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In this paper, three electrical techniques (frequency dependent conductance analysis, AC transconductance (AC-gm), and positive gate bias stress) were used to evaluate three different gate dielectrics (Plasma-Enhanced Atomic Layer Deposition Si3N4, Rapid Thermal Chemical Vapor Deposition Si3N4, and Atomic Layer Deposition (ALD) Al2O3) for AlGaN/GaN Metal-Insulator- Semiconductor High-Electron-Mobility Transistors. From these measurements, the interface state density (Dit), the amount of border traps, and the threshold voltage (VTH) shift during a positive gate bias stress can be obtained. The results show that the VTH shift during a positive gate bias stress is highly correlated to not only interface states but also border traps in the dielectric. A physical model is proposed describing that electrons can be trapped by both interface states and border traps. Therefore, in order to minimize the VTH shift during a positive gate bias stress, the gate dielectric needs to have a lower interface state density and less border traps. However, the results also show that the commonly used frequency dependent conductance analysis technique to extract Dit needs to be cautiously used since the resulting value might be influenced by the border traps and, vice versa, i.e., the gm dispersion commonly attributed to border traps might be influenced by interface states. [ABSTRACT FROM AUTHOR]

In this paper, we perform a comparative analysis of the degradation induced by a channel hot carrier (CHC) in bulk n-FinFETs with rotated (100) and nonrotated (110) sidewall surfaces. CHC degradation includes several components, and separating each contribution is necessary for identifying different mechanisms in devices with different surface orientations. First, the permanent and recoverable components are separated based on the recovery phenomenon after the CHC stress, ascribed to the electron detrapping from the oxide bulk defects. Then, the contribution of generated interface states to the permanent component is quantified by charge pumping measurements. The nonrotated bulk FinFETs showed higher threshold voltage degradation at the maximum bulk current stress condition due to the higher interface precursor defect density compared with the rotated devices. On the other hand, the rotated bulk FinFETs showed higher threshold voltage degradation at the stress condition of VG = VD due to higher bulk defect trapping, ascribed to the lower physical oxide thickness. [ABSTRACT FROM PUBLISHER]

The channel hot carrier degradation mechanisms in n-FinFET devices are studied. In long channel devices, interface degradation by hot carriers mainly degrades the device at the maximum impact ionization condition (VG\sim VD/2). At higher VG closer to VD, cold and hot carrier injection to the oxide bulk defect increases and dominates at the VG=VD stress condition. On the other hand, in short channel devices, hot carriers are generated continuously with respect to VG and highly at VG=VD, and this hot carrier injection into the oxide bulk defect is the main degradation mechanism. [ABSTRACT FROM PUBLISHER]

Due to a significantly reduced negative-bias temperature instability (NBTI), (Si)Ge channel pMOSFETs are shown to offer sufficient reliability at ultrathin equivalent oxide thickness. The intrinsically superior NBTI robustness of the MOS system consisting of a Ge-based channel and a \SiO2/ \HfO2 dielectric stack is ascribed to a reduced availability of interface precursor defects and to a significantly reduced interaction of channel carriers with gate dielectric defects due to a favorable energy decoupling. Owing to this effect, a significantly reduced time-dependent variability of nanoscale devices is also observed. The superior reliability is shown to be process and architecture independent by comparing both our results on a variety of Ge-based device families and published data of other groups. [ABSTRACT FROM PUBLISHER]

In this paper, the potential of Silicon-Germanium (SiGe) technology for VLSI logic applications is investigated from a circuit perspective for the first time. The study is based on experimental measurements on 45-nm SiGe pMOSFETs with a high-\kappa/metal gate stack, as well as on 45-nm Si pMOSFETs with identical gate stack for comparison. In the reference SiGe technology, an innovative technological solution is adopted that limits the SiGe material only to the channel region. The resulting SiGe device merges the higher speed of the Ge technology with the lower leakage of the Si technology. Appropriate circuit- and system-level metrics are introduced to identify the advantages offered by SiGe technology in VLSI circuits. Analysis is performed in the context of next-generation VLSI circuits that fully exploit circuit- and system-level techniques to improve the energy efficiency through aggressive voltage scaling, other than low-leakage techniques. Analysis shows that the SiGe technology has more efficient leakage-delay and dynamic energy-delay trade-offs at nominal supply, compared to Si technology. Moreover, it is shown that the traditional analysis performed at nominal supply actually underestimates the benefits of SiGe pMOSFETs, since the speed advantage of SiGe VLSI circuits is further emphasized at low voltages. This demonstrates that SiGe VLSI circuits benefit from aggressive voltage scaling significantly more than Si circuits, thereby making SiGe devices a very promising alternative to Si transistors in next-generation VLSI systems. [ABSTRACT FROM PUBLISHER]

Extraction of interfacial trap density Nit in extremely reduced gate oxides with equivalent oxide thickness (EOT) below 1 nm by conventional charge pumping is virtually impossible due to the high gate leakage current through the very thin oxide. However, interface quality assessment in subnano EOT devices is essential for the reliability and performance improvement of future logic devices. In this paper, an accurate approach to determine the interfacial trap density in a 5.8- \\rm\AA EOT device is performed by an advanced charge pumping technique employing ring-oscillator-connected devices. A consistency comparison of this technique to the conventional charge pumping is done by a frequency sweep on the 10.1-\\rm \AA EOT device. Clear charge pumping currents are obtained on the 5.8- \\rm\AA EOT oxide, and further analysis by varying the applied frequency and amplitude is performed. The interface trap density in the 5.8-\\rm\AA EOT device is found to be higher than that in the 10.1- \\rm\AA EOT device due to the physically reduced interfacial layer in the thinner EOT device. Moreover, direct tunneling-based calculation gives the charge injection distance as about 2 \\rm\AA inside the oxide. Stress-induced defect generation is investigated by applying dc stress between charge pumping and Idrain - Vgate measurements. The 5.8- \\rm\AA EOT device shows higher initial Nit but lower stress-induced Nit as compared with the 10.1- \\rm\AA EOT device. The bulk trap Not generated after stress is higher in the 5.8- \\rm\AA EOT device due to the higher initial bulk trap density. [ABSTRACT FROM AUTHOR]

• Multi-energy level agnostic approach describes defects generation during time-dependent dielectric breakdown. • Defect generation is both fluence and energy-carrier-driven. • Considering the bond strength distribution, the accepted power-law trend for defect generation is naturally obtained by Monte Carlo simulations. • Low-frequency AC time to-breakdown increased compared to DC. Defect generation during time-dependent dielectric breakdown stress is investigated by a multi-energy level agnostic model. Monte Carlo simulations show that the characteristic power-law increase of the generated defects with stress time is readily obtained when considering distributed bond strengths. DC and AC unipolar simulations show the proportionality between the time-to-breakdown and the fluence and energy of the injected carriers. These results are consistent with the experimental observations of a fluence and energy-driven process in thin oxides. [ABSTRACT FROM AUTHOR]