基塔耶夫链中的Majorana子与普通金属侧联
1School of Physics, University of Hyderabad, Prof. C. R. Rao Road, GachibowliC. R. Rao Road, Gachibowli, Hyderabad 500046, India.
概括
在与基塔耶夫链相结合的正常金属中,即使在微不足道的阶段,Majorana子也可以出现. 基塔耶夫链的拓相可以在正常金属中诱导额外的马约拉纳费米子.
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.
背景情况:
- 马约拉纳费米子是异国情调的粒子,具有量子计算应用的巨大潜力.
- 基塔耶夫模型是研究1D系统中Majorana子出现的关键理论框架.
研究的目的:
- 为了调查Majorana费米子在正常金属 (NM) 中出现的可能性,与基塔耶夫链 (KC) 合在其拓上微不足道的阶段.
- 要确定一个拓相基塔耶夫链能否在相邻的正常金属中诱导马约拉纳费米子.
主要方法:
- 理论分析一个与基塔耶夫链接的一侧合的普通金属.
- 进行了广泛的参数空间探索,以确定Majorana子出现的条件.
- 对磁流效应的研究和绕数计算的拓不变量.
主要成果:
- 在正常金属中出现Majorana子的肯定证据,即使Kitaev链处于拓学上微不足道的阶段.
- 证明拓相基塔耶夫链可以在邻近的正常金属中诱导额外的Majorana子.
- 在合系统中识别支持零,一或两对Majorana费米子的场景.
结论:
- 在特定条件下,Majorana子可以在与Kitaev链合的正常金属中实现.
- 基塔耶夫链的拓性质在诱导邻近的正常金属中的马约拉纳费米子中起着至关重要的作用.
- 该系统可以对Majorana费米子的数量进行调节控制,这对拓量子计算架构有潜在的影响.
更多相关视频
04:51Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
Published on: July 8, 2021
2.7K
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
8.1K
相关概念视频
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
Theory of Metallic Conduction
1.3K
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
1.3K
Bonding in Metals
47.1K
Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”.
47.1K
Biasing of Metal-Semiconductor Junctions
239
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...
239
Properties of Transition Metals
25.4K
Transition metals are defined as those elements that have partially filled d orbitals. As shown in Figure 1, the d-block elements in groups 3–12 are transition elements. The f-block elements, also called inner transition metals (the lanthanides and actinides), also meet this criterion because the d orbital is partially occupied before the f orbitals.
25.4K
Metal-Semiconductor Junctions
333
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...
333
