Kac–Moody algebra
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In mathematics, a Kac–Moody algebra is a Lie algebra, usually infinite-dimensional, that can be defined through a generalized root system. Kac–Moody algebras have applications throughout mathematics and mathematical physics. They are named for the Russian-American mathematician Victor Kac and the Canadian mathematician Robert Moody.
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[edit] Definition
A Kac–Moody algebra is specified by the following pieces of data:
- An n by n generalized Cartan matrix C = (cij) of rank r.
- A vector space over the complex numbers of dimension 2n − r.
- A set of n linearly independent elements of and a set of n linearly independent elements of the dual space, such that . The are known as coroots, while the are known as roots.
The Kac–Moody algebra is defined by generators ei and fi and the elements of and relations
- for
- , for
- , for
- for
- for applications of
- for applications of
Where is used as an alternate notation for the Commutator.
A real (possibly infinite-dimensional) Lie algebra is also considered a Kac–Moody algebra if its complexification is a Kac–Moody algebra.
[edit] Interpretation
is a Cartan subalgebra of the Kac–Moody algebra.
If g is an element of the Kac–Moody algebra such that
where ω is an element of , then g is said to have weight ω. The Kac–Moody algebra can be diagonalized into weight eigenvectors. The Cartan subalgebra h has weight zero, ei has weight α*i and fi has weight −α*i. If the Lie bracket of two weight eigenvectors is nonzero, then its weight is the sum of their weights. The condition for simply means the α*i are simple roots.
[edit] Types of Kac–Moody algebras
C can be decomposed as DS where D is a positive diagonal matrix and S is a symmetric matrix.
- finite-dimensional simple Lie algebras (S is positive definite)
- affine (S is positive semidefinite)
- hyperbolic (S is indefinite)
S can never be negative definite or negative semidefinite because its diagonal entries are positive.