Jordan–Chevalley decomposition

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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.

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Predicate Object
instanceOf concept in linear algebra
concept in representation theory
mathematical theorem
alsoKnownAs Jordan decomposition NERFINISHED
additive Jordan decomposition NERFINISHED
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 NERFINISHED
influences modern representation theory of Lie algebras
structure theory of linear algebraic groups
namedAfter Camille Jordan NERFINISHED
Claude Chevalley NERFINISHED
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 NERFINISHED
rational canonical form
representation theory of Lie algebras
representation theory of algebraic groups
structure theory of linear operators

Referenced by (2)

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Camille Jordan knownFor Jordan–Chevalley decomposition
Fitting lemma relatedTo Jordan–Chevalley decomposition