23 research outputs found

    Electromechanical Switches Fabricated by Electrophoretic Deposition of Single Wall Carbon Nanotube Films

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    University of Minnesota Ph.D. dissertation.August 2015. Major: Electrical/Computer Engineering. Advisor: Stephen Campbell. 1 computer file (PDF); xi, 110 pages.Power dissipation is a critical problem of CMOS devices especially for mobile applications. Many efforts have been made to solve the problem, but there are still major issues associated with scaling the device size. Micro electromechanical (MEMS) and nano electromechanical (NEMS) devices are one candidate to solve the problems because of their excellent standby leakage. However, the switches have a tradeoff between low operating power and high device speed. Suspended beams with low mass density and good mechanical properties provide a way to optimize the device. Carbon nanotubes (CNTs) have the low mass density and excellent mechanical properties to enable high performance MEMS/NEMS devices. However, the high temperature required for the direct synthesis for CNTs makes it difficult for them to be compatible with a substrate containing transistors. Therefore, continuous film deposition techniques are investigated with low temperature (< 300 C). Electrophoretic deposition (EPD) is a simple and versatile processing method to deposit carbon nanotubes on the substrate at room temperature. The movement of the charged CNTs in suspension occurs by an applied electric field. The deposited CNT film thickness can be controlled through the applied voltage and process time. We demonstrate the use of an EPD process to deposit various thicknesses of CNT films. Film thicknesses are studied as a function of, deposition time, electric field strength, and suspension concentration. The deposition mechanism of the EPD process for carbon nanotube layers was explained with experimental data. We determined the film mass density and electrical/optical properties of SWCNT films. Rutherford backscattering spectroscopy was used to determine the film mass density. Films created in this manner had a mass density that varies with thickness from 0.12 to 0.54 g/cm3 and a resistivity of 2.1410-3 ฮฉโˆ™cm. For the mechanical property measurements, we describe a technique to fabricate free-standing thin films using modified Langmuir-Blodgett method. Then we extracted the Youngโ€™s modulus of the film from the load-displacement data from nanoindentation using the appropriate modeling. The Youngโ€™s modulus had a range of 4.72 to 5.67 GPa, independent of deposited thickness. We fabricated two-terminal fixed beam switches with SWCNT thin films using the EPD process. Device pull-in voltages under 1V were achieved by decreasing the air-gap. The pull-in voltages were compared with the calculated results using the device geometry and extracted Youngโ€™s modulus from nanoindentation. Generally good agreement was observed. Also, we found a range of 2.4 to 3.5 MHz resonant frequency. However, we encountered several problems with the device including a gradual turn-on, hysteresis between pull-in and pull-out voltage, changes in the pull-in voltages with repeated on-off cycling, and early failure due to moisture absorption during testing in the air. Mechanisms for these observations are postulated. Further work is needed to improve device performance and reliability

    ๋‹ค๊ธฐ๋Šฅ AFM์„ ํ†ตํ•œ ๊ณ ์œ ์ „์œจ ๋ฐ•๋ง‰์˜ ๊ณ ๊ธ‰ ๊ณ„์ธก ๋ฐ 3์ฐจ์› ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ๋ฅผ ์œ„ํ•œ ๋ฒŒ์ง€ ์ œ๊ฑฐ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์œตํ•ฉ๊ณผํ•™๊ธฐ์ˆ ๋Œ€ํ•™์› ์œตํ•ฉ๊ณผํ•™๋ถ€(๋‚˜๋…ธ์œตํ•ฉ์ „๊ณต), 2019. 2. ๊น€์—ฐ์ƒ.Scanning probe microscopy (SPM) is widely used to analyze the surface structures and properties of semiconductor and bio-molecular films. The merits of the SPM method are that it does not require any process for sample preparation and minimizes damages of the probing sample. Moreover, the growth of industries related to semiconductor and nano-bio devices has led to the development of nanotechnology. Many researchers now become aware of the importance of local variations, such as the local doping profiles of semiconductors, the work function of two-dimensional materials, the surface profiles of bio-molecular films, the diodic behavior of nanofluidic devices, the surface roughness of semiconductor thin films, and the distribution of local surface charge. Thus, the researchers are seeking appropriate SPM equipment to analyze the local variations. In recent years, atomic force microscopes have emerged that can perform various functions. Especially, low-noise atomic force microscopy can be used to measure linewidths of nanoscale next-generation semiconductors or inspection for ultra-thin films. Therefore, Korea Research Institute of Standards and Science has developed a low noise atomic force microscope considering the industrial application. As well as, it has been developed to perform sophisticated nano/micro patterns by adding the function of nano-indentation. The low-noise atomic force microscope avoids the installation of an internal stage due to the nature of the development background. Although it contributes significantly to the signal integrity of the low-noise atomic force microscope, it serves as a weakness to limit the scan area of the test sample. Therefore, it is essential to have an independent external stage to compensate the weakness. In this paper, we have developed the middle range moving stage for the measurements of the standard reference samples. The maximum travel length of the external 4-axis stage is 10 mm. For image scanning of a specific area of interest, the sample is positioned with micron accuracy through an external stage and then finely positioned using a PI XY piezo scanner. We confirmed that the position error of the developed stage can be ignored by the reproducibility experiment. Subsequently, the sidewall of the improved vertical parallel structure (IVPS) was measured. The repeatability and reproducibility (R&R) of the CD measurement was estimated using the CDR30-EBD tip. Finally, we found that the tip wear was minimized by measuring the TGX1 sample with the undercut structure. Thus, the development of independent external stages can be useful for many tasks that require large scanning areas. In the industrial semiconductor fabrication, the inspection of thin films is performed through optical equipment to check the uniformity of wafers. In the next-generation semiconductor industry, high-capacity and low-power devices with complex lithography patterns and ultra-thin insulating films are emerging. Therefore, in order to improve the yield of semiconductor devices, it is necessary to inspect not only the thickness of these thin films but also local variations. Indeed, the surface roughness of the semiconductor process may affect the formation of the ultrathin film, and even if the process of the ultra-thin films is optimized by the atomic layer deposition (ALD), the performance of the device may be degraded due to the roughened surface. Therefore, atomic force microscopy is the most suitable method for quantifying the properties of thin films and for analyzing the local surface structures. In this thesis, critical roughness (CR) was defined for the first time in a nanoscale by devising a roughness scaling process as a method for managing hafnium oxide film, which is a high-k insulating film of a MOS transistor. The surface roughness of the substrate was processed by a wet etching method, and an ALD process was used to obtain a hafnium oxide film. This is a study on the influence of the roughness of the lower layer on the roughness of the upper layer, and this definition makes it possible to present the criteria of the standard production in the in-line oxide film process. Moreover, we confirmed that the CR value defined in this study was effective by realizing the MIM diode structures with different roughness. Furthermore, new research methods were introduced through the indentation lithography. The first study suggests that nano- and micro-patterns can be formed on biofilms that is impracticable by electron beam lithography. The indentation method can be a means to compensate the weaknesses of electron beam lithography. The second study is to selectively remove the bulges generated during the indentation process. For many years, it was a quite important issue because the formation of the bulge was a major factor impeding the development of indentation technology. All in all, in this thesis, various research themes realized by the multi-functional AFM are presented. The new definition of the roughness contributed to the in-line process control. The patterned biofilm could be used as a standard sample of the TOF-SIMS imaging. The selective removal of the bulges suggested a new method for three-dimensional nanolithography. Therefore, this research is expected to be a cost effective technology in the industry and to be used in various research fields.์Šค์บ๋‹ ํ”„๋ฃจ๋ธŒ ํ˜„๋ฏธ๊ฒฝ (SPM)์€ ๋ฐ˜๋„์ฒด ๋ฐ ์ƒ์ฒด ๋ถ„์ž ํ•„๋ฆ„์˜ ํ‘œ๋ฉด ๊ตฌ์กฐ ๋ฐ ํŠน์„ฑ์„ ๋ถ„์„ํ•˜๋Š” ๋ฐ ๋„๋ฆฌ ์‚ฌ์šฉ๋œ๋‹ค. SPM ๋ฐฉ๋ฒ•์˜ ์žฅ์ ์€ ์‹œ๋ฃŒ ์ค€๋น„๋ฅผ ์œ„ํ•œ ์–ด๋– ํ•œ ๊ณต์ •๋„ ํ•„์š”๋กœ ํ•˜์ง€ ์•Š์œผ๋ฉฐ ์กฐ์‚ฌ ์‹œ๋ฃŒ์˜ ์†์ƒ์„ ์ตœ์†Œํ™”ํ•œ๋‹ค๋Š” ๊ฒƒ์ด๋‹ค. ๋˜ํ•œ, ๋ฐ˜๋„์ฒด ๋ฐ ๋‚˜๋…ธ ๋ฐ”์ด์˜ค ๋””๋ฐ”์ด์Šค์™€ ๊ด€๋ จ๋œ ์‚ฐ์—…์˜ ์„ฑ์žฅ์€ ๋‚˜๋…ธ ๊ธฐ์ˆ ์˜ ๋ฐœ์ „์œผ๋กœ ์ด์–ด์ง€๊ณ  ์žˆ๋‹ค. ๊ทธ๋ž˜์„œ ๋งŽ์€ ์—ฐ๊ตฌ์ž๋“ค์€ ๋ฐ˜๋„์ฒด์˜ ๊ตญ์†Œ ๋„ํ•‘ ํ”„๋กœํŒŒ์ผ, ๋ฐ˜๋„์ฒด ๋ฐ•๋ง‰์˜ ํ‘œ๋ฉด ๊ฑฐ์น ๊ธฐ, 2 ์ฐจ์› ์žฌ๋ฃŒ์˜ ์ผ ํ•จ์ˆ˜, ๊ตญ์†Œ ํ‘œ๋ฉด ์ „ํ•˜ ๋ถ„ํฌ, ์œ ๊ธฐ-๋ฐ”์ด์˜ค ๋ถ„์ž ๋ฐ•๋ง‰, ๋‚˜๋…ธ ์œ ์ฒด ์žฅ์น˜์˜ ํ‘œ๋ฉด ๋“ฑ์„ ๋ถ„์„ํ•˜๊ธฐ์œ„ํ•ด SPM ์žฅ๋น„๋ฅผ ํ™œ์šฉํ•˜๊ณ  ์žˆ๋‹ค. ์ตœ๊ทผ์—๋Š” ํ‘œ๋ฉด ๋ถ„์„ ๊ธฐ๋Šฅ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ์—ฌ๋Ÿฌ๊ฐ€์ง€ ๊ธฐ๋Šฅ์„ ์ˆ˜ํ–‰ํ•  ์ˆ˜ ์žˆ๋Š” ์›์ž๋ ฅ ํ˜„๋ฏธ๊ฒฝ๋“ค์ด ๋“ฑ์žฅํ•˜๊ณ  ์žˆ๋‹ค. ๊ทธ ์ค‘์—์„œ๋„ ์ €์†Œ์Œ ์›์ž๋ ฅ ํ˜„๋ฏธ๊ฒฝ์€ ๋‚˜๋…ธ ์Šค์ผ€์ผ์˜ ์ฐจ์„ธ๋Œ€ ๋ฐ˜๋„์ฒด ์„ ํญ์„ ์ธก์ •ํ•˜๊ฑฐ๋‚˜ ์ดˆ๋ฐ•๋ง‰์˜ ํ‘œ๋ฉด ๊ฒ€์‚ฌ์— ์ด์šฉ๋  ์ˆ˜ ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ์‚ฐ์—…์ ์ธ ์‘์šฉ์„ ๊ณ ๋ คํ•˜์—ฌ ํ•œ๊ตญํ‘œ์ค€๊ณผํ•™์—ฐ๊ตฌ์›์—์„œ๋Š” ์ €์†Œ์Œ ์›์ž๋ ฅ ํ˜„๋ฏธ๊ฒฝ์„ ๊ฐœ๋ฐœํ•˜์˜€๊ณ , ๋‚˜๋…ธ ์ธ๋ดํ…Œ์ด์…˜ ๊ธฐ๋Šฅ์„ ์ถ”๊ฐ€ํ•˜์—ฌ R&D ์ˆ˜์ค€์—์„œ ์ˆ˜์‹ญ ๋‚˜๋…ธ์˜ ์ •๊ตํ•œ ํŒจํ„ด์„ ํ˜•์„ฑํ•  ์ˆ˜ ์žˆ๋Š” ๊ณต์ • ๋ฐฉ๋ฒ•์„ ๊ฐœ๋ฐœํ•˜๊ณ  ์žˆ๋‹ค. ์ €์†Œ์Œ ์›์ž๋ ฅ ํ˜„๋ฏธ๊ฒฝ์€ ๊ฐœ๋ฐœ ๋ฐฐ๊ฒฝ์˜ ํŠน์„ฑ์ƒ ๋‚ด๋ถ€์ ์ธ ์‹œ๋ฃŒ ์ด๋™ ์Šคํ…Œ์ด์ง€์˜ ์„ค์น˜๋ฅผ ์ง€์–‘ํ•œ๋‹ค. ์ด๋Š” ์ €์†Œ์Œ ์›์ž๋ ฅ ํ˜„๋ฏธ๊ฒฝ์˜ ์ˆ˜์ทจ ์‹ ํ˜ธ ์•ˆ์ •์„ฑ์— ํฌ๊ฒŒ ๊ธฐ์—ฌํ•˜๋Š” ์ตœ์„ ์˜ ์„ ํƒ์ด๊ธด ํ•˜์ง€๋งŒ, ๊ฒ€์‚ฌ ์‹œ๋ฃŒ์˜ ์ธก์ • ์˜์—ญ์„ ์ถ•์†Œ์‹œํ‚ค๋Š” ์•ฝ์ ์œผ๋กœ ์ž‘์šฉํ•˜๊ณ  ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ์ด๋ฅผ ๋ณด์™„ํ•  ์ˆ˜ ์žˆ๋Š” ๋…๋ฆฝ์ ์ธ ์™ธ๋ถ€ ์Šคํ…Œ์ด์ง€๋Š” ํ•„์ˆ˜์ ์ด๋ผ๊ณ  ํ•  ์ˆ˜ ์žˆ๊ธฐ๋•Œ๋ฌธ์—, ์ด ๋…ผ๋ฌธ์—์„œ๋Š” ์ค‘๊ฑฐ๋ฆฌ ์ด๋™ ์Šคํ…Œ์ด์ง€ ๊ฐœ๋ฐœ์„ ํ†ตํ•ด ๊ธฐ์ค€ ์‹œ๋ฃŒ์˜ ์ž„๊ณ„ ์น˜์ˆ˜๋ฅผ ์ธก์ • ํ•  ์ˆ˜ ์žˆ๋„๋ก ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ์™ธ๋ถ€ 4 ์ถ• ์Šคํ…Œ์ด์ง€์˜ ์ตœ๋Œ€ ์ด๋™ ๊ธธ์ด๋Š” 10 mm์ด๋ฉฐ, ํŠน์ • ๋Œ€์ƒ ์˜์—ญ์˜ ์ด๋ฏธ์ง€ ์Šค์บ๋‹์˜ ๊ฒฝ์šฐ, ์ƒ˜ํ”Œ์„ ์™ธ๋ถ€ ์Šคํ…Œ์ด์ง€๋ฅผ ํ†ตํ•ด ๋งˆ์ดํฌ๋ก  ์ •ํ™•๋„์˜ ์œ„์น˜ ์ง€์ •์„ ๊ฑฐ์นœ ํ›„, PI XY piezo ์Šค์บ๋„ˆ๋ฅผ ์ด์šฉํ•˜์—ฌ ๋ฏธ์„ธ ์œ„์น˜ ์„ค์ •์„ ํ•œ๋‹ค. ๊ฐœ๋ฐœ๋œ ์Šคํ…Œ์ด์ง€์˜ ์œ„์น˜ ์—๋Ÿฌ๋Š” ์žฌํ˜„์„ฑ ์‹คํ—˜์„ ํ†ตํ•ด ๋ฌด์‹œํ•  ์ˆ˜ ์žˆ์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ด์–ด์„œ, ๊ฐœ์„ ๋œ ์ˆ˜์ง ํ‰ํ–‰ ๊ตฌ์กฐ(IVPS)์˜ ์ธก๋ฒฝ์„ ์ธก์ •ํ•˜๊ณ  CD ์ธก์ •์˜ ๋ฐ˜๋ณต์„ฑ ๋ฐ ์žฌํ˜„์„ฑ์„ CDR30-EBD ํŒ์„ ์‚ฌ์šฉํ•˜์—ฌ ์ถ”์ •ํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ๋Œ์ถœ ๊ตฌ์กฐ๋กœ ๋œ TGX1 ์ƒ˜ํ”Œ์„ ์ธก์ •ํ•˜์—ฌ ํŒ ๋งˆ๋ชจ๋ฅผ ์ตœ์†Œํ™” ํ•  ์ˆ˜ ์žˆ์Œ์„ ํ™•์ธํ–ˆ๋‹ค. ๋”ฐ๋ผ์„œ ๋…๋ฆฝ์ ์ธ ์™ธ๋ถ€ ์Šคํ…Œ์ด์ง€์˜ ๊ฐœ๋ฐœ์€ ํ–ฅํ›„ ๋„“์€ ์˜์—ญ์„ ์Šค์บ”ํ•ด์•ผํ•˜๋Š” ์—ฌ๋Ÿฌ๊ฐ€์ง€ ์ž„๋ฌด์— ์œ ์šฉํ•˜๊ฒŒ ์ ์šฉ๋  ์ˆ˜ ์žˆ๋‹ค. ์‚ฐ์—…์˜ in-line ์‹œ์Šคํ…œ์—์„œ๋Š” ๋Œ€๋ฉด์  ์›จ์ดํผ์˜ ๊ท ์ผ๋„๋ฅผ ๊ฒ€์‚ฌํ•˜๊ธฐ ์œ„ํ•ด ๊ด‘ํ•™์ ์ธ ์ธก์ •์žฅ๋น„๋ฅผ ํ†ตํ•ด ๋ฐ•๋ง‰ ๊ฒ€์‚ฌ๋ฅผ ์ˆ˜ํ–‰ํ•œ๋‹ค. ํ•˜์ง€๋งŒ ์ตœ๊ทผ ์ฐจ์„ธ๋Œ€ ๋ฐ˜๋„์ฒด ์‚ฐ์—…์—์„œ๋Š” ๊ณ ์šฉ๋Ÿ‰ ๋ฐ ์ €์ „๋ ฅ ๋””๋ฐ”์ด์Šค์˜ ์ถœํ˜„์œผ๋กœ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ ํŒจํ„ด์ด ์ ์  ๋ณต์žกํ•ด์ง€๊ณ  ์ ˆ์—ฐ์ฒด ๋ฐ•๋ง‰์˜ ๋‘๊ป˜๋Š” ์ˆ˜ ๋‚˜๋…ธ ๋ฏธํ„ฐ์—์„œ ์„œ๋ธŒ ๋‚˜๋…ธ ๋ฏธํ„ฐ ๋ฒ”์œ„๋กœ ์ถ•์†Œ๋˜๊ณ  ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ๊ฐ€๊นŒ์šด ๋ฏธ๋ž˜์˜ in-line ๊ณต์ •์—์„œ๋Š” ๋ฐ˜๋„์ฒด ์žฅ์น˜์˜ ์ƒ์‚ฐ ์ˆ˜์œจ ํ–ฅ์ƒ์„ ์œ„ํ•ด์„œ, ์ด๋“ค ๋ฐ•๋ง‰์˜ ๋‘๊ป˜๋ฟ๋งŒ ์•„๋‹ˆ๋ผ 3์ฐจ์› (3D) ํ‘œ๋ฉด ์ •๋ณด๋ฅผ ๊ฒ€์‚ฌํ•˜๋Š” ๊ฒƒ์ด ํ•„์š”ํ•ด์ง€๊ณ  ์žˆ๋‹ค. ์‹ค์ œ ๋ฐ˜๋„์ฒด ๊ณต์ •์„ ๊ฑฐ์นœ ํ‘œ๋ฉด์˜ ๊ฑฐ์น ๊ธฐ๋Š” ํ–ฅํ›„ ์ดˆ๋ฐ•๋ง‰ ๊ณต์ •์— ์˜ํ–ฅ์„ ๋ฏธ์น˜๊ธฐ๋„ ํ•˜๋ฉฐ, ํ‘œ๋ฉด์ด ๊ฑฐ์นœ ์ƒํƒœ์—์„œ๋Š” ์›์ž์ธต ์ฆ์ฐฉ๋ฒ•(atomic layer deposition, ALD)์— ์˜ํ•ด ์ดˆ๋ฐ•๋ง‰ ๊ณต์ •์ด ์ตœ์ ํ™”๋˜์–ด ์žˆ๋‹คํ•˜๋”๋ผ๋„ ์†Œ์ž์— ์˜ํ–ฅ์„ ์ค„ ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์ด๋‹ค. ๋”ฐ๋ผ์„œ ๋ฐ•๋ง‰์˜ ์„ฑ์งˆ์„ ์ •๋Ÿ‰ํ™”ํ•˜๊ณ  ๊ตญ์†Œ์  ํ‘œ๋ฉด ๊ตฌ์กฐ๋ฅผ ๋ถ„์„ํ•˜๊ธฐ์œ„ํ•ด์„œ๋Š” ์›์ž๋ ฅ ํ˜„๋ฏธ๊ฒฝ์ด ๊ฐ€์žฅ ์ ํ•ฉํ•œ ๋ถ„์„๋ฒ•์ด๋ผ๊ณ  ํ•  ์ˆ˜ ์žˆ๋‹ค. ์ด ๋…ผ๋ฌธ์—์„œ๋Š” MOS ํŠธ๋ Œ์ง€์Šคํ„ฐ์˜ high-k ์ ˆ์—ฐ๋ง‰์ธ ํ•˜ํ”„๋Š„ ์‚ฐํ™”๋ง‰ ๊ณต์ •๊ด€๋ฆฌ๋ฅผ ์œ„ํ•œ ๋ฐฉ์•ˆ์œผ๋กœ roughness scaling method๋ฅผ ๊ณ ์•ˆํ•˜์—ฌ ๋‚˜๋…ธ ์Šค์ผ€์ผ์—์„œ ์ตœ์ดˆ๋กœ ์ž„๊ณ„๊ฑฐ์น ๊ธฐ(critical roughness, CR)์„ ์ •์˜ํ•˜์˜€๋‹ค. ๊ธฐํŒ์˜ ํ‘œ๋ฉด๊ฑฐ์น ๊ธฐ๋Š” ์Šต์‹ ์‹๊ฐ ๋ฐฉ์‹์œผ๋กœ ์ง„ํ–‰ํ•˜์˜€์œผ๋ฉฐ, ํ•˜ํ”„๋Š„ ์‚ฐํ™”๋ง‰์„ ์–ป๊ธฐ ์œ„ํ•ด ALD ๊ณต์ •์„ ์ด์šฉํ•˜์˜€๋‹ค. ์ด๋Š” ํ•˜๋ถ€ ์ธต์˜ ๊ฑฐ์น ๊ธฐ๊ฐ€ ์ƒ๋ถ€ ์ธต์˜ ๊ฑฐ์น ๊ธฐ์— ์ฃผ๋Š” ์˜ํ–ฅ์„ฑ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ์ด๋ฉฐ, ์ด ์ •์˜๋ฅผ ํ†ตํ•ด in-line ์‚ฐํ™”๋ง‰ ๊ณต์ •์ƒ์—์„œ ์ƒ์‚ฐ๊ด€๋ฆฌ์˜ ๊ธฐ์ค€์„ ์ œ์‹œํ•  ์ˆ˜ ์žˆ๊ฒŒ ๋˜์—ˆ๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์ดˆ๋ฐ•๋ง‰ ๊ฑฐ์น ๊ธฐ์— ๋”ฐ๋ฅธ MIM ๋‹ค์ด์˜ค๋“œ ๊ตฌ์กฐ๋ฅผ ์‹คํ˜„ํ•จ์œผ๋กœ์จ ์ด ์—ฐ๊ตฌ์—์„œ ์ •์˜๋œ CR๊ฐ’์ด ์‹คํšจ์„ฑ์„ ๊ฐ€์ง์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ ์ด ๋…ผ๋ฌธ์—์„œ๋Š” ๋‹ค๊ธฐ๋Šฅ์„ฑ ์›์žํ˜„๋ฏธ๊ฒฝ์„ ์ด์šฉํ•˜์—ฌ ๋‚˜๋…ธ ์ธ๋ดํ…Œ์ด์…˜ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ๊ทธ ์ฒซ๋ฒˆ์งธ ์—ฐ๊ตฌ๋Š” ์ „์ž๋น” ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ๋กœ๋Š” ์ œ์ž‘ํ•  ์ˆ˜ ์—†๋Š” ๋ฐ”์ด์˜ค ํ•„๋ฆ„ ์ƒ์— ๋‚˜๋…ธ ๋ฐ ๋งˆ์ดํฌ๋กœ ํŒจํ„ด์„ ํ˜•์„ฑํ•จ์œผ๋กœ์จ ์ „์ž๋น” ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ์˜ ์ทจ์•ฝ์ ์„ ๋ณด์™„ํ•  ์ˆ˜ ๊ณต์ • ๋ฐฉ๋ฒ•์ด ๋  ์ˆ˜ ์žˆ์Œ์„ ์ œ์‹œํ•˜๋Š” ๊ฒƒ์ด๋ฉฐ, ๋‘๋ฒˆ์งธ ์—ฐ๊ตฌ๋Š” ๋‚˜๋…ธ ์ธ๋ดํ…Œ์ด์…˜์˜ ๊ทผ๋ณธ์ ์ธ ๋ฌธ์ œ์ ์ธ ๋ฒŒ์ง€๋ฅผ ์„ ํƒ์ ์œผ๋กœ ์ œ๊ฑฐํ•˜๋Š” ์—ฐ๊ตฌ์ด๋‹ค. ์šฐ์„  ๋‹ค๊ธฐ๋Šฅ์„ฑ ์›์žํ˜„๋ฏธ๊ฒฝ ํ™œ์šฉ์˜ ์ฒซ๋ฒˆ์งธ ์—ฐ๊ตฌ๋กœ๋Š” ๋ฐ”์ด์˜ค ํ•„๋ฆ„์ƒ์— ๋‚˜๋…ธ/๋งˆ์ดํฌ๋กœ ํŒจํ„ด์„ ํ˜•์„ฑํ•˜๋Š” ์ผ์ด๋‹ค. ์ด ํŒจํ„ด๋œ ๋ฐ”์ด์˜ค ํ•„๋ฆ„์€ ๋น„ํ–‰ ์‹œ๊ฐ„ 2 ์ฐจ ์ด์˜จ ์งˆ๋Ÿ‰ ๋ถ„์„ (TOF-SIMS)์˜ ํ™”ํ•™์  ์„ฑ๋ถ„ ์ด๋ฏธ์ง• ๋ฐ ๊นŠ์ด ๋ถ„์„์— ์œ ์šฉํ•œ ๊ฐ•๋ ฅํ•œ ์‹œ๋ฃŒ๋กœ ์‚ฌ์šฉ๋  ์ˆ˜ ์žˆ๋‹ค. TOF-SIMS ๋ถ„์„์—์„œ Arn + ๊ฐ€์Šค ํด๋Ÿฌ์Šคํ„ฐ ์ด์˜จ ์†Œ์Šค (GCIB)๋Š” ์ฃผ๋กœ ํ‘œ๋ฉด ๋ถ„์„์˜ ์†Œ์Šค๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๋‚ฎ์€ ์†์ƒ ๋‹จ๋ฉด ๋ฐ ๋ถ„์ž ๊นŠ์ด ํ”„๋กœํŒŒ์ผ ๋ง ์‹คํ—˜์„ ์œ„ํ•œ ๋น ๋ฅธ ์นจ์‹ ์†๋„๋ฅผ ๊ฐ–๋Š” ์นจ์‹ ์†Œ์Šค๋กœ์„œ ๋„๋ฆฌ ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ SIMS ๋ถ„์„์—์„œ 3D depth profile์— ๋Œ€ํ•œ ์นจ์‹ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ์ดํ•ดํ•˜๋ ค๋ฉด ์ž˜ ์ •์˜ ๋œ 3D ์œ ๊ธฐ ๋ฏธ์„ธ ํŒจํ„ด์œผ๋กœ ๋ณด์ •ํ•ด์•ผ ํ•˜๋Š”๋ฐ, ์ด๋•Œ ๋‚˜๋…ธ ์ธ๋ดํ…Œ์ด์…˜ ๊ธฐ์ˆ ์„ ์ด์šฉํ•œ๋‹ค. ์ด ๊ธฐ๋ฒ•์€ TOF-SIMS์˜ 3D ํ™”ํ•™์  ์„ฑ๋ถ„ ๋ถ„์„/์ด๋ฏธ์ง•์„์œ„ํ•œ ํ‘œ์ค€ ๋ฐ”์ด์˜ค ์‹œ๋ฃŒ๋กœ ์‚ฌ์šฉ๋  ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€ํ•œ๋‹ค. ๋‘๋ฒˆ์งธ ์ธ๋ดํ…Œ์ด์…˜ ํ™œ์šฉ ์—ฐ๊ตฌ๋Š” ํƒ์นจ์ด ์†Œํ”„ํŠธ ํ•„๋ฆ„์„ ๋ˆ„๋ฅผ ๋•Œ ๋ฐœ์ƒํ•˜๋Š” ๋ฒŒ์ง€๋ฅผ ์„ ํƒ์ ์œผ๋กœ ์ œ๊ฑฐํ•˜๋Š” ์—ฐ๊ตฌ๋กœ์จ, PMMA ํ•„๋ฆ„์ด ๋‚˜๋…ธ ํŒจํ„ด ํ˜•์„ฑ์ธต์ด ๋˜๋„๋ก ์‚ฌ์šฉํ•œ๋‹ค. ๊ทธ๋™์•ˆ ๋ฒŒ์ง€๋Š” ์ธ๋ดํ…Œ์ด์…˜ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ์˜ ๋ฐœ์ „์„ ์ €ํ•ดํ•˜๋Š” ๊ฐ€์žฅ ํฐ ์š”์ธ์œผ๋กœ์จ ์„ ํƒ์ ์ธ ์ œ๊ฑฐ๊ฐ€ ์–ด๋ ค์šด ๊ฒƒ์œผ๋กœ ์•Œ๋ ค์ ธ ์žˆ์—ˆ๋‹ค. ํ•˜์ง€๋งŒ ์ด ๋…ผ๋ฌธ์—์„œ๋Š” ํ˜„์ƒ์•ก์„ ์ด์šฉํ•œ ๊ฐ„๋‹จํ•œ ๋ฐฉ์‹์œผ๋กœ ๋‹ค๋‹จ๊ณ„์˜ ๋ฒŒ์ง€ ์—†๋Š” ํŒจํ„ฐ๋‹ ๋ฐฉ์‹์„ ์ตœ์ดˆ๋กœ ์†Œ๊ฐœํ•จ์œผ๋กœ์จ ์ƒˆ๋กœ์šด ์ฐจ์›์˜ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ ๊ธฐ๋ฒ•์„ ์ œ์•ˆํ•˜๊ณ  ์žˆ๋‹ค. ๋˜ํ•œ ์ด ๊ธฐ๋ฒ•์€ 3์ฐจ์› ๋‚˜๋…ธ ํŒจํ„ด์„ ์„ฑ๊ณต์ ์œผ๋กœ ๋ณต์ œ ๋ชฐ๋“œ์— ์ „์‚ฌํ•  ์ˆ˜ ์žˆ์œผ๋ฏ€๋กœ ๊ณต์ • ๋น„์šฉ ์ ˆ๊ฐ ํšจ๊ณผ๋Š” ๋ฌผ๋ก ์ด๊ณ , ๋‹ค์–‘ํ•œ ์—ฐ๊ตฌ ๋ถ„์•ผ์—์„œ ์ด๋ฅผ ํ™œ์šฉํ•  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€ํ•œ๋‹ค.Abstract ............................... iv List of Figures ....................... xiii List of Tables ........................ xxi Chapter 1 Introduction 1 1.1 Multifunctional atomic force microscopy 1 1.2 Background on development of external stage for low noise AFM 2 1.3 Industrial applications for low noise atomic force microscopy 4 1.3.1 Critical dimension 4 1.3.2 Emergence of ultrathin films 7 1.4 Applications of indentation lithography using low noise atomic force microscopy 8 1.4.1 Demand for biological applications 8 1.4.2 Various lithography techniques 13 1.4.3 Strengths and limitations of AFM indentation lithography 13 1.5. The aims of this study 15 1.6. Reference 16 Chapter 2 Development of external automation stage for LN-AFM 25 2.1 Configurations of LN-AFM 25 2.2 Development of independent external stage 29 2.2.1 Configurations of the external stage 29 2.2.2 Position adjustment method 34 2.2.3 Position accuracy test 38 2.3. Reference 45 Chapter 3 Industrial applications using the LN-AFM with the external stage 47 3.1 Industrial demands 47 3.2 Critical dimension measurements 49 3.2.1 Vector approach probing method 49 3.2.2 Advantages and limitations 50 3.2.3 CD measurement using vertical structure 50 3.2.4 Tip wear test 55 3.3 Critical roughness measurements 58 3.3.1 Fabrication of ultrathin film using atomic layer deposition 58 3.3.2 Reliability of surface roughness measurements 60 3.3.3 Interfacial effects using roughness scaling method 63 3.3.4 Definition of critical roughness 68 3.3.5 Effectiveness of the critical roughness 74 3.3.6 Inline applications for the morphology analysis of ultrathin hafnium oxide films 76 3.4. Reference 81 Chapter 4 Applications of indentation lithography 88 4.1 Patterned organic films for 3D depth profiles of TOF-SIMS imaging 88 4.1.1 Fabrication method of organic dual layer for 3D TOF-SIMS 88 4.1.2 Results for organic dual layer for 3D TOF-SIMS 90 4.1.3 Fabrication issues of patterned organic dual layer 92 4.1.4 3D depth profile of patterned organic dual layer 97 4.2 Bulge-free indentation technique 100 4.2.1 PMMA bulge removal using IPA/DI developer 100 4.2.2 Mechanism study on the selective bulge removal process 105 4.2.3 Optimal condition for bulge-free indentation 108 4.2.4 3D bulge-free nano-patterns 112 4.3. Reference 115 Chapter 5 Conclusion 119 5.1 Discussion and conclusion 119 5.2 Reference 124 ๊ตญ ๋ฌธ ์ดˆ ๋ก 126Docto

    Properties and behaviour of Pb-free solders in flip-chip scale solder interconnections

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    Due to pending legislations and market pressure, lead-free solders will replace Snโ€“Pb solders in 2006. Among the lead-free solders being studied, eutectic Snโ€“Ag, Snโ€“Cu and Snโ€“Agโ€“Cu are promising candidates and Snโ€“3.8Agโ€“0.7Cu could be the most appropriate replacement due to its overall balance of properties. In order to garner more understanding of lead-free solders and their application in flip-chip scale packages, the properties of lead free solders, including the wettability, intermetallic compound (IMC) growth and distribution, mechanical properties, reliability and corrosion resistance, were studied and are presented in this thesis. [Continues.

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    Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 2012.Cataloged from PDF version of thesis.Includes bibliographical references (p. 215-225).Planarization processes are a key enabling technology for continued performance and density improvements in integrated circuits (ICs). Dielectric material planarization is widely used in front-end-of-line (FEOL) processing for device isolation and in back-end-of-line (BEOL) processing for interconnection. This thesis studies the physical mechanisms and variations in the planarization using chemical mechanical polishing (CMP). The major achievement and contribution of this work is a systematic methodology to physically model and characterize the non-uniformities in the CMP process. To characterize polishing mechanisms at different length scales, physical CMP models are developed in three levels: wafer-level, die-level and particle-level. The wafer-level model investigates the CMP tool effects on wafer-level pressure non-uniformity. The die-level model is developed to study chip-scale non-uniformity induced by layout pattern density dependence and CMP pad properties. The particle-level model focuses on the contact mechanism between pad asperities and the wafer. Two model integration approaches are proposed to connect wafer-level and particle-level models to the die-level model, so that CMP system impacts on die-level uniformity and feature size dependence are considered. The models are applied to characterize and simulate CMP processes by fitting polishing experiment data and extracting physical model parameters. A series of physical measurement approaches are developed to characterize CMP pad properties and verify physical model assumptions. Pad asperity modulus and characteristic asperity height are measured by nanoindentation and microprofilometry, respectively. Pad aging effect is investigated by comparing physical measurement results at different pad usage stages. Results show that in-situ conditioning keeps pad surface properties consistent to perform polishing up to 16 hours, even in the face of substantial pad wear during extended polishing. The CMP mechanisms identified from modeling and physical characterization are applied to explore an alternative polishing process, referred to as pad-in-a-bottle (PIB). A critical challenge related to applied pressure using pad-in-a-bottle polishing is predicted.by Wei Fan.Ph.D

    Reliability Analysis of Electrotechnical Devices

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    This is a book on the practical approaches of reliability to electrotechnical devices and systems. It includes the electromagnetic effect, radiation effect, environmental effect, and the impact of the manufacturing process on electronic materials, devices, and boards

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    The advances of microelectromechanical systems (MEMS) and devices have been instrumental in the demonstration of new devices and applications, and even in the creation of new fields of research and development: bioMEMS, actuators, microfluidic devices, RF and optical MEMS. Experience indicates a need for MEMS book covering these materials as well as the most important process steps in bulk micro-machining and modeling. We are very pleased to present this book that contains 18 chapters, written by the experts in the field of MEMS. These chapters are groups into four broad sections of BioMEMS Devices, MEMS characterization and micromachining, RF and Optical MEMS, and MEMS based Actuators. The book starts with the emerging field of bioMEMS, including MEMS coil for retinal prostheses, DNA extraction by micro/bio-fluidics devices and acoustic biosensors. MEMS characterization, micromachining, macromodels, RF and Optical MEMS switches are discussed in next sections. The book concludes with the emphasis on MEMS based actuators

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