Abstract

This paper theoretically revisits the low-frequency noise behavior of the inversion-channel silicon-on-insulator metal-oxide-semiconductor field-effect transistor (SOI MOSFET) and the buried-channel SOI MOSFET because the quality of both Si/SiO2 interfaces (top and bottom) should modulate the low-frequency fluctuation characteristics of both devices. It also addresses the low-frequency noise behavior of sub-100-nm channel SOI MOSFETs. We deepen the discussion of the low-frequency noise behavior in the subthreshold bias range in order to elucidate the device’s potential for future low-voltage and low-power applications. As expected, analyses suggest that the weak inversion channel near the top surface of the SOI MOSFET is strongly influenced by interface traps near the top surface of the SOI layer because the traps are not well shielded by low-density surface inversion carriers in the subthreshold bias range. Unexpectedly, we find that the buried channel is primarily influenced by interface traps near the top surface of the SOI layer, not by traps near the bottom surface of the SOI layer. This is not due to the simplified capacitance coupling effect. These interesting characteristics of current fluctuation spectral intensity are explained well by the theoretical models proposed here.

Highlights

  • It has long been considered that there are two possible explanations for the low-frequency noise (LFN) exhibited by metal-oxide-semiconductor field-effect transistors (MOSFETs)

  • This paper reconsidered low-frequency noise behavior in the inversion-channel SOI MOSFET and the buried-channel SOI MOSFET because it is anticipated that the quality of both Si/SiO2 interfaces should modulate the low-frequency noise characteristics of both devices

  • The low-frequency noise behavior in the subthreshold bias range was discussed in some detail in order to consider device suitability for future low-voltage and low-power applications

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Summary

Introduction

It has long been considered that there are two possible explanations for the low-frequency noise (LFN) exhibited by metal-oxide-semiconductor field-effect transistors (MOSFETs). They are carrier density fluctuations due to interface traps near the oxide/semiconductor interface [1,2,3], and carrier mobility fluctuations [4,5,6]. Hooge introduced a specific parameter (the so-called Hooge parameter) to characterize the 1/f noise [4]. Related to these theories, the quantum 1/f noise model was proposed by Peter H. It is considered that the difficulty of understanding the 1/f noise behavior stems from the fact that the Hooge parameter depends on device material and structure [9,15,16]

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