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Related Concept Videos

Ferromagnetism01:31

Ferromagnetism

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...
Magnetic Force Between Two Parallel Currents01:13

Magnetic Force Between Two Parallel Currents

Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and  the vector product of the length vector along the current element and the field due to the first conductor. According to the...
Magnetic Field Due To A Thin Straight Wire01:27

Magnetic Field Due To A Thin Straight Wire

Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

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...
Magnetic Field Due to Two Straight Wires01:18

Magnetic Field Due to Two Straight Wires

Consider two parallel straight wires carrying a current of 10 A and 20 A in the same direction and separated by a distance of 20 cm. Calculate the magnetic field at a point "P2", midway between the wires. Also, evaluate the magnetic field when the direction of the current is reversed in the second wire.

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Related Experiment Video

Updated: Jun 11, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

A perpendicular-anisotropy CoFeB-MgO magnetic tunnel junction.

S Ikeda, K Miura, H Yamamoto

    Nature Materials
    |July 13, 2010
    PubMed
    Summary

    Researchers developed novel magnetic tunnel junctions (MTJs) using CoFeB-MgO for next-generation memory. These perpendicular MTJs offer high thermal stability, low switching current, and a high tunnel magnetoresistance ratio.

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

    Published on: July 20, 2022

    Related Experiment Videos

    Last Updated: Jun 11, 2026

    Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
    09:06

    Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

    Published on: March 24, 2019

    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

    Area of Science:

    • Spintronics and Nanomaterials Science
    • Solid State Physics and Materials Engineering

    Background:

    • Magnetic tunnel junctions (MTJs) are crucial for high-density non-volatile memory and logic devices.
    • Achieving perpendicular magnetic anisotropy is key for enhanced thermal stability and low switching currents.
    • Existing electrode materials for perpendicular anisotropy in MTJs have limitations in simultaneously meeting thermal stability, switching current, and magnetoresistance requirements.

    Discussion:

    • This study leverages interfacial perpendicular anisotropy at the ferromagnetic electrode-tunnel barrier interface.
    • The CoFeB-MgO material combination, known for high tunnel magnetoresistance in in-plane MTJs, is utilized.
    • The approach avoids novel materials, integrating into existing MTJ fabrication processes.

    Key Insights:

    • Perpendicular MTJs fabricated with Ta/CoFeB/MgO/CoFeB/Ta structures exhibit a tunnel magnetoresistance ratio exceeding 120%.
    • These MTJs demonstrate high thermal stability at dimensions as small as 40 nm.
    • A low critical current for magnetization switching of 49 microA was achieved.

    Outlook:

    • The findings pave the way for realizing high-performance, energy-efficient spintronic memory and logic devices.
    • Further research can optimize the CoFeB-MgO interface for even greater device performance.
    • This work offers a viable path towards scalable, next-generation magnetic memory technologies.