磁気は,原子から鉄,コバルト,ニッケル・クラスターの質量まで広がる
まとめ
鉄,コバルト,ニッケル・クラスターの磁性は,小さなサイズでも現れます. 磁気モメントはクラスターの大きさとともに大きくなり,塊の値に近づき,振動はおそらくスピン密度波によるものである.
科学分野:
- マテリアルサイエンス 材料科学
- 凝縮物質物理学 凝縮物質物理学
- 表面科学とは,地表科学である.
背景:
- ナノスケール材料の磁気性を理解することは,新しい技術の開発に不可欠です.
- クラスターの大きさ,温度,磁気特性の関係については,詳細な調査が必要である.
研究 の 目的:
- 鉄,コバルト,ニッケル・クラスターにおける磁力の発展を調査する.
- 磁気特性をクラスタサイズと温度と相関させるため.
- これらのクラスターにおける磁気力の根本的なメカニズムを解明する.
主な方法:
- 分子ビームの傾斜測定を用いた.
- 実験は,80~1000Kの温度範囲で実施されました.
- クラスターの大きさは,数十から数百の原子まで様々でした.
主要な成果:
- 鉄磁気は,最小のクラスターでも観察されました.
- 磁気モメントはクラスターの大きさとともに増加し,鉄,コバルト,ニッケルの大量値に近づきました.
- 磁気モメントの振動が検出され,表面に誘発されたスピン密度波による可能性がある.
- 鉄のクラスターでは,高磁気モーメントから低磁気モーメントへの結晶学的相変化が確認されました.
結論:
- 磁気殻モデルは,磁気における観測された傾向を効果的に説明します.
- 表面効果は,これらのクラスターの磁気行動に重要な役割を果たします.
- 大きさに依存する磁気と相変遷は,鉄,コバルト,ニッケル・クラスターの重要な特徴である.
関連する概念動画
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...
Colors and Magnetism
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human eye.
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human eye.
Magnetic Moment of an Electron
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
Diamagnetism
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.
Valence Bond Theory
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
Paramagnetism
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...


