KTaO3 (111) インターフェースにおける二次元超伝導性とアニゾトロプ的輸送
Changjiang Liu1, Xi Yan2,3,4, Dafei Jin5
1Materials Science Division, Argonne National Laboratory, Lemont, IL 60439, USA. anand@anl.gov changjiang.liu@anl.gov.
まとめ
超伝導性は,電子ガスの111方向のKTaO3インターフェイスで発生し,2.2ケルビンに達する. カリウムタンタラート (KTaO3) システムでのこの発見は,以前同様の材料で観察されたものより著しく高い.
科学分野:
- 凝縮物質物理学
- 材料科学
- 量子材料について
背景:
- 非従来の量子状態は 物質界面の ユニークな電子構造から生じる
- オキシド間のインターフェイスは,超伝導性を含む新興電子現象をホストすることが知られている.
研究 の 目的:
- 電子ガスの超伝導性の可能性を (111) 方向のKTaO3を含むインターフェースで調査する.
- LaAlO3/SrTiO3のような確立されたシステムとの KTaO3 インターフェースの超伝導特性を比較する.
主な方法:
- KTaO3と絶縁層 (EuOまたはLaAlO3) の間のインターフェースの製造
- クリティカルフィールドと電流-電圧の特性を含む電気輸送測定.
- 超伝導的移行温度を決定する温度依存の抵抗測定
主要な成果:
- EuO/KTaO3 (111) とLaAlO3/KTaO3 (111) インターフェイスにおける電子ガスの超伝導性の発見.
- LaAlO3/SrTiO3よりも大きさのオーダーである2.2ケルビンまでの超伝導的移行温度が観察されました.
- 超伝導性の二次元性は確認されました 超伝導性以前のEuO/KTaO3 (111) サンプルでは,明確なストライプ状の相が現れた.
結論:
- (111) 方向の KTaO3 インターフェースは,新興超伝導性の新しいプラットフォームを提供します.
- 観測された超伝導性は,他の酸化接点と比較して大幅に強化されています.
- ストライプフェーズの出現は,これらのインターフェースの電子フェーズの複雑な相互作用を示唆しています.
関連する概念動画
Types Of Superconductors
1.4K
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...
1.4K
Theory of Metallic Conduction
1.6K
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,...
1.6K
Superconductor
1.5K
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...
1.5K
Magnetostatic Boundary Conditions
1.4K
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
1.4K
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
Boundary Conditions for Current Density
1.2K
Current density becomes discontinuous across an interface of materials with different electrical conductivities. The normal component of the current density is continuous across the boundary.
1.2K


