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The isotypic component of
weight In science and engineering, the weight of an object is the force acting on the object due to gravity. Some standard textbooks define weight as a Euclidean vector, vector quantity, the gravitational force acting on the object. Others define weigh ...
\lambda of a Lie algebra module is the sum of all submodules which are isomorphic to the highest weight module with weight \lambda.


Definition

* A finite-dimensional
module Module, modular and modularity may refer to the concept of modularity. They may also refer to: Computing and engineering * Modular design, the engineering discipline of designing complex devices using separately designed sub-components * Modul ...
V of a
reductive Lie algebra In mathematics, a Lie algebra is reductive if its adjoint representation is completely reducible, whence the name. More concretely, a Lie algebra is reductive if it is a direct sum of a semisimple Lie algebra and an abelian Lie algebra: \mathfr ...
\mathfrak (or of the corresponding
Lie group In mathematics, a Lie group (pronounced ) is a group that is also a differentiable manifold. A manifold is a space that locally resembles Euclidean space, whereas groups define the abstract concept of a binary operation along with the additio ...
) can be decomposed into
irreducible In philosophy, systems theory, science, and art, emergence occurs when an entity is observed to have properties its parts do not have on their own, properties or behaviors that emerge only when the parts interact in a wider whole. Emergence ...
submodules : V = \oplus_^N V_i . * Each finite-dimensional irreducible representation of \mathfrak is uniquely identified (up to isomorphism) by its
highest weight 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 multiplic ...
:\forall i \in \ \exists \lambda \in P(\mathfrak) : V_i \simeq M_\lambda, where M_\lambda denotes the
highest weight module 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 multipli ...
with highest weight \lambda. * In the decomposition of V , a certain isomorphism class might appear more than once, hence : V \simeq \oplus_ ( \oplus_^ M_) . This defines the isotypic component of weight \lambda of V: \lambda(V) := \oplus_^ V_i \simeq \mathbb^ \otimes M_ where d_\lambda is maximal.


See also

*
Lie algebra representation In the mathematical field of representation theory, a Lie algebra representation or representation of a Lie algebra is a way of writing a Lie algebra as a set of matrices (or endomorphisms of a vector space) in such a way that the Lie bracket is g ...
*
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 multiplic ...
* Semisimple representation#Isotypic decomposition


References

* * {{Cite journal , doi = 10.1007/s00220-005-1330-9 , last = Heinzner , first = P. , author2=A. Huckleberry , author3=M. R Zirnbauer , title = Symmetry classes of disordered fermions , journal = Communications in Mathematical Physics , volume = 257 , issue = 3 , pages = 725–771 , year = 2005 , arxiv = math-ph/0411040 , bibcode = 2005CMaPh.257..725H Representation theory of Lie algebras