基于原子薄半导体的内存逻辑
Guilherme Migliato Marega1,2, Yanfei Zhao1,2, Ahmet Avsar1,2
1Electrical Engineering Institute, École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland.
Nature
|November 5, 2020
概括
研究人员使用大面积二硫化物 (MoS2) 开发了新的内存逻辑设备. 这些由大脑启发的计算元素结合了逻辑和记忆,
科学领域:
- 材料科学
- 电气工程
- 计算机科学
背景情况:
- 机器学习需要节能硬件,
- 在内存计算,模仿大脑,整合逻辑和存储,以减少数据中心计算的能源成本.
- 开发适合内存计算设备的材料平台仍然是一个重大的工程挑战.
研究的目的:
- 探索大面积二硫化物 (MoS2) 作为逻辑内存设备的活性通道材料.
- 为集成逻辑和内存功能设计浮门场效应晶体管 (FGFET).
- 用这些新的设备架构来证明可重新配置的逻辑电路的可行性.
主要方法:
- 用于设备制造的大面积MoS2薄膜的制造.
- 浮门场效应晶体管 (FGFET) 的设计和特征.
- 在FGFET框架内实施和测试可编程逻辑门,包括NOR门.
主要成果:
- 证明了FGFET导电的精确和连续调节.
- 使用基于MoS2的FGFET成功实现了一个可编程的NOR逻辑门.
- 扩展设计以实现更复杂的可编程逻辑功能,展示功能完整性.
结论:
- 像MoS2这样的原子薄半导体对低功耗电子来说是有前途的.
- 基于MoS2的FGFET可实现集成逻辑和内存的高效内存计算.
- 这种方法为下一代AI和机器学习的节能电子硬件铺平了道路.
相关概念视频
MOS Capacitor
1.3K
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...
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
1.3K
Semiconductors
1.2K
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...
1.2K
Types of Semiconductors
1.2K
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
1.2K
Biasing of Metal-Semiconductor Junctions
451
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...
451
Metal-Semiconductor Junctions
717
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...
717
Fermi Level Dynamics
510
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...
510


