322 research outputs found

    Hybrid CMOS/memristor circuits

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    Abstract โ€” This is a brief review of recent work on the prospective hybrid CMOS/memristor circuits. Such hybrids combine the flexibility, reliability and high functionality of the CMOS subsystem with very high density of nanoscale thin film resistance switching devices operating on different physical principles. Simulation and initial experimental results demonstrate that performance of CMOS/memristor circuits for several important applications is well beyond scaling limits of conventional VLSI paradigm. I

    Redox-Active Molecules for Novel Nonvolatile Memory Applications

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    The continuous complementary metalโ€oxideโ€semiconductor (CMOS) scaling is reaching fundamental limits imposed by the heat dissipation and shortโ€channel effects, which will finally stop the increase of integration density and the MOSFET performance predicted by Mooreโ€™s law. Molecular technology has been aggressively pursued for decades due to its potential impact on future microโ€/nanoelectronics. Molecules, especially redoxโ€active molecules, have become attractive due to their intrinsic redox behavior, which provides an excellent basis for lowโ€power, highโ€density, and highโ€reliability nonvolatile memory applications. This chapter briefly reviews the development of molecular electronics in the application of nonvolatile memory. From the mechanical motion of molecules in the Langmuirโ€Blodgett film to new families of redoxโ€active molecules, memory devices involving hybrid molecular technology have shown advantageous potential in fast speed, lowโ€power, and highโ€density nonvolatile memory and will lead to promising onโ€chip memory as well as future portable electronics applications

    Integration of Ferroelectric HfO2 onto a III-V Nanowire Platform

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    The discovery of ferroelectricity in CMOS-compatible oxides, such as doped hafnium oxide, has opened new possibilities for electronics by reviving the use of ferroelectric implementations on modern technology platforms. This thesis presents the ground-up integration of ferroelectric HfO2 on a thermally sensitive III-V nanowire platform leading to the successful implementation of ferroelectric transistors (FeFETs), tunnel junctions (FTJs), and varactors for mm-wave applications. As ferroelectric HfO2 on III-V semiconductors is a nascent technology, a special emphasis is put on the fundamental integration issues and the various engineering challenges facing the technology.The fabrication of metal-oxide-semiconductor (MOS) capacitors is treated as well as the measurement methods developed to investigate the interfacial quality to the narrow bandgap III-V materials using both electrical and operando synchrotron light source techniques. After optimizing both the films and the top electrode, the gate stack is integrated onto vertical InAs nanowires on Si in order to successfully implement FeFETs. Their performance and reliability can be explained from the deeper physical understanding obtained from the capacitor structures.By introducing an InAs/(In)GaAsSb/GaSb heterostructure in the nanowire, a ferroelectric tunnel field effect transistor (ferro-TFET) is fabricated. Based on the ultra-short effective channel created by the band-to-band tunneling process, the localized potential variations induced by single ultra-scaled ferroelectric domains and individual defects are sensed and investigated. By intentionally introducing a gate-source overlap in the ferro-TFET, a non-volatile reconfigurable single-transistor solution for modulating an input signal with diverse modes including signal transmission, phase shift, frequency doubling, and mixing is implemented.Finally, by fabricating scaled ferroelectric MOS capacitors in the front-end with a dedicated and adopted RF and mm-wave backend-of-line (BEOL) implementation, the ferroelectric behavior is captured at RF and mm-wave frequencies

    Reconfigurable Multifunctional van der Waals Ferroelectric Devices and Logic Circuits

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    In this work, we demonstrate the suitability of Reconfigurable Ferroelectric Field-Effect- Transistors (Re-FeFET) for designing non-volatile reconfigurable logic-in-memory circuits with multifunctional capabilities. Modulation of the energy landscape within a homojunction of a 2D tungsten diselenide (WSe2_2) layer is achieved by independently controlling two split-gate electrodes made of a ferroelectric 2D copper indium thiophosphate (CuInP2_2S6_6) layer. Controlling the state encoded in the Program Gate enables switching between p, n and ambipolar FeFET operating modes. The transistors exhibit on-off ratios exceeding 106^6 and hysteresis windows of up to 10 V width. The homojunction can change from ohmic-like to diode behavior, with a large rectification ratio of 104^4. When programmed in the diode mode, the large built-in p-n junction electric field enables efficient separation of photogenerated carriers, making the device attractive for energy harvesting applications. The implementation of the Re-FeFET for reconfigurable logic functions shows how a circuit can be reconfigured to emulate either polymorphic ferroelectric NAND/AND logic-in-memory or electronic XNOR logic with long retention time exceeding 104^4 seconds. We also illustrate how a circuit design made of just two Re-FeFETs exhibits high logic expressivity with reconfigurability at runtime to implement several key non-volatile 2-input logic functions. Moreover, the Re-FeFET circuit demonstrates remarkable compactness, with an up to 80% reduction in transistor count compared to standard CMOS design. The 2D van de Waals Re-FeFET devices therefore exhibit groundbreaking potential for both More-than-Moore and beyond-Moore future of electronics, in particular for an energy-efficient implementation of in-memory computing and machine learning hardware, due to their multifunctionality and design compactness.Comment: 23 pages, 5 figures; Supporting Information: 12 pages, 6 figure

    Planar Electrostatically Doped Reconfigurable Schottky Barrier FDSOI Field-Effect Transistor Structures

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    In the last 50 years, our economy and society have obviously been influenced and shaped to a great extent by electronic devices. This substantial impact of electronics is the result of a continuous performance improvement based on the scaling, i.e. shrinking, of MOSFET devices in complementary integrated circuits, following Moore's law. As the MOSFET feature sizes are approaching atomistic dimensions, the scaling trend slowed down considerably and is even threatened for sub-10 nm technology nodes. Further, additional advancements are increasingly difficult to realize both from the technological and especially the economical perspective. Therefore, technologies that have the potential to supersede the CMOS technology in the future are the topic of intensive investigation by both researchers and the industry. An attractive solution is the leveraging of existing semiconductor technologies based on emerging research devices (ERD) offering novel characteristics, which enable new circuit architectures in future nanoscale logic circuits. A possible ERD contender are polarity controllable or reconfigurable MOSFET (RFET) concepts. Generally, RFET devices are able to switch between n- and p-type conduction by the application of an electrical signal. Therefore, RFET promise increased complex systems with a lower device count decreasing the costs per basic logic function based on their higher logic expressiveness. The focus of this work lies in the successful transfer of a predecessor silicon nanowire (NW) RFET technology into a planar RFET device, while simultaneously optimizing the resulting RFET for reconfigurable as well as conventional CMOS circuits. As for the predecessor NW RFET, the planar approach features a doping-less CMOS compatible fabrication process on a conventional SOI substrate and obtains its reconfigurability by electrostatic doping. The device can be regarded as a entanglement of two MOSFET in one structure, i.e. a depletion mode FET centered on top of a backside enhancement mode Schottky barrier FET (SBFET). The backside SBFET establishes the conductive channel consisting of the desired charge carrier type via an appropriate potential on its gate electrode. The topside FET controls the charge carrier flow between source and drain by locally depleting this channel given an opposite potential on its gate electrode with respect to the backside gate electrode. Two generations of devices have been successfully processed, while different gate electrode materials, i.e. nickel, aluminum and reactively sputtered tungsten-titanium-nitride, have been introduced to the device structure. As n- and p-type symmetry of the very same device is essential for RFET circuit design, tungsten-titanium-nitride is experimentally identified as a possible mid-gap metal gate electrode for RFET devices. Also, a Schottky barrier adjustment process for ideal n- and p-type symmetry based on silicide induced dopant segregation is experimentally demonstrated. Extensive electrical characterizations supported by calibrated TCAD simulations are presented, demonstrating experimental sub-threshold slopes of 65 mV/dec and on-to-off current ratios of over 9 decades. Based on TCAD simulations and supported by experimental results, the design space of the device concept is explored in order to gather predictive results for future scaled device optimization. Further, the high temperature (HT) performance is evaluated and compared to the predecessor NW RFET devices as well as to a state-of-the-art industrial high reliability HT MOSFET clearly illustrating the on par performance of the planar RFET concept with respect to off-state leakage current

    ํ”„๋กœ๊ทธ๋žจ ๊ฐ€๋Šฅํ•œ ํ•˜๋ถ€ ์ „๊ทน ์–ด๋ ˆ์ด ๊ตฌ์กฐ๋ฅผ ๊ฐ–๋Š” ๊ณ ํšจ์œจ ์žฌ๊ตฌ์„ฑ ๊ฐ€๋Šฅ ์†Œ์ž

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2016. 8. ์ด์ข…ํ˜ธ.๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ๋น„ ํœ˜๋ฐœ์„ฑ ๋ฉ”๋ชจ๋ฆฌ (NVM) ๊ธฐ๋Šฅ์„ ๊ฐ–๋Š” ํ”„๋กœ๊ทธ๋žจ ๊ฐ€๋Šฅํ•œ ํ•˜๋ถ€ ์ „๊ทน ์–ด๋ ˆ์ด (Bottom gate array) ๋กœ ๊ตฌ์„ฑ๋œ ์ƒˆ๋กœ์šด ํด๋ฆฌ ์‹ค๋ฆฌ์ฝ˜ ์žฌ๊ตฌ์„ฑ ๊ฐ€๋Šฅ ์†Œ์ž๋ฅผ ์ตœ์ดˆ๋กœ ๊ณ ์•ˆํ•˜๊ณ  ์ œ์ž‘ ๋ฐ ๋ถ„์„ํ•˜์˜€๋‹ค. ์ œ์•ˆ๋œ ์†Œ์ž๋Š” ์†Œ์ž์˜ ํฌ๊ธฐ, ์‹ ๋ขฐ์„ฑ, ๊ท ์ผ์„ฑ ๋ฐ ์žฌํ˜„์„ฑ ์ธก๋ฉด์—์„œ ๋งค์šฐ ํšจ์œจ์ ์ด๋‹ค. ํ•˜๋ถ€ ์ „๊ทน ์–ด๋ ˆ์ด์— ์ง์ ‘ ๋ฐ”์ด์–ด์Šค๋ฅผ ์ธ๊ฐ€ํ•˜๊ฑฐ๋‚˜, ๋˜๋Š” ํ•˜๋ถ€ ์ „๊ทน์˜ ํ”„๋กœ๊ทธ๋žจ/์ด๋ ˆ์ด์ฆˆ ์ƒํƒœ๋ฅผ ๋ณ€ํ™” ์‹œํ‚ด์œผ๋กœ์จ, ์ œ์•ˆ๋œ ์žฌ๊ตฌ์„ฑ๊ฐ€๋Šฅ ์†Œ์ž๋Š” n-/p-MOSFET, n-p/p-n ๋‹ค์ด์˜ค๋“œ ์ค‘ ํ•˜๋‚˜์˜ ํ˜•ํƒœ๋กœ ๋™์ž‘ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ, ์†Œ์ž์˜ MOSFET ๋™์ž‘์—์„œ, ๋ฌธํ„ฑ ์ „์•• (Vth)๊ณผ ์ ‘ํ•ฉ ์ €ํ•ญ (RC)์€ ํ•˜๋ถ€ ์ „๊ทน์— ์˜ํ•ด ๋…๋ฆฝ์ ์œผ๋กœ ์ œ์–ด ๊ฐ€๋Šฅํ•˜๋ฉฐ ์ด๋Š” ์ œ์•ˆ๋œ ์žฌ๊ตฌ์„ฑ ๊ฐ€๋Šฅ ์†Œ์ž์˜ ๊ณ ์œ ํ•œ ์žฅ์ ์ด๋‹ค. ์ œ์ž‘๋œ ์†Œ์ž๋Š” n-/p-MOSFET ๋™์ž‘์—์„œ ๊ธฐ์กด์˜ ํด๋ฆฌ ์‹ค๋ฆฌ์ฝ˜ ์ฑ„๋„ ๊ธฐ๋ฐ˜ ์†Œ์ž๋“ค๊ณผ ์œ ์‚ฌํ•œ ์•ฝ 120mV/dec ์˜ ์—ญ์น˜ํ•˜ ๊ธฐ์šธ๊ธฐ (subthreshold swing, SS) ๋ฐ 106 ์ด์ƒ์˜ on/off ์ „๋ฅ˜ ๋น„ ํŠน์„ฑ์„ ๊ฐ–๋Š”๋‹ค. ๋‘ ๊ฐœ์˜ ๋™์ผํ•œ ์žฌ๊ตฌ์„ฑ ๊ฐ€๋Šฅ ์†Œ์ž๋ฅผ ์ด์šฉํ•˜์—ฌ ์ œ์ž‘๋œ ํ’€ ์Šค์œ™ CMOS ์ธ๋ฒ„ํ„ฐ ๋กœ์ง ๊ฒŒ์ดํŠธ์˜ ๋™์ž‘๋„ ์„ฑ๊ณต์ ์œผ๋กœ ๊ตฌํ˜„๋˜์—ˆ๋‹ค. ์ œ์ž‘๋œ ์†Œ์ž์˜ DC I-V ํŠน์„ฑ, ๋“œ๋ ˆ์ธ ์ „๋ฅ˜์˜ ์˜จ๋„ ์˜์กด์„ฑ ๋ฐ ์ €์ฃผํŒŒ ์žก์Œ ํŠน์„ฑ ์ธก์ •์„ ํ†ตํ•˜์—ฌ, ํ•˜๋ถ€ ์ „๊ทน ์ „์••๊ณผ ์ฑ„๋„ ์ €ํ•ญ ๋ฐ ์‡ผํŠธํ‚ค ์ ‘ํ•ฉ ์ €ํ•ญ์˜ ๊ด€๊ณ„๋ฅผ ์—ฐ๊ตฌํ•˜์˜€๋‹ค. ์ด๋ฅผ ํ†ตํ•˜์—ฌ ์•Œ๋ฃจ๋ฏธ๋Š„ ์†Œ์Šค/๋“œ๋ ˆ์ธ์€ n ํ˜น์€ p ํ˜•์œผ๋กœ ์ „๊ธฐ์ ์œผ๋กœ ๋„ํ•‘๋œ ํด๋ฆฌ ์‹ค๋ฆฌ์ฝ˜ ์ฑ„๋„๊ณผ ์‡ผํŠธํ‚ค ์ ‘ํ•ฉ์„ ํ˜•์„ฑํ•˜๊ฒŒ ๋˜๊ณ , ์†Œ์ž์˜ ์ „๋ฅ˜๋Š” ์‡ผํŠธํ‚ค ์—ญ๋ฐฉํ–ฅ ์ ‘ํ•ฉ ํ„ฐ๋„๋ง์— ์˜ํ•˜์—ฌ ๊ฒฐ์ •๋จ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ œ์ž‘๋œ ์†Œ์ž์— ๋Œ€ํ•œ ๋ถ„์„์„ ๋ฐ”ํƒ•์œผ๋กœ ์†Œ์ž์˜ ์ œ์ž‘ ๊ณต์ • ์ตœ์ ํ™”๋ฅผ ์ง„ํ–‰ํ•˜์˜€์œผ๋ฉฐ, ์ œ์ž‘ ๊ณต์ • ์ตœ์ ํ™”๋ฅผ ํ†ตํ•˜์—ฌ ๊ฐœ์„ ๋œ ๊ท ์ผ์„ฑ๊ณผ ํ‰ํƒ„๋„๋ฅผ ๊ฐ–๋Š” ์•ˆ์ •๋œ ํ•˜๋ถ€ ์ „๊ทน ๊ตฌ์กฐ๋ฅผ ๊ตฌํ˜„ํ•˜์˜€๊ณ  ์ด๋ฅผ ํ†ตํ•ด ๊ฐœ์„ ๋œ ํ”„๋กœ๊ทธ๋žจ/์ด๋ ˆ์ด์ฆˆ ์„ฑ๋Šฅ๊ณผ ์˜จ ์ปค๋ŸฐํŠธ์˜ ์ฆ๊ฐ€๋ฅผ ํ™•์ธํ•˜์˜€๋‹ค. ์ตœ์ ํ™”๋œ ์†Œ์ž์˜ ์—ญ์น˜ํ•˜ ๊ธฐ์šธ๊ธฐ๋Š” ์ด์ค‘ ๊ฒŒ์ดํŠธ ๋™์ž‘์—์„œ ์•ฝ 90 mV/dec ๋กœ ๊ฒŒ์ดํŠธ ์ œ์–ด๋ ฅ์ด ํ–ฅ์ƒ๋˜์—ˆ๊ณ , on/off ์ „๋ฅ˜๋น„๋Š” 107 ์ด์ƒ์œผ๋กœ ์ฆ๊ฐ€ํ•˜์˜€๋‹ค. ๊ณต์ • ์ตœ์ ํ™”๋ฅผ ํ†ตํ•ด ๊ฐ๊ฐ์˜ ์†Œ์ž๋ฅผ ์™„์ „ํžˆ ๊ฒฉ๋ฆฌ ์‹œํ‚ด์œผ๋กœ์จ, ๋„ค ๊ฐœ์˜ ๋™์ผํ•œ ์žฌ๊ตฌ์„ฑ ๊ฐ€๋Šฅ ์†Œ์ž๋ฅผ ์ด์šฉํ•˜์—ฌ ์ œ์ž‘๋œ NAND/NOR ๋กœ์ง ๊ฒŒ์ดํŠธ์˜ ๋™์ž‘ ๋˜ํ•œ ์„ฑ๊ณต์ ์œผ๋กœ ๊ตฌํ˜„ํ•˜์˜€๋‹ค. ๋˜ํ•œ, ์‹คํ—˜๊ณผ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ํ†ตํ•˜์—ฌ ์†Œ์Šค/๋“œ๋ ˆ์ธ ๋ฉ”ํƒˆ์˜ ์ข…๋ฅ˜์™€ ๊ฒŒ์ดํŠธ ์Šคํƒ์˜ ์ „๊ธฐ์  ๋‘๊ป˜๊ฐ€ ์†Œ์ž์˜ ํŠน์„ฑ์— ๋ฏธ์น˜๋Š” ์˜ํ–ฅ์— ๋Œ€ํ•ด์„œ๋„ ๋ถ„์„ ํ•˜์˜€๋‹ค.A novel poly-Si reconfigurable device with programmable bottom gate array having non-volatile memory (NVM) functionality was demonstrated for the first time. The device is very efficient in terms of device size, reliability, uniformity, and reproducibility. By changing bias or program/erase state (PGM/ERS) of the bottom gates (BGs), a device can be transformed to behave one of the following devices: n-/p-MOSFET, n-p, and p-n diode. Threshold voltage (Vth) and contact resistance (Rc) of MOSFETs can be controlled independently by the BGs. The subthreshold swing (SS) and Ion/Ioff of the n-/p-MOSFETs are ~120 mV/dec and >106, respectively, which are comparable to those of conventional poly-Si devices. Full-swing CMOS inverter logic gates implemented by using two identical reconfigurable devices were successfully demonstrated. Relationship between bottom gate biases and resistance of channel and Schottky junction was investigated by DC I-V, temperature dependency of ID, and low frequency noise measurement. Aluminum source/drain (S/D) layer forms Schottky junction with poly-Si body being electrically doped with n- or p-type, and the current mechanism is dominated by Schottky reverse junction tunneling. Optimization of fabrication process was performed and stable BG structure with enhanced uniformity and flatness was achieved. The optimized device demonstrated enhanced PGM/ERS performance and improved on-current characteristics. Gate controllability was also enhanced in the double gate operation with SS of ~90 mV/dec, and Ion/Ioff increased to more than 107. A full-swing CMOS inverter and NAND/NOR logic gates implemented by using four identical reconfigurable devices were also successfully demonstrated with complete device isolation by process optimization. The effect of S/D metal and electrical oxide thickness (EOT) of the gate stack on the device characteristics were investigated by both experiments and simulations.Chapter 1.Introduction 1 1.1 Motivation 1 1.2 Background of Reconfigurable Devices 9 1.3 Thesis Organization 16 Chapter 2.Proposed Reconfigurable Device 18 2.1 Structure and Features of Proposed Reconfigurable Device 18 2.2 Fundamentals of Proposed Reconfigurable Device 24 Chapter 3.Fabrication of Proposed Reconfigurable Device 30 3.1 Mask Layout and Fabrication Issues 30 3.2 Bottom Gate Formation 38 3.2.1 Nitride Spacer Method. 38 3.2.2 Poly-Si CMP Method 42 3.3 Overall Fabrication Process 47 Chapter 4.Characterization of Proposed Reconfigurable Device 55 4.1 I-V Characteristics of n- and p-MOSFETs 55 4.2 MOSFET I-V with PGM/ERS State of Bottom Gates 61 4.3 p-n / n-p diode operations 67 4.4 Logic Gate Operations 72 Chapter 5.Analysis of Schottky Contact Resistance 75 5.1 Schottky barrier modulation by bottom gate bias 75 5.2 Temperature Dependence of Reconfigurable Device 81 5.3 Noise characteristics of MOSFET with bottom gate biases 84 Chapter 6.Process Optimization and On-current Improvement 87 6.1 Performance of Proposed Device 87 6.2 Process Optimization 89 6.2.1 SiO2 fin Method 89 6.2.2 Enhanced I-V characteristics 96 6.3 On-current Improvement 102 Chapter 7.Conclusions 105 Bibliography 108 Abstract in Korean 116Docto

    Crosstalk computing: circuit techniques, implementation and potential applications

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    Title from PDF of title [age viewed January 32, 2022Dissertation advisor: Mostafizur RahmanVitaIncludes bibliographical references (page 117-136)Thesis (Ph.D.)--School of Computing and Engineering. University of Missouri--Kansas City, 2020This work presents a radically new computing concept for digital Integrated Circuits (ICs), called Crosstalk Computing. The conventional CMOS scaling trend is facing device scaling limitations and interconnect bottleneck. The other primary concern of miniaturization of ICs is the signal-integrity issue due to Crosstalk, which is the unwanted interference of signals between neighboring metal lines. The Crosstalk is becoming inexorable with advancing technology nodes. Traditional computing circuits always tries to reduce this Crosstalk by applying various circuit and layout techniques. In contrast, this research develops novel circuit techniques that can leverage this detrimental effect and convert it astutely to a useful feature. The Crosstalk is engineered into a logic computation principle by leveraging deterministic signal interference for innovative circuit implementation. This research work presents a comprehensive circuit framework for Crosstalk Computing and derives all the key circuit elements that can enable this computing model. Along with regular digital logic circuits, it also presents a novel Polymorphic circuit approach unique to Crosstalk Computing. In Polymorphic circuits, the functionality of a circuit can be altered using a control variable. Owing to the multi-functional embodiment in polymorphic-circuits, they find many useful applications such as reconfigurable system design, resource sharing, hardware security, and fault-tolerant circuit design, etc. This dissertation shows a comprehensive list of polymorphic logic gate implementations, which were not reported previously in any other work. It also performs a comparison study between Crosstalk polymorphic circuits and existing polymorphic approaches, which are either inefficient due to custom non-linear circuit styles or propose exotic devices. The ability to design a wide range of polymorphic logic circuits (basic and complex logics) compact in design and minimal in transistor count is unique to Crosstalk Computing, which leads to benefits in the circuit density, power, and performance. The circuit simulation and characterization results show a 6x improvement in transistor count, 2x improvement in switching energy, and 1.5x improvement in performance compared to counterpart implementation in CMOS circuit style. Nevertheless, the Crosstalk circuits also face issues while cascading the circuits; this research analyzes all the problems and develops auxiliary circuit techniques to fix the problems. Moreover, it shows a module-level cascaded polymorphic circuit example, which also employs the auxiliary circuit techniques developed. For the very first time, it implements a proof-of-concept prototype Chip for Crosstalk Computing at TSMC 65nm technology and demonstrates experimental evidence for runtime reconfiguration of the polymorphic circuit. The dissertation also explores the application potentials for Crosstalk Computing circuits. Finally, the future work section discusses the Electronic Design Automation (EDA) challenges and proposes an appropriate design flow; besides, it also discusses ideas for the efficient implementation of Crosstalk Computing structures. Thus, further research and development to realize efficient Crosstalk Computing structures can leverage the comprehensive circuit framework developed in this research and offer transformative benefits for the semiconductor industry.Introduction and Motivation -- More Moore and Relevant Beyond CMOS Research Directions -- Crosstalk Computing -- Crosstalk Circuits Based on Perception Model -- Crosstalk Circuit Types -- Cascading Circuit Issues and Sollutions -- Existing Polymorphic Circuit Approaches -- Crosstalk Polymorphic Circuits -- Comparison and Benchmarking of Crosstalk Gates -- Practical Realization of Crosstalk Gates -- Poential Applications -- Conclusion and Future Wor
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