Defect-centric perspective of time-dependent BTI variability
Introduction
As the vertical scaling of metal–oxide–semiconductor field effect transistor (MOSFET) devices continues, the oxide electric field increases and the so-called Bias Temperature Instability (BTI) becomes one of the most critical factors, complicating the qualification of the future technology nodes [1], [2], [3]. Furthermore, the number of stochastically behaving gate oxide defects in each device decreases to a numerable level due to the lateral downscaling, while their relative impact on the device characteristics increases. For all these reasons, BTI lifetime cannot be described any longer by a unique number, and BTI lifetime distribution has to be taken into consideration. As a consequence, even in the ideal case of the average BTI lifetime meeting the ITRS [4] specifications, a fraction of nanoscaled devices will fail at low overdrives. In this paper, the necessary physical understanding to predict the BTI lifetime distributions is developed and is introduced into an “atomistic” circuit simulator that takes realistic workloads into account.
We start by briefly reviewing the elementary definitions and experimental observations of BTI in large area and in nm-scaled devices. Contrary to the continuous relaxation curves observed on large area devices after bias temperature stress, giant discrete threshold voltage VTH shifts are measured on nanoscaled devices and linked to drain random telegraphic noise (ID-RTN) [5]. We then demonstrate that many properties of gate oxide defects, such as characteristic emission and capture times and VTH impact can be directly extracted from BTI relaxation measurements in deeply scaled devices [6]. Afterward we show how the understanding of gate oxide defect properties can be used to explain time dependent BTI variability in deeply scaled technologies. Finally, an atomistic simulator based on existing industry-standard tools is presented for circuit assessments.
Section snippets
Bias Temperature Instability BTI in large and in nm-scaled devices
During CMOS circuit operation the devices typically undergo electrical stress at elevated temperature resulting in a shift of the device parameters such as its threshold voltage, channel mobility, transconductance, and subthreshold slope, instigating a decrease of the FET’s drive current. Since these instabilities are strongly accelerated by temperature T and gate bias VG, they are known by the acronym BTI (Bias Temperature Instability). These phenomena are mainly the consequence of charging of
BTI: a non-steady state case of random telegraph noise
From the quantized recovery behavior observed in nanoscaled FETs it is straightforward to understand the recoverable component of BTI as the dynamic non-steady state case of random telegraph noise (RTN) [16]. As in the case of ID-RTN, the large quantized ΔVTH’s observed in Fig. 2 are explained by the non-uniform potential at the Si/SiO2 interface caused by the random distributions of dopants in the channel and charged traps in the dielectric. The potential fluctuations produce variations of the
Kinetic of individual traps
As previously stated, a new methodology has been introduced to study the statistical properties of individual traps called time dependent defect spectroscopy (TDDS) [6]. In this section, we explain this methodology and the way to obtain the response of single gate oxide traps in a deeply-scaled FETs during DC and AC bias temperature stress. We demonstrate that the behavior of individual traps as a function of the stress time and duty factor is dictated by their characteristic capture and
Bias temperature variability
In large devices the random properties of many defects average out resulting in a well-defined lifetime as we showed in Section 2. However, in deeply scaled devices, the stochastic nature of a handful of defects becomes apparent. For this reason, the application of identical workload in such nanoscaled devices results in distributions of the parameter shifts [15], [29]. Therefore, the well-defined bias temperature instability (BTI) lifetime of large devices becomes widely distributed [12], [22]
Atomistic approach to BTI variability in circuit simulators
Our “atomistic” simulation framework proposed previously [22], [34] is shown in Fig. 15. It allows simulating the impact of workload-dependent variability on circuits (i.e., “reliability distributions under operating conditions”). The framework accepts the studied circuit in the form of a standard netlist. All or selected FET devices of the input circuit are annotated (i.e., “enhanced”) with unique defect properties randomly selected from distributions obtained previously on the simulated
Conclusions
In this article we have summarized some recent insights into BTI achieved from the comprehensive study of deeply scaled devices. Among the most relevant, it is the close link between RTN and the recoverable component of BTI, indicating that identically behaving traps are responsible of both effects. Useful information about the kinetic properties of individual traps has been straightforwardly extracted from the recently developed technique TDDS. This helped to understand the charge exchange
References (35)
- et al.
NBTI degradation: from physical mechanisms to modelling
Microelectron Reliab
(2006) - et al.
Temperature and voltage dependences of the capture and emission times of individual traps in high-k dielectrics
Microelectron Eng
(2011) - Cartier E, Kerber A, Ando T, Frank MM, Choi K, Krishnan S, et al. Fundamental aspects of HfO2-based high-k metal gate...
- Cho M, Aoulaiche M, Degraeve R, Kaczer B, Franco J, Kauerauf T, et al. Positive and negative bias temperature...
- Franco J, Kaczer B, Eneman G, Mitard J, Stesmans A, Afanas’ev V, et al. 6Å EOT Si0.45Ge0.55 pMOSFET with optimized...
- International Technology Roadmap for Semiconductors....
- Kaczer B, Grasser T, Martin-Martinez J, Simoen E, Aoulaiche M, Roussel Ph.J, et al. NBTI from the perspective of defect...
- Grasser T, Reisinger H, Wagner P, Schanovsky F, Goes W, Kaczer B. The time dependent defect spectroscopy (TDDS) for the...
- Toledano-Luque M, Kaczer B, Grasser T, Roussel Ph.J, Franco J, Groeseneken G. Toward a streamlined projection of small...
- Grasser T, Kaczer B, Hehenberger P, Goes W, O’Connor R, Reisinger H, et al. Simultaneous extraction of recoverable and...
Statistics of multiple trapped charges in the gate oxide of deeply scaled MOSFET devices—application to NBTI
IEEE Electron Device Lett
RTS amplitudes in decananometer mosfets: 3-D simulation study
IEEE Trans Electron Dev
Simulation of statistical aspects of charge trapping and related degradation in bulk mosfets in the presence of random discrete dopants
IEEE Trans Electron Dev
Comprehensive analysis of random telegraph noise instability and its scaling in deca–nanometer flash memories
IEEE Trans Electron Dev
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