적층 나노시트 구조의 음의 정전용량 전계 효과 트랜지스터

학위논문(박사) -- 서울대학교대학원 : 공과대학 전기·정보공학부, 2022. 8. 최우영.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.집적회로 기술의 발전은 소자의 소형화를 통한 속도 및 용량의 향상을 위해 발전을 거듭해왔다. 그러나 소형화를 거듭할수록 증가하는 누설전류의 문제로 전력 밀도가 급격하게 증가하고 있다. 상보형 금속-산화막-반도체(CMOS) 기술은 눈부신 공정기술의 성장에 힘입어 한계를 끊임없이 극복해왔으나, 기존의 금속-산화막-반도체 전계-효과-트랜지스터(MOSFET)의 물리적 한계는 극복할 수 없는 문제이다. 이에 따라 논리 반도체에 관한 연구는 CMOS를 연장하는 방향과 CMOS를 뛰어넘는 방향으로 나뉘어 진행되고 있다. CMOS를 연장하는 방향은 뛰어난 정전기적 게이트 장악력을 갖는 차세대 CMOS 구조로 유망한 게이트-올-어라운드 전계-효과-트랜지스터(GAAFET)에 관한 연구가 주를 이룬다. 특히 높은 전류 구동력을 가질 수 있는 나노시트(NS) 구조가 가장 유망한데, 게이트 장악력이 전류 구동력과 상충된다는 단점이 있다. 이에 따라 NS GAAFET 기술을 위해서는 더 높은 수준의 유효산화막두께 (EOT) 스케일링이 필수적이다. 한편, CMOS를 뛰어넘는 방향의 연구는 MOSFET의 물리적 한계를 극복하기 위해 새로운 메커니즘을 갖는 소자를 개발하는 방향으로 이루어진다. 다양한 후보군 중 CMOS 호환성과 전류 구동능력이 뛰어난 음의 정전용량 전계-효과-트랜지스터(NCFET)이 저전력, 고성능 동작을 위한 미래 CMOS 소자로 각광받고 있다. 강유전체의 음의 정전용량 (NC) 효과를 이용한 NCFET은 Landau 모델에 의해 이론적으로 증명되었으나, 열역학적으로 안정한 상태와 60 mV/dec 이하의 문턱전압-이하-기울기(SS)를 동시에 구현하기 불가능하다는 문제가 있다. 본 학위논문에서는 안정한 정전용량 향상 특성을 가지며 높은 성능을 갖는 NS GAA NCFET을 구현하였다. 강유전체(ferroelectric)-반강유전체(antiferroelectric) 혼합상(mixed-phase) 하프늄-지르코늄-옥사이드(HZO) 박막의 정전용량 향상 효과를 커패시터 및 FET 제작을 통해 효과를 검증하였다. 또한 높은 게이트 장악력을 가지며 집적회로에서 요구하는 전류 구동력을 만족시킬 수 있는 적층형 나노시트 게이트-올-어라운드(stacked NS GAA) 구조에 혼합상 NC 박막을 적용한 FET을 시연하고 성능의 우수성을 확인하였다. 동일하게 제작된 MOSFET 대비 향상된 SS와 구동 전류(Ion)를 확인하였고, 다양한 성능 지수를 토대로 저전력, 고성능 로직 소자로서의 타당성을 검증하였다.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 초 록 115박

Multiple-Independent-Gate Field-Effect Transistors for High Computational Density and Low Power Consumption

Transistors are the fundamental elements in Integrated Circuits (IC). The development of transistors significantly improves the circuit performance. Numerous technology innovations have been adopted to maintain the continuous scaling down of transistors. With all these innovations and efforts, the transistor size is approaching the natural limitations of materials in the near future. The circuits are expected to compute in a more efficient way. From this perspective, new device concepts are desirable to exploit additional functionality. On the other hand, with the continuously increased device density on the chips, reducing the power consumption has become a key concern in IC design. To overcome the limitations of Complementary Metal-Oxide-Semiconductor (CMOS) technology in computing efficiency and power reduction, this thesis introduces the multiple- independent-gate Field-Effect Transistors (FETs) with silicon nanowires and FinFET structures. The device not only has the capability of polarity control, but also provides dual-threshold- voltage and steep-subthreshold-slope operations for power reduction in circuit design. By independently modulating the Schottky junctions between metallic source/drain and semiconductor channel, the dual-threshold-voltage characteristics with controllable polarity are achieved in a single device. This property is demonstrated in both experiments and simulations. Thanks to the compact implementation of logic functions, circuit-level benchmarking shows promising performance with a configurable dual-threshold-voltage physical design, which is suitable for low-power applications. This thesis also experimentally demonstrates the steep-subthreshold-slope operation in the multiple-independent-gate FETs. Based on a positive feedback induced by weak impact ionization, the measured characteristics of the device achieve a steep subthreshold slope of 6 mV/dec over 5 decades of current. High Ion/Ioff ratio and low leakage current are also simultaneously obtained with a good reliability. Based on a physical analysis of the device operation, feasible improvements are suggested to further enhance the performance. A physics-based surface potential and drain current model is also derived for the polarity-controllable Silicon Nanowire FETs (SiNWFETs). By solving the carrier transport at Schottky junctions and in the channel, the core model captures the operation with independent gate control. It can serve as the core framework for developing a complete compact model by integrating advanced physical effects. To summarize, multiple-independent-gate SiNWFETs and FinFETs are extensively studied in terms of fabrication, modeling, and simulation. The proposed device concept expands the family of polarity-controllable FETs. In addition to the enhanced logic functionality, the polarity-controllable SiNWFETs and FinFETs with the dual-threshold-voltage and steep-subthreshold-slope operation can be promising candidates for future IC design towards low-power applications

Developing ultrasensitive and CMOS compatible ISFETs in the BEOL of industrial UTBB FDSOI transistors

Le marché des capteurs a récemment connu une croissance spectaculaire alimentée par l'application remarquable de capteurs dans l'électronique de consommation, l'industrie de l'automatisation, les appareils portables, le secteur automobile et l'internet des objets de plus en plus adopté. La technologie avancée des complementary metal oxide semiconductor (CMOS), les technologies de nano et de micro-fabrication et les plateformes de synthèse de matériaux innovantes sont également des moteurs du développement incroyable de l'industrie des capteurs. Ces progrès ont permis la réalisation de capteurs dotés de nombreuses caractéristiques telles que la précision accrue, les dimensions miniaturisées, l’intégrabilité, la production de masse, le coût très réduit et le temps de réponse rapide. Les ion-sensitive field-effect transistors (ISFETs) sont des capteurs à l'état solide (bio) chimiques, destinés à la détection des ions H+ (pH), Na+ et K+. Malgré cela, la commercialisation des ISFETs est encore à ses balbutiements, après près de cinq décennies de recherche et développement. Cela est dû principalement à la sensibilité limitée, à la controverse sur l'utilisation de l'électrode de référence pour le fonctionnement des ISFETs et à des problèmes de stabilité. Dans cette thèse, les ISFETs ultrasensibles et compatibles CMOS sont intégrés dans le BEOL des transistors UTBB FDSOI standard. Un circuit diviseur capacitif est utilisé pour polariser la grille d’avant afin d'assurer des performances stables du capteur. En exploitant la fonction d’amplification intrinsèque fournie par les transistors UTBB FDSOI, nous avons présenté des ISFET ultra sensibles. L'amplification découle du fort couplage électrostatique entre la grille avant et la grille arrière du FDSOI et des capacités asymétriques des deux grilles. Un changement de tension au niveau de la grille avant apparaît sur la grille arrière sous la forme d'un décalage amplifié de la tension. L'amplification, représentée par le facteur de couplage (γ), est égale au rapport de la capacité de l'oxyde de grille et de la capacité de le buried oxide (BOX). Par conséquent, en fonctionnalisant la détection du pH sur la grille avant pour les dispositifs FDSOI, la modification du potentiel de surface sur la grille avant est détectée par la grille arrière et amplifiée du facteur de couplage (γ), donnant lieu à un capteur chimique à l'état solide à sensibilité ultra-élevée. L'intégration de la fonctionnalité de détection a été réalisée en back end of line (BEOL), ce qui offre les avantages d'une fiabilité et d'une durée de vie accrues du capteur, d'une compatibilité avec le processus CMOS standard et d'une possibilité d'intégration d'un circuit diviseur capacitif. Le fonctionnement des MOSFETs, sans une polarisation appropriée de la grille avant, les rend vulnérables aux effets de grilles flottantes indésirables. Le circuit diviseur capacitif résout ce problème en polarisant la grille avant tout enmaintenant la fonctionnalité de détection sur la même grille par un couplage capacitif au métal commun du BEOL. Par conséquent, le potentiel au niveau du métal BEOL est une somme pondérée du potentiel de surface au niveau de la grille de détection et de la polarisation appliquée au niveau de la grille de contrôle. Le capteur proposé est modélisé et simulé à l'aide de TCAD-Sentaurus. Un modèle mathématique complet a été développé. Il fournit la réponse du capteur en fonction du pH de la solution (entrée du capteur) et des paramètres de conception du circuit diviseur capacitif et du transistor UTBB FDSOI. Dans ce cas, des résultats cohérents ont été obtenus des travaux de modélisation et de simulation, avec une sensibilité attendue de 780 mV / pH correspondant à un film de détection ayant une réponse de Nernst. La modélisation et la simulation du capteur proposé ont également été validées par une fabrication et une caractérisation du capteur de pH à grille étendue avec validation de son concept. Ces capteurs ont été développés par un traitement séparé du composant de détection de pH, qui est connecté électriquement au transistor uniquement lors de la caractérisation du capteur. Ceci permet une réalisation plus rapide et plus simple du capteur sans avoir besoin de masques et de motifs par lithographie. Les capteurs à grille étendue ont présenté une sensibilité de 475 mV/pH, ce qui est supérieur aux ISFET de faible puissance de l'état de l’art. Enfin, l’intégration de la fonctionnalité de détection directement dans le BEOL des dispositifs FDSOI UTBB a été poursuivie. Une sensibilité expérimentale de 730 mV/pH a été obtenue, ce qui confirme le modèle mathématique et la réponse simulée. Cette valeur est 12 fois supérieure à la limite de Nernst et supérieure aux capteurs de l'état de l’art. Les capteurs sont également évalués pour la stabilité, la résolution, l'hystérésis et la dérive dans lesquels d'excellentes performances sont démontrées. Une nouvelle architecture de détection du pH est également démontrée avec succès, dans laquelle la détection est fonctionnalisée au niveau de la diode de protection de la grille plutôt que de la grille avant des dispositifs UTBB FDSOI. La commutation de courant abrupte, aussi basse que 9 mV/decade, pourrait potentiellement augmenter la sensibilité de polarisation fixée à 6,6 decade/pH. Nous avons démontré expérimentalement une sensibilité de 1,25 decade/pH supérieure à la sensibilité reportée à l’état de l’art.Abstract: The sensor market has recently seen a dramatic growth fueled by the remarkable application of sensors in the consumer electronics, automation industry, wearable devices, the automotive sector, and in the increasingly adopted internet of things (IoT). The advanced complementary metal oxide semiconductor (CMOS) technology, the nano and micro fabrication technologies, and the innovative material synthesis platforms are also driving forces for the incredible development of the sensor industry. These technological advancements have enabled realization of sensors with characteristic features of increased accuracy, miniaturized dimension, integrability, volume production, highly reduced cost, and fast response time. Ion-sensitive field-effect transistors (ISFETs) are solid state (bio)chemical sensors, for pH (H+), Na+, K+ ion detection, that are equipped with the promise of the highly aspired features of CMOS devices. Despite this, the commercialization of ISFETs is still at the stage of infancy after nearly five decades of research and development. This is due mainly to the limited sensitivity, the controversy over the use of the reference electrode for ISFET operation, and because of stability issues. In this thesis, ultrasensitive and CMOS compatible ISFETs are integrated in the back end of line (BEOL) of standard UTBB FDSOI transistors. A capacitive divider circuit is employed for biasing the front gate for stable performance of the sensor. Exploiting the intrinsic amplification feature provided by UTBB FDSOI transistors, we demonstrated ultrahigh sensitive ISFETs. The amplification arises from the strong electrostatic coupling between the front gate and the back gate of the FDSOI, and the asymmetric capacitances of the two gates. A change in voltage at the front gate appears at the back gate as an amplified shift in voltage. The amplification, referred to as the coupling factor (γ), is equal to the ratio of the gate oxide capacitance and the buried oxide (BOX) capacitance. Therefore, functionalizing the pH sensing at the front gate of FDSOI devices, the change in surface potential at the front gate is detected at the back gate amplified by the coupling factor (γ), giving rise to an ultrahigh-sensitive solid state chemical sensor. Integration of the sensing functionality was made in the BEOL which gives the benefits of increased reliability and life time of the sensor, compatibility with the standard CMOS process, and possibility for embedding a capacitive divider circuit. Operation of the MOSFETs without a proper front gate bias makes them vulnerable for undesired floating body effects. The capacitive divider circuit addresses these issues by biasing the front gate simultaneously with the sensing functionality at the same gate through capacitive coupling to a common BEOL metal. Therefore, the potential at the BEOL metal would be a weighted sum of the surface potential at the sensing gate and the applied bias at the control gate. The proposed sensor is modeled and simulated using TCAD-Sentaurus. A complete mathematical model is developed which provides the output of the sensor as a function of the solution pH (input to the sensor), and the design parameters of the capacitive divider circuit and the UTBB FDSOI transistor. In that case, consistent results have been obtained from the modeling and simulation works, with an expected sensitivity of 780 mV/pH corresponding to a sensing film having Nernst response. The modeling and simulation of the proposed sensor was further validated by a proof of concept extended gate pH sensor fabrication and characterization. These sensors were developed by a separated processing of just the pH sensing component, which is electrically connected to the transistor only during characterization of the sensor. This provides faster and simpler realization of the sensor without the need for masks and patterning by lithography. The extended gate sensors showed 475 mV/pH sensitivity which is superior to state of the art low power ISFETs. Finally, integration of the sensing functionality directly in the BEOL of the UTBB FDSOI devices was pursued. An experimental sensitivity of 730 mV/pH is obtained which is consistent with the mathematical model and the simulated response. This is more than 12-times higher than the Nernst limit, and superior to state of the art sensors. Sensors are also evaluated for stability, resolution, hysteresis, and drift in which excellent performances are demonstrated. A novel pH sensing architecture is also successfully demonstrated in which the detection is functionalized at the gate protection diode rather than the front gate of UTBB FDSOI devices. The abrupt current switching, as low as 9 mV/decade, has the potential to increase the fixed bias sensitivity to 6.6 decade/pH. We experimentally demonstrated a sensitivity of 1.25 decade/pH which is superior to the state of the art sensitivity

Insulators for 2D nanoelectronics: the gap to bridge

Nanoelectronic devices based on 2D materials are far from delivering their full theoretical performance potential due to the lack of scalable insulators. Amorphous oxides that work well in silicon technology have ill-defined interfaces with 2D materials and numerous defects, while 2D hexagonal boron nitride does not meet required dielectric specifications. The list of suitable alternative insulators is currently very limited. Thus, a radically different mindset with respect to suitable insulators for 2D technologies may be required. We review possible solution scenarios like the creation of clean interfaces, production of native oxides from 2D semiconductors and more intensive studies on crystalline insulators

Insulators for 2D nanoelectronics: the gap to bridge

Nanoelectronic devices based on 2D materials are far from delivering their full theoretical performance potential due to the lack of scalable insulators. Amorphous oxides that work well in silicon technology have ill-defined interfaces with 2D materials and numerous defects, while 2D hexagonal boron nitride does not meet required dielectric specifications. The list of suitable alternative insulators is currently very limited. Thus, a radically different mindset with respect to suitable insulators for 2D technologies may be required. We review possible solution scenarios like the creation of clean interfaces, production of native oxides from 2D semiconductors and more intensive studies on crystalline insulators

Ferroelectric Field Effect Transistor for Memory and Switch Applications

Silicon technology has advanced at exponential rates both in performances and productivity through the past four decades. However the limit of CMOS technology seems to be closer and closer and in the future we might see an increasing number of hybrid approaches where other technologies add to the CMOS performance, while maintaining a back-bone of CMOS logic. Ferro-electricity in ultra-thin films has been investigated as a credible candidate for nonvolatile memory thanks to the bistability of polarization. 1 transistor (1T) ferroelectric memory cells have been proposed and experimentally studied in order to reduce the size of 1T-1C (1Transistor-1Capacitor) design with consequent advantages in terms of size, read-out operation and costs. More recently ferroelectrics have been proposed by Salahuddin and Datta as dielectric materials in order to lower the 60mV/dec limit of the subthreshold swing (SS) in silicon Metal Oxide Semiconductor Field Effect Transistors, MOSFETs. The objective of this thesis is to study the ferroelectric transistor performance for both memory and switch application. For this purpose different Ferroelectric Field Effect Transistors, Fe-FETs, structures have been designed, fabricated and characterized. An organic ferroelectric polymer, vinylidene fluoride trifluorethylene, P(VDF-TrFE), of 100nm and 40nm thickness has been successfully integrated into the gate stack of bulk and SOI MOSFET and, later, on a Tunnel FET, TFET, structure. The 1T ferroelectric FET memory cells have shown a programming time in the order of ms at 9V as programming voltage. The retention of a few seconds, however, is the main limiting factor for the usage of this device for NV-memory applications. The retention failure mechanisms have been studied and investigated for future improvement. For the first time this work experimentally demonstrates that a subthreshold swing lower than 60mv/dec can be achieved in a ferroelectric transistor thanks to the voltage amplification arising from the ferroelectric material. This unique finding has been first measured in a 40nm P(VDF-TrFE)/10nm SiO2 gate stack MOSFET and then, confirmed, in a 100nm P(VDF-TrFE)/10nm SiO2 gate MOSFET with an intermediate contact between the two dielectrics. This internal node contact allows the study of the voltage amplification due to the ferroelectric material. Finally a temperature study of the performance of a ferroelectric Fully Depleted Silicon on Insulator, FD SOI, transistor has been done. A model based on Landau's theory has been carried out and it has been experimentally validated for both the subthreshold and the strong inversion regions. It has been demonstrated for the first time that, because of the divergence of the ferroelectric permittivity at the Curie temperature, Tc, a ferroelectric transistor has a maximum and a minimum, respectively of its transconductance and subthreshold swing, at Tc

저전력 동작을 위하여 채널에 직각인 터널방향과 수직형 구조를 가지는 터널 전계효과 트랜지스터

학위논문 (박사)-- 서울대학교 대학원 : 전기·컴퓨터공학부, 2016. 8. 박병국.In this work, Tunnel Field-Effect Transistors (TFETs) with a novel structure will be proposed as a substituting devices which can implement steeper switching than the conventional MOSFETs do in low power operation. It is experimentally demonstrated that applying a vertical structure with a perpendicular tunnel to the channel can achieve an operation of high electrical performance and it can be integrated in a bulk Si substrate. First of all, Si and SiGe TFETs with a planar structure are fabricated and measured to extract model parameters. From the measured results, the parameters of band-to-band tunnel (BTBT) model, which can be used to simulate TFETs accurate are calibrated. In this regard, Synopsys Sentaurus Device will be used for this purpose. Then, based on the simulation of planar TFETs, the proposed devices will be presented as the vertical TFETs with the perpendicular tunnel junction based on the bulk Si substrate. The perpendicular tunnel junction and the large tunnel area are employed on the source side to achieve a steep subthreshold swing (SS) and high ON-current (ION), which can lead to TFETs outstanding performance. Moreover, the ION can be increased easily by adjusting a height of overlap region between a source and a gate. Although, the TFETs show good electrical performance, there is a hump phenomenon in transfer curve. In order to suppress the hump phenomenon in the transfer curves, the hump behavior in the proposed device should be investigated. After investigating it, the hump behavior is found to be originated from the two different tunnel regions. Moreover their threshold voltages originated from different tunnel show different values. In order to improve the electrical performance, a capping layer which can be made by gradual doping is inserted on the source. Then, the hump behavior can be expected to decrease. Finally, the proposed TFETs will be fabricated on the bulk Si substrate. A thin intrinsic Si is epitaxially grown on the source region which forms the perpendicular tunnel junction to the channel, resulting in abrupt band bending. The fabricated the proposed TFETs show 17 mV/dec minimum subthreshold swing (SS) and 104 ON/OFF current ratio (ION/IOFF ) for sub-0.7 V gate overdrive. In addition, SS is maintained less than 60 mV/dec while a drain current increases from complete OFF-state (10−13) to more than two orders of magnitude (10−11). In conclusion, the proposed device are fabricated successfully. From this study, it is demonstrated that the proposed TFETs will be one of the most promising candidate for a next-generation low-power device.Chapter 1 Introduction 1 1.1 Power issues on CMOS technologies 1 1.2 Tunnel Field Effect Transistors 3 1.3 Issue for TFETs 6 1.4 Propose of the Target Device 8 1.5 Thesis outline 10 Chapter 2 Planar Si & SiGe TFET 12 2.1 Device fabrication 12 2.2 Measured Results 14 2.3 BTBT model calibrations 17 2.4 Summary 19 2.5 Appendix: Process Flow 19 Chapter 3 Simulation of the Proposed TFETs 24 3.1 Introduction 25 3.2 Device structure and Fabrication Method 25 3.3 Simulation Results and Discussion 27 3.4 Summary of Simulation 34 Chapter 4 Fabrication of the Proposed TFETs 36 4.1 Introduction 37 4.2 Device Structure and Fabrication Method 37 4.3 Experimental results 47 4.4 Discussion 52 4.4.1 High OFF leakage current 52 4.4.2 Short channel effect 54 4.4.3 Current Saturation by Drain 56 4.4.4 Process Optimization 59 4.5 Summary 61 4.6 Appendix: Process Flow 61 Chapter 5 Conclusion 68 5.1 Summary of Contributions 68 5.2 Future works for TFETs Design 69 Chapter 6 Appendix 71 6.1 Super-linear onset in TFETs 71 6.2 Introduction 72 6.3 Device Structure 72 6.4 Simulation Results 73 6.5 Drain Threshold Voltage 79 6.6 Tunnel Resistance 80 6.7 Conclusion 86 Bibliography 88 초록 95Docto

Electrical Characterisation of III-V Nanowire MOSFETs

The ever increasing demand for faster and more energy-efficient electricalcomputation and communication presents severe challenges for the semiconductor industry and particularly for the metal-oxidesemiconductorfield-effect transistor (MOSFET), which is the workhorse of modern electronics. III-V materials exhibit higher carrier mobilities than the most commonly used MOSFET material Si so that the realisation of III-V MOSFETs can enable higher operation speeds and lower drive voltages than that which is possible in Si electronics. A lowering of the transistor drive voltage can be further facilitated by employing gate-all-around nanowire geometries or novel operation principles. However, III-V materials bring about their own challenges related to material quality and to the quality of the gate oxide on top of a III-V MOSFET channel.This thesis presents detailed electrical characterisations of two types of (vertical) III-V nanowire transistors: MOSFETs based on conventional thermionic emission; and Tunnel FETs, which utilise quantum-mechanical tunnelling instead to control the device current and reach inverse subthreshold slopes below the thermal limit of 60 mV/decade. Transistor characterisations span over fourteen orders of magnitude in frequency/time constants and temperatures from 11 K to 370 K.The first part of the thesis focusses on the characterisation of electrically active material defects (‘traps’) related to the gate stack. Low-frequency noise measurements yielded border trap densities of 10^18 to 10^20 cm^-3 eV^-1 and hysteresis measurements yielded effective trap densities – projected to theoxide/semiconductor interface – of 2x10^12 to 3x10^13 cm^-2 eV^-1. Random telegraph noise measurements revealed that individual oxide traps can locally shift the channel energy bands by a few millielectronvolts and that such defects can be located at energies from inside the semiconductor band gap all the way into the conduction band.Small-signal radio frequency (RF) measurements revealed that parts of the wide oxide trap distribution can still interact with carriers in the MOSFET channel at gigahertz frequencies. This causes frequency hystereses in the small-signal transconductance and capacitances and can decrease the RF gains by a few decibels. A comprehensive small-signal model was developed, which takes into account these dispersions, and the model was applied to guide improvements of the physical structure of vertical RF MOSFETs. This resulted in values for the cutoff frequency fT and the maximum oscillation frequency fmax of about 150 GHz in vertical III-V nanowire MOSFETs.Bias temperature instability measurements and the integration of (lateral) III-V nanowire MOSFETs in a back end of line process were carried out as complements to the main focus of this thesis. The results of this thesis provide a broad perspective of the properties of gate oxide traps and of the RF performance of III-V nanowire transistors and can act as guidelines for further improvement and finally the integration of III-V nanowire MOSFETs in circuits

Tunnel Field Effect Transistors:from Steep-Slope Electronic Switches to Energy Efficient Logic Applications

The aim of this work has been the investigation of homo-junction Tunnel Field Effect Transistors starting from a compact modelling perspective to its possible applications. Firstly a TCAD based simulation study is done to explain the main device characteristics. The main differences of a Tunnel FET with respect to a conventional MOSFET is pointed out and the differences have been explained. A compact DC/AC model has been developed which is capable of describing the I-V characteristics in all regimes of operation. The model takes in to account ambi-polarity, drain side breakdown and all tunneling related physics. A temperature dependence is also added to the model to study the temperature independent behavior of tunneling. The model was further implemented in a Verilog-A based circuit simulator. Following calibration to experimental results of Silicon and strained-Silicon TFETs, the model has been also used to benchmark against a standard CMOS node for digital and analog applications. The circuits built with Tunnel FETs showed interesting temperature behavior which was superior to the compared CMOS node. In the same work, we also explore and propose solutions for using TFETs for low power memory applications. Both volatile and non-volatile memory concepts are investigated and explored. The application of a Tunnel FET as a capacitor-less memory has been experimentally demonstrated for the first time. New device concepts have been proposed and process flows for the same are developed to realize them in the clean room in EPFL