# Weight (representation theory)

In the mathematical field of representation theory, a **weight** of an algebra *A* over a field **F** is an algebra homomorphism from *A* to **F**, or equivalently, a one-dimensional representation of *A* over **F**. It is the algebra analogue of a multiplicative character of a group. The importance of the concept, however, stems from its application to representations of Lie algebras and hence also to representations of algebraic and Lie groups. In this context, a **weight of a representation** is a generalization of the notion of an eigenvalue, and the corresponding eigenspace is called a **weight space**.

The notion is closely related to the idea of a multiplicative character in group theory, which is a homomorphism *χ* from a group *G* to the multiplicative group of a field **F**. Thus *χ*: *G* → **F**^{×} satisfies *χ*(*e*) = 1 (where *e* is the identity element of *G*) and

Indeed, if *G* acts on a vector space *V* over **F**, each simultaneous eigenspace for every element of *G*, if such exists, determines a multiplicative character on *G*: the eigenvalue on this common eigenspace of each element of the group.

The notion of multiplicative character can be extended to any algebra *A* over **F**, by replacing *χ*: *G* → **F**^{×} by a linear map *χ*: *A* → **F** with:

for all *a*, *b* in *A*. If an algebra *A* acts on a vector space *V* over **F** to any simultaneous eigenspace, this corresponds an algebra homomorphism from *A* to **F** assigning to each element of *A* its eigenvalue.

If *A* is a Lie algebra (which is generally not an associative algebra), then instead of requiring multiplicativity of a character, one requires that it maps any Lie bracket to the corresponding commutator; but since **F** is commutative this simply means that this map must vanish on Lie brackets: *χ*([a,b])=0. A **weight** on a Lie algebra **g** over a field **F** is a linear map λ: **g** → **F** with λ([*x*, *y*])=0 for all *x*, *y* in **g**. Any weight on a Lie algebra **g** vanishes on the derived algebra [**g**,**g**] and hence descends to a weight on the abelian Lie algebra **g**/[**g**,**g**]. Thus weights are primarily of interest for abelian Lie algebras, where they reduce to the simple notion of a generalized eigenvalue for space of commuting linear transformations.

If *G* is a Lie group or an algebraic group, then a multiplicative character θ: *G* → **F**^{×} induces a weight *χ* = dθ: **g** → **F** on its Lie algebra by differentiation. (For Lie groups, this is differentiation at the identity element of *G*, and the algebraic group case is an abstraction using the notion of a derivation.)

then it is called a *weight module;* this corresponds to there being a common eigenbasis (a basis of simultaneous eigenvectors) for all the represented elements of the algebra, i.e., to their being simultaneously diagonalizable matrices (see diagonalizable matrix).

The last point is the most difficult one; the representations may be constructed using Verma modules.