Jordan–Chevalley decomposition

E904578

The Jordan–Chevalley decomposition is a fundamental result in linear algebra and representation theory that expresses a linear operator (or matrix) as the sum or product of commuting semisimple and nilpotent parts.

All labels observed (3)

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Statements (48)

Predicate Object
instanceOf concept in linear algebra ⓘ
concept in representation theory ⓘ
mathematical theorem ⓘ
alsoKnownAs Jordan decomposition ⓘ
additive Jordan decomposition ⓘ
appliesTo linear operators ⓘ
square matrices ⓘ
assumption base field often assumed algebraically closed ⓘ
characteristic of the field often assumed to be zero or sufficiently large ⓘ
component nilpotent part ⓘ
semisimple part ⓘ
unipotent part ⓘ
context finite-dimensional vector spaces ⓘ
describes decomposition of a linear operator into semisimple and nilpotent parts ⓘ
field linear algebra ⓘ
representation theory ⓘ
generalizes Jordan normal form for matrices ⓘ
hasForm additive decomposition ⓘ
multiplicative decomposition ⓘ
historicalPeriod 20th century mathematics ⓘ
holdsIn any finite-dimensional representation of a Lie algebra over an algebraically closed field of characteristic zero ⓘ
any finite-dimensional representation of a linear algebraic group over an algebraically closed field of characteristic zero ⓘ
implies eigenvalues of the operator are eigenvalues of its semisimple part ⓘ
nilpotent part has only zero as eigenvalue ⓘ
influencedBy Jordan normal form ⓘ
influences modern representation theory of Lie algebras ⓘ
structure theory of linear algebraic groups ⓘ
namedAfter Camille Jordan ⓘ
Claude Chevalley ⓘ
over algebraically closed field of characteristic zero ⓘ
property decomposition is unique ⓘ
semisimple and nilpotent parts are polynomials in the original operator ⓘ
semisimple and nilpotent parts commute ⓘ
relatedConcept nilpotent operator ⓘ
primary decomposition theorem ⓘ
semisimple operator ⓘ
spectral decomposition ⓘ
unipotent operator ⓘ
requires minimal polynomial factorization into distinct and repeated irreducible factors ⓘ
statement every invertible linear operator can be written as the product of a semisimple operator and a unipotent operator that commute ⓘ
every linear operator can be written as the sum of a semisimple operator and a nilpotent operator that commute ⓘ
toolFor analyzing representations via semisimple and nilpotent elements ⓘ
defining semisimple and unipotent elements in algebraic groups ⓘ
usedIn Jordan normal form ⓘ
rational canonical form ⓘ
representation theory of Lie algebras ⓘ
representation theory of algebraic groups ⓘ
structure theory of linear operators ⓘ

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Referenced by (5)

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

Camille Jordan → knownFor → Jordan–Chevalley decomposition ⓘ
Fitting lemma → relatedTo → Jordan–Chevalley decomposition ⓘ
Jordan normal form theorem → hasVariant → Jordan–Chevalley decomposition ⓘ
Jordan–Chevalley decomposition → alsoKnownAs → Jordan decomposition ⓘ
linked to: Jordan–Chevalley decomposition
Jordan–Chevalley decomposition → alsoKnownAs → additive Jordan decomposition ⓘ
linked to: Jordan–Chevalley decomposition