跳到主要內容

臺灣博碩士論文加值系統

(216.73.216.146) 您好!臺灣時間:2026/06/14 10:33
字體大小: 字級放大   字級縮小   預設字形  
回查詢結果 :::

詳目顯示

我願授權國圖
: 
twitterline
研究生:許理鈞
研究生(外文):Lee-Chun Hsu
論文名稱:旁波瓣抑制光柵與相位相依光柵結構之研究
論文名稱(外文):Studies of Sidelobe Suppression for a Periodic Dielectric Waveguide and Phase Dependent Gratings
指導教授:孫迺翔孫迺翔引用關係
指導教授(外文):Nai-Hsiang Sun
學位類別:碩士
校院名稱:義守大學
系所名稱:電機工程學系碩士班
學門:工程學門
學類:電資工程學類
論文種類:學術論文
論文出版年:2007
畢業學年度:95
語文別:中文
論文頁數:115
中文關鍵詞:旁波瓣抑制相立相依光柵
外文關鍵詞:GratingsSidelobe SuppressionPhase Dependent
相關次數:
  • 被引用被引用:4
  • 點閱點閱:766
  • 評分評分:
  • 下載下載:0
  • 收藏至我的研究室書目清單書目收藏:0
本論文分為兩個研究重點,分別探討相位相依光柵結構以及旁波瓣抑制光柵結構。我們以Floquet Bloch理論作為分析之基礎,針對TI、GSE兩種不同折射率分佈結構,求出傳輸、反射與輻射之頻譜。在相位相依光柵結構部份,以雙邊光源入射至光柵區,討論兩光源產生相位差對傳輸與反射的影響。由結果顯示,在一階布拉格效應時,當相位差使輸出為全透射時,相位差加?則會有全反射的現象。在二階布拉格效應時,輻射能量會隨著相位差做週期性變化,如果希望不受到相位影響,可選擇特定光柵區長度,則輻射能量不隨相位改變。在旁波瓣抑制光柵結構部份,為了抑制旁波,我們以Gaussian apodization,討論傳輸反射頻譜。由於在介電質波導結構Gaussian apodized連續函數在製程上不容易製作,我們將光柵離散化分為四十區,每光柵區長度相同,以duty cycle為調變量。由結果顯示,調變duty cycle後的結構,其反射頻譜即有抑制旁波的效果,在我們結構中抑制旁波效果最佳為降低30dB,但不具對稱性。
We analyze the sidelobe suppression for a periodic dielectric waveguide and the phase dependent gratins in this thesis. The Floquet Bloch theory is used to simulate TI and GSE structures of dielectric waveguides to obtain the transmission and reflection spectrum. For phase dependent gratings, we use two input signals. The calculated results show that at first Bragg, the propagation direction of a signal varies with different phases. At second Bragg, radiation power also varies with phase differences. Moreover, a grating length with phase independent for radiation powers is discovered in this study. For sidelobe suppression gratings, Gaussian apodization profile for duty cycle is used to suppress the sidelobe. Since Gaussian apodized distribution is a continue function, we divide the grating region by forty regions. Each grating region corresponds to a uniform duty cycle. The result shows that the sidelobe suppression is around 30dB.
中文摘要i
英文摘要ii
誌謝iii
目錄v
圖目錄vi
表目錄xii
第一章 緒論1
1.1 前言1
1.2 研究動機2
1.2.1 相位相依光柵2
1.2.2 旁波瓣抑制光柵4
1.3 研究方法5
1.3.1 相位相依光柵5
1.3.2 旁波瓣抑制光柵6
1.4 論文架構概述9
第二章 雙邊輸入相位相依光柵分析10
2.1 Floquet-Bloch理論10
2.2 輻射損失11
2.3 雙邊入射相位相依光柵結構理論分析15
2.4 傳輸、反射與輻射理論分析18
第三章 Gaussian Apodized旁波瓣抑制理論分析21
3.1 雙邊入射至二段不同光柵21
3.2 雙邊入射至多段不同光柵25
第四章 雙邊輸入相位相依光柵模擬結果29
4.1 TI結構29
4.1.1 雙邊入射至一階布拉格光柵結構30
4.1.2 雙邊入射至二階布拉格光柵結構42
4.2 GSE雷射結構51
4.2.1 雙邊入射至一階布拉格光柵結構52
4.2.2 雙邊入射至二階布拉格光柵結構62
第五章 單邊輸入旁波瓣抑制光柵模擬結果70
5.1 以四十區光柵的duty cycle做旁波抑制調變70
5.1.1 GSE結構71
5.1.2 TI結構76
5.1.3 TI結構增加p-spacer厚度80
5.2 調整光柵週期83
5.2.1 GSE結構:以等效折射率虛部共振最強處找出光柵週期83
5.2.2 GSE結構:以共振區等效折射率實部中點找出光柵週期90
5.2.3 TI結構95
5.2.4 TI結構增加p-spacer厚度103
第六章 結論108
參考文獻111
[1] D. Marcuse, “Directional couplers made of nonidenticalasymmetric slabs. Part I : Shnchronous couplers,” J. Lightwave Technol., vol. LT-5, pp. 113-118, Jan. 1987.
[2]H.Kogelnik and C.V.Shank,“Stimulated emission in a periodic structure,” Appl.Phys.Lett.,vol.18,pp.152-154,Feb.May1971.
[3] M.Okamoto, K. Sato, H. Mawatari, F. Kano, K. Magari, Y. Kondo and Y. Itaya,“TM mode gain enhancement in GaInAs/InP Lasers with tensile strained-layer superlattice,”IEEE J. of Quantum Electron., vol. QE-27, no. 6, pp. 1463-1469,June 1991.
[4] H. A. Haus and W. P. Huang, “Coupled-mode theory,” Proceedings of IEEE, vol.79, no. 10, pp. 1505-1518, Oct. 1991.
[5] H. Kogelnik, “Coupled wave theory for thick hologram gratings,”Bell Syst. Tech. J., vol. 48, pp. 2909-2947, Nov. 1969.
[6] G. A. Evans, D. P. Bour, N.W. Carlson, R. Amantea, J. M. Hammer, H. Lee, M. Lurie, R. C. Lai, P. F.Pelka, R. E. Farkas, J. B. Kirk, S. K. Liew,W. F, Reichert, C. A. Wang, H. K. Choi, J. N.Walpole, J. K.Butler, W. F. Ferguson, Jr., R. K. DeFreez, and M. Felisky,“Characteristics of coherent two-dimensional grating surface emitting diode laser arrays during CW operation,” IEEE Journal of Quantum Electronics,vol. 27, pp. 1594-1605, 1991.
[7] G. A. Evans, and J. M. Hammer, “Surface emitting semiconductor lasers and arrays,” Academic Press,Inc., San Diego, ISBN 0-12-244070-6, 1993
[8] Taha Masood, Steve Patterson, Nuditha V. Amarasinghe, Scott McWilliams, Duy Phan, Darren Lee,Zuhair A. Hilali, Xiong Zhang, GaryA. Evans, and Jerome K. Butler, “Single-frequency 1310-nmAlInGaAs-InP grating- outcoupled surface-emitting lasers,” IEEE Photon. Technol. Lett. Vol. 16, pp.726-728, 2004.
[9] Charles A. Brackett, “Dense wavelength division multiplexing networks: principles and applications,” IEEE J. on Selected Areas in Communications., vol. 8, pp. 948-964, August 1990
[10] T. L. Koch and U. Koren, "Semiconductor lasers for coherent optical fiber communication," J. Lightwave Technol., vol. 8, no. 3, pp. 274-293,1990
[11] Hatakeyama, H.; Kudo, K.; Yokoyama, Y.; Naniwae, K.; Sasaki, T.; “Wavelength -selectable microarray light sources for wide-band DWDM applications,” IEEE J. Quantum Electronics, vol. 8, pp. 1341-1348, Dec. 2002.
[12] S. D. Roh, S. G. Patterson, N. V. Amarasinghe, T. Masood, J. Castillega, S. McWilliams, D. Phan, D. Lee,J. B. Kirk, and GaryA. Evans, “Dual-wavelength AlInGaAs-InP grating-outcoupled surface-emittinglaser with an integrated two-dimensional photonic lattice outcoupler,”IEEE Photon. Technol. Lett. Vol.17, pp. 270-272, 2005.
[13] M. J. N. Lima, A. L. J. Teixeira and J. R. F. da Rocha, “Optimization of apodized fiber grating filters for WDM systems,” in Proc. IEEE LEOS Annu. Meeting, vol. 2, pp. 876-877, 1999.
[14] K. Ennser, M. N. Zervas and R. I. Laming, “Optimization of apodized linearly chirped fiber gratings for optical communications,” IEEE J.Quantum Electron, vol. 34, no. 5, pp.770-778, 1998.
[15] D. Marcuse, “Directional couplers made of nonidentical asymmetrical slabs. Part II: Grating- assisted couplers,” J. of Lightwave Tech., vol. LT-5, pp. 268-273, Feb. 1987.
[16] H. A. Haus, W. P. Huang, S. Kawakami, and N. A. Whitaker, “Coupled-mode theory of optical waveguides,” J.of Lightwave Tech., vol. LT-5, pp. 16-23, Jan. 1987.
[17] W. P. Huang and H. A. Haus, “Power exchange in grating-assisted couplers,” J. of Lightwave Tech., vol. LT-7, pp. 920-924, June 1989.
[18]W. P. Huang and J. W. Y. Lit, “Nonorthogonal coupled-mode theory of grating-assisted codirectional couplers,” J. of Lightwave Tech., vol. LT-9, pp. 845-852, July 1991.
[19]W. P. Huang, “Coupled-mode theory for optical waveguides: an overview,” J. Opt. Soc. Am. A, vol. 11, pp. 963-983, March 1994.
[20]S. T. Peng, T. Tamir, and H. L. Bertoni, “Theory of Periodic Dielectric Waveguides,” IEEE Trans. Microwave Theory Tech., vol. MTT-23, pp. 123-133, Jan. 1975.
[21]K. C. Chang, V. Shah, and T. Tamir, “Scattering and Guiding of Waves by Dielectric Gratings with Arbitrary Profiles,” J. Opt. Soc. Amer., vol. 70 , pp. 804-813, July 1980.
[22]W. Streifer, D. R.Scifres, and R. D. Burnham, “Analysis of grating-coupled radiation in GaAs:GaAlAs Lasers and waveguides,” IEEE J. Quantum Electronics, vol. 12, pp. 422-428, July 1976.
[23]N. H. Sun, J. K. Butler, J. P. Shih and G. A. Evans, "Grating Assisted Coupling of Highly Asymmetric Dielectric Waveguides," Technical Digest CLEO ''96, pp. 217-218, 1996.
[24]B. E. Little, “A variational coupled-mode theory including radiation loss for grating-assisted couplers,” J. Lightwave Technol., vol. 14, pp. 188-195, Feb. 1996.
[25]N.-H. Sun, J. K. Butler, G. A. Evans, Lily Pang, and Philip Congdon, “Analysis of grating-assisted directional couplers using the Floquet-Bloch theory,” J. of Lightwave Technol., Dec. 1997.
[26]V. M. N. Passaro, “Optimal design of grating-assisted directional couplers,” J. Lightwave Technol., vol. 18, no. 7, pp. 973-984, July 2000.
[27] S. F. Mahmoud and J. C. Beal, “Scattering of surface waves ata dielectric discontinuity on a planar waveguide,”IEEE Trans.Microwave Theory Tech., vol. MTT-23, p. 193, Feb. 1975.
[28]Chih-Cheng Chou, Nai-Hsiang Sun, Jerome K. Butler, and Gary A. Evans “Radiation loss of grating-assisted directional couplers using the Floquet-Bloch theory,” Technical Digest CLEO/PR 2003, pp. 350, Taipei, Taiwan, 2003.
[29]Nai-Hsiang Sun, Szu-Chou Chang, Jerome K. Butler, and Gary A. Evans “Analysis of Transmission and Reflection Characteristics of contra-directional coupling in Corrugated Waveguides,” Technical Digest CLEO/PR 2003, pp.351, Taipei, Taiwan, 2003.
[30]Nai-Hsiang Sun, Chih-Ming Lin, Jerome K. Butler, and Gary A. Evans, “Dispersion relationships for moderately deep gratings in distributed Bragg reflector lasers,” IEEE LEOS 2004 Summer Topical meetings, pp. 47-48, San Diego, California, 2004.
[31] T. Erdogan, “Cladding-mode resonances in short- and long-period fiber grating filters,” J. Opt. Soc. Am A Vol. 14, pp. 1760-1773.
[32]William Streifer, Don R. Scifres, and Robert D. Burnham, “Analysis of Grating-Coupled Radiation in GaAs:GaAlAs Lasers and Waveguides,” IEEE J. of Quantum electronics, vol. QE-12, no. 7, pp. 422-428, July 1976
[33] 張賜洲 著,光柵結構光波導元件能量傳輸與反射之分析,義守大學電機工程學系碩士論文,中華民國91年。
[34]Jerome K. Buttler, Nai-Hsiang Sun, Gary A. Evans, Lily Pang, and Philip Congdon, “Grating-Assisted Coupling of Light Between Semiconductor and Glass Waveguides,” IEEE J. of Lightwave technology, vol.16, no. 6, pp.1038-1048, June 1998
QRCODE
 
 
 
 
 
                                                                                                                                                                                                                                                                                                                                                                                                               
第一頁 上一頁 下一頁 最後一頁 top