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  1. NTU Theses and Dissertations Repository
  2. 電機資訊學院
  3. 電機工程學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/28324
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.authorChin-Yu Changen
dc.contributor.author張勤煜zh_TW
dc.date.accessioned2021-06-13T00:05:12Z-
dc.date.available2012-07-31
dc.date.copyright2007-07-31
dc.date.issued2007
dc.date.submitted2007-07-30
dc.identifier.citation[1]R. G. Hunsperger, Integrated Optics: Theory and Technology 5th Ed., Springer, 2002.
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[9]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.
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[11]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.
[12]T. L. Ting, L. Y. Chen, and W. S. Wang, “Wet etching X-cut LiNbO3 using diluted joint proton source,” Microwave and Opt. Tech. Lett., vol. 48, pp. 2108-2111, 2006.
[13]E. Y. B. Pun, K. K. Loi, and P. S. Chung, “Proton-exchanged optical waveguides in z-cut LiNbO3 using phosphoric acid,” J. Lightwave Tech., vol. 11, pp. 277-284, 1993.
[14]K. Yamamoto, and T. Taniuchi, “Characteristics of phrophosphoric acid proton-exchanged waveguides in LiNbO3,” Appl. Phys. Lett., vol. 70, no. 11, pp. 6633-6668, 1991.
[15]丁天倫,「改良式鈮酸鋰脊形光波導之特性與應用」國立台灣大學光電工程學研究所博士論文,2006。
[16]B. Glance, “Polarization independent coherent optical receiver,” J. Lightwave Tech., vol. 5, no. 2, pp. 274-276, 1987.
[17]W. J. Minford, R. Depaula, and G. A. Bogert, “Interferometer fiber optical gyroscope using a novel 3 3 integrated optic polarizer/ splitter,” in Dig. Conf. Optical Fiber Sensors, pp. 385-392, 1988.
[18]M. Kobayashi, H. Terui and K. Egashira, “An optical TE-TM mode splitter,” Appl. Phys. Lett., vol 32, no.5, pp.300-302,1979.
[19]O. Mikami, “LiNbO3 coupled-waveguided TE/TM mode splitter,” Appl. Phys. Lett., vol 36, pp.491-493,1980.
[20]H. Maruyama, M. Haruna, and H. Nishiahra, “TE-TM mode splitter using directional coupling between heterogeneous waveguides in LiNbO3,” J. Lightwave Techno., vol. 13, no 7, pp. 1550-1554, 1995.
[21]N. Goto and G. L. Yip, “A TE-TM mode splitter in LiNbO3 by proton exchanged and Ti diffusion,” J. Lightwave Technol., vol. 7, no 10, pp. 1567-1574, 1989.
[22]Y. Fujii and H. Hidaka, “A passive TE/TM mode splitter device by the Ion-exchange LiNbO3 waveguide,” Tran. IECE Japan., vol.E68, no.2, pp.111-112, 1985.
[23]P. K. Wei and W. S. Wang, “Novel TE-TM mode splitter on lithium niobate using nickel indiffused and proton exchange techniques,” Electron Lett., vol. 30, no. 1, pp. 35-37,1994.
[24]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。
[25]林松傑,「鎳擴散質子交換極化分離器之研製」,國立台灣大學電機工程學研究所碩士論文,1996。
[26]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, 2005.
[27]R. C. Alferness, “Efficient waveguide electro-optic TE TM mode converter/wavelength filter,” Appl. Phys. Lett., vol. 36, no. 7, pp. 513-515, 1980.
[28]C. Y. Chang, C. C. Lai, and W. S. Wang, “Variable TE-TM mode splitter using nickel diffusion and annealed proton-exchange lithium niobate waveguide,” accepted by Japan J. Appl. Phys.
[29]http://www.taipower.com.tw/left_bar/power_life/electromagnetic_field/electromagnetic_field_of_live/electromagnetic_field_of_live_2.htm
[30]A. Holmes-Siedle, “Radiation effects in space, nuclear power and accelerators : impact on optics and light sensor,” SPIE Critical Review of Science and Technology on Advancement of Photonics for Space, vol. CR66, pp. 37-57, 1997.
[31]E. W. Taylor, “Radiation effects in LiNbO3,” in Properties in Lithium Niobate, IEE EMIS DATAREVIEWS Series no. 28, K. K. Wong, Ed. United Kingdom: INSPEC, 2002, pp. 359-371.
[32]Y. Ohmori, M. Yamaguchi, K. Yoshino, and Y. Inuishi, “Optical damage in LiNbO3 induced by X-ray irradiation,” Japan. J. Appl. Phys., vol. 16, No. 1, pp.181-182, 1977.
[33]E. Colby, G. Lum, T. Plettner, and J. Spencer, “Gamma radiation studies on optical materials,” IEEE Trans. Nucl. Sci., vol. 49, No. 6, pp.2857-2867, Dec. 2002.
[34]K.P. Lor, Q. Liu, and K.S. Chaing, “UV-written long-period gratings on polymer waveguides,” IEEE Photon. Tech. Lett., vol.17 pp. 594-596, 2005.
[35]F. Berghmans, F. Vos, and M. Decreton, “Evaluation of three different optical fiber temperature sensor types for application in gamma radiation environment,” IEEE Trans. Nucl. Sci., vol. 45, pp. 1537-1542, June 1998.
[36]C. C. Lai, C. Y. Chang, and W. S. Wang, “Study of Gamma- Irradiation Damage in LiNbO3 Waveguides,” IEEE Photon. Tech. Lett., vol. 19, no. 13, pp. 1002-1004, 2007.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/28324-
dc.description.abstract本論文探討可調脊形光極化分離器之原理和製作方法,同時又探討γ射線對於該元件之波導所造成的影響。在鈮酸鋰基板上所製作的脊形結構,可改用苯甲酸與己二酸的混合酸作為質子交換源,結果有較佳的脊形結構外觀比。
元件架構為一非對稱y形分岔,下半部輸入端為一光極化轉換器,上半部輸出端為一光極化分離器。輸入端為鎳擴散波導,其兩旁外加一對指狀電極;輸出端兩分支波導分別由質子交換波導和鎳擴散波導。利用鎳擴散光波導製程極化相依的特性,選擇在適當的條件下製作可導普極化方向和非普極化方向的輸入端鎳波導,與只導普極化方向的直分支鎳波導。至於只導非普極化方向的彎曲分支波導,則利用質子交換波導只導非普極化方向的特性來製作。而指狀電極結構的極化轉換器,TE極化方向和TM極化方向可以藉由外加電場轉換,以調變輸出的TE極化方向和TM極化方向之光功率比。製作出來的可調脊形光極化分離器,在TE和TM極化光的訊熄比分別為25dB和18dB。當外加調變電壓為70V時,TM和TE極化光分別有85%和50%的轉換效率。此轉換效率優於先前所發表的結果。
在γ射線輻射效應的影響下,本研究結果發現脊形結構的熱退火質子交換式光波導具有最優異的抗輻射性與最低的傳播損耗。每增加10KGy的輻射照射劑量約只增加0.06dB/cm的傳播損耗。
zh_TW
dc.description.abstractThe principle and fabrication of tunable ridge-type optical polarization splitter is studied and the influence of the gamma ray irradiation on the waveguides of the splitter is discussed. The ridge structure on the lithium niobate substrate is fabricated by using a mixture of benzoic acid and adipic acid to have a larger depth-to-width ratio.
The splitter is essentially an asymmetric y-branch waveguide. The lower part is a polarization converter and the upper part is a TE/TM polarization splitter. The polarization converter consists of a nickel indiffusion waveguide and a pair of finger-type electrodes deposited on both side of the waveguide. The two branch of the polarization splitter is fabricated by using nickel indiffusion and annealed proton exchange (APE). Using the process-dependent polarization property of the nickel indiffusion waveguide, the input waveguide supporting both ordinary and extraordinary waves and the straight branch waveguide supporting only ordinary wave are successfully fabricated by choosing proper process parameters. The bent branch waveguide supporting only extraordinary wave is fabricated by APE waveguide due to its property of just supporting extraordinary wave. When an incident laser is passing through the polarization converter, the power ratio of TE and TM polarization can be adjusted by an applied electric field. Then the TE- and TM-polarization powers are split by the following TE/TM polarization splitter.
The extinction ratio of TE and TM polarization are 25dB and 18dB, respectively. When a voltage of 70V is applied to the electrodes, 85% and 50% of the power in TM- and TE-branch waveguide are converted to the power in TE- and TM-branch waveguide, respectively, which are greater than those reported previously.
Moreover, under the irradiation of gamma ray, the ridged APE waveguide exhibits the highest anti-radioactivity. The measured power transmission loss of ridged APE waveguide is 0.06 dB/cm per 10KGy, which is the lowest loss among all the waveguides tested.
en
dc.description.provenanceMade available in DSpace on 2021-06-13T00:05:12Z (GMT). No. of bitstreams: 1
ntu-96-D88921010-1.pdf: 1704919 bytes, checksum: 0bfd359ef7bdf94ab8cceb2c01c6d295 (MD5)
Previous issue date: 2007
en
dc.description.tableofcontents第一章 緒論 1
1-1 研究背景 1
1-2 研究動機 3
1-3 內容簡介 5
第二章 蝕刻製程與脊形結構 7
2-1 脊形結構簡介 7
2-2 質子交換溼式蝕刻法製程 8
第三章 可調光極化分離器 21
3-1 光極化分離器種類 21
3-2 可調脊形光極化分離器簡介 26
第四章 元件設計、製程與量測結果分析 29
4-1 元件設計 29
4-1-1光極化分離器波導之選擇 29
4-1-2光極化轉換器電極週期之選擇 33
4-1-3光極化轉換器電極長度之選擇 34
4-1-4光極化轉換器電極緩衝層之選擇 34
4-2 元件製程 35
4-2-1脊形結構蝕刻 36
4-2-2極化分離器之製作 36
4-2-3極化轉換器之製作 40
4-3 元件量測 42
4-3-1 量測系統說明 42
4-3-2 光極化分離器量測結果 43
4-3-3 光極化轉換器調變結果 44
第五章 Γ射線對於鈮酸鋰光波導之影響 49
5-1 Γ射線簡介 49
5-2 Γ射線照射研究動機 51
5-3 Γ射線照射實驗 52
5-4 Γ射線照射後元件量測結果與討論 54
第六章 結論與未來展望 59
參考文獻 63
中英文名詞對照表 67
dc.language.isozh-TW
dc.subject脊形zh_TW
dc.subject伽瑪輻射zh_TW
dc.subject光極化分離器zh_TW
dc.subject光波導zh_TW
dc.subject鋰酸鋰zh_TW
dc.subject可調zh_TW
dc.subjectlithium niobateen
dc.subjecttunableen
dc.subjectridge-Typeen
dc.subjectoptical polarization splitteren
dc.subjectgamma irradiationen
dc.subjectoptical waveguideen
dc.title可調脊形光極化分離器及伽瑪輻射效應之研究zh_TW
dc.titleStudy of Tunable Ridge-Type Optical Polarization Splitter and Gamma Irradiation Effecten
dc.typeThesis
dc.date.schoolyear95-2
dc.description.degree博士
dc.contributor.oralexamcommittee胡振國,李清庭,張宏鈞,彭隆瀚,魏培坤
dc.subject.keyword可調,脊形,光極化分離器,伽瑪輻射,光波導,鋰酸鋰,zh_TW
dc.subject.keywordtunable,ridge-Type,optical polarization splitter,gamma irradiation,optical waveguide,lithium niobate,en
dc.relation.page71
dc.rights.note有償授權
dc.date.accepted2007-07-30
dc.contributor.author-college電機資訊學院zh_TW
dc.contributor.author-dept電機工程學研究所zh_TW
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