Cartan matrix

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Scientists Sophus Lie Henri Poincaré Wilhelm Killing Élie Cartan Hermann Weyl Claude Chevalley Harish-Chandra Armand Borel
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A generalized Cartan matrix is a square matrix ${\displaystyle A=(a_{ij})}$ with integral entries such that

1. For diagonal entries, ${\displaystyle a_{ii}=2}$.
2. For non-diagonal entries, ${\displaystyle a_{ij}\leq 0}$.
3. ${\displaystyle a_{ij}=0}$ if and only if ${\displaystyle a_{ji}=0}$
4. ${\displaystyle A}$ can be written as ${\displaystyle DS}$, where ${\displaystyle D}$ is a diagonal matrix, and ${\displaystyle S}$ is a symmetric matrix.

For example, the Cartan matrix for G₂ can be decomposed as such:

${\displaystyle {\begin{bmatrix}2&-3\\-1&2\end{bmatrix}}={\begin{bmatrix}3&0\\0&1\end{bmatrix}}{\begin{bmatrix}{\frac {2}{3}}&-1\\-1&2\end{bmatrix}}.}$

The third condition is not independent but is really a consequence of the first and fourth conditions.

We can always choose a D with positive diagonal entries. In that case, if S in the above decomposition is positive definite, then A is said to be a Cartan matrix.

The Cartan matrix of a simple Lie algebra is the matrix whose elements are the scalar products

${\displaystyle a_{ji}=2{(r_{i},r_{j}) \over (r_{j},r_{j})}}$ [1]

(sometimes called the Cartan integers) where r_i are the simple roots of the algebra. The entries are integral from one of the properties of roots. The first condition follows from the definition, the second from the fact that for ${\displaystyle i\neq j,r_{j}-{2(r_{i},r_{j}) \over (r_{i},r_{i})}r_{i}}$ is a root which is a linear combination of the simple roots r_i and r_j with a positive coefficient for r_j and so, the coefficient for r_i has to be nonnegative. The third is true because orthogonality is a symmetric relation. And lastly, let ${\displaystyle D_{ij}={\delta _{ij} \over (r_{i},r_{i})}}$ and ${\displaystyle S_{ij}=2(r_{i},r_{j})}$. Because the simple roots span a Euclidean space, S is positive definite.

Conversely, given a generalized Cartan matrix, one can recover its corresponding Lie algebra. (See Kac–Moody algebra for more details).

In modular representation theory, and more generally in the theory of representations of finite-dimensional associative algebras A that are not semisimple, a Cartan matrix is defined by considering a (finite) set of principal indecomposable modules and writing composition series for them in terms of irreducible modules, yielding a matrix of integers counting the number of occurrences of an irreducible module.

In M-theory, one may consider a geometry with two-cycles which intersects with each other at a finite number of points, at the limit where the area of the two-cycles go to zero. At this limit, there appears a local symmetry group. The matrix of intersection numbers of a basis of the two-cycles is conjectured to be the Cartan matrix of the Lie algebra of this local symmetry group.[3]

This can be explained as follows. In M-theory one has solitons which are two-dimensional surfaces called membranes or 2-branes. A 2-brane has a tension and thus tends to shrink, but it may wrap around a two-cycles which prevents it from shrinking to zero.

One may compactify one dimension which is shared by all two-cycles and their intersecting points, and then take the limit where this dimension shrinks to zero, thus getting a dimensional reduction over this dimension. Then one gets type IIA string theory as a limit of M-theory, with 2-branes wrapping a two-cycles now described by an open string stretched between D-branes. There is a U(1) local symmetry group for each D-brane, resembling the degree of freedom of moving it without changing its orientation. The limit where the two-cycles have zero area is the limit where these D-branes are on top of each other, so that one gets an enhanced local symmetry group.

Now, an open string stretched between two D-branes represents a Lie algebra generator, and the commutator of two such generator is a third one, represented by an open string which one gets by gluing together the edges of two open strings. The latter relation between different open strings is dependent on the way 2-branes may intersect in the original M-theory, i.e. in the intersection numbers of two-cycles. Thus the Lie algebra depends entirely on these intersection numbers. The precise relation to the Cartan matrix is because the latter describes the commutators of the simple roots, which are related to the two-cycles in the basis that is chosen.

Generators in the Cartan subalgebra are represented by open strings which are stretched between a D-brane and itself.

• Dynkin diagram
• Exceptional Jordan algebra
• Fundamental representation
• Killing form
• Simple Lie group

• Fulton, William; Harris, Joe (1991). Representation theory: A first course. Graduate Texts in Mathematics. 129. Springer-Verlag. p. 334. ISBN 0-387-97495-4.
• Humphreys, James E. (1972). Introduction to Lie algebras and representation theory. Graduate Texts in Mathematics. 9. Springer-Verlag. pp. 55–56. doi:10.1007/978-1-4612-6398-2. ISBN 0-387-90052-7.
• Kac, Victor G. (1990). Infinite Dimensional Lie Algebras (3rd ed.). Cambridge University Press. ISBN 978-0-521-46693-6..

• "Cartan matrix", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
• Weisstein, Eric W. "Cartan matrix". MathWorld.