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    ๋†’์€ ์ „๋ฅ˜ ๊ตฌ๋™๋Šฅ๋ ฅ์„ ๊ฐ€์ง€๋Š” SiGe ๋‚˜๋…ธ์‹œํŠธ ๊ตฌ์กฐ์˜ ํ„ฐ๋„๋ง ์ „๊ณ„ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2021. 2. ๋ฐ•๋ณ‘๊ตญ.The development of very-large-scale integration (VLSI) technology has continuously demanded smaller devices to achieve high integration density for faster computing speed or higher capacity. However, in the recent complementary-metal-oxide-semiconductor (CMOS) technology, simple downsizing the dimension of metal-oxide-semiconductor field-effect transistor (MOSFET) no longer guarantees the boosting performance of IC chips. In particular, static power consumption is not reduced while device size is decreasing because voltage scaling is slowed down at some point. The increased off-current due to short-channel effect (SCE) of MOSFET is a representative cause of the difficulty in voltage scaling. To overcome these fundamental limits of MOSFET, many researchers have been looking for the next generation of FET device over the last ten years. Tunnel field-effect transistor (TFET) has been intensively studied for its steep switching characteristics. Nevertheless, the poor current drivability of TFET is the most serious obstacle to become competitive device for MOSFET. In this thesis, TFET with high current drivability in which above-mentioned problem is significantly solved is proposed. Vertically-stacked SiGe nanosheet channels are used to boost carrier injection and gate control. The fabrication technique to form highly-condensed SiGe nanosheets is introduced. TFET is fabricated with MOSFET with the same structure in the CMOS-compatible process. Both technology-computer-aided-design (TCAD) simulation and experimental results are utilized to support and examine the advantages of proposed TFET. From the perspective of the single device, the improvement in switching characteristics and current drivability are quantitatively and qualitatively analyzed. In addition, the device performance is compared to the benchmark of previously reported TFET and co-fabricated MOSFET. Through those processes, the feasibility of SiGe nanosheet TFET is verified. It is revealed that the proposed SiGe nanosheet TFET has notable steeper switching and low leakage in the low drive voltage as an alternative to conventional MOSFET.์ดˆ๊ณ ๋ฐ€๋„ ์ง‘์ ํšŒ๋กœ ๊ธฐ์ˆ ์˜ ๋ฐœ์ „์€ ๊ณ ์ง‘์ ๋„ ๋‹ฌ์„ฑ์„ ํ†ตํ•ด ๋‹จ์œ„ ์นฉ์˜ ์—ฐ์‚ฐ ์†๋„ ๋ฐ ์šฉ๋Ÿ‰ ํ–ฅ์ƒ์— ๊ธฐ์—ฌํ•  ์†Œํ˜•์˜ ์†Œ์ž๋ฅผ ๋Š์ž„์—†์ด ์š”๊ตฌํ•˜๊ณ  ์žˆ๋‹ค. ํ•˜์ง€๋งŒ ์ตœ์‹ ์˜ ์ƒ๋ณดํ˜• ๊ธˆ์†-์‚ฐํ™”๋ง‰-๋ฐ˜๋„์ฒด (CMOS) ๊ธฐ์ˆ ์—์„œ ๊ธˆ์†-์‚ฐํ™”๋ง‰-๋ฐ˜๋„์ฒด ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ (MOSFET) ์˜ ๋‹จ์ˆœํ•œ ์†Œํ˜•ํ™”๋Š” ๋” ์ด์ƒ ์ง‘์ ํšŒ๋กœ์˜ ์„ฑ๋Šฅ ํ–ฅ์ƒ์„ ๋ณด์žฅํ•ด ์ฃผ์ง€ ๋ชปํ•˜๊ณ  ์žˆ๋‹ค. ํŠนํžˆ ์†Œ์ž์˜ ํฌ๊ธฐ๊ฐ€ ์ค„์–ด๋“œ๋Š” ๋ฐ˜๋ฉด ์ •์  ์ „๋ ฅ ์†Œ๋ชจ๋Ÿ‰์€ ์ „์•• ์Šค์ผ€์ผ๋ง์˜ ๋‘”ํ™”๋กœ ์ธํ•ด ๊ฐ์†Œ๋˜์ง€ ์•Š๊ณ  ์žˆ๋Š” ์ƒํ™ฉ์ด๋‹ค. MOSFET์˜ ์งง์€ ์ฑ„๋„ ํšจ๊ณผ๋กœ ์ธํ•ด ์ฆ๊ฐ€๋œ ๋ˆ„์„ค ์ „๋ฅ˜๊ฐ€ ์ „์•• ์Šค์ผ€์ผ๋ง์˜ ์–ด๋ ค์›€์„ ์ฃผ๋Š” ๋Œ€ํ‘œ์  ์›์ธ์œผ๋กœ ๊ผฝํžŒ๋‹ค. ์ด๋Ÿฌํ•œ ๊ทผ๋ณธ์ ์ธ MOSFET์˜ ํ•œ๊ณ„๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•˜์—ฌ ์ง€๋‚œ 10์—ฌ๋…„๊ฐ„ ์ƒˆ๋กœ์šด ๋‹จ๊ณ„์˜ ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ ์†Œ์ž๋“ค์ด ์—ฐ๊ตฌ๋˜๊ณ  ์žˆ๋‹ค. ๊ทธ ์ค‘ ํ„ฐ๋„ ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ(TFET)์€ ๊ทธ ํŠน์œ ์˜ ์šฐ์ˆ˜ํ•œ ์ „์› ํŠน์„ฑ์œผ๋กœ ๊ฐ๊ด‘๋ฐ›์•„ ์ง‘์ค‘์ ์œผ๋กœ ์—ฐ๊ตฌ๋˜๊ณ  ์žˆ๋‹ค. ๋งŽ์€ ์—ฐ๊ตฌ์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ , TFET์˜ ๋ถ€์กฑํ•œ ์ „๋ฅ˜ ๊ตฌ๋™ ๋Šฅ๋ ฅ์€ MOSFET์˜ ๋Œ€์ฒด์žฌ๋กœ ์ž๋ฆฌ๋งค๊น€ํ•˜๋Š” ๋ฐ ๊ฐ€์žฅ ํฐ ๋ฌธ์ œ์ ์ด ๋˜๊ณ  ์žˆ๋‹ค. ๋ณธ ํ•™์œ„๋…ผ๋ฌธ์—์„œ๋Š” ์ƒ๊ธฐ๋œ ๋ฌธ์ œ์ ์„ ํ•ด๊ฒฐํ•  ์ˆ˜ ์žˆ๋Š” ์šฐ์ˆ˜ํ•œ ์ „๋ฅ˜ ๊ตฌ๋™ ๋Šฅ๋ ฅ์„ ๊ฐ€์ง„ TFET์ด ์ œ์•ˆ๋˜์—ˆ๋‹ค. ๋ฐ˜์†ก์ž ์œ ์ž…๊ณผ ๊ฒŒ์ดํŠธ ์ปจํŠธ๋กค์„ ํ–ฅ์ƒ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ์ˆ˜์ง ์ ์ธต๋œ ์‹ค๋ฆฌ์ฝ˜์ €๋งˆ๋Š„(SiGe) ๋‚˜๋…ธ์‹œํŠธ ์ฑ„๋„์ด ์‚ฌ์šฉ๋˜์—ˆ๋‹ค. ๋˜ํ•œ, ์ œ์•ˆ๋œ TFET์€ CMOS ๊ธฐ๋ฐ˜ ๊ณต์ •์„ ํ™œ์šฉํ•˜์—ฌ MOSFET๊ณผ ํ•จ๊ป˜ ์ œ์ž‘๋˜์—ˆ๋‹ค. ํ…Œํฌ๋†€๋กœ์ง€ ์ปดํ“จํ„ฐ ์ง€์› ์„ค๊ณ„(TCAD) ์‹œ๋ฎฌ๋ ˆ์ด์…˜๊ณผ ์‹ค์ œ ์ธก์ • ๊ฒฐ๊ณผ๋ฅผ ํ™œ์šฉํ•˜์—ฌ ์ œ์•ˆ๋œ ์†Œ์ž์˜ ์šฐ์ˆ˜์„ฑ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋‹จ์œ„ CMOS ์†Œ์ž์˜ ๊ด€์ ์—์„œ, ์ „์› ํŠน์„ฑ๊ณผ ์ „๋ฅ˜ ๊ตฌ๋™ ๋Šฅ๋ ฅ์˜ ํ–ฅ์ƒ์„ ์ •๋Ÿ‰์ , ์ •์„ฑ์  ๋ฐฉ๋ฒ•์œผ๋กœ ๋ถ„์„ํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ , ์ œ์ž‘๋œ ์†Œ์ž์˜ ์„ฑ๋Šฅ์„ ๊ธฐ์กด ์ œ์ž‘ ๋ฐ ๋ณด๊ณ ๋œ TFET ๋ฐ ํ•จ๊ป˜ ์ œ์ž‘๋œ MOSSFET๊ณผ ๋น„๊ตํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ๊ณผ์ •์„ ํ†ตํ•ด, ์‹ค๋ฆฌ์ฝ˜์ €๋งˆ๋Š„ ๋‚˜๋…ธ์‹œํŠธ TFET์˜ ํ™œ์šฉ ๊ฐ€๋Šฅ์„ฑ์ด ์ž…์ฆ๋˜์—ˆ๋‹ค. ์ œ์•ˆ๋œ ์‹ค๋ฆฌ์ฝ˜์ €๋งˆ๋Š„ ๋‚˜๋…ธ์‹œํŠธ ์†Œ์ž๋Š” ์ฃผ๋ชฉํ•  ๋งŒํ•œ ์ „์› ํŠน์„ฑ์„ ๊ฐ€์กŒ๊ณ  ์ €์ „์•• ๊ตฌ๋™ ํ™˜๊ฒฝ์—์„œ ํ•œ์ธต ๋” ๋‚ฎ์€ ๋ˆ„์„ค ์ „๋ฅ˜๋ฅผ ๊ฐ€์ง์œผ๋กœ์จ ํ–ฅํ›„ MOSFET์„ ๋Œ€์ฒดํ• ๋งŒํ•œ ์ถฉ๋ถ„ํ•œ ๊ฐ€๋Šฅ์„ฑ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค.Chapter 1 Introduction 1 1.1. Power Crisis of Conventional CMOS Technology 1 1.2. Tunnel Field-Effect Transistor (TFET) 6 1.3. Feasibility and Challenges of TFET 9 1.4. Scope of Thesis 11 Chapter 2 Device Characterization 13 2.1. SiGe Nanosheet TFET 13 2.2. Device Concept 15 2.3. Calibration Procedure for TCAD simulation 17 2.4. Device Verification with TCAD simulation 21 Chapter 3 Device Fabrication 31 3.1. Fabrication Process Flow 31 3.2. Key Processes for SiGe Nanosheet TFET 33 3.2.1. Key Process 1 : SiGe Nanosheet Formation 34 3.2.2. Key Process 2 : Source/Drain Implantation 41 3.2.3. Key Process 3 : High-ฮบ/Metal gate Formation 43 Chapter 4 Results and Discussion 53 4.1. Measurement Results 53 4.2. Analysis of Device Characteristics 56 4.2.1. Improved Factors to Performance in SiGe Nanosheet TFET 56 4.2.2. Performance Comparison with SiGe Nanosheet MOSFET 62 4.3. Performance Evaluation through Benchmarks 64 4.4. Optimization Plan for SiGe nanosheet TFET 66 4.4.1. Improvement of Quality of Gate Dielectric 66 4.4.2. Optimization of Doping Junction at Source 67 Chapter 5 Conclusion 71 Bibliography 73 Abstract in Korean 81 List of Publications 83Docto

    Design and Modelling of Tunnel Field Effect Transistor- using TCAD Modeling

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    The purpose of this research was to suggest a junction-less strategy for a vertical Tunnel Field Effect Transistor, which would increase the device's efficiency. In this study, we examine the similarities and differences between a negative capacitor TFET and a vertically generated TFET with a source pocket and a heterostructure-based nanowire gate. And how the channel transit impacts the output qualities of a sub-100 nanometer sized device. The Silvaco TCAD (a commercially available tool) was used to simulate a tri-layer high-K dielectric made of hafnium zirconium oxide (HZO) and titanium dioxide (TiO2) materials as gate stacking to the V-TFET and GAA-NC-TFET structures, and the tunnelling and transport parameters were calibrated experimentally. A short bandgap material, GaSb, in the home region to enhance carrier tunnelling via the mentioned three source (GaSb)-channel (Si) heterojunction at varying biases were utilized. Motion, tube length, and saturating velocity are only few of the transport channel characteristics that are investigated. As a result of the building's vertical orientation, the electric field is enhanced, allowing for an ION current of up to 104 Am2. The most unexpected result of this device is that a high ION/IOFF may increase mobility and reduce saturation velocity, perhaps reducing the drain voltage at saturation. The proposed biosensor's sensitivity was multiplied by 108 when vertical and lateral tunnelling were used in tandem. We apply a variety of optimisation strategies to deal with this problem, despite the fact that quantum confinement reduces the effect of mobility variations on device performance. When biomolecules were positively charged, the drain current increased, and when they were negatively charged, the drain current decreased

    Vertical III-V Nanowire Transistors for Low-Power Electronics

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    Power dissipation has been the major challenge in the downscaling of transistor technology. Metal-Oxide-Semiconductor Field-Effect Transistors (MOSFETs) have struggled to keep a low power consumption while still maintaining a high performance due to the low carrier mobilities of Si but also due to their inherent minimum inverse subthreshold slope (S โ‰ฅ 60 mV/dec) which is limited by thermionic emission. This thesis work studied the capabilities and limitations of III-V based vertical nanowire n-type Tunneling Field-Effect Transistor (TFET) and p-type MOSFET (PMOS). InAs/InGaAsSb/GaSb heterojunction was employed in the whole study. The main focus was to understand the influence of the device fabrication processes and the structural factors of the nanowires such as band alignment, composition and doping on the electrical performance of the TFET. Optimizations of the device processes including spacer technology improvement, Equivalent Oxide Thickness (EOT) downscaling, and gate underlap/overlap were explored utilizing structural characterizations. Systematic fine tuning of the band alignment of the tunnel junction resultedin achieving the best performing sub-40 mV/dec TFETs with S = 32 mV/decand ION = 4ฮผA/ฮผm for IOFF = 1 nA/ฮผm at VDS = 0.3 V. The suitability of employing TFET for electronic applications at cryogenic temperatures has been explored utilizing experimental device data. The impact of the choice of heterostructure and dopant incorporation were investigated to identify the optimum operating temperature and voltage in different temperature regimes. A novel gate last process self-aligning the gate and drain contacts to the intrinsic and doped segments, respectively was developed for vertical InGaAsSb-GaAsSb core-shell nanowire transistors leading to the first sub-100 mV/dec PMOS with S = 75 mV/dec, significant ION/ IOFF = 104 and IMIN < 1 nA/ฮผm at VDS = -0.5 V

    A review of selected topics in physics based modeling for tunnel field-effect transistors

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    The research field on tunnel-FETs (TFETs) has been rapidly developing in the last ten years, driven by the quest for a new electronic switch operating at a supply voltage well below 1 V and thus delivering substantial improvements in the energy efficiency of integrated circuits. This paper reviews several aspects related to physics based modeling in TFETs, and shows how the description of these transistors implies a remarkable innovation and poses new challenges compared to conventional MOSFETs. A hierarchy of numerical models exist for TFETs covering a wide range of predictive capabilities and computational complexities. We start by reviewing seminal contributions on direct and indirect band-to-band tunneling (BTBT) modeling in semiconductors, from which most TCAD models have been actually derived. Then we move to the features and limitations of TCAD models themselves and to the discussion of what we define non-self-consistent quantum models, where BTBT is computed with rigorous quantum-mechanical models starting from frozen potential profiles and closed-boundary Schr\uf6dinger equation problems. We will then address models that solve the open-boundary Schr\uf6dinger equation problem, based either on the non-equilibrium Green's function NEGF or on the quantum-transmitting-boundary formalism, and show how the computational burden of these models may vary in a wide range depending on the Hamiltonian employed in the calculations. A specific section is devoted to TFETs based on 2D crystals and van der Waals hetero-structures. The main goal of this paper is to provide the reader with an introduction to the most important physics based models for TFETs, and with a possible guidance to the wide and rapidly developing literature in this exciting research field

    Vertical III-V Nanowire Tunnel Field-Effect Transistor

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    In this thesis fabrication and optimization of vertical III-V Tunneling Field-Effect transistors was explored. Usage of vertical nanowires, allows for combination of materials with large lattice mismatch in the same nanowire structure. TFETs in this thesis were fabricated using vertical InAs/GaSb or InAs/InGaAsSb/GaSb nanowires of high material quality. Usage of these material systems allowed for fabrication of devices with staggered and broken band-gap alignment. To fully harvest the benefits from these structures, the fabrication process was optimized. This was performed by exploring different spacer and gate technologies, required for vertical devices. Furthermore, improvement of electrostatics was achieved by reduction of the channel diameter and high-ฮบ interface. Further improvements of the performance were achieved by scaling of the device dimensions such as nanowire lengths, spacer thickness, and gate-length. Used fabrication techniques allowed us to fabricate devices with a channel diameter of 11 nm. By switching from InAs/GaSb to InAs/InGaAsSb/GaSb allowed for optimization of the heterojunction, which allowed us to fabricate devices with record performance, reaching a minimum subthreshold swing of 48 mV/decade and a record high I60 of 0.31 ฮผA/ฮผm at a drive voltage of 0.3 V. Stability of the process allowed us to demonstrate data from a large number of TFETs with ability to operate below the thermal limit of 60 mV/decade. This allowed us to study correlations between important device parameter such as: I60, on-current, subthreshold swing, and off-current. Using transmission electron microscopy, the heterojunction was characterized. Furthermore, TCAD modeling was performed to understand what limits the performance of these devices. Also, electrical measurement of the random telegraph noise allowed us to understand the impact the oxide defects have on highly scaled devices

    Development of a thin-film space-charge- limited triode Final report, Mar. 1965 - Jun. 1966

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    Development of thin film space charge limited triod

    EFFECTS OF SOURCE DOPING PROFILE ON DEVICE CHARACTERISTICS OF LATERAL AND VERTICAL TUNNEL FIELD-EFFECT TRANSISTORS

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    The source doping engineering, the low bandgap material and the vertical tunneling structure have recently been considered as most effective techniques to resolve the on-current issue in tunnel field-effect transistors (TFETs). In this paper, the effects of source doping profile, including the concentration and gradient, on the device characteristics are adequately elucidated in lateral and vertical TFETs using low bandgap germanium to allow a comprehensive comparison between the two major TFET architectures for the first time. Similar dependences of the on-current on the source concentration are observed in lateral and vertical TFETs, except that the on-current of vertical TFETs is always greater than that of lateral TFETs approximately one order of magnitude. With different contributions of the lateral and vertical tunneling components in the subthreshold region, the subthreshold swing of vertical TFETs first decreases at small concentrations, then increases at medium values, and finally decreases again at high concentrations, whereas that of lateral counterparts always decreases exponentially with increase in the source concentration. The on-current of lateral TFETs is significantly decreased, while that of vertical TFETs is almost invariable with increasing the source doping gradient. With competitive advantages of the vertical TFET architecture in on-current, subthreshold swing and device fabrication, vertical TFETs using low bandgap semiconductors are promising for use in low power applications
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