A dynamic threshold voltage MOSFET (DTMOS) for very low voltageoperation

A new mode of operation for Silicon-On-Insulator (SOI) MOSFET is experimentally investigated. This mode gives rise to a Dynamic Threshold voltage MOSFET (DTMOS). DTMOS threshold voltage drops as gate voltage is raised, resulting in a much higher current drive than regular MOSFET at low V_dd. On the other hand, V_t is high at V_gs =0, thus the leakage current is low. Suitability of this device for ultra low voltage operation is demonstrated by ring oscillator performance down to V_dd=0.5 V     

Enhancement-Mode GaAs MOSFETs With an In0.3 Ga0.7As Channel, a Mobility of Over 5000 cm2/V ·s, and Transconductance of Over 475 μS/μm

We present metal-gate high-k-dielectric enhancement-mode (e-mode) III-V MOSFETs with the highest reported effective mobility and transconductance to date. The devices employ a GaGdO high-k (k = 20) gate stack, a Pt gate, and a delta-doped InGaAs/AlGaAs/GaAs hetero-structure. Typical 1-mum gate length device figures of merit are given as follows: saturation drive current, I_d,sat = 407 muA/mum; threshold voltage, V_t = +0.26 V; maximum extrinsic transconductance, g_m = 477 muS/mum (the highest reported to date for a III-V MOSFET); gate leakage current, I_g = 30 pA; subthreshold swing, S = 102 mV/dec; on resistance, R_on = 1920 Omega-mum; I_on/I_off ratio = 6.3 x 10⁴; and output conductance, g_d = 11 mS/mm. A peak electron mobility of 5230 cm²/V. s was extracted from low-drain-bias measurements of 20 mum long-channel devices, which, to the authors' best knowledge, is the highest mobility extracted from any e-mode MOSFET. These transport and device data are highly encouraging for future high-performance n-channel complementary metal-oxide-semiconductor solutions based on III-V MOSFETs.     

Threshold voltage-minimum gate length trade-off in buried channelPMOS devices for scaled supply voltage CMOS technologies

The trade-off between threshold voltage (V_th) and the minimum gate length (L_min) is discussed for optimizing the performance of buried channel PMOS transistors for low voltage/low power high-speed digital CMOS circuits. In a low supply voltage CMOS technology it is desirable to scale V_th and L_min for improved circuit performance. However, these two parameters cannot be scaled independently due to the channel punch-through effect. Statistical process/device modeling, split lot experiments, circuit simulations, and measurements are performed to optimize the PMOS transistor current drive and CMOS circuit speed. We show that trading PMOS transistor V_th for a smaller L_min results in faster circuits for low supply voltage (3.3 to 1.8 V) n⁺-polysilicon gate CMOS technology, Circuit simulation and measurements are performed in this study. Approximate empirical expressions are given for the optimum buried channel PMOS transistor V _th for minimizing CMOS circuit speed for cases involving: (1) constant capacitive load and (2) load capacitance proportional to MOS gate capacitance. The results of the numerical exercise are applied to the centering of device parameters of a 0.5 μm 3.3 V CMOS technology that (a) matches the speed of our 0.5 μm 5 V CMOS technology, and (b) achieves good performance down to 1.8 V power supply. For this process the optimum PMOS transistor V_th (absolute value) is approximately 0.85-0.90 V     

Impact of boron penetration at P+-poly/gate oxideinterface on deep-submicron device reliability for dual-gate CMOStechnologies

In this paper, we investigate the onset of boron penetration at the P⁺-poly/gate oxide interface. It is found that conventional detection methods such as shifts in flatband voltage or threshold voltage (V_t) and charge-to-breakdown (Q_BD) performance in accumulation mode failed to reveal boron species near this interface. On the contrary, under constant current stressing with inversion mode bias conditions, significantly lower Q_BD and large V_t shift have been observed due to boron penetration near the P⁺-poly/gate oxide interface. These results suggest that onset of boron penetration at the P⁺ -poly/gate oxide interface does not alter fresh device characteristics, but it induces severe reliability degradation for the gate oxide. Tradeoffs of boron penetration and poly depletion are also studied in this work with different combinations of polysilicon thickness, BF₂ implant energy and dose, and the post-implant RTA temperature     

1200V大容量SiC MOSFET器件研制

采用平面栅MOSFET器件结构,结合优化终端场限环设计、栅极bus-bar设计、JFET注入设计以及栅氧工艺技术,基于自主碳化硅工艺加工平台,研制了1200V大容量SiC MOSFET器件.测试结果表明,器件栅极击穿电压大于55V,并且实现了较低的栅氧界面态密度.室温下,器件阈值电压为2.7V,单芯片电流输出能力达到50A,器件最大击穿电压达到1600V.在175℃下,器件阈值电压漂移量小于0.8V;栅极偏置20V下,泄漏电流小于45nA.研制器件显示出优良的电学特性,具备高温大电流SiC芯片领域的应用潜力.     

The impact of device scaling and power supply change on CMOS gateperformance

Based a new empirical mobility model that is solely dependent on V _gs, V_t, and T_ox and a corresponding saturation drain current (I_dsat) model, the impact of device scaling and power supply voltage change on CMOS inverter's performance is investigated in this paper. It shows that the T_ox which maximizes inverter's speed may be thicker than reliability consideration requires. In addition, very high speed can be achieved even at low V_dd (for low power applications) if V_t can be lowered     

CMOS Integration of Dual Work Function Phase-Controlled Ni Fully Silicided Gates (NMOS:NiSi, PMOS:Ni2Si, and Ni31Si12) on HfSiON

The CMOS integration of dual work function (WF) phase-controlled Ni fully silicided (FUSI) gates on HfSiON was investigated. For the first time, the integration of NiSi FUSI gates on n-channel MOS (NMOS) and Ni₃₁Si₁₂ FUSI gates on p-channel MOS (PMOS) with good V_t control to short gate lengths (L_G=50 nm, linear V_t of 0.49 V for NMOS, and -0.37 V for PMOS) is demonstrated. A poly-Si etch-back step was used to reduce the poly-Si height on PMOS devices, allowing for the linewidth-independent formation of NiSi on NMOS and Ni-rich silicides on PMOS with a two-step rapid thermal processing (RTP) silicidation process. The process space for the scalable formation of NiSi on NMOS and Ni₂Si or Ni₃₁ Si₁₂ on PMOS devices was investigated. It was found that within the process window for linewidth-independent NiSi FUSI formation on 100-nm poly-Si NMOS devices, it is possible to control the silicide formation on PMOS devices by adjusting the poly-Si etch-back and RTP1 conditions to obtain either Ni₂Si or Ni₃₁Si₁₂ FUSI gates. A reduction in the PMOS threshold voltage of 90 mV and improved device performance (18% I_on improvement at I_off=100 nA/mum) was obtained for Ni ₃₁Si₁₂ compared to Ni₂Si FUSI gates, as well as a V_t reduction of 350 mV when compared to a single WF flow using NiSi FUSI gates on PMOS     

Hot-carrier effects and lifetime prediction in off-state operationof deep submicron SOI N-MOSFETs

Hot-carrier effects (HCE) induced by the parasitic bipolar transistor (PBT) action are thoroughly investigated in deep submicron N-channel SOI MOSFETs for a wide range of temperature and gate length. A multistage device degradation is highlighted for all the experimental conditions. Original V_t variations are also obtained for short-channel devices, a reduction of the threshold voltage being observed for intermediate values of stress time in the case of high stress drain biases. At low temperature (LT), an improvement of the device aging can be obtained in the low V_d range because of the significant reduction of the leakage current in the PBT regime. However, in the case of high V_d, since the strong leakage current cannot be suppressed at LT, the device aging is larger than that obtained at room temperature. On the other hand, the device lifetime in off-state operation is carefully predicted as a function of gate length with various methods. Numerical simulations are also used in order to propose optimized silicon-on-insulator (SOI) architectures for alleviating the PBT action and improving the device performance and reliability     

工作在动态阈值MOS的特性研究

通过将衬底和栅极连接在一起实现了MOSFET的动态阈值,DTMOS与标准的MOSFET相比具有更高的迁移率,在栅极电压升高时DTMOS阈值电压会随之降低,从而获得了比标准的MOSFET大的电流驱动能力。DTMOS是实现低电压、低功耗的一种有效手段。     

High-Performance Inversion-Type Enhancement-Mode InGaAs MOSFET With Maximum Drain Current Exceeding 1 A/mm

High-performance inversion-type enhancement- mode (E-mode) n-channel In_0.65Ga_0.35As MOSFETs with atomic-layer-deposited Al₂O₃ as gate dielectric are demonstrated. A 0.4-mum gate-length MOSFET with an Al₂O₃ gate oxide thickness of 10 nm shows a gate leakage current that is less than 5 times 10^-6 A/cm² at 4.0-V gate bias, a threshold voltage of 0.4 V, a maximum drain current of 1.05 A/mm, and a transconductance of 350 mS/mm at drain voltage of 2.0 V. The maximum drain current and transconductance scale linearly from 40 mum to 0.7 mum. The peak effective mobility is ~1550 cm²/V ldr s at 0.3 MV/cm and decreases to ~650 cm²/V ldr s at 0.9 MV/cm. The obtained maximum drain current and transconductance are all record-high values in 40 years of E-mode III-V MOSFET research.     

Research for radiation-hardened high-voltage SOI LDMOS

Based on the silicon-on-insulator (SOI) technology and radiation-hardened silicon gate (RSG) process, a radiation-hardened high-voltage lateral double-diffused MOSFET (LDMOS) device is presented in this paper. With the gate supply voltage of 30 V, the LDMOS device has a gate oxide thickness of 120 nm, and the RSG process is effective in reducing the total ionizing dose (TID) radiation-induced threshold voltage shift. The p-type ion implantation process and gate-enclosed layout topology are used to prevent radiation-induced leakage current through a parasitic path under the bird's beak and at the deep trench corner, and the device is compatible with high-voltage SOI CMOS process. In the proposed LDMOS, the total ionizing dose radiation degradation for the ON bias is more sensitive than the OFF bias. The experiment results show that the SOI LDMOS has a negative threshold voltage shift of 1.12 V, breakdown voltage of 135 V, and off-state leakage current of 0.92 pA/μm at an accumulated dose level of 100 krad (Si).     

Analytical models for n+-p+ double-gate SOIMOSFET's

Previously, we proposed n⁺-p⁺ double-gate SOI MOSFET's, which have n⁺ polysilicon for the back gate and p⁺ polysilicon for the front gate to enable adjustment of the threshold voltage, and demonstrated high speed operation. In this paper, we establish analytical models for this device, This transistor has two threshold voltages related to n⁺ and p⁺ polysilicon gates: V_th1 and V_th2, respectively. V _th1 is a function of the gate oxide thickness t_Ox and SOI thickness t_Si and is about 0.25 V when t_Ox/t_Si=5, while V_th2 is insensitive to t_Ox and t_Si and is about 1 V. We also derive models for conduction charge and drain current and verified their validity by numerical analysis. Furthermore, we establish a scaling theory unique to the device, and show how to design the device parameters with decreasing gate length. We show numerically that we can design sub 0.1 μm gate length devices with an an appropriate threshold voltage and an ideal subthreshold swing     

Fabrication of Self-Aligned Enhancement-Mode $ hbox{In}_{0.53}hbox{Ga}_{0.47}hbox{As}$ MOSFETs With $ hbox{TaN/HfO}_{2}hbox{/AlN}$ Gate Stack

In this letter, we report the fabrication and characterization of self-aligned inversion-type enhancement-mode In_0.53Ga_0.47As metal-oxide-semiconductor field-effect transistors (MOSFETs). The In_0.53Ga_0.47As surface was passivated by atomic layer deposition of a 2.5-nm-thick AIN interfacial layer. In_0.53Ga_0.47As MOS capacitors showed an excellent frequency dispersion behavior. A maximum drive current of 18.5 muA/mum was obtained at a gate overdrive of 2 V for a MOSFET device with a gate length of 20 mum. An I_on/_off ratio of 104, a positive threshold voltage of 0.15 V, and a subthreshold slope of ~165 mV/dec were extracted from the transfer characteristics. The interface-trap density is estimated to be ~7-8 times 10¹² cm^-2 ldr eV^-1 from the subthreshold characteristics of the MOSFET.     

Electrical Properties of nMOSFETs Using the NiSi:Yb FUSI Electrode

In this letter, nMOSFETs using a NiSi:Yb fully silicide (FUSI) electrode are demonstrated for the first time. We report that the integration of NiSi:Yb FUSI into our reference n-FETs with the respective SiON / HfSiON gate dielectrics results in a V_t reduction from 0.55/0.52 down to 0.30/0.43 V, without degradation of the gate dielectric integrity, channel interface states, and long channel device mobility     

A dual-mode NAND flash memory: 1-Gb multilevel and high-performance512-Mb single-level modes

A 116.7-mm² NAND flash memory having two modes, 1-Gb multilevel program cell (MLC) and high-performance 512-Mb single-level program cell (SLC) modes, is fabricated with a 0.15-μm CMOS technology. Utilizing simultaneous operation of four independent banks, the device achieves 1.6 and 6.9 MB/s program throughputs for MLC and SLC modes, respectively. The two-step bitline setup scheme suppresses the peak current below 60 mA. The wordline ramping technique avoids program disturbance. The SLC mode uses the 0.5-V incremental step pulse and self-boosting program inhibit scheme to achieve high program performance, and the MLC mode uses 0.15-V incremental step pulse and local self-boosting program inhibit scheme to tightly control the cell threshold voltage V_th distributions. With the small wordline and bitline pitches of 0.3-μm and 0.36-μm, respectively, the cell V_th shift due to the floating gate coupling is about 0.2 V. The read margins between adjacent two program states are optimized resulting in the nonuniform cell V_th distribution for MLC mode     

Simulation of a high performance MOSFET with a quantum wirestructure incorporating a periodically bent Si-SiO2 interface

A MOSFET using a serrated quantum wire structure that produces one-dimensional electron confinement shows excellent subthreshold characteristics and enhanced drive capability compared to a conventional MOSFET with a flat Si-SiO₂ interface. We studied the quantum wire structure with its periodically bent Si-SiO₂ interface using simulations. The potential in the convex regions of the silicon is 0.34 V higher than that in the concave ones when the bending angle is 90°, the bending period is 100 nm, substrate doping is 3.0×10 ¹⁷ cm^-3, and a gate voltage is 0.1 V. Because of this increase in potential in the convex regions, electrons are confined in a narrow width of 13 nm in the convex regions. This 1-D electron confinement effect by the bent Si-SiO₂ interface is clearly observed at low gate voltage and is reduced as the gate voltage becomes higher. Due to the confinement effect, drain current in the MOSFET with this quantum wire structure is 270 times higher than that of a MOSFET with a flat Si-SiO₂ interface at a gate voltage of 0.05 V. In addition, the short-channel effect is more effectively suppressed in this MOSFET than in a conventional MOSFET     

Analysis and impact of process variability on performance of junctionless double gate VeSFET

This paper presents an in-depth analysis of junctionless double gate vertical slit FET (JLDG VeSFET) device under process variability. It has been observed that junctionless FETs (JLDG VeSFET) are significantly less sensitive to many process parameter variations due to their inherent device structure and geometric properties. Sensitivity analysis reveals that the slit width, oxide thickness, radius of the device, gate length and channel doping concentration imperceptibly affect the device performance of JLDG VeSFET in terms of variation in threshold voltage, on current, off current and subthreshold slope (Ssub) as compared to its junction based counterpart i.e. MOSFET, because various short channel effects are well controlled in this device. The maximum variation in off current for JLDG VeSFET due to variation in different devices parameters is 5.6% whereas this variation is 38.8% for the MOS junction based device. However, variation in doping concentration in the channel region displays a small deviation in the threshold voltage and on current characteristics of the MOSFET device as compared to JL DG VeSFET.     

A novel 0.1 μm MOSFET structure with inverted sidewall andrecessed channel

To solve the problems of trade-off between the short channel effect and the performance enhancement of sub-quartermicrometer MOSFETs, we have developed a recessed channel MOSFET structure called ISRC (Inverted-Sidewall Recessed-Channel). The oxide thickness is 4 nm and the effective channel length is 0.1 μm, which is the smallest Si-MOSFET ever reported in the recessed channel structures. The maximum saturation transconductance at V_D=2 V is 446 mS/mm for the 0.1 μm n-channel device. The threshold voltage roll-off is kept within 64 mV when the gate length varies from 1.4 μm to 0.1 μm and good subthreshold characteristics are achieved for 0.1 μm channel device     

Comparison of radio frequency physical vapor deposition target material used for LaOx cap layer deposition in 32 nm NMOSFETs

The MOSFET gate length reduction down to 32 nm requires the introduction of a metal gate and a high-K dielectric as gate stack, both stable at high temperature. Here we use a nanometric layer of Lanthanum to shift the device threshold voltage from 500 mV. Because this layer plays a key role in the device performance and strongly depends on its deposition process, we have compared two LaO_x deposition methods in terms of physical properties and influence on electrical NMOS device parameters. Chemical characterizations have shown a different oxidization state according to Lanthanum thickness deposited. It has been related to threshold voltage shift and gate leakage current variations on NMOS transistors. Furthermore mobility extractions have shown that Lanthanum is a cause of mobility degradation.     

Hot-carrier-induced degradation in short p-channel nonhydrogenatedpolysilicon thin-film transistors

The effects of low gate voltage |V_g| stress (V_g =-2.5 V, V_d=-12 V) and high gate voltage |V_g| stress (V_g=V_d=-12 V) on the stability of short p-channel nonhydrogenated polysilicon TFTs were studied. The degradation mechanisms were identified from the evolution with stress time of the static device parameters and the low-frequency drain current noise spectral density. After low |V_g| stress, transconductance overshoot, kinks in the transfer characteristics, and positive threshold voltage shift were observed. Hot-electron trapping in the gate oxide near the drain end and generation of donor-type interface deep states in the channel region are the dominant degradation mechanisms. After high |V_g| stress, transconductance overshoot and "turn-over" behavior in the threshold voltage were observed. Hot-electron trapping near the drain junction dominates during the initial stages of stress, while channel holes are injected into the gate oxide followed by interface band-tail states generation as the stress proceeds