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With the reduction of the interconnect dimensions and the increased impact of process variations and process induced damage on the circuit performance, the standard Cu/Low-k damascene interconnects are now reaching their application limits. The increase in Cu resistivity with scaling and the enhanced reliability concerns at smaller dimensions are the main drivers towards replacing Cu with an alternative material.In this Ph.D thesis work, the performance of graphene interconnects are evaluated and benchmarked against the state-of-the-art Cu/Low-k interconnects in terms of capacitance, resistance, interconnect delay, circuit delay and power consumptions. Initially, the models used to evaluate graphene's capacitance and resistance, which are a combination of original models and models from literature, are discussed. Then, the models are calibrated to both in-house and published experimental data, in order to obtain reliable predictions as a function of the input parameters. Lastly, using the calibrated models, graphene and Cu interconnects are benchmarked by varying graphene's width, quality, number of layers, doping concentration and contact configuration.We show that up to 65% capacitance reduction can be achieved when switching from Cu to graphene interconnects thanks to the reduced graphene thickness. Moreover, depending on the doping technique implemented, capacitance benefits can be obtained when assuming up to and beyond fifty graphene layers. Regarding the resistance, we demonstrate that the edge contact configuration is the preferred option for graphene interconnects, as it gives the lowest total line resistance, independently from the doping concentration or the number of graphene layers considered. When comparing graphene resistance with the one of Cu, we show how the benchmark heavily depends on the graphene quality and doping concentration. In the best case considered in this dissertation, that is HNO3 stage-1 intercalated graphene, we see that a first cross-over between Cu and graphene interconnects occurs for 17 nm interconnect width for 50 graphene layers, while only 26 layers are needed to match Cu resistance at 10 nm half-pitch interconnects. As far as the interconnect RC delay is concerned, we show that, thanks to the lower interconnect capacitance, the cross-over between Cu and graphene interconnects moves towards a lower number of layers compared to the resistance benchmark, while for circuit delay, the contact resistance between graphene and the contacting metal highly impacts graphene performance for interconnect lengths lower than 3.2 μm. Finally, we benchmark graphene against Cu for the 3 nm logic technology node, showing that up to 16% delay reduction can be achieved while also lowering the power consumption. Alternatively, 34% power reduction can be achieved for the same delay of Cu by modifying the graphene interconnect configuration.
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The continuous scaling of Metal Oxide Semiconductor Field Effect Transistor (MOSFET) dimensions for over more than 5 decades has enabled the steady increase of transistor performance and density, while reducing the relative cost. These factors led to a tremendous growth of the semiconductor industry and it is remarkable that Silicon has always been the preferred channel material.The journey of scaling Si-channel-based MOSFETs was challenging due to a myriad of issues such as short channel effects, and gate-oxide scaling limit, and in particular, low drive current. Many were overcome with clever engineering solutions, even leading to a commercially available 7nm CMOS technology node (anno 2019). However, MOSFETs for mobile applications needed to deliver high drive current at low operating voltage (low-power). To this end, alternative channel materials with high intrinsic carrier mobilities, such as InGaAs and SiGe, emerged as promising candidates. While InGaAs MOS devices with enhanced performance have already been demonstrated, their long-term Bias Temperature Instability (BTI) reliability remains a concern.In this work, we demonstrate a gate-stack for InGaAs devices that meets all the BTI targets for DC operation, while maintaining high channel mobility (~3500 cm2/V-s) and sufficient ON-current for a 0.75V III-V technology. We also observed that BTI reliability of InGaAs devices is poorer at lower temperatures, unlike that observed in Si-channel devices, thereby implying an apparent opposite temperature activation of BTI. Novel electrical characterization techniques and semi-empirical models were developed that (i) enabled the engineering of a gate-stack with necessary electrical properties for improved BTI reliability, and (ii) provided in-depth understanding of the impact of temperature on BTI degradation. The poor gate-stack reliability is ascribed to the unfavorable alignment of defect energy distributions with the channel conduction band, such that a high defect density is accessible for channel carriers at low operating oxide fields. A semi-empirical model was developed which precisely estimates the oxide field dependence on the applied gate-voltage, and further calculates the effective charging defect density in order to reproduce the experimental results. This model was used to compare the defect energy distributions of different gate-stacks, and ultimately to develop a tri-layer gate-stack for InGaAs MOS devices with a more favorable alignment of defect energy distributions, necessary to meet all the BTI reliability targets.The apparent opposite temperature activation of charge trapping in the gate-oxide was found to be specific to InGaAs devices, and hence required a more fundamental insight into the origin of the increased Vth degradation. The Non-radiative Multiphonon (NMP) theory, which describes the charge trapping process from the microscopic-physics perspective, was used to analytically model the distributions of activation energies for charge capture and emission into/from the gate-oxide defects. The activation energies were then transformed into Capture/Emission Time (CET) maps. A thorough analysis of the CET maps confirmed that the increased Vth degradation at lower temperatures is the result of different properties associated with the multiple sub-populations of oxide defects, active in the measurement range. We further concluded that such an analysis is essential for an accurate estimation of long-term BTI degradation under both DC and AC operating conditions, while also providing us with a robust semi-empirical modelling tool that has a direct association with the microscopic mechanisms causing BTI.
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The need for reliable, cheap and dense memory devices has never been so important specially with the inception of Internet of Things (IoT) which willrequire further expansion in data storage solutions. Flash NAND technology has been playing a crucial role in this on-going expansion and has becomea driving force in the semiconductor industry. This memory is cost-effective, dense, robust, and non-volatile. This technology suffers, however, from a fewdrawbacks, such as slow speed, large cell size and high power consumption at chip level due to required periphery (e.g. charge pumps). Looking for alternative memories without these issues while keeping the advantages of this technology is therefore very attractive. As of today, 3-D NAND technology has no potential replacement candidate and among the storage class memory (SCM) devices, neither have comparableproperties. Addressing the 3-D NAND issues while keeping the advantages of this technology would be very appealing. Such device would be a serious candidate for 3-D NAND replacement and/or storage-type SCM. The discovery in 2010 of ferroelectric hafnium oxide (FE-HfO2), which spontaneous polarization can be reversed with the application of an electric field, has generated a regained interest in FE memories. Ferroelectricity can enable devices with low power consumption and fast speed. In this thesis, a novel memory concept is investigated which combines the advantages of the ferroelectricity through the application of FE-HfO2 filmsin a vertical architecture while retaining the high density of the vertical 3-D NAND structure. Using planar capacitors, the influence of multiple factors onFE properties is thoroughly investigated and an optimized film is developed for further 3-D integration. In-depth studies of two specific effects in FE, wake-upand imprint, are conducted. Empirical models are proposed to describe the origin of these phenomena. The optimized FE-HfO2 films are integrated in a3-D cylindrical capacitor. FE properties are demonstrated, confirming that vertically etched Si/oxide sidewalls and cylindrical structures do not inhibit the crystallization into the FE phase. Finally 3-D NAND-type macaroni ferroelectric field effect transistor (FeFET) devices are fabricated with a memory windowup to 2 V, fast write/erase pulse down to 100 ns, flash-like endurance and extrapolated retention to 10 years at 85ºC. To complete the study, disturb and charge-trapping effects are analyzed. This technology offers low-power highdensity high-speed non-volatile memory that decreases the speed gap between the central processing unit (CPU) and storage.
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