188 research outputs found

    Characterization of self-heating effects and assessment of its impact on reliability in finfet technology

    Get PDF
    The systematically growing power (heat) dissipation in CMOS transistors with each successive technology node is reaching levels which could impact its reliable operation. The emergence of technologies such as bulk/SOI FinFETs has dramatically confined the heat in the device channel due to its vertical geometry and it is expected to further exacerbate with gate-all-around transistors. This work studies heat generation in the channel of semiconductor devices and measures its dissipation by means of wafer level characterization and predictive thermal simulation. The experimental work is based on several existing device thermometry techniques to which additional layout improvements are made in state of the art bulk FinFET and SOI FinFET 14nm technology nodes. The sensors produce excellent matching results which are confirmed through TCAD thermal simulation, differences between sensor types are quantified and error bars on measurements are established. The lateral heat transport measurements determine that heat from the source is mostly dissipated at a distance of 1ยตm and 1.5ยตm in bulk FinFET and SOI FinFET, respectively. Heat additivity is successfully confirmed to prove and highlight the fact that the whole system needs to be considered when performing thermal analysis. Furthermore, an investigation is devoted to study self-heating with different layout densities by varying the number of fins and fingers per active region (RX). Fin thermal resistance is measured at different ambient temperatures to show its variation of up to 70% between -40ยฐC to 175ยฐC. Therefore, the Si fin has a more dominant effect in heat transport and its varying thermal conductivity should be taken into account. The effect of ambient temperature on self-heating measurement is confirmed by supplying heat through thermal chuck and adjacent heater devices themselves. Motivation for this work is the continuous evolution of the transistor geometry and use of exotic materials, which in the recent technology nodes made heat removal more challenging. This poses reliability and performance concerns. Therefore, this work studies the impact of self-heating on reliability testing at DC conditions as well as realistic CMOS logic operating (AC) conditions. Front-end-of-line (FEOL) reliability mechanisms, such as hot carrier injection (HCI) and non-uniform time dependent dielectric breakdown (TDDB), are studied to show that self-heating effects can impact measurement results and recommendations are given on how to mitigate them. By performing an HCI stress at moderate bias conditions, this dissertation shows that the laborious techniques of heat subtraction are no longer necessary. Self-heating is also studied at more realistic device switching conditions by utilizing ring oscillators with several densities and stage counts to show that self-heating is considerably lower compared to constant voltage stress conditions and degradation is not distinguishable

    Characterisation of thermal and coupling effects in advanced silicon MOSFETs

    Get PDF
    PhD ThesisNew approaches to metal-oxide-semiconductor field effect transistor (MOSFET) engineering emerge in order to keep up with the electronics market demands. Two main candidates for the next few generations of Mooreโ€™s law are planar ultra-thin body and buried oxide (UTBB) devices and three-dimensional FinFETs. Due to miniature dimensions and new materials with low thermal conductivity, performance of advanced MOSFETs is affected by self-heating and substrate effects. Self-heating results in an increase of the device temperature which causes mobility reduction, compromised reliability and signal delays. The substrate effect is a parasitic source and drain coupling which leads to frequency-dependent analogue behaviour. Both effects manifest themselves in the output conductance variation with frequency and impact analogue as well as digital performance. In this thesis self-heating and substrate effects in FinFETs and UTBB devices are characterised, discussed and compared. The results are used to identify trade-offs in device performance, geometry and thermal properties. Methods how to optimise the device geometry or biasing conditions in order to minimise the parasitic effects are suggested. To identify the most suitable technique for self-heating characterisation in advanced semiconductor devices, different methods of thermal characterisation (time and frequency domain) were experimentally compared and evaluated alongside an analytical model. RF and two different pulsed I-V techniques were initially applied to partially depleted silicon-on-insulator (PDSOI) devices. The pulsed I-V hot chuck method showed good agreement with the RF technique in the PDSOI devices. However, subsequent analysis demonstrated that for more advanced technologies the time domain methods can underestimate self-heating. This is due to the reduction of the thermal time constants into the nanosecond range and limitations of the pulsed I-V set-up. The reduction is related to the major increase of the surface to volume ratio in advanced MOSFETs. Consequently the work showed that the thermal properties of advanced semiconductor devices must be characterised within the frequency domain. For UTBB devices with 7-8 nm Si body and 10 nm ultra-thin buried oxide (BOX) the analogue performance degradation caused by the substrate effects can be stronger than the analogue performance degradation caused by self-heating. However, the substrate effects can be effectively reduced if the substrate doping beneath the buried ii oxide is adjusted using a ground plane. In the MHz โ€“ GHz frequency range the intrinsic voltage gain variation is reduced ~6 times when a device is biased in saturation if a ground plane is implemented compared with a device without a ground plane. UTBB devices with 25 nm BOX were compared with UTBB devices with 10 nm BOX. It was found that the buried oxide thinning from 25 nm to 10 nm is not critical from the thermal point of view as other heat evacuation paths (e.g. source and drain) start to play a role. Thermal and substrate effects in FinFETs were also analysed. It was experimentally shown that FinFET thermal properties depend on the device geometry. The thermal resistance of FinFETs strongly varies with the fin width and number of parallel fins, whereas the fin spacing is less critical. The results suggest that there are trade-offs between thermal properties and integration density, electrostatic control and design complexity, since these aspects depend on device geometry. The high frequency substrate effects were found to be effectively reduced in devices with sub-100 nm wide fins.Engineering and Physical Sciences Research Council (EPSRC) and EU fundin

    Silicon Nanowire FinFETs

    Get PDF

    Miniaturized Transistors, Volume II

    Get PDF
    In this book, we aim to address the ever-advancing progress in microelectronic device scaling. Complementary Metal-Oxide-Semiconductor (CMOS) devices continue to endure miniaturization, irrespective of the seeming physical limitations, helped by advancing fabrication techniques. We observe that miniaturization does not always refer to the latest technology node for digital transistors. Rather, by applying novel materials and device geometries, a significant reduction in the size of microelectronic devices for a broad set of applications can be achieved. The achievements made in the scaling of devices for applications beyond digital logic (e.g., high power, optoelectronics, and sensors) are taking the forefront in microelectronic miniaturization. Furthermore, all these achievements are assisted by improvements in the simulation and modeling of the involved materials and device structures. In particular, process and device technology computer-aided design (TCAD) has become indispensable in the design cycle of novel devices and technologies. It is our sincere hope that the results provided in this Special Issue prove useful to scientists and engineers who find themselves at the forefront of this rapidly evolving and broadening field. Now, more than ever, it is essential to look for solutions to find the next disrupting technologies which will allow for transistor miniaturization well beyond siliconโ€™s physical limits and the current state-of-the-art. This requires a broad attack, including studies of novel and innovative designs as well as emerging materials which are becoming more application-specific than ever before

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

    Get PDF
    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

    Strain-Engineered MOSFETs

    Get PDF
    This book brings together new developments in the area of strain-engineered MOSFETs using high-mibility substrates such as SIGe, strained-Si, germanium-on-insulator and III-V semiconductors into a single text which will cover the materials aspects, principles, and design of advanced devices, their fabrication and applications. The book presents a full TCAD methodology for strain-engineering in Si CMOS technology involving data flow from process simulation to systematic process variability simulation and generation of SPICE process compact models for manufacturing for yield optimization

    Benchmarking of FinFET, Nanosheet, and Nanowire FET Architectures for Future Technology Nodes

    Get PDF
    Nanosheet (NS) and nanowire (NW) FET architectures scaled to a gate length ( LG ) of 16 nm and below are benchmarked against equivalent FinFETs. The device performance is predicted using a 3D finite element drift-diffusion/Monte Carlo simulation toolbox with integrated 2D Schrรถdinger equation based quantum corrections. The NS FET is a viable replacement for the FinFET in high performance (HP) applications when scaled down to LG of 16 nm offering a larger on-current ( ION ) and slightly better sub-threshold characteristics. Below LG of 16 nm, the NW FET becomes the most promising architecture offering an almost ideal sub-threshold swing, the smallest off-current ( IOFF ), and the largest ION/IOFF ratio out of the three architectures. However, the NW FET suffers from early ION saturation with the increasing gate bias that can be tackled by minimizing interface roughness and/or by optimisation of a doping profile in the device body

    Benchmarking of FinFET, Nanosheet, and Nanowire FET Architectures for Future Technology Nodes

    Get PDF
    Nanosheet (NS) and nanowire (NW) FET architectures scaled to a gate length (L G ) of 16 nm and below are benchmarked against equivalent FinFETs. The device performance is predicted using a 3D finite element drift-diffusion/Monte Carlo simulation toolbox with integrated 2D Schrรถdinger equation based quantum corrections. The NS FET is a viable replacement for the FinFET in high performance (HP) applications when scaled down to L G of 16 nm offering a larger on-current (I ON ) and slightly better sub-threshold characteristics. Below L G of 16 nm, the NW FET becomes the most promising architecture offering an almost ideal sub-threshold swing, the smallest off-current (I OFF ), and the largest I ON /I OFF ratio out of the three architectures. However, the NW FET suffers from early ION saturation with the increasing gate bias that can be tackled by minimizing interface roughness and/or by optimisation of a doping profile in the device bodyThis work was supported in part by the Spanish Government under Project TIN2013-41129-P and Project TIN2016-76373-P, in part by the Xunta de Galicia and FEDER Funds under Grant GRC 2014/008, and in part by the Consellerรญa de Cultura, Educaciรณn e Ordenaciรณn Universitaria (accreditation 2016โ€“2019) under Grant ED431G/08. The work of Guillermo Indalecio was supported by the Programa de Axudas รก Etapa Posdoutoral da Xunta de Galicia under Grant 2017/077. The work of Natalia Seoane was supported by the RyC Programme of the Spanish Ministerio de Ciencia, Innovaciรณn y Universidades under Grant RYC-2017-23312S

    ํ•€ํŽซ ์†Œ์ž์—์„œ์˜ ํ•ซ์บ๋ฆฌ์–ด ์‹ ๋ขฐ์„ฑ ๋ถ„์„

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2021. 2. ์‹ ํ˜•์ฒ .CMOS ๋กœ์ง ์†Œ์ž๋Š” ํผํฌ๋จผ์Šค๋ฅผ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด ์ง€์†์ ์œผ๋กœ ์ถ•์†Œํ™” ๋˜๊ณ  ์žˆ๋‹ค. ํ•˜์ง€๋งŒ ๊ตฌ์กฐ ํŒŒ๋ผ๋ฏธํ„ฐ๋“ค์˜ ์ถ•์†Œํ™”์— ๋น„ํ•ด ๋™์ž‘ ์ „์••์€ ์ถฉ๋ถ„ํžˆ ๊ฐ์†Œํ•˜์ง€ ์•Š๋Š”๋‹ค. ๋”ฐ๋ผ์„œ ์†Œ์ž ๋‚ด ์ˆ˜์ง ์ „๊ณ„๋‚˜ ์˜จ๋„๊ฐ€ ์ฆ๊ฐ€ํ•˜๋Š” ์ถ”์„ธ์ด๊ธฐ ๋•Œ๋ฌธ์— ์‹ ๋ขฐ์„ฑ์€ ๊ณ„์†ํ•ด์„œ ๋ฌธ์ œ๊ฐ€ ๋˜๊ณ  ์žˆ๋‹ค. ์ตœ๊ทผ 3D ์†Œ์ž์˜ ์‹ ๋ขฐ์„ฑ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๋Š” ๋งŽ์ด ์ง„ํ–‰๋˜๊ณ  ์žˆ์ง€๋งŒ empirical ๋ชจ๋ธ๋ง๊ณผ ๊ด€๋ จ๋œ ์—ฐ๊ตฌ๊ฐ€ ๋Œ€๋ถ€๋ถ„์ด๋‹ค. ๋”ฐ๋ผ์„œ ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์‹ค์ œ ์ธก์ •์„ ๊ธฐ๋ฐ˜์œผ๋กœ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ์ด์šฉํ•˜์—ฌ ๋ฌผ๋ฆฌ์  ์ด๋ก  ์ค‘์‹ฌ์œผ๋กœ ๋กœ์ง ์†Œ์ž์˜ ํ•ซ์บ๋ฆฌ์–ด ์‹ ๋ขฐ์„ฑ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. ๋จผ์ € ํ•ซ์บ๋ฆฌ์–ด ๋ชจ๋ธ์˜ ์ •ํ™•์„ฑ์„ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด์„œ TCAD ์‹œ๋ฎฌ๋ ˆ์ด์…˜์— electron-electron scattering์„ ์ ์šฉํ•˜์˜€๋‹ค. ์ถ”๊ฐ€์ ์œผ๋กœ 3D FinFET์˜ ์ธก์ • ๋ฐ์ดํ„ฐ์™€ calibration์„ ์ง„ํ–‰ํ•˜์—ฌ ๋ชจ๋ธ์˜ ์ •ํ•ฉ์„ฑ์„ ํ™•์ธํ•˜์˜€๋‹ค. calibration ๊ณผ์ •์—์„œ๋Š” ๋ชจ๋“  scattering ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๊ณ ๋ คํ•˜๊ธฐ ์œ„ํ•ด ๋‹ค์–‘ํ•œ ์ „์••๊ณผ ์˜จ๋„ ์กฐ๊ฑด์ด ํ•„์š”ํ•˜๋‹ค. ๋”ฐ๋ผ์„œ ๋‹ค์–‘ํ•œ ์ „์•• ์กฐ๊ฑด์— ๋”ฐ๋ฅธ HCD๋ฅผ ๋ถ„์„ํ•˜๊ณ , calibration์„ ์ง„ํ–‰ํ•˜์—ฌ HCD ๋ชจ๋ธ์˜ ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ์ถ”์ถœํ•˜์˜€๋‹ค. ๋‹ค์Œ์œผ๋กœ ์ „์•• ์กฐ๊ฑด์— ๋”ฐ๋ฅธ HCD์˜ ์˜จ๋„ ๊ฒฝํ–ฅ์„ฑ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. oxide trap๊ณผ ๋‹ฌ๋ฆฌ interface trap์€ ์ „์•• ์กฐ๊ฑด์— ๋”ฐ๋ผ ๋‹ค๋ฅธ ์˜จ๋„ ๊ฒฝํ–ฅ์„ฑ์„ ๋ณด์ธ๋‹ค. ๋”ฐ๋ผ์„œ interface trap์„ 3๊ฐ€์ง€ ์„ฑ๋ถ„์œผ๋กœ ๋ถ„๋ฆฌํ•˜์—ฌ ๊ฐ ์„ฑ๋ถ„์˜ ์˜จ๋„ ๊ฒฝํ–ฅ์„ฑ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. Multiple particle process(MP)๊ณผ field enhanced thermal degradation process(FP)๋Š” ์ „์•• ์กฐ๊ฑด๊ณผ ์ƒ๊ด€์—†์ด ์ผ์ •ํ•œ ์˜จ๋„ ๊ฒฝํ–ฅ์„ฑ์„ ๊ฐ€์ง„๋‹ค. ๋ฐ˜๋ฉด Single particle process(SP)๋Š” scattering์˜ ์˜ํ–ฅ์„ ๋ฐ›๊ธฐ ๋•Œ๋ฌธ์— ์˜จ๋„ ๊ฒฝํ–ฅ์„ฑ์€ ์ „์•• ์กฐ๊ฑด์— ๋”ฐ๋ผ ๋‹ฌ๋ผ์ง„๋‹ค. ์˜จ๋„ ๊ฒฝํ–ฅ์„ฑ ๋ถ„์„ ๊ณผ์ •์—์„œ๋„ calibration์„ ์ง„ํ–‰ํ•˜๋ฉฐ ์—ฌ๋Ÿฌ ๋ฒˆ์˜ iteration์„ ํ†ตํ•ด ๋‹ค์–‘ํ•œ ์ „์•• ๋ฐ ์˜จ๋„๊ฐ€ ๊ณ ๋ ค๋œ ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ์ถ”์ถœํ•œ๋‹ค. ์ถ”์ถœ๋œ ํŒŒ๋ผ๋ฏธํ„ฐ๋ฅผ ์ ์šฉํ•œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๋ชจ๋ธ์€ ๊ธฐ์กด์˜ ๋ชจ๋ธ๋ณด๋‹ค ๋” ์ •ํ™•ํ•˜๊ฒŒ HCD ์ธก์ • ๊ฒฐ๊ณผ๋ฅผ ์˜ˆ์ธกํ•˜์˜€๋‹ค. ๊ฒฐ๊ณผ์ ์œผ๋กœ ๋ฌผ๋ฆฌ์  ์ด๋ก ์— ๊ทผ๊ฑฐํ•˜์—ฌ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๋ชจ๋ธ ๊ตฌ์ถ•ํ•จ์œผ๋กœ์จ HCD ๋ถ„์„์˜ ์ •ํ™•์„ฑ์„ ํ–ฅ์ƒ์‹œ์ผฐ๋‹ค. ํ•˜์ง€๋งŒ ๊ฐ€์† ์กฐ๊ฑด๊ณผ ๋™์ž‘ ์กฐ๊ฑด์˜ self-heating ํšจ๊ณผ๊ฐ€ ๋‹ค๋ฅด๊ธฐ ๋•Œ๋ฌธ์— ์†Œ์ž๊ฐ€ ์‹ค์ œ CMOS ํšŒ๋กœ์˜ ๋™์ž‘ ์กฐ๊ฑด์—์„œ interface trap์„ ๋ฐœ์ƒ์‹œํ‚ค๋Š” ๋ฉ”์ปค๋‹ˆ์ฆ˜์€ ๋‹ค๋ฅผ ์ˆ˜ ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ์šฐ๋ฆฌ๋Š” ๋™์ž‘ ์˜์—ญ์—์„œ์˜ ๊ฐ ์„ฑ๋ถ„์˜ ๋น„์œจ๊นŒ์ง€ ์˜ˆ์ธกํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ ์šฐ๋ฆฌ๋Š” 10 nm node ์†Œ์ž์—์„œ nFinFET์— ๋น„ํ•ด pFinFET์—์„œ ๋†’์€ ์—ดํ™”๊ฐ€ ๋ฐœ์ƒํ•˜๋Š” ์›์ธ์— ๋Œ€ํ•ด ๋ถ„์„ํ•˜์˜€๋‹ค. pFinFET์€ ์†Œ์Šค/๋“œ๋ ˆ์ธ ๋ฌผ์งˆ๋กœ SiGe๋ฅผ ์‚ฌ์šฉํ•˜๊ธฐ ๋•Œ๋ฌธ์— nFinFET์— ๋น„ํ•ด self-heating ํšจ๊ณผ๊ฐ€ ์‹ฌํ•˜์—ฌ ์†Œ์ž ์˜จ๋„๊ฐ€ ๋„ ๋†’๋‹ค. ์ด๋ก ์ ์œผ๋กœ MP ๋ฉ”์ปค๋‹ˆ์ฆ˜์˜ lifetime์€ ์˜จ๋„๊ฐ€ ์ฆ๊ฐ€ํ• ์ˆ˜๋ก ๊ฐ์†Œํ•˜๊ธฐ ๋•Œ๋ฌธ์— MP์— ์˜ํ•œ ์—ดํ™” ๋˜ํ•œ ๊ฐ์†Œํ•œ๋‹ค. ๋”ฐ๋ผ์„œ ์†Œ์ž ์˜จ๋„๊ฐ€ ๋” ๋†’์€ pFinFET์—์„œ nFinFET์— ๋น„ํ•ด ๋” ๋งŽ์€ MP๊ฐ€ ๋ฐœ์ƒํ•˜๊ธฐ ์–ด๋ ต๋‹ค. ํ•˜์ง€๋งŒ nFinFET ๊ณผ ๋‹ฌ๋ฆฌ pFinFET์—์„œ๋Š” Si-H bond์˜ electron๊ณผ hole์ด ๋ฐ˜์‘ํ•˜์—ฌ interface trap์„ ์ƒ์„ฑ์‹œํ‚ค๋Š” RD ๊ฐ€ ๋ฐœ์ƒํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ RD๋Š” ์˜จ๋„๊ฐ€ ๋†’์„์ˆ˜๋ก ๋” ๋งŽ์€ ์—ดํ™”๊ฐ€ ๋ฐœ์ƒํ•˜๊ธฐ ๋•Œ๋ฌธ์—, pFinFET์—์„œ nFinFET๋ณด๋‹ค ๋” ๋งŽ์€ ์—ดํ™”๊ฐ€ ๋ฐœ์ƒํ•˜๋Š” ํ˜„์ƒ์„ ์„ค๋ช…ํ•  ์ˆ˜ ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ ์šฐ๋ฆฌ๋Š” HCD ์กฐ๊ฑด์ด์ง€๋งŒ ์†Œ์ž ์˜จ๋„๊ฐ€ ๋†’์€ pFinFET์—์„œ ์ถ”๊ฐ€์ ์ธ RD ๋ฉ”์ปค๋‹ˆ์ฆ˜์ด ๋ฐœ์ƒํ•  ์ˆ˜ ์žˆ๋‹ค๊ณ  ์ œ์•ˆํ•œ๋‹ค. ๋‹ค์–‘ํ•œ ์ „์•• ์กฐ๊ฑด์—์„œ์˜ ์ „๋ฅ˜ ์—ดํ™”์œจ์„ ํ†ตํ•ด ์ฃผ์š” ์—ดํ™” ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๋ถ„์„ํ•˜์˜€์œผ๋ฉฐ pFinFET์—์„œ๋Š” RD๊ฐ€ ์ฃผ์š”ํ•จ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋˜ํ•œ TCAD ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ์ด์šฉํ•˜์—ฌ HCD ์กฐ๊ฑด์—์„œ ๋ฐœ์ƒํ•  ์ˆ˜ ์žˆ๋Š” RD๋ฅผ ์˜ˆ์ธกํ•˜์˜€๋‹ค. ๊ทธ ๊ฒฐ๊ณผ RD๋ฅผ ์ œ์™ธํ•œ ์ˆœ์ˆ˜ hot carrier ์„ฑ๋ถ„์€ pFinFET๋ณด๋‹ค nFinFET์—์„œ ๋” ๋งŽ์ด ๋ฐœ์ƒํ•œ๋‹ค.CMOS logic devices have been scaled down to improve performance. However, the operating voltage is not sufficiently reduced compared to the scale down in physical dimensions. Therefore, since the electric field and temperature of the device gradually increase, reliability is still a critical issue in logic devices. Recently, many studies on the reliability of 3D devices are being conducted, but most of the studies are related to empirical modeling. Therefore, in this study, based on the actual measurement results, the hot carrier degradation(HCD) reliability of the logic device was analyzed focusing on the physical theory using Technology computer-aided design (TCAD) simulation. First, electron-electron scattering(EES) was applied to the TCAD simulation to improve the accuracy of the hot carrier model. Additionally, calibration between the measurement data of 14 nm node FinFET and the model was performed to confirm the consistency. The calibration process required various voltage and temperature conditions to account for all scattering mechanisms. Therefore, HCD was analyzed according to various voltage conditions, and the parameters of the HCD model were extracted by calibration process. Next, temperature dependence under various HCD conditions was analyzed. Unlike oxide traps, interface traps show different temperature dependence depending on HCD voltage conditions. Therefore, the interface traps were separated into three components and the temperature dependence was analyzed for each component. Multiple particle process (MP) and Field enhanced thermal degradation process (FP) have a constant temperature dependence regardless of voltage conditions. On the other hand, the temperature dependence of Single particle process (SP) varies depending on the voltage condition because SP is affected by scattering. In the process of temperature dependence analysis, calibration is also performed and parameters considering various voltages and temperatures were extracted through several iterations. The improved model to which the extracted parameters were applied showed more precise prediction of degradation compared to that of the previous model. As a results, accuracy of the HCD analysis was improved by establishing the HCD simulation framework based on physical theories. However, since the self-heating effect of the acceleration condition and the operation condition are different, the HCD mechanism that occurs in the actual CMOS circuit may also be different. Therefore, we predicted the ratio of each component under operating condition. Finally, in 10 nm node devices, we analyzed the cause of higher HCD in pFinFETs than in nFinFETs. Self-heating effect is severe in pFinFETs because SiGe is used as the source/drain material which makes the device temperature higher than nFinFETs. Theoretically, because the lifetime of multiple particle(MP) mechanism decreases as temperature increases, degradation due to MP decreases. Therefore, it is difficult for the HCD mechanisms to occur more in pFinFETs which has higher temperature than nFinFETs. However, in pFinFETs unlike nFinFETs, reaction-diffusion (RD) mechanism can occur in which holes react with the electrons of Si-H bonds to generate interface traps. Also, since RD deteriorates more as the temperature increases, the phenomenon that more degradation occurs in pFinFET than nFinFET can be explained by the RD mechanism. Therefore, we propose an additional RD mechanism that is caused by high device temperature in pFinFETs even in HCD condition. Main components were investigated through measurements of current degradation rate in various voltage conditions, and it was found that RD is dominant in pFinFETs. Also, RD that can occur in HCD condition was predicted through TCAD simulation. As a results, degradation due to pure hot carriers without RD occurs more in nFinFETs than in pFinFETs.Abstract i Chapter 1. Introduction 1 Chapter 2. Hot Carrier Degradation Model 4 2.1. Physical theory 4 2.2. TCAD simulation 8 2.3. Calibration process 14 2.4. Summary 22 Chapter 3. Analysis on Temperature Dependence of HCD 25 3.1. Introduction 25 3.2. Temperature dependence according to acceleration conditions 26 3.3. Calibration process 30 3.4. Mechanism separation 33 3.5. HCD prediction in the nominal voltage 35 3.6. Summary 36 Chapter 4. Comparative Analysis of HCD in nMOS/pMOS FinFET 39 4.1. Introduction 39 4.2. Comparison of HCD in the long/short channel FinFET 40 4.3. Self-heating effect in n/pFinFET 44 4.4. Bias Temperature Instability(BTI) in n/pFinFET 47 4.5. Summary 59 Chapter 5. Conclusion 64 Abstract in Korean 66 List of Publications 69Docto
    • โ€ฆ
    corecore