477 research outputs found

    Random Discrete Dopant Induced Variability in Negative Capacitance Transistors

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    In this work we investigate the impact of random discrete dopants (RDD) induced statistical variability in ferroelectric negative capacitance field effect transistors (NCFETs). We couple the 3D `atomistic' statistical device simulator GARAND with the Landau - Khalatnikov equation of the ferroelectric for this study. We found that the negative capacitance effect provided by the ferroelectric layer can lead to suppression of the RDD induced variability in the threshold voltage (Vt), OFF-current (IOFF), and ON-current (ION). This immunity to RDD induced variability increases with increase in the ferroelectric thickness

    Modeling and Simulation of Negative Capacitance MOSFETs

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    The current and voltage characteristics of a MOSFET device are maily characterized by the source to channel barrier which is controlled by the gate voltage. The Boltazmann statistics which govern the number of carriers that are able to cross the barrier indicates that to increase the current by a decade, atleast 60 mV of rise in gate voltage is required. As a result of this limitation, the threshold voltage of modern MOSFETs cannot be less than about 0.3 V for an ION to IOFF ratio of 5 decades. This has put a fundamental bottleneck in voltage downscaling increasing the power consumption in modern IC based chips with billions of transistors. Sayeef Salahuddin and Supriyo Dutta proposed the idea of including ferroelectric in MOSFET gate stack which allows an internal voltage ampli๏ฟฝcation at the MOSFET channel which can be used to achieve a smaller subthreshold swing which would further reduce the power consumption of the devices. In this thesis we have undertaken a simulation based study of such devices to study how the inclusion of negative capacitance ferroelectrics leads changes in various device characteristics. Initially we have taken a compact modeling based approach to study device characteristics in latest industry standard FinFET devices. For this purpose we have used the BSIM-CMG Verilog A model and modi๏ฟฝed the model appropriately to include the e๏ฟฝect of negative capacitance ferroelectric in the gate stack. This simulation allowed us to observe that negative capacitance (NC) devices can indeed give a subthreshold swing lesser than 60 mV/dec. Further other interesting properties like negative output resistance and drain induced barrier rising are observed. Using the compact models developed above, we have analyzed some simple circuits with NC devices. Initially an inverter shows a hysteresis in the transfer characteristics. This can be attributed to negative di๏ฟฝerential resistance. Ring oscillator analysis shows that RO frequency for NC devices is lesser than that of regular devices due to enhanced gate capacitance and slower response of ferroelectrics. Scaling analysis has been performed to see the performance of NC devices in future technologies. For this we used TCAD analysis coupled with Landau Khalatnikov equation. This analysis shows that NC devices are more e๏ฟฝective in suppressing short channel e๏ฟฝects like DIBL and can hence be used for further downscaling of the devices. Finally we develop models to take into account the multidomain Landau equations for ferroelec- tric into account. We have performed such an analysis for a ferroelectric resistor series network. A similar analysis is performed for short channel double gate MOSFET without inter layer metal be- tween ferroelectric and the internal MOS device. This analysis showed that coupling factor between ferroelectric domains plays an important role in the device characteristics

    III-V and 2D Devices: from MOSFETs to Steep-Slope Transistors

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    With silicon CMOS technology approaching the scaling limit, alternating channel materials and novel device structures have been extensively studied and attracted a lot of attention in solid-state device research. In this dissertation, solid-state electron devices for post-Si CMOS applications are explored including both new materials such as III-V and 2D materials and new device structures such as tunneling field-effect transistors and negative capacitance field-effect transistors. Multiple critical challenges in applying such new materials and new device structures are addressed and the key achievements in this dissertation are summarized as follows: 1) Development of fabrication process technology for ultra-scaled planar and 3D InGaAs MOSFETs. 2) Interface passivation by forming gas anneal on InGaAs gate-all-around MOSFETs. 3) Characterization methods for ultra-scaled MOSFETs, including a correction to subthreshold method and low frequency noise characterization in short channel devices. 4) Development of short channel InGaAs planar and 3D gate-allaround tunneling field-effect transistors. 5) Negative capacitance field-effect transistors with hysteresis-free and bi-directional sub-thermionic subthreshold slope and the integration with various channel materials such as InGaAs and MoS2

    ฮฒ\beta-Ga2_2O3_3 Nano-membrane Negative Capacitance Field-effect Transistor with Steep Subthreshold Slope for Wide Bandgap Logic Applications

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    Steep-slope ฮฒ\beta-Ga2_2O3_3 nano-membrane negative capacitance field-effect transistors (NC-FETs) are demonstrated with ferroelectric hafnium zirconium oxide in gate dielectric stack. Subthreshold slope less than 60 mV/dec at room temperature is obtained for both forward and reverse gate voltage sweeps with a minimum value of 34.3 mV/dec at reverse gate voltage sweep and 53.1 mV/dec at forward gate voltage sweep at VDSV_{DS}=0.5 V. Enhancement-mode operation with threshold voltage ~0.4 V is achieved by tuning the thickness of ฮฒ\beta-Ga2_2O3_3 membrane. Low hysteresis of less than 0.1 V is obtained. The steep-slope, low hysteresis and enhancement-mode ฮฒ\beta-Ga2_2O3_3 NC-FETs are promising as nFET candidate for future wide bandgap CMOS logic applications.Comment: 21 pages, 5 figure

    ์ ์ธต ๋‚˜๋…ธ์‹œํŠธ ๊ตฌ์กฐ์˜ ์Œ์˜ ์ •์ „์šฉ๋Ÿ‰ ์ „๊ณ„ ํšจ๊ณผ ํŠธ๋žœ์ง€์Šคํ„ฐ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2022. 8. ์ตœ์šฐ์˜.The development of integrated circuit (IC) technology has continued to improve speed and capacity through miniaturization of devices. However, power density is increasing rapidly due to the increasing leakage current as miniaturization advances. Although the remarkable advancement of process technology has allowed complementary-metal-oxide-semiconductor (CMOS) technology to consistently overcome its constraints, the physical limitations of the metal-oxide-semiconductor field-effect transistor (MOSFET) are unmanageable. Accordingly, research on logic device is being divided into a CMOS-extension and a beyond-CMOS. CMOS-extension focuses on the gate-all-around field-effect transistors (GAAFETs) which is a promising architecture for future CMOS thanks to the excellent electrostatic gate controllability. Particularly, nanosheet (NS) architecture with high current drivability required in ICs, is the most promising. However, NS GAAFET has a trade-off relation between the controllability and the drivability, which requires the necessity of a higher-level effective oxide thickness (EOT) scaling for further scaling of NS GAAFET. On the other hand, beyond-CMOS mainly focuses on developing devices with novel mechanisms to overcome the MOSFETs' physical limits. Among several candidates, negative capacitance field-effect transistors (NCFETs) with exceptional CMOS compatibility and current drivability are highlighted as future logic devices for low-power, high-performance operation. Although the NCFET utilizing the negative capacitance (NC) effect of a ferroelectric has been demonstrated theoretically by the Landau model, it is challenging to be implemented due to the fact that stabilized NC and sub-thermionic subthreshold swing (SS) are incompatible. In this dissertation, a GAA NCFET that maintains a stable capacitance boosting by NC effect and exhibits high performance is demonstrated. A ferroelectric-antiferroelectric mixed-phase hafnium-zirconium-oxide (HZO) thin film was introduced, whose effect was confirmed by capacitors and FET experiments. Furthermore, the mixed-phase HZO was demonstrated on a stacked nanosheet gate-all-around (stacked NS GAA) structure, the advanced CMOS technology, which exhibits a superior gate controllability as well as a satisfactory drivability for ICs. The hysteresis-free stable NC operation with the superior performance was confirmed in NS GAA NCFET. The improved SS and on-current (Ion) compared to MOSFETs fabricated in the same manner were validated, and its feasibility as a low-power, high-performance logic device was proven based on a variety of figure of merits.์ง‘์ ํšŒ๋กœ ๊ธฐ์ˆ ์˜ ๋ฐœ์ „์€ ์†Œ์ž์˜ ์†Œํ˜•ํ™”๋ฅผ ํ†ตํ•œ ์†๋„ ๋ฐ ์šฉ๋Ÿ‰์˜ ํ–ฅ์ƒ์„ ์œ„ํ•ด ๋ฐœ์ „์„ ๊ฑฐ๋“ญํ•ด์™”๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์†Œํ˜•ํ™”๋ฅผ ๊ฑฐ๋“ญํ• ์ˆ˜๋ก ์ฆ๊ฐ€ํ•˜๋Š” ๋ˆ„์„ค์ „๋ฅ˜์˜ ๋ฌธ์ œ๋กœ ์ „๋ ฅ ๋ฐ€๋„๊ฐ€ ๊ธ‰๊ฒฉํ•˜๊ฒŒ ์ฆ๊ฐ€ํ•˜๊ณ  ์žˆ๋‹ค. ์ƒ๋ณดํ˜• ๊ธˆ์†-์‚ฐํ™”๋ง‰-๋ฐ˜๋„์ฒด(CMOS) ๊ธฐ์ˆ ์€ ๋ˆˆ๋ถ€์‹  ๊ณต์ •๊ธฐ์ˆ ์˜ ์„ฑ์žฅ์— ํž˜์ž…์–ด ํ•œ๊ณ„๋ฅผ ๋Š์ž„์—†์ด ๊ทน๋ณตํ•ด์™”์œผ๋‚˜, ๊ธฐ์กด์˜ ๊ธˆ์†-์‚ฐํ™”๋ง‰-๋ฐ˜๋„์ฒด ์ „๊ณ„-ํšจ๊ณผ-ํŠธ๋žœ์ง€์Šคํ„ฐ(MOSFET)์˜ ๋ฌผ๋ฆฌ์  ํ•œ๊ณ„๋Š” ๊ทน๋ณตํ•  ์ˆ˜ ์—†๋Š” ๋ฌธ์ œ์ด๋‹ค. ์ด์— ๋”ฐ๋ผ ๋…ผ๋ฆฌ ๋ฐ˜๋„์ฒด์— ๊ด€ํ•œ ์—ฐ๊ตฌ๋Š” CMOS๋ฅผ ์—ฐ์žฅํ•˜๋Š” ๋ฐฉํ–ฅ๊ณผ CMOS๋ฅผ ๋›ฐ์–ด๋„˜๋Š” ๋ฐฉํ–ฅ์œผ๋กœ ๋‚˜๋‰˜์–ด ์ง„ํ–‰๋˜๊ณ  ์žˆ๋‹ค. CMOS๋ฅผ ์—ฐ์žฅํ•˜๋Š” ๋ฐฉํ–ฅ์€ ๋›ฐ์–ด๋‚œ ์ •์ „๊ธฐ์  ๊ฒŒ์ดํŠธ ์žฅ์•…๋ ฅ์„ ๊ฐ–๋Š” ์ฐจ์„ธ๋Œ€ CMOS ๊ตฌ์กฐ๋กœ ์œ ๋งํ•œ ๊ฒŒ์ดํŠธ-์˜ฌ-์–ด๋ผ์šด๋“œ ์ „๊ณ„-ํšจ๊ณผ-ํŠธ๋žœ์ง€์Šคํ„ฐ(GAAFET)์— ๊ด€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ์ฃผ๋ฅผ ์ด๋ฃฌ๋‹ค. ํŠนํžˆ ๋†’์€ ์ „๋ฅ˜ ๊ตฌ๋™๋ ฅ์„ ๊ฐ€์งˆ ์ˆ˜ ์žˆ๋Š” ๋‚˜๋…ธ์‹œํŠธ(NS) ๊ตฌ์กฐ๊ฐ€ ๊ฐ€์žฅ ์œ ๋งํ•œ๋ฐ, ๊ฒŒ์ดํŠธ ์žฅ์•…๋ ฅ์ด ์ „๋ฅ˜ ๊ตฌ๋™๋ ฅ๊ณผ ์ƒ์ถฉ๋œ๋‹ค๋Š” ๋‹จ์ ์ด ์žˆ๋‹ค. ์ด์— ๋”ฐ๋ผ NS GAAFET ๊ธฐ์ˆ ์„ ์œ„ํ•ด์„œ๋Š” ๋” ๋†’์€ ์ˆ˜์ค€์˜ ์œ ํšจ์‚ฐํ™”๋ง‰๋‘๊ป˜ (EOT) ์Šค์ผ€์ผ๋ง์ด ํ•„์ˆ˜์ ์ด๋‹ค. ํ•œํŽธ, CMOS๋ฅผ ๋›ฐ์–ด๋„˜๋Š” ๋ฐฉํ–ฅ์˜ ์—ฐ๊ตฌ๋Š” MOSFET์˜ ๋ฌผ๋ฆฌ์  ํ•œ๊ณ„๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์ƒˆ๋กœ์šด ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๊ฐ–๋Š” ์†Œ์ž๋ฅผ ๊ฐœ๋ฐœํ•˜๋Š” ๋ฐฉํ–ฅ์œผ๋กœ ์ด๋ฃจ์–ด์ง„๋‹ค. ๋‹ค์–‘ํ•œ ํ›„๋ณด๊ตฐ ์ค‘ CMOS ํ˜ธํ™˜์„ฑ๊ณผ ์ „๋ฅ˜ ๊ตฌ๋™๋Šฅ๋ ฅ์ด ๋›ฐ์–ด๋‚œ ์Œ์˜ ์ •์ „์šฉ๋Ÿ‰ ์ „๊ณ„-ํšจ๊ณผ-ํŠธ๋žœ์ง€์Šคํ„ฐ(NCFET)์ด ์ €์ „๋ ฅ, ๊ณ ์„ฑ๋Šฅ ๋™์ž‘์„ ์œ„ํ•œ ๋ฏธ๋ž˜ CMOS ์†Œ์ž๋กœ ๊ฐ๊ด‘๋ฐ›๊ณ  ์žˆ๋‹ค. ๊ฐ•์œ ์ „์ฒด์˜ ์Œ์˜ ์ •์ „์šฉ๋Ÿ‰ (NC) ํšจ๊ณผ๋ฅผ ์ด์šฉํ•œ NCFET์€ Landau ๋ชจ๋ธ์— ์˜ํ•ด ์ด๋ก ์ ์œผ๋กœ ์ฆ๋ช…๋˜์—ˆ์œผ๋‚˜, ์—ด์—ญํ•™์ ์œผ๋กœ ์•ˆ์ •ํ•œ ์ƒํƒœ์™€ 60 mV/dec ์ดํ•˜์˜ ๋ฌธํ„ฑ์ „์••-์ดํ•˜-๊ธฐ์šธ๊ธฐ(SS)๋ฅผ ๋™์‹œ์— ๊ตฌํ˜„ํ•˜๊ธฐ ๋ถˆ๊ฐ€๋Šฅํ•˜๋‹ค๋Š” ๋ฌธ์ œ๊ฐ€ ์žˆ๋‹ค. ๋ณธ ํ•™์œ„๋…ผ๋ฌธ์—์„œ๋Š” ์•ˆ์ •ํ•œ ์ •์ „์šฉ๋Ÿ‰ ํ–ฅ์ƒ ํŠน์„ฑ์„ ๊ฐ€์ง€๋ฉฐ ๋†’์€ ์„ฑ๋Šฅ์„ ๊ฐ–๋Š” NS GAA NCFET์„ ๊ตฌํ˜„ํ•˜์˜€๋‹ค. ๊ฐ•์œ ์ „์ฒด(ferroelectric)-๋ฐ˜๊ฐ•์œ ์ „์ฒด(antiferroelectric) ํ˜ผํ•ฉ์ƒ(mixed-phase) ํ•˜ํ”„๋Š„-์ง€๋ฅด์ฝ”๋Š„-์˜ฅ์‚ฌ์ด๋“œ(HZO) ๋ฐ•๋ง‰์˜ ์ •์ „์šฉ๋Ÿ‰ ํ–ฅ์ƒ ํšจ๊ณผ๋ฅผ ์ปคํŒจ์‹œํ„ฐ ๋ฐ FET ์ œ์ž‘์„ ํ†ตํ•ด ํšจ๊ณผ๋ฅผ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋†’์€ ๊ฒŒ์ดํŠธ ์žฅ์•…๋ ฅ์„ ๊ฐ€์ง€๋ฉฐ ์ง‘์ ํšŒ๋กœ์—์„œ ์š”๊ตฌํ•˜๋Š” ์ „๋ฅ˜ ๊ตฌ๋™๋ ฅ์„ ๋งŒ์กฑ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ์ ์ธตํ˜• ๋‚˜๋…ธ์‹œํŠธ ๊ฒŒ์ดํŠธ-์˜ฌ-์–ด๋ผ์šด๋“œ(stacked NS GAA) ๊ตฌ์กฐ์— ํ˜ผํ•ฉ์ƒ NC ๋ฐ•๋ง‰์„ ์ ์šฉํ•œ FET์„ ์‹œ์—ฐํ•˜๊ณ  ์„ฑ๋Šฅ์˜ ์šฐ์ˆ˜์„ฑ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋™์ผํ•˜๊ฒŒ ์ œ์ž‘๋œ MOSFET ๋Œ€๋น„ ํ–ฅ์ƒ๋œ SS์™€ ๊ตฌ๋™ ์ „๋ฅ˜(Ion)๋ฅผ ํ™•์ธํ•˜์˜€๊ณ , ๋‹ค์–‘ํ•œ ์„ฑ๋Šฅ ์ง€์ˆ˜๋ฅผ ํ† ๋Œ€๋กœ ์ €์ „๋ ฅ, ๊ณ ์„ฑ๋Šฅ ๋กœ์ง ์†Œ์ž๋กœ์„œ์˜ ํƒ€๋‹น์„ฑ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค.Abstract i Contents iv List of Table vii List of Figures viii Chapter 1 Introduction 1 1.1 Power and Area Scaling Challenges 1 1.2 Nanosheet Gate-All-Around FETs 5 1.2.1 Gate-All-Around FETs 5 1.2.2 Nanosheet GAAFETs 6 1.3 Negative Capacitance FETs 11 1.3.1 Negative Capacitance in Ferroelectric Materials 11 1.3.2 Negative Capacitance for Steep Switching Devices 14 1.3.3 Stable NC vs. Sub-thermionic SS 17 1.4 Scope and Organization of Dissertation 21 Chapter 2 Stacked NS GAA NCFET with Ferroelectric-Antiferroelectric-Mixed-Phase HZO 22 2.1 Mixed-Phase HZO for Capacitance Boosting 22 2.2 NS GAA NCFET using Mixed-Phase HZO 25 Chapter 3 HZO ALD Stack Optimization 28 3.1 Metal-Ferroelectric-Interlayer-Silicon (MFIS) / MFM Capacitors 29 3.1.1 Fabrication of MFIS Capacitors 29 3.1.2 Electrical Characteristics of MFIS / MFM Capacitors 33 3.2 SOI Planar NCFETs 38 3.2.1 DC Measurements 38 3.2.2 Direct Capacitance Measurements 47 3.2.3 Speed Measurements 49 Chapter 4 Device Fabrication of Stacked NS GAA NCFET 51 4.1 Initial Process Flow of NS GAA NCFET 52 4.2 Process Issues and Solution 56 4.2.1 External Resistance 56 4.2.2 TiN Gate Sidewall Spacer 60 4.2.3 Unintentionally Etched Sacrificial Layer 65 4.2.4 Discussions 68 4.3 Channel Release Process 69 4.3.1 Consideration in Channel Release Process 69 4.3.2 Methods for SiGe Selective Etching 72 4.3.3 SiGe Selective Etching using Carboxylic Acid Solution 75 4.4 Revised Process of NS GAA NCFET 78 Chapter 5 Electrical Characteristics of Fabricated NS GAA NCFET 84 5.1 DC Characteristics 85 5.1.1 NS GAA NCFET vs. Planar SOI NCFET 85 5.1.2 Performance Enhancement of NS GAA NCFET 88 5.1.3 Performance Evaluation 96 5.2 Operating Temperature Properties 99 Chapter 6 Conclusion 102 Bibliography 105 ์ดˆ ๋ก 115๋ฐ•
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