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http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/50479Full metadata record
| ???org.dspace.app.webui.jsptag.ItemTag.dcfield??? | Value | Language |
|---|---|---|
| dc.contributor.advisor | 管傑雄 | |
| dc.contributor.author | Cheng-Huan Chung | en |
| dc.contributor.author | 鍾政桓 | zh_TW |
| dc.date.accessioned | 2021-06-15T12:42:29Z | - |
| dc.date.available | 2021-08-03 | |
| dc.date.copyright | 2016-08-03 | |
| dc.date.issued | 2016 | |
| dc.date.submitted | 2016-07-27 | |
| dc.identifier.citation | [1] James D. Plummer, Michael Deal, Peter D. Griffin “Silicon VLSI Technology: Fundamentals, Practice, and Modeling ”, Prentice Hall
[2] Stepanova, Maria, Dew, Steven “Nanofabrication - Techniques and Principles ”,Springer [3] T. H. P. Chang, “Proximity effect in electron-beam lithography ”, J. Appl. Phys., Vol. 12. No.6, Nov/Dec. 1975 [4] Vitor R. Manfrinato ,Jianguo Wen, Lihua Zhang “Determining the Resolution Limits of Electron-Beam Lithography: Direct Measurement of the Point-Spread Function ,” Nano Lett. 2014, 14, 4406−4412 [5] Bo Wu and Andrew R. Neureuther “Energy deposition and transfer in electron-beam lithography ,” J. Vac. Sci. Technol. B 19, Nov/Dec 2001 [6] Ananthan Raghunathana and John G. Hartley ,“Influence of secondary electrons in high- energy electron beam lithography,” J. Vac. Sci. Technol. B, Vol. 31, No. 1, Jan/Feb 2013 [7] R.J. Boiko and B.J. Hughes ,“Quantitative lithographic performance of proximity correction for electron beam lithography,” J. Vac. Sci. Technoi. B 8 (6), Nov/Dec 1990 [8] Xiaokang Huang, Greg Bazan, and Gary H. Bernstein,“New technique for computation and challenges for electron-beam lithography” ,J. Vac. Sci, Technol. B 11(6), Nov/Dec 1993 [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] Mihir Parikh and David F. Kyser, “Energy deposition functions in electron resist films on substrates” , J. Appl. Phys. 50(2), February 1979 [12] 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. 54 (7). July 1983 [13] Xiaokang Huang, Gary H. Bernstein, Greg Bazán, and Davide A. Hill, “Spatial density of lines exposed in poly(methylmethacrylate) by electron beam lithography”, J.Vac. Sci. Technol. A 11(4), Jul/Aug 1993 [14] S. J. Wind, M. G. Rosenfield, G. Pepper, W. W. Molzen, and P. D. Gerber, “Proximity correction for electron beam lithography using a three‐Gaussian model of the electron energy distribution” , J. Vac. Sci. Technol. B 7 (6), Nov/Dec 1989 [15] M. Rooksa, 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 [16] David C. Joy, “The spatial resolution limit of electron lithography”, Bell Laboratories, Murray Hill, NJ 07974, U.S.A. [17] E. Boa-e, E. van der Drift, J. Romijn and B. Rousseeuw, “Experimental study on proximity effects in high voltage E-beam lithography”, Microelectronic Engineering 11 (1990) 351-354 [18] 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 [19] Keith Mountfield, Andrew Eckert, XiaoMin Yang and Earl Johns, “E-beam proximity effect parameters of sub-100nm features” , Proc. of SPIE Vol. 5376 [20]W. Patrick and P. Vettiger, “Optimization of the proximity parameters for the electron beam exposure of nanometer gate‐length GaAs metal–semiconductor field effect transistors” , J. Vac. Sci. Technol. B 6, 2037 (1988) [21] Anushka Gangnaik , Yordan M. Georgiev , Brendan McCarthy , Nikolay Petkov , Vladimir Djara and Justin D. Holmes, “Characterisation of a novel electron beam lithography resist, SML and its comparison to PMMA and ZEP resists” , Microelectronic Engineering 123 (2014) 126–130 [22] Anushka Gangnaik, Yordan M. Georgiev, and Justin D. Holmes , “Correlation of lithographic performance of the electron beam resists SML and ZEP with their chemical structure” , J. Vac. Sci. Technol. B 33(4), Jul/Aug 2015 [23] Mohammad Ali Mohammad, Steven K Dew and Maria Stepanova , “SML resist processing for high-aspect-ratio and high-sensitivity electron beam lithography”,Nanoscale Research Letters 2013, 8:139 [24] Bryan Cord, Jodie Lutkenhaus, and Karl K. Berggren , “Optimal temperature for development of poly(methylmethacrylate)” , J. Vac. Sci. Technol. B 25, Nov/Dec 2007 [25]L. E. Ocola and A. Stein , “Effect of cold development on improvement in electron-beam nanopatterning resolution and line roughness” , J. Vac. Sci. Technol. B 24(6) Nov/Dec 2006 [26] Landobasa Y. M. Tobing, Liliana Tjahjana, and Dao Hua Zhang, “Large contrast enhancement by sonication assisted cold development process for low dose and ultrahigh resolution patterning on ZEP520A positive tone resist” ,J. Vac. Sci. Technol. B 30(5), Sep/Oct 2012 [27] Takeru Okada, Jiro Fujimori, Makoto Aida, Megumi Fujimura, Tatsuya Yoshizawa, Masahiro Katsumura, and Tetsuya Iida, “Enhanced resolution and groove-width simulation in cold development of ZEP520A” ,J. Vac. Sci. Technol. B 29(2), Mar/Apr 2011 | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/50479 | - |
| dc.description.abstract | 微影技術是積體電路IC製程的關鍵技術,也是讓摩爾定律能夠繼續前進的重要推手,半導體工業之所以能夠快速發展,晶片能夠越做越小且價格越來越便宜都與微影技術的發展息息相關,一直以來光學微影是半導體製程的主流,其優點為可大量生產且速度快成本低廉,相較於其他微影技術有很大的優勢,然而隨著晶片越來越小傳統的光學微影技術已經面臨了極限,需要新的微影技術研究,目前電子束微影(E-beam, Electron Beam Lithography)及極紫外光微影(EUV, Extreme Ultraviolet Lithography)是未來顯影技術研究的主流。
本論文主要研究如何改善電子束微影中的鄰近效應。為了改善鄰近效應我們使用了三種方法,改變電子阻劑、縮短顯影時間、降低顯影溫度,在變換電子阻劑的實驗中我們分析了使用不同電子阻劑的優缺點,並選擇了適合進行後續實驗的電子阻劑,接者我們利用電子束系統設計出單點實驗,透過曝光劑量與顯影條件的改變來觀察高斯單點的直徑變化,從實驗結果我們發現透過結合短顯影時間與低溫顯影二種條件,能夠大幅降低鄰近效應,繪製出較小的圖案。之後我們藉由實驗的結果以及傳統電子束散射的理論基礎一步步推導了適用於短顯影時間的速率模型並進行了擬合,發現擬合結果非常好,且各種參數都能夠有很好的物理解釋,接著我們利用低溫短顯影的技術以及模型理論,進行了不同週期奈米線的實驗,成功製作出了9nm的小線寬,並更進一步做出週期30nm的小線寬圖形,同時也證實模型的預測正確而且由高斯單點得到的低溫短顯影實驗結果確實可以運用於畫線上而且有相同的趨勢,最後我們透過反應式離子蝕刻和蒸鍍的方式成功的將我們的圖案轉移至基板上,製作出了小週期奈米線的結構。 | zh_TW |
| dc.description.abstract | Lithography is the key technology in integrated circuits manufacturing process, and the improvement of it is the main reason that Moore's law can keep going. The rapid development of semiconductor industry and chips can become smaller and cheaper are closely related to the progress of lithography.For a long time, optical lithography is the mainstream in semiconductor industry, it is superior to other lithography method because of its mass production with high speed and low cost. However, with chips size become smaller and smaller optical lithography has reached its limit, it is necessary to investigate a new method for lithography, E-beam (Electron Beam Lithography) and EUV (Extreme Ultraviolet Lithography) are the main research direction lithography method in the future.
In this thesis, we focus on how to reduce the proximity effect in electron beam lithography. We propose three method to solve proximity effect, including changing the resist, shortening the developing time, and reducing the developing temperature. After the experiment of changing resist, we compare the pros and cons in different resist, and we choose the most suitable resist for our subsequent experiment. Then we use the electron beam system to design single spot experiment and observing the diameter broadening of spots by changing exposure dose and developing condition. Through the experiment result, we found that by combining the short time and low temperature development we can reduce the proximity effect substantially. We further use the experiment result and traditional electron scattering research to derive our model for short interval development, then we fitted our model with experiment data and found that it fitted very well and every coefficient in our model have a good physical meaning. We next use our model to write different pitch lines pattern, and succeed in making 9nm small line width and 30nm small pitch line patterns, and also proved our single spot experiment result can apply to write line patterns and have the same trend. Finally, we use reactive ion etch and evaporation to transfer our pattern to silicon substrate successfully. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-15T12:42:29Z (GMT). No. of bitstreams: 1 ntu-105-R03943061-1.pdf: 4984214 bytes, checksum: 9f36dd9174d6368dbd2e8eba242b1ccb (MD5) Previous issue date: 2016 | en |
| dc.description.tableofcontents | 目錄
口試委員審定書 I 誌謝 II 摘要 III Abstract IV 目錄 VI 圖目錄 VIII 表目錄 X 第一章 概論 1 1.1.前言 1 1.2研究動機 2 1.3章節概要 2 第二章 電子束微影製程理論探討 4 2.1微影製程介紹 4 2.1.1光學微影 4 2.1.2電子束微影 5 2.2 電子散射原理 6 2.2.1電子散射 6 2.2.2 鄰近效應與電荷累積 7 2.3 電子散射模型 7 2.3.1傳統散射模型 7 2.3.2 圈環法(Doughnut mehod) 9 第三章 電子束低溫短顯影製程與量測方法 12 3.1 電子束低溫短顯影製程與量測機台介紹 12 3.1.1 電子束微影系統 12 3.1.2 電子槍蒸鍍系統 13 3.1.3 反應式離子蝕刻系統 (Reactive Ion Etching, RIE) 13 3.1.4 冷凍循環水槽 14 3.1.5掃描式電子顯微鏡(Scanning Electron Microscope, SEM) 15 3.1.6聚焦離子束(Focus Ion Beam, FIB) 16 3.2 製程步驟與參數 16 3.2.1電子束微影製程技術 17 3.2.2圖形轉移技術 20 3.3 實驗設計及量測方法 21 3.3.1單點實驗設計 21 3.3.2單點圖形量測方法 22 3.3.3.奈米週期線圖案設計 23 第四章 實驗數據結果與討論 25 4.1 不同電子阻的比較 25 4.1.1不同電子阻的單點實驗結果 25 4.1.2不同電子阻的優缺點分析 27 4.2 不同顯影條件的比較 27 4.2.1 短顯影時間條件下的單點實驗 28 4.2.2溫度降低對顯影機制的影響 28 4.2.3不同溫度下的單點實驗 30 4.3短顯影速率模型 31 4.3.1 短顯影速率模型推導 31 4.3.2 常溫模型擬合結果與參數分析 34 4.3.3 變溫條件下模型擬合結果與參數分析 37 4.3.4 鄰近效應影響範圍R2討論 38 4.4 模型運用 39 4.4.1短顯影散射模型運用於奈米線圖形 39 4.4.2不同週期的奈米線 40 4.5 奈米圖形轉移 44 第五章 結論與未來展望 46 5.1 結論 46 5.2未來研究方向 46 參考文獻 47 | |
| dc.language.iso | zh-TW | |
| dc.subject | 鄰近效應 | zh_TW |
| dc.subject | 鄰近效應 | zh_TW |
| dc.subject | 電子束微影 | zh_TW |
| dc.subject | 顯影速率 | zh_TW |
| dc.subject | 電子散射 | zh_TW |
| dc.subject | 小線寬圖形 | zh_TW |
| dc.subject | 圖形轉移 | zh_TW |
| dc.subject | 圖形轉移 | zh_TW |
| dc.subject | 小線寬圖形 | zh_TW |
| dc.subject | 電子散射 | zh_TW |
| dc.subject | 顯影速率 | zh_TW |
| dc.subject | 電子束微影 | zh_TW |
| dc.subject | proximity effect | en |
| dc.subject | E-beam lithography | en |
| dc.subject | developing rate | en |
| dc.subject | electron scattering | en |
| dc.subject | small line width pattern | en |
| dc.subject | pattern transfer | en |
| dc.subject | E-beam lithography | en |
| dc.subject | proximity effect | en |
| dc.subject | developing rate | en |
| dc.subject | electron scattering | en |
| dc.subject | small line width pattern | en |
| dc.subject | pattern transfer | en |
| dc.title | 電子束微影之低溫短顯影研究 | zh_TW |
| dc.title | Investigation of electron beam lithography with the low-temperature short-interval development technology | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 104-2 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 孫允武,孫建文,徐大正,陳啟東 | |
| dc.subject.keyword | 電子束微影,鄰近效應,顯影速率,電子散射,小線寬圖形,圖形轉移, | zh_TW |
| dc.subject.keyword | E-beam lithography,proximity effect,developing rate,electron scattering,small line width pattern,pattern transfer, | en |
| dc.relation.page | 49 | |
| dc.identifier.doi | 10.6342/NTU201601447 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2016-07-27 | |
| 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 |
| Appears in Collections: | 電子工程學研究所 | |
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| ntu-105-1.pdf Restricted Access | 4.87 MB | Adobe PDF |
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