MOS field threshold increase by phosphorus-implanted field

The threshold voltage of the field regions of p-channel Si gate devices can be controllably increased by phosphorus ion implantation prior to field oxidation without any additional masking step. For a 1.25-µ field oxide thickness, an increase of more than 20 V in intermediate field threshold can be achieved without lowering junction breakdown voltage.     

TaSi2gate for VLSI CMOS circuits

It is shown, that lateral shrinkage of 2-µm CMOS devices and reduction of the gate oxide thickness to about 20 nm is significantly facilitated by replacing the n⁺-poly-Si or polycide gates by TaSi2. Due to its higher work function, TaSi2allows the simultaneous reduction of the channel doping in the n-channel and the charge compensation in the p-channel without changing the threshold voltages. Thus compared with n⁺-poly-Si gate n-channel transistors substrate sensitivity and substrate current are reduced, and low-level breakdown strength is raised. In p-channel transistors, the subthreshold current behavior and UT(L)-dependence are improved. Consequently, the channel length of both n- and p-channel transistors can be reduced by about 0.5 µm without significant degradation. The MOS characteristics Nss, flatband and threshold voltage stability, and dielectric strength appear similar for TaSi2and n+-poly Si gate transistors.     

Effects of ionizing radiation on SOI/CMOS Devices fabricated in zone-melting-recrystallized Si films on SiO2

The effects of ionizing radiation on SOI/CMOS devices fabricated in zone-melting-recrystallized Si films on SiO2-coated Si substrates have been investigated as a function of the negative bias applied to the substrate during irradiation and measurement. For these devices, which have a thin gate oxide 10 nm thick, the optimum substrate bias is - 5 V. For total doses up to 10⁷rad(Si), with this bias they exhibit low subthreshold leakage currents (<0.2-pA/µm channel width), small threshold voltage shifts (<-0.18 V for n-channel devices and <-0.46 V for p-channel devices) and very little transconductance degradation (<5 percent).     

Fabrication of SOS MOSFETs using two-step doping with excimer laser

Using two-step doping with excimer laser, p-channel MOSFETs were fabricated in thin silicon films on sapphire (SOS). Source and drain p ⁺ layers were formed using two-step doping with only one melting pulse of excimer laser. Devices were processed at room temperature except for the LPCVD gate oxide deposition at 450°C. High-quality thin film transistors (TFTs) were fabricated with on/off current ratio of 7 and a field effect hole mobility of 145 cm²/V s     

Edge hole direct tunneling leakage in ultrathin gate oxidep-channel MOSFETs

This paper examines the edge direct tunneling (EDT) of holes from p⁺ polysilicon to underlying p-type drain extensions in off-state p-channel MOSFETs having ultrathin gate oxides that are 1.2 nm-2.2 nm thick. It is for the first time found that for thinner oxides, hole EDT is more pronounced than both conventional gate-induced drain leakage (GIDL) and gate-to-channel tunneling. As a result, the induced gate and drain leakage is more accurately measured per unit gate width. Terminal currents versus input voltage are measured from a CMOS inverter with gate oxide thickness T_OX=1.23 nm, exhibiting the impact of EDT in two standby modes. For the first time, a physical model is derived for the oxide field E_OX at the gate edge by accounting for the heavy and light holes' subbands in the quantized accumulation polysilicon surface. This model relates E_OX to the gate-to-drain voltage, oxide thickness, and doping concentration of the drain extension. Once E_OX is known, an existing direct tunneling (DT) model consistently reproduces EDT current-voltage (I-V), and the tunneling path size extracted falls adequately within the gate-to-drain overlap region. The ultimate oxide thickness limit due to hole EDT is projected     

P-channel MOSFET's with ultrathin N2O gate oxides

The performance and reliability of p-channel MOSFETs utilizing ultrathin (~62 Å) gate dielectrics grown in pure N₂O ambient are reported. Unlike (reoxidized) NH₃-nitrided oxide devices, p-MOSFETs with N₂O-grown oxides show improved performance in both linear and saturation regions compared to control devices with gate oxides grown in O₂. Because both electron and hole trapping are suppressed in N₂O-grown oxides, the resulting p-MOSFETs show considerably enhanced immunity to channel hot-electron and -hole-induced degradation (e.g., hot-electron-induced punchthrough)     

p-Channel MOSFET's in LPCVD PolySilicon

p-channel MOSFET's have been fabricated in LPCVD polysilicon. A 5000-Å n⁺poly acts as the gate electrode on which a 500-Å thermal oxide is grown to act as the gate insulator. Then a 1500-Å LPCVD polysilicon layer is deposited at 620°C and is subsequently boron doped to form the conductive channel. Devices with channel length as small as 2 µm show well-behaved transistor characteristics. The drive current and leakage current are as suitable for usage as load element in memory applications. At large gate voltages the accumulation hole mobility is 9 cm²/V.s. The drain-to-source breakdown voltage exceeds -20 V.     

Quantum-well p-channel AlGaAs/InGaAs/GaAs heterostructureinsulated-gate field-effect transistors with very high transconductance

Quantum-well p-channel pseudomorphic AlGaAs/InGaAs/GaAs heterostructure insulated-gate field-effect transistors with enhanced hole mobility are described. The devices exhibit room-temperature transconductance, transconductance parameter, and maximum drain current as high as 113 mS/mm, 305 mS/V/mm, and 94 mA/mm, respectively, in 0.8-μm-gate devices. Transconductance, transconductance parameter, and maximum drain current as high as 175 mS/mm, 800 mS/V/mm, and 180 mA/mm, respectively were obtained in 1-μm p-channel devices at 77 K. From the device data hole field-effect mobilities of 860 cm²/V-s at 300 K and 2815 cm²/V-s at 77 K have been deduced. The gate current causes the transconductance to drop (and even to change sign) at large voltage swings. Further improvement of the device characteristics may be obtained by minimizing the gate current. To this end, a type of device structure called the dipole heterostructure insulated-gate field-effect transistor is proposed     

Shielded silicon gate complementary MOS integrated circuit

An electrostatic shield for complementary MOS integrated circuits was developed to minimize the adverse effects of stray electric fields created by the potentials in the metal interconnections. The process is compatible with silicon gate technology. n-doped polycrystalline silicon was used for all the gates and the shield. The effectiveness of the shield was demonstrated by constructing a special field plate over certain transistors. The threshold voltages obtained on a oriented silicon substrate ranged from 1.5 to 3 V for either channel. Integrated inverters performed satisfactorily from 3 to 15 V, limited at the low end by the threshold voltages and at the high end by the drain breakdown voltage of the n-channel transistors. The stability of the new structure with an n-doped silicon gate as measured by the shift inC-Vcurve under 200°C ± 20 V temperature-bias conditions was better than conventional aluminum gate or p-doped silicon gate devices, presumably due to the doping of gate oxide with phosphorous. The advantages of the new structure are: avoidance of field inversion, elimination of guard rings, and thinner and more stable oxides.     

IGFET circuit performance-n-channel versus p-channel

The n-channel insulated-gate field-effect transistor offers a factor of 2 to 3.4 mobility advantage (depending on crystal orientation and substrate doping level) over p-channel devices. In addition, several advantages result from the fact that the work function difference between an aluminum gate and the silicon substrate is about -0.8 volt for a p substrate compared with about zero for an n substrate. In particular, this results in a low threshold voltage that allows the use of a substrate bias to adjust the threshold voltage over a useful design range resulting in an added flexibility in choice of thresholds and substrate doping, a reduction in the effect of source-substrate bias on device threshold, decreased junction capacitance, and larger parasitic thick-oxide thresholds for a given insulator thickness. The speed, power, and density advantages of the n-channel device are illustrated for logic and memory circuits using representative n- and p-channel device designs.     

Characteristics and limitation of scaled-down MOSFET's due to two-dimensional field effect

Practical limitations of minimum-size MOS-LSI devices are investigated through measurement of experimental devices. It is assumed that scaled-down MOSFET's are limited by three physical phenomena. These are 1) poor threshold control which is caused by drain electric field, 2) reduced drain breakdown voltage due to lateral bipolar effects, and 3) hot-electron injection into the gate oxide film which yields performance variations during device operation. Experimental models of these phenomena are proposed and the smallest possible MOSFET structure, for a given supply voltage, is considered. It is concluded that the smallest feasible device has a channel length of 0.52 µm and a gate oxide thickness of 9.4 nm when the supply voltage is 1.5 V. Reliable threshold control is most difficult to realize in an MOS-LSI with the smallest devices.     

一种P-GaN栅结合混合帽层结构的HEMT器件

为了进一步提升P-GaN栅HEMT器件的阈值电压和击穿电压,提出了一种具有P-GaN栅结合混合掺杂帽层结构的氮化镓高电子迁移率晶体管(HEMT)。新器件利用混合掺杂帽层结构,调节整体极化效应,可以进一步耗尽混合帽层下方沟道区域的二维电子气,提升阈值电压。在反向阻断状态下,混合帽层可以调节栅极右侧电场分布,改善栅边电场集中现象,提高器件的击穿电压。利用Sentaurus TCAD进行仿真,对比普通P-GaN栅增强型器件,结果显示,新型结构器件击穿电压由593 V提升至733 V,增幅达24%,阈值电压由0.509 V提升至1.323 V。     

Threshold voltage variations with temperature in MOS transistors

Variations with temperature in the threshold voltage of n- and p-channel MOS transistors are obtained by calculation as well as measurement, with the results comparing quite closely. The amount of voltage change per °C under normal operating conditions is found to be dependent upon the channel doping concentration. The calculations show that for either n- or p-channel devices the voltage change per °C is -4 mV/°C for an impurity concentration of 3 × 10¹⁶/cm³and -2 mV/°C for an impurity concentration of 10¹⁵/cm³. This information is important because if the MOS transistor is subjected to a changing temperature environment, the accompanying threshold voltage change may be intolerable.     

High-Performance Metal-Induced Laterally Crystallized Polycrystalline Silicon P-Channel Thin-Film Transistor With $hbox{TaN/HfO}_{2}$ Gate Stack Structure

In this letter, high-performance low-temperature poly-Si p-channel thin-film transistor with metal-induced lateral- crystallization (MILC) channel layer and TaN/HfO₂ gate stack is demonstrated for the first time. The devices of low threshold voltage V_TH ~ 0.095 V, excellent subthreshold swing S.S. ~83 mV/dec, and high field-effect mobility mu_FE ~ 240 cm²/V ldr s are achieved without any defect passivation methods. These significant improvements are due to the MILC channel film and the very high gate-capacitance density provided by HfO₂ gate dielectric with the effective oxide thickness of 5.12 nm.     

应变Si1-xGex沟道PMOSFET空穴局域化研究

为充分利用应变 Si Ge材料相对于 Si较高的空穴迁移率 ,研究了 Si/Si Ge/Si PMOSFET中垂直结构和参数同沟道开启及空穴分布之间的依赖关系。在理论分析的基础上 ,以数值模拟为手段 ,研究了栅氧化层厚度、Si帽层厚度、Si Ge层 Ge组分及厚度、缓冲层厚度及衬底掺杂浓度对阈值电压、交越电压和空穴分布的影响与作用 ,特别强调了 δ掺杂的意义。模拟和分析表明 ,栅氧化层厚度、Si帽层厚度、Si Ge层 Ge组分、衬底掺杂浓度及 δ掺杂剂量是决定空穴分布的主要因素 ,而 Si Ge层厚度、缓冲层厚度和隔离层厚度对空穴分布并不敏感。最后总结了沟道反型及空穴分布随垂直结构及参数变化的一般规律 ,为优化器件设计提供了参考。     

New observation and the modeling of gate and drain currents inoff-state P-MOSFET's

The work reports new observations concerning the gate and drain currents measured at off-state conditions in buried-type p-channel LDD MOSFET devices. Detailed investigation of the observed phenomena reveals that 1) the drain current can be separated into two distinct components: band-to-band tunneling in the gate-to-drain overlap region and collection of holes generated via impact ionization by electrons inside the oxide; and 2) the gate current can be separated into two distinct components: the hot electron injection into the oxide and the Fowler-Nordheim electron tunneling through the oxide, At low negative drain voltage, the dominant component of the drain current is the hole generation inside the oxide. At high negative drain voltage, the drain current is essentially due to band-to-band tunneling, and it is correlated with the hot-electron injection-induced gate current     

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     

Mobility degradation in very thin Oxide p-channel MOSFET's

The effective hole mobility in large-area p-channel MOSFET's decreases systematically over a wide range of oxide fields as the gate oxide thickness decreases from 240 to 31 Å. A scattering mechanism based on the variations of the gate-charge-induced Coulomb scattering potential in the channel resulting from gate oxide thickness and/or structural fluctuations over the gate area is proposed to explain the results.     

p-Channel MOS transistor in indium antimonide

A p-channel MOS transistor in InSb single crystal, operating at 77 K, is described. The source and drain are defined by etching a mesa structure in a cadmium diffused p layer into a tellurium-doped InSb substrate. The gate is formed by evaporation of chromium gold on top of a layer of SiO2, deposited at 215°C. The MOS transistor is characterized by a threshold voltage of -3 V and an effective hole mobility of 330 cm². V^-1.s^-1.