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Magnetic Force On A Current-Carrying Conductor01:25

Magnetic Force On A Current-Carrying Conductor

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Moving charges experience a force in a magnetic field. Since the magnetic fields produced by moving charges are proportional to the current, a conductor carrying a current creates a magnetic field around it.
Consider a compass placed near a current-carrying wire. The wire experiences a force that aligns the needle of the compass tangentially around the wire. Thus, the current-carrying wire produces concentric circular loops of magnetic field. The magnetic field generated by a wire can be...
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Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

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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...
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The Hall Effect01:30

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Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
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Magnetic Force01:18

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In addition to the electric forces between electric charges, moving electric charges exert magnetic forces on each other. A magnetic field is created by a moving charge or a group of moving charges known as the electric current. A magnetic force is experienced by a second current or moving charge in response to this magnetic field. Fundamentally, interactions between moving electrons in the atoms of two bodies produce magnetic forces between them.
The magnetic force acting on a moving charge...
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Lenz's Law01:15

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The direction in which the induced emf drives the current around a wire loop can be found through the negative sign. However, it is usually easier to determine this direction with Lenz's law, named in honor of its discoverer, Heinrich Lenz (1804–1865). Lenz's law states that the direction of the induced emf drives the current around a wire loop always to oppose the change in magnetic flux that causes the emf.
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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...
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在异磁CRSb中的方向依赖导电极性.

Banik Rai1, Krishnendu Patra1, Satyabrata Bera2

  • 1Department of Condensed Matter and Materials Physics, S. N. Bose National Centre for Basic Sciences, Salt Lake City, Kolkata, 700106, India.

Advanced science (Weinheim, Baden-Wurttemberg, Germany)
|May 9, 2025
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概括

在变磁抗氧化物 (CrSb) 中观察到方向依赖导电极性 (DDCP). 这种由不同的电子和孔带驱动的现象,在单一材料中提供可调的p型和n型功能.

关键词:
费米表面几何学费米表面几何学这是西贝克效应 (Seebeck effect).改变磁铁可以改变磁铁.取决于方向的导电极性.电力运输是电力运输的重要组成部分.

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科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 材料科学 材料科学 材料科学
  • 这就是Spintronics.

背景情况:

  • 抗氧化物 (CrSb) 被认为是一种有前途的变磁材料.
  • 变磁提供独特的自旋电磁性,与传统的铁磁性和反铁磁性不同.

研究的目的:

  • 通过实验研究CrSb.的电子传输特性.
  • 探索CrSb中方向依赖导电极性 (DDCP) 的现象.
  • 通过理论计算阐明DDCP的基本机制.

主要方法:

  • 实验测量包括霍尔效应和西贝克热力.
  • 密度函数理论 (DFT) 的计算.
  • 有控制的兴奋剂研究 (Cr$_{0.98}$V$_{0.02}$Sb).

主要成果:

  • 在CrSb中观察到的DDCP:沿c轴的孔主导导和ab平面的电子主导导.
  • DFT的计算证实了多载体机制,涉及不同的电子和孔带,负责DDCP.
  • 发现DDCP对兴奋剂敏感,实验验证显示其在V兴奋剂CrSb.中消失.

结论:

  • 由于DDCP,CrSb表现出可调节的电子行为.
  • 这些发现表明,CrSb在需要p型和n型功能的设备中的潜在应用.
  • 这项工作为进一步探索用于先进电子应用的变磁材料提供了基础.