模糊的接口诱导了约瑟夫森交叉点的电气传输特性控制
Junling Qiu1, Huihui Sun2, Chuanbing Han1
1Laboratory for Advanced Computing and Intelligence Engineering, Zhengzhou, 450001, China.
Scientific reports
|July 27, 2024
概括
我们开发了一种新方法来分析约瑟夫森结点,发现接口上的氧比率显著影响电气性能和量子比特性能. 这项研究有助于识别缺陷,以改善芯片制造.
科学领域:
- 材料科学 材料科学 材料科学
- 量子计算是一种量子计算.
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 约瑟夫森连接处的接口微结构对于超导量子比特性能至关重要.
- 了解原子结构和电气行为之间的联系是具有挑战性的.
研究的目的:
- 提出一种新的方法来定义约瑟夫森结接口的界面.
- 通过材料分析和第一原则计算,研究影响节点电气性能的因素.
主要方法:
- 材料分析技术. 材料分析技术.
- 第一原则计算.第一原则计算.
- 用于数据增强的生成对抗网络.
主要成果:
- 接口上的氧比率显著影响接口的电气性能.
- 最佳的氧比率 (0.67-1.1) 会导致更低的屏障高度和更好的交叉性能.
- 当屏障厚度固定时,氧比率的影响是突出的.
结论:
- 对约瑟夫森连接的微观分析可以识别工艺缺陷,以提高芯片产量.
- 在约瑟夫森结点中建立了微观结构和宏观性能之间的强烈相关性.
相关概念视频
Biasing of Metal-Semiconductor Junctions
235
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...
235
Biasing of FET
247
Biasing a Junction Field Effect Transistor (JFET) is crucial for setting operational parameters and ensuring efficient functioning in electronic circuits. JFETs are characterized by using a single carrier type in N-channel or P-channel configurations, where the channel is surrounded by PN junctions. These junctions are central to the device's ability to control current flow.
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
247
Biasing of P-N Junction
485
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...
485
Metal-Semiconductor Junctions
324
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...
324
P-N junction
503
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...
503
Characteristics of JFET
469
Junction Field Effect Transistors (JFETs) exhibit specific operational characteristics based on the relationship between the drain current (id) and the drain-source voltage (Vds), along with varying gate-source voltages (Vgs).
The core of a JFET's operation is controlling drain current by modulating the gate-source voltage. When the drain and gate voltage are set to zero, the JFET exhibits no net current flow, representing a state of equilibrium. The drain current increases linearly as the...
The core of a JFET's operation is controlling drain current by modulating the gate-source voltage. When the drain and gate voltage are set to zero, the JFET exhibits no net current flow, representing a state of equilibrium. The drain current increases linearly as the...
469


