請用此 Handle URI 來引用此文件：
http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/65483完整後設資料紀錄
| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 王維新(Way-Seen Wang) | |
| dc.contributor.author | Yu-Hsuan Yang | en |
| dc.contributor.author | 楊宇軒 | zh_TW |
| dc.date.accessioned | 2021-06-16T23:45:49Z | - |
| dc.date.available | 2012-07-27 | |
| dc.date.copyright | 2012-07-27 | |
| dc.date.issued | 2012 | |
| dc.date.submitted | 2012-07-24 | |
| dc.identifier.citation | [1]http://edm.itri.org.tw/enews/epaper/10005/d01.htm
[2]http://www.moneydj.com/kmdj/wiki/wikiviewer.aspx?keyid=0c4335a6-780a-45aa-9998-e8512a613fa1 [3]Company, OSIA, 2009/09 [4]P. A. Franken, G. Weinreich, C. W. Peters, and A. E. Hill, 'Generation of optical harmonics,' Physical Review Letters, vol. 7, pp. 118-119, 1961. [5] J. A. Armstrong, N. Bloembergen, J. Ducuing, and P. S. Pershan, 'Interactions between light waves in a nonlinear dielectric,' Physical Review, vol. 127, pp. 1918-1939, 1962. [6] M. Uebernickel, C. Fiebig, G. Blume, K. Paschke, B. Eppich, R. Güther, and G. Erbert, “400 mW and 16.5% wavelength conversion efficiency at 488 nm using a diode laser and a PPLN crystal in single pass configuration,” Jpn. J. Appl. Phys., vol. 93, pp. 823-827, 2008. [7] Y. Kitaoka, T. Yokoyama, K. Mizuuchi, and K. Yamamoto, “Miniaturized blue laser using second harmonic generation,” Jpn. J. Appl. Phys., vol.39 no. 6A, pp.3416-3418, 2000. [8] K. Sakai, Y. Koyata, N. Shimada, K. Shibata, Y. Hanamaki, S. Itakura, T. Yagi, and Y. Hirano1, “Master-oscillator power-amplifier scheme for efficient green-light generation in a planar MgO:PPLN waveguide,” Opt. Lett., vol., 33, no.5, pp. 431-433,2008. [9] Y. Kitaoka, T. Yokoyama, K. Mizuuchi, and K. Yamamoto, “Miniaturized blue laser using second harmonic generation,” Jpn. J. Appl. Phys., vol. 39, no. 6A, pp. 3416-3418, 2000. [10] H. K. Nguyen..etc., “107-mW low-noise green-light emission by freuency doubling of a reliable 1060-nm DFB semiconductor laser diode,” IEEE Photonics Technol. Lett., vol. 18, no. 5, 2006. [11] C. Langrock, E. Diamanti, R. V. Roussev, Y. Yamamoto, and M. M. Fejer, “Highly efficient single-photon detection at communication wavelengths by use of up conversion in reverse-proton-exchanged periodically poled LiNbO3 waveguides,” Opt. Lett., vol., 30, no.13, pp. 1725-1727, 2005. [12] Y. L. Lee, B. A. Yu, C. Jung, Y. C. Noh, J. Lee, and D. K. Ko, “ All-optical wavelength conversion and tuning by the cascaded sum- and difference frequency generation (cSFG/DFG) in a temperature gradient controlled Ti:PPLN channel waveguide,” J. of the Optical Society of America, vol.13, no.8, pp. 2988-2993, 2005. [13] W. M. Young and R. S. Feigelson, “Photorefractive-damage- resistant Zn-diffused waveguides in MgO:LiNbO3,” Opt. Lett., vol. 16, no.13, pp. 995-997, 1991. [14] 徐文浩，“鋅鎳擴散式鈮酸鋰光波導元件之特性與應用”，國立台灣大學光電工程學研究所博士論文，2006年。 [15] X. Zhen, R. Wang, W. Xu, Y. Xu, and L. Zhao, “Study on photodamage of Mg:Ga:LiNbO3 crystal wave-guide substrate,” Optical Materials, pp.427-431, 2002. [16] 黃文宏，“鎵擴散式鈮酸鋰光波導特性之研究”，國立台灣大 學光電工程學研究所博士論文，2008年。 [17] 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, 1978. [18] J. L. Jackel, “Suppression of out diffusion in Ti diffused LiNbO3: a review,” J. Opt. Commun., vol. 3, pp. 82-85, 1982. [19] 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, 1996. [20] R. L. Byer, J. F. Young, and R. S. Feigelson, “Growth of high-quality LiNbO3 crystals from congruent melt,” J. Appl. Phys., vol. 41, pp. 2320, 1970. [21]J. Hirohashi, “Characterization of domain switching and optical damage properties in ferroelectrics,” Department of Applied Physics Royal Institute of Technology, 2006. [22] INSPEC, Properties of Lithium Niobate, EMIS Datareviews, series no.5, 1989. [23] A. Yariv and P. Yeh, Optical Waves in Crystals: Propagation and Control of Laser Radiation, Wiley, 1984. [24] R. V. Schmidt and I. P. Kaminow, “Metal-diffused optical waveguides in LiNbO3,” Appl. Phys. Lett., vol. 25, no. 8, pp. 458-460, 1974. [25] D. F. Clark, A. C. G. Nutt, K. K. Wong, P. J. Laybourn, and D. L. Rue, “Characteristic of proton exchanges slab waveguide on Z-cut LiNbO3 waveguide,” J. Appl. Phys., vol. 40, pp. 6218-6220, 1983. [26] V. M. N. Passaro, M. N. Armenise, D. Nesheva, and E. Y. B. Pun, “LiNbO3 optical waveguides formed in a new proton source,” J. Lightwave Tech., vol. 20, pp. 71-77, no. 1, 2002. [27] J. Noda, M. Fukuma, and A. Saito, “Effect of Mg diffusion on Ti-diffused LiNbO3 waveguide,” J. Appl. Phys., vol. 49, no. 6, pp. 3150-3154, 1978. [28] C. S. Lau, P. K. Wei, C. W. Su, and W. S. Wang, “Fabrication of magnesium-oxide-induced lithium outdiffusion waveguides,” IEEE Photon. Tech. Lett, vol. 4, no. 8, pp. 872-875, 1992. [29] R. G. Hunsperger, Intergrated Optics: Theory and Technology 5th ed., Springer, 2002. [30] 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，1996年。 [31] M. Passlack, E. F. Schubert, W. S. Hobson, M. Hong, N. Moriya, S. N. G. Chu, K. Konstadinidis, J. P. Mannaerts, M. L. Schnoes, and G. J. Zydzik, “Ga2O3 films for electronic and optoelectronic applications,” J. Appl. Phys., vol. 77, no. 2, pp. 686-693, Jan. 1995. [32] X. H. Zhen, R. Wang, W. S. Xu, Y. H. Xu, and L. C. Zhao, “Study on photodamage of Mg:Ga:LiNbO3 crystal wave-guide substrate,” Opt. Mater., vol. 19, pp. 427-431, 2002. [33] 劉俊緯“摻雜氧化鎂鈮酸鋰準相位匹配大溫度頻寬綠光倍頻雷 射晶片研製”，國立台灣大學光電工程學研究所博士論文，2010 年。 [34]K. Mizuuchi, K.Yamamoto,“Waveguide second-harmonic generation device with broadened flat quasi-phase-matching response by use of a grating structure with located phase shifts,” Opt. Lett., vol. 23, no.24, pp.1880-1882, 1998. [35]N. E. Yu, J.H. Ro, and M. Cha, S. Kurimura, T. Taira, “Broadband quasi-phase-matched second-harmonic generation in MgO-doped periodically poled LiNbO3 at the communications band,” Opt. Lett., vol. 27, no. 12, pp. 1046-1048, 2002. [36] M.L. Bortz, M. Fujimura, and M.M. Fejer “Increased acceptance bandwidth for quasi-phase matched second harmonic generation in LiNbO3 waveguides,” Electron. Lett., vol. 30, no.1, pp.34-35, 1994. [37]A. Tehranchi and R. Kashyap, “Design of novel unapodized and apodized step-chirped quasi-phase matched gratings for broadband frequency converters based on second-harmonic generation ” J. of Lightwave Technology, vol. 26, no3, pp. 343-349, 2008. [38] 林揆倫“具脊狀波導結構之準相位匹配綠光倍頻晶體研究”，國立台灣大學光電工程學研究所博士論文，2008年。 [39] 陳柏超, “應用於準相位匹配二次諧波產生藍光元件之質子交換波導設計與製作,” 國立清華大學電機工程學研究所, 2000。 [40] G. D. Miller, Periodically poled lithium niobate: modeling, fabrication, and nonlinear-optical performance, 1998. [41] 李俊瑩，“摻雜氧化鎂鈮酸鋰之準相位匹配綠光倍頻雷射晶片研製”，國立台灣大學光電工程學研究所碩士論文，2009。 [42] 林垠呈，“摻雜氧化鎂鈮酸鋰之帶狀波導綠光倍頻雷射晶片之研製”，國立台灣大學光電工程學研究所碩士論文，2010。 [43] L. E. Myers, R. C. Eckardt, M. M. Fejer, and R. L. Byer, “Quasi-phase-matched optical parametric oscillators in bulk periodically poled LiNbO3,” J. of the Optical Society of America B, vol. 12, pp. 2102, 1995. [44] Dieter H. Jundt , 'Temperature-dependent Sellmeier equation for the index of refraction in congruent lithium niobate'. Opt. Lett., vol. 22, No.20, pp. 1553–1555,1997 | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/65483 | - |
| dc.description.abstract | 本論文探討在Z切鈮酸鋰基板製作具有帶狀波導之多週期極化反轉結構。入射基頻光波長為1064nm，經由準相位匹配倍頻產生532nm的綠光。
所使用之帶狀波導有鋅鎳共同擴散式與鎵擴散式等兩種，線寬均為160μm。其中鋅鎳共同擴散式波導可導TM和TE兩種模態光，而鎵擴散式波導僅可導TM模態光。 量測結果顯示具有鋅鎳共同擴散式波導溫度頻寬為45℃，倍頻轉換效率為15% ; 而具有鎵擴散式波導則溫度頻寬為50℃，倍頻轉換效率為13.3%。相較於單一週期波導晶片顯示多週期晶片在鋅鎳共同擴散式波導上之溫度頻寬增加9倍，而轉換效率卻僅下降1.47倍 ; 在鎵波導上之溫度頻寬增加了7倍，而轉換效率卻僅下降1.33倍。因此週期性極化反轉結構上加光波導，可增加光場侷限，有助於倍頻轉換效率的提升。 | zh_TW |
| dc.description.abstract | Segment-chirped grating structure is used for the fabrication of multi-periodically poled lithium niobate (PPLN) for second harmonic generation (SHG) of green laser. To enhance the optical confinement, some metal diffused waveguides are fabricated on the structure. Green laser of wavelength 532nm is obtained by the quasi-phase matching second harmonic generation (QPM-SHG), when launched with an incident laser of wavelength 1064nm.
Zinc-and-nickel co-diffusion and gallium diffusion waveguides of the same linewidth 160 μm are fabricated. TM and TE modes are supported in the zinc-and-nickel co-diffusion waveguide, but only TM modes are supported in the gallium diffusion waveguide. PPLN with the zinc-and-nickel co-diffusion waveguide has a temperature bandwidth of 45˚C and a green laser conversion efficiency of 15%. PPLN with the gallium diffusion waveguide has a temperature bandwidth of 50˚C and a green laser conversion efficiency of 13.3%. As compared with single period waveguide PPLN, the temperature bandwidth of segment-chirped grating ZnNi:PPLN is broadened by a factor of 9, whereas the conversion efficiency is reduced only by a factor of 1.47. As for the Ga:PPLN, the temperature broadening factor 7 and the conversion efficiency reduction factor is 1.33. That shows waveguides provide significant optical confinement to compensate for the decrease in conversion efficiencies of PPLN. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-16T23:45:49Z (GMT). No. of bitstreams: 1 ntu-101-R99943106-1.pdf: 3626277 bytes, checksum: 304596ed404a20213143d342366a0bb6 (MD5) Previous issue date: 2012 | en |
| dc.description.tableofcontents | 中文摘要………………………………………………………I
英文摘要…………………………………………………………III 目錄……………………………………………………………….V 附圖目錄……………………………...…………………VIII 附表目錄……………………………...…………………XI 第一章 緒論………………………………………………….1 1-1 研究背景….……………...………………………………...1 1-2 研究動機………………...…………………………………4 1-3 內容簡介……………...……………………………………6 第二章 光波導及非線性光學原理……………………………………..6 2-1 材料性質介紹……………………………………………...6 2-2 光波導簡介……………………………………………….12 2-3-1金屬擴散式平面波導原理………………………….…..15 2-3-2鋅鎳擴散式光波導…………………………...………....16 2-3-3鎵擴散式光波導…………………………...…………....18 2-4 非線性光學簡介………………………………..………..20 2-5雙折射相位匹配……...….……………………..25 2-6準相位匹配理論介紹……...……………………..27 2-6-1一維空間準相位匹配……...………………..27 2-6-2二維空間準相位匹配……...………………..30 2-6-3可接受波長頻寬與溫度頻寬……...…..33 2-7-1增加可接受波長頻寬與溫度頻寬……...…..35 2-7-2級聯結構增加可接受頻寬…………………..37 2-8波導中準相位匹配之修正……...……………..39 第三章 光波導與週期性極化反轉元件製作…………..40 3-1週期性極化反轉製作與結果………..……….………...40 3-1-1區段啁啾型光柵……………………………….41 3-1-2高壓電致極化反轉介紹……….………………42 3-1-3高壓電致極化反轉設備架構………………...44 3-1-4液態電極結構……………...………………….45 3-1-5週期性極化反轉製作與結果…………………...46 3-2鋅鎳共同擴散與鎵擴散帶狀波導製作……….……...51 第四章 光學量測與分析………………………………………………60 4-1 光波導特性量測………………………………………….60 4-1-1 光場量測架構…………………...60 4-1-2 光場分析圖…..…………….62 4-2 綠光倍頻轉換量測架構………………………………….63 4-3 倍頻結果與分析………………………………………….66 4-4 匹配溫度位移分析……………………………………….74 第五章 結論……………………………………………………………80 參考文獻………………………………………………………………..83 中英文名詞對照表…………………………………………………….90 | |
| dc.language.iso | zh-TW | |
| dc.subject | 極化反轉 | zh_TW |
| dc.subject | 鈮酸鋰 | zh_TW |
| dc.subject | 綠光雷射 | zh_TW |
| dc.subject | 區段啁啾光柵 | zh_TW |
| dc.subject | 二倍頻 | zh_TW |
| dc.subject | Segment chirped grating | en |
| dc.subject | second harmonic | en |
| dc.subject | Poling | en |
| dc.subject | green laser | en |
| dc.subject | Lithium niobate | en |
| dc.title | 多週期極化反轉鈮酸鋰帶狀波導綠光雷射晶片之研製 | zh_TW |
| dc.title | Design and Fabrication of Multi-Periodically Poled Lithium Niobate Strip Waveguide Green Lasers | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 100-2 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 蔡宛卲(Wan-Shao Tsai),王子建(Tzyy-Jiann Wang),彭隆瀚(Lung-Han Peng) | |
| dc.subject.keyword | 極化反轉,區段啁啾光柵,綠光雷射,鈮酸鋰,二倍頻, | zh_TW |
| dc.subject.keyword | Poling,Segment chirped grating,green laser,Lithium niobate,second harmonic, | en |
| dc.relation.page | 93 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2012-07-24 | |
| dc.contributor.author-college | 電機資訊學院 | zh_TW |
| dc.contributor.author-dept | 電子工程學研究所 | zh_TW |
| 顯示於系所單位： | 電子工程學研究所 | |
文件中的檔案：
| 檔案 | 大小 | 格式 | |
|---|---|---|---|
| ntu-101-1.pdf 未授權公開取用 | 3.54 MB | Adobe PDF |
系統中的文件，除了特別指名其著作權條款之外，均受到著作權保護，並且保留所有的權利。