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  1. NTU Theses and Dissertations Repository
  2. 電機資訊學院
  3. 電子工程學研究所
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/64803
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor管傑雄
dc.contributor.authorShao-Wen Changen
dc.contributor.author張韶文zh_TW
dc.date.accessioned2021-06-16T22:59:41Z-
dc.date.available2017-08-28
dc.date.copyright2012-08-28
dc.date.issued2012
dc.date.submitted2012-08-07
dc.identifier.citation[1] Mihir Parikh, “Corrections to proximity effects in electron beam lithography.
I. Theory,” J. Appl. Phys., Vol. 50, No.6, June 1979
[2] Mihir Parikh, “Corrections to proximity effects in electron beam lithography. II. Implementation,” J. Appl. Phys., Vol. 50, No.6, June 1979
[3] Mihir Parikh, “Corrections to proximity effects in electron beam lithography. III.
Experiments,” J. Appl. Phys., Vol. 50. No.6, June 1979
[4] L. Stevens, R. Jonckheere, E. Froyen, S. Decoutere and D. Lanneer, “Determination of the proximity parameters in electron beam lithography using doughnut – structures,” Microelectronic Engineering 5 ,141-150, 1986
[5] T. H. P. Chang, 'Proximity effect in electron-beam lithography,' J. Appl. Phys., Vol. 12. No.6, Nov./Dec. 1975
[6] Norihiko Samoto and Ryuichi Shimizu, “Theoretical study of the ultimate resolution in electron beam lithography by Monte Carlo simulation, including secondary electron generation: Energy dissipation profile in polymethylmethacrylate,”
J. Appl. Phys, Vol. 54. No.7. July 1983
[7] Chen, Y., Vieu, C. and Launois, 'High Resolution X-ray Lithography and Electron-beam Lithography : Limits and Prospectives, ' Condensed Matter News, Vol. 6, pp. 22-30
[8] C. S. Whelan, D. M. Tanenbaum and D. C. La Tulipe, “Low energy electron beam top surface image processing using chemically amplified AXT resist,” J. Vac. Sci. Technol. B, Vol. 15, No. 6, Nov/Dec 1997
[9] Jian Zhang, Mina Fouad, Mustafa Yavuz, ann Bo Cui, “Charging effect reduction in electron beam lithography with nA beam current,” Microelectronic Engineering 88 2196–2199, 2011
[10] K. M. Satyalakshmi, A. Olkhovets, M. G. Metzler, C. K. Harnett, D. M. Tanenbaum and H. G. Craighead, “Charge induced pattern distortion in low energy electron beam lithography,” J. Vac. Sci. Technol. B, Vol. 18, No. 6, 2000
[11] L. Stevens, R. Jonckheere, E. Froyen, S. Decoutere, D. Lanneer, “Determination of the proximity parameters in electrons in electron beam lithography using doughnut-structures,” Microelectronic Engineering 5 1986 141 – 150, 1986
[12] D.S. Macintyre, I. Young, A. Glidle, X. Cao, J.M.R. Weaver, S. Thoms, “High resolution e-beam lithography using a thin titanium layer to promote resist adhesion, Microelectronic Engineering 83 1128–1131,2006
[13] Hyunjung Yi A Joonyeon Chang, “Proximity-effect correction in electron-beam lithography on metal multi-layers,” J Mater Sci 2007 42:5159–5164, 2007
[14] M. Kotera, K. Yagura and H. Niu, “Dependence of linewidth and its edge roughness on electron beam exposure dose,” J. Vac. Sci. Technol. B, Vol. 23, No. 6, Nov/Dec 2005
[15] R. J. Hawryluk, Andrew M. Hawryluk, Henry I. Smith, “Energy dissipation in a thin polymer film by electron beam scattering,” Journal of Applied Physics, Vol. 45, No.6, June 1974
[16] L. Marton, “Experiments on Low-Energy Electron Scattering and Energy Losses,” Reviews of Modern Physics, vol.28, july 1956
[17] L. H. A. Leunissen, W. Zhang, W. Wu, S. H. Brongersma, “Impact of line edge roughness on copper interconnects,” J. Vac. Sci. Technol. B, Vol. 24, No. 4, Jul/Aug 2006
[18] Yuansheng Ma, Yang-chun Cheng, Franco Cerrina, T. Barwicz and H. I. Smith, “Local line edge roughness in microphotonic devices: An electron-beam
lithography study,” J. Vac. Sci. Technol. B, Vol. 25, No. 1, Jan/Feb 2007
[19] D. Rio, C. Constancias, M. Saied, B. Icard, and L. Pain, “Study on line edge roughness for electron beam acceleration voltages from 50 to 5 kV,” J. Vac. Sci. Technol. B, Vol. 27, No. 6, Nov/Dec 2009
[20] G. Patrick Watson, Diana Fu, Steven D. Berger and Donald Tennant, “Measurement of the backscatter coefficient using resist response
curves for 20–100 keV electron beam lithography on Si,” J. Vac. Sci. Technol. B, Vol. 14, No. 6, Nov/Dec 1996
[21] G. Patrick Watson, Steven D. Berger, J. Alex Liddle, Linus A. Fetter, Reginald C. Farrow, Regine G. Tarascon, Masis Mkrtchyan, Anthony E. Novembre, Myrtle I. Blakey, and Kevin J. Bolan, “Precise measurement of the effective backscatter coefficient for 100-keV electron-beam lithography on Si,” J. Vac. Sci. Technol. B, Vol. 13, No. 6, Nov/Dec 1995
[22] Hyunjung Yi, Joonyeon Chang, “Proximity-effect correction in electron-beam lithography on metal multi-layers,” J Mater Sci 42:5159–5164, 2007
[23] L. Stevens, R. Jonckheere, E. Froyen, S. Decoutere and D. Lanneer, “Determination of the proximity parameters in electron beam lithography using doughnut – structures,” Microelectronic Engineering 5 ,141-150, 1986
[24] M. Rooks, N. Belic, E. Kratschmer and R. Viswanathan, “Experimental optimization of the electron-beam proximity effect forward scattering parameter,”
J. Vac. Sci. Technol. B, Vol. 23, No. 6, Nov/Dec 2005
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/64803-
dc.description.abstract隨著半導體工業的快速發展及積體電路製程上的微縮,微影技術是推動著莫爾定律繼續前進的關鍵技術,電子束微影及EUV是未來勢在必行的發展技術,當要製作微小及密度高的積體電路時,電子束微影更是最佳的選擇,另一方面,隨著尺寸微縮,微影圖型的均勻性嚴重影響著電晶體的臨界電壓及漏電流,亦是急需解決的課題。
本篇論文主要貢獻分兩部分,我們提出一套分析流程,觀測巨觀微影圖形尺寸及品質與微觀下電子的運行軌跡,第二部份針對電子束微影建立基板環境的設計標準及方法,有效解決電子束中的鄰近效應(Proximity Effect)及電荷累積效應(Charging Effect),這些效應即是限制電子束解析度的關鍵因素。
微影圖形上依據ITRS標準使用線形圖形的線寬(LW)及邊緣粗糙程度(LER),除此之外,為了分析電子注入基板後的運行機制,我們利用圈環法(Doughnut)實驗求得電子曝光強度分布。
以此分析流程,在不同特性的基板進行一系列實驗,歸納出理想的微影基板製作的標準;首先,我們發現利用二氧化矽薄膜可有效降低電子束鄰近效應,使曝光顯影圖形趨近於所設計圖形,探究電子注入基板後的物理現象,發現氧化層薄膜有效降低電子的背向散射能量,使得注入區域外的額外曝光降低,集中電子束的能量分布範圍。
接著在基板上設計接地金屬的結構,實驗結果顯示存在接地金屬結構的基板,可以製作出狹窄的線寬,能進一步逼近線寬的極限,在電子曝光強度分布上觀察出造成此現象的原因,我們發現有了接地金屬結構的基板,有效解決電子於基板上的累積,使電子偏移的現象降低,電子正向散射的範圍大幅縮小。
最後我們透過改變光阻厚度、增加氧化層厚度及改變接地鈦金屬位置,將導電度及原子序不同的材料基板進行圈環法的實驗,我們發現了電子散射及電荷累積問題存在的關聯性,這現象將顯著影響電子束微影的品質,也將是我們在未來將會深入探討的課題;論文最後我們提出一基板設計的方法,包括沉積薄氧化層及建置接地金屬結構,在此結構上進行電子束微影,可達到最佳的電子束解析度以及最細的線寬。
zh_TW
dc.description.abstractIn the near future, most integrated circuits will be made by e-beam or EUV technique. Especially, as anufacturers seek to make ever smaller and denser chips, e-beam lithography will be the method of choice. But there are still some problems with small chips. The leakage current is a crucial one. One of the reasons to anticipate gate leakage variability is gate line edge roughness (LER). Higher LER always degrades the transistor leakage current. This phenomenon occurs distinctly in small size transistors.
  In this thesis, we adopt a quantitative research method to analyze the performance of E-beam beam lithography. By using this analytical procedure, we design an ideal substrate to solve the nonideal effects in E-beam lithography. In this substrate, we can make patterns of smaller sizes and with uniform edges.
  First, we use two quantitative research methods to obtain detailed information in E-beam lithography. One is the doughnut experiment. We use it to get the parameters in E-beam exposure intensity distribution (EID). Using these parameters, we can calculate the electron exposure intensity and distribution. Further analysis of EID provides us with, information about the election’s scattering and trajectory. The second method is followed by ITRS’s standard. Using the SEM image of a developed pattern and image processing, we measure the line width (LW) and line edge roughness (LER). These are the important parameters that define the quality of lithography technology.

  As the end of this thesis, we put forward a series of methods to design the ideal substrate for E-beam Lithography. These methods combine depositing oxide films and manufacturing grounded metal structures. Oxide films on substrates suppress the backscattering electrons. And the grounded structures can minimize the effect that charged electrons have of distorting the trajectory of the incident electron beam. Using these two methods, we find that the resulting patterns on this designed substrate have the best quality. Moreover the patterns have narrower line width and smaller line edge roughness. With this novel method, e-beam lithography system may turn into a powerful tool for manufacturing denser chips with greater quality.
en
dc.description.provenanceMade available in DSpace on 2021-06-16T22:59:41Z (GMT). No. of bitstreams: 1
ntu-101-R99943165-1.pdf: 2467723 bytes, checksum: eb202c0b5e631b3239178a5af29a0e7b (MD5)
Previous issue date: 2012
en
dc.description.tableofcontents口試委員審定書 Ⅰ
誌謝 Ⅲ
摘要 Ⅴ
Abstract Ⅶ
第一章 概論 1
1.1 前言 1
1.2 研究動機 2
1.3 論文架構 4
第二章 電子束微影理論及分析 5
2.1 電子束微影簡介 5
2.2 電子束微影常見問題 8
2.2.1 鄰近效應 (Proximity Effect) 8
2.2.2 電荷累積效應(Charging Effect) 8
2.3電子束之數值計算與分析方法 9
2.3.1 蒙地卡羅法(Monte-Carlo Method) 9
2.3.2 高斯模型描述電子曝光強度分布 10
2.3.3 實驗分析法求得電子曝光強度分布 11
第三章 元件製備及量測方法 13
3.1製程/量測儀器簡介 13
3.1.1 電子槍蒸鍍系統(Electron beam evaporator, E-Gun) 13
3.1.2 電子束微影(E-Beam Lithography) 14
3.1.3 掃描式電子顯微鏡(Scanning electron microscope, SEM) 15
3.1.4 聚焦離子束(Focus Ion Beam, FIB) 16
3.2 接地金屬基板 18
3.2.1 接地金屬結構製作流程 18
3.2.2 製程技術介紹 19
3.3 實驗結果量測與數據分析 25
3.3.1 圈餅法實驗流程 25
3.3.2 評鑑微影圖形實驗方法 29
第四章 實驗結果與討論 32
4.1 沉積二氧化矽降低背向散射電子 32
4.1.1 沉積二氧化矽層於矽基板上之EID比較 33
4.1.2 微影線圖形(Line Pattern)於氧化層基板上之比較 36
4.2 接地金屬結構置於基板改善電荷累積 39
4.2.1接地金屬結構於基板上之EID比較 41
4.2.2微影線圖形(Line Pattern)於接地金屬結構基板上之比較 44
4.3 影響電子曝光強度分布EID之因素研究 48
4.3.1光阻劑厚度對電子束EID之影響 48
4.3.2鈦金屬與二氧化矽層於矽基板之比較 50
第五章 結論 51
第六章 未來展望 52
參考文獻 53
dc.language.isozh-TW
dc.subject電荷累積zh_TW
dc.subject線邊緣粗糙程度zh_TW
dc.subject鄰近效應zh_TW
dc.subject線寬zh_TW
dc.subject半導體尺寸微縮zh_TW
dc.subject電子束微影zh_TW
dc.subject積體電路zh_TW
dc.subject閘極漏電流zh_TW
dc.subjectLeakage currenten
dc.subjectIntegrated circuiten
dc.subjectProximity effecten
dc.subjectCharging effecten
dc.subjectLine Widthen
dc.subjectLine edge roughnessen
dc.subjectE-beam lithographyen
dc.title利用硬體結構改善電子束微影中鄰近效應及電荷累積效應zh_TW
dc.titleApplying Hardware Structures to Suppress Proximity Effect and Charging Effect in E-beam Lithographyen
dc.typeThesis
dc.date.schoolyear100-2
dc.description.degree碩士
dc.contributor.oralexamcommittee孫建文,孫允武,田維誠
dc.subject.keyword積體電路,電子束微影,鄰近效應,電荷累積,閘極漏電流,半導體尺寸微縮,線寬,線邊緣粗糙程度,zh_TW
dc.subject.keywordE-beam lithography,Integrated circuit,Proximity effect,Charging effect,Line Width,Line edge roughness,Leakage current,en
dc.relation.page56
dc.rights.note有償授權
dc.date.accepted2012-08-08
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
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