绘制多终端约瑟夫森交叉口的拓近距离诱导的差距.
M Wisne1, Y Deng1, I M A Lilja2
1Department of Physics and Astronomy, <a href="https://ror.org/000e0be47">Northwestern University</a>, 2145 Sheridan Road, Evanston, Illinois 60208, USA.
Physical review letters
|January 3, 2025
概括
研究人员探索了多终端约瑟夫森结 (MTJJs) 作为拓晶体. 测量MTJJ阻力揭示了准粒子密度状态的拓调制,为研究拓物理提供了一种新技术.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子材料是一种量子材料.
- 超导电性 超导电性 超导电性
背景情况:
- 多终端约瑟夫森结 (MTJJs) 被提出为人工拓晶体.
- MTJJs的拓性质与正常金属中的准粒子状态密度 (DOS) 的调制有关.
- 这些调制在理论上可以通过道测量进行探测.
研究的目的:
- 展示一种实用的方法来揭示MTJJs中的拓效应.
- 研究MTJJ电阻与相位差异之间的关系.
- 建立一种探测准粒子DOS调制的技术.
主要方法:
- 扩散式多终端约瑟夫森连接器 (MTJJs) 的制造和测量.
- 使用正常接触来进行电阻测量.
- 分析电阻作为超导相差的函数.
主要成果:
- 观察到扩散型MTJJs的抗力丰富的结构.
- 证明了电阻测量可以揭示准粒子DOS中的拓调制.
- 建立了电阻变化和相位差异之间的相关性.
结论:
- 电阻测量提供了一种简单而强大的技术,用于探索MTJJ中的拓效应.
- 该研究验证了MTJJ作为研究拓现象的平台.
- 这些发现为拓量子设备的进一步研究开辟了道路.
相关概念视频
Biasing of Metal-Semiconductor Junctions
173
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...
173
P-N junction
391
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...
391
Metal-Semiconductor Junctions
238
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...
238
Biasing of P-N Junction
343
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...
343
Path Between Thermodynamics States
2.9K
Consider the two thermodynamic processes involving an ideal gas that are represented by paths AC and ABC in Figure 1:
2.9K
Characteristics of JFET
297
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...
297


