Analysis of drain-induced barrier rising in short-channel negative-capacitance FETs and its applications

We investigate the performance of hysteresis-free short-channel negative-capacitance FETs (NCFETs) by combining quantum-mechanical calculations with the Landau-Khalatnikov equation. When the subthreshold swing (SS) becomes smaller than 60 mV/dec, a negative value of drain-induced barrier lowering is obtained. This behavior, drain-induced barrier rising (DIBR), causes negative differential resistance in the output characteristics of the NCFETs. We also examine the performance of an inverter composed of hysteresis-free NCFETs to assess the effects of DIBR at the circuit level. Contrary to our expectation, although hysteresis-free NCFETs are used, hysteresis behavior is observed in the transfer properties of the inverter. Furthermore, it is expected that the NCFET inverter with hysteresis behavior can be used as a Schmitt trigger inverter

Analytical model of subthreshold swing in junctionless gate-all-around (GAA) FET with ferroelectric

An analytical SS model is presented to observe the subthreshold swing (SS) of a junctionless gate-all-around (GAA) FET with ferroelectric in this paper. For the gate structure, a multilayer structure of metal-ferroelectric-metal-insulator-semiconductor (MFMIS) was used, and the SS was calculated in $15 \leqslant {P_r} \leqslant 30\,\mu C/c{m^2}$ and $0.8 \leqslant {E_c} \leqslant 1.5\,MV/cm$, which are the ranges of remanent polarization and coercive field suggested in various experiments in the case of HZO as the ferroelectric material. It was found that the SSs from the presented analytical SS model agree well with those derived from the relationship between drain current and gate voltage using a 2D potential distribution in the range of device parameters used for simulation. As a result of analyzing the SS of the junctionless GAA FET with ferroelectric using the analytical SS model presented in this paper, the SS decreased because the voltage across the inner gate decreased when the ferroelectric thickness increased. It was observed that the condition of SS < 60 mV/dec was sufficiently obtained according to changes in device parameters such as channel length, channel radius and ferroelectric thickness, and that the SS maintained a constant value according to the ratio of remanent polarization and coercive field Pr/Ec. As Pr/Ec increases, the SS increases as the ferroelectric capacitance increases. As the channel length becomes smaller, the change in SS according to Pr/Ec is more severe

Analysis of Drain-Induced Barrier Lowering for Gate-All-Around FET with Ferroelectric

This study presents an analytical model for the drain-induced barrier lowering (DIBL) of a junctionless gate-all-around FET with ferroelectric, utilizing a 2D potential model. A multilayer structure of metal-ferroelectric-metal-insulator-semiconductor is used as the gate, as well as the remanent polarization and coercive field values corresponding to HZO are used. The DIBLs obtained with the proposed model demonstrate good agreement with those obtained using the second derivative method, which relies on the 2D relationship between drain current and gate voltage. The results demonstrate that an increase in ferroelectric thickness leads to a negative DIBL value due to the ferroelectric charge. Additionally, there exists an inverse relationship between ferroelectric thickness and channel length to achieve a DIBL value of 0. This condition is satisfied only with the increase of the ferroelectric thickness as the channel radius and insulator thickness increase. The DIBLs increase with higher remanent polarization and lower coercive field, remaining constant when the ratio of remanent polarization and coercive field is maintained

A study of silicon and germanium junctionless transistors

Technology boosters, such as strain, HKMG and FinFET, have been introduced into semiconductor industry to extend Moore’s law beyond 130 nm technology nodes. New device structures and channel materials are highly demanded to keep performance enhancement when the device scales beyond 22 nm. In this work, the properties and feasibility of the proposed Junctionless transistor (JNT) have been evaluated for both Silicon and Germanium channels. The performance of Silicon JNTs with 22 nm gate length have been characterized at elevated temperature and stressed conditions. Furthermore, steep Subthreshold Slopes (SS) in JNT and IM devices are compared. It is observed that the floating body in JNT is relatively dynamic comparing with that in IM devices and proper design of the device structure may further reduce the VD for a sub- 60 mV/dec subthreshold slope. Diode configuration of the JNT has also been evaluated, which demonstrates the first diode without junctions. In order to extend JNT structure into the high mobility material Germanium (Ge), a full process has been develop for Ge JNT. Germanium-on-Insulator (GeOI) wafers were fabricated using Smart-Cut with low temperature direct wafer bonding method. Regarding the lithography and pattern transfer, a top-down process of sub-50-nm width Ge nanowires is developed in this chapter and Ge nanowires with 35 nm width and 50 nm depth are obtained. The oxidation behaviour of Ge by RTO has been investigated and high-k passivation scheme using thermally grown GeO2 has been developed. With all developed modules, JNT with Ge channels have been fabricated by the CMOScompatible top-down process. The transistors exhibit the lowest subthreshold slope to date for Ge JNT. The devices with a gate length of 3 μm exhibit a SS of 216 mV/dec with an ION/IOFF current ratio of 1.2×103 at VD = -1 V and DIBL of 87 mV/V

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Department of PhysicsSubthreshold swing is one of most important parameters in controversial metal-oxide-semiconductor (CMOS) technology, which is related on power consumption. In the metal-oxide-semiconductor field effect transistor (MOSFET), there is thermodynamic limit of subthreshold swing of 60 mV/dec at room temperature. In order to achieve the subthreshold swing, edge-over MOSFET structure is proposed, transistor channel of EO MOSFET is formed on sidewall of insulating pillar. Therefore, transistor channel length increases even though the lateral transistor channel length is maintained. Since the subthreshold swing is deteriorated by the short channel effect, relatively long channel due to existence of insulating pillar has advantage to suppress the subthreshold swing in nano-meter scale. By technology computer aided design (TCAD) modeling, electrical characteristics are demonstrated. Low drain induced barrier lowering (DIBL) of 13.7 mV/V and steep subthreshold swing of 62.6 mV/dec are estimated. Ternary characteristics of EO ternary inverter are investigated by TCAD Mixed mode, the voltage transfer characteristics (VTC) of EO ternary inverter gives an apparent ternary voltage states. In according to structures of EO resistor and EO MOSFET, EO ternary inverter can be formed perpendicular to substrate, therefore, which allows thin lateral dimension of the inverter. Reliability of ternary operation is explained with static noise margin (SNM) and transient response. In the transient response, ternary operation is maintained at 10 MHz frequency, and a propagation delay of 1.69 ns is evaluated. Theoretical approach to thermionic emission at Dirac semimetal source is performed. In the Dirac semimetal, since density of states are determined by linear energy dispersion near the Dirac point, thermionic emission current can be controlled by difference between Dirac point and fermi level and Schottky barrier height. As absence of direct injection of carriers from contact to Si, equation of thermionic emission is different with that of conventional up-down source/substrate structure. In case of graphene, there are singularities at negative infinity, hence the possibility of constant thermionic current exists regardless of the gate biasing of MOSFET. Meanwhile, lowest subthreshold swing of 30 mV/dec for 3 dimensional Dirac semimetal source is discussed.clos

Transport properties and low-frequency noise in low-dimensional structures

Les propriétés électriques et physiques de structures à faible dimensionalité ont été étudiées pour des applications dans des domaines divers comme l électronique, les capteurs. La mesure du bruit bruit à basse fréquence est un outil très utile pour obtenir des informations relatives à la dynamique des porteurs, au piègeage des charges ou aux mécanismes de collision. Dans cette thèse, le transport électronique et le bruit basse fréquence mesurés dans des structures à faible dimensionnalité comme les dispositifs multi-grilles (FinFET, JLT ), les nanofils 3D en Si/SiGe, les nanotubes de carbone ou à base de graphène sont présentés. Pour les approches top-down et bottom-up , l impact du bruit est analysé en fonction de la dimensionalité, du type de conduction (volume vs surface), de la contrainte mécanique et de la présence de jonction metal-semiconducteur.Electrical and physical properties of low-dimensional structures have been studied for the various applications such as electronics, sensors, and etc. Low-frequency noise measurement is also a useful technique to give more information for the carrier dynamics correlated to the oxide traps, channel defects, and scattering. In this thesis, the electrical transport and low-frequency noise of low-dimensional structure devices such as multi-gate structures (e.g. FinFETs and Junctionless FETs), 3-D stacked Si/SiGe nanowire FETs, carbon nanotubes, and graphene are presented. From the view point of top-down and bottom-up approaches, the impacts of LF noise are investigated according to the dimensionality, conduction mechanism (surface or volume conduction), strain technique, and metal-semiconductor junctions.SAVOIE-SCD - Bib.électronique (730659901) / SudocGRENOBLE1/INP-Bib.électronique (384210012) / SudocGRENOBLE2/3-Bib.électronique (384219901) / SudocSudocFranceF

Multigate MOSFETs for digital performance and high linearity, and their fabrication techniques

The aggressive downscaling of complementary metal–oxide–semiconductor (CMOS) technology is facing great challenges to overcome severe short-channel effects. Multigate MOSFETs are one of the most promising candidates for scaling beyond Si CMOS, due to better electrostatic control as compared to conventional planar MOSFETs. Conventional dry etching-induced surface damage is one of the main sources of performance degradation for multigate transistors, especially for III-V high mobility materials. It is also challenging to increase the fin aspect ratio by dry etching because of the non-ideal anisotropic etching profile. Here, we report a novel method, inverse metal-assisted chemical etching (i-MacEtch), in lieu of conventional RIE etching, for 3D fin channel formation. InP junctionless FinFETs with record high-aspect-ratio (~ 50:1) fins are demonstrated by this method for the first time. The i-MacEtch process flow eliminates dry-etching-induced plasma damage, high energy ion implantation damage, and high temperature annealing, allowing for the fabrication of InP fin channels with atomically smooth sidewalls. The sidewall features resulting from this unique and simplified process ensure high interface quality between high-k dielectric layer and InP fin channel. Experimental and theoretical analyses show that high-aspect-ratio FinFETs, which could deliver more current per area under much relaxed horizontal geometry requirements, are promising in pushing the technology node ahead where conventional scaling has met its physical limits. The performance of the FinFET was further investigated through numerical simulation. A new kind of FinFET with asymmetric gate and source/drain contacts has been proposed and simulated. By benchmarking with conventional symmetric FinFET, better short-channel behavior with much higher current density is confirmed. The design guidelines are provided. The overall circuit delay can be minimized by optimizing gate lengths according to different local parasites among circuits in interconnection-delay-dominated SoC applications. Continued transistor scaling requires even stronger gate electrostatic control over the channel. The ultimate scaling structure would be gate-all-around nanowire MOSFETs. We demonstrate III-V junctionless gate-all-around (GAA) nanowire (NW) MOSFETs for the first time. For the first time, source/drain (S/D) resistance and thermal budget are minimized by regrowth using metalorganic chemical vapor deposition (MOCVD) in III-V MOSFETs. The fabricated short-channel (Lg=80 nm) GaAs GAA NWFETs with extremely narrow nanowire width (WNW= 9 nm) show excellent transconductance (gm) linearity at biases (300 mV), characterized by the high third intercept point (2.6 dBm). The high linearity is especially important for low power applications because it is insensitive to bias conditions

Development of inversion-mode and junctionless Indium-Gallium-Arsenide MOSFETs

This PhD covers the development of planar inversion-mode and junctionless Al2O3/In0.53Ga0.47As metal-oxidesemiconductor field-effect transistors (MOSFETs). An implant activation anneal was developed for the formation of the source and drain (S/D) of the inversionmode MOSFET. Fabricated inversion-mode devices were used as test vehicles to investigate the impact of forming gas annealing (FGA) on device performance. Following FGA, the devices exhibited a subthreshold swing (SS) of 150mV/dec., an ION/IOFF of 104 and the transconductance, drive current and peak effective mobility increased by 29%, 25% and 15%, respectively. An alternative technique, based on the fitting of the measured full-gate capacitance vs gate voltage using a selfconsistent Poisson-Schrödinger solver, was developed to extract the trap energy profile across the full In0.53Ga0.47As bandgap and beyond. A multi-frequency inversion-charge pumping approach was proposed to (1) study the traps located at energy levels aligned with the In0.53Ga0.47As conduction band and (2) separate the trapped charge and mobile charge contributions. The analysis revealed an effective mobility (μeff) peaking at ~2850cm2/V.s for an inversion-charge density (Ninv) = 7*1011cm2 and rapidly decreasing to ~600cm2/V.s for Ninv = 1*1013 cm2, consistent with a μeff limited by surface roughness scattering. Atomic force microscopy measurements confirmed a large surface roughness of 1.95±0.28nm on the In0.53Ga0.47As channel caused by the S/D activation anneal. In order to circumvent the issue relative to S/D formation, a junctionless In0.53Ga0.47As device was developed. A digital etch was used to thin the In0.53Ga0.47As channel and investigate the impact of channel thickness (tInGaAs) on device performance. Scaling of the SS with tInGaAs was observed for tInGaAs going from 24 to 16nm, yielding a SS of 115mV/dec. for tInGaAs = 16nm. Flat-band μeff values of 2130 and 1975cm2/V.s were extracted on devices with tInGaAs of 24 and 20nm, respectivel

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

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