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  1. NTU Theses and Dissertations Repository
  2. 電機資訊學院
  3. 光電工程學研究所
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/29149
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor王倫
dc.contributor.authorChao-Te Leeen
dc.contributor.author李昭德zh_TW
dc.date.accessioned2021-06-13T00:43:04Z-
dc.date.available2009-07-27
dc.date.copyright2007-07-27
dc.date.issued2007
dc.date.submitted2007-07-23
dc.identifier.citation[1] C. C. Lee, Thin Film Optics and Coating Technology, Yi
Hsien, Publishing Co., Taipei, Taiwan, 2002.
[2] Clapham P B and Hutley M C, “Reduction of lens
reflexion by the 'moth eye' principle”, Nature 244
281, 1973.
[3] Wilson S J and Hutley M C, “The optical properties
of 'moth eye' antireflection surfaces”, Opt. Acta 29
993, 1982.
[4] K. Knop, “Rigorous diffraction theory for
transmission phase gratings with deep rectangular
profiles”, J. Opt. Soc. Am. 68, pp.1206-1210, 1978.
[5] M. G. Moharam and T. K. Gaylord,, “Diffraction
analysis of dielectric surface-relief gratings”, J.
Opt. Soc. Am. 72, pp.1385-1392, 1982.
[6] P. Lalanne and M. Morris, “Highly improved
convergence of the coupled wave method for TM
polarization”, J. Opt. Soc. Am. A 13, pp.779-784,
1996.
[7] L. Li, “Use of Fourier series in the analysis of
discontinuous periodic structures”, J. Opt. Soc. Am.
A 10, pp.1184-1189, 1996.
[8] M.G. Mharam, et al., 'Formulation for stable and
efficient implementation of the rigorous coupled-wave
analysis of binary gratings', J. Opt. Soc.Am. A, Vol.
12, No.5, 1995.
[9] Y. Ono and M. Shinzo, “Transmission spectrum analysis
of three-dimensional photonic crystals by the
effective medium theory”, in Digests of Diffractive
Optics 2003, European Optical Society Topical Meeting
Digests Series (European Optical Society, Oxford,
UK,) pp. 20–21, 2003.
[10] M. Born and E. Wolf, Principles of Optics, 7th
(expanded) ed. (Cambridge University Press,
Cambridge), Chap. 15, p. 837, 1999.
[11] D. H. Raguin and G. M. Morris, “Antireflection
structured surfaces for the infrared spectral
region”, Appl. Opt. 32, pp.1154–1167, 1993.
[12] Y. Kanamori and K. Hane, “Broadband antireflection
gratings fabricated upon silicon substrates”, Opt.
Lett. Vol. 24, No. 20, p.1422, 1999.
[13] Philippe Lalanney, etc. “Antireflection behavior of
silicon subwavelength periodic structures for visible
light”, Nanotechnology 8, pp.53–56, 1997.
[14] Y. Kanamori, E. Roy, Y. Chen, Microelectron.
“Antireflection sub-wavelength gratings fabricated by
spin-coating replication”, Eng. 78-79, pp.287-293,
2005.
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/29149-
dc.description.abstract在許多理論與實驗的文獻中,二維次波長週期性結構已經被證實有寬頻抗反射效果,目的在增進光的穿透效率。預期在未來的太陽能電池、手機等光電產業將大量被使用,甚至取代原有鍍膜抗反射技術,因此本論文將探討抗反射結構的設計與製作。
  爲了控制抗反射的頻寬以及效率,我們使用嚴格耦合波動理論精確計算出週期性結構的週期、深度、以及形狀,由模擬結果可知深寬比越高,則越有抗反射效果。
  爲製作抗反射結構,我們使用雙光束干涉微影曝光,將抗反射圖案製作於矽晶圓表面,並利用電漿蝕刻技術(ICP),製作高深寬比抗反射周期結構於矽晶圓上。
  同時我們利用奈米壓印技術,把抗反射結構複製於曲面基材上。此製程優點可以大量複製,降低成本。
  另外在干涉微影方面,傳統平面分光鏡會產生鬼影(ghost image)進而影響曝光圖案品質。因此,我們利用光學薄膜電磁波理論,設計了特製薄膜分光鏡(pellicle beamsplitter),入射角可調在40與50度附近,理論上相當符合干涉微影實驗製程上的需求,我們並嘗試使用薄膜分光鏡作為製程上的改良。
zh_TW
dc.description.abstractIn many theoretical and experimental studies, it has been proved that 2D subwavelength periodic structure contributes to the effect of broadband antireflection, in order to increase the light transmittance. We anticipated that this kind of structure will be widely used in solar cells, cell phone, etc. Even it could replace the traditional antireflection thin film coating. In this thesis, we will discuss the design and fabrication of the AR structure.
In order to control the reflectance spectrum and efficiency, we utilized rigorous coupled wave analysis (RCWA) to calculate the period, depth, and shape of the periodic structure precisely. From the simulation results we realized that, the high-aspect-ratio structure will contribute to better AR performance.
We utilize two beam interference lithography to fabricate AR structure on Si substrates. And by means of inductive couple plasma (ICP) etching, to fabricate the high aspect ratio, periodic, AR structure on into Si.
By means of nanoimprint technique, we replicated the AR structure on curved substrates. This technique contributes to the results of mass production, cost reduction.
In addition, traditional plate beamsplitter will results in ghost image in interference lithography degenerate the quality of exposed pattern. Therefore, according to the optical thin film theory, we designed the specific pellicle beamsplitter. The incident angle of the pellicle beamsplitter is around 40 degree and 50 degree, which will meet the expectation of our experimental process. We also tried to use it to improve our fabrication process.
en
dc.description.provenanceMade available in DSpace on 2021-06-13T00:43:04Z (GMT). No. of bitstreams: 1
ntu-96-R94941037-1.pdf: 2937700 bytes, checksum: 0e45848c40b6d65572ef27b537b6c257 (MD5)
Previous issue date: 2007
en
dc.description.tableofcontentsAbstract(Chinese)........................................II
Abstract(English).......................................III
Contents..................................................V
Chapter 1. Introduction...................................1
1-1 Characteristic of Anti-reflection(AR) effect..........1
1-2 Two beam interference with pellicle beamsplitter......8
1-3 Organization of the thesis...........................10
Chapter 2 Theory and simulation of AR surface............12
2-1 Modeling of subwavelength optics.....................12
2-1-1 Approaches to rigorous diffraction theory........12
2-1-2 Effective medium theory (EMT)....................18
2-2 Simulation of subwavelength grating by using G-solver
software.............................................23
Chapter 3. Pellicle beamsplitter design..................27
3-1 Introduction to pellicle beamsplitter..............27
3-2 HR 50T/50R multilayer coating at 45o incident
angle..............................................29
3-3 Pellicle beamsplitter simulation by employing
Essential Macleod software..........................33
3-4 Pellicle BS energy and uniformity measurement.......35
3-5 Summary.............................................39
Chapter 4. AR surfaces fabrication and results...........40
4-1 Processing of AR flat surface........................40
4-1-1 Two beam interference lithography.................40
4-1-2 Cr evaporate coating and PR lift-off.............44
4-1-3 Pattern transfer by ICP-RIE.......................45
4-2 Processing of AR curved surface......................53
4-2-1 Photoresist pattern...............................53
4-2-2 PDMS stamp fast casting for pattern transfer......54
4-2-3 Pattern transfer to SU-8 photoresist by
nanoimprint.......................................55
Chapter 5. Measurement results of AR surfaces............62
5-1 Measurement of AR flat Si surface ...................62
5-2 Measurement of AR curved glass surface...............64
Chapter 6 Conclusion and future works....................68
6-1 Conclusion...........................................68
6-2 Future works.........................................71
References...............................................72
dc.language.isoen
dc.subject曲面抗反射結構zh_TW
dc.subject干涉微影zh_TW
dc.subject奈米壓印zh_TW
dc.subjectAntireflection curved structureen
dc.subjectinterference lithographyen
dc.subjectnanoimprinten
dc.title利用干涉微影與奈米壓印技術製作寬頻抗反射次波長結構於平面與曲面基材上zh_TW
dc.titleFabrication of Broadband Antireflection Subwavelength Structures on Flat and Curved Substrates by Interference Lithography and Nanoimprint Techniqueen
dc.typeThesis
dc.date.schoolyear95-2
dc.description.degree碩士
dc.contributor.oralexamcommittee王青柏,陳學禮
dc.subject.keyword曲面抗反射結構,干涉微影,奈米壓印,zh_TW
dc.subject.keywordAntireflection curved structure,interference lithography,nanoimprint,en
dc.relation.page73
dc.rights.note有償授權
dc.date.accepted2007-07-25
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
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