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     

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 new two-mode channel FET (TMT) for super-low-noise and high-powerapplications

A super-low-noise two-mode channel FET (TMT) with high- and plateau-shaped transconductance (g_m) characteristics has been developed. It has two electron transport modes against the applied gate voltage (V_gs). That is, the electrons mainly drift in a highly doped channel region at a shallow V_gs. A plateau g_m region and the maximum g_m were achieved at a V_gs range of -0.25~+0.5 V and 535 mS/mm, respectively. The minimum noise figure and associated gain for the TMT were superior in the low-drain-current (I_ds) region and nearly equal in the middle and high I_ds region to those of an AlGaAs/InGaAs pseudomorphic HEMT fabricated using the same wafer process and device geometry     

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     

Detection of the trapped electron distribution of PMOSFET's afterhot-carrier stress

A method of obtaining the spatial distribution of hot-carrier-induced trapped electrons in the gate oxide (N_0t(x)) of PMOSFETs is introduced with the aid of a two-dimensional simulator. The measured I_ds versus V_ds for various V_gs for low drain bias and I_ds versus V_gs have been compared with data obtained from the simulation concerning the obtained spatial distribution of trapped electrons in the gate oxide. There exists a high degree of agreement between the measured current-voltage characteristics after hot-carrier stress and the simulation results concerning the newly obtained spatial distribution of trapped electrons in the gate oxide     

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     

Nonlinear GaAs MESFET modeling using pulsed gate measurements

The effects of traps in GaAs MESFETs are studied using a pulsed gate measurement system. The devices are pulsed into the active region for a short period (typically 1 μs) and are held in the cutoff region for the rest of a 1-ms period. While the devices are on, the drain current is sampled and a series of pulsed gate I-V curves are obtained. The drain current obtained under the pulsed gate conditions for a given V_GS and V_DS gives a better representation of the instantaneous current for a corresponding V_gs and V_ds in the microwave cycle because of the effects of traps. The static and pulsed gate curves were used in a nonlinear time-domain model to predict harmonic current. The results showed that analysis using pulsed gate curves yielded better predictions of harmonic distortion than analysis based on conventional state I-V curves under large-signal conditions     

Effects of localized interface defects caused by hot-carrier stressin n-channel MOSFETs at low temperature

Hot-carrier stressing was carried out on 1-μm n-type MOSFETs at 77 K with fixed drain voltage V_d=5.5 V and gate voltage V_g varying from 1.5 to 6.5 V. It was found that the maximum transconductance degradation ΔG_m and threshold voltage shift ΔV_t, do not occur at the same V_g. As well, ΔK_t is very small for the V_g <V_d stress regime, becomes significant at V_g≈V_d, and then increases rapidly with increasing V_g, whereas ΔG_m has its maximum maximum in the region of maximum substrate current. The behavior is explained by the localized nature of induced defects, which is also responsible for a distortion of the transconductance curves and even a slight temporary increase in the transconductance during stress     

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     

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     

1/f noise in MODFETs at low drain bias

The 1/f noise in normally-on MODFETs biased at low drain voltages is investigated. The experimentally observed relative noise in the drain current S_I/I² versus the effective gate voltage V_G=V_GS-V_off shows three regions which are explained. The observed dependencies are S_I/I²∝V_G ^m with the exponents m=-1, -3, 0 with increasing values of V_G. The model explains m =-1 as the region where the resistance and the 1/f noise stem from the 2-D electron gas under the gate electrode; the region with m=0 at large V_G or V_GS≅0 is due to the dominant contribution of the series resistance. In the region at intermediate V_G , m=-3, the 1/f noise stems from the channel under the gate electrode, and the drain-source resistance is already dominated by the series resistance     

DC I-V characteristics of field emitter triodes

A simple model that is applicable to Spindt-type emitter triodes is presented. Experimentally, it has been observed that the gate current at zero collector voltage follows the same Fowler-Nordheim law as the collector current at high collector voltage, and that for low emission current densities, the sum of gate and collector currents is constant for any collector voltage and is given by the Fowler-Nordheim current I_FN. Based on these observations, a simple model has been developed to calculate the I-V characteristics of a triode. By measuring the Fowler-Nordheim emission, emission area and field enhancement can be obtained assuming a value for the barrier height. Incorporating the gate current, the collector current can be calculated from I_c=I_FN-I_g as a function of collector voltage. The model's accuracy is best at low current density. At higher emission currents, deviations occur at low collector voltages because the constancy of gate and collector currents is violated     

Off-state gate current in n-channel MOSFETs with nitrided oxidegate dielectrics

The authors report on the off-state gate current (I_g ) characteristics of n-channel MOSFETs using thin nitrided oxide (NO) gate dielectrics prepared by rapid thermal nitridation at 1150°C for 10-300 s. New phenomena observed in NO devices are a significant I_g at drain voltages as low as 4 V and an I_g injection efficiency reaching 0.8, as compared to 8.5 V and 10^-7 in SiO₂ devices with gate dielectrics of the same thickness. Based on the drain bias and temperature dependence, it is proposed that I_g in MOSFETs with heavily nitrided oxide gate dielectrics arises from hot-hole injection, and the enhancement of gate current injection is due to the lowering of valence-band barrier height for hole emission at the NO/Si interface. The enhanced gate current injection may cause accelerated device degradation in MOSFETs. However, it also presents potential for device applications such as EPROM erasure     

Gate-controlled negative differential resistance in drain currentcharacteristics of AlGaAs/InGaAs/GaAs pseudomorphic MODFETs

The observation of negative differential resistance (NDR) and negative transconductance at high drain and gate fields in depletion-mode AlGaAs/InGaAs/GaAs MODFETs with gate lengths L _g ~0.25 μm is discussed. It is shown that under high bias voltage conditions, V_ds>2.5 V and V_gs>0 V, the device drain current characteristic switches from a high current state to a low current state, resulting in reflection gain in the drain circuit of the MODFET. The decrease in the drain current of the device corresponds to a sudden increase in the gate current. It is shown that the device can be operated in two regions: (1) standard MODFET operation for V_gs<0 V resulting in f_max values of >120 GHz, and (2) a NDR region which yields operation as a reflection gain amplifier for V_gs >0 V and V_ds>2.5 V, resulting in 2 dB of reflection gain at 26.5 GHz. The NDR is attributed to the redistribution of charge and voltage in the channel caused by electrons crossing the heterobarrier under high-field conditions. The NDR gain regime, which is controllable by gate and drain voltages, is a new operating mode for MODFETs under high bias conditions     

A comprehensive study on p+ polysilicon-gate MOSFET'sinstability with fluorine incorporation

It is reported that fluorine can jeopardize p⁺-gate devices under moderate annealing temperatures. MOSFETs with BF₂ or boron-implanted polysilicon gates were processed identically except at gate implantation. Evidence of boron penetration through 12.5-nm oxide and a large quantity of negative charge penetration (10 ¹² cm^-2) by fluorine even at moderate annealing conditions is reported. The degree of degradation is aggravated as fluorine dose increases. A detailed examination of the I-V characteristics of PMOSFET with fluorine incorporated p⁺-gate revealed that the long gate-length device had abnormal abrupt turn-on I_d-V_g characteristics, while the submicrometer-gate-length devices appeared to be normal. The abnormal turn-on I_d-V_g characteristics associated with long-gate-length p⁺-gate devices vanished when the device was subjected to X-ray irradiation and/or to a high-voltage DC stressing at the source/drain. The C-V characteristics of MOS structures of various gate dopants, processing ambients, doping concentrations, and annealing conditions were studied. Based on all experimental results, the degradation model of p⁺-gate devices is presented. The incorporation of fluorine in the p⁺ gate enhances boron penetration through the thin gate oxide into the silicon substrate and creates negative-charge interface states. The addition of H/OH species into F-rich gate oxide will further aggravate the extent of F-enhanced boron penetration by annealing out the negative-charge interface states     

A simple characterization method for silicon-on-insulator materialsusing a depletion-mode MOSFET

A simple method is proposed for extracting the electrical parameters of a silicon-on-insulator (SOI) material from a depletion-mode MOSFET. It is based on an analysis of static input current-voltage I_D(V_G) and transconductance-voltage g_m(V_G) characteristics in the linear region. Functions varying linearly with gate voltage are constructed from I_D(V_G) and g_m(V_G) functions. These new functions allow a straightforward determination of the parameters usually obtained from a capacitance-voltage measurement (doping level, oxide charge, etc.) and also the bulk-layer and accumulation-layer carrier mobility     

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     

Examination of oxide damage during high-current stress of n-MOStransistors

Damage to n-channel MOSFETs under different levels of drain current stress is compared. It is shown that the post-stress I _d-V_gs characteristics show distinctly different behavior for different stresses. These differences are interpreted in terms of the location of the stress damage along the Si-SiO₂ interface. It is shown that damage from low drain current stress occurs at the Si-SiO₂ interface just inside the drain junction, under strong gate control. Damage from high drain current stress occurs at the Si-SiO₂ interface deeper inside the drain junction region, under weak gate control. The damage localization interpretation is supported by simulations and by localized Fowler-Nordheim injection experiments. It is further shown that at intermediate levels of drain current injection, the damage occurs at the Si-SiO₂ interface in both drain regions. The differences are explained in terms of the bipolar action at high drain current levels, which forces the channel charge away from the Si-SiO₂ interface at the drain junction edge     

A model for the temperature-dependent saturated ID-VD characteristics of an a-Si:H thin-filmtransistor

A simplified analytical expression for the temperature dependent saturated I_D-V_D characteristics of hydrogenated amorphous silicon (a-Si:H) thin-film transistors, between -50°C and 90°C, is presented and experimentally verified. The results show that the experimental transfer and output characteristics at several temperatures are easily modeled by a single equation. The model is based on three functions obtained from the experimental data of I_D versus V_G, over a range of temperature. Theoretical results confirm the simple form of the model in terms of the device geometry. As the temperature increased, the saturated drain current increased and, at a fixed gate voltage the device saturated at increasingly larger drain voltages while the threshold voltage decreased. Good agreement between the measured data and the model was obtained up to 363 K. Also observed at temperatures larger than 363 K was a decrease in I_D and more severe gate voltage hysteresis characteristics     

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