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Related Concept Videos

MOS Capacitor01:25

MOS Capacitor

A Metal-Oxide-Semiconductor (MOS) capacitor is a fundamental structure used extensively in semiconductor device technology, particularly in the fabrication of integrated circuits and MOSFETs (metal-oxide-semiconductor field-effect transistors). The MOS capacitor consists of three layers: a metal gate, a dielectric oxide, and a semiconductor substrate.
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
Characteristics of MOSFET01:17

Characteristics of MOSFET

Metal-oxide-semiconductor field-effect Transistors, or MOSFETs, play a critical role in electronic circuits. They are primarily utilized for amplifying and switching signals.
Various vital parameters influence their functionality, which is crucial for theory and electronics applications. First, channel dimensions, precisely length, and width, are pivotal. The size of these channels affects the transistor's ability to carry current and switching speeds; shorter channels typically enable quicker...
MOSFET: Depletion Mode01:20

MOSFET: Depletion Mode

Depletion-mode MOSFETs represent a unique subset of MOSFET technology, functioning fundamentally differently from their enhancement-mode counterparts. Unlike enhancement MOSFETs, which require a positive gate-source voltage (Vgs) to turn on, depletion-mode MOSFETs are inherently conductive and "normally on" devices.
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity arises...
MOSFET: Enhancement Mode01:22

MOSFET: Enhancement Mode

Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
P-N junction01:11

P-N junction

A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...

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In Situ Transmission Electron Microscopy with Biasing and Fabrication of Asymmetric Crossbars Based on Mixed-Phased a-VOx
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Minimum voltage for threshold switching in nanoscale phase-change memory.

Dong Yu1, Sarah Brittman, Jin Seok Lee

  • 1Department of Chemistry and Chemical Biology, Harvard University, Cambridge, Massachusetts 02138, USA.

Nano Letters
|September 5, 2008
PubMed
Summary
This summary is machine-generated.

Threshold switching in phase-change memory (PCM) changes from constant field to constant voltage scaling below 10 nm. This enables the miniaturization of PCM bits to the true nanometer scale.

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Area of Science:

  • Materials Science
  • Electrical Engineering
  • Nanotechnology

Background:

  • Phase-change memory (PCM) relies on the amorphous-to-crystalline transition for data storage.
  • Understanding the size scaling of the threshold voltage is crucial for device miniaturization.
  • Previous studies have not fully elucidated the scaling laws at the nanometer scale.

Purpose of the Study:

  • To investigate the size scaling of the threshold voltage in individual GeTe and Sb2Te3 nanowires for PCM applications.
  • To determine the critical size at which the scaling law for threshold switching changes.
  • To establish the feasibility of true nanometer-scale PCM bit fabrication.

Main Methods:

  • Fabrication of planar devices with individual GeTe and Sb2Te3 nanowires.
  • Electrical characterization to measure threshold voltage and switching behavior.
  • Analysis of scaling laws based on amorphous domain length.

Main Results:

  • Observed a change in the scaling law from constant field to constant voltage as amorphous domain length decreased below 10 nm.
  • Identified carrier multiplication via inelastic scattering as the underlying mechanism for this crossover.
  • Demonstrated that the threshold switching behavior is size-dependent at the nanoscale.

Conclusions:

  • The size scaling of threshold voltage in PCM is governed by different laws at the nanoscale.
  • The observed crossover indicates that PCM bits can be reliably scaled down to the true nanometer regime.
  • This research paves the way for next-generation, ultra-dense phase-change memory devices.