网关定义的约瑟夫森弱链在单层WTe2中
Michael D Randle1, Masayuki Hosoda2, Russell S Deacon1,3
1Advanced Device Laboratory, RIKEN, 2-1 Hirosawa, Wako, Saitama, 351-0198, Japan.
Advanced materials (Deerfield Beach, Fla.)
|June 26, 2023
概括
单层二化 (WTe2) 显示出对拓量子计算的前景. 研究人员制造了约瑟夫森弱链装置,这对于推进具有拓超导体的容错量子计算至关重要.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子计算是一种量子计算.
- 材料科学 材料科学 材料科学
背景情况:
- 拓绝缘体和超导体是研究Majorana束状态和容错拓量子计算的关键.
- 单层二化 (WTe2) 具有量子自旋霍尔绝缘体 (QSHI) 和可调的超导特性的独特组合.
研究的目的:
- 为了研究使用单层WTe2.2制造的约瑟夫森弱链装置的特性.
- 探索 WTe2 的潜力,作为一个多功能材料,用于全合一的拓约瑟夫森弱链.
主要方法:
- 使用单层WTe2.2制造网关定义的约瑟夫森弱链装置.
- 在制造的连接处测试磁干扰的实验测量.
- 考虑二维超导电线的关键作用的分析.
主要成果:
- 使用单层WTe2.2成功制造约瑟夫森弱链装置.
- 确定了二维超导线对解释磁干扰模式的关键影响.
- 为这种具有挑战性的材料建立了简单的制造程序.
结论:
- 这些结果代表了向创建多功能全合一拓约瑟夫森弱链的重要第一步.
- 单层WTe2是推进拓量子计算技术的一个有前途的材料.
相关概念视频
Metal-Semiconductor Junctions
395
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...
395
Network Covalent Solids
13.6K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
13.6K
P-N junction
590
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...
590
Bewley Lattice Diagram
771
The Bewley lattice diagram, developed by L. V. Bewley, effectively organizes the reflections occurring during transmission-line transients. It visually represents how voltage waves propagate and reflect within a transmission line, making it easier to understand the complex interactions that occur.
771
Biasing of Metal-Semiconductor Junctions
284
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...
284
Spin–Spin Coupling: One-Bond Coupling
1.0K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.0K


