McKay graph


Affine (extended) Dynkin diagrams

In mathematics, the McKay graph of a finite-dimensional representation V of a finite group G is a weighted quiver encoding the structure of the representation theory of G. Each node represents an irreducible representation of G. If χ i, χ j are irreducible representations of G, then there is an arrow from χ i to χ j if and only if χ j is a constituent of the tensor product V⊗χi. Then the weight nij of the arrow is the number of times this constituent appears in V⊗χi. For finite subgroups H of ⁠GL(2,ℂ),⁠ the McKay graph of H is the McKay graph of the defining 2-dimensional representation of H.

If G has n irreducible characters, then the Cartan matrix cV of the representation V of dimension d is defined by cV=(dδij−nij)ij, where δ is the Kronecker delta. A result by Robert Steinberg states that if g is a representative of a conjugacy class of G, then the vectors ((χi(g))i are the eigenvectors of cV to the eigenvalues d−χV(g), where χV is the character of the representation V.

The McKay correspondence, named after John McKay, states that there is a one-to-one correspondence between the McKay graphs of the finite subgroups of ⁠SL(2,ℂ)⁠ and the extended Dynkin diagrams, which appear in the ADE classification of the simple Lie algebras.

Definition

Let G be a finite group, V be a representation of G and χ be its character. Let {χ1,…,χd} be the irreducible representations of G. If

V⊗χi=∑jnijχj,

then define the McKay graph ΓG of G, relative to V, as follows:

We can calculate the value of nij using inner product ⟨⋅,⋅⟩ on characters:

nij=⟨V⊗χi,χj⟩=1|G|∑g∈GV(g)χi(g)χj(g)‾.

The McKay graph of a finite subgroup of ⁠GL(2,ℂ)⁠ is defined to be the McKay graph of its canonical representation.

For finite subgroups of ⁠SL(2,ℂ),⁠ the canonical representation on ⁠ℂ2⁠ is self-dual, so nij=nji for all i, j. Thus, the McKay graph of finite subgroups of ⁠SL(2,ℂ)⁠ is undirected.

In fact, by the McKay correspondence, there is a one-to-one correspondence between the finite subgroups of ⁠SL(2,ℂ)⁠ and the extended Coxeter-Dynkin diagrams of type A-D-E.

We define the Cartan matrix cV of V as follows:

cV=(dδij−nij)ij,

where δij is the Kronecker delta.

Some results

Examples

χi×ψj1≤i≤k,1≤j≤ℓ
are the irreducible representations of A × B, where χi×ψj(a,b)=χi(a)ψj(b),(a,b)∈A×B. In this case, we have
⟨(cA×cB)⊗(χi×ψℓ),χn×ψp⟩=⟨cA⊗χk,χn⟩⋅⟨cB⊗ψℓ,ψp⟩.
Therefore, there is an arrow in the McKay graph of G between χi×ψj and χk×ψℓ if and only if there is an arrow in the McKay graph of A between χi, χk and there is an arrow in the McKay graph of B between ψ j, ψℓ. In this case, the weight on the arrow in the McKay graph of G is the product of the weights of the two corresponding arrows in the McKay graphs of A and B.
S=(i00−i),  V=(0ii0),  U=12(εε3εε7),
where ε is a primitive eighth root of unity. In fact, we have
T‾={Uk,SUk,VUk,SVUk∣k=0,…,5}.
The conjugacy classes of T‾ are:
C1={U0=I},
C2={U3=−I},
C3={±S,±V,±SV},
C4={U2,SU2,VU2,SVU2},
C5={−U,SU,VU,SVU},
C6={−U2,−SU2,−VU2,−SVU2},
C7={U,−SU,−VU,−SVU}.
The character table of T‾ is
Conjugacy ClassesC1C2C3C4C5C6C7
χ1 1 1 1 1 1 1 1
χ2 1 1 1 ω ω2 ω ω2
χ3 1 1 1 ω2 ω ω2 ω
χ4 3 3 −1 0 0 0 0
c 2 −2 0 −1 −1 1 1
χ5 2 −2 0 −ω −ω2 ω ω2
χ6 2 −2 0 −ω2 −ω ω2 ω
Here ω=e2πi/3. The canonical representation V is here denoted by c. Using the inner product, we find that the McKay graph of T‾ is the extended Coxeter–Dynkin diagram of type E~6.

See also

References

  1. ↑ Steinberg, Robert (1985), "Subgroups of SU2, Dynkin diagrams and affine Coxeter elements", Pacific Journal of Mathematics, 18: 587–598, doi:10.2140/pjm.1985.118.587
  2. ↑ McKay, John (1982), "Representations and Coxeter Graphs", "The Geometric Vein", Coxeter Festschrift, Berlin: Springer-Verlag

Further reading