Characterization of SiC MESFETs with narrow channel layer

SiC MESFETs with a narrow channel layer are proposed to alleviate the short-channel effects, in particular the drain-induced barrier lowering (DIBL) effect that results in threshold voltage that is dependent on the gate length and the drain voltage applied. Such narrow channel layer 4H-SiC MESFETs were fabricated and characterized. The thickness and doping concentration of the channel layer are 0.08 μm and 8.0 × 10¹⁷ cm⁻³, respectively. The measurement results showed that the threshold voltage of the MESFETs is about −1.1 V and is independent of the gate length from 1 to 3 μm, and the drain voltage applied up to 40 V. Good saturation behavior with fairly low output conductance was also achieved, which is desirable for small signal applications. The results obtained for the narrow channel layer MESFETs are also compared with those measured for conventional devices with thicker channel layer of 0.20 μm and doping concentration of 2.5 × 10¹⁷ cm⁻³.     

Stackable nonvolatile memory with ultra thin polysilicon film and low-leakage (Ti, Dy)xOy for low processing temperature and low operating voltages

We report the fabrication process as well as material and electrical characterization of ultra thin body (UTB) thin film transistors (TFTs) for stackable nonvolatile memories by using in situ phosphorous doped low-temperature polysilicon followed by the chemical mechanical polishing (CMP) process. The resulting polysilicon film is about 13 nm thick with approximately 10¹⁹ cm⁻³ doping. Root mean square surface roughness below 1 nm is achieved. Metal nanocrystals and high-k dielectric are selected for storage nodes and tunneling barriers to achieve low operating voltages. The number density and average diameter of nanocrystals embedded in the gate stack are 7.5 × 10¹¹ cm⁻² and 5.8 nm, respectively. Furthermore, scanning transmission electron microscopy (STEM), convergent beam electron diffraction (CBED) and electron energy loss spectroscopy (EELS) are performed for material characterization. The dielectric constant of the (Ti, Dy)_xO_y film is 35, and the off-state leakage current at −1 V bias and 2.8 nm equivalent oxide thickness is 5 × 10⁻⁷ A/cm². We obtain a memory window of about 0.95 V with ±6 V program/erase voltages. Our results show that UTB TFT is a promising candidate for the three-dimensional integration in high-density nonvolatile memory applications.     

FinFET based SRAM bitcell design for 32 nm node and below

The methodology of designing FinFET bitcell is presented in detail. Determination of Fin configuration (i.e., Fin thickness, space, height, and number) in the bitcell involves consideration of both layout and electrical optimization. Once optimized through the proposed method, FinFET bitcell can provide higher cell current, lower leakage current and much lower V_ccmin with smaller bitcell area, as compared to planar bitcell, which allows continuous scaling of SRAM bitcell <0.1 μm² below 32 nm node.     

Evaluation of process parameter space of bulk FinFETs using 3D TCAD

Using full 3D TCAD, an evaluation of process parameter space of bulk FinFET is presented from the point of view of DRAM, SRAM and I/O applications. Process and device simulations are performed with varying uniform fin doping, anti-punch implant dose and energy, fin width, fin height and gate oxide thickness. Bulk FinFET architecture with anti-punch implant is introduced beneath the channel region to reduce the punch-through and junction leakage. For 30 nm bulk FinFET, anti-punch implant with low energy of 15 to 25 keV and dose of 5.0 × 10¹³ to 1.0 × 10¹⁴ cm⁻² is beneficial to effectively suppress the punch-through leakage with reduced GIDL and short channel effects. Our simulations show that bulk FinFETs are approximately independent of back bias effect. With identical fin geometry, bulk FinFETs with anti-punch implant show same I_ON-I_OFF behavior and approximately equal short channel effects like SOI FinFETs.     

Characterization of ultra-thin SiO2 by capacitance-voltage and charge pumping measurements

In this paper, we present results on electrical measurements of ultra thin SiO₂ layers (from 3.5 nm down to 1.7 nm), used as gate dielectric in metal-oxide-semiconductors (MOS) devices. Capacitance-voltage (C-V) measurements and simulations on MOS capacitors have been used for extracting the electrical oxide thickness. The SiO₂/Si interface and oxide quality have been analyzed by charge pumping (CP) measurements. The mean interface traps density is measured by 2-level CP, and the energy distribution within the semiconductor bandgap of these traps are investigated by 3-level charge pumping measurements. A comparison of the energy distribution of the SiO₂/Si interface traps is made using classical and quantum simulations to extract the surface potential as a function of the gate signal. When the gate oxide thickness <3.5 nm, we prove that it is mandatory to take into account the quantum effects to obtain a more accurate energy distribution of the SiO₂/Si interface traps. We also explain the increase of the apparent interface traps density measured by 2-levels CP with the increase of the oxide thickness, for transistors made from the same technological process.     

Investigation of high-performance sub-50 nm junctionless nanowire transistors

The performances of the junctionless nanowire transistor (JNT) are evaluated under high-performance (HP) ITRS device technical requirements for the 25 nm technology node. The electrical characteristics of the devices are obtained from numerical simulations. The threshold voltage of JNT can be easily adjusted by changing different variable parameters such as fin width, fin thickness, doping concentration, gate oxide thickness and gate work function. The variation of threshold voltage with physical parameters is analyzed. The current drive is controlled by doping concentration and nanowire size. For gate length down to 25 nm, a 30-40% increase in drain current is also reported by using a fin aspect ratio of 2 instead of 1. Additional source and drain implantation can be applied to improve the current drive.     

Advantage of further scaling in gate dielectrics below 0.5 nm of equivalent oxide thickness with La2O3 gate dielectrics

N-type metal-oxide-semiconductor field-effect transistor (MOSFET) with an equivalent oxide thickness (EOT) of 0.37 nm has been demonstrated with La₂O₃ as a gate dielectric for the first time. Despite the existence of parasitic capacitances at gate electrode and inversion layer in the channel, a sufficient drain current increment in both linear and saturation regions have been observed, while scaling the gate oxide from 0.48 to 0.37 nm in EOT. Therefore, continuous scaling of EOT below 0.5 nm is still effective for further improvement in device performance.     

Composition and electrical characteristics of Al2O3-HfO2-HfTiO nanolaminates on Si

A dielectric constant of 27 was demonstrated in the as deposited state of a 5 nm thick, seven layer nanolaminate stack comprising Al₂O₃, HfO₂ and HfTiO. It reduces to an effective dielectric constant (k_eff) of ∼14 due to a ∼0.8 nm interfacial layer. This results in a quantum mechanical effective oxide thickness (EOT) of ∼1.15 nm. After annealing at 950 °C in an oxygen atmosphere k_eff reduces to ∼10 and EOT increases to 1.91 nm. A small leakage current density of about 8 × 10⁻⁷ and 1 × 10⁻⁴ A/cm², respectively at electric field 2 and 5 MV/cm and a breakdown electric field of about 11.5 MV/cm was achieved after annealing at 950 °C.     

Quantum mechanical analytical modeling of nanoscale DG FinFET: evaluation of potential,threshold voltage and source/drain resistance

Two-dimensional (2D) quantum mechanical analytical modeling has been presented in order to evaluate the 2D potential profile within the active area of FinFET structure. Various potential profiles such as surface, back to front gate and source to drain potential have been presented in order to appreciate the usefulness of the device for circuit simulation purposes. As we move from source end of the gate to the drain end of the gate, there is substantial increase in the potential at any point in the channel. This is attributed to the increased value of longitudinal electric field at the drain end on application of a drain to source voltage. Further, in this paper, the detailed study of threshold voltage and its variation with the process parameters are presented. A threshold voltage roll-off with fin thickness is observed for both theoretical and experimental results. The fin thickness is varied from 10 nm to 60 nm. The percentage roll-off for our model is 77% and that for experimental result it is 75%. Form the analysis of source/drain (S/D) resistance, it is observed that for a fixed fin width, as the channel length increases, there is an enhancement in the parasitic S/D resistance. This can be inferred from the fact that as the channel length decreases, quantum confinement along the S/D direction becomes more extensive. For our proposed devices a close match is obtained with the results through the analytical model and reported experimental results, thereby validating our proposed QM analytical model for DG FinFET device.     

Pentacene thin-film transistors with sol-gel derived amorphous Ba0.6Sr0.4TiO3 gate dielectric

An amorphous Ba_0.6Sr_0.4TiO₃ (BST) film with the thickness of 200 nm was deposited on indium-tin-oxide (ITO)-coated glass substrate through sol-gel route and post-annealing at 500 °C. The dielectric constant of the BST film was determined to be 20.6 at 100 kHz by measuring the Ag/BST/ITO parallel plate capacitor, and no dielectric tunability was observed with the bias voltage varying from −5 to 5 V. The BST film shows a dense and uniform microstructure as well as a smooth surface with the root-mean-square (RMS) roughness of about 1.4 nm. The leakage current density was found to be 3.5 × 10⁻⁸ A/cm² at an applied voltage of −5 V. The transmittance of the BST/ITO/glass structure is more than 70% in the visible region. Pentacene based transistor using the as-prepared BST film as gate insulator exhibits a low threshold voltage of −1.3 V, the saturation field-effect mobility of 0.68 cm²/Vs, and the current on/off ratio of 3.6 × 10⁵. The results indicate that the sol-gel derived BST film is a promising high-k gate dielectric for large-area transparent organic transistor arrays on glass substrate.     

Submicron-meter tunneling field-effect poly-Si thin-film transistors with a thinned channel layer

Submicron-meter poly-Si tunneling-effect thin-film transistor (TFT) devices with a thinned channel layer have been investigated. With reducing the gate length to be shorter than 1 μm, the poly-Si TFT device with conventional MOSFET structure is considerably degraded. The tunneling field-effect transistor (TFET) structure can be employed to alleviate the short channel effect, thus largely suppressing the off-state leakage. However, for a poly-Si channel layer of 100 nm thickness, the TFET structure causes a small on-state current, which may not provide well sufficient driving current. By reducing the channel layer thickness to be 20 nm, the on-state current for the TFET structure can be largely increased, due to the enhanced bending of energy band for a thinned channel layer. As a result, for the TFET poly-Si TFTs at a gate bias of 5 V and a drain bias of 3 V, a 20-nm channel layer leads to an on-state current of about 1 order larger than that by a 100-nm channel layer, while still keeping an off-state leakage smaller than 0.1 pA/μm. Accordingly, the submicron-meter TFET poly-Si TFT devices with a thinned channel layer would show good feasibility for implementing high packing density of poly-Si TFT devices.     

Titanium-aluminum oxynitride (TAON) as high-k gate dielectric for sub-32 nm CMOS technology

High-k insulators for the next generation (sub-32 nm CMOS (complementary metal-oxide-semiconductor) technology), such as titanium-aluminum oxynitride (TAON) and titanium-aluminum oxide (TAO), have been obtained by Ti/Al e-beam evaporation, with additional electron cyclotron resonance (ECR) plasma oxynitridation and oxidation on Si substrates, respectively. Physical thickness values between 5.7 and 6.3 nm were determined by ellipsometry. These films were used as gate insulators in MOS capacitors fabricated with Al electrodes, and they were used to obtain capacitance-voltage (C-V) measurements. A relative dielectric constant of 3.9 was adopted to extract the equivalent oxide thickness (EOT) of films from C-V curves under strong accumulation condition, resulting in values between 1.5 and 1.1 nm, and effective charge densities of about 10¹¹ cm⁻². Because of these results, nMOSFETs with Al gate electrode and TAON gate dielectric were fabricated and characterized by current-voltage (I-V) curves. From these nMOSFETs electrical characteristics, a sub-threshold slope of 80 mV/dec and an EOT of 0.87 nm were obtained. These results indicate that the obtained TAON film is a suitable gate insulator for the next generation (MOS) devices.     

Enhanced electrical and photosensing properties of pentacene organic thin-film phototransistors by modifying the gate dielectric thickness

The effects of dielectric layer thickness on the electrical performance and photosensing properties of organic pentacene thin-film transistors have been investigated. To improve the electrical performance of pentacene thin-film transistors (TFTs), the poly-4-vinylphenol (PVP) polymer with various thicknesses was used in fabrication of the pentacene transistors. The pentacene thin-film transistor with the PVP dielectric layer of 70 nm exhibited a field-effect mobility of 4.46 cm²/Vs in the saturation region, a threshold voltage of −4.0 V, a gate voltage swing of 2.1 V/decade and an on/off current ratio of 5.1 × 10⁴. In the OFF-state, the photoresponse of the transistors increases linearly with illumination intensity. The pentacene transistor with the thinner dielectric layer thickness indicates the best photosensing behavior. It is evaluated that the electrical performance and photosensing properties of pentacene thin-film transistors can be improved by using various thickness dielectric layer.     

Oxide thickness dependence of plasma charging damage

Charging damage induced in oxides with thickness ranging from 8.7 to 2.5 nm is investigated. Results of charge-to-breakdown (Q_bd) measurements performed on control devices indicate that the polarity dependence increases with decreasing oxide thickness at both room and elevated temperature (180°C) conditions. As the oxide thickness is thinned down below 3 nm, the Q_bd becomes very sensitive to the stressing current density and temperature. Experimental results show that severe antenna effect would occur during plasma ashing treatment in devices with gate oxides as thin as 2.6 nm. It is concluded that high stressing current level, negative plasma charging, and high process temperature are key factors responsible for the damage.     

Improved self-gain in deep submicrometer strained silicon-germanium pMOSFETs with HfSiOx/TiSiN gate stacks

The self-gain of surface channel compressively strained SiGe pMOSFETs with HfSiO_x/TiSiN gate stacks is investigated for a range of gate lengths down to 55 nm. There is 125% and 700% enhancement in the self-gain of SiGe pMOSFETs compared with the Si control at 100 nm and 55 nm lithographic gate lengths, respectively. This improvement in the self-gain of the SiGe devices is due to 80% hole mobility enhancement compared with the Si control and improved electrostatic integrity in the SiGe devices due to less boron diffusion into the channel. At 55 nm gate length, the SiGe pMOSFETs show 50% less drain induced barrier lowering compared with the Si control devices. Electrical measurements show that the SiGe devices have larger effective channel lengths. It is shown that the enhancement in the self-gain of the SiGe devices compared with the Si control increases as the gate length is reduced thereby making SiGe pMOSFETs with HfSiO_x/TiSiN gate stacks an excellent candidate for analog/mixed-signal applications.     

Effects of the Ag content on the geometrical and electrical characteristics of the screen-printed etched gate electrodes of OTFTs using Ag ink

During the fabrication of gate electrodes by Ag ink screen-printing combined with a wet-etching process, the effects of the Ag content on the geometrical and electrical characteristics such as the thickness and surface roughness of gate electrode, step coverage with the gate dielectric, leakage current associated with the step coverage, and the electrical performance of organic thin film transistors (OTFTs) were investigated. An increase of Ag content resulted in the thick and densely-packed Ag electrode, which had a stable and excellent conductivity. But, the large thickness of Ag electrode caused the worse step coverage of PVP (polyvinylphenol) dielectric layer on the edge of the Ag gate electrode, therefore, for Ag contents more than 40 wt.%, MIM (metal-insulator-metal) devices and OTFTs with the Ag gate electrodes had very large leakage current (>10⁻⁴ A/cm²) and off-state current (>∼19 pA/μm) due to the poor step coverage of PVP dielectric layers, respectively. Finally, we found that an Ag content of 20-30 wt.% was suitable for the screen-printed etched gate electrode of OTFTs using Ag ink. This range generated a mobility of 0.18 cm²/V s, an on/off current of 5 × 10⁶, and an off-state current of 0.002 pA/μm, which are suitable to drive e-paper.     

FinFET for high sensitivity ion and biological sensing applications

A double-gate (DG) fin field effect transistor (FinFET) is discussed as new label-free ion and biological sensor. Simulations as function of channel doping, geometrical dimensions, operation point and materials investigated the device response to an external potential difference which provides a body threshold voltage modulation. The simulation results presented in this work clearly state the key features for an ultrasensitive FET based sensor: an enhancement low doped and partially gated transistor operating in weak-moderate inversion regime. The optimized sensitivity, obtained when the width of the fin is equal to the gate height (w_NW ∼ h_g), reaches a value of 85% for an extraction current, I_d, of 0.1 μA. These results pave the way for the fabrication process of an innovative CMOS compatible sensing system.     

Effect of the interface states on the cell parameters of a thin film quasi-monocrystalline porous silicon as an active layer

Unlike crystalline silicon, quasi-monocrystalline porous silicon (QMPS) layers have a top surface with small voids in the body. What is more pertinent to the present study is the fact that, at a given wavelength of interest for solar cells, these layers are often reported, in the literature, to have a higher absorption coefficient than crystalline silicon. The present study builds on existing literature, suggesting an analytical model that simulates the performance of an elementary thin QMPS (as an active layer) solar cell. Accordingly, the effects that the interface states located at the void-silicon interface and that the porosity of this material have on the cell parameters are investigated. Furthermore, the effects of the optimum base doping, QMPS thickness, and porosity on the photovoltaic parameters were taken into consideration. The results show that the optimum base doping depends on the QMPS thickness and porosity. For an 8 μm thickness, the film QMPS layer gives a 35.4 mA/cm² for short-circuit current density, 15% for conversion efficiency, and 527 mV for open-circuit voltage when the value of the interface states is about 10¹² cm⁻² and the base doping is about 2×10¹⁸ cm⁻³ under AM 1.5 conditions.     

Source/drain optimization of underlapped lightly doped nanoscale double-gate MOSFETs

The impact of the spacer length at the source (L_s) and drain (L_d) on the performance of symmetrical lightly-doped double-gate (DG) MOSFET with gate length L = 20 nm is analyzed, with the type and doping concentration of the spacers kept the same as in the channel material. Using the transport parameters extracted from experimental data of a double-gate FinFET, simulations were performed for optimization of the underlapped gate-source/drain structure. The simulation results show that the subthreshold leakage current is significantly suppressed without sacrificing the on-state current for devices designed with asymmetrical source/drain extension regions, satisfying the relations L_s = L/2 and L_d = L. In independent drive configuration, the top-gate response can be altered by application of a control voltage on the bottom-gate. In devices with asymmetrical source/drain extension regions, simulations demonstrate that the threshold voltage controllability is improved when the drain extension region length is increased.     

GaN基HEMT器件结构设计及其性能仿真北大核心

利用Silvaco TCAD器件模拟软件研究了AlGaN/GaN高电子迁移率晶体管(HEMT)器件势垒层的厚度、沟道宽长比和掺杂浓度对器件的转移特性和跨导曲线的影响。结果表明,器件势垒层厚度的变化可以调节器件的电流开关比和开启电压,实现由耗尽型器件向增强型器件的转变;沟道宽长比的改变可以调节器件的开启电压,并且随着沟道宽长比的增加,栅极电压控制量子阱中二维电子气的能力增强;势垒层适量掺杂提高了输出电流,并且使跨导的峰值增大,但过度掺杂会造成器件不易关断情况出现。