208 research outputs found

    Current transport modeling of carbon nanotube field effect transistors for analysis and design of integrated circuits

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    The purpose of this study was to develop a complete current transport model for carbon nanotube field effect transistors (CNT-FETs) applicable in the analysis and design of integrated circuits. The model was derived by investigating the electronic structure of carbon nanotubes and using basic laws of electrostatics describing a field effect transistor. We first derived analytical expressions for the carrier concentration in carbon nanotubes for different chiral vectors (n,m) by studying and characterizing their electronic structure. Results showed a strong relation to the diameter and wrapping angle of carbon nanotubes. The charge distribution in a CNT-FET is characterized from the charge neutrality and potential balance conditions. Mathematical techniques are used to derive analytically approximated equations describing the carbon nanotube potential in terms of the terminal voltages. These equations are validated by comparing them with the respective numerical solutions; furthermore, the expressions for the carbon nanotube potential are used to derive current transport equations for normal and subthreshold operations. Threshold and saturation voltages expressions are each derived in the process and the I-V characteristics for CNT-FETs are calculated using different combinations of chiral vectors. Results showed a strong dependence of the I-V characteristics on the wrapping angle and diameter of carbon nanotubes, as expected from the carrier concentration modeling. Results were also compared with available experimental data showing close agreement within the limitations and approximations used in the analysis. In addition, the current model equations were used to generate the voltage transfer characteristics for basic logic circuits based on complementary CNT-FETs. The voltage transfer characteristics exhibit characteristics similar to the voltage transfer characteristics of standard CMOS logic devices, with a sharp transition near the logic threshold voltage depending on the input conditions. A small-signal radio frequency (rf) model was also developed and it is shown to have cut-off frequencies in the upper GHz range with a strong dependence on the chiral vector and corresponding transconductance (gm). Finally, due to the rapid growth of carbon nanotubes as bio- and chemical sensing devices, we have also presented, using our current model equations, possible methods to interpret and analyze CNT-FETs when utilized as biosensors

    Carbon Nanotube Interconnect Modeling for Very Large Scale Integrated Circuits

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    In this research, we have studied and analyzed the physical and electrical properties of carbon nanotubes. Based on the reported models for current transport behavior in non-ballistic CNT-FETs, we have built a dynamic model for non-ballistic CNT-FETs. We have also extended the surface potential model of a non-ballistic CNT-FET to a ballistic CNT-FET and developed a current transport model for ballistic CNT-FETs. We have studied the current transport in metallic carbon nanotubes. By considering the electron-electron interactions, we have modified two-dimensional fluid model for electron transport to build a semi-classical one-dimensional fluid model to describe the electron transport in carbon nanotubes, which is regarded as one-dimensional system. Besides its accuracy compared with two-dimensional fluid model and Lรผttinger liquid theory, one-dimensional fluid model is simple in mathematical modeling and easier to extend for electronic transport modeling of multi-walled carbon nanotubes and single-walled carbon nanotube bundles as interconnections. Based on our reported one-dimensional fluid model, we have calculated the parameters of the transmission line model for the interconnection wires made of single-walled carbon nanotube, multi-walled carbon nanotube and single-walled carbon nanotube bundle. The parameters calculated from these models show close agreements with experiments and other proposed models. We have also implemented these models to study carbon nanotube for on-chip wire inductors and it application in design of LC voltage-controlled oscillators. By using these CNT-FET models and CNT interconnects models, we have studied the behavior of CNT based integrated circuits, such as the inverter, ring oscillator, energy recovery logic; and faults in CNT based circuits

    A Three-dimensional simulation study of the performance of Carbon Nanotube Field Effect Transistors with doped reservoirs and realistic geometry

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    In this work, we simulate the expected device performance and the scaling perspectives of Carbon nanotube Field Effect Transistors (CNT-FETs), with doped source and drain extensions. The simulations are based on the self-consistent solution of the 3D Poisson-Schroedinger equation with open boundary conditions, within the Non-Equilibrium Green's Function formalism, where arbitrary gate geometry and device architecture can be considered. The investigation of short channel effects for different gate configurations and geometry parameters shows that double gate devices offer quasi ideal subthreshold slope and DIBL without extremely thin gate dielectrics. Exploration of devices with parallel CNTs show that On currents per unit width can be significantly larger than the silicon counterpart, while high-frequency performance is very promising.Comment: Submitted to IEEE TE

    ์‹ ์ถ•์„ฑ ์žˆ๊ณ  ์ฐฉ์šฉ ๊ฐ€๋Šฅํ•œ ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ ๊ธฐ๋ฐ˜ ์ „์ž ๊ธฐ์ˆ 

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ํ˜‘๋™๊ณผ์ • ๋ฐ”์ด์˜ค์—”์ง€๋‹ˆ์–ด๋ง์ „๊ณต, 2020. 8. ๊น€๋Œ€ํ˜•.Networks of carbon nanotubes (CNTs) are a promising candidate for use as a basic building block for next-generation soft electronics, owing to their superior mechanical and electrical properties, chemical stability, and low production cost. In particular, the CNTs, which are produced as a mixture of metallic and semiconducting CNTs via chemical vapor deposition, can be sorted according to their electronic types, which makes them useful for specific purposes: semiconducting CNTs can be employed as channel materials in transistor-based applications and metallic CNTs as electrodes. However, the development of CNT-based electronics for soft applications is still at its infant stage, mainly limited by the lack of solid technologies for developing high-performance deformable devices whose electrical performances are comparable to those fabricated using conventional inorganic materials. In this regard, soft CNT electronics with high mechanical stability and electrical performances have been pursued. First, wearable nonvolatile memory modules and logic gates were fabricated by employing networks of semiconducting CNTs as the channel materials, with strain-tolerant device designs for high mechanical stability. The fabricated devices exhibited low operation voltages, high device-to-device uniformity, on/off ratios, and on-current density, while maintaining its performance during ~30% stretching after being mounted on the human skin. In addition, various functional logic gates verified the fidelity of the reported technology, and successful fabrication of non-volatile memory modules with wearable features has been reported for the first time at the time of publication. Second, the networks of semiconducting CNTs were used to fabricate signal amplifiers with a high gain of ~80, which were then used to amplify electrocardiogram (ECG) signals measured using a wearable sensor. At the same time, color-tunable organic light-emitting diodes (CTOLEDs) were developed based on ultra-thin charge blocking layer that controlled the flow of excitons during different voltage regimes. Together, they were integrated to construct a health monitoring platform whereby real-time ECG signals could be detected while simultaneously notifying its user of the ECG status via color changes of the wearable CTOLEDs. Third, intrinsically stretchable CNT transistors were developed, which was enabled by the developments of thickness controllable, vacuum-deposited stretchable dielectric layer and vacuum-deposited metal thin films. Previous works employed strain-tolerant device designs which are based on the use of filamentary serpentine-shaped interconnections, which severely sacrifice the device density. The developed stretchable dielectric, compatible with the current vacuum-based microfabrication technology, exhibited excellent insulating properties even for nanometer-range thicknesses, thereby enabling significant electrical performance improvements such as low operation voltage and high device uniformity/reproducibility, which has not been realized in the most advanced intrinsically stretchable transistors of today.ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ๋Š” ๋›ฐ์–ด๋‚œ ์ „๊ธฐ์ , ํ™”ํ•™์ , ๊ทธ๋ฆฌ๊ณ  ๊ธฐ๊ณ„์  ํŠน์„ฑ์„ ๊ฐ–๊ณ  ์žˆ์–ด ์ฐจ์„ธ๋Œ€ ์œ ์—ฐ ์ „์ž์†Œ์ž์˜ ํ•ต์‹ฌ ์†Œ์žฌ ์ค‘ ํ•˜๋‚˜๋กœ ๊ฐ๊ด‘์„ ๋ฐ›๊ณ  ์žˆ์œผ๋‚˜, ์•„์ง๊นŒ์ง€ ์ด๋ฅผ ์ด์šฉํ•œ ์‹ค์šฉ์ ์ธ ์œ ์—ฐ ์ „์ž์†Œ์ž์˜ ๊ฐœ๋ฐœ์€ ์‹คํ˜„๋˜์ง€ ์•Š๊ณ  ์žˆ๋‹ค. ์ด๋Š” ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ์˜ ์ „๊ธฐ์  ํŠน์„ฑ๋Œ€๋กœ ์™„๋ฒฝํžˆ ๋ถ„๋ฅ˜ํ•ด ๋‚ผ ์ˆ˜ ์žˆ๋Š” ๊ธฐ์ˆ , ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ๋ฅผ ์†Œ์ž์˜ ์›ํ•˜๋Š” ์œ„์น˜์— ์ •ํ™•ํžˆ ์›ํ•˜๋Š” ์–‘๋งŒํผ ๋„คํŠธ์›Œํฌ ํ˜•ํƒœ ํ˜น์€ ์ •๋ ฌ๋œ ํ˜•ํƒœ๋กœ ์ฆ์ฐฉํ•˜๋Š” ๊ธฐ์ˆ , ๊ทธ๋ฆฌ๊ณ  ์œ ์—ฐ ์ „์ž์†Œ์ž๋ฅผ ๊ตฌ์„ฑํ•˜๋Š” ๋‹ค๋ฅธ ๋ฌผ์งˆ๋“ค์˜ ๊ฐœ๋ฐœ ๊ธฐ์ˆ ์˜ ๋ถ€์žฌ ๋•Œ๋ฌธ์ด๋‹ค. ์ง€๋‚œ 10์—ฌ๋…„๊ฐ„ ํ•ด๋‹น ๊ธฐ์ˆ ๋“ค์€ ๊ด‘๋ฒ”์œ„ํ•˜๊ฒŒ ์—ฐ๊ตฌ๋˜์–ด์ง€๊ณ  ์žˆ์œผ๋‚˜, ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ๋ฅผ ํ™œ์šฉํ•œ ์šฐ์ˆ˜ํ•œ ์œ ์—ฐ ์ „์ž์†Œ์ž ๊ฐœ๋ฐœ์„ ์œ„ํ•œ ํ•ต์‹ฌ ๊ธฐ์ˆ ๋“ค์˜ ๋ฐœ์ „์€ ์•„์ง ์ดˆ๊ธฐ ๋‹จ๊ณ„์— ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ์ด ๋…ผ๋ฌธ์„ ํ†ตํ•ด ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ๋ฅผ ์œ ์—ฐ ์ „์ž์†Œ์ž์— ์ ์šฉ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ์ƒˆ๋กœ์šด ๊ธฐ์ˆ ์„ ์†Œ๊ฐœํ•˜๊ณ ์ž ํ•œ๋‹ค. ์ฒซ๋ฒˆ์งธ๋กœ ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ์™€ ์œ ์—ฐ ์ „์ž์†Œ์ž์˜ ์†Œ์ž ๋””์ž์ธ์„ ์ด์šฉํ•˜์—ฌ ํ”ผ๋ถ€์œ„์— ์ฆ์ฐฉ ๊ฐ€๋Šฅํ•œ ๋น„ํœ˜๋ฐœ์„ฑ ๋ฉ”๋ชจ๋ฆฌ ์†Œ์ž๋ฅผ ์ œ์ž‘ํ•˜์˜€๊ณ , ํ•ด๋‹น ๊ธฐ์ˆ ์„ ์ด์šฉํ•˜์—ฌ ํ”ผ๋ถ€์œ„์—์„œ ์•ˆ์ „ํ•˜๊ฒŒ ๋™์ž‘ํ•  ์ˆ˜ ์žˆ๋Š” ๋‹ค์–‘ํ•œ ๊ธฐ์ดˆ ํšŒ๋กœ๋“ค์„ ๊ตฌํ˜„ํ•˜์˜€๋‹ค. ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ ๊ธฐ๋ฐ˜ ๋ฉ”๋ชจ๋ฆฌ ์ „์ž ์†Œ์ž ๋ฐ ํšŒ๋กœ๋Š” ๋‹ค์–‘ํ•œ ์™ธ๋ถ€ ์‘๋ ฅ์ด ๊ฐ€ํ•ด์ ธ๋„ ์•ˆ์ •์ ์œผ๋กœ ๋™์ž‘์„ ํ•˜์˜€๊ณ , ๊ฐœ๋ฐœ๋œ ๊ธฐ์ˆ ์„ ํ†ตํ•ด ๋ณด๋‹ค ์‹ค์šฉ์ ์ธ ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ ๊ธฐ๋ฐ˜ ์œ ์—ฐ ์ „์ž ์†Œ์ž์˜ ์ œ์ž‘ ์กฐ๊ฑด์„ ํ™•๋ฆฝํ•  ์ˆ˜ ์žˆ์—ˆ๋‹ค. ๋‘๋ฒˆ์งธ๋กœ ์œ„์— ๊ฐœ๋ฐœ๋œ ๊ธฐ์ˆ ์„ ๋ฐ”ํƒ•์œผ๋กœ, ๋ณด๋‹ค ๋ณต์žกํ•œ ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ ๊ธฐ๋ฐ˜ ์œ ์—ฐ ํšŒ๋กœ ๋ฐ ๊ตฌ๋™์ „์••์— ๋”ฐ๋ผ ๋ฐœ๊ด‘์ƒ‰์ด ๋ณ€ํ™˜ํ•˜๋Š” ์ƒ‰๋ณ€ํ™˜ ์†Œ์ž๋ฅผ ์ œ์ž‘ํ•˜์—ฌ ํ•ด๋‹น ์†Œ์ž๋“ค์ด ํ”ผ๋ถ€์œ„์— ๋ถ€์ฐฉ๋˜์–ด ์ž˜ ์ž‘๋™๋˜๋„๋ก ๊ตฌํ˜„ํ•˜์˜€๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์ด ๋‘ ๊ฐ€์ง€ ์›จ์–ด๋Ÿฌ๋ธ” ์ „์ž์†Œ์ž๋ฅผ ํ†ตํ•ฉํ•˜์—ฌ ์‹ค์‹œ๊ฐ„์œผ๋กœ ์‹ฌ์ „๋„๋ฅผ ์ธก์ •ํ•˜์—ฌ ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ ๊ธฐ๋ฐ˜ ์ „์ž์†Œ์ž๋ฅผ ํ†ตํ•ด ํ•ด๋‹น ์‹ ํ˜ธ๋ฅผ ์ฆํญ์‹œํ‚ค๊ณ , ์‹ ํ˜ธ์˜ ์ƒํƒœ๋ฅผ ์ƒ‰๋ณ€ํ™˜ ์†Œ์ž๋กœ ๋‚˜ํƒ€๋‚ผ ์ˆ˜ ์žˆ๋Š” ์‹ฌ์ „๋„ ๋ชจ๋‹ˆํ„ฐ ์‹œ์Šคํ…œ์„ ๊ตฌํ˜„ํ•˜์˜€๋‹ค. ์„ธ๋ฒˆ์งธ๋กœ ์ง„๊ณต ์ฆ์ฐฉ์ด ๊ฐ€๋Šฅํ•œ ์œ ์—ฐ ์ ˆ์—ฐ์ฒด๋ฅผ ๊ฐœ๋ฐœํ•˜์—ฌ, ๊ธฐ์กด์˜ ์œ ์—ฐ ์ „์ž์†Œ์ž๋“ค์ด ๊ฐ€์ง€๊ณ  ์žˆ๋˜ ๊ทน๋ช…ํ•œ ํ•œ๊ณ„๋ฅผ ๊ทน๋ณตํ•˜์˜€๋‹ค (๋†’์€ ๊ตฌ๋™ ์ „์••, ๋‚ฎ์€ ์ง‘์ ๋„, ๋Œ€๋ฉด์  ์†Œ์ž ์„ ๋Šฅ ๊ท ์ผ๋„ ๋“ฑ). ๊ธฐ์กด์˜ ์•ก์ƒ ๊ธฐ๋ฐ˜ ์ฆ์ฐฉ์„ ์œ„์ฃผ๋กœ ํ•œ ์œ ์—ฐ ์ „์ž ์†Œ์ž๋“ค์€ ๋ฌด๊ธฐ๋ฌผ์งˆ ๊ธฐ๋ฐ˜ ์ „์ž์†Œ์ž ๋Œ€๋น„ ๊ทน์‹ฌํ•œ ์„ฑ๋Šฅ ์ €ํ•˜๋ฅผ ๋ณด์—ฌ์ฃผ์—ˆ๋Š”๋ฐ, ์ด๋ฅผ ํ•ด๊ฒฐํ•˜๊ธฐ ์œ„ํ•ด ์ƒˆ๋กœ์šด ์ ˆ์—ฐ๋ฌผ์งˆ์„ ๊ฐœ๋ฐœํ•˜๊ณ  ํƒ„์†Œ ๋‚˜๋…ธํŠœ๋ธŒ ๊ธฐ๋ฐ˜ ์œ ์—ฐ ์ „์ž์†Œ์ž์— ์ ์šฉํ•˜์—ฌ ๊ทธ ๊ฐ€๋Šฅ์„ฑ์„ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค.Chapter 1. Introduction 1 1.1 Discovery of CNTs and their benefits for soft electronic applications 1 1.2 Electrical sorting of CNTs 5 1.3 Deposition methods of solution-processed semiconducting CNTs 7 1.4 Conclusion 23 1.5 References 24 Chapter 2. Stretchable Carbon Nanotube Charge-Trap Floating-Gate Memory and Logic Devices for Wearable Electronics 32 2.1 Introduction 32 2.2 Experimental section 34 2.3 Results and discussion 36 2.4 Conclusion 62 2.5 References 63 Chapter 3. Wearable Electrocardiogram Monitor Using Carbon Nanotube Electronics and Color-Tunable Organic Light-Emitting Diodes 67 3.1 Introduction 67 3.2 Experimental section 70 3.3 Results and discussion 73 3.4 Conclusion 97 3.5 References 98 Chapter 4. Medium-Scale Electronic Skin Based on Carbon Nanotube Transistors with Vacuum-Deposited Stretchable Dielectric Film 102 4.1 Introduction 102 4.2 Experimental section 106 4.3 Result and discussion 111 4.4 Conclusion 135 4.5 References 136Docto

    Silicene Nanomesh

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    Similar to graphene, zero band gap limits the application of silicene in nanoelectronics despite of its high carrier mobility. By using first-principles calculations, we reveal that a band gap is opened in silicene nanomesh (SNM) when the width W of the wall between the neighboring holes is even. The size of the band gap increases with the reduced W and has a simple relation with the ratio of the removed Si atom and the total Si atom numbers of silicene. Quantum transport simulation reveals that the sub-10 nm single-gated SNM field effect transistors show excellent performance at zero temperature but such a performance is greatly degraded at room temperature

    Imperfection-Aware Design of CNFET Digital VLSI Circuits

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    Carbon nanotube field-effect transistor (CNFET) is one of the promising candidates as extensions to silicon CMOS devices. The CNFET, which is a 1-D structure with a near-ballistic transport capability, can potentially offer excellent device characteristics and order-of-magnitude better energy-delay product over standard CMOS devices. Significant challenges in CNT synthesis prevent CNFETs today from achieving such ideal benefits. CNT density variation and metallic CNTs are the dominant type of CNT variations/imperfections that cause performance variation, large static power consumption, and yield degradation. We present an imperfection-aware design technique for CNFET digital VLSI circuits by: 1) Analytical models that are developed to analyze and quantify the effects of CNT density variation on device characteristics, gate and system levels delays. The analytical models, which were validated by comparison to real experimental/simulation data, enables us to examine the space of CNFET combinational, sequential and memory cells circuits to minimize delay variations. Using these model, we drive CNFET processing and circuit design guidelines to manage/overcome CNT density variation. 2) Analytical models that are developed to analyze the effects of metallic CNTs on device characteristics, gate and system levels delay and power consumption. Using our presented analytical models, which are again validated by comparison with simulation data, it is shown that the static power dissipation is a more critical issue than the delay and the dynamic power of CNFET circuits in the presence of m-CNTs. 3) CNT density variation and metallic CNTs can result in functional failure of CNFET circuits. The complete and compact model for CNFET probability of failure that consider CNT density variation and m-CNTs is presented. This analytical model is applied to analyze the logical functional failures. The presented model is extended to predict opportunities and limitations of CNFET technology at todays Gigascale integration and beyond.\u2

    Modeling of Nano-Transistor Using 14-Nm Technology Node

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    Latest process technologies in transistor development demonstrate massive changes in the size of transistor chip. In this chapter, a 14-nm technology node is used to model nanosize transistor. The 14-nm technology node consists of multiple numbers of carbon nanotube. Carbon nanotube is a very good energy efficient and low-cost material. Carbon nanotube demonstrates excellent characteristics in metallic and semiconducting characteristics by analyzing electrical properties. At first, the nanotube device physics and material properties are briefly explained in this chapter. Further, a nanotube device is designed for semiconducting properties. The gate length of nanotube is 14ย nm which is placed on the gate channel. Finally, the model of 14-nm nano-transistor will be demonstrated for low-energy consumption which can be considered as a better replacement of CMOS
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