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Ferromagnetism01:31

Ferromagnetism

2.7K
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...
2.7K
Paramagnetism01:30

Paramagnetism

2.8K
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...
2.8K
Types Of Superconductors01:28

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
Magnetostatic Boundary Conditions01:28

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
Diamagnetism01:26

Diamagnetism

2.7K
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....
2.7K
Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

1.8K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.8K

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Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
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原子工程铁层产生室温磁电多铁层

Julia A Mundy1, Charles M Brooks2, Megan E Holtz1

  • 1School of Applied and Engineering Physics, Cornell University, Ithaca, New York 14853, USA.

Nature
|September 23, 2016
PubMed
概括

研究人员开发了一种新方法,用于创建单相多铁材料,并与室温附近的铁电和强磁性相结合,使先进的存储器件能够控制电场的磁性.

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Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers
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科学领域:

  • 凝聚物质物理学
  • 材料科学
  • 固态化学

背景情况:

  • 具有同时电磁排序的多铁材料是下一代记忆器件的关键.
  • 已知的单相多铁元素由于具有竞争性的铁电和磁性要求而罕见,通常具有较弱的磁性或较低的操作温度.

研究的目的:

  • 提出一种新的方法来构建单相多铁材料,并与室温附近的铁电和强磁顺序.
  • 为了使电场对磁场的控制成为潜在的设备应用.

主要方法:

  • 通过将FeO单层引入六边形LuFeO3矩阵来合成 (LuFeO3) m/LuFe2O4) 1超级格子.
  • 使用几何铁电LuFeO3的平面来诱导铁磁LuFe2O4层中的铁电.
  • 使用表轴工程和利用网格扭曲.

主要成果:

  • 成功创建了单相多铁材料,并与室温附近的铁电和铁磁顺序结合.
  • 在超级网格结构中将LuFe2O4的磁转换温度从240K提高到281K.
  • 证明了对200K的磁场的直接电场控制

结论:

  • 开发的方法使得高温磁电多铁的设计成为可能.
  • 这种方法结合了几何挫折,格子扭曲和表轴工程来获得新的材料特性.
  • 这些发现为具有电场调节磁性的先进记忆装置铺平了道路.