In mathematics, the term Cartan matrix has three meanings. All of these are named after the French mathematician Élie Cartan. Amusingly, the Cartan matrices in the context of Lie algebras were first investigated by Wilhelm Killing, whereas the Killing form is due to Cartan.^{[citation needed]}

Lie algebras

Lie groups and Lie algebras
Classical groups General linear GL(n) Special linear SL(n) Orthogonal O(n) Special orthogonal SO(n) Unitary U(n) Special unitary SU(n) Symplectic Sp(n)
Simple Lie groups Classical An Bn Cn Dn Exceptional G2 F4 E6 E7 E8
Other Lie groups Circle Lorentz Poincaré Conformal group Diffeomorphism Loop Euclidean
Lie algebras Lie group–Lie algebra correspondence Exponential map Adjoint representation Killing form Index Simple Lie algebra Loop algebra Affine Lie algebra
Semisimple Lie algebra Dynkin diagrams Cartan subalgebra Root system Weyl group Real form Complexification Split Lie algebra Compact Lie algebra
Representation theory Lie group representation Lie algebra representation Representation theory of semisimple Lie algebras Representations of classical Lie groups Theorem of the highest weight Borel–Weil–Bott theorem
Lie groups in physics Particle physics and representation theory Lorentz group representations Poincaré group representations Galilean group representations
Scientists Sophus Lie Henri Poincaré Wilhelm Killing Élie Cartan Hermann Weyl Claude Chevalley Harish-Chandra Armand Borel
Glossary Table of Lie groups
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A (symmetrizable) generalized Cartan matrix is a square matrix ${\displaystyle A=(a_{ij})}$ with integer 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).

Classification

An ${\displaystyle n\times n}$ matrix A is decomposable if there exists a nonempty proper subset ${\displaystyle I\subset \{1,\dots ,n\))$ such that ${\displaystyle a_{ij}=0}$ whenever ${\displaystyle i\in I}$ and ${\displaystyle j\notin I}$. A is indecomposable if it is not decomposable.

Let A be an indecomposable generalized Cartan matrix. We say that A is of finite type if all of its principal minors are positive, that A is of affine type if its proper principal minors are positive and A has determinant 0, and that A is of indefinite type otherwise.

Finite type indecomposable matrices classify the finite dimensional simple Lie algebras (of types ${\displaystyle A_{n},B_{n},C_{n},D_{n},E_{6},E_{7},E_{8},F_{4},G_{2))$), while affine type indecomposable matrices classify the affine Lie algebras (say over some algebraically closed field of characteristic 0).

Determinants of the Cartan matrices of the simple Lie algebras

The determinants of the Cartan matrices of the simple Lie algebras are given in the following table (along with A₁=B₁=C₁, B₂=C₂, D₃=A₃, D₂=A₁A₁, E₅=D₅, E₄=A₄, and E₃=A₂A₁).^[2]

Another property of this determinant is that it is equal to the index of the associated root system, i.e. it is equal to ${\displaystyle |P/Q|}$ where P, Q denote the weight lattice and root lattice, respectively.

Representations of finite-dimensional algebras

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.

Cartan matrices in M-theory

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.