通过纠状态道化在量子点接触中的门电压依赖的差电导率
1Asia Pacific Center for Theoretical Physics, Pohang, Gyeongbuk 37673, Republic of Korea.
概括
量子点接触显示了由于纠状态道化导致的门电压依赖导电性. 这种行为是由局部自转位移驱动的,从不对称到对称的Kondo合的过渡,由Green解释.
科学领域:
- 量子电子学 量子电子学
- 凝聚物质物理学 凝聚物质物理学
- 旋转电子 旋转电子
背景情况:
- 量子点接触器 (QPC) 是非常重要的纳米电子设备.
- 在QPC中,Kondo效应表现出受局部旋转影响的复杂行为.
- 纠状态道可以显著改变电荷传输特性.
研究的目的:
- 调查QPCs中的门电压依赖的差电导率.
- 阐明纠状态道化和局部自旋位移的作用.
- 分析从不对称到对称的Kondo合的过渡.
主要方法:
- 在Liouville空间中利用了Green的函数技术.
- 由运算符表示的系统构造的基向量.
- 现象学上确定模型参数以适应实验数据.
主要成果:
- 在QPC中证明了网关电压依赖的差电导率.
- 观察到门电压诱导的局部自旋位移.
- 在低电压下识别了左右不对称的Kondo合,在高电压下过渡到对称的合.
- 发现左和右动态之间的纠创造了一个连贯的侧峰,这对导电线形状至关重要.
结论:
- 纠状态道是理解QPC导电性的关键.
- 在Liouville空间中的Green的函数技术有效地模拟了这些现象.
- 这项研究成功地复制了实验观察到的门电压依赖导电特性.
更多相关视频
11:33All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
Published on: January 19, 2018
9.9K
11:42Fabrication of Gate-tunable Graphene Devices for Scanning Tunneling Microscopy Studies with Coulomb Impurities
Published on: July 24, 2015
15.6K
相关概念视频
P-N junction
689
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...
689
Metal-Semiconductor Junctions
517
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...
517
Carrier Transport
567
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
567
Biasing of Metal-Semiconductor Junctions
336
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...
336
Fermi Level Dynamics
348
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...
348
Electric Potential Energy of Two Point Charges
4.9K
The electric potential energy of a test charge in a uniform eclectic field can be generalized to any electric field produced by static charge distribution. Consider a positive test charge in an electric field produced by another static positive charge. If the test charge is moved away from the static charge, then the electric field does the positive work on the test charge, and the electric potential energy of the test charge decreases as it moves away from the static charge. Here the electric...
4.9K
