Jove
Visualize
お問い合わせ
JoVE
x logofacebook logolinkedin logoyoutube logo
JoVEについて
概要リーダーシップブログJoVEヘルプセンター
著者向け
出版プロセス編集委員会範囲と方針査読よくある質問投稿
図書館員向け
推薦の声購読アクセスリソース図書館諮問委員会よくある質問
研究
JoVE JournalMethods CollectionsJoVE Encyclopedia of Experimentsアーカイブ
教育
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab Manual教員リソースセンター教員サイト
利用規約
プライバシーポリシー
ポリシー

関連する概念動画

Superconductor01:24

Superconductor

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...
Types Of Superconductors01:28

Types Of Superconductors

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...
Ferromagnetism01:31

Ferromagnetism

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...
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

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,...
Types of Semiconductors01:20

Types of Semiconductors

Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
P-N junction01:11

P-N junction

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...

こちらも読む

関連記事

共著者、ジャーナル、引用グラフによってこの研究に関連する記事。

並び替え
Same author

LncRNA SOX21-AS1 Promotes the Progression of Pancreatic Cancer by Sponging miR-9-3p and Upregulating YOD1.

The Kaohsiung journal of medical sciences·2025
Same author

Understanding the Beneficial Role of Transition-Metal Layer Na<sup>+</sup> Substitution on the Structure and Electrochemical Properties of the P2-Layered Cathode Na<sub>2+</sub> Ni<sub>2-</sub>TeO<sub>6</sub>.

Chemistry of materials : a publication of the American Chemical Society·2025
Same author

Superconductivity under pressure in a chromium-based kagome metal.

Nature·2024
Same author

Exotic Magnetism in Perovskite KOsO_{3}.

Physical review letters·2024
Same author

Tunable positions of Weyl nodes via magnetism and pressure in the ferromagnetic Weyl semimetal CeAlSi.

Nature communications·2024
Same author

Interphase Stabilization of LiNi<sub>0.5</sub> Mn<sub>1.5</sub> O<sub>4</sub> Cathode for 5 V-Class All-Solid-State Batteries.

Small (Weinheim an der Bergstrasse, Germany)·2023

関連する実験動画

Updated: Jun 20, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

鉄のない新しいピニクチド超伝導体.

Jian-Tao Han1, Jian-Shi Zhou, Jin-Guang Cheng

  • 1Texas Materials Institute, ETC 9.102, University of Texas at Austin, Austin, Texas 78712, USA.

Journal of the American Chemical Society
|October 1, 2009
PubMed
まとめ

2つの新しい化合物,リチウム銅酸化物 (LiCu2P2) とリチウム鉄酸化物 (LiFeP) が合成され,超伝導性を示すことが判明しました. LiCu2P2は3.5Kで超伝導し,LiFePは4.1Kで超伝導する.

科学分野:

  • マテリアルサイエンス 材料科学
  • 固体化学 固体化学
  • 凝縮物質物理学 凝縮物質物理学

背景:

  • 新材料における超伝導性は,技術的進歩にとって極めて重要です.
  • リン酸化合物は,超伝導体の新興クラスである.
  • 構造と性質の関係を理解することは,新しい超伝導材料を発見する鍵です.

研究 の 目的:

  • 新しいリチウム含有フォスフィード化合物を合成し,特徴づけること.
  • LiCu2P2とLiFePの結晶構造と超伝導性を研究する.
  • これらの新しい材料における構造-超伝導性の相関の可能性を調査する.

主な方法:

  • LiCu2P2とLiFePの合成のための固体反応.
  • クリスタル構造の決定のためのX線 difraktion.
  • 超伝導性を特定するための抵抗性と磁化測定.

主要な成果:

  • LiCu2P2は,BaFe2As2.2と同様の結晶構造で合成されました.
  • LiFePは,LiFeAsに似た結晶構造で合成されました.
  • LiCu2P2で3.5K,LiFePで4.1Kで超伝導性が観察されました.

さらに関連する動画

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
04:51

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

Published on: July 8, 2021

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

関連する実験動画

Last Updated: Jun 20, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
04:51

Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride

Published on: July 8, 2021

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

結論:

  • LiCu2P2とLiFePの成功した合成は,超伝導性の宿主としてのフォスフィドの生存可能性を実証しています.
  • 観測された超伝導的移行温度は,関連化合物の将来の研究のためのベースラインデータを提供します.
  • 既知の超伝導体との構造的類似性は,化学的改変を通じて特性を調節する可能性を示唆しています.