Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

The Hall Effect01:30

The Hall Effect

4.8K
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.
4.8K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

2.1K
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...
2.1K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.6K
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...
1.6K
Magnetic Fields01:27

Magnetic Fields

7.7K
A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
7.7K
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

1.3K
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.
1.3K
Torque On A Current Loop In A Magnetic Field01:13

Torque On A Current Loop In A Magnetic Field

6.2K
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...
6.2K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Relationships between psychosocial aspects of stuttering and self-disclosure of stuttering in a Japanese sample.

Journal of fluency disorders·2026
Same author

Emergent Spin Supersolids in Frustrated Quantum Materials.

Advanced materials (Deerfield Beach, Fla.)·2026
Same author

Surface Magnon Propagation in a van der Waals Antiferromagnet.

Physical review letters·2026
Same author

Spin Seebeck Effect of Triangular Lattice Spin Supersolid.

Physical review letters·2025
Same author

High-sensitive mechanical response in metal-insulator nanogranular films with large gauge factor.

Scientific reports·2025
Same author

Doping Effects on Magnetic and Electronic Transport Properties in (Ba<sub>1-x</sub>Rb<sub>x</sub>)(Zn<sub>1-y</sub>Mn<sub>y</sub>)<sub>2</sub>As<sub>2</sub> (0.1 ≤ x, y ≤ 0.25).

Nanomaterials (Basel, Switzerland)·2025

Related Experiment Video

Updated: Mar 11, 2026

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

10.6K

Spin current, spin accumulation and spin Hall effect.

Saburo Takahashi1, Sadamichi Maekawa2

  • 1Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan; CREST, Japan Science and Technology Agency (JST), Kawaguchi 332-0012, Japan.

Science and Technology of Advanced Materials
|November 24, 2016
PubMed
Summary

This study explores nonlocal spin transport in nanodevices, detailing how factors like interface resistance and spin diffusion length influence spin injection and accumulation. It also explains the spin Hall effect

Keywords:
spin Hall effectspin accumulationspin currentspin detectionspin diffusion lengthspin injectionspin polarized transportspin-orbit interaction

More Related Videos

Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
07:42

Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains

Published on: July 20, 2022

3.5K
Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
15:58

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing

Published on: December 3, 2013

6.1K

Related Experiment Videos

Last Updated: Mar 11, 2026

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

10.6K
Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
07:42

Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains

Published on: July 20, 2022

3.5K
Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
15:58

Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing

Published on: December 3, 2013

6.1K

Area of Science:

  • Condensed matter physics
  • Spintronics
  • Nanotechnology

Background:

  • Investigates nonlocal spin transport in nanostructured devices featuring ferromagnetic (F1, F2) and normal (N) conductors.
  • Examines the critical role of interface resistance, electrode resistance, spin polarization, and spin diffusion length in spin transport dynamics.

Approach:

  • Analyzes the conditions necessary for efficient spin injection, spin accumulation, and spin current generation within the device.
  • Demonstrates that the spin Hall effect, arising from spin-orbit scattering in nonmagnetic conductors, facilitates spin-charge current conversion.

Key Points:

  • Spin transport efficiency is tunable via interface and electrode resistances.
  • Spin diffusion length significantly impacts spin accumulation levels.
  • Spin Hall effect is a key mechanism for spin-charge conversion in nonlocal geometries.

Conclusions:

  • Proposes a novel method for evaluating spin-orbit coupling in nonmagnetic metals.
  • Provides a comprehensive understanding of nonlocal spin transport for spintronic applications.
  • Highlights the importance of interface engineering for optimizing spin-based devices.