PulseExploreJournal ClubDebatesTrendingResearchersJournals
Instagram
HomeExploreJournal ClubTrending
Synapse
⌘+K
Synapse
April 1, 2026physica status solidi (RRL) - Rapid Research Letters0 citationsOpen Access

Transition from Metal‐Oxide‐Semiconductor to Ideal Capacitor Behavior Triggered by Tunneling in the Inversion Population Regime

View Full Paper
PPPedro Pereyra

Key Points

  • The aim is to analyze the transition of MOS behavior due to tunneling in the inversion population regime.
  • Derived analytical solutions to the nonlinear Poisson equation for MOS structures.
  • Calculated inversion-layer width, electric potential, and charge distribution based on gate voltage and impurity concentration.
  • Examined tunneling effects through the Esaki barrier during inversion.
  • Identified rapid changes in physical quantities during early-stage inversion, followed by saturation past the threshold voltage.
  • Reconfigured charge distribution indicates a shift towards ideal capacitor behavior with localized voltage drop across the oxide.
  • Demonstrated that tunneling current becomes dominant during the inversion process.

Abstract

An analytical solution to the nonlinear Poisson equation governing the inversion layer in metal‐oxide‐semiconductor (MOS) structures has recently been obtained, resolving a fundamental challenge in semiconductor theory first identified in 1955. This breakthrough enables the derivation of explicit expressions for relevant physical quantities, such as the inversion‐layer width, electric potential, and charge distribution, as functions of gate voltage V G , distance from oxide‐semiconductor interface and impurity concentration. These quantities exhibit rapid variation during early‐stage inversion but saturate once V G exceeds the threshold voltage by a few tenths of a volt signaling a transition in the MOS response to gate voltage. The onset of tunneling through the Esaki barrier leads to increased charge accumulation near the interface, reshaping the charge distribution into a two‐dimensional profile and shifting the potential drop from the semiconductor to the oxide layer. This reconfiguration resembles the behavior of an ideal parallel‐plate capacitor, with charge confined at the interface and the voltage drop localized across the oxide. We analyze this mechanism in detail and demonstrate, through explicit calculations, that the tunneling current through the Esaki‐like barrier formed during inversion becomes dominant. These results offer a new analytical foundation for quantum‐aware device modeling.

Ask AI
Helpful
Bookmark
Share
View Full Paper

Cite This Study

Pedro Pereyra (2026) studied this question.

synapsesocial.com/papers/69ccb71716edfba7beb88e0fhttps://doi.org/10.1002/pssr.202500450
Ask AI
Helpful
Bookmark
Share
View Full Paper