Loop algebra

In mathematics, loop algebras are certain types of Lie algebras, of particular interest in theoretical physics.

In mathematics, loop algebras are certain types of Lie algebras, of particular interest in theoretical physics. ==Definition== For a Lie algebra \mathfrak{g} over a field K , if K[t,t^{-1}] is the space of Laurent polynomials, then L\mathfrak{g} := \mathfrak{g}\otimes K[t,t^{-1}], with the inherited bracket [X\otimes t^m, Y\otimes t^n] = [X,Y]\otimes t^{m+n}. \mathfrak{g}\otimes C^\infty(S^1), is an infinite-dimensional Lie algebra with the Lie bracket given by [g_1\otimes f_1,g_2 \otimes f_2]=[g_1,g_2]\otimes f_1 f_2. Here and are elements of \mathfrak{g} and and are elements of . This isn't precisely what would correspond to the direct product of infinitely many copies of \mathfrak{g} , one for each point in , because of the smoothness restriction. Instead, it can be thought of in terms of smooth map from to \mathfrak{g} ; a smooth parametrized loop in \mathfrak{g} , in other words. This is why it is called the loop algebra. Defining \mathfrak{g}_i to be the linear subspace \mathfrak{g}_i = \mathfrak{g}\otimes t^i the bracket restricts to a product [\cdot\, , \, \cdot]: \mathfrak{g}_i \times \mathfrak{g}_j \rightarrow \mathfrak{g}_{i+j}, hence giving the loop algebra a \mathbb{Z} -graded Lie algebra structure. In particular, the bracket restricts to the 'zero-mode' subalgebra \mathfrak{g}_0 \cong \mathfrak{g} . d: L\mathfrak{g} \rightarrow L\mathfrak{g} d(X\otimes t^n) = nX\otimes t^n and so can be thought of formally as d = t\frac{d}{dt} . It is required to define affine Lie algebras, which are used in physics, particularly conformal field theory. ==Loop group== Similarly, a set of all smooth maps from to a Lie group forms an infinite-dimensional Lie group (Lie group in the sense we can define functional derivatives over it) called the loop group. The Lie algebra of a loop group is the corresponding loop algebra. ==Affine Lie algebras as central extension of loop algebras== If \mathfrak{g} is a semisimple Lie algebra, then a nontrivial central extension of its loop algebra L\mathfrak g gives rise to an affine Lie algebra. Furthermore, this central extension is unique. The central extension is given by adjoining a central element \hat k , that is, for all X\otimes t^n \in L\mathfrak{g} , [\hat k, X\otimes t^n] = 0, and modifying the bracket on the loop algebra to [X\otimes t^m, Y\otimes t^n] = [X,Y] \otimes t^{m + n} + mB(X,Y) \delta_{m+n,0} \hat k, where B(\cdot, \cdot) is the Killing form. The central extension is, as a vector space, L\mathfrak{g} \oplus \mathbb{C}\hat k (in its usual definition, as more generally, \mathbb{C} can be taken to be an arbitrary field). Using the language of Lie algebra cohomology, the central extension can be described using a 2-cocycle on the loop algebra. This is the map \varphi: L\mathfrak g \times L\mathfrak g \rightarrow \mathbb{C} satisfying \varphi(X\otimes t^m, Y\otimes t^n) = mB(X,Y)\delta_{m+n,0}. Then the extra term added to the bracket is \varphi(X\otimes t^m, Y\otimes t^n)\hat k. ===Affine Lie algebra=== In physics, the central extension L\mathfrak g \oplus \mathbb C \hat k is sometimes referred to as the affine Lie algebra. In mathematics, this is insufficient, and the full affine Lie algebra is the vector space \hat \mathfrak{g} = L\mathfrak{g} \oplus \mathbb C \hat k \oplus \mathbb C d where d is the derivation defined above. On this space, the Killing form can be extended to a non-degenerate form, and so allows a root system analysis of the affine Lie algebra. ==References==

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