二酸莫耳濃度下且其他條件均相同時,以混合酸製作的脊形結構擁有較大的脊形深度,與較垂直的脊形側壁外觀。而且蝕刻出的表面仍相當平滑,適合用於製作脊形光波導。 在擴散模型方面,以二次離子質譜儀縱深分析,搭配數值方法反推出氫離子於鈮酸鋰晶體中的濃度相依擴散率。再以時域有限差分法,求解非線性的氫離子擴散微分方程式,並以實驗所得之蝕刻深度驗證擴散模型正確性。根據此法,本研究成功建立氫離子相對濃度的擴散模型,可用於後續之研究。 在元件的應用上,本研究以純苯甲酸和混合酸所製作的脊形結構,製作S形彎曲結構。實驗結果顯示因為脊形側壁所提供的光場橫向侷限性較傳統平面通道式波導為大,元件傳輸率因此明顯上升。而且以混合酸製作的脊形側壁較垂直,其S形彎曲波導的傳輸率較以純苯甲酸製作的樣本更高。這樣的脊形蝕刻法提供了縮短元件長度的可能性,在積體光學上,有一定的實用價值。 | zh_TW |
| dc.description.abstract | In this dissertation, by mixing benzoic and adipic acid as the source of proton exchange, wet etched ridge waveguides are successfully fabricated in LiNbO3. Systematic investigations are put on the fabrication characteristics, etching results, H+ diffusion behaviors, and advantages of relative applications.
In Z-cut LiNbO3, the fabrication process with proposed joint proton source is almost identical to that with pure benzoic acid. In X-cut LiNbO3, however, there exists differentiation. To equally reduce the acidity of both acids, traditional lithium benzoate is no longer suitable for diluting joint proton source, and lithium carbonate is used instead. The etching results show that with certain mole percentages of adipic acid and other things being equal, the etched ridge structures possess larger ridge depths and more vertical ridge sidewalls. Besides, the etched surfaces are still smooth with respect to operating wavelengths, and suitable for producing optical ridge waveguide. To study diffusion behaviors, secondary ion mass spectrometer (SIMS) along with the Boltzmann-Matano inverse method is used to derive concentration-dependent diffusivity of H+ in Z-cut LiNbO3. With the derived diffusivity, FDTD-based diffusion simulator successfully solves the nonlinear diffusion equation numerically. The etching depths of the experimental results meet well with the simulations. The diffusion model of hydrogen ion in Z-cut LiNbO3 is built and applicable for future use. For realistic applications, the optical ridge waveguides can be used to fabricate S-bend structure. The experimental results reveal that the lateral confinement of optical field provided by sidewalls of ridge structures is much larger than that of traditional channel waveguides. Thus, the transmission of the S-bend structure can be enhanced. In addition, the sidewalls of samples made by join proton source are more vertical, transmission can therefore further improved. The proposed wet etching method gives an opportunity to shorten the device. In the realm of integrated optics, the practical use is possible. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-13T05:45:30Z (GMT). No. of bitstreams: 1 ntu-95-D91941013-1.pdf: 5138375 bytes, checksum: e292ee5093e562c68a5ff0714ae0259b (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 5 2-1 研究目標與架構 5 2-2 蝕刻行為分析 7 2-3 擴散行為分析 8 2-4 數值分析模擬 9 2-5 光波導特性量測 13 第三章 蝕刻製程與脊形結構分析 15 3-1 質子交換溼式蝕刻法之製程簡介 15 3-2 脊形結構於Z切晶片 17 3-3 脊形結構於X切晶片 33 第四章 質子交換擴散模型 49 4-1 二次離子質譜儀實驗結果分析 49 4-2 濃度相依擴散率之分析 56 第五章 S形彎曲波導之研製 69 5-1 脊形光波導製程 69 5-2 脊形光波導之數值模擬 73 5-3 脊形光波導之量測 81 第六章 結論 91 參考文獻 95 中英文名詞對照表 101 | |
| dc.language.iso | zh-TW | |
| dc.subject | 擴散模型 | zh_TW |
| dc.subject | 鈮酸鋰 | zh_TW |
| dc.subject | 脊形光波導 | zh_TW |
| dc.subject | 積體光學 | zh_TW |
| dc.subject | 質子交換 | zh_TW |
| dc.subject | 溼式蝕刻 | zh_TW |
| dc.subject | 氫離子 | zh_TW |
| dc.subject | lithium niobate | en |
| dc.subject | diffusion model | en |
| dc.subject | hydrogen ion | en |
| dc.subject | wet etching | en |
| dc.subject | proton exchange | en |
| dc.subject | integrated optics | en |
| dc.subject | optical ridge waveguide | en |
| dc.title | 改良式鈮酸鋰脊形光波導之特性與應用 | zh_TW |
| dc.title | Characterizations and Applications of Improved Lithium Niobate Ridge Waveguides | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 94-2 | |
| dc.description.degree | 博士 | |
| dc.contributor.oralexamcommittee | 魏培坤,彭隆瀚,胡振國,涂元光,張宏鈞 | |
| dc.subject.keyword | 鈮酸鋰,脊形光波導,積體光學,質子交換,溼式蝕刻,氫離子,擴散模型, | zh_TW |
| dc.subject.keyword | lithium niobate,optical ridge waveguide,integrated optics,proton exchange,wet etching,hydrogen ion,diffusion model, | en |
| dc.relation.page | 104 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2006-07-14 | |
| 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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