铁电领域 墙 p-n 交叉点
Jesi R Maguire1, Conor J McCluskey1, Kristina M Holsgrove1
1School of Mathematics and Physics, Queen's University Belfast, Belfast BT7 1NN, U.K.
Nano letters
|November 10, 2023
概括
研究人员绘制了酸薄膜中的电潜. 域壁连接处的行为不同于半导体连接处,影响未来的纳米电子应用.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 纳米技术纳米技术
背景情况:
- 尼奥酸盐中的铁电域壁具有独特的电气性质.
- 了解这些特性对于开发新型纳米电子设备至关重要.
- 传统的半导体连接物理可能不直接适用于铁电领域壁.
研究的目的:
- 为了研究沿导域壁的电潜力的空间分布.
- 分析这些域墙内的p-n连接点的行为.
- 为了确定控制这些墙内连接的基础物理.
主要方法:
- 使用高压凯尔文探针力显微镜 (KPFM) 进行潜在映射.
- 检查了X切割的单晶铁电酸薄膜.
- 在当前运行过程中进行的操作测量.
主要成果:
- 沿域墙绘制了电电位和电场的概况.
- 在域壁内观察到的p-n连接仅仅通过电阻变化来解释.
- 没有额外的物理,如载体耗尽或空间电荷场,是需要解释的.
结论:
- 铁电领域墙壁的内墙连接不需要传统的半导体连接物理.
- 半导体连接的关键是费米水平差异,在这些域壁中不存在.
- 与外部半导体系统相比,域壁纳米电子将表现出不同的行为,影响设备功能.
相关概念视频
P-N junction
543
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...
543
Biasing of P-N Junction
551
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
551
Metal-Semiconductor Junctions
354
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...
354
Ferromagnetism
2.4K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.4K
Biasing of Metal-Semiconductor Junctions
261
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...
261
Electrostatic Boundary Conditions in Dielectrics
1.2K
When an electric field passes from one homogeneous medium to another, crossing the boundary between the two mediums imparts a discontinuity in the electric field. This results in electrostatic boundary conditions that depend on the type of mediums the field propagates through.
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
Consider a case where both the mediums across a boundary are two different dielectric materials. Recall that the electric field and electric displacement are proportional and related through the material's...
1.2K


