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研究生:盧頴新
研究生(外文):Ying-Hsin Lu
論文名稱:前瞻式金氧半場效電晶體之可靠度與熱載子劣化研究
論文名稱(外文):Investigation on the Reliability and Hot Carrier degradation in Advance MOSFET
指導教授:張鼎張
指導教授(外文):Ting-Chang Chang
學位類別:博士
校院名稱:國立中山大學
系所名稱:物理學系研究所
學門:自然科學學門
學類:物理學類
論文種類:學術論文
論文出版年:2018
畢業學年度:107
語文別:英文
論文頁數:147
中文關鍵詞:金氧半場效電晶體、矽覆絕緣、鰭式電晶體、熱載子劣化、偏壓不穩定性
外文關鍵詞:MOSFETs、SOI、FinFETs、hot carrier degradation、BTI
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  • 收藏至我的研究室書目清單書目收藏:0
自1960年,世界上第一顆電晶體由Bell實驗室的D. Kahng和Martin Atalla首次實作成功。此時電晶體的通道長度還維持在25 微米(μm),氧化層厚度為100 奈米(nm)。五年後,Intel創辦人之一Gordon Moore提出 “Moore’s Law”,其內容為: 積體電路上可容納的電晶體,約每隔兩年便會增加一倍。並且隨著科技的進步,10奈米的鰭式電晶體(FinFET)已經順利量產並應用至高端電子產品當中。在積體電路的微縮工程上,除了通道長度的微縮工程作為首要關鍵技術以外;調變積體電路中起始電壓(Threshold Voltage, Vth)也是的重要關鍵技術之一。例如,超薄氧化層、通道的離子佈植調製、閘極堆疊調製…等。而在不同的調製手法都將對電晶體的基本電性以及可靠度帶來不一樣的影響。
因此,我們在第一部分主要針對閘極堆疊調製中的金屬退火順序做研究。在此章節,我們研究金屬前/後金屬沉積退火對於二氧化鉿層的影響。並透過基本電性與負偏壓溫度不穩定性(Negative-Bias-Temperature Instability ,NBTI)探討其影響。在初始電性中,最明顯的差異是由閘極材料和半導體之間的功函數差異導致臨界電壓(Vth)的不同。 此外,快速量測的結果顯示,金屬沉積後退火的元件在NBTI後有更嚴重的Vth劣化,這源於HfO2中更多的氮間隙缺陷。並且,透過快速雙掃描量測(Fast I-V Double Sweep)的分析,我們證實了這種現象是由於製作過程中所產生的缺陷所致。
為了更進一步驗證氮間隙缺陷對於元件的影響,在第二部份我們使用快速測量研究不同TiN閘極的氮濃度對HfO2層中間隙陷阱的影響。 在前一章節,我們透過快速量測以及NBTI,發現了氮間隙缺陷的存在。在本章節中,我們可以進一步發現金屬中氮含量越高,並受到熱擴散的影響,使得在二氧化鉿層會存有更多的氮間隙缺陷。在可靠度方面,由於氮間隙缺陷在二氧化鉿層中扮演著電洞捕獲中心的存在。因此,在常溫下進行NBTI時,我們觀察到電晶體劣化的主因大部分是由於電洞捕獲現象,而非傳統Reaction-Diffusion Model所導致的次臨界擺福(Subthreshold Swing,S.S.)下降。並且,透過NBTI前後的快速雙掃描量測,可以發現擁有較多氮間隙缺陷的元件,在劣化後會有較大的遲滯現象。這也代表著二氧化鉿層內部的鍵結受到氮間隙缺陷的影響,更容易斷鍵形成新的電洞捕獲中心。
針對第一與第二部分的氮鍵隙缺陷。在第三部分,我們透過氮化處理個過程,進而消除二氧化鉿層中的氧空位與氮間隙缺陷。根據以往的研究,氧化鉿中的氧空位可以通過擴散氮鈍化,從而提高n-MOSFET的性能和可靠性。另一方面,對於p-MOSFET元件,氮擴散到溝道界面中以產生界面缺陷,導致元件的S.S.退化。但是,當HfO2薄膜中的氮濃度較高時,相對應的會產生更多氮間隙缺陷。這些間隙缺陷位於HfO2中,缺陷能量深度靠近價電帶的位子。因此,當電洞從通道傳輸到柵極時,電洞會被捕獲到氮間隙缺陷中。在這個部份,我們研究了氮化時間的減少和元件的退火時間,以進一步改善氧化鉿層的氮和氧空位鍵合,並減少氮界面缺陷。還研究了不同氮濃度和退火時間對器件性能和可靠性的影響。
最後,在MOSFET技術的演進中,除了在Moore’s Law中演進的電晶體以外,另一個研究的方向則是在於增加功能的多樣性,稱為More than More。在其發展的部分,包含了眾多不同功能的元件,如RF、高壓元件、CMOS image sensor等,此章節我們將討論在silicon-on-insulator(SOI)元件中的異常恢復現象做討論。通過不同的熱載流子劣化(HCD)測量序列可以闡明電洞注入導致異常恢復的行為。 根據HCD結果,通道表面能帶因為電洞注入的關係,能帶下拉並且暫時屏蔽界面缺陷。 此外,不同電壓應力的實驗結果表明,電洞注入的量是由閘極和漏極之間的電場所決定。
Since 1960, the world’s the first metal-oxide-semiconductor-field-effect transistors (MOSFETs) were invented by Kahng and Atalla in Bell Lab. The transistor length is 25 μm, and gate oxide thickness is 100nm. Nowadays, MOSFETs have become the dominant devices for ultra-large-scale integration (ULSI) circuits due to its low cost, power consumption and easy to scale down. In 1965, Gordon Moore, one of Intel''s founders, first proposed Moore’s Law: The number of components per integrated circuit will doubling every year. And with the advancement of technology, the 10 nm fin transistor (fin FET) has been mass-produced and applied to advance electronic products. In the micro-engineering of the integrated circuit, in addition to the miniaturization of the channel length as the primary key technology; the threshold voltage (Vth) in the modulated integrated circuit is also one of the key technologies. For example, ultra-thin oxide layers, ion implantation modulation of channels, gate stack modulation, etc. Different modulation methods will have different effects on the basic electrical properties and reliability of the transistor.
Therefore, in the first part, we mainly study the metal annealing sequence in gate stack modulation. In this section, we study the effect of metal pre/post metal deposition annealing on the cerium oxide layer. In the initial electrical characteristics, the most apparent difference is threshold voltage (Vth) resulting from the work-function difference between the gate material and the semiconductor. Furthermore, fast I-V measurements indicate that the device with post-metal deposition annealing shows more degradation of Vth in NBTI, which originates from the more nitrogen interstitial defects in HfO2. This phenomenon is confirmed to be due to the process-related pre-existing defects by an analysis of double sweep fast I-V measurements.
In order to further verify the effect of nitrogen interstitial defects on the MOSFET, in the second part we used fast I-V measurements to study the effect of different TiN gate nitrogen concentrations on the interstitial defect in the HfO2 layer. In the previous section, we discovered the existence of nitrogen interstitial defects through fast I-V measurement and NBTI. In this part, we can further find that the higher nitrogen content in the metal, and the nitrogen is affected by the thermal diffusion, the more nitrogen interstitial defects will exist in the HfO2 layer. In the reliability, the nitrogen interstitial defect takes the role of the hole trapping center in the HfO2 layer. Therefore, when performing NBTI at room temperature, we observed that the main cause of transistor degradation is mostly due to hole trapping, rather than the decline of Subthreshold Swing (S.S.) caused by the traditional Reaction-Diffusion Model. Moreover, through the fast I-V double sweep measurement after NBTI, it can be found that devices with more nitrogen interstitial defects have a large hysteresis after deterioration. This also means that the bond inside the HfO2 layer is affected by the nitrogen interstitial defect, and it is easier to break the bond to form a new hole capture center.
Therefore, for the nitrogen interstitial defects for the first and second portions. In the third part, we eliminate the oxygen vacancies and nitrogen interstitial defects in the HfO2 layer by different nitridation process. Based on previous studies, the oxygen vacancy in hafnium oxide could be passivated by the diffusion nitrogen, thus, enhancing the performance and reliability of n-MOSFET. On the other hand, as for p-MOSFET device, the nitrogen diffuses into the channel interface to generate interface defects, causing S.S. degradation to the device. However, in the HfO2 thin film, the nitrogen interstitial defect will be generated when the concentration of nitrogen is higher. These interstitial defects are located in HfO2 with the energy level below the mid-gap. Therefore, the holes can be trapped into the nitrogen interstitial defects while they transport from the channel to the gate. This work investigates the reduction of nitridation time and annealing time to device to further verify the hafnium oxide layer of nitrogen and oxygen vacancies bonding to reduce nitrogen interface defects. The influence of different nitrogen concentration and annealing time to device performance and reliability are also investigated.
Finally, In the evolution of MOSFET technology, in addition to the evolution of the transistor in Moore''s Law, another research direction is to increase the diversity of functions, called More than More. In its development, it contains many different functional components, such as RF, high voltage components, CMOS image sensor, etc. In this section we will discuss an abnormal recovery phenomenon induced by hole injection during hot carrier degradation in silicon-on-insulator n-type metal-oxide-semiconductor transistors. How the hole injection induces the abnormal recovery behavior can be clarified by different hot carrier degradation (HCD) measurement sequences. According to this HCD result, the channel surface energy band is drawn down and the interface defect will be temporarily shielded, an effect caused by the trapped hole. Furthermore, results of different stress voltage experiments indicate that the amount of hole injection is determined by the electric field between the gate and drain.
摘要 iii
Abstract vi
Figure Captions xiii
Chapter 1 1
1.1 Basic Background 1
1.1.1 Overview of Moore’s Law, Roadmap of scaling down 1
1.1.2 Overview of high-k/metal gate MOSFETs and FinFETs 3
1.1.3 Overview of Silicon-on-Insulator (SOI) MOSFETs 4
Reference 7
Chapter 2 Parameter Extraction and Measurement Technique 16
2.1 Method of Device Parameter Extraction 16
2.1.1 Determination of threshold voltage (VT) 16
2.1.2 Determination of the subthreshold swing 18
2.1.3 Determination of the low-field effect mobility 19
2.2 Method of Device Parameter Extraction 19
2.2.1 Charge pumping technique 20
2.2.2 Fast I-V Technique 21
Reference 22
Chapter 3 30
3.1 Introduction 31
3.2 Experiment 32
3.3 Result and Discussion 33
3.4 Summary 38
Reference 39
Chapter 4 49
4.1 Introduction 50
4.2 Experiment 51
4.3 Result and Discussion 52
4.4 Summary 58
Reference 60
Chapter 5 71
5.1 Introduction 71
5.2 Experiment 73
5.3 Result and Discussion 74
5.4 Summary 80
Reference 82
Chapter 6 94
6.1 Introduction 94
6.2 Experiment 95
6.3 Result and Discussion 96
6.4 Summary 102
Reference 104
Conclusion 118
Publication List 122
Vita 簡 歷 127
[1.1] Moore, Gordon. "Progress In Digital Integrated Electronics" (PDF). Retrieved July 15,2015.
[1.2] http://www.intel.com/content/www/us/en/silicon-innovations/advancing-moores-law-in-2014-presentation.html
[1.3] http://www.intel.com/content/www/us/en/silicon-innovations/standards-22nm-3d-tri-gate-transistors-presentation.html.
[1.4] J. Robertson, etl. “Band structures and band offsets of high K dielectrics on Si,” Appied Surface Science, vol. 190, pp. 2-10, 2002
[1.5] C. Kang, “A study on the material and device characteristics of hafnium oxynitride MOSFETs with TaN gate electrodes”, PhD Dissertation, University of Texas at Austin, 2004.
[1.6] John Robertson, “Band offsets of wide-band-gap oxides and implications for future electronic devices”, Journal of Vacuum Science & Technology B:Microelectronics and Nanometer Structures, vol. 18(2000),Issue 3, p. 1785
[1.7] Alpa Dashora, N. Patel, D.C. Kothari, B.L. Ahuja, A. Miotello, “Formation of an intermediate band in the energy gap of TiO2 by Cu–N-codoping: First principles study and experimental evidence” Solar Energy Materials & Solar Cells 125 (2014) 120–126
[1.8] C. H. Dai, T. C. Chang, A. K. Chu, Y. J. Kuo, Y. C. Hung, W. H. Lo, S. H. Ho, C. E. Chen, J. M. Shih, W. L. Chung et al.,” Charge trapping induced frequency-dependence degradation in n-MOSFETs with high-k/metal gate stacks,” Thin Solid Films, 520, 1511 (2011).
[1.9] M. Chang, M. Jo, S. Jung, J. Lee, S. Jeon, and H. Hwang, “Transient charge trapping and detrapping properties of a thick SiO 2 / Al 2 O 3 stack studied by short single pulse I d - V g,”Appl. Phys. Lett., 94, 262107 (2009).
[1.10] W. J. Zhu, Member, IEEE, and T. P. Ma, Fellow,” Temperature Dependence of Channel Mobility in HfO2-Gated NMOSFETs,” IEEE Electron Device Lett., 25, 2, p.89-p.91 (2004).
[1.11] R. Chau, Senior Member, IEEE, S. Datta, Member, IEEE, M. Doczy, B. Doyle, J. Kavalieros, and M.Metz,” High-/Metal–Gate Stack and Its MOSFET Characteristics,” Electron Devices Lett., 25, 6, p.408-p.410 (2004).
[1.12] T.-s. Park, S. Choi, D. Lee, J. Yoo, B. Lee, J. Kim, et al., "Fabrication of body-tied FinFETs (Omega MOSFETs) using bulk Si wafers," in VLSI Technology, 2003. Digest of Technical Papers. 2003 Symposium on, 2003, pp. 135-136.
[1.13] T.-S. Park, H. J. Cho, J. D. Choe, I. H. Cho, D. Park, E. Yoon, et al., "Characteristics of body-tied triple-gate pMOSFETs," IEEE electron device letters, vol. 25, pp. 798-800, 2004.
[1.14] J. W. Lee, Y. Sasaki, M. J. Cho, M. Togo, G. Boccardi, R. Ritzenthaler, et al., "Plasma doping and reduced crystalline damage for conformally doped fin field effect transistors," Applied Physics Letters, vol. 102, p. 223508, 2013.
[1.15] K. Eriguchi, "Modeling of plasma-induced damage during the etching of ultimately-scaled transistors in ULSI circuits--A model prediction of damage in three dimensional structures," in APS Meeting Abstracts, 2014, p. 2004.
[1.16] P. Aminzadeh, M. Alavi, and D. Scharfetter, "Temperature dependence of substrate current and hot carrier-induced degradation at low drain bias," in VLSI Technology, 1998. Digest of Technical Papers. 1998 Symposium on, 1998, pp. 178-179.
[1.17] T. Kamata, K. Tanabashi, and K. Kobayashi, "Substrate current due to impact ionization in MOS-FET," Japanese Journal of Applied Physics, vol. 15, p. 1127, 1976.
[1.18] S. Ramaswamy, A. Amerasekera, and M.-C. Chang, "A unified substrate current model for weak and strong impact ionization in sub-0.25/spl mu/m NMOS devices," in Electron Devices Meeting, 1997. IEDM''97. Technical Digest., International, 1997, pp. 885-888.
[1.19] P. Olejarz, K. Park, S. MacNaughton, M. R. Dokmeci and S. Sonkusale, “0.5 μW Sub-Threshold Operational Transconductance Amplifiers Using 0.15 μm Fully Depleted Silicon-on-Insulator (FDSOI) Process” J. Low Power Electron. Appl. 2012, 2, 155-167
[1.20] X. Luo, Y. G. Wang, T. F. Lei, L. Lei, D. P. Fu, G. L. Yao, M. Qiao, B. Zhang, Z. Li, “Novel High Voltage LDMOS on Partial SOI with double-sided Charge Trenches,” in IEEE ISPSD, pp. 76-79 (2011).
[2.1] D. K. Schroder, Semiconductor material and device characterization: John Wiley & Sons, 2006.
[2.2] J. S. Brugler and P. G. A. Jerpers, “Charging Pumping in MOS Device”, IEEE Trans. Electron Devices. ED-16, pp. 297 (1969).
[2.3] G. Groeseneken, H. E. Maes, N. Beltran and R. F. De Keersmeacker, “A Reliable Approach to Charge-Pumping Measurement in MOS transistors”, IEEE Trans. Rlrctron Devices, ED-31, pp. 42 (1984).
[2.4] P. Heremans, J. Witters, G. Groeseneken and H. E. Maes, “Analysis of the Charge Pumping Technigue and Its Application for Evaluation of MOSFET Degradation”, IEEE Trans. Electron Device, 36, pp.1318 (1989).
[2.5] Dieter K. Schroder, “Semiconductor Material And Device Characterization,” p.355
[2.6] Man Chang, Minseok Jo, Seungjae Jung, Joonmyoung Lee, Sanghun Jeon, and Hyunsang Hwang,” Transient charge trapping and detrapping properties of a thick SiO2/Al2O3 stack studied by short single pulse Id-Vg ,” Applied Physics Lett., 94, 262107 (2009)
[3.1]T. C. Chang, F. Y. Jian, S. C. Chen, and Y. T. Tsai, Mater. Today 14, 608 (2011).
[3.2]M. C. Chen, T. C. Chang, C. T. Tsai, S. Y. Huang, S. C. Chen, C. W. Hu, S. M. Sze, and M. J. Tsai, Appl. Phys. Lett. 96, 262110 (2010).
[3.3]Y. C. Chen, T. C. Chang, H. W. Li, S. C. Chen, J. Lu, W. F. Chung, Y. H. Tai, and T. Y. Tseng, Appl. Phys. Lett. 96, 262104 (2010).
[3.4]M. C. Chen, T. C. Chang, S. Y. Huang, K. C. Chang, H. W. Li, S. C. Chen, J. Lu, and Y. Shi, Appl. Phys. Lett. 94, 162111 (2009).
[3.5]S. W. Tsao, T. C. Chang, S. Y. Huang, M. C. Chen, S. C. Chen, C. T. Tsai, Y. J. Kuo, Y. C. Chen, and W. C. Wu, Solid-State Electron. 54, 1497 (2010).
[3.6]S. H. Ho, T. C. Chang, C. W. Wu, W. H. Lo, C. E. Chen, J. Y. Tsai, H. P. Luo,T. Y. Tseng, O. Cheng, C. T. Huang, and S. M. Sze, Appl. Phys. Lett. 101, 052105 (2012).
[3.7]K. Joshi, S. Mukhopadhyay, N. Goel and S. Mahapatra, IEEE IRPS, 5A.3.1 (2012).
[3.8]G. Bersuker, J. H. Sim, C. D. Young, R. Choi, P. M. Zeitzoff, G. A. Brown, B. H. Lee, and R. W. Murto, Microelectron. Reliab. 44, 1509 (2004).
[3.9]H. R. Harris, R. Choi, J. H. Sim, C. D. Young, P. Majhi, B. H. Lee, and G. Bersuker, IEEE Electron Device Lett. 26, 839 (2005).
[3.10]S Mahapatra, N Goel, S Desai, S Gupta, B Jose S. Mukhopadhyay, K. Joshi, A. Jain, A. E. Islam, Member, IEEE, and M. A. Alam, Fellow, IEEE, IEEE Trans. Electron Devices, 60, 901 (2013).
[3.11]S. H. Ho, T. C. Chang, Y. H. Lu, C. E. Chen, J. Y. Tsai, K. J. Liu, T. Y. Tseng, O. Cheng, C. T. Huang, and C. S. Lu, Appl. Phys. Lett. 104, 113503 (2014).
[3.12]H. Küflüo˜glu, and M.A. Alam, Electron Devices, IEEE Transactions on. 54, 1101 (2007) .
[3.13]D. S. Ang and S. Wang, IEEE Electron Device Lett. 27, 914 (2006).
[3.14]C. Z. Zhao and J. F. Zhang, Appl. Phys. Lett. 97, 073703 (2005).
[3.15]D. Ielmini, M. Manigrasso, F. Gattel, and G Valentini, IEEE IRPS, 26, (2009).
[3.16]T. Grasser, B. Kaczer, W. Goes, Th. Aichinger, Ph. Hehenberger, and M. Nelhiebel, IEEE IRPS, 33 (2009).
[3.17]M. Denais, V. Huard, C. Parthasarathy, G. Ribes, F. Perrier, N. Revil, and A. Bravaix, IEEE Trans. Device Mater. Reliab. 4, 715 (2004).
[3.18]M. Choi, J. L. Lyons, A. Janotti, and C. G. Van de Walle, Appl. Phys. Lett. 102, 142902 (2013).
[4.1] T.-C. Chang, F.-Y. Jian, S.-C. Chen, and Y.-T. Tsai, "Developments in nanocrystal memory," Materials today, vol. 14, pp. 608-615, 2011.
[4.2] M.-C. Chen, T.-C. Chang, C.-T. Tsai, S.-Y. Huang, S.-C. Chen, C.-W. Hu, et al., "Influence of electrode material on the resistive memory switching property of indium gallium zinc oxide thin films," Applied Physics Letters, vol. 96, p. 262110, 2010.
[4.3] Y. C. Chen, T. C. Chang, H. W. Li, S. C. Chen, J. Lu, W. F. Chung, Y. H. Tai, and T. Y. Tseng, Appl. Phys. Lett. 96, 262104 (2010).
[4.4] Y. T. Tsai, T. C. Chang, C. C. Lin, S. C. Chen, C. W. Chen, S. M. Sze, F. S. Yeh, and T. Y. Tseng, Electrochemical and Solid State Lett. 14, H135 (2011).
[4.5] W. R. Chen, T. C. Chang, J. L. Yeh, S. M Sze, and C. Y. Chang, Appl. Phys. Lett. 92, 152114 (2008).
[4.6] T. Yang M. F. Li ; C. Shen ; C. H. Ang ; Chunxiang Zhu ; Y. C. Yeo ; G. Samudra ; S. C. Rustagi ; M. B. Yu and, D.L. Kwong, Dig. Tech. Pap. - Symp. VLSI Technol. 2005, 14.
[4.7] Y. H. Lu, T.C. Chang, S.H. Ho, C.E. Chen, J.Y. Tsai, K.J. Liu, X.W. Lia, T.Y. Tseng, O. Cheng, C.T. Huang and C.S. Lu, ECS Solid State Lett. 4, 37 (2015).
[4.8] S. Mahapatra, K. Ahmed, D. Varghese, A. E. Islam, G. Gupta, L. Madhav, D. Saha, and M. A. Alam, Reliability Physics Symposium (IRPS), 2007, 15.
[4.9] W. C. Wu, T.S. Chao, T.H. Chiu, J.C. Wang, C.S. Lai, M.W. Ma, and W.C. Lo, IEEE Electron Device Lett. 29, 1340 (2008).
[4.10] E.C. Lee, Phys. Rev. B 77, (2008) 104108.
[4.11] J. Robertson and C. W. Chen, “Schottky barrier heights of tantalum oxide, barium strontium titanate, lead titanate, and strontium bismuth tantalate,’’ Appl. Phys. Lett, vol. 74, no. 8, pp. 1168 Feb. 1999.
[4.12] N. Mise, M. Kadoshima, T. Morooka, T. Eimori, Y. Nara, and Y. Ohji, “Universal Correlation between Flatband Voltage and Electron Mobility in TiN/HfSiON Devices with MgO or La2O3 Incorporation and Stack Variation,’’ J. Appl. Phys. vol. 47, no. 10, pp. 7780, Oct. 2008.
[4.13] E. P. Gusev, H. -C. Lu ; E. L. Garfunkel ; T. Gustafsson ; M. L. Green, “Growth and characterization of ultrathin nitrided silicon oxide films,” IBM J. Res. & Dev., vol. 43, no. 3, pp. 265. May. 1999.
[4.14] R. Choi, C.S. Kang, B.H. Lee, K. Onishi, R. Nieh, S. Gopalan, E. Dharmarajan, and J. C. Lee, “High-quality ultra-thin HfO/sub 2/ gate dielectric MOSFETs with TaN electrode and nitridation surface preparation,’’ Dig. Tech. Pap. - Symp. VLSI Technol., pp. 15. Jun. 2001.
[4.15] H. Küflüo˜glu, and M.A. Alam, IEEE Trans. Electron Devices 54, 1101 (2007).
[4.16] D. K. Schroder and J.A. Babcock, J. Appl. Phys. 94, 1 (2003).
[4.17] X. Garros, M. Cassé, G. Reimbold, F. Martin, C. Leroux, A. Fanton, O. Renault, V. Cosnier, and F. Boulanger, Dig. Tech. Pap. - Symp. VLSI Technol. 2008, 68.
[4.18] S. Mahapatra, K. Ahmed, D. Varghese, A. E. Islam, G. Gupta, L. Madhav, D. Saha, and M. A. Alam, IEEE Trans. Device Mater. Reliab. 60, 901 (2013).
[4.19] C.H. Liu, M.T. Lee, C.Y. Lin, J. Chen, Y.T. Loh, F.T. Liou, K. Schruefer, A.A. Katsetos, Z.Yang, and N. Rovedo, J. Appl. Phys. 41, 2423 (2002).
[4.20] J. L. Gavartin, A. L. Shluger, A. S. Foster, and G. I. Bersuker, J. Appl. Phys. 97, 053704 (2005).
[4.21] M. Choi, J.L. Lyons, A. Janotti, and C.G. Van de Walle, Appl. Phys. Lett. 102, 142902 (2013).
[5.1] T. Yang M. F. Li ; C. Shen ; C. H. Ang ; Chunxiang Zhu ; Y. C. Yeo ; G. Samudra ; S. C. Rustagi ; M. B. Yu and, D.L. Kwong, “Fast and Slow Dynamic NBTI components in p-MOSFET with SiON dielectric and their impact on device life-time and circuit application,” Dig. Tech. Pap. - Symp. VLSI Technol. pp. 14, Jun. 2005.
[5.2] Y. H. Lu, T.C. Chang, S.H. Ho, C.E. Chen, J.Y. Tsai, K.J. Liu, X.W. Lia, T.Y. Tseng, O. Cheng, C.T. Huang and C.S. Lu, “The Impact of Pre/Post-metal Deposition Annealing on Negative-Bias-Temperature Instability in HfO2 Stack p-Channel Metal-Oxide-Semiconductor Field Effect Transistors,” ECS Solid State Lett. vol. 4, no. 8, pp. 37 Jun. 2015.
[5.3] S. Mahapatra, K. Ahmed, D. Varghese, A. E. Islam, G. Gupta, L. Madhav, D. Saha, and M. A. Alam, “On the Physical Mechanism of NBTI in Silicon Oxynitride p-MOSFETs: Can Differences in Insulator Processing Conditions Resolve the Interface Trap Generation versus Hole Trapping Controversy?,” Reliability Physics Symposium (IRPS), pp. 15, May. 2007.
[5.4] W. C. Wu, T. S. Chao, T. H. Chiu, J. C. Wang, C. S. Lai, M. W. Ma, and W. C. Lo, IEEE Electron Device Lett. 29, 1340 (2008).
[5.5] X. Garros, M. Cassé, G. Reimbold, F. Martin, C. Leroux, A. Fanton, O. Renault, V. Cosnier and F. Boulanger,” Guidelines to improve mobility performances and BTI reliability of advanced High-K/Metal gate stacks,” 2008 Symposium on VLSI Technology Digest of Technical Papers, p.68-p.69 (2008)
[5.6] E. C. Lee, “Nitrogen-induced interface defects in Si oxynitride,” Phys. Rev. B, vol. 77, no. 10, pp. 104108, Mar. 2008. DOI: 10.1103/PhysRevB.77.104108
[5.7] G. Lucovsky, Z. Jing, and D. R. Lee, “Defect properties of Si-, O-, N-, and H-atoms at Si—SiO2 interfaces”, Journal of Vacuum Science & Technology B 14, 2832 (1996).
[5.8] C. P. Ewels, R. Jones, S. Öberg, J. Miro and P. Deák, “Shallow Thermal Donor Defects in Silicon”, Physical Review Letters, vol. 77, no. 5, 865-868, (1996).
[5.9] H.Wakabayashi, Y. Saito, K. Takeuchi, T. Mogami, and T. Kunio, “A Dual-Metal Gate CMOS Technology Using Nitrogen-Concentration-Controlled TiNx Film”, IEEE Transactions on Electron Devices, vol. 48, no. 10, 2001.
[5.10] J. L. Gavartin, A. L. Shluger, A. S. Foster, and G. I. Bersuker, “The role of nitrogen-related defects in high-k dielectric oxides: Density-functional studies” Journal of Applied Physics 97, 053704 (2005)
[5.11] M. Choi, J. L. Lyons, A. Janotti, and C. G. Van de Walle, “Impact of carbon and nitrogen impurities in high-k dielectrics on metal-oxide-semiconductor devices”, Applied Physics Letters 102, 142902 (2013).
[5.12] C. H. Choi, T. S. Jeon, R. Clark, and D. L. Kwong, “Electrical Properties and Thermal Stability of CVD HfOxNy Gate Dielectric With Poly-Si Gate Electrode” IEEE Electron Device Lett. 24, 215 (2003).
[5.13] C. S. Kang, H. J. Cho, K. Onishi, R. Nieh, R. Choi, S. Gopalan, S. Krishnan, J. H. Han, and J. C. Lee, “Bonding states and electrical properties of ultrathin HfOxNy gate dielectrics”, Applied Physics Letters 81, 2593 (2002).
[5.14] J. F. Zhang and W. Eccleston, “Positive Bias Temperature Instability in MOSFET’s”, IEEE Transactions on Electron Devices, vol. 45, no. 1, 1998.
[5.15] J. F. Zhang, S. Taylor, and W. Eccleston, “Electron trap generation in thermally grown SiO2 under Fowler-Nordheim stress”, Journal of Applied Physics 71, 725 (1992)
[5.16] A. I. Chou, K. Lai, K. Kumar, P. Chowdhury, and J. C. Lee, “Modeling of stress-induced leakage current in ultrathin oxides with the trapassisted tunneling mechanism”, Appl. Phys. Lett. 70, 3407 (1997).
[5.17] D. J. Dumin, and J. R. Maddux, “Correlation of Stress-Induced Leakage Current in Thin Oxides with Trap Generation Inside the Oxides”,
[5.18] S. I. Takagi, N. Yasuda, and A. Toriumi, “A New I–V Model for Stress-Induced Leakage Current Including Inelastic Tunneling”, IEEE Transactions on Electron Devices, vol. 46, no. 2, 1999.
[5.19] S. Mahapatra, N. Goel, S. Desai, S. Gupta, B. Jose, S. Mukhopadhyay, K. Joshi, A. Jain, A. E. Islam, and M. A. Alam, “A Comparative Study of Different Physics-Based NBTI Models” IEEE Transactions on Electron Devices, vol. 60, no. 3, 2013.
[5.20] K. Joshi, S. Mukhopadhyay, N. Goel, and S. Mahapatra, “A Consistent Physical Framework for N and P BTI in HKMG MOSFETs”, 2012 IEEE International Reliability Physics Symposium (IRPS)
[5.21] H. Küflüo˜glu, and M.A. Alam, “A Generalized Reaction–Diffusion Model with Explicit H–H2 Dynamics for Negative-Bias Temperature-Instability (NBTI) Degradation”, IEEE Trans. Electron Devices, 54, 1101 (2007).
[5.22] K. O. Jeppson and C. M. Svensson, “Negative bias stress of MOS devices at high electric fields and degradation of MNOS devices”, Journal of Applied Physics 48, 2004 (1977).
[5.23] S. M. Sze and Kwok K. NG, “Physics of Semiconductor Devices”, Third Edition, p227.
[5.24] K. Xiong, J. Robertson, M. C. Gibson, and S. J. Clark, “Defect energy levels in HfO2 high-dielectric-constant gate oxide”.
[5.25] H. Takeuchi, D. Ha, and T. J. King, “Observation of bulk HfO2 defects by spectroscopic ellipsometry”, Journal of Vacuum Science & Technology A 22, 1337 (2004).
[5.26] J. Robertson, “High dielectric constant oxides”, Phys. J. Appl. Phys. 28, 265–291 (2004).
[5.27] G. Brezeanu, M. Brezeanu, and F. Bernea, “High-K Dielectrics in Nanoµelectronics”, Nat''l Seminar of Nanoscience & Nanotechnology, September edition. 2010.
[5.28] Shimeng Yu, X. Guan, and H. S. Philip Wong, “Conduction mechanism of TiN/HfOx/Pt resistive switching memory: A trap-assisted-tunneling model”, Appl. Phys. Lett. 99, 063507 (2011).
[6.1] T.-C. Chang, F.-Y. Jian, S.-C. Chen, and Y.-T. Tsai, “Developments in nanocrystal memory,” Mater. Today, vol. 14, no. 12, pp. 608-615, Dec. 2011.
[6.2] M.-C. Chen, T.-C. Chang, C.-T. Tsai, S.-Y. Huang, S.-C. Chen, C.-W. Hu, S. M. Sze, and M.-J. Tsai, “Influence of electrode material on the resistive memory switching property of indium gallium zinc oxide thin films,” App. Phys. Lett., vol. 96, no. 26, pp. 262110, Jun. 2010.
[6.3] Y. C. Chen, T. C. Chang, H. W. Li, S. C. Chen, J. Lu, W. F. Chung, Y. H. Tai, and T. Y. Tseng, “Bias-induced oxygen adsorption in zinc tin oxide thin film transistors under dynamic stress,” Appl. Phys. Lett. vol. 96, no. 26, pp. 262104, Jun. 2010.
[6.4] L.T. Su, J.E. Chung, D.A. Antoniadis, K.E. Goodson, and M.l. Flik, “Measurement and modeling of self-heating in SOI nMOSFET''s” IEEE Transactions on Electron Devices. vol. 41, no. 1, pp. 69, Aug. 2002.
[6.5] C. Hu, S.C. Tam, F.C. Hsu, P.K. Ko, T.Y. Chan, and K.W. Terrill, “Hot-Electron-Induced MOSFET Degradation-Model, Monitor, and Improvement” IEEE Transactions on Electron Devices. vol. 32, no. 2, pp. 375, Feb. 1985.
[6.6] C.H. Dai, T.C. Chang, A.K. Chu, Y.J. Kuo, F.Y. Jian, W.H. Lo, S.H. Ho, C.E. Chen, W.L. Chung, J.M. Shih, G. Xia, O. Cheng, and C.T. Huang, “On the Origin of Gate-Induced Floating-Body Effect in PD SOI p-MOSFETs,” IEEE Electron Device Lett., vol. 32, no. 7, pp. 847, Jul. 2011.
[6.7] S. Tyaginov and T. Grasser, “Modeling of hot-carrier degradation: Physics and controversial issues,” Integrated Reliability Workshop Final Report (IRW). pp. 206 Oct. 2012.
[6.8] T. Wang, C.T. Chan, C.J. Tang, C.W. Tsai, Howard C.H. Wang, M.H. Chi, and D.D. Tang, “A novel transient characterization technique to investigate trap properties in HfSiON gate dielectric MOSFETs-from single electron emission to PBTI recovery transient,” IEEE Transactions on Electron Devices. vol. 53, no. 5, pp. 1073, May. 2006.
[6.9] T.-C. Ong, M. Levi, P.-K. Ko, and C. Hu, “Recovery of threshold voltage after hot-carrier stressing,” IEEE Transactions on Electron Devices. vol. 35, no. 7, pp. 978, Jul. 1988.
[6.10] C.-H. Dai, T.-C. Chang, A.-K. Chu, Y.-J. Kuo, Y.-C. Hung, W.-H. Lo, et al., "Charge trapping induced frequency-dependence degradation in n-MOSFETs with high-k/metal gate stacks," Thin Solid Films, vol. 520, pp. 1511-1515, 2011.
[6.11] R. R. Troutman, "VLSI limitations from drain-induced barrier lowering," IEEE Journal of Solid-State Circuits, vol. 14, pp. 383-391, 1979.
[6.12] F.-C. Hsu, R. S. Muller, and C. Hu, "A simplified model of short-channel MOSFET characteristics in the breakdown mode," IEEE Transactions on Electron Devices, vol. 30, pp. 571-576, 1983.
[6.13] V. De and S. Borkar, "Technology and design challenges for low power and high performance," in Proceedings of the 1999 international symposium on Low power electronics and design, 1999, pp. 163-168.
[6.14] V. Subramanian, A. Mercha, B. Parvais, J. Loo, C. Gustin, M. Dehan, et al., "Impact of fin width on digital and analog performances of n-FinFETs," Solid-State Electronics, vol. 51, pp. 551-559, 2007.
[6.15] D. Hisamoto, W.-C. Lee, J. Kedzierski, H. Takeuchi, K. Asano, C. Kuo, et al., "FinFET-a self-aligned double-gate MOSFET scalable to 20 nm," IEEE Transactions on Electron Devices, vol. 47, pp. 2320-2325, 2000.
[6.16] T.-s. Park, S. Choi, D. Lee, J. Yoo, B. Lee, J. Kim, et al., "Fabrication of body-tied FinFETs (Omega MOSFETs) using bulk Si wafers," in VLSI Technology, 2003. Digest of Technical Papers. 2003 Symposium on, 2003, pp. 135-136.
[6.17] T.-S. Park, H. J. Cho, J. D. Choe, I. H. Cho, D. Park, E. Yoon, et al., "Characteristics of body-tied triple-gate pMOSFETs," IEEE electron device letters, vol. 25, pp. 798-800, 2004.
[6.18] J. W. Lee, Y. Sasaki, M. J. Cho, M. Togo, G. Boccardi, R. Ritzenthaler, et al., "Plasma doping and reduced crystalline damage for conformally doped fin field effect transistors," Applied Physics Letters, vol. 102, p. 223508, 2013.
[6.19] K. Eriguchi, "Modeling of plasma-induced damage during the etching of ultimately-scaled transistors in ULSI circuits--A model prediction of damage in three dimensional structures," in APS Meeting Abstracts, 2014, p. 2004.
[6.20] P. Aminzadeh, M. Alavi, and D. Scharfetter, "Temperature dependence of substrate current and hot carrier-induced degradation at low drain bias," in VLSI Technology, 1998. Digest of Technical Papers. 1998 Symposium on, 1998, pp. 178-179.
[6.21] T. Kamata, K. Tanabashi, and K. Kobayashi, "Substrate current due to impact ionization in MOS-FET," Japanese Journal of Applied Physics, vol. 15, p. 1127, 1976.
[6.22] S. Ramaswamy, A. Amerasekera, and M.-C. Chang, "A unified substrate current model for weak and strong impact ionization in sub-0.25/spl mu/m NMOS devices," in Electron Devices Meeting, 1997. IEDM''97. Technical Digest., International, 1997, pp. 885-888.
[6.23] T. Irisawa, T. Numata, N. Sugiyama, and S.-i. Takagi, "On the origin of increase in substrate current and impact ionization efficiency in strained-Si n-and p-MOSFETs," IEEE Transactions on Electron Devices, vol. 52, pp. 993-998, 2005.
[6.24] T. Chan, P. Ko, and C. Hu, "A simple method to characterize substrate current in MOSFET''s," IEEE Electron Device Letters, vol. 5, pp. 505-507, 1984.
[6.25] W.-C. Lee and C. Hu, "Modeling CMOS tunneling currents through ultrathin gate oxide due to conduction-and valence-band electron and hole tunneling," IEEE Transactions on Electron Devices, vol. 48, pp. 1366-1373, 2001.
[6.26] K. F. Schuegraf and C. Hu, "Hole injection SiO 2 breakdown model for very low voltage lifetime extrapolation," IEEE Transactions on Electron Devices, vol. 41, pp. 761-767, 1994.
[6.27] H. Lin, J. Lin, and R. C. Chang, "Inversion-layer induced body current in SOI MOSFETs with body contacts," IEEE Electron Device Letters, vol. 24, pp. 111-113, 2003.
[6.28] C.-H. Dai, T.-C. Chang, A.-K. Chu, Y.-J. Kuo, S.-C. Chen, C.-C. Tsai, et al., "On the origin of hole valence band injection on GIFBE in PD SOI n-MOSFETs," IEEE Electron Device Letters, vol. 31, pp. 540-542, 2010.
[6.29] C.-H. Dai, T.-C. Chang, A.-K. Chu, Y.-J. Kuo, F.-Y. Jian, W.-H. Lo, et al., "On the origin of gate-induced floating-body effect in PD SOI p-MOSFETs," IEEE Electron Device Letters, vol. 32, pp. 847-849, 2011.
[6.30] C.-H. Dai, T.-C. Chang, A.-K. Chu, Y.-J. Kuo, S.-C. Chen, C.-T. Tsai, et al., "Enhanced gate-induced floating-body effect in PD SOI MOSFET under external mechanical strain," Surface and Coatings Technology, vol. 205, pp. 1470-1474, 2010.
[6.31] W.-h. Lo, T.-C. Chang, C.-H. Dai, W.-L. Chung, C.-E. Chen, S.-H. Ho, et al., "Impact of mechanical strain on GIFBE in PD SOI p-MOSFETs as indicated from NBTI degradation," IEEE Electron Device Letters, vol. 33, pp. 303-305, 2012.
[6.32] W. Zhu, T.-P. Ma, T. Tamagawa, J. Kim, and Y. Di, "Current transport in metal/hafnium oxide/silicon structure," IEEE Electron Device Letters, vol. 23, pp. 97-99, 2002.
[6.33] C.-T. Sah, R. N. Noyce, and W. Shockley, "Carrier generation and recombination in pn junctions and pn junction characteristics," Proceedings of the IRE, vol. 45, pp. 1228-1243, 1957.
[6.34] D. J. Dumin and J. R. Maddux, "Correlation of stress-induced leakage current in thin oxides with trap generation inside the oxides," IEEE Transactions on Electron Devices, vol. 40, pp. 986-993, 1993.
[6.35] S.-H. Ho, T.-C. Chang, Y.-s. Lu, W.-H. Lo, C.-E. Chen, J.-Y. Tsai, et al., "Analysis of anomalous traps measured by charge pumping technique in HfO2/metal gate n-channel metal-oxide-semiconductor field-effect transistors," Applied Physics Letters, vol. 101, p. 233509, 2012.
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