ヴァン・デル・ワールスの金属半導体結合におけるショットキー・モットの限界に近づく
Yuan Liu1,2, Jian Guo1, Enbo Zhu1
1Department of Materials Science and Engineering, University of California, Los Angeles, CA, USA.
Nature
|May 18, 2018
まとめ
研究者らは,ヴァン・ダー・ワールズのレイヤリングを用いて理想的な金属半導体結合を作り,トランジスタにおける高電荷キャリアの移動性を達成し,高度な電子機器のための調整可能なショットキー・バリアを実証した.
科学分野:
- 材料科学
- 凝縮物質物理学
- ナノテクノロジー
背景:
- 金属半導体結合は電子機器にとって不可欠ですが,理想的な動作はインタフェースの障害によって妨げられます.
- ショットキー・バリアの高さは,理想的には,ショットキー・モットルによる金属半導体作業機能に依存する.
- 既存のインターフェースは 化学的障害とフェルミレベルのピニングに苦しんでおり 理想的な性能を阻害しています
研究 の 目的:
- 理想的なヴァン・デル・ワールスの金属半導体結合の作成と特徴付け
- インターフェースの障害のない調節可能なショットキーバリアの高さを実証する.
- この新しいインターフェース戦略を使用して高性能トランジスタと光ダイオードを実現します.
主な方法:
- ヴァン・デル・ワールスのヘテロ構造は,2次元半導体に原子的に平らな金属フィルムをレイニングすることによって製造される.
- 銀とプラチナの薄膜を使用し,特定の作業機能を持っています.
- 充電媒体の移動性と光ダイオード特性を含む装置の性能の特徴
主要な成果:
- 化学的混乱とフェルミレベルのピニングのない金属半導体インターフェースを達成しました.
- スコットキー・バリアの高さは,スコットキー・モットの限界に近づいており,金属加工機能で調節できます.
- 高室温電子 (260 cm2/Vs) と穴 (175 cm2/Vs) の移動性を有する製造されたトランジスタ.
- 1.02Vのオープン回路電圧を持つシルバー/モリブデン硫化物/プラチナ光ダイオードを開発した.
結論:
- この研究は,理想的な金属半導体結合の基本的限界を検証しています.
- ヴァン・デル・ワールスの統合は,金属を組み込むための無害で非常に効率的な戦略を提供します.
- このアプローチにより,高性能の電子機器と光電子機器が実現できます.
さらに関連する動画
14:16Fabrication of Schottky Diodes on Zn-polar BeMgZnO/ZnO Heterostructure Grown by Plasma-assisted Molecular Beam Epitaxy
Published on: October 23, 2018
7.9K
08:12Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
Published on: December 5, 2015
12.6K
関連する概念動画
Metal-Semiconductor Junctions
671
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...
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...
671
Biasing of Metal-Semiconductor Junctions
431
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
431
Schottky Barrier Diode
698
Schottky barrier diodes are specialized semiconductor devices characterized by their unique construction. This construction involves combining a metal layer with a moderately doped n-type semiconductor material. This combination leads to the formation of a Schottky barrier, a pivotal element that defines the diode's operational characteristics. The core functionality of Schottky barrier diodes is their capacity to allow current to flow in only one direction due to their distinctive...
698
Fermi Level Dynamics
486
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
486
Semiconductors
1.1K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.1K
P-N junction
853
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...
853
