Coxeter number Created 2026-09-24 Updated 2026-09-24
The finite representation type of a quiver condition means there are only finitely many isomorphism classes of indecomposable finite-dimensional -modules. Equivalently, every finite-dimensional module is a direct sum of members of a finite list of indecomposables.
For the case, we give the reflection argument underlying the Gabriel theorem, rather than using its conclusion as the proof. Since the underlying graph is a tree, every orientation is acyclic. At a sink , write
for the sum of the incoming arrow maps. If an indecomposable is not the simple , then is surjective: a nonzero complementary subspace to its image at the sink would be a direct summand supported only at . The Bernstein–Gelfand–Ponomarev reflection functor reverses the arrows and replaces by , with reversed maps the component projections. The source reflection replaces that kernel by the cokernel of its inclusion into , recovering . The inclusion is injective, so the reflected representation has no direct summand at the new source. If it decomposed, applying the inverse would decompose . Thus reflection preserves indecomposability except that it annihilates .
On a dimension vector of a quiver representation, it acts by the integral simple reflection
Let . These reflections preserve the positive-definite quadratic form . Positivity can be checked without a classification theorem: label the graph by the chain and attach vertex to . The leading principal minors are , all positive.
Choose a topological ordering so arrows point from smaller to larger indices. Reflect successively at sinks . This restores the orientation after one full cycle. The transformation of dimension vectors is the Coxeter element . If has diagonal entries one and entry above the diagonal at an arrow, direct multiplication of the reflection matrices gives
Thus has no fixed vector. It is an integral isometry of a positive definite form, so it has finite order : the image of each lattice basis vector lies in a finite set of vectors of the same norm, giving only finitely many possible isometries. Since and is invertible,
If an indecomposable survived all reflection cycles, its dimension vectors would all be nonzero and componentwise nonnegative, contradicting their zero sum. Therefore it reaches a simple at one of the finitely many reflection steps and is then annihilated. Applying the inverse reflections uniquely reconstructs it from that simple. There are at most such stopping positions, proving
This supplies the requested finite-type proof sketch.
A simply-laced positive-definite Coxeter graph has no multiple edges and has positive-definite symmetric Cartan matrix, with diagonal entries and entry precisely across an edge. Its connected components are exactly the ADE classification
The graph underlying is . For simple roots with and , its roots are
There is one base for each Weyl chamber, hence six bases. The Weyl group is generated by the two root reflections with
so . Relative to a chosen base, the two Coxeter elements are and ; both have order three.
A representation of the quiver is one linear map . Choosing bases that put in rank normal form decomposes it into copies of
These are indecomposable and have dimension vectors , , and , the three positive roots of . More generally, Gabriel theorem says that for any orientation of a simply-laced positive-definite Dynkin graph, indecomposable quiver representations are in bijection with its positive roots. The finite ADE root system therefore gives finitely many indecomposables.
The Coxeter number is the order of a Coxeter element. In the stated families the values are
Here is the dihedral group of order , is the symmetric group, is the signed symmetric group, and is the even signed symmetric group.
Let be the matrix whose th column consists of the coordinates of in the basis . Define the upper-triangular matrix and lower-triangular matrix by
The first identity in part b says , so . The second says that the matrix of is . Since has diagonal entries one, , and therefore
Thus is the characteristic polynomial of the Coxeter element in its geometric representation.
At , the diagonal entries of are , while every off-diagonal entry is
Hence is exactly the Coxeter Gram matrix , and part c gives
For a Finite Coxeter group the Gram matrix is positive definite, and for a Hyperbolic Coxeter group it is nondegenerate with Lorentzian signature. In either case , so is not an eigenvalue of and the Coxeter element fixes no nonzero vector.
For an Affine Coxeter group, the Gram form has a nonzero radical. If , then for every , and every generating reflection satisfies
Their product therefore fixes . Thus every affine Coxeter element has a nonzero fixed vector.