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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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...
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.
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved in...
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.
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Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
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Published on: January 21, 2016

Quantum renormalization of the spin Hall effect.

Bo Gu1, Jing-Yu Gan, Nejat Bulut

  • 1Advanced Science Research Center, Japan Atomic Energy Agency, Tokai 319-1195, Japan.

Physical Review Letters
|September 28, 2010
PubMed
Summary

Spin-orbit interaction (SOI) in iron (Fe) impurities within gold (Au) is significantly altered by quantum spin fluctuations and electron correlations. This finding explains experimental observations of the spin Hall effect but not the anomalous Hall effect.

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Area of Science:

  • Condensed Matter Physics
  • Quantum Many-Body Theory
  • Materials Science

Background:

  • The spin Hall effect (SHE) and anomalous Hall effect (AHE) are crucial phenomena in spintronics.
  • Understanding the microscopic origins of these effects, particularly in systems with magnetic impurities, is essential for device applications.
  • Previous studies have not fully reconciled experimental observations of SHE and AHE in gold (Au) with iron (Fe) impurities.

Purpose of the Study:

  • To investigate the microscopic mechanisms governing spin-orbit interaction (SOI) in an Fe impurity embedded in an Au host.
  • To elucidate the role of quantum spin fluctuations and Coulomb correlations in renormalizing SOI.
  • To explain the contrasting experimental observations of the gigantic spin Hall effect and the absent anomalous Hall effect in Au:Fe.

Main Methods:

  • Utilizing quantum Monte Carlo (QMC) simulations.
  • Employing a realistic multiorbital Anderson impurity model.
  • Analyzing the renormalization effects of quantum spin fluctuation and Coulomb correlation (U) on SOI.

Main Results:

  • Demonstrated that spin-orbit interaction (SOI) is strongly renormalized by quantum spin fluctuation.
  • Showed that SOI is also significantly renormalized by Coulomb correlation (U).
  • Established a theoretical basis for the experimentally observed gigantic spin Hall effect in Au with Fe impurities, while explaining the absence of the anomalous Hall effect.

Conclusions:

  • Quantum spin fluctuations and Coulomb correlations are key mechanisms renormalizing spin-orbit interaction in Fe impurities within Au.
  • This renormalization provides a unified explanation for the distinct experimental behaviors of the spin Hall effect and anomalous Hall effect.
  • The study resolves past discrepancies in calculated orbital angular momenta for Fe impurities in Au host metals.