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Related Concept Videos

The Hall Effect01:30

The Hall Effect

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.
Atomic Nuclei: Nuclear Magnetic Moment00:59

Atomic Nuclei: Nuclear Magnetic Moment

All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis. This...
Torque On A Current Loop In A Magnetic Field01:13

Torque On A Current Loop In A Magnetic Field

The most common application of magnetic force on current-carrying wires is in electric motors. These consist of loops of wire, which are placed between the magnets with a magnetic field. When current flows through the loops, the magnetic field applies torque, which causes the shaft to rotate, thus converting electrical energy to mechanical energy.
Consider a rectangular current-carrying loop containing N turns of wire, placed in a uniform magnetic field. The net force on a current-carrying loop...

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Magnetic Tweezers for the Measurement of Twist and Torque
11:41

Magnetic Tweezers for the Measurement of Twist and Torque

Published on: May 19, 2014

Inverse spin Hall effect driven by spin motive force.

Junya Shibata1, Hiroshi Kohno

  • 1Kanagawa Institute of Technology, 1030 Shimo-Ogino Atsugi, Kanagawa 243-0292, Japan. shibata@gen.kanagawa-it.ac.jp

Physical Review Letters
|March 5, 2009
PubMed
Summary

Researchers explored the inverse spin Hall effect in ferromagnetic conductors, finding that a spin motive force induces a charge Hall current. This effect is significantly enhanced compared to the conventional anomalous Hall effect.

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Area of Science:

  • Condensed Matter Physics
  • Spintronics
  • Materials Science

Background:

  • The spin Hall effect involves electric fields inducing spin currents.
  • Understanding inverse effects is crucial for spintronic devices.

Purpose of the Study:

  • To investigate the inverse spin Hall effect in ferromagnetic conductors.
  • To analyze charge Hall current generation from spin motive forces.

Main Methods:

  • Theoretical analysis considering skew-scattering and side-jump processes.
  • Incorporating spin-orbit interaction at impurities.
  • Modeling spin-dependent effective electric fields (E_s).

Main Results:

  • Derived Hall current density formula: sigma_SH * n x E_s.
  • Quantified spin Hall conductivity (sigma_SH).
  • Observed enhancement factor of P-2 compared to anomalous Hall effect.

Conclusions:

  • The spin motive force significantly induces charge Hall currents in ferromagnetic materials.
  • The inverse spin Hall effect shows enhanced Hall angles due to spin polarization (P).
  • Potential applications in domain-wall dynamics within ferromagnetic nanowires were estimated.