Characterization of various stress-induced oxide traps in MOSFET'sby using a subthreshold transient current technique

An oxide trap characterization technique by measuring a subthreshold current transient is developed. This technique consists of two alternating phases, an oxide charge detrapping phase and a subthreshold current measurement phase. An analytical model relating a subthreshold current transient to oxide charge tunnel detrapping is derived. By taking advantage of a large difference between interface trap and oxide trap time-constants, this transient technique allows the characterization of oxide traps separately in the presence of interface traps. Oxide traps created by three different stress methods, channel Fowler-Nordheim (F-N) stress, hot electron stress and hot hole stress, are characterized. By varying the gate bias in the detrapping phase and the drain bias in the measurement phase, the field dependence of oxide charge detrapping and the spatial distribution of oxide traps in the channel direction can be obtained. Our results show that 1) the subthreshold current transient follows a power-law time-dependence at a small charge detrapping field, 2) while the hot hole stress generated oxide traps have a largest density, their spatial distribution in the channel is narrowest as compared to the other two stresses, and 3) the hot hole stress created oxide charges exhibit a shortest effective detrapping time-constant     

A new technique to extract oxide trap time constants in MOSFET's

A new technique to determine oxide trap time constants in a 0.6 μm n-MOSFET subject to hot electron stress has been proposed. In this method, we used GIDL current as a direct monitor of the oxide charge detrapping-induced transient characteristics. An analytical model relating the GIDL current evolution to oxide trap time constants was derived. Our result shows that under a field-emission dominant oxide charge detrapping condition, Vgs=-4 V and Vds=3 V, the hot electron stress generated oxide traps exhibit two distinct time constants from seconds to several tens of seconds     

Hot hole stress induced leakage current (SILC) transient in tunneloxides

The mechanisms and transient characteristics of hot hole stress induced leakage current (SILC) in tunnel oxides are investigated. Positive oxide charge assisted tunneling is found to be a dominant SILC mechanism in a hot hole stressed device. The SILC transient is attributed to oxide hole detrapping and thus annihilation of positive charge assisted tunneling centers. Our characterization shows that the leakage current transient in a 100-Å oxide obeys a power law time dependence f^-n with the power factor n significantly less than one. An analytical model accounting for the observed time dependence is proposed     

Hot-carrier stress effects on gate-induced-drain leakage current in n-channel MOSFETs studied by hydrogen/deuterium isotope effect

The degradation of gate-induced-drain leakage (GIDL) current under hot-carrier stress (HCS) has been studied in n-channel MOSFETs that were annealed in hydrogen (H) or deuterium (D). It is found that the degradation of GIDL current (I/sub GIDL/) can be effectively suppressed by deuterium passivation of interface traps. By using the H/D isotope effect, the impacts of oxide charge trapping (/spl Delta/N/sub ox/) and interface trap generation (/spl Delta/N/sub it/) on I/sub GIDL/ are successfully separated. The results indicate that, depending on stress and measurement conditions, I/sub GIDL/ may increase or decrease under HCS. /spl Delta/N/sub ox/ alters I/sub GIDL/ at high electric fields by varying the band-to-band tunneling current. /spl Delta/N/sub it/ alters I/sub GIDL/ at a low electric field by introducing a trap-assisted leakage component. Furthermore, evidence of hole trapping at the peak substrate current stress is indisputably presented for the first time and its impact on I/sub GIDL/ is discussed.     

Hot carrier effects in n-MOSFETs with SiO2/HfO2/HfSiO gate stack and TaN metal gate

Charge trapping and trap generation in field-effect transistors with SiO₂/HfO₂/HfSiO gate stack and TaN metal gate electrode are investigated under uniform and non-uniform charge injection along the channel. Compared to constant voltage stress (CVS), hot carrier stress (HCS) exhibits more severe degradation in transconductance and subthreshold swing. By applying a detrapping bias, it is demonstrated that charge trapping induced degradation is reversible during CVS, while the damage is permanent for hot carrier injection case.     

Role of positive trapped charge in stress-induced leakage current for flash EEPROM devices

The transient behavior of hot hole (HH) stress-induced leakage current (SILC) in tunnel oxides is investigated. The dominant SILC mechanism is positive oxide charge-assisted tunneling (PCAT). The transient effect of SILC is attributed to positive oxide charge detrapping and thus the reduction of PCAT current. A correlation between SILC and stress-induced substrate current is observed. Our study shows that both SILC and stress-induced substrate current have power law time-dependence t/sup -n/ with the power factor n about 0.7 and 1, respectively. Numerical analysis for PCAT current incorporating a trapped charge caused Coulombic potential in the tunneling barrier is performed to evaluate the time- and field-dependence of SILC and the substrate current. Based on our model, the evolution of threshold voltage shift with read-disturb time in a flash EEPROM cell is derived. Finally, the dependence of SILC on oxide thickness is explored. As oxide thickness reduces from 100 /spl Aring/ to 53 /spl Aring/, the dominant SILC mechanism is found to change from PCAT to neutral trap-assisted tunneling (TAT).     

Hot-carrier-stress effects on gate-induced drain leakage current inn-channel MOSFETs

The effects of hot-carrier stress on gate-induced drain leakage (GIDL) current in n-channel MOSFETs with thin gate oxides are studied. It is found that the effects of generated interface traps (ΔD _it) and oxide trapped charge on the GIDL current enhancement are very different. Specifically, it is shown that the oxide trapped charge only shifts the flat-band voltage, unlike ΔD _it. Besides band-to-band (B-B) tunneling, ΔD _it introduces an additional trap-assisted leakage current component. Evidence for this extra component is provided by hole injection. While trapped-charge induced leakage current can be eliminated by a hole injection subsequent to stress, such injection does not suppress interface-trap-induced leakage current     

New results on electron injection, hole injection, and trapping in MONOS nonvolatile memory devices

Charge injection and trapping in silicon nitride layers are studied with the three-terminal metal-oxide-nitride-oxide-semiconductor (MONOS) gated-diode structure. A new experimental technique based on the linear voltage ramp is developed which measures electron and hole currents separately in the semiconductor during the actual charge injection (nonsteady-state measurement as opposed to the steady-state method) across the tunneling oxide. In addition, the technique measures the flat-band voltage shift and minimizes the back tunneling of the injected charge (a problem with the pulse measurement). The blocking oxide between the gate electrode and the nitride layer prevents any injection from the gate electrode. The main conclusion from these studies is that the semiconductor injects electrons and holes into the nitride layer for positive and negative polarities of the gate bias, respectively. This result is in sharp contrast with the existing interpretations based on a single-carrier type. It is speculated that the recombination of electrons and holes takes place in the nitride layer via an "amphoteric" trap. At small levels of charge injection, centroids of the trapped charge (measured from the tunneling oxide-nitride interface) for both electron and hole injection conditions are found to be located at 75-80 Å at room temperature and 15-20 Å at 100 K.     

Determination of trapped oxide charge in flash EPROMs and MOSFETswith thin oxides

A technique for determining the sign and the effective density of the trapped oxide charge near the junction transition region, based on the measurement of the gate-induced drain leakage (GIDL) current, is used to investigate the hot-carrier effects resulting from the erase operation and bit-line stress in flash EPROM devices. While the trapped oxide charge depends on the stress conditions, it has been found that a significant amount of hole trapping is likely when a sufficiently large potential difference exists between the gate and junction for either an abrupt or graded junction     

Evolution of oxide charge trapping under bias temperature stressing

Transient oxide-charge trapping and detrapping, commonly regarded as a parasitic effect in the interpretation of dynamic bias-temperature stress (BTS) data, may play an important role on the long term reliability of the gate oxide as revealed by recent studies on the SiON and HfO₂ gate dielectrics. Specifically, it is found that transient charge trapping (one which relaxes upon removal of the applied electrical stress) is transformed into more permanent trapped charge when the applied electrical cum thermal stress exceeds a certain threshold. Below the threshold, cyclical transient charge trapping and detrapping behavior is observed. The observations imply that the oxide structure may be modified by the applied stress, making it susceptible to permanent defect generation. In addition, it is found that when the transformation of hole trapping occurs under negative-bias temperature stress, a correlated increase of the gate current is always observed, which points to the transformation process being the origin for bulk oxide trap generation. However, when the transformation of electron trapping occurs under positive-bias temperature stress, an increase of the gate current is not always observed. From ab initio simulation, we show that an intrinsic oxide defect – the oxygen vacancy-interstitial (V_O − O_i) – could consistently explain the experimental observations. An interesting feature of the V_O − O_i defect is that it can exists in various metastable configurations with the interstitial oxygen O_i in different positions around the vacancy V_O, corresponding to different trap energy states in the oxide bandgap. This characteristic is able to account for the BTS induced generation of deep-level trapped charges as well as transformation of transient (or shallow) to permanent (or deep) charge trapping.     

Origin of positive charge generated in thin SiO2 filmsduring high-field electrical stress

The characteristics of electron capture in a 131-Å silicon dioxide after hot-hole injection have been studied, which have been compared with those after high-field Fowler-Nordheim (FN) electron injection. After hole injection from the silicon substrate into the oxide, positive charges accumulated in the oxide and electrons could be captured even at low oxide fields only under the positive gate polarity. The charge centroid of the captured electrons was near the substrate-SiO ₂ interface. The low-field electron capture can be explained based on the electron tunneling from the substrate into the positive charge and neutral trap centers created near the substrate-SiO₂ interface. In order to investigate the initial stage of the oxide degradation due to high-field FN stress, electrons were injected from the gate and the charge fluence was selected to be -1.0 C/cm². After the high-field stress, positive charges appeared in the oxide and electrons were captured only under the positive gate polarity by the positive charge and neutral trap centers, which were distributed near the interface. These facts are explained on the basis of the model describing that hole injection and trapping are the dominant causes for the generation of the positive charge centers during high-field FN stress     

Post-stress interface trap generation induced by oxide-field stresswith FN injection

Interface trap generation in nMOS transistors during both stressing and post-stress periods under the conditions of oxide field (dynamic and dc) stress with FN injection is investigated with charge pumping technique. In contrast to the post-stress interface trap generation induced by hot carrier stress which is a logarithmical function of post-stress time, the post-stress interface trap generation induced by oxide-field stress with FN injection first increases with post-stress time but then becomes saturated. The mechanisms for the interface trap generation in both stressing and post-stress periods are described     

Current transient in polyimide-passivated InP/InGaAs heterojunction bipolar transistors: systematic experiments and physical model

We present the first comprehensive experimental investigation of base current transient in InP/InGaAs heterojunction bipolar transistors (HBTs) induced by polyimide passivation, and its influence on the device characteristics. We have confirmed that the trapping and detrapping of static charge in the polyimide at the polyimide/semiconductor interface is the root cause for the current transient effect. Experimental and theoretical evidence indicates that the base current transient is caused by the change of the base-emitter junction surface potential as a result of the decrease in the number of trapped electrons in the polyimide film. A physical model accounting for the time-dependence of surface recombination current induced by electron detrapping in the polyimide is derived and predicts the current transient behavior. The physical understanding is helpful for further optimization of polyimide passivation process for HBTs.     

Excess currents induced by hot hole injection and FN electroninjection in thin SiO2 films

The behavior of excess currents induced by Fowler-Nordheim electron injection stress (FN electron injection) has been investigated for 6.0-nm oxides. Excess currents are induced by FN electron injection in 6.0-nm oxides together with positive charges being induced in it. To clarify the role of hole injection in FN electron injection, the behavior of excess currents induced by substrate hot hole injection has also been investigated in 6.0-nm oxides. The leakage behavior after hot hole injection is the same as FN electron injection. The excess currents induced both by the FN electron injection and by the substrate hot hole injection are due to trap-assisted tunneling and field enhancement at the cathode due to the positive trapped charge. The charge centroid of the positive charges induced by both stresses are located 3.0 nm from the Si/SiO₂ interface which is at the center of 6.0-nm oxide. The excess currents induced by hot hole injection and FN electron injection are caused by traps in SiO₂ films produced by injected holes from the anode     

A novel hot carrier reliability monitor for LDD p-MOSFETs

The gate-edge shape of an LDD p-MOSFET exhibits large influences upon the hot carrier induced degradation and its performances. It is observed that the gate-to-drain tunneling current is strongly correlated to the reentrant gate oxide thickness and to the device degradation. A simple model is then constructed to provide an explanation for the observation. Under the tunneling current measurement conditions, a thicker oxide at the gate-edge leads to a weaker peak electric field in the p-LDD and to a lower gate-to-drain current. On the other hand, under the hot carrier stressing conditions, the thicker oxide decreases the oxide electric field and thus suppresses the hot electron injection. The observed correlation can be employed to monitor the process induced gate-edge (overlap) variation.     

Degradation of ultra-thin gate oxide LDD NMOSFET under GIDL stress

The degradation of device under GIDL(gate-induced drain leakage current)stress has been studied using LDD NMOSFETs with 1.4 nm gate oxides.Experimental result shows that the degradation of device parameters depends more strongly on Vd than on Vg.The characteristics of the GIDL current are used to analyze the damage generated during the stress.It is clearly found that the change of GIDL current before and after stress can be divided into two stages.The trapping of holes in the oxide is dominant in the first stage,but that of electrons in the oxide is dominant in the second stage.It is due to the common effects of edge direct tunneling and band-to-band tunneling.SILC(stress induced leakage current)in the NMOSFET decreases with increasing stress time under GIDL stress.The degradation characteristic of SILC also shows saturating time dependence.SILC is strongly dependent on the measured gate voltage.The higher the measured gate voltage,the less serious the degradation of the gate current.A likely mechanism is presented to explain the origin of SILC during GIDL stress.     

Characterization of hot-hole injection induced SILC and relateddisturbs in flash memories

In this paper, we have proposed a new method for the study of disturb failure mechanisms caused by stress induced leakage current (SILC) in source-side erased flash memories. This method is able to directly separate the individual components of SILC due to either carrier charging/discharging in the oxide or the positive charge/trap assisted electron tunneling into the floating gate. In addition, the present method is very sensitive with capability of measuring ultralow current (<10^-19 A). Results show that, at low oxide field, the disturb is mainly contributed by the so-called charging/discharging of carriers into/from the oxide due to the capacitance coupling effect. While at high oxide field, the positive charge/trap assisted electron tunneling induced floating-gate charge variation is the major cause of disturb failure     

0.275μm nMOST's中陷阱辅助隧穿电流对漏端LDD区DCIV谱峰的影响

应用direct-current current voltage(DCIV)和电荷泵(change pumping)技术研究了LDD nMOST's在热电子应力下产生的界面陷阱.测试和分析的结果显示,一股额外的漏端电流影响了DCIV谱峰中表征漏区的D峰.这股电流主要是陷阱辅助隧穿电流.     

0.275μm nMOST''''s中陷阱辅助隧穿电流对漏端LDD区DCIV谱峰的影响(英文)

应用 direct- currentcurrent voltage(DCIV)和电荷泵 (change pum ping)技术研究了 L DD n MOST’s在热电子应力下产生的界面陷阱 .测试和分析的结果显示 ,一股额外的漏端电流影响了 DCIV谱峰中表征漏区的 D峰 .这股电流主要是陷阱辅助隧穿电流 .     

高压pLEDMOS器件在不同应力条件下导通电阻的衰退及改进方法

实验测试结果揭示高压pLEDMOS器件在不同的应力条件下,导通电阻的衰退结果不同,半导体器件专业软件MEDICI模拟结果表明Si/SiO2表面的陷阱产生以及热电子的注入和俘获导致了高压pLEDMOS器件在不同的应力条件下产生不同的导通电阻衰退.文中同时提出了一种改进方法:用场氧代替厚栅氧作为高压pLEDMoS器件的栅氧,MEDICI模拟结果显示该方法可以明显降低/减缓高压pLEDMOS导通电阻的衰退.