591 research outputs found

    Nanoparticle Engineering for Chemical-Mechanical Planarization

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    Increasing reliance on electronic devices demands products with high performance and efficiency. Such devices can be realized through the advent of nanoparticle technology. This book explains the physicochemical properties of nanoparticles according to each step in the chemical mechanical planarization (CMP) process, including dielectric CMP, shallow trend isolation CMP, metal CMP, poly isolation CMP, and noble metal CMP. The authors provide a detailed guide to nanoparticle engineering of novel CMP slurry for next-generation nanoscale devices below the 60nm design rule. This comprehensive text also presents design techniques using polymeric additives to improve CMP performance

    ์„ธ๋ฅจ ์‚ฐํ™”๋ฌผ๊ณผ ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜์˜ ์›จ์ดํผ์˜ ์ƒํ˜ธ์ž‘์šฉ์— ๋Œ€ํ•œ ์ง์ ‘์ , ์ •๋Ÿ‰์  ๋ถ„์„ ๋ฐ pH-๋ฒ”์šฉ์  CMP ํ›„ ์„ธ์ • ์šฉ์•ก์˜ ๊ฐœ๋ฐœ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ™”ํ•™์ƒ๋ฌผ๊ณตํ•™๋ถ€, 2022. 8. ๊น€์žฌ์ •.The size of the semiconductor devices reduces and their density increases, the semiconductor manufacturing process is becoming more important. In particular, the chemical mechanical polishing (CMP) process for silicon-based wafers mainly used in the shallow trench isolation (STI) process is increasing. CMP is a process of polishing the wafers at a relatively high pressure and speed, and a lot of contamination and scratches due to abrasives in the slurry are inevitably left. However, as the scaling down of semiconductor devices intensifies and the requirements in the manufacturing process increase, it is becoming more important to minimize contamination and scratches. Especially, the residual abrasives after STI-CMP may interfere with the uniform deposition of photoresist in lithography. Ceria abrasive is known to show high polishing rate on silicon oxide due to strong chemical interaction in contrast to silicon nitride, so nitride is usually used as a stopping layer. In the CMP process, the chemical interaction of ceria and silicon oxide is advantageous, but in the subsequent cleaning process to remove it, the chemical interaction becomes a troublesome. Therefore, it is very important to understand how the chemical interaction between the two occurs during the CMP and cleaning processes. In the past, cleaning was carried out using the lift-off method to etch the surface of silicon oxide using cleaning solutions such as standard cleaning 1 (SC-1), Sulfuric acid peroxide mixture (SPM), and diluted HF, but recently, new cleaning solution removing as little as possible the thinly deposited silicon oxide and selectively removing only ceria is necessary. In this study, the interaction of ceria abrasives on silicon nitride and oxide, was directly investigated through atomic force microscope (AFM). The adhesion energy was measured and compared to elucidate the reason why ceria could remove silicon oxide well compared to nitride. In addition, the change in adhesion energy value according to the surface oxidation state of ceria abrasive was measured by AFM, and the adsorption rate was measured by quartz crystal microbalance (QCM). Activation energy was calculated and compared using the measured adsorption rates at various temperature. To develop a cleaning solution that can be used at acidic pH, we developed a cleaning solution that can maintain the zeta potential negatively even under various conditions, and confirmed the cleaning efficiency.๋ฐ˜๋„์ฒด ์†Œ์ž์˜ ํฌ๊ธฐ๊ฐ€ ๊ฐ์†Œํ•˜๊ณ  ๋ฐ€๋„๊ฐ€ ์ฆ๊ฐ€ํ•˜๋ฉด์„œ ๋ฐ˜๋„์ฒด ์ œ์กฐ ๊ณต์ •์˜ ์ค‘์š”์„ฑ์ด ๋†’์•„์ง€๊ณ  ์žˆ๋‹ค. ํŠนํžˆ ๋ฐ˜๋„์ฒด ์ œ์กฐ ๊ณต์ • ์ค‘ ํŠธ๋žœ์ง€์Šคํ„ฐ๋ฅผ ๋…๋ฆฝ์ ์œผ๋กœ ์‚ฌ์šฉํ•˜๊ธฐ ์œ„ํ•ด ๋„์ž…๋œ STI ๊ณต์ •์—์„œ ์ฃผ๋กœ ์‚ฌ์šฉ๋˜๋Š” ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜์˜ ์›จ์ดํผ๋“ค์— ๋Œ€ํ•œ ํ™”ํ•™์ , ๊ธฐ๊ณ„์  ์—ฐ๋งˆ ๊ณต์ •์˜ ์ค‘์š”๋„๊ฐ€ ๋†’์•„์ง€๊ณ  ์žˆ๋‹ค. ํ™”ํ•™์ , ๊ธฐ๊ณ„์  ์—ฐ๋งˆ ๊ณต์ •์€ ๋น„๊ต์  ๊ฐ•ํ•œ ์••๋ ฅ, ์†๋„๋กœ ์›จ์ดํผ๋ฅผ ๊ฐˆ์•„๋‚ด๋Š” ๊ณต์ •์œผ๋กœ, ์Šฌ๋Ÿฌ๋ฆฌ ๋‚ด ์—ฐ๋งˆ์žฌ๋“ค๋กœ ์ธํ•œ ๋งŽ์€ ์˜ค์—ผ ๋ฐ ์Šคํฌ๋ž˜์น˜๊ฐ€ ํ•„์—ฐ์ ์œผ๋กœ ๋‚จ๊ฒŒ ๋œ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ๋ฐ˜๋„์ฒด ๊ณต์ •์˜ ํ•„์š”์กฐ๊ฑด์ด ๋†’์•„์ง€๋ฉด์„œ, ์˜ค์—ผ ๋ฐ ์Šคํฌ๋ž˜์น˜๋ฅผ ์ตœ์†Œํ•œ์œผ๋กœ ์ค„์ด๋Š” ๊ฒƒ์ด ๋งค์šฐ ์ค‘์š”ํ•ด์ง€๊ณ  ์žˆ๋‹ค. ํŠนํžˆ STI ๊ณผ์ •์—์„œ์˜ ํ™”ํ•™์ , ๊ธฐ๊ณ„์  ์—ฐ๋งˆ ํ›„ ์ž”์กด ์—ฐ๋งˆ์žฌ๋Š” ์ดํ›„ ๊ณต์ •์ธ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ ๋“ฑ์—์„œ ํฌํ† ๋ ˆ์ง€์ŠคํŠธ์˜ ๋„ํฌ๋ฅผ ๋ฐฉํ•ดํ•˜๊ณ  ๋‹จ์ฐจ๋ฅผ ์œ ๋„ํ•˜์—ฌ ์ตœ์ข…์ ์œผ๋กœ ํŠธ๋žœ์ง€์Šคํ„ฐ์˜ ์ „๊ธฐ์  ๊ตฌ๋™์„ ๋ฐฉํ•ดํ•  ์ˆ˜ ์žˆ๋‹ค. STI ๊ณผ์ •์—์„œ์˜ ํ™”ํ•™์ , ๊ธฐ๊ณ„์  ์—ฐ๋งˆ์—๋Š” ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ์„ ๊ฐˆ์•„๋‚ด๊ธฐ ์œ„ํ•ด์„œ ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ์— ๋Œ€ํ•œ ์„ ํƒ๋„๊ฐ€ ๋†’์€ ์„ธ๋ฆฌ์•„ ์—ฐ๋งˆ์žฌ๋ฅผ ์ฃผ๋กœ ์‚ฌ์šฉํ•œ๋‹ค. ์„ธ๋ฆฌ์•„ ์—ฐ๋งˆ์žฌ๋Š” ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ๊ณผ ๊ฐ•ํ•œ ํ™”ํ•™์  ์ƒํ˜ธ์ž‘์šฉ์„ ํ•˜์—ฌ ๋†’์€ ์—ฐ๋งˆ์œจ์„ ๋ณด์ด๋Š” ๊ฒƒ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ์œผ๋ฉฐ, ์‹ค๋ฆฌ์ฝ˜ ์งˆํ™”๋ฌผ์€ ์ž˜ ๊ฐˆ์•„๋‚ด์ง€ ๋ชปํ•˜์—ฌ, ์งˆํ™”๋ฌผ์„ ์—ฐ๋งˆ ์ œ์–ด ์ธต์œผ๋กœ ์‚ฌ์šฉํ•œ๋‹ค. ํ™”ํ•™์ , ๊ธฐ๊ณ„์  ์—ฐ๋งˆ ๊ณผ์ •์—์„œ๋Š” ์„ธ๋ฆฌ์•„์™€ ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ ์‚ฌ์ด์˜ ํ™”ํ•™์  ์ƒํ˜ธ์ž‘์šฉ์ด ์žฅ์ ์œผ๋กœ ์ž‘์šฉํ•˜์ง€๋งŒ, ์ดํ›„ ์ด๋ฅผ ์ œ๊ฑฐํ•˜๋Š” ์„ธ์ • ๊ณต์ •์—์„œ๋Š” ํ™”ํ•™์  ์ƒํ˜ธ์ž‘์šฉ์ด ๋˜๋ ค ๊ณจ์นซ๊ฑฐ๋ฆฌ๊ฐ€ ๋œ๋‹ค. ๋”ฐ๋ผ์„œ ์—ฐ๋งˆ ๊ณผ์ • ๋ฐ ์„ธ์ • ๊ณผ์ •์—์„œ ์–ด๋– ํ•œ ๋ฉ”์ปค๋‹ˆ์ฆ˜์œผ๋กœ ๋‘˜์˜ ํ™”ํ•™์  ์ƒํ˜ธ์ž‘์šฉ์ด ์ผ์–ด๋‚˜๋Š”์ง€ ์ดํ•ดํ•˜๋Š” ๊ฒƒ์ด ๋งค์šฐ ์ค‘์š”ํ•˜๋‹ค. ๊ทธ๋ฆฌ๊ณ  ๊ธฐ์กด์—๋Š” ๊ธฐํŒ ์„ธ์ •์„ ์œ„ํ•ด ์ผ๋ถ€ ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ง‰์„ ๋…น์—ฌ๋‚ด๋Š” ๊ฐ•ํ•œ ์„ธ์ • ์šฉ์•ก์„ ํ™œ์šฉํ•˜์—ฌ ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ง‰ ํ‘œ๋ฉด์„ ์–‡๊ฒŒ ๊นŽ์•„๋‚ด๋Š” lift-off ๋ฐฉ๋ฒ•์œผ๋กœ ์„ธ์ •์„ ์ง„ํ–‰ํ•˜์˜€์œผ๋‚˜, ์ตœ๊ทผ์—๋Š” ์–‡๊ฒŒ ๋„ํฌ๋œ ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ์„ ์ตœ๋Œ€ํ•œ ์ ๊ฒŒ ์ œ๊ฑฐํ•˜๋ฉฐ ์„ธ๋ฆฌ์•„ ์—ฐ๋งˆ์žฌ๋งŒ ์„ ํƒ์ ์œผ๋กœ ์ œ๊ฑฐํ•  ์ˆ˜ ์žˆ๋Š” ์„ธ์ • ์šฉ์•ก์˜ ๊ฐœ๋ฐœ์ด ํ•„์š”ํ•œ ์ƒํ™ฉ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์‹ค๋ฆฌ์ฝ˜ ์งˆํ™”๋ฌผ๊ณผ ์‚ฐํ™”๋ฌผ ์›จ์ดํผ์™€ ์„ธ๋ฆฌ์•„ ์—ฐ๋งˆ์žฌ ์‚ฌ์ด์˜ ์ƒํ˜ธ์ž‘์šฉ์„ ์›์ž ํž˜ ํ˜„๋ฏธ๊ฒฝ์„ ํ†ตํ•ด ์ง์ ‘์ ์œผ๋กœ ๊ด€์ฐฐํ•˜๊ณ , ์ ‘์ฐฉ ์—๋„ˆ์ง€๋ฅผ ์ธก์ •ํ•˜๊ณ  ๋น„๊ตํ•˜์—ฌ ์‹ค๋ฆฌ์ฝ˜ ์งˆํ™”๋ฌผ์— ๋น„ํ•ด ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ์—์„œ ์„ธ๋ฆฌ์•„ ์—ฐ๋งˆ์žฌ์— ๋Œ€ํ•œ ์„ธ์ •์ด ๋” ์–ด๋ ค์šด ์ด์œ ๋ฅผ ๋ฐํžˆ๊ณ ์ž ํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์„ธ๋ฆฌ์•„ ์—ฐ๋งˆ์žฌ์˜ ํ‘œ๋ฉด ์‚ฐํ™” ์ƒํƒœ์— ๋”ฐ๋ฅธ ์ ‘์ฐฉ ์—๋„ˆ์ง€ ๊ฐ’์˜ ๋ณ€ํ™”๋ฅผ ์›์ž ํž˜ ํ˜„๋ฏธ๊ฒฝ์„ ํ†ตํ•ด ์ธก์ •ํ•˜์˜€๊ณ , ์ˆ˜์ • ๋ฏธ์„ธ์ €์šธ์„ ํ†ตํ•ด ํก์ฐฉ ์†๋„๋ฅผ ์ธก์ •ํ•˜์˜€๋‹ค. ์ธก์ •๋œ ํก์ฐฉ ์†๋„๋ฅผ ์ด์šฉํ•˜์—ฌ ํ™œ์„ฑํ™” ์—๋„ˆ์ง€๋ฅผ ๊ณ„์‚ฐํ•˜๊ณ  ๋น„๊ตํ•˜์˜€๋‹ค. ์„ธ๋ฆฌ์•„์™€ ์‹ค๋ฆฌ์ฝ˜ ์‚ฐํ™”๋ฌผ ์‚ฌ์ด์˜ ์ƒํ˜ธ์ž‘์šฉ์ด ๋น„๊ต์  ์ ์€ ์‚ฐ์„ฑ ์กฐ๊ฑด์—์„œ๋„ ์„ธ๋ฆฌ์•„ ์ž…์ž์˜ ์ œํƒ€ ์ „์œ„๊ฐ€ ์Œ์˜ ๊ฐ’์„ ์œ ์ง€ํ•  ์ˆ˜ ์žˆ๋Š” ์„ธ์ • ์šฉ์•ก์˜ ๊ฐœ๋ฐœ์„ ์œ„ํ•ด ์ธ์‚ฐ ๊ธฐ๋ฐ˜์˜ ์ฒจ๊ฐ€์ œ๋“ค์ด ์—ฐ๊ตฌ๋˜์—ˆ๊ณ , ์„ธ์ • ํšจ์œจ์ด ํ‰๊ฐ€๋˜์—ˆ๋‹ค.Chapter I. Introduction 1 1.1. Necessity of CMP in shallow trench isolation 1 1.2. Ceria abrasive for STI-CMP and its interaction with silicon oxide 6 1.3. Post-CMP cleaning process 10 1.4. Methods for analyzing the adsorption behavior 14 1.5. Main issues in post-CMP ceria cleaning and the necessity of pH-independent cleaning solution 19 1.6. Purpose of this research 26 Chapter II. Experimental 28 2.1. Interaction between ceria and silicon-based wafers 28 2.2. The impact of surficial oxidation state of ceria on the ceria-SiO2 interaction 31 2.3. Development of pH-independent post-CMP cleaning solution 34 Chapter III. Results and Discussion 38 3.1. Interaction between ceria and silicon-based wafers 38 3.1.1. Electrostatic interaction between ceria and Si3N4 or SiO2 38 3.1.2. Adhesion energy measurement with AFM 45 3.2. The impact of oxidation state of ceria on the ceria-SiO2 interaction 50 3.2.1. Chemical treatment for controlling oxidation state of ceria 50 3.2.2. Adhesion energy between ceria and SiO2 measured by AFM 58 3.2.3. Adsorption behavior of ceria on SiO2 investigated by QCM 62 3.3. Development of pH-independent post-CMP cleaning solution 68 3.3.1. Zeta potential of ceria nanoparticles with PA, EA, and ATMP 68 3.3.2. Cleaning solution for ceria abrasives 79 Chapter IV. Conclusion 83 References 86 ๊ตญ๋ฌธ ์ดˆ๋ก 93๋ฐ•

    ใƒˆใƒฉใƒณใ‚ธใ‚นใ‚ฟใƒปใ‚ขใƒฌใ‚คๆ–นๅผใซๅŸบใฅใใ‚ขใƒŠใƒญใ‚ฐใƒฌใ‚คใ‚ขใ‚ฆใƒˆใซใŠใ‘ใ‚‹ๅฏ†ๅบฆๆœ€้ฉๅŒ–

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    In integrated circuit design of advanced technology nodes, layout density uniformity significantly influences the manufacturability due to the CMP variability. In analog design, especially, designers are suffering from passing the density checking since there are few useful tools. To tackle this issue, we focus on a transistor-array(TA)-style analog layout, and propose a density optimization algorithm consistent with complicated design rules. Based on TA-style, we introduce a density-aware layout format to explicitly control the layout pattern density, and provide the mathematical optimization approach. Hence, a design flow incorporating our density optimization can drastically reduce the design time with fewer iterations. In a design case of an OPAMP layout in a 65nm CMOS process, the result demonstrates that the proposed approach achieves more than 48ร— speed-up compared with conventional manual layout, meanwhile, it shows a good circuit performance in the post-layout simulation.ๅŒ—ไนๅทžๅธ‚็ซ‹ๅคง

    Modeling of chemical mechanical polishing for shallow trench isolation

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    Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 2002.Includes bibliographical references (p. 195-201).This thesis presents the nonlinear analysis, design, fabrication, and testing of an axial-gap magnetic induction micro machine, which is a two-phase planar motor in which the rotor is suspended above the stator via mechanical springs, or tethers. The micro motor is fabricated from thick layers of electroplated NiFe and copper, by our collaborators at Georgia Institute of Technology. The rotor and the stator cores are 4 mm in diameter each, and the entire motor is about 2 mm thick. During fabrication, SU-8 epoxy is used as a structural mold material for the electroplated cores. The tethers are designed to be compliant in the azimuthal direction, while preventing axial deflections and maintaining a constant air gap. This enables accurate measurements of deflections within the rotor plane via a computer microvision system. The small scale of the magnetic induction micro machine, in conjunction with the good thermal contact between its electroplated stator layers, ensures an isothermal device which can be cooled very effectively. Current densities over 109 A/m2 simultaneously through each phase is repeatedly achieved during experiments; this density is over two orders of magnitude larger than what can be achieved in conventional macro-scale machines.(cont.) More than 5 Nm of torque is obtained for an air gap of about 5 zm, making this micro motor the highest torque density micro-scale magnetic machine to date. About 0.3 buNm for the large air gap of 70 m is also achieved in systematic tests that reveal the influence of strong eddy-currents and associated nonlinear saturation within the micro motor Eddy-current effects are modeled using a finite-difference vector potential formulation. Its results demonstrate the presence of flux crowding on the stator surface, which leads to heavy saturation. To capture saturation effects, a fully nonlinear finite-difference time-domain simulation is developed to solve Maxwell's Equations within the computational space of the micro machine. To mitigate the inherent stiffness in the partial differential equations, the speed of light is artificially reduced by five orders of magnitude, taking special care that assumptions of magnetoquasistatic behavior are still met. The results from this model are in very good agreement with experimental data from the tethered magnetic induction micro motor.by Brian Lee.Ph.D

    3D-deflectometry : fast nanotopography measurement for the semiconductor industry

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    Simulation study of scaling design, performance characterization, statistical variability and reliability of decananometer MOSFETs

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    This thesis describes a comprehensive, simulation based scaling study โ€“ including device design, performance characterization, and the impact of statistical variability โ€“ on deca-nanometer bulk MOSFETs. After careful calibration of fabrication processes and electrical characteristics for n- and p-MOSFETs with 35 nm physical gate length, 1 nm EOT and stress engineering, the simulated devices closely match the performance of contemporary 45 nm CMOS technologies. Scaling to 25 nm, 18 nm and 13 nm gate length n and p devices follows generalized scaling rules, augmented by physically realistic constraints and the introduction of high-k/metal-gate stacks. The scaled devices attain the performance stipulated by the ITRS. Device a.c. performance is analyzed, at device and circuit level. Extrinsic parasitics become critical to nano-CMOS device performance. The thesis describes device capacitance components, analyzes the CMOS inverter, and obtains new insights into the inverter propagation delay in nano-CMOS. The projection of a.c. performance of scaled devices is obtained. The statistical variability of electrical characteristics, due to intrinsic parameter fluctuation sources, in contemporary and scaled decananometer MOSFETs is systematically investigated for the first time. The statistical variability sources: random discrete dopants, gate line edge roughness and poly-silicon granularity are simulated, in combination, in an ensemble of microscopically different devices. An increasing trend in the standard deviation of the threshold voltage as a function of scaling is observed. The introduction of high-k/metal gates improves electrostatic integrity and slows this trend. Statistical evaluations of variability in Ion and Ioff as a function of scaling are also performed. For the first time, the impact of strain on statistical variability is studied. Gate line edge roughness results in areas of local channel shortening, accompanied by locally increased strain, both effects increasing the local current. Variations are observed in both the drive current, and in the drive current enhancement normally expected from the application of strain. In addition, the effects of shallow trench isolation (STI) on MOSFET performance and on its statistical variability are investigated for the first time. The inverse-narrow-width effect of STI enhances the current density adjacent to it. This leads to a local enhancement of the influence of junction shapes adjacent to the STI. There is also a statistical impact on the threshold voltage due to random STI induced traps at the silicon/oxide interface

    Yield modeling for deep sub-micron IC design

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    Modeling and Optimization of Chemical Mechanical Planarization (Cmp) Using Neural Networks, Anfis and Evolutionary Algorithms

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    Higher density nano-devices and more metallization layers in microelectronic chips are unceasing goals to the present semiconductor industry. However, topological imperfections (higher non-uniformity) on the wafer surfaces and lower material removal rates (MRR) seriously hamper these pursuing motivations. Since'90, industry has been using chemical mechanical planarization/polishing (CMP) to overcome these obstacles for fabricating integrated circuits (IC) with interconnect geometries of < 0.18 &amp;#956;m. Obviously, the much needed understanding of this new technique is derived basically on the ancient lapping process. Modeling and simulation are critical to transfer CMP from an engineering 'art' to an engineering 'science'. Many efforts in CMP modeling have been made in the last decade, but the available analytical MRR and surface uniformity models cannot precisely describe this highly complicated process, involving simultaneous chemical reactions (and etching), and mechanical abrasion. In this investigation, neural networks (NN), adaptive-based-network fuzzy inference system (ANFIS), and evolutionary algorithms (EA) techniques were applied to successfully overcome the aforementioned modeling and simulation problems. In addition, fine-tuning techniques for re-modifying ANFIS models for sparse-data case using are developed. Furthermore, multi-objective evolutionary algorithms (MOEA) are firstly applied to search for the optimal input settings for CMP process to trade-off the higher MRR and lower non-Uniformity by using the previously constructed models. The results also show the simulation of MOEA optimization can certainly provide accurate guidance to search the optimal input settings for CMP process to produce lower non-uniform wafer surfaces under higher MRR.Mechanical & Aerospace Engineerin

    Electrical Design for Manufacturability Solutions: Fast Systematic Variation Analysis and Design Enhancement Techniques

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    The primary objectives in this research are to develop computer-aided design (CAD) tools for Design for Manufacturability (DFM) solutions that enable designers to conduct more rapid and more accurate systematic variation analysis, with different design enhancement techniques. Four main CAD tools are developed throughout my thesis. The first CAD tool facilitates a quantitative study of the impact of systematic variations for different circuits' electrical and geometrical behavior. This is accomplished by automatically performing an extensive analysis of different process variations (lithography and stress) and their dependency on the design context. Such a tool helps to explore and evaluate the systematic variation impact on any type of design. Secondly, solutions in the industry focus on the "design and then fix philosophy", or "fix during design philosophy", whereas the next CAD tool involves the "fix before design philosophy". Here, the standard cell library is characterized in different design contexts, different resolution enhancement techniques, and different process conditions, generating a fully DFM-aware standard cell library using a newly developed methodology that dramatically reduce the required number of silicon simulations. Several experiments are conducted on 65nm and 45nm designs, and demonstrate more robust and manufacturable designs that can be implemented by using the DFM-aware standard cell library. Thirdly, a novel electrical-aware hotspot detection solution is developed by using a device parameter-based matching technique since the state-of-the-art hotspot detection solutions are all geometrical based. This CAD tool proposes a new philosophy by detecting yield limiters, also known as hotspots, through the model parameters of the device, presented in the SPICE netlist. This novel hotspot detection methodology is tested and delivers extraordinary fast and accurate results. Finally, the existing DFM solutions, mainly address the digital designs. Process variations play an increasingly important role in the success of analog circuits. Knowledge of the parameter variances and their contribution patterns is crucial for a successful design process. This information is valuable to find solutions for many problems in design, design automation, testing, and fault tolerance. The fourth CAD solution, proposed in this thesis, introduces a variability-aware DFM solution that detects, analyze, and automatically correct hotspots for analog circuits

    5nm ์ดํ•˜ 3D Transistors์˜ Self-Heating ๋ฐ ์ „์—ดํŠน์„ฑ๋ถ„์„ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2021.8. ์‹ ํ˜•์ฒ .In this thesis, Self-Heating Effect (SHE) is investigated using TCAD simulations in various Sub-10-nm node Field Effect Transistor (FET). As the node decreases, logic devices have evolved into 3D MOSFET structures from Fin-FET to Nanosheet-FET. In the case of 3D MOSFET, there are thermal reliability issues due to the following reasons: โ…ฐ) The power density of the channel is high, โ…ฑ) The channel structure surrounded by SiO2, โ…ฒ) The overall low thermal conductivity characteristics due to scaling down. Many papers introduce the analysis and prediction of temperature rise by SHE in the device, but there are no papers presenting the content of mitigation of temperature rise. Therefore, we have studied the methods of decreasing the maximum lattice temperature (TL,max) such as shallow trench isolation (STI) composition engineering in Fin-FET, thermal analysis according to DC/AC/duty cycle in nanowire-FET, and active region ( e.g., gate metal thickness, channel width, channel number etc..) optimization in nanosheet-FET. In addition, lifetime affected by hot carrier injection (HCI) / bias-temperature instability (BTI) is also analyzed according to various thermal relaxation methods presented.์ด ๋…ผ๋ฌธ์—์„œ๋Š” ๋‹ค์–‘ํ•œ Sub-10nm ๋…ธ๋“œ ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ (FET)์—์„œ TCAD ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ์‚ฌ์šฉํ•˜์—ฌ ์ž์ฒด ๋ฐœ์—ด ํšจ๊ณผ (SHE)๋ฅผ ์กฐ์‚ฌํ•ฉ๋‹ˆ๋‹ค. ๋…ธ๋“œ๊ฐ€ ๊ฐ์†Œํ•จ์— ๋”ฐ๋ผ ๋…ผ๋ฆฌ ์žฅ์น˜๋Š” Fin-FET์—์„œ Nanosheet-FET๋กœ 3D MOSFET ๊ตฌ์กฐ๋กœ ์ง„ํ™”ํ–ˆ์Šต๋‹ˆ๋‹ค. 3D MOSFET์˜ ๊ฒฝ์šฐ โ…ฐ) ์ฑ„๋„์˜ ์ „๋ ฅ ๋ฐ€๋„๊ฐ€ ๋†’์Œ, โ…ฑ) SiO2๋กœ ๋‘˜๋Ÿฌ์‹ธ์ธ ์ฑ„๋„ ๊ตฌ์กฐ, โ…ฒ) ์ถ•์†Œ๋กœ ์ธํ•ด ์ „์ฒด์ ์œผ๋กœ ๋‚ฎ์€ ์—ด์ „๋„ ํŠน์„ฑ ๋“ฑ ๋‹ค์Œ๊ณผ ๊ฐ™์€ ์ด์œ ๋กœ ์—ด ์‹ ๋ขฐ์„ฑ ๋ฌธ์ œ๊ฐ€ ์žˆ์Šต๋‹ˆ๋‹ค. ํ•œํŽธ, ๋งŽ์€ ๋…ผ๋ฌธ์ด device์—์„œ SHE์— ์˜ํ•œ ์˜จ๋„ ์ƒ์Šน์˜ ๋ถ„์„ ๋ฐ ์˜ˆ์ธก์„ ์†Œ๊ฐœํ•˜์ง€๋งŒ ์˜จ๋„ ์ƒ์Šน ์™„ํ™”์˜ ๋‚ด์šฉ์„ ์ œ์‹œํ•˜๋Š” ๋…ผ๋ฌธ์€ ๊ฑฐ์˜ ์—†์Šต๋‹ˆ๋‹ค. ๋”ฐ๋ผ์„œ Fin-FET์˜ STI (Shallow Trench Isolation) ๊ตฌ์„ฑ ๊ณตํ•™, nanowire-FET์˜ DC / AC / ๋“€ํ‹ฐ ์‚ฌ์ดํด์— ๋”ฐ๋ฅธ ์—ด ๋ถ„์„, nanosheet-FET์—์„œ ์†Œ์ž์˜ ์ค‘์š”์˜์—ญ(์˜ˆ: ๊ฒŒ์ดํŠธ ๊ธˆ์† ๋‘๊ป˜, ์ฑ„๋„ ํญ, ์ฑ„๋„ ๋ฒˆํ˜ธ ๋“ฑ)์˜ ์ตœ์ ํ™”๋ฅผ ํ†ตํ•ด์„œ ์ตœ๋Œ€ ๊ฒฉ์ž ์˜จ๋„ (TL,max)๋ฅผ ๋‚ฎ์ถ”๋Š” ๋ฐฉ๋ฒ•๋“ฑ์„ ์—ฐ๊ตฌํ–ˆ์Šต๋‹ˆ๋‹ค. ๋˜ํ•œ ๋” ๋‚˜์•„๊ฐ€์„œ HCI (Hot Carrier Injection) / BTI (Bias-Temperature Instability)์˜ ์˜ํ–ฅ์„ ๋ฐ›๋Š” ์ˆ˜๋ช…๋„ ์ œ์‹œ๋œ ๋‹ค์–‘ํ•œ ์—ด ์™„ํ™” ๋ฐฉ๋ฒ•์— ๋”ฐ๋ผ ๋ถ„์„ํ•˜์—ฌ ์†Œ์ž์˜ ์ œ์ž‘์— ์žˆ์–ด ์—ด์  ํŠน์„ฑ๊ณผ ์ˆ˜๋ช…์„ ์ข‹๊ฒŒ ๋งŒ๋“œ๋Š” ์ง€ํ‘œ๋ฅผ ์ œ์‹œํ•ฉ๋‹ˆ๋‹ค .Chapter 1 Introduction 1 1.1. Development of Semconductor structure 1 1.2. Self-Heating Effect issues in semiconductor devices 3 Chapter 2 Thermal-Aware Shallow Trench Isolation Design Optimization for Minimizing Ioff in Various Sub-10-nm 3-D Transistor 7 2.1. Introduction 7 2.2. Device Structure and Simulation Condition 7 2.3. Results and Discussion 12 2.4. Summary 27 Chapter 3 Analysis of Self Heating Effect in DC/AC Mode in Multi-channel GAA-Field Effect Transistor 32 3.1. Introduction 32 3.2. Multi-Channel Nanowire FET and Back End Of Line 33 3.3. Work Flow and Calibration Process 35 3.4. More Detailed Thermal Simulation of Nanowire-FET 37 3.5. Performance Analysis by Number of Channels 38 3.6. DC Characteristic of SHE in Nanowire-FETs 40 3.7. AC Characteristics of SHE in Nanowire-FETs 43 3.8. Summary 51 Chapter 4 Self-Heating and Electrothermal Properties of Advanced Sub-5-nm node Nanoplate FET 56 4.1. Introduction 56 4.2. Device Structure and Simulation Condition 57 4.3. Thermal characteristics by channel number and width 62 4.4. Thermal characteristics by inter layer-metal thickness (TM) 64 4.5. Life Time Prediction 65 4.6. Summary 67 Chapter 5 Study on Self Heating Effect and life time in Vertical-channel Field Effect Transistor 72 5.1. Introduction 72 5.2. Device Structure and Simulation Condition 72 5.3. Temperature and RTH according to channel width(TW) 76 5.4. Thermal properties according to air spacers and air gap 77 5.5. Ion boosting according to Channel numbers 81 5.6. Temperature imbalance of multi-channel VFETs 82 5.7. Mitigation of the channel temperature imbalance 86 5.8. Life time depending on various analysis conditions 88 5.9. Summary 89 Chapter 6 Conclusions 93 Appendix A. A Simple and Accurate Modeling Method of Channel Thermal Noise Using BSIM4 Noise Models 95 A.1. Introduction 95 A.2. Overall Schematic of the RF MOSFET Model 97 A.3. Verification of the DC Characteristics of the RF MOSFET Model 98 A.4. Verification of the MOSFET Model with Measured Y-parameters 100 A.5. Verification of the MOSFET Model with Measured Noise Parameters 101 A.6. Thermal Noise Extraction and Modeling (TNOIMOD = 0) 103 A.7. Verification of the Enhanced Model with Noise Parameters 112 A.8. Holistic Model (TNOIMOD = 1) 114 A.9. Evaluation the validity of the model for drain bias 115 A.10. Conclusion 117 Abstract in Korean 122๋ฐ•
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