トポロジカルマター トポロジカルマター トポロジカルマター トポロジカルマター トポロジカルマター トポロジカルマター トポロジカルマター 超伝導体上の鉄磁性原子鎖におけるマヨラナフェルミオンの観測
Stevan Nadj-Perge1, Ilya K Drozdov1, Jian Li1
1Joseph Henry Laboratories and Department of Physics, Princeton University, Princeton, NJ 08544, USA.
まとめ
研究者は,一次元トポロジカルな超伝導体を実現するために,鉛 (Pb) に鉄 (Fe) の原子鎖を作り出した. 彼らはマジョラーナフェルミオン,これらのシステムの端に存在すると予測されたエキゾチックな粒子の証拠を観察しました.
科学分野:
- 凝縮物質物理学 凝縮物質物理学
- 材料科学 材料科学とは
- 量子物理学とは,量子物理学のことです.
背景:
- トポロジカルな超伝導体は,その端にマジョラーナ・フェルミオンのようなエキゾチックな準粒子を宿している.
- これらのシステムは,量子コンピューティングと基礎物理学の進歩に不可欠です.
- 一次元のトポロジカル超伝導体を製造することは,依然として大きな課題です.
研究 の 目的:
- 一次元のトポロジカルな超伝導体を実現するために.
- エンジニアリングされた原子鎖におけるマジョラーナフェルミオンの存在を調査するために.
主な方法:
- 超伝導性鉛 (Pb) 基板の上に鉄磁鉄 (Fe) 原子鎖を製造する.
- 高解像度スペクトル画像技術を使用して,電子特性を探査します.
- 状態の電子密度を分析し,ユニークなスペクトルシグネチャを特定する.
主要な成果:
- 超伝導性は,Feの原子鎖の大部分で誘導された.
- チェーンエッジでゼロエネルギーエンドステートの出現が観察されました.
- これらの終末状態は,トポロジカル・フェーズ形成の強力な証拠を提供します.
結論:
- 実験セットアップは,トポロジカルな超伝導体のための条件を成功裏に作成しました.
- エッジbound Majorana フェルミオンが検出され,理論的な予測が確認されました.
- この研究は,新しい量子電子装置の道を開く.
関連する概念動画
Ferromagnetism
2.8K
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...
2.8K
Types Of Superconductors
1.6K
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
1.6K
Superconductor
1.9K
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
1.9K
Theory of Metallic Conduction
1.9K
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,...
1.9K
Atomic Nuclei: Magnetic Resonance
1.2K
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
1.2K
Atomic Nuclei: Nuclear Relaxation Processes
1.1K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.1K


