Linked from

The 18 pages that link to Exchange interaction, each with the reason it gives.

• Electron configurationRelated: It helps explain why parallel spins can stabilize half-filled subshells.

• FerromagnetismRelated: Its energy favors parallel neighboring spins in common ferromagnets.

• Curie temperatureRelated: It drives the alignment that thermal agitation overcomes above the Curie temperature.

• Magnetic domainRelated: It aligns neighboring moments, helping create a uniformly magnetized region.

• AntiferromagnetismRelated: Its sign and strength determine whether neighboring moments align antiparallel.

• Hartree–Fock methodRelated: Antisymmetry creates an exchange term in the effective interaction between electrons.

• Electron correlationCompared with: It is distinct from correlation caused by electrons responding to one another’s positions.

• FerrimagnetismRelated: Exchange interactions establish the antiparallel alignment between ferrimagnetic sublattices.

• Hund's rulesRelated: It helps explain the energetic preference for parallel spins behind the first rule.

• MagnetismRelated: It can align atomic moments into ordered magnetic states.

• Heisenberg modelRelated: It produces the effective coupling between neighboring spins.

• Fritz LondonRelated: Electron exchange creates the energetic distinction between bonding and antibonding molecular states.

• Permanent magnetRelated: It drives the collective alignment underlying ferromagnetism.

• Curie–Weiss law (magnetism)Related: Its effective influence aligns or opposes neighboring moments, shifting the characteristic temperature.

• Spontaneous magnetizationRelated: In ferromagnets, it can favor parallel alignment of neighboring magnetic moments.

• Classical spin modelsRelated: Its sign and strength determine whether neighboring spins favor alignment or opposition.

• Hund's rule of maximum multiplicityRelated: Exchange effects help explain why parallel-spin arrangements can have lower energy.

• Magnetic systemsRelated: It produces collective magnetic order that cannot be explained by classical dipoles alone.