862 research outputs found

    III-V Microdisk lasers on silicon-on-insulator : fabrication optimizations and novel applications

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    Thin film technology for optoelectronics and their thermal management

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    Thin-film semiconductor optoelectronics are important for applications from optical communication, solid-state lighting, and wearable electronics to biomedical sensors. It is now possible to separate the micrometer-thick device layers from their native substrates and transfer them onto new platforms to optimize system performance and integration. The understanding of thermal management for such devices is very important in order to control the junction temperature effectively. Here, the laser-lift-off (LLO) technique was theoretically and experimentally studied. The temperature distribution at the III-nitride/sapphire interface induced by absorption of 248-nm KrF excimer energetic laser pulses was simulated to verify the experimental results. A 1.5-m-thick n-type Al0.6Ga0.4N membrane was separated from a c-plane sapphire substrate and then bonded to a Si substrate. The electrical behaviour of Ti/Al/Ti/Au contacts on the N-polar n-Al0.6Ga0.4N membrane was characterized. Furthermore, free-standing semipolar InGaN/GaN light-emitting diodes (LEDs) emitting at 445 nm were first realized by separation from patterned r-plane sapphire substrate using LLO. The LEDs showed a turn-on voltage of 3.6 V and output power of 0.87 mW at 20 mA. Electroluminescence measurements showed stronger emission intensity along the inclined c-direction. The -3 dB bandwidth of the LEDs is in excess of 150 MHz at 20 mA and a back-to-back data transmission rate at 300 Mbps is demonstrated. This indicates that the LEDs can be used for high bandwidth visible light communications. For thermal management of thin-film optoelectronics, a GaAs based laser diode (LD) was investigated. The 2-dimensional temperature distribution of the transfer-bonded LD was simulated; where the power dissipation, the thermal resistance of different cavity lengths and configurations were investigated. This can be utilized to optimize the device design and the choice of carrier substrate for efficient thermal management of thin-film optoelectronics

    Tailoring quantum structures for active photonic crystals

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    GaAs nano-ridge laser diodes fully fabricated in a 300 mm CMOS pilot line

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    Silicon photonics is a rapidly developing technology that promises to revolutionize the way we communicate, compute, and sense the world. However, the lack of highly scalable, native CMOS-integrated light sources is one of the main factors hampering its widespread adoption. Despite significant progress in hybrid and heterogeneous integration of III-V light sources on silicon, monolithic integration by direct epitaxial growth of III-V materials remains the pinnacle in realizing cost-effective on-chip light sources. Here, we report the first electrically driven GaAs-based multi-quantum-well laser diodes fully fabricated on 300 mm Si wafers in a CMOS pilot manufacturing line. GaAs nano-ridge waveguides with embedded p-i-n diodes, InGaAs quantum wells and InGaP passivation layers are grown with high quality at wafer scale, leveraging selective-area epitaxy with aspect-ratio trapping. After III-V facet patterning and standard CMOS contact metallization, room-temperature continuous-wave lasing is demonstrated at wavelengths around 1020 nm in more than three hundred devices across a wafer, with threshold currents as low as 5 mA, output powers beyond 1 mW, laser linewidths down to 46 MHz, and laser operation up to 55 {\deg}C. These results illustrate the potential of the III-V/Si nano-ridge engineering concept for the monolithic integration of laser diodes in a Si photonics platform, enabling future cost-sensitive high-volume applications in optical sensing, interconnects and beyond.Comment: 40 pages with 16 figures. pdf includes supplementary informatio

    High speed directly modulated III-V-on-silicon DFB lasers

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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

    GaSb/Silicon-on-insulator heterogeneous photonic integrated circuits for the short-wave infrared

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    Coaxial recess integration of InGaAs/InP edge emitting laser diodes with waveguides on silicon substrates : a complete solution to laser integration on ICs

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    Thesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Electrical Engineering and Computer Science, 2012.This electronic version was submitted by the student author. The certified thesis is available in the Institute Archives and Special Collections.Cataloged from student-submitted PDF version of thesis.Includes bibliographical references (p. 279-289).In this thesis, the first demonstration of the full integration of 1.55[mu]m InGaAs/InP edge emitting platelet laser diodes with SiON/SiO2 dielectric waveguides on a silicon substrate is presented. Small footprint laser platelets (300[mu]m long by 150[mu mwide and 6.3[mu]m high), are integrated and bonded in recesses etched in SiO2 deposited on a Si substrate, and are coaxially coupled to the dielectric waveguides fabricated on the same wafer. Lasers assembled in 6.5[mu]m deep recesses are securely solder-bonded in place with a thin film Al/In bonding layer, which also brings the laser platelet back side n-contact to the wafer front side for measurements. The Al/In bonding layer composition and thickness are carefully optimized to provide highly reproducible vertical alignment to maximize the coupling of the laser output beam to the dielectric waveguide. Lasers are bonded into the recesses with this solder-bonding layer during a pressure assisted temperature cycle at 220ยฐC. The low temperature nature of the bonding phase makes this integration technique CMOS compatible. The integrated lasers show lasing operation with threshold currents of Ith=17mA and Ith=19mA for pulsed and continuous wave drives respectively, at T=15ยฐC. The output spectrum shows single mode lasing near 1550[mu]m, and a side mode suppression ratio of 25dB which is significantly higher than typical Fabry Perot cavity laser diodes. Furthermore, the integrated lasers have a characteristic temperature, T0, of 76K which is improved from 60K for non-integrated lasers. Also the integrated lasers consistently show lower threshold currents compared to their non-integrated counterparts. The coupling loss between the laser and dielectric waveguide is extracted to be as low as 1dB, a value that can be further reduced by improved horizontal alignment and better matching the widths of laser stripe and dielectric waveguide. Overall, this recess integration approach is CMOS compatible, is highly modular, compact and flexible, permits testing and selection of devices prior to integration, and allows integration of lasers emitting at different wavelengths on the same chip. It eliminates the need for wafer bonding III/V substrates to the host Si IC along with added complexity and cost it involves, and can be implemented using easily accessible technologies.by Shaya Famenini.Ph.D
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