Temperature dependency of 0.1 μm partially depleted SOI CMOSFET

This work investigates the floating body effect (FBE) on the partially depleted SOI devices at various temperatures for high-performance 0.1 μm MOSFET. The thermal effect on the device's characteristics was investigated with respect to the body contacted MOSFET (BC-SOI) and floating body MOSFET without body contacted (FB-SOI). It is found that the threshold voltage (Vth) and the off state drain current (I_OFF) of the BC-SOI devices are more temperature sensitive than those of the FB-SOI devices. For operation at higher temperatures, there is no apparent difference in driving capability between the BC-SOI and FB-SOI MOSFETs     

A room temperature 0.1 μm CMOS on SOI

An advanced 0.1 μm CMOS technology on SOI is presented. In order to minimize short channel effects, relatively thick nondepleted (0.15 μm) SOI film, highly nonuniform channel doping and source-drain extension-halo were used. Excellent short channel effects (SCE) down to channel lengths below 0.1 μm were obtained. It is shown that undepleted SOI results in better short channel effect when compared to ultrathin depleted SOI. Devices with little short channel effect all the way to below 500 Å effective channel length were obtained. Furthermore, utilization of source-drain extension-halo minimizes the bipolar effect inherent in the floating body. These devices were applied to a variety of circuits: Very high speeds were obtained: Unloaded delay was 20 ps, unloaded NAND (FI=FO=3) was 64 ps, and loaded NAND (FI=FO=3, C_L=0.3 pF) delay was 130 ps at supply of 1.8 V. This technology was applied to a self-resetting 512 K SRAM. Access times of 2.5 ns at 1.5 V and 3.5 ns at 1.0 V were obtained     

Threshold voltage sensitivity of 0.1 μm channel lengthfully-depleted SOI NMOSFET's with back-gate bias

We found threshold voltage sensitivity to silicon thickness variation in 0.1 μm channel length fully-depleted SOI NMOSFET's can be reduced with lightly-doped channel and back-gate bias. However, after the back-interface is accumulated, the reduction is small and threshold voltage roll-off due to high drain bias increases     

Investigation on hot-carrier-induced degradation of SOI NLIGBT

The hot-carrier-induced (HCI) degradations of silicon-on-insulator (SOI) lateral insulated gate N-type bipolar transistor (NLIGBT) are investigated in detail by DC voltage stress experiment, TCAD simulation and charge pumping test. The substrate current I_sub and on-state resistance Ron at different voltage stress conditions are measured to assess the HCI effect on device performance. The electric field and impact ionization rate are simulated to assist in providing better physical insights. And charge pumping current is measured to determinate the front-gate interface states density directly. The degradation mechanisms under different gate voltage stress conditions are then presented and summarized.     

Hot-carrier-induced degradation for partially depleted SOI 0.25-0.1 /spl mu/m CMOSFET with 2-nm thin gate oxide

Hot-carrier-induced degradation of partially depleted SOI CMOSFETs was investigated with respect to body-contact (BC-SOI) and floating-body (FB-SOI) for channel lengths ranging from 0.25 down to 0.1 /spl mu/m with 2 nm gate oxide. It is found that the valence-band electron tunneling is the main factor of device degradation for the SOI CMOSFET. In the FB-SOI nMOSFET, both the floating body effect (FBE) and the parasitic bipolar transistor effect (PBT) affect the hot-carrier-induced degradation of device characteristics. Without apparent FBE on pMOSFET, the worst hot-carrier stress condition of the 0.1 /spl mu/m FB-SOI pMOSFET is similar to that of the 0.1 /spl mu/m BC-SOI pMOSFET.     

Radiation source dependence of performance degradation in thin gate oxide fully-depleted SOI n-MOSFETs

The degradation of the electrical performance of thin gate oxide fully depleted SOI n-MOSFETs and its dependence on the radiation particles are investigated. The transistors are irradiated with 7.5-MeV protons and 2-MeV electrons at room temperature without bias. The shift of threshold voltage and the coupling effect with the degraded opposite gate are clarified. A remarkable reduction of the floating body effects is observed after irradiation. The degradation of the extracted parameters is discussed by a comparison with the damage coefficients.     

Electrical stress on irradiated thin gate oxide partially depleted SOI nMOSFETs

The effect of hot-carrier stress on 60 MeV proton irradiated thin gate oxide partially depleted SOI nMOSFETs has been studied. The results are compared with those from the electrical stress of non-irradiated devices. Whereas no significant differences are observed for the front channel degradation, hot-electron trapping in the buried oxide is found to be enhanced in the irradiated devices. This hot-electron trapping leads to a compensation or neutralization of the effects caused by the radiation-induced positive trapped charges. It is shown that a similar hot-electron trapping enhancement can be achieved in non-irradiated devices stressed under certain back gate bias conditions.     

Hot-carrier-induced degradation of drain current hysteresis and transients in thin gate oxide floating body partially depleted SOI nMOSFETs

The impact of hot-carrier degradation on drain current (I_D) hysteresis and switch-off I_D transients of thin gate oxide floating body PD SOI nMOSFETs is analyzed. An extended characterization of these floating body effects (FBEs) is carried out for a wide range of transistor geometries and bias conditions. The results show a link between the hot-carrier-induced damage of the front channel and the reduction of the FBEs. This is further supported by unbiased thermal annealing experiments, which are found to give rise to a partial recovery of the hot-carrier induced damage and FBEs.     

Counter doping into uniformly and heavily doped channel region ofsub-0.1 μm SOI MOSFETs

We proposed counter doping into a heavily and uniformly doped channel region of SOI MOSFETs. This enabled us to suppress the short channel effects with proper threshold voltage V_th and to eliminate parasitic edge or back gate transistors. We derived a model for V_th as a function of the projected range, Rp and dose, Φ_D, of the counter doping, and showed that V_th is invariable even when the as-implanted counter doping profile redistributes. Using this technology, we demonstrated a V_th roll-off free 0.075 μm-L_Geff nMOSFET with low off-state current     

Simulation and two-dimensional analytical modeling of subthresholdslope in ultrathin-film SOI MOSFETs down to 0.1 μm gate length

The subthreshold slope in ultra-thin-film fully depleted SOI MOSFETs is investigated for channel lengths from the long channel region down to 0.1 μm. A doping effect is found which allows improvement of the S-factor by increasing the channel doping concentration. In order to explain this phenomenon and to clarify the mechanism of S -factor degradation at short gate lengths, a two-dimensional analytical model is developed. A modified boundary condition for the two-dimensional Poisson equation is introduced to account for the nonlinear potential distribution inside the buried oxide. It is found that the S-factor short-channel degradation is governed by three mechanisms: the rise of capacitances at the channel source and drain ends due to the two-dimensional potentional distribution; the subthreshold current flow at the back channel surface; and the modulation of the effective current channel thickness during the gate voltage swing in the subthreshold region. The analytical model results are compared to those of numerical device simulation, and a good agreement is found     

Reduced reverse narrow channel effect in thin SOI nMOSFETs

The effects of narrow channel width on the threshold voltage of deep submicron silicon-on-insulator (SOI) nMOSFETs with LOCOS isolation have been investigated. The reverse narrow channel effect (RNCE) in SOI devices is found to be dependent on the thickness of the active silicon film. A thinner silicon film is found to depict less threshold voltage fall-off. These results can be explained by a reduced oxide/silicon interface area in the transistor width direction, thus the boron segregation due to silicon interstitials with high recombination rate is reduced     

Comparative analysis of hot electron injection and induced devicedegradation in scaled 0.1 μm SOI n-MOSFETs using Monte Carlosimulation

A self-consistent Monte Carlo (MC) simulator is employed to investigate and compare hot electron phenomena in three competing design strategies for 0.1 μm SOI n-MOSFETs operating under low voltage conditions, i.e., V_d considerably less than the Si-SiO₂ injection barrier height φ_b. Simulations of these designs reveal that non-local carrier transport effects and two-dimensional current how play a significant role in determining the relative rate and location of hot electron injection into both the front and back oxides. Specifically, simulations indicate that electron-electron interactions near the drain edge are a main source of electron energies exceeding φ_b. The hot electron injection distributions are then coupled with an empirical model to generate interface state distributions at both the front and back oxide interfaces. These interface states are incorporated into a drift-diffusion simulator to examine relative hot-electron-induced device degradation for the three 0.1 μm SOI designs. Simulations suggest that both the Si layer thickness and doping distribution affect device sensitivity to hot-electron-induced interface states. In particular, the simulations show that a decrease in the channel doping results in increased sensitivity to back oxide charge. In the comparison of the heavily-doped designs, the design with a thinner T_Si experiences significantly more hot-electron-induced oxide damage in the back oxide and more degradation from the charged states at the back interface     

Optimization of series resistance in sub-0.2 μm SOI MOSFET's

The optimization of device series resistance in ultrathin film SOI devices is studied through 3-D simulations and process experiments. The series resistance is dependent on the contact resistivity of the silicide to silicon and the silicide geometry. To achieve low series resistance, very thin silicides that do not fully consume the SOI film are needed. A novel cobalt salicidation technology using titanium/cobalt laminates is used to demonstrate sub-0.2 μm, thin-film SOI devices with excellent performance and very low device series resistance     

Optimization of series resistance in sub-0.2 μm SOI MOSFET's

The optimization of device series resistance in ultra-thin film SOI devices is studied through 2-D simulations and process experiments. The series resistance is dependent on the contact resistivity of the silicide to silicon and the silicide geometry. To achieve low series resistance, very thin silicides that do not fully consume the SOI film are needed. A novel cobalt salicidation technology using titanium/cobalt laminates is used to demonstrate sub-0.2 μm, thin-film SOI devices with excellent performance and very low device series resistance     

Experimental high performance sub-0.1 μm channel nMOSFET's

Very high performance sub-0.1 μm channel nMOSFET's are fabricated with 35 Å gate oxide and shallow source-drain extensions. An 8.8-ps/stage delay at V_dd=1.5 V is recorded from a 0.08 μm channel nMOS ring oscillator at 85 K. The room temperature delay is 11.3 ps/stage. These are the fastest switching speeds reported to date for any silicon devices at these temperatures. Cutoff frequencies (f_T) of a 0.08 μm channel device are 93 GHz at 300 K, and 119 GHz at 85 K, respectively. Record saturation transconductances, 740 mS/mm at 300 K and 1040 mS/mm at 85 K, are obtained from a 0.05 μm channel device. Good subthreshold characteristics are achieved for 0.09 μm channel devices with a source-drain halo process     

Technology challenges for integration near and below 0.1 μm

Technology challenges for silicon integrated circuits with a design rule of 0.1 μm and below are addressed. We begin by reviewing the state-of-the-art CMOS technology at 0.25 μm currently in development, covering a logic-oriented processes and dynamic random access memory (DRAM) processes. CMOS transistor structures are compared by introducing a figure of merit. We then examine scaling guidelines for 0.1 μm which has started to deviate for optimized performance from the classical theory of constant-field scaling. This highlights the problem of nontrivial subthreshold current associated with the scaled-down CMOS with low threshold voltages. Interconnect issues are then considered to assess the performance of microprocessors in 0.1 μm technology. 0.1 μm technology will enable a microprocessor which runs at 1000 MHz with 500 million transistors. Challenges below 0.1 μm are then addressed. New transistor and circuit possibilities such as silicon on insulator (SOI), dynamic-threshold (DT) MOSFET, and back-gate input MOS (BMOS) are discussed. Two problems below 0.1 μm are highlighted. They are threshold voltage control and pattern printing. It is pointed out that the threshold voltage variations due to doping fluctuations is a limiting factor for scaling CMOS transistors for high performance. The problem with lithography below 0.1 μm is the low throughput for a single probe. The use of massively parallel scanning probe assemblies working over the entire wafer is suggested to overcome the problem of low throughput     

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     

High performance 0.1 μm gate-length p-type SiGe MODFET's andMOS-MODFET's

High performance p-type modulation-doped field-effect transistors (MODFET's) and metal-oxide-semiconductor MODFET (MOS-MODFET) with 0.1 μm gate-length have been fabricated on a high hole mobility SiGe-Si heterojunction grown by ultrahigh vacuum chemical vapor deposition. The MODFET devices exhibited an extrinsic transconductance (g_m) of 142 mS/mm, a unity current gain cut-off frequency (f_T) of 45 GHz and a maximum oscillation frequency (f_MAX) of 81 GHz, 5 nm-thick high quality jet-vapor-deposited (JVD) SiO₂ was utilized as gate dielectric for the MOS-MODFET's. The devices exhibited a lower gate leakage current (1 nA/μm at V_gs=6 V) and a wider gate operating voltage swing in comparison to the MODFET's. However, due to the larger gate-to-channel distance and the existence of a parasitic surface channel, MOS-MODFET's demonstrated a smaller peak g _m of 90 mS/mm, f_T of 38 GHz, and f_max of 64 GHz. The threshold voltage shifted from 0.45 V for MODFET's to 1.33 V for MOS-MODFET's. A minimum noise figure (NF_min) of 1.29 dB and an associated power gain (G_a) of 12.8 dB were measured at 2 GHz for MODFET's, while the MOS-MODFET's exhibited a NF _min of 0.92 dB and a G_a of 12 dB at 2 GHz. These DC, RF, and high frequency noise characteristics make SiGe/Si MODFET's and MOS-MODFET's excellent candidates for wireless communications     

0.1 μm Schottky-collector AlAs/GaAs resonant tunneling diodes

The Schottky-collector resonant tunneling diode (RTD) is an RTD with the normal N+ collector and ohmic contact replaced by a Schottky contact, thereby eliminating the associated parasitic resistance. With submicron Schottky contact dimensions, the remaining components of the parasitic series resistance can be greatly reduced, resulting in an increased maximum frequency of oscillation, f_max. AlAs/GaAs Schottky-collector RTDs were fabricated using 0.1 μm T-gate technology developed for high electron mobility transistors. From their measured dc and microwave parameters, and including the effect of the quantum well lifetime, f_max=900 GHz is computed     

Experimental 0.1 μm p-channel MOSFET withp+-polysilicon gate on 35 Å gate oxide

Very-high-transconductance 0.1 μm surface-channel pMOSFET devices are fabricated with p⁺-poly gate on 35 Å-thick gate oxide. A 600 Å-deep p⁺ source-drain extension is used with self-aligned TiSi₂ to achieve low series resistance. The saturation transconductances, 400 mS/mm at 300 K and 500 mS/mm at 77 K, are the highest reported to date for pMOSFET devices