Abstract

In this work, the impacts of various pulsing schemes on endurance are comprehensively investigated. Trapezoidal and triangular waveforms are considered in endurance cycling tests. For endurance cycling with the trapezoidal waveforms, different rising time (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">r</sub> )/falling time (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</sub> ), e.g., 0.05– <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5 \mu \text{s}$ </tex-math></inline-formula> , with a fixed pulse width (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">width</sub> ) and different pulse width (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">width</sub> ), i.e., 0- <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$10 \mu \text{s}$ </tex-math></inline-formula> , with fixed rising time (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">r</sub> )/falling time (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</sub> ) are used. As for the endurance cycling with the triangular waveforms, the frequencies are ranged from 1 kHz to 1 MHz. The results indicate that a shorter rising time (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">r</sub> )/falling time (T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">f</sub> ) results in a completely different endurance characteristic, and a longer T <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">width</sub> leads to an earlier breakdown. Furthermore, the higher frequency of the triangular waveform results in a larger remnant polarization (2Pr) after endurance cycling. Overall, the endurance is highly dependent on the pulsing schemes, suggesting that a standardized methodology for the endurance evaluation is necessary for fair benchmarks and qualification of the ferroelectric-based technologies.

Highlights

  • In this work, the impacts of various pulsing schemes on endurance are comprehensively investigated

  • To the best of our knowledge, the effects of the pulsing scheme on the endurance are comprehensively studied for the first time in Si-doped HfO2 metal–ferroelectric–insulator– semiconductor (MFIS) capacitors by considering the endurance cycling tests with 1) different Tr/Tf values with a fixed Twidth in the trapezoidal waveform, 2) different Twidth values with a fixed Tr/Tf in the trapezoidal waveform, and 3) different frequencies in the triangular waveform

  • It is the first time to report that the endurance cycling tests with a shorter Tr/Tf results in the completely different 2Pr characteristics, leading to a larger 2Pr in the case of ±3V and an earlier breakdown in the case of ±4V, which is most probably due to the overshoot

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Summary

Introduction

The impacts of various pulsing schemes on endurance are comprehensively investigated. HfO2-based ferroelectric devices with high endurance have been developed [2], [5], the pulsing schemes for evaluating are inconsistent.

Results
Conclusion
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