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    3-5์กฑ ํ™”ํ•ฉ๋ฌผ ๋ฐ˜๋„์ฒด์˜ ์›จ์ดํผ ์ ‘ํ•ฉ๊ณผ ์—ํ”ผํƒ์…œ ๋ฆฌํ”„ํŠธ ์˜คํ”„๋ฅผ ํ†ตํ•œ ๋‹ค์ค‘ ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์žฌ๋ฃŒ๊ณตํ•™๋ถ€, 2019. 2. ์œค์˜์ค€.Group III-V compound semiconductors, having a band gap from ultraviolet to infrared regions, have been widely used as imagers to visualize a single band. With the recent arrival of the Internet-of-things (IOTs) era, new applications such as time of flight (TOF) sensors, normalized difference vegetation index (NVDI) and night vision systems have gained interest. Therefore, the importance of multicolor photodetectors is raised. To implement multicolor photodetectors, an epitaxy method has been commonly used with III-V compound semiconductors. For example, quantum wells, quantum dots and type-II based structures and metamorphically grown bulk heteroepitaxial structures have been employed. Although an epitaxy method seems to be quite simple, there are several problems including limitation of material choice due to the discrepancy of lattice constants between thin films and substrates, performance degradation originated from internal defects and complexity of growth. Therefore, to avoid these disadvantages of the epitaxy method, a heterogeneous integration method has been an alternative because the integration of devices grown on different substrates is possible. Thus, it has been considered to be a promising method to combine photodetectors with simple bulk structures. However, although there is a significant advantage to the heterogeneous integration method, current multicolor photodetectors have exhibited limitations regarding pixel density and vertical misalignment due to problems related to conventional integration methods. Therefore, in this thesis, the heterogeneous integration of III-V compound semiconductors was investigated for fabricating multicolor photodetectors with high pixel density and highly accurate alignment. Firstly, a research on heterogeneous integration of GaAs based thin film devices with other substrates was carried out. We studied wafer bonding and epitaxial lift off process which have advantages including large area transferability, cost-effectiveness and high quality of layers compared with wafer splitting and transfer printing methods. To fabricate multicolor photodetectors on single substrates, a stable rigid-to-rigid heterogeneous integration method is highly required. However, there have only been few reports regarding rigid-to-rigid transfer by using epitaxial lift off due to the difficulty involving byproducts and gas bubbles generated during the wet etching of the sacrificial layer for wafer separation. This has been a hindrance compared with thin film on flexible substrates which can accelerate wafer separation by using strain and external equipment. In order to overcome this problem, high throughput epitaxial lift off process was proposed through a pre-patterning process and surface hydrophilization. The pre-patterning process can maximize the etching area of the AlAs sacrificial layer and rapidly remove bubbles. In addition, acetone, which is a hydrophilic solution, was mixed with hydrofluoric acid in order to reduce the surface contact angle and viscosity. It resulted in an effective penetration of the etching solution and the suppression of byproducts. Consequently, it was possible to transfer GaAs thin films on rigid substrates within 30 minutes for a 2 inch wafer which has been the fastest compared with previous reports. Also, using this template, electronic and optoelectronic devices were successfully fabricated and operated. Secondly, we have studied to overcome restrictions of bulk photodetector for InSb binary material including the detection limit and cryogenic operation. To extend the detection limit of bulk InSb toward the LWIR range, the ideal candidate of III-V bulk materials is indium arsenide antimonide (InAsSb) material due to its corresponding band gaps ranging from SWIR to LWIR. By combining bulk InAsSb with other bulk materials with previously developed integration methods, we could ultimately fabricate a multicolor photodetector ranging from ultraviolet to LWIR with only bulk structures. Thus, in order to verify the viability of this material, a p-i-n structure based photodetector with an InAs0.81Sb0.19 absorption layer was grown on a GaAs substrate. To enhance an ability to be operated at a high temperature, an optimum InAlSb barrier layer was designed by technology computer aided design (TCAD). Also, InAsSb/InAlSb heterojunction photodetector was grown by molecular beam epitaxy (MBE). As a result, we have demonstrated the first room temperature operation of heterojunction photodetectors in MWIR range among InAsSb photodetectors with similar Sb compositions. Additionally, it has a higher responsivity of 15 mA/W compared with commercialized photodetectors. This MWIR photodetector with room temperature operability could help the reduction of the volume for final detector systems due to the elimination of Dewar used in InSb photodetectors. In other words, from this experiments, it is suggested that there is a strong potential of InAsSb bulk structures for detecting LWIR. Finally, the study on the monolithic integration was carried out to verify the feasibility of multicolor photodetectors by integration of bulk structures. Among procured photodetectors with detection ranging from visible to MWIR at room temperature operation, visible GaAs and near-infrared InGaAs photodetector were used for establishing the optimized fabrication process due to materials process maturity. By using previously developed high throughput ELO process, GaAs photodetectors were transferred onto InGaAs photodetectors to form visible/near-infrared multicolor photodetectors. It was found that top GaAs PD and bottom InGaAs PD were vertically well aligned without an off-axis tilt in x-ray diffraction (XRD) measurement. Also, similar dark currents of each photodetector were observed compared with reference photodetectors. Finally, with incidence of laser illumination, photoresponses were clearly revealed in visible band and near-infrared band of material characteristics, respectively. These results suggested high throughput ELO process enables the monolithic integration of bulk based multicolor photodetectors on a single substrate with high pixel density and nearly perfect vertical alignment. In the future, depending on the target applications, photodetectors with desired wavelengths could be simply grown as bulk structures and fabricated for multicolor imagers.์ž์™ธ์„ ๋ถ€ํ„ฐ ์ ์™ธ์„  ์˜์—ญ์˜ ๋ฐด๋“œ๊ฐญ์„ ๊ฐ€์ง„ 3-5์กฑ ํ™”ํ•ฉ๋ฌผ ๋ฐ˜๋„์ฒด๋Š” ๋‹จ์ผ ํŒŒ์žฅ๋Œ€์—ญ์„ ์‹œ๊ฐํ™”ํ•˜๋Š” imager ๋กœ ๋„๋ฆฌ ์‚ฌ์šฉ๋˜๊ณ  ์žˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜, ์ตœ๊ทผ ์‚ฌ๋ฌผ์ธํ„ฐ๋„ท ์‹œ๋Œ€๊ฐ€ ๋„๋ž˜ํ•จ์— ๋”ฐ๋ผ, time of flight (TOF) ์„ผ์„œ, ์‹์ƒ์ง€์ˆ˜ ์ธก์ •, night vision ๋“ฑ์˜ ์ƒˆ๋กœ์šด ์‘์šฉ์ฒ˜๊ฐ€ ์ฆ๊ฐ€ํ•˜๊ณ  ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ๊ธฐ์กด์˜ ๋‹จ์ผํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๊ฐ€ ์•„๋‹Œ, ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ์˜ ์ค‘์š”์„ฑ์ด ์ฆ๋Œ€๋˜๊ณ  ์žˆ์œผ๋ฉฐ, ์ด๋Ÿฐ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•ด์„œ 3-5์กฑ์„ ํ™”ํ•ฉ๋ฌผ ๋ฐ˜๋„์ฒด์˜ epitaxy ๋ฐฉ๋ฒ•์ด ํ”ํžˆ ์‚ฌ์šฉ๋˜์–ด ์™”๋‹ค. ์˜ˆ๋ฅผ ๋“ค์–ด, ๋‹ค๋ฅธ ๊ฒฉ์ž ์ƒ์ˆ˜๋ฅผ ๊ฐ€์ง„ ๋ฒŒํฌ ๊ตฌ์กฐ๋ฅผ metamorphic ์„ฑ์žฅ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ์„ฑ์žฅํ•˜๊ฑฐ๋‚˜, ๋˜๋Š” ์–‘์ž์šฐ๋ฌผ, ์–‘์ž์  ๊ทธ๋ฆฌ๊ณ  type-II ๊ธฐ๋ฐ˜์˜ ๊ตฌ์กฐ๊ฐ€ ์ ์šฉ๋˜์–ด์•ผ๋งŒ ํ–ˆ๋‹ค. Epitaxy ๋ฐฉ๋ฒ•์€ ๋งค์šฐ ๊ฐ„๋‹จํ•œ ๋ฐฉ๋ฒ•์ฒ˜๋Ÿผ ๋ณด์ด์ง€๋งŒ, ๊ธฐํŒ๊ณผ ์„ฑ์žฅํ•˜๋ ค๋Š” ๋ฌผ์งˆ๊ฐ„์˜ ๊ฒฉ์ž์ƒ์ˆ˜์˜ ์ฐจ์ด๋กœ ์ธํ•ด ์ œํ•œ๋˜๋Š” ๋ฌผ์งˆ ์„ ํƒ, ๋‚ด๋ถ€ ๊ฒฐํ•จ์— ์˜ํ•œ ์„ฑ๋Šฅ๊ฐ์†Œ ๊ทธ๋ฆฌ๊ณ  ์„ฑ์žฅ์˜ ๋ณต์žกํ•จ ๋“ฑ ์—ฌ๋Ÿฌ ๋ฌธ์ œ๊ฐ€ ์กด์žฌํ•œ๋‹ค. ๊ทธ๋ž˜์„œ, epitaxy ๋ฐฉ๋ฒ•์˜ ๋‹จ์ ๋“ค์„ ํšŒํ”ผํ•˜๊ธฐ ์œ„ํ•˜์—ฌ, ๋‹ค๋ฅธ ๊ธฐํŒ์—์„œ ์„ฑ์žฅ๋œ ์†Œ์ž์˜ ์ง‘์ ์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•  ์ˆ˜ ์žˆ๋Š”, ์ด์ข… ์ง‘์  ๋ฐฉ๋ฒ•์ด ๋Œ€์•ˆ์ด ๋˜์–ด์™”๋‹ค. ์ด๋ฅผ ์ด์šฉํ•˜๋ฉด, ๊ฐ„๋‹จํ•œ ๋ฒŒํฌ ๊ตฌ์กฐ์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ๊ฒฐํ•ฉํ•  ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์— ๋งค์šฐ ์œ ๋งํ•œ ๋ฐฉ๋ฒ•์œผ๋กœ ์—ฌ๊ฒจ์ง€๊ณ  ์žˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜, ์ด์ข… ์ง‘์  ๋ฐฉ๋ฒ•์˜ ๋›ฐ์–ด๋‚œ ์žฅ์ ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , ํ˜„์žฌ์˜ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋Š” ์ง‘์  ๋ฐฉ๋ฒ•์˜ ๋ฌธ์ œ๋กœ ์ˆ˜์ง ์ •๋ ฌ ์˜ค์ฐจ ๋ฐ ํ”ฝ์…€ ๋ฐ€๋„ ์ธก๋ฉด์—์„œ ํ•œ๊ณ„์ ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ๋”ฐ๋ผ์„œ, ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๊ณ ๋ฐ€๋„/ ๊ณ ์ •๋ ฌ๋œ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ ์ œ์ž‘์„ ์œ„ํ•œ 3-5์กฑ ๊ธฐ๋ฐ˜์˜ ํ™”ํ•ฉ๋ฌผ ๋ฐ˜๋„์ฒด์˜ ์ด์ข… ์ง‘์  ๋ฐฉ๋ฒ•์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ๋จผ์ €, 3-5์กฑ GaAs ๊ธฐ๋ฐ˜์˜ ๋ฐ•๋ง‰์†Œ์ž๋ฅผ ๋‹ค๋ฅธ ๊ธฐํŒ๊ณผ ์ด์ข… ์ง‘์ ํ•˜๋Š” ์—ฐ๊ตฌ๋ฅผ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ๊ธฐ์กด์˜ wafer splitting ๊ณผ transfer printing ๋ฐฉ๋ฒ•๊ณผ ๋น„๊ตํ–ˆ์„ ๋•Œ ๋Œ€๋ฉด์  ์ „์‚ฌ, ์ €๋ ดํ•œ ๊ฐ€๊ฒฉ ๊ทธ๋ฆฌ๊ณ  ๊ณ ํ’ˆ์งˆ layer๋“ฑ ์žฅ์ ๋“ค์ด ์žˆ๋Š” ์›จ์ดํผ ์ ‘ํ•ฉ๊ณผ ์—ํ”ผํƒ์…œ ๋ฆฌํ”„ํŠธ ์˜คํ”„ (epitaxial lift off) ๋ฐฉ๋ฒ•์— ๋Œ€ํ•ด์„œ ์—ฐ๊ตฌ๋ฅผ ํ•˜์˜€๋‹ค. ๋‹จ์ผ ๊ธฐํŒ์ƒ์— ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ์ œ์ž‘ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š”, rigid-to-rigid ์ด์ข… ์ง‘์  ๋ฐฉ๋ฒ•์ด ๋ฐ˜๋“œ์‹œ ํ•„์š”ํ•˜๋‹ค. ๊ทธ๋Ÿฌ๋‚˜, strain ๊ณผ ์™ธ๋ถ€ ์žฅ์น˜๋ฅผ ์ด์šฉํ•˜์—ฌ ๊ธฐํŒ ๋ถ„๋ฆฌ๋ฅผ ๊ฐ€์†ํ™” ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ์œ ์—ฐ๊ธฐํŒ ์ƒ์˜ ๋ฐ•๋ง‰์ „์‚ฌ์™€ ๋‹ฌ๋ฆฌ, ์Šต์‹ ์‹๊ฐ ์‹œ ์ƒ์„ฑ๋˜๋Š” ๋ถ€์‚ฐ๋ฌผ๋“ค๊ณผ ๊ฐ€์Šค ๊ธฐํฌ๋“ค ๋•Œ๋ฌธ์— ์—ํ”ผํƒ์…œ ๋ฆฌํ”„ํŠธ ์˜คํ”„ ๋ฐฉ๋ฒ•์„ ์ด์šฉํ•œ rigid-to-rigid ์ „์‚ฌ์— ๋Œ€ํ•ด์„œ๋Š” ๋งค์šฐ ์ ์€ ๊ฒฐ๊ณผ๋งŒ์ด ๋ณด๊ณ ๋˜์—ˆ๋‹ค. ์ด๋Ÿฐ ๋ฌธ์ œ๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด์„œ, pre-patterning ๊ณผ์ •๊ณผ ํ‘œ๋ฉด ์นœ์ˆ˜ํ™”๋ฅผ ํ†ตํ•œ ๊ณ ์† ์—ํ”ผํƒ์…œ ๋ฆฌํ”„ํŠธ ์˜คํ”„๋ฅผ ์ œ์•ˆํ•˜์˜€๋‹ค. ์ด pre-patterning ๊ณผ์ •์€ AlAs ํฌ์ƒ์ธต์˜ ์‹๊ฐ ์˜์—ญ์„ ๊ทน๋Œ€ํ™” ์‹œํ‚ฌ ์ˆ˜ ์žˆ์œผ๋ฉฐ, ๊ธฐํฌ๋ฅผ ๋น ๋ฅด๊ฒŒ ์ œ๊ฑฐํ•  ์ˆ˜ ์žˆ๋‹ค. ๊ทธ๋ฆฌ๊ณ , ์นœ์ˆ˜์„ฑ ์šฉ์•ก์ธ ์•„์„ธํ†ค์„ ๋ถˆ์‚ฐ๊ณผ ์„ž์–ด์ฃผ๋ฉด ์ ๋„์™€ ํ‘œ๋ฉด ์ ‘์ด‰ ๊ฐ์„ ์ค„์ผ ์ˆ˜ ์žˆ๋‹ค. ์ด๊ฒƒ์€ ์‹๊ฐ ์šฉ์•ก์˜ ํšจ๊ณผ์ ์ธ ์นจํˆฌ์™€ ๋ถ€์‚ฐ๋ฌผ์„ ์–ต์ œ์‹œํ‚ค๋Š” ๊ฒฐ๊ณผ๋ฅผ ๋ณด์˜€๋‹ค. ๊ฒฐ๊ณผ์ ์œผ๋กœ, 2 ์ธ์น˜ ํฌ๊ธฐ์˜GaAs ๊ธฐ๋ฐ˜ ๋ฐ•๋ง‰๋“ค์„ rigid ๊ธฐํŒ์ƒ์— 30๋ถ„ ์ด๋‚ด๋กœ ์ „์‚ฌ๊ฐ€ ๊ฐ€๋Šฅํ–ˆ์œผ๋ฉฐ ์ด๋Š” ๊ธฐ์กด์˜ ๋ณด๊ณ ๋“ค๊ณผ ๋น„๊ตํ–ˆ์„ ๋•Œ ๊ฐ€์žฅ ๋น ๋ฅธ ๊ฒฐ๊ณผ์ด๋‹ค. ๋˜ํ•œ ์ด ํ…œํ”Œ๋ฆฟ์„ ์ด์šฉํ•˜์—ฌ ๊ด‘/์ „์ž ์†Œ์ž๋ฅผ ์„ฑ๊ณต์ ์œผ๋กœ ์ œ์ž‘ ๋ฐ ๋™์ž‘์‹œ์ผฐ๋‹ค. ๋‘ ๋ฒˆ์งธ๋กœ, ๊ธฐ์กด์˜ InSb ๋ฌผ์งˆ์„ ์ด์šฉํ•œ ๋ฒŒํฌ ๊ตฌ์กฐ์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๊ฐ€ ๊ฐ€์ง„ ํŒŒ์žฅํ•œ๊ณ„ ๊ทธ๋ฆฌ๊ณ  ์ €์˜จ๋™์ž‘ ๋“ฑ์˜ ์ œ์•ฝ๋“ค์„ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•œ ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ๋ฒŒํฌ ๊ตฌ์กฐ์˜ ํŒŒ์žฅ ํ•œ๊ณ„๋ฅผ ์›์ ์™ธ์„  ๋Œ€์—ญ๊นŒ์ง€ ๋Š˜์ด๊ธฐ ์œ„ํ•œ, 3-5์กฑ ๋ฌผ์งˆ ์ค‘ ์ด์ƒ์ ์ธ ๋ฌผ์งˆ์€ ์ธ๋“ ์•„์„ธ๋‚˜์ด๋“œ ์•ˆํ‹ฐ๋ชจ๋‚˜์ด๋“œ (indium arsenide antimonide) ์ด๋‹ค. ์™œ๋ƒํ•˜๋ฉด InAsxSb1-x๋Š” SWIR ๋ถ€ํ„ฐ LWIR ์˜ ํ•ด๋‹นํ•˜๋Š” ๋ฐด๋“œ ๊ฐญ์„ ๊ฐ€์ง€๊ณ  ์žˆ๊ธฐ ๋•Œ๋ฌธ์ด๋‹ค. ์ด ๋ฌผ์งˆ ๊ธฐ๋ฐ˜์˜ ๊ตฌ์กฐ์™€ ๊ฐœ๋ฐœ๋œ ๊ณต์ •์„ ์‚ฌ์šฉํ•˜๋ฉด, ์šฐ๋ฆฌ๋Š” ๊ถ๊ทน์ ์œผ๋กœ ์ž์™ธ์„ ๋ถ€ํ„ฐ ์›์ ์™ธ์„ ๊นŒ์ง€์˜ ์˜์—ญ์„ ๋ฒŒํฌ ๊ตฌ์กฐ๋งŒ์„ ์‚ฌ์šฉํ•˜์—ฌ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ๊ตฌํ˜„ํ•  ์ˆ˜ ์žˆ๊ฒŒ ๋œ๋‹ค. ๋”ฐ๋ผ์„œ, ์ด ๋ฌผ์งˆ์˜ ๊ฐ€๋Šฅ์„ฑ์„ ๊ฒ€์ฆํ•˜๊ธฐ ์œ„ํ•ด์„œ, InAs0.81Sb0.19 ์˜ ํก์ˆ˜์ธต์„ ๊ฐ€์ง„ p-i-n ๊ตฌ์กฐ ๊ธฐ๋ฐ˜์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ GaAs ๊ธฐํŒ์ƒ์—์„œ ์„ฑ์žฅํ•˜์˜€๋‹ค. ๊ณ ์˜จ์—์„œ ๋™์ž‘ ํŠน์„ฑ์„ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•˜์—ฌ, ์ตœ์ ์˜ InAlSb ๋ฐฐ๋ฆฌ์–ด๋ฅผ TCAD๋กœ ๋””์ž์ธํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ, InAsSb/InAlSb ์ด์ข… ์ ‘ํ•ฉ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋Š” ๋ถ„์ž์„  ์ฆ์ฐฉ ์žฅ๋น„๋ฅผ ์ด์šฉํ•˜์—ฌ ์„ฑ์žฅ๋˜์—ˆ๋‹ค. ๊ทธ ๊ฒฐ๊ณผ๋กœ, ์šฐ๋ฆฌ๋Š” ๋น„์Šทํ•œ Sb ์กฐ์„ฑ์„ ๊ฐ€์ง„ InAsSb ๊ธฐ๋ฐ˜์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋“ค ์ค‘์—์„œ, ์ฒ˜์Œ์œผ๋กœ ์ค‘์ ์™ธ์„  ๋Œ€์—ญ์˜ ์ด์ข… ์ ‘ํ•ฉ ๊ตฌ์กฐ์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ์ƒ์˜จ ๋™์ž‘ ํ•˜๋Š” ๊ฒƒ์„ ์‹œ์—ฐํ•˜์˜€๋‹ค. ๊ฒŒ๋‹ค๊ฐ€, ๊ทธ๊ฒƒ์€ ์ƒ์šฉํ™” ๋œ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ณด๋‹ค ๋†’์€ ๊ด‘ ์‘๋‹ต ํŠน์„ฑ(15 mA/W)์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ์ด ์ƒ์˜จ์—์„œ ๋™์ž‘ํ•˜๋Š” ์ค‘์ ์™ธ์„  ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋Š” InSb ๊ด‘ ๊ฒ€์ถœ๊ธฐ์— ์‚ฌ์šฉ๋˜๋Š” Dewar ๋ฅผ ์ œ๊ฑฐํ•จ์œผ๋กœ์จ, ์ตœ์ข… ๊ฒ€์ถœ๊ธฐ ์‹œ์Šคํ…œ์˜ ๋ถ€ํ”ผ๋ฅผ ๊ฐ์†Œ ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ์ด ์‹คํ—˜์œผ๋กœ๋ถ€ํ„ฐ, ๋ฒŒํฌ ๊ตฌ์กฐ๋กœ ์›์ ์™ธ์„  ๋Œ€์—ญ์„ ๊ฒ€์ถœํ•˜๊ธฐ ์œ„ํ•œ InAsSb ๋ฌผ์งˆ์˜ ํฐ ์ž ์žฌ์„ฑ์ด ์žˆ๋‹ค๋Š” ๊ฒƒ์„ ์˜๋ฏธํ•œ๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ๋ฒŒํฌ ๊ตฌ์กฐ์˜ ์ง‘์ ์„ ํ†ตํ•œ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ์˜ ์‹คํ˜„์ด ๊ฐ€๋Šฅํ•œ์ง€ ํ™•์ธํ•˜๊ธฐ ์œ„ํ•ด์„œ ๋ชจ๋†€๋ฆฌ์‹(monolithic) ์ง‘์ ์— ๊ด€ํ•œ ์—ฐ๊ตฌ๋ฅผ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. ํ™•๋ณด๋œ ์ƒ์˜จ ๋™์ž‘์ด ๊ฐ€๋Šฅํ•œ ๊ฐ€์‹œ๊ด‘์„ ๋ถ€ํ„ฐ MWIR ๊ฒ€์ถœ ํŒŒ์žฅ์„ ๊ฐ€์ง„ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋“ค ์ค‘์—์„œ, ์ตœ์ ์˜ ์ œ์ž‘ ์ˆœ์„œ๋ฅผ ํ™•๋ฆฝํ•˜๊ธฐ ์œ„ํ•ด์„œ ๋ฌผ์งˆ์— ๊ด€ํ•œ ์„ฑ์ˆ™๋„๊ฐ€ ๋†’์€ ๊ฐ€์‹œ๊ด‘์„  GaAs ๊ทธ๋ฆฌ๊ณ  ๊ทผ์ ์™ธ์„  InGaAs ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ์‚ฌ์šฉํ•˜์˜€๋‹ค. ๊ฐ€์‹œ๊ด‘/๊ทผ์ ์™ธ์„  ๋Œ€์—ญ์˜ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ํ˜•์„ฑํ•˜๊ธฐ ์œ„ํ•ด์„œ, GaAs ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ InGaAs ๊ด‘ ๊ฒ€์ถœ๊ธฐ ์ƒ์œผ๋กœ ๊ฐœ๋ฐœ๋œ ๊ณ ์† ์—ํ”ผํƒ์…œ ๋ฆฌํ”„ํŠธ ์˜คํ”„ ๊ธฐ๋ฒ•์„ ์‚ฌ์šฉํ•˜์—ฌ ์ „์‚ฌํ•˜์˜€๋‹ค. GaAs ๊ด‘ ๊ฒ€์ถœ๊ธฐ์™€ InGaAs ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋Š” off-axis ์—†์ด ์ˆ˜์ง์œผ๋กœ ์ž˜ ์ •๋ ฌ๋˜์—ˆ์Œ์„ x-ray ๋ถ„๊ด‘๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ํ™•์ธํ•˜์˜€๋‹ค. ๋˜ํ•œ, ๊ฐ๊ฐ์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ์˜ ๊ธฐ์ค€ ์†Œ์ž๋“ค๊ณผ ๋น„๊ตํ–ˆ์„ ๋•Œ ๋น„์Šทํ•œ ์•” ์ „๋ฅ˜๊ฐ€ ๋‚˜ํƒ€๋‚ฌ๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ๋ ˆ์ด์ € ์ž…์‚ฌ๋ฅผ ํ†ตํ•ด, ๋‘ ๊ฐœ์˜ ๊ด‘ ๊ฒ€์ถœ๊ธฐ ๋Œ€ํ•œ ๊ด‘ ๋ฐ˜์‘์€ ๋ฌผ์งˆ ํŠน์„ฑ๋“ค์— ๋”ฐ๋ผ ๊ฐ€์‹œ๊ด‘๊ณผ ๊ทผ์ ์™ธ์„ ์—์„œ ๊ฐ๊ฐ ๋ช…ํ™•ํ•˜๊ฒŒ ๋‚˜ํƒ€๋‚ฌ๋‹ค. ์ด๋Ÿฌํ•œ ๊ฒฐ๊ณผ๋“ค์€ ๊ณ ์† ์—ํ”ผํƒ์…œ ๋ฆฌํ”„ํŠธ ์˜คํ”„ ๊ธฐ๋ฒ•์ด ๋†’์€ ํ”ฝ์…€ ๋ฐ€๋„ ๋ฐ ๊ฑฐ์˜ ์™„๋ฒฝํ•œ ์ˆ˜์ง ์ •๋ ฌ๋„๋ฅผ ๊ฐ–๋Š” ํ•œ ๊ธฐํŒ์ƒ์˜ ๋ฒŒํฌ ๊ธฐ๋ฐ˜์˜ ๋‹ค์ค‘ํŒŒ์žฅ ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ์ง‘์ ํ•  ์ˆ˜ ์žˆ๋‹ค๋Š” ๊ฒƒ์„ ์˜๋ฏธํ•œ๋‹ค. ๋ฏธ๋ž˜์˜ ๋ชฉํ‘œํ•˜๋Š” ์‘์šฉ์ฒ˜์— ๋”ฐ๋ผ, ์›ํ•˜๋Š” ํŒŒ์žฅ๋“ค์„ ๊ฐ–๋Š” ๊ด‘ ๊ฒ€์ถœ๊ธฐ๋ฅผ ๋ฒŒํฌ ๊ตฌ์กฐ๋กœ ๊ฐ„๋‹จํ•˜๊ฒŒ ์„ฑ์žฅํ•  ์ˆ˜ ์žˆ๊ณ , ๋‹ค์ค‘ํŒŒ์žฅ ์ด๋ฏธ์ง• ์‹œ์Šคํ…œ์„ ์ œ์ž‘ ํ•  ์ˆ˜ ์žˆ๋‹ค.List of Figures i Chapter.1 Introduction 1 1.1 Photodetectors based on III-V compound semiconductors 1 1.2 Imaging applications 4 1.2.1. Single color imaing 4 1.2.2. Multicolor imaing 4 1.2.3. Development trend of photodetectors 5 1.3 Approches for forming multicolor photodectors 9 1.3.1. Epitaxy 9 1.3.2. Heterogeneous integration 17 1.3.3. Summary of each method 21 1.4 Overview of heterogeneous integration technology 23 1.4.1. Introduction 23 1.4.2. Direct bonding 24 1.4.3. Cold-weld bonding 26 1.4.4. Eutectic bonding 26 1.4.5. Adhesive bonding 28 1.4.7. Wafer splitting 31 1.4.8. Epitaxial lift off (ELO) 33 1.4.9. Benchmark of differenct heterogeneous intergration methods 35 1.5 Thesis overview 37 1.6 Bibliography 40 Chapter. 2 Method for heterogeneous integration of III-V compound semiconductors on other substrates 45 2.1 Introduction 45 2.1.1 The origin of low throughput in conventional ELO 46 2.1.2 Previous works for ehancement of ELO throughput 48 2.1.3 Approach: high-throughput ELO process 53 2.1.4 Experimental procedure 55 2.2 Results and discussion 57 2.3 Summary 65 2.4 Biblography 66 Chapter. 3 Verification of thin film devices by using a high throughput heterogeneous integration method 70 3.1 Introduction 70 3.2 Growth of device structures and heterogeneous integration 72 3.2.1. Device structures 72 3.2.2. Wafer bonding and ELO 74 3.3 Y2O3 bonded HEMTs on Si substrate 75 3.3.1 Fabrication process 75 3.3.2. Material characterization of HEMTs on Si 76 3.3.3. Electrical characterization of HEMTs on Si 80 3.3.4. Investigation of wafer reusability by using HEMT structure 83 3.4 Pt/Au bonded optoelectonic devices 86 3.4.1. Fabrication process of solar cells and HPTs on Si 86 3.4.2. Evaluation of Pt/Au metal bonding 88 3.4.3. Characterization of solar cells and HPTs 91 3.5 Estimation of production cost via recycling III-V wafers 95 3.6 Summary 101 3.7 Bibliography 102 Chapter. 4 Design and characterization of III-V based photodtectors 106 4.1 Introduction 106 4.1.1. The potential of Induim arsenide antimonide (InAsSb) 106 4.1.2. Challenges of InAsSb p-i-n PDs for compact detector systems 110 4.2 Barrier layer design and material characterization for growing HJPDs 113 4.2.1. Simulation of an optimum barrier layer for InAs0.8Sb0.2 113 4.2.2. Growth of a high quality InAsSb layer with an AlGaSb buffer layer grown on GaAs substrates 115 4.2.3. Ohmic contact formation with metal species 120 4.2.4. Growth and fabrication of InAsSb based HJPDs 126 4.3 Analysis of electrical and optical characteristics for fabricated PDs 129 4.4 Summary 138 4.5 Bibliography 139 Chapter. 5 Monolithic integration of visible/near-infrared photodetectors 145 5.1 Introduction 145 5.2 Fabrication process and material characterization of multicolor PD 148 5.3 Analysis of the electrical and optical characteristics of the fabricated multicolor PDs 154 5.4 Summary 163 5.5 Bibliography 164 Chapter. 6 Conclusions 169 ๊ตญ ๋ฌธ ์ดˆ ๋ก 172Docto

    MOCVD Growth and Electrical Characterization of AlInGaN Heterojunctions

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    III-N-based electronics and optoelectronics are reaching great levels of sophistication in the areas of power electronics, RF amplifiers, lighting, and display technologies. Much of the success of these technologies can be traced to superior or unique material properties that make III-N solid state devices the ideal choices for their applications. Consequently, state of the art devices are being pushed to the limit of what may be fabricated due to strain considerations in the AlGaN and InGaN systems. In order to continue the advancement of III-N based technologies toward greater performance, into new niches, and open up new markets, it is necessary to exploit the entire (Al,In,Ga)N system to its fullest potential.The utility of AlInGaN is multifaceted. These materials can be used for strain management, fabrication of lattice-matched devices, and polarization engineering to manipulate electric fields within device active regions, or even create high-conductivity charge slabs. Unlike ternary alloys, there is no single unique combination of band gap, polarization charge, and lattice constant, which results in greater device design freedom. However, to effectively utilize these materials, reliable growth processes must be established, and the material parameters critical to device design must be characterized.This thesis describes the progress in AlInGaN development at UCSB beginning with identification and exploration of the AlInGaN growth parameter space, using understanding from ternary alloys as a springboard into quaternary growth. From there, the thesis progresses to the establishment of a design toolbox for AlInGaN based devices via electrical characterization of these materials. Challenges associated with the AlInGaN system, coupled with sparse literature on the topic, necessitated the design of experiments to isolate and characterize the material parameters from measurements of solid-state devices. Electrical characterization focused on the net polarization charge at heterojunction interfaces, as well as the effects of Schottky barrier height inhomogeneity on both electrostatics and transport in diodes. The quantum mechanical scattering at the metal-semiconductor junction will be discussed, as will its physical origin and impact on diode current. A major goal of this thesis was to establish a device design toolbox populated with information of experimentally calculated net polarization charge at AlInGaN/GaN interfaces and Schottky barrier heights. This goal was accomplished and the information was established for future device designers in the field.The thesis concludes with a discussion of the application and exploitation of the unique effects observed in AlInGaN materials to device design. Future outlook will be given on avenues for research in AlInGaN materials and AlInGaN-based devices, and direction will be provided to finish populating the (electrical) device design toolbox with conduction band offset measurements

    AlGaN/GaN ์ „๋ ฅ์†Œ์ž์˜ ํŠน์„ฑ ํ–ฅ์ƒ์„ ์œ„ํ•œ ์‹๊ฐ๊ณผ ์ ˆ์—ฐ๋ง‰์— ๊ด€ํ•œ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2020. 8. ์„œ๊ด‘์„.์ตœ๊ทผ ์—๋„ˆ์ง€ ์œ„๊ธฐ์™€ ํ™˜๊ฒฝ๊ทœ์ œ ๊ฐ•ํ™”, ์นœํ™˜๊ฒฝ ๋…น์ƒ‰์„ฑ์žฅ ๋“ฑ์˜ ์ด์Šˆ๊ฐ€ ๋Œ€๋‘๋˜์–ด ์—๋„ˆ์ง€ ์ ˆ๊ฐ๊ณผ ํ™˜๊ฒฝ ๋ณดํ˜ธ ๋ถ„์•ผ์— IT ๊ธฐ์ˆ ์„ ์ ‘๋ชฉ, ํ™œ์šฉํ•˜๋Š” ๊ทธ๋ฆฐ IT ํŒจ๋Ÿฌ๋‹ค์ž„์ด ๋ถ€๊ฐ๋˜๊ณ  ์žˆ๋‹ค. ํ˜„์žฌ ๊ณ ์œ ๊ฐ€ ํ™˜๊ฒฝ๊ทœ์ œ ๊ฐ•ํ™”์— ๋Œ€์‘ํ•˜๊ธฐ ์œ„ํ•ด ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์ž๋™์ฐจ, ์ „๊ธฐ์ž๋™์ฐจ ๋“ฑ ์นœํ™˜๊ฒฝ ๋ฏธ๋ž˜ํ˜• ์ž๋™์ฐจ ๊ฐœ๋ฐœ์ด ์š”๊ตฌ๋˜๊ณ  ์žˆ์œผ๋ฉฐ, ์ž๋™์ฐจ์—์„œ ์ „์žฅ๋ถ€ํ’ˆ์ด ์ฐจ์ง€ํ•˜๋Š” ์›๊ฐ€๋น„์ค‘์€ ์•ฝ 40%๊นŒ์ง€ ๋‹ฌํ•  ๊ฒƒ์œผ๋กœ ์ „๋ง๋˜๊ณ  ์ด ์ค‘ ๋ฐ˜๋„์ฒด๊ฐ€ ์ฐจ์ง€ํ•˜๋Š” ๋น„์šฉ์€ ์•ฝ 30% ์ •๋„๋กœ ์ถ”์ •๋œ๋‹ค. ์ด๋Ÿฌํ•œ ์ž๋™์ฐจ ์ „์žฅ๋ถ€ํ’ˆ์—์„œ ์ „๋ ฅ์†Œ์ž๊ฐ€ ํ•ต์‹ฌ๋ถ€ํ’ˆ์œผ๋กœ ์ž๋ฆฌ ์žก์„ ์ „๋ง์ด๋‹ค. ์ง€๊ธˆ๊นŒ์ง€๋Š” ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜์˜ ์ „๋ ฅ์†Œ์ž ๊ธฐ์ˆ ์ด ์ „๋ ฅ๋ฐ˜๋„์ฒด ์‹œ์žฅ์˜ ๋Œ€๋ถ€๋ถ„์„ ์ฃผ๋„ํ•˜๊ณ  ์žˆ์ง€๋งŒ ์ „๋ ฅ๊ธฐ๊ธฐ ๋กœ๋“œ๋งต์— ์˜ํ•˜๋ฉด ์ „๋ ฅ๋ฐ€๋„๊ฐ€ ํ•ด๋ฅผ ๊ฑฐ๋“ญํ•˜๋ฉด์„œ ์ง€์†์ ์œผ๋กœ ์ฆ๊ฐ€ํ•˜๊ธฐ ๋•Œ๋ฌธ์— ๋‚ด์—ด, ๋‚ด์••, ์ „๋ ฅ์†์‹ค, ์ „๋ ฅ๋ฐ€๋„ ๋“ฑ์—์„œ ๋‚˜ํƒ€๋‚˜๋Š” ๋งŽ์€ ํ•œ๊ณ„๋ฅผ ๊ฐ€์ง€๊ณ  ์žˆ๋Š” ํ˜„์žฌ์˜ ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜ ์ „๋ ฅ์‹œ์Šคํ…œ์€ ํšจ์œจ์ด ๋ˆˆ์— ๋„๊ฒŒ ๊ฐ์†Œํ•  ๊ฒƒ์ด ์ž๋ช…ํ•˜๋ฏ€๋กœ ์ „๋ ฅ์‹œ์Šคํ…œ์˜ ์ „๋ ฅ์ „์†กํšจ์œจ๊ณผ ์‹ ๋ขฐ์„ฑ์˜ ์ค‘์š”์„ฑ์ด ํฌ๊ฒŒ ๋Œ€๋‘๋˜๊ณ  ์žˆ๋‹ค. ์ด ๊ฐ™์€ ์‚ฌํšŒ์  ์š”๊ตฌ๋กœ ๋ณผ ๋•Œ ํ˜„์žฌ์˜ ์‹ค๋ฆฌ์ฝ˜ ์ „๋ ฅ์†Œ์ž์˜ ๊ธฐ์ˆ ์  ํ•œ๊ณ„๋ฅผ ๋›ฐ์–ด๋„˜๋Š” ๊ณ ํšจ์œจ์˜ ์ฐจ์„ธ๋Œ€ ์ „๋ ฅ๋ฐ˜๋„์ฒด ์†Œ์ž์˜ ๊ฐœ๋ฐœ์ด ์‹œ๊ธ‰ํžˆ ์š”๊ตฌ๋˜๋ฉฐ SiC์™€ GaN์™€ ๊ฐ™์€ ๊ด‘๋Œ€์—ญ ๋ฐ˜๋„์ฒด๊ฐ€ ์ฐจ์„ธ๋Œ€ ์ „๋ ฅ๋ฐ˜๋„์ฒด ์†Œ์žฌ๋กœ ์œ ๋ ฅํ•ด์ง€๊ณ  ์žˆ๋‹ค. ๋˜ํ•œ ์ „๋ ฅ์‹œ์Šคํ…œ์—์„œ๋Š” ์‹œ์Šคํ…œ์˜ ์•ˆ์ „์„ฑ๊ณผ ํšŒ๋กœ์˜ ๊ฐ„๋žตํ™”๋ฅผ ์œ„ํ•˜์—ฌ normally-off (์ฆ๊ฐ•ํ˜•) ์ „๋ ฅ์†Œ์ž๊ฐ€ ์š”๊ตฌ๋˜๊ธฐ ๋•Œ๋ฌธ์— normally-off (์ฆ๊ฐ•ํ˜•) GaN ์ „๋ ฅ์†Œ์ž์— ๋Œ€ํ•œ ๊ฐœ๋ฐœ์ด ํ•„์ˆ˜์ ์ด๋‹ค. ๋ณธ ๊ทธ๋ฃน์—์„œ๋Š” gate-recess ๊ณต์ •์„ ์ด์šฉํ•˜์—ฌ normally-off ๋™์ž‘์„ ์‹คํ˜„ํ•˜๋Š” ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๊ณ , gate-recess ์‹œ ๋ฐœ์ƒํ•˜๋Š” ์‹๊ฐ ๋ฐ๋ฏธ์ง€๋ฅผ ์ค„์ด๊ณ  ์šฐ์ˆ˜ํ•œ ์„ฑ๋Šฅ์˜ ๊ฒŒ์ดํŠธ ์ ˆ์—ฐ๋ง‰์„ ๊ฐœ๋ฐœํ•˜์—ฌ GaN ์ „๋ ฅ ๋ฐ˜๋„์ฒด ์†Œ์ž์˜ ์ „๊ธฐ์  ํŠน์„ฑ ๋ฐ ์‹ ๋ขฐ์„ฑ์„ ๊ฐœ์„ ํ•˜๋Š” ์—ฐ๊ตฌ๋ฅผ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ์‹๊ฐ ์—ฐ๊ตฌ์—์„œ๋Š” ์ตœ์ข…์ ์œผ๋กœ ์…€ํ”„ DC ๋ฐ”์ด์–ด์Šค๊ฐ€ ๋‚ฎ์€ O2, BCl3 ํ”Œ๋ผ์ฆˆ๋งˆ๋ฅผ ์ด์šฉํ•œ atomic layer etching์„ ๊ฐœ๋ฐœํ•˜์˜€๊ณ , ์ด๋ฅผ ํ†ตํ•ด ๊ฑฐ์น ๊ธฐ๊ฐ€ ์ž‘๊ณ  ํ‘œ๋ฉด N vacancy๊ฐ€ ์ ์€ ๊ณ ํ’ˆ์งˆ์˜ (Al)GaN ํ‘œ๋ฉด์„ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋ฐ•๋ง‰ ์—ฐ๊ตฌ์—์„œ๋Š” Oxide ๋ฐ•๋ง‰ ์ฆ์ฐฉ ์‹œ, (Al)GaN ํ‘œ๋ฉด์— ์ƒ์„ฑ๋˜์–ด ๊ณ„๋ฉด ํŠน์„ฑ์„ ์•…ํ™”์‹œํ‚ค๋Š” Ga2O3 ์ƒ์„ฑ์„ ๋ง‰๊ธฐ์œ„ํ•ด ALD AlN layer๋ฅผ ๊ฐœ๋ฐœ ๋ฐ ์ ์šฉํ•˜์—ฌ ๋ฐ•๋ง‰/(Al)GaN ๊ณ„๋ฉด ํŠน์„ฑ์„ ํ–ฅ์ƒ์‹œ์ผฐ๋‹ค. ์ด๋กœ ์ธํ•ด ์†Œ์ž์˜ ๋™์ž‘์ „๋ฅ˜ ์ฆ๊ฐ€ ๋ฐ Dit ๊ฐ์†Œ ๊ฒฐ๊ณผ๋ฅผ ์–ป์„ ์ˆ˜ ์žˆ์—ˆ๊ณ  ์ŠคํŠธ๋ ˆ์Šค์— ๋”ฐ๋ฅธ ๋ฌธํ„ฑ์ „์•• ์ด๋™ ํŠน์„ฑ์˜ ๊ฐ์†Œ๋กœ ์†Œ์ž์˜ ์‹ ๋ขฐ์„ฑ ๋˜ํ•œ ๊ฐœ์„ ์‹œํ‚ฌ ์ˆ˜ ์žˆ์—ˆ๋‹ค. ์ด๋Š” ํƒ€ ๊ธฐ๊ด€์˜ ๊ฒฐ๊ณผ์™€ ๋น„๊ตํ•ด๋„ ๋’ค๋–จ์–ด์ง€์ง€ ์•Š๋Š” ์šฐ์ˆ˜ํ•œ ํŠน์„ฑ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ๊ฒฐ๋ก ์ ์œผ๋กœ ๋ณธ ์—ฐ๊ตฌ์˜ ์ž‘์€ ํ”Œ๋ผ์ฆˆ๋งˆ ๋ฐ๋ฏธ์ง€๋ฅผ ๊ฐ–๋Š” ์‹๊ฐ๊ณต์ •๊ณผ ๊ณ ํ’ˆ์งˆ ์ ˆ์—ฐ๋ง‰ ๊ฐœ๋ฐœ์„ ํ†ตํ•ด ์šฐ์ˆ˜ํ•œ ํŠน์„ฑ์˜ GaN ์ „๋ ฅ์†Œ์ž๋ฅผ ๊ตฌํ˜„ํ•  ์ˆ˜ ์žˆ์—ˆ๊ณ  ํ–ฅํ›„ ์ฐจ์„ธ๋Œ€ ์ „๋ ฅ์†Œ์ž์— ์ ์šฉ์„ ์œ„ํ•œ ๊ฐ€๋Šฅ์„ฑ์„ ํ™•๋ณดํ•˜์˜€๋‹ค.The Si technology for power devices have already approached its theoretical limitations due to its physical and material properties, despite the considerable efforts such as super junction MOSFET, trench gate, and insulated gate bipolar transistors. To overcome these limitations, many kinds of compound materials such as GaN, GaAs, SiC, Diamond and InP which have larger breakdown voltage and high electron velocity than Si also have been studied as future power devices. GaN has been considered as a breakthrough in power applications due to its high critical electric field, high saturation velocity and high electron mobility compared to Si, GaAs, and SiC. Especially, AlGaN/GaN heterostructure field-effect transistors (HFETs) have been considered as promising candidates for high power and high voltage applications. However, these AlGaN/GaN heterostructure field-effect transistors with the 2DEG are naturally normally-on, which makes the devices difficult to deplete the channel at zero gate bias. Among the various methods for normally-off operation of GaN devices, gate-recess method is a promising method because it can be easier to implement than other approaches and ensure normally-off operation. However, charge trapping at the interface between gate dielectric and (Al)GaN and in the gate dielectric is a big issue for recessed gate MIS-HEMTs. This problem leads to degradation of channel mobility, on-resistance and on-current of the devices. Especially, Vth hysteresis after a positive gate voltage sweep and Vth shift under a gate bias stress are important reliability challenges in gate recessed MIS-HEMTs. The scope of this work is mainly oriented to achieve high quality interface at dielectric/(Al)GaN MIS by studying low damage etching methods and the ALD process of various dielectric layers. In the etching study, various etching methods for normally-off operation have been studied. Also, etching damage was evaluated by various methods such as atomic force microscopy (AFM), photoluminescence (PL) measurements, X-ray photoelectron spectroscopy (XPS) measurements and electrical properties of the recessed schottky devices. Among the etching methods, the ALE shows the smoothest etched surface, the highest PL intensity and N/(Al+Ga) ratio of the etched AlGaN surface and the lowest leakage current of the gate recessed schottky devices. It is suggested that the ALE is a promising etching technique for normally-off gate recessed AlGaN/GaN MIS-FETs. In the study of dielectrics, excellent electrical characteristics and small threshold voltยฌage drift under positive gate bias stress are achieved by employing the SiON interfacial layer. However, considerable threshold voltage drift is observed under the higher positive gate bias stress even at the devices using the SiON interfacial layer. For further improvement of interface and reliability of devices, we develop and optimize an ALD AlN as an interfacial layer to avoid the formation of poor-quality oxide at the dielectric/(Al)GaN interface. We also develop an ALD AlHfON as a bulk layer, which have a high dielectric constant and low leakage current and high breakdown field characteristics. Devices with AlN/AlON/AlHfON layer show smaller I-V hysteresis of ~10 mV than that of devices with AlON/AlHfON layer. The extracted static Ron values of devices with AlN/AlON/AlHfON and AlON/AlHfON are 1.35 and 1.69 mโ„ฆยทcm2, respectively. Besides, the effective mobility, Dit and threshold voltage instability characteristics are all improved by employing the ALD AlN. In conclusion, for high performance and improvement of reliability of normally-off AlGaN/GaN MIS-FETs, this thesis presents an etching technique for low damage etching and high-quality gate dielectric layer and suggests that the ALE and ALD AlN/AlON/AlHfON gate dielectric are very promising for the future normally-off AlGaN/GaN MIS-FETsChapter 1. Introduction 1 1.1. Backgrounds 1 1.2. Normally-off Operation in AlGaN/GaN HFETs 3 1.3. Issues and Feasible Strategies in AlGaN/GaN MIS-HFETs 11 1.4. Research Aims 15 1.5. References 17 Chapter 2. Development and Evaluation of Low Damage Etching processes 22 2.1. Introduction 22 2.2. Various Evaluation Methods of Etching Damage 24 2.3. Low-Damage Dry Etching Methods 29 2.3.1. Inductively Coupled Plasma-Reactive Ion Etching Using BCl3/Cl2 Gas Mixture 29 2.3.2. Digital Etching Using Plasma Asher and HCl 34 2.3.3. Atomic Layer Etching Using Inductively Coupled Plasmaโ€“Reactive Ion Etching System (ICP-RIE) 50 2.4. Conclusion 75 2.5. References 76 Chapter 3. SiON/HfON Gate Dielectric Layer by ALD for AlGaN/GaN MIS-FETs 80 3.1. Introduction 80 3.2. ALD Processes for SiON and HfON 83 3.3. Electrical Characteristics of ALD SiON, HfON and SiON/HfON Dual Layer on n-GaN 87 3.4. Device Characteristics of Normally-off AlGaN/GaN MIS-FETs with SiON/HfON Dual Layer 95 3.5. Conclusion 113 3.6. References 114 Chapter 4. High Quality AlN/AlON/AlHfON Gate Dielectric Layer by ALD for AlGaN/GaN MIS-FETs 120 4.1. Introduction 120 4.2. Development of ALD AlN/AlON/AlHfON Gate Stack 122 4.2.1. Process Optimization for ALD AlN 122 4.2.2. ALD AlN as an Interfacial Layer 144 4.2.3. Thickness Optimization of AlN/AlON/ AlHfON Layer 149 4.2.4. ALD AlHfON Optimization 159 4.2.5. Material Characteristics of AlN/AlON/AlHfON Layer 167 4.3. Device Characteristics of Normally-off AlGaN/GaN MIS-FETs with AlN/AlON/AlHfON Layer 171 4.4. Conclusion 182 4.5. References 183 Chapter 5. Concluding Remarks 188 Appendix. 190 A. N2 Plasma Treatment Before Dielectric Deposition 190 B. Tri-gate Normally-on/off AlGaN/GaN MIS-FETs 200 C. AlGaN/GaN Diode with MIS-gated Hybrid Anode and Edge termination 214 Abstract in Korean 219 Research Achievements 221Docto

    Organic functionalisation, doping and characterisation of semiconductor surfaces for future CMOS device applications

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    Organic Functionalisation, Doping and Characterisation of Semiconductor Surfaces for Future CMOS Device Applications Semiconductor materials have long been the driving force for the advancement of technology since their inception in the mid-20th century. Traditionally, micro-electronic devices based upon these materials have scaled down in size and doubled in transistor density in accordance with the well-known Mooreโ€™s law, enabling consumer products with outstanding computational power at lower costs and with smaller footprints. According to the International Technology Roadmap for Semiconductors (ITRS), the scaling of metal-oxide-semiconductor field-effect transistors (MOSFETs) is proceeding at a rapid pace and will reach sub-10 nm dimensions in the coming years. This scaling presents many challenges, not only in terms of metrology but also in terms of the material preparation especially with respect to doping, leading to the moniker โ€œMore-than-Mooreโ€. Current transistor technologies are based on the use of semiconductor junctions formed by the introduction of dopant atoms into the material using various methodologies and at device sizes below 10 nm, high concentration gradients become a necessity. Doping, the controlled and purposeful addition of impurities to a semiconductor, is one of the most important steps in the material preparation with uniform and confined doping to form ultra-shallow junctions at source and drain extension regions being one of the key enablers for the continued scaling of devices. Monolayer doping has shown promise to satisfy the need to conformally dope at such small feature sizes. Monolayer doping (MLD) has been shown to satisfy the requirements for extended defect-free, conformal and controllable doping on many materials ranging from the traditional silicon and germanium devices to emerging replacement materials such as III-V compounds This thesis aims to investigate the potential of monolayer doping to complement or replace conventional doping technologies currently in use in CMOS fabrication facilities across the world

    Study of High-k Dielectrics and their Interfaces on Semiconductors for Device Applications

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    This thesis has focused on two emerging applications of high-k dielectrics in Metal-Oxide-Semiconductor Field Effect Transistors (MOSFETs) and in Metal-InsulatorSemiconductor High Electron Mobility Transistors (MIS-HEMTs). The key aim has been to propose the best routes for passivation of semiconductor/high-k oxide interfaces by investigating the band alignments and interface properties of several oxides, such as Tm2O3, Ta2O5, ZrO2, Al2O3 and MgO, deposited on different semiconductors: Si, Ge, GaN, InGaAs and InGaSb. The electrical characterisation of fabricated MIS capacitor and (MIS)-HEMT devices have also been performed. Thulium silicate (TmSiO) has been identified as a promising candidate for integration as interfacial layer (IL) in HfO2/TiN MOSFETs. The physical properties of Tm2O3/IL/Si interface have been elucidated, where IL (TmSiO) has been formed using different post-deposition annealing (PDA) temperatures, from 550 to 750 ยฐC. It has been found that the best-scaled stack (sub-nm IL) is formed at 550 ยฐC PDA with a graded interface layer and a strong SiOx (Si 3+) component. A large valence band offset (VBO) of 2.8 eV and a large conduction band offset (CBO) of 1.9 eV have been derived for Tm2O3/Si by X-ray photoelectron spectroscopy (XPS) and variable angle spectroscopic ellipsometry. Further increase of device performance can be achieved by replacing Si with GaN for high frequency, high power and high-temperature operation. In this thesis, several GaN cleaning procedures have been considered: 30% NH4OH, 20% (NH4)2S, and 37% HCl. It has been found that the HCl treatment shows the lowest oxygen contamination and Garich surface, and hence has been used prior sputtering of Ta2O5, Al2O3, ZrO2 and MgO on GaN. The large VBOs of 1.1 eV and 1.2 eV have been derived for Al2O3 and MgO on GaN respectively, using XPS and Krautโ€™s method; the corresponding CBOs are 2.0 eV and 2.8 eV respectively, taking into account the band gaps of Al2O3 (6.5 eV) and MgO (7.4 eV) determined from XPS O 1s electron energy spectra. The lowest leakage currents were obtained for devices with Al2O3 and MgO, i.e. 5.3 ร—10-6 A/cm2 and 3.2 ร—10-6 A/cm2 at 1 V, respectively in agreement with high band offsets (> 1 eV). Furthermore, the effect of different surface treatments (HCl, O2 plasma and 1-Octadecanethiol (ODT)) prior to atomic layer deposition of Al2O3 on the GaN/AlGaN/GaN heterostructure has been investigated. The MIS-HEMTs fabricated using the low-cost ODT GaN surface treatment have been found to exhibit superior performance for power switching applications such as a low threshold voltage, VT of -12.3 V, hysteresis of 0.12 V, a small subthreshold voltage slope (SS) of 73 mV/dec, and a low density of interface states, Dit of 3.0 x10^12 cm-2eV-1. A comprehensive novel study of HfO2/InGaAs and Al2O3/InGaSb interfaces have also been conducted for use in III-V based MOSFETs. The addition of the plasma H2/TMA/H2 pre-cleaning has been found to be very effective in recovering etch damage on InGaAs, especially for (110) orientation, and led to the improvement of electrical characteristics. Furthermore, the combination of H2 plasma exposure and forming gas anneal yielded significantly improved metrics for Al2O3/InGaSb over the control HCltreated sample, with the 150 W plasma treatment giving both the highest capacitance and the lowest stretch out

    Advanced gallium nitride technology for microwave power amplifiers

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    Gallium nitride (GaN) based technology has been heavily researched over the past two decades due to its ability to deliver higher powers and higher frequencies that are demanded by the market for various applications. One of GaNโ€™s main advantages lies in its ability to form heterojunctions to wider bandgap materials such as Aluminium Gallium Nitride (AlGaN) and Aluminium Nitride (AlN). The heterostructure results in the formation of the so called 2 dimensional electron gas (2DEG), which exhibits high electron densities of up to 6E13 cmโˆ’2 and high electron mobilities of up to 2000 cm2/Vยทs that enable the devices to support high current densities. Furthermore, it supports very high breakdown fields of 3.3 MV/cm due to its wide bandgap of 3.4 eV. The main objective of this work was to further advance the transistor technology using simple, cost effective and reliable techniques. The AlN/GaN material system exhibits higher sheet carrier concentrations compared to the conventional ternary AlGaN barrier, but introduces additional challenges due to its reduced thickness of 2-6 nm compared to 18-30 nm of AlGaN. The additional challenges of the thin AlN binary barrier include strain relaxation, high gate leakage currents and high Ohmic contact resistances due to its high bandgap of 6.2 eV. In this work, a thin (5 nm) in-situ SiNx passivation layer was employed to reduce the strain relaxation, reduce gate leakage currents and improve Ohmic contacts resistances. The optimised Ohmic contact annealing condition resulted in an Ohmic contact resistance of 0.4 ฮฉยทmm and a sheet resistance of 300 ฮฉ

    Optimisation of high-efficiency UV and visible light sources utilising lateral localisation in InAlN and InGaN based nano-structure devices

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    III-nitride semiconductor materials (including GaN, InN and AlN and their alloys), have the capability to emit light at wavelengths spanning from the near IR to the deep UV. However, understanding these materials is challenging due to the presence of strong polarisation fields and large difference in optimum growth temperature between binary compounds are two such examples. InAlN is perhaps the least well understood III-N alloy. It has potential be applied for optoelectronic devices operating in the UV spectral range. However, the variation of band-gap with alloy composition, particularly in the low In content regime, is not understood. In this work, a strongly composition dependent bowing parameter has been observed for ~100 nm thick InxAl1โˆ’xN epitaxial layers with 0 โ‰ค x โ‰ค 0.224, grown by metalorganic vapour phase epitaxy (MOVPE), prepared on AlN/Al2O3-templates. Also a double absorption edge was observed for InAlN with x < 0.01, attributed to crystal-field splitting of the highest valence band states. These results indicate that the ordering of the valence bands is changed at much lower In contents than linear interpolation of the valence band parameters would predict. Coupling our results with the published literature data the band-gap and bowing parameter of InAlN across the full composition range were determined. Additionally, applying the InAlN band-gap data with those for other alloys the refractive index of III-N alloys is predicted using an Adachi model resulting in a very good agreement with previous experimental data where available. For InAlN/AlGaN multi-quantum-wells (MQWs) excited by photoluminescence (PL) and emitting between 300-350 nm, high apparent internal quantum efficiencies (IQE) (IPL(300 K)/IPL(T)max) of up to 70% were obtained. This is attributed to the exceptionally strong carrier localisation in this material, which is also manifested by a high Stokes shift (0.52 eV) of the luminescence. A non-monotonic dependence of luminescence efficiency on indium content with a maximum at about 18% In was explained as a trade-off between a strain relaxation for higher indium contents and a type I to type II band line-up conversion for low In content alloys. Nanoscale materials have attracted a lot of attention due to their ability to decrease dislocations as well as build-in field reduction. In the second part of this thesis, GaN nanostructures, were used as templates for InGaN MQW growth targeting nano-LED structures. Two nano-structuring methods were examined; using GaN nano-columns (NCs) following an etch regrowth methodology, and selective area aperture growth (SAG). In the former case we determined the optimal etch conditions for the GaN columns and conditions for overgrowth InGaN QWS. The rod tops formed semipolar facets. InGaN QWs grown on these pyramids were found to be extremely thin leading to difficulties in obtaining PL in our case. Using the SAG approach, nano-pyramids were formed in nano-apertures, with good uniformity. InGaN QWs exhibited blue PL, which cathodoluminescence (CL) showed to be made up of two spectral features, attributed to the pyramid nano-facets and pyramid apex tips, respectively

    Feature Papers in Electronic Materials Section

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    This book entitled "Feature Papers in Electronic Materials Section" is a collection of selected papers recently published on the journal Materials, focusing on the latest advances in electronic materials and devices in different fields (e.g., power- and high-frequency electronics, optoelectronic devices, detectors, etc.). In the first part of the book, many articles are dedicated to wide band gap semiconductors (e.g., SiC, GaN, Ga2O3, diamond), focusing on the current relevant materials and devices technology issues. The second part of the book is a miscellaneous of other electronics materials for various applications, including two-dimensional materials for optoelectronic and high-frequency devices. Finally, some recent advances in materials and flexible sensors for bioelectronics and medical applications are presented at the end of the book
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