Van Vleck paramagnetism

E665838

Van Vleck paramagnetism is a quantum-mechanical form of paramagnetism arising from the mixing of electronic energy levels by an applied magnetic field, even in systems with no permanent magnetic moment in the ground state.

All labels observed (2)

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Statements (45)

Predicate Object
instanceOf form of paramagnetism ⓘ
quantum-mechanical magnetic phenomenon ⓘ
appearsIn insulating rare-earth salts ⓘ
lanthanide compounds ⓘ
some organic radicals with singlet ground states ⓘ
arisesFrom second-order perturbation of electronic states by a magnetic field ⓘ
canCoexistWith Curie paramagnetism ⓘ
Pauli paramagnetism ⓘ
canOccurIn closed-shell ions ⓘ
insulating solids ⓘ
molecular crystals ⓘ
rare-earth ions ⓘ
systems with singlet ground states ⓘ
transition-metal complexes ⓘ
category magnetochemistry ⓘ
quantum magnetism ⓘ
solid-state physics ⓘ
contributesTo total magnetic susceptibility of solids ⓘ
contributionType orbital contribution to paramagnetism ⓘ
dependsOn crystal-field splitting ⓘ
quantum-mechanical mixing of electronic energy levels ⓘ
spin–orbit coupling ⓘ
describedBy Van Vleck susceptibility formula ⓘ
distinctFrom Curie paramagnetism ⓘ
Langevin paramagnetism ⓘ
Pauli paramagnetism ⓘ
fieldRegime usually treated in low-field limit ⓘ
frameworkDevelopedBy John Hasbrouck Van Vleck ⓘ
importantIn crystal-field theory ⓘ
interpretation of EPR spectra ⓘ
magnetism of coordination compounds ⓘ
rare-earth magnetism ⓘ
magnetizationProportionalTo applied magnetic field ⓘ
mathematicallyExpressedAs sum over excited states of squared magnetic-moment matrix elements divided by energy separations ⓘ
namedAfter John Hasbrouck Van Vleck ⓘ
occursIn systems with no permanent magnetic moment in the ground state ⓘ
relatedTo magnetic susceptibility theory ⓘ
second-order Zeeman effect ⓘ
requires excited electronic states close in energy to the ground state ⓘ
non-zero matrix elements of the magnetic moment operator between ground and excited states ⓘ
susceptibilitySign positive ⓘ
temperatureDependence often nearly temperature independent ⓘ
weak ⓘ
usedIn analysis of magnetic anisotropy ⓘ
interpretation of temperature-independent paramagnetism in solids ⓘ

How these facts were elicited

Referenced by (3)

Full triples — surface form annotated when it differs from this entity's canonical label.

John Hasbrouck Van Vleck → knownFor → Van Vleck paramagnetism ⓘ
Van Vleck paramagnetism → describedBy → Van Vleck susceptibility formula ⓘ
linked to: Van Vleck paramagnetism
John Hasbrouck Van Vleck → knownFor → Van Vleck paramagnetism ⓘ
subject linked to: John