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 Electrical Double Layer01:30

The Electrical Double Layer

In the region where two bulk phases meet, an intricate electric charge distribution arises due to charge transfer, ion adsorption, molecular orientation, and charge distortion. This complex distribution is commonly referred to as the electrical double layer.When a solid electrode interfaces with ions in an electrolyte solution, the speed of electron transfer dictates the rates of oxidation and reduction. The electrode acquires a charge through the escape of atoms into the solution as cations or...
Debye–Huckel–Onsager Conductance Equation01:28

Debye–Huckel–Onsager Conductance Equation

The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect. According to this equation,...
Types of Reversible Electrodes01:24

Types of Reversible Electrodes

For electrode reversibility to be maintained, all the reactants and products involved in the half-reaction must be present at the electrode. There are several types of reversible electrodes (half-cells).In metal-metal-ion electrodes, a metal balances electrochemically with a solution of its own ions. Examples are Cu2+|Cu and Zn2+|Zn. Metals that react with the solvent, like group 1 and most group 2 metals, which react with water, and zinc, which reacts with aqueous acidic solutions, cannot be...
Electrochemical Systems01:24

Electrochemical Systems

Electrochemical systems provide a fascinating insight into the dynamic interplay of charged species within various phases. One notable example is the interaction between a membrane permeable to K⁺ ions but not to Cl⁻ ions, separating an aqueous KCl solution from pure water. As K⁺ ions diffuse through the membrane, they generate net charges on each phase, leading to a potential difference between them.Similarly, when a piece of Zn is immersed in an aqueous ZnSO₄ solution, the Zn metal, composed...
Standard Electrode Potentials03:02

Standard Electrode Potentials

On comparing the reactivity of silver and lead, it is observed that the two ionic species, Ag+ (aq) and Pb2+ (aq), show a difference in their redox reactivity towards copper: the silver ion undergoes spontaneous reduction, while the lead ion does not. This relative redox activity can be easily quantified in electrochemical cells by a property called cell potential. This property is commonly known as cell voltage in electrochemistry, and it is a measure of the energy which accompanies the charge...
Fermi Level01:18

Fermi Level

The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...

You might also read

Related Articles

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

Sort by
Same author

Effect of Co substitution on the magnetic and electron-transport properties of Mn2PtSn.

Journal of physics. Condensed matter : an Institute of Physics journal·2015
Same author

Structural and magnetic transitions in cubic Mn3Ga.

Journal of physics. Condensed matter : an Institute of Physics journal·2014
Same author

Hf-Co and Zr-Co alloys for rare-earth-free permanent magnets.

Journal of physics. Condensed matter : an Institute of Physics journal·2014
Same author

Permanent magnetism of intermetallic compounds between light and heavy transition-metal elements.

Journal of physics. Condensed matter : an Institute of Physics journal·2014
Same author

Inspired by nature: investigating tetrataenite for permanent magnet applications.

Journal of physics. Condensed matter : an Institute of Physics journal·2014
Same author

On the synthesis and physical properties of iron doped SnO2 nanoparticles.

Journal of nanoscience and nanotechnology·2013

Related Experiment Video

Updated: May 31, 2026

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

Finite-temperature depolarization in half metals.

R Skomski1

  • 1Department of Physics and Astronomy and Nebraska Center for Materials and Nanoscience, University of Nebraska, Lincoln, NE 68588, USA.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|June 23, 2011
PubMed
Summary

Thermal spin mixing in half-metallic ferromagnets means conductivity is always nonzero, even in the

Area of Science:

  • Condensed matter physics
  • Materials science

Background:

  • Half-metallic ferromagnets ideally exhibit complete spin polarization.
  • Understanding temperature effects on spin polarization is crucial for spintronic applications.

Purpose of the Study:

  • Investigate the temperature dependence of spin polarization in type-I half-metallic ferromagnets.
  • Compare their behavior to other magnetic materials.

Main Methods:

  • Analysis of spin-down density of states (DOS) at finite temperatures.
  • Consideration of intersublattice interactions, spin-orbit coupling, and crystal imperfections.
  • Modeling using a version of the Kondo model and unrestricted Hartree-Fock approximation.

Main Results:

More Related Videos

Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
06:53

Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks

Published on: June 9, 2023

In Situ Neutron Powder Diffraction Using Custom-made Lithium-ion Batteries
11:25

In Situ Neutron Powder Diffraction Using Custom-made Lithium-ion Batteries

Published on: November 10, 2014

Related Experiment Videos

Last Updated: May 31, 2026

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
10:36

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating

Published on: April 12, 2018

Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
06:53

Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks

Published on: June 9, 2023

In Situ Neutron Powder Diffraction Using Custom-made Lithium-ion Batteries
11:25

In Situ Neutron Powder Diffraction Using Custom-made Lithium-ion Batteries

Published on: November 10, 2014

  • Stable atomic moments lead to nonzero spin-down DOS at finite temperatures, causing thermal spin mixing.
  • Half-metallic ferromagnetism is an idealized limit due to thermal spin mixing.
  • Increasing interatomic hopping destabilizes moments, reducing spin polarization via Stoner-type excitations.
  • Conclusions:

    • Thermal spin mixing limits the practical realization of ideal half-metallic ferromagnetism.
    • The hybridization gap closure temperature (T(*)) depends on hybridization gap and band width.
    • One-electron contributions are more significant than correlations for spin polarization behavior.