Combined effects of hot-carrier stressing and ionizing radiation inSiO2, NO, and ONO MOSFETs

N-channel MOSFETs with different gate dielectrics, such as silicon dioxide, silicon dioxide annealed in nitrous oxide (NO), and reoxidized nitrided oxide (ONO), were first hot-carrier (HC) stressed and then irradiated to a total dose of 1.5 Mrd. For equal substrate current stressing NO devices have the least degradation, whereas the threshold voltage (V_t) shift due to irradiation is maximum for these devices. For all three types of gate dielectrics the V _t shift due to irradiation of HC stressed devices was higher than that of the unstressed device. However, for ONO devices the V _t shift due to irradiation of the hot-electron stressed (stressing with V_d=V_g=6.5 V) device was less than that of the unstressed device     

Current-crowding effect in diagonal MOSFET's

Electrical and reliability characteristics of diagonally shaped n-channel MOSFETs have been extensively investigated. Compared with the conventional device structure, diagonal MOSFETs show longer device lifetime under peak I_sub condition (V_g =0.5 V_d). However, in the high-gate-bias region (V_g=V_d), diagonal MOSFETs exhibit a significantly higher degradation rate. From the I_sub versus gate voltage characteristics, this larger degradation rate under high gate bias is concluded to be due mainly to the current-crowding effect at the drain corner. For a cell-transistor operating condition (V_g>V_d), this current-crowding effect in the diagonal transistor can be a serious reliability concern     

Si/a-Si:H heterojunction microwave bipolar transistors with cut-offfrequencies ft above 5 GHz

The fabrication of a silicon heterojunction microwave bipolar transistor with an n⁺ a-Si:H emitter is discussed, and experimental results are given. The device provides a base sheet resistance of 2 kΩ/□ a base width 0.1 μm, a maximum current gain of 21 (V_CE=6 V, I_c=15 mA), and an emitter Gummel number G _E of about 1.4×10¹⁴ Scm^-4. From the measured S parameters, a cutoff frequency f_t of 5.5 GHz and maximum oscillating frequency f_max of 7.5 GHz at V_CE=10 V, I_c=10 mA are obtained     

Collector-assisted operation of micromachined field-emitter triodes

The field at the tip of a field emitter triode can be expressed by E=βV_g+_γV _c, where V_g and V_c the gate and collector voltages, respectively. For small gate diameters and tips below or in the plane of the gate and/or large tip-to-collector distances, _γV_c<<βV _g. The-device is operated in the gate-induced field emission mode and the corresponding I-V_c curves are pentode-like. By increasing the gate diameter and/or recessing the gates from the tips, collector-assisted operation can be achieved at reasonable collector voltages. Results are presented for two devices with gate diameters of 3.6 and 2.0 μm. By obtaining γ at different emitter-to-collector distances, I-V_c and transconductance g_m-V_g curves are calculated and compared with experimental results. It is shown that as a consequence of collector-assisted operation, the transconductance of a device can be increased significantly     

Low-power performance of 0.5-μm JFET for low-cost MMIC's inpersonal communications

The low-power microwave performance of an enhancement-mode ion-implanted GaAs JFET is reported. A 0.5-μm×100-μm E-JFET with a threshold voltage of V_th=0.3 V achieved a maximum DC transconductance of g_m=489 mS/mm at V _ds=1.5 V and I_ds=18 mA. Operating at 0.5 mW of power with V_ds=0.5 V and I_ds =1 mA, the best device on a 3-in wafer achieved a noise figure of 0.8 dB with an associated gain of 9.6 dB measured at 4 GHz. Across a 3-in wafer the average noise figure was F_min=1.2 dB and the average associated gain was G_a=9.8 dB for 15 devices measured. These results demonstrate that the E-JFET is an excellent choice for low-power personal communication applications     

New hot-carrier degradation mode in PMOSFETs with W gate electrodes

Hot-carrier degradation of W gate PMOSFETs, which are surface-channel devices because of the work function of W, has been investigated in comparison with polycide (WSi_x/n⁺ poly-Si) ones. In W gate PMOSFETs, transconductance g_m and threshold voltage V_th decrease on the drain avalanche hot-carrier (DAHC) stress, and Δg_m /g_m0 and ΔV_th become minimum at V_G≅V_D/2. By using the charge-pumping technique, it is found that, after stressing at the same stress condition, the interface state density of W gate devices is about 10 times larger than that of polycide ones but the densities of trapped electrons are almost equal. These results indicate that the difference of hot-carrier degradation between W and polycide gate devices is mainly caused by the difference of the interface state density     

A coupled study by floating-gate and charge-pumping techniques ofhot carrier-induced defects in submicrometer LDD n-MOSFET's

The creation of defects by hot-carrier effect in submicrometer (0.85-μm) LDD n-MOSFETs is analyzed by the floating-gate and the charge-pumping techniques. It is emphasized that the floating-gate technique is an attractive tool for characterizing the oxide traps located in the drain-gate overlap region, near the oxide spacer of the LDD structures. This work gives new insight into the creation of acceptorlike oxide traps which are electrically active only after electron injection phases. These defects are generated in the whole stress gate bias range (from V_d/8 to V_d) by hot-hole and/or hot-electron injections, and their generation rates (10^-9 and 10^-2 for electron and hole injections, respectively) are one decade greater than for the interface state generation. Two-dimensional simulations show that they are mainly responsible for the I_d-V_g degradation of the LDD MOSFETs, and that the trap concentrations deduced from charge-pumping experiments are consistent with the I _d-V_g degradation     

High-speed and large noise margin tolerance E/D logic gates withLDD structure DMTs fabricated using selective RIE technology

The authors describe a novel design concept for enhancement (E) and depletion (D) mode FET formation using i-AlGaAs/n-GaAs doped-channel hetero-MISFET (DMT) and a novel self-aligned gate process technology for submicrometer-gate DMT-LSIs based on E/D logic gates. 0.5-μm gate E-DMTs (D-DMTs) with a lightly doped drain (LDD) structure show an average V_t of 0.18 (-0.46) V, a V_t standard deviation of 22.6 (24.9) mV, and a maximum transconductance of 450 (300) mS/mm. The V_t shift is less than 50 mV with a decrease in gate length down to 0.5 μm. The gate forward turn-on voltage V_f is more than 0.9 V, i.e. about 1.6 times that for MESFETs. This superiority in V _f, preserved in the high-temperature range, leads to an improvement in noise margin tolerance by a factor of three. In addition, 31-stage ring oscillators operate with a power consumption of 20 (1.0) mW/gate and a propagation delay of 4.8 (14.5) ps/gate. Circuit simulation based on the experimental data predicts 140 ps/gate and 1 mW/gate for DMT direct-coupled FET logic circuits under standard loading conditions. DMTs and the technology developed here are very attractive for realizing low-power and/or high speed LSIs     

Characterization of oxide trap and interface trap creation duringhot-carrier stressing of n-MOS transistors using the floating-gatetechnique

A technique has been developed to differentiate between interface states and oxide trapped charges in conventional n-channel MOS transistors. The gate current is measured before and after stress damage using the floating-gate technique. It is shown that the change in the I_g-V_g characteristics following the creation and filling of oxide traps by low gate voltage stress shows distinct differences when compared to that which occurs for interface trap creation at mid gate voltage stress conditions, permitting the identification of hot-carrier damage through the I_g- V_g characteristics. The difference is explained in terms of the changes in occupancy of the created interface traps as a function of gate voltage during the I_g-V _g measurements     

A lifetime prediction method for hot-carrier degradation insurface-channel p-MOS devices

Hot carrier degradation of p-MOS devices at low gate voltages (V_g<V_d) is examined. It is shown that the electronic gate current is the principal factor in stress damage in this gate voltage range and that the damage itself consists of trapped electrons, localized close to the drain junction. The saturation of the transconductance change as a function of time which is seen at long stress times of high stress voltages results from a change in the injected gate current as a function of time. This is caused by changes in electric field in the silicon due to charge trapping in the oxide during stress. The saturation effect can, however, be transformed into a simple power law if the time axis is multiplied by the square of the instantaneous gate current. This allows for the development of a lifetime-prediction method. The method is applied to 1.0-μm p-MOS devices, and a lifetime is estimated     

The effect of substrate bias on hot-carrier damage in NMOS devices

Hot-carrier stressing carried out as a function of substrate voltage on 2-μm NMOS devices under bias conditions V_d =8 V and V_g=5.5 V is discussed. The time power-law dependence of stressing changes as a function of substrate bias (V_b), having a power-law gradient of 0.5 for V_b=0 V and 0.3 for V_b=-9 V. Investigation of the type of damage resulting from stressing shows that at V_b=0 V, interface state generation results, while at V_b=-9 V, the damage is mostly by charge trapping. Measurements of the gate current under these two substrate bias conditions show that the gate electron current increases by over two orders of magnitude upon application of a strong back bias. It is suggested that the electron trapping arises from this enhanced gate electron current under large substrate voltage conditions     

Oxide charge buildup and spread-out during channel-hot-carrierinjection in NMOSFETs

Oxide charge buildup during channel-hot-carrier (CHC) injection was investigated by the use of a modified charge-pumping technique. An apparent `turnaround' effect in local oxide charge density during low gate voltage (V_T<V_g<1/2 V_d) stressing was observed. It can be explained by the dynamic evolution of the damage location caused by the continuous changes in the electric field distribution during CHC. Dependence on channel length is also presented     

Application of the floating-gate technique to the study of then-MOSFET gate current evolution due to hot-carrier aging

The evolution of the gate current-voltage (I_g- V_gs) characteristics of n-MOSFETs induced by DC stresses at different gate voltage over drain voltage (V_ds ) ratios is studied by the floating-gate (FG) measurement technique. It is shown that the I_g-V_gs curves are always lowered after aging, and that the kinetics are dependent on the aging conditions. A time power law is representative of the V_gs=V_ds case. It is demonstrated that electron traps are created in the oxide by both hot-hole and hot-electron injection stresses. They are not present in the devices before aging. They can be easily charged and discharged by short electron and hole injections, respectively     

A lifetime prediction method for oxide electron trap damage createdduring hot-electron stressing of n-MOS transistors

Electron trap creation under conditions of hot-electron stress (i.e., stress at V_d=V_g) is examined. It is shown that a relationship exists linking lifetime to the injected gate current and drain current, offering a lifetime prediction method for these types of traps. Comparing this type of damage to interface trap (N_it) creation, it is found that larger energies (approximately 1.5 times that for N_it) are required to generate this defect. It is shown that an extrapolation technique can be used to obtain gate currents at working circuit voltages, extending the prediction of lifetimes for oxide trap creation to low voltages     

Degradation of N2O-annealed MOSFET characteristics inresponse to dynamic oxide stressing

The performance of n-MOSFETs with furnace N₂O-annealed gate oxides under dynamic Fowler-Nordheim bipolar stress was studied and compared with that of conventional oxide (OX). Time-dependent dielectric breakdown at high frequency was shown to be improved for the N₂ O-annealed devices compared with that for devices with OX. In addition, a smaller V_t shift after stress was found for nitrided samples. The shift decreased with increasing stressing frequency and annealing temperature. Measurements of both G_m and D_it revealed a peak frequency at which the degradation was the worst. A hole trapping/migration model has been proposed to explain this     

Electron transport in 0.15-μm gate In0.52Al0.48As/In0.53Ga0.47As HEMT

Magneto-transport and cyclotron resonance measurements were made to determine directly the density, mobility, and the effective mass of the charge carriers in a high-performance 0.15-μm gate In_0.52 Al_0.48As/In_0.53Ga_0.47As high-electron-mobility transistor (HEMT) at low temperatures. At the gate voltage V_G=0 V, the carrier density n _g under the gate is 9×10¹¹ cm^-2, while outside of the gate region n_g=2.1×10¹² cm^-2. The mobility under the gate at 4.2 K is as low as 400 cm²/V-s when V_G<0.1 V and rapidly approaches 11000 cm²/V-s when V_G>0.1 V. The existence of this high mobility threshold is crucial to the operation of the device and sets its high-performance region in V_G>0.1 V     

Gate-length dependence of DC and microwave properties ofsubmicrometer In0.53Ga0.47As HIGFETs

In_0.52Al_0.48As/In_0.53Ga_0.47 As/InP heterostructure insulated-gate field-effect transistors (HIGFETs) with gate lengths from 1.1 and 0.3 μm have been fabricated, and their electrical performance is characterized at DC and microwave frequencies. The refractory-gate self-aligned process, applied to devices with In_0.53Ga_0.47As channels, yields an unprecedented combination of very-high speed and excellent uniformity. HIGFETs with L_g=0.6 μm showed average peak transconductance g_m of 528 mS/mm and unity-current-gain cutoff frequency f_t of 50 GHz. The uniformity of g_m was better than 1%, and the voltage of the g_m peak was uniform to ±30 mV. HIGFETs with L_g=0.3 μm showed f₁ up to 63 GHz, but suffered from serious short-channel effect, due to excessive thickness of the InGaAs channel layer. A self-aligned technique for gate resistance reduction is shown to substantially improve microwave power gain     

Doubly strainedIn0.41Al0.59As/n+-In0.65Ga0.35As HFET with high breakdown voltage

An In_0.41Al_0.59As/n⁺-In_0.65 Ga_0.35As HFET on InP was designed and fabricated, using the following methodology to enhance device breakdown: a quantum-well channel to introduce electron quantization and increase the effective channel bandgap, a strained In_0.41Al_0.59As insulator, and the elimination of parasitic mesa-sidewall gate leakage. The In_0.65Ga_0.35As channel is optimally doped to N_D=6×10¹⁸ cm^-3. The resulting device (L_g=1.9 μm, W_g =200 μm) has f_t=14.9 GHz, f_max in the range of 85 to 101 GHz, MSG=17.6 dB at 12 GHz V_B=12.8 V, and I_D(max)=302 mA/mm. This structure offers the promise of high-voltage applications at high frequencies on InP     

Dependence of ionization current on gate bias in GaAs MESFETs

The nonmonotonic behavior of gate current I_g as a function of gate-to-source voltage V_gs is reported for depletion-mode double-implant GaAs MESFETs. Experiments and numerical simulations show that the main contribution to I_g (in the range of drain biases studied) comes from impact-ionization-generated holes collected at the gate electrode, and that the bell shape of the I_g(V_gs) curve is strongly related to the drop of the electric field in the channel of the device as V_gs is moved towards positive values     

Time-dependent dielectric breakdown characteristics ofN2O oxide under dynamic stressing

Time-dependent dielectric breakdown (TDDB) characteristics of MOS capacitors with thin (120-Å) N₂O gate oxide under dynamic unipolar and bipolar stress have been studied and compared to those with control thermal gate oxide of identical thickness. Results show that N₂O oxide has significant improvement in t _BD (2×under-V_g unipolar stress, 20×under+V_g unipolar stress, and 10×under bipolar stress). The improvement of t_BD in N₂O oxide is attributed to the suppressed electron trapping and enhanced hole detrapping due to the nitrogen incorporation at the SiO₂/Si interface