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 \chi_i, \chi_j are irreducible representations of G then there is an arrow from \chi_i to \chi_j if and only if \chi_j is a constituent of the tensor product V\otimes\chi_i. Then the weight nij of the arrow is the number of times this constituent appears in V \otimes\chi_i. For finite subgroups H of GL(2, C), the McKay graph of H is the McKay graph of the canonical representation of H.

If G has n irreducible characters, then the Cartan matrix cV of the representation V of dimension d is defined by  c_V = (d\delta_{ij} -n_{ij})_{ij} , where δ is the Kronecker delta. A result by Steinberg states that if g is a representative of a conjugacy class of G, then the vectors  ((\chi_i(g))_i are the eigenvectors of cV to the eigenvalues  d-\chi_V(g) , where  \chi_V 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  \chi be its character. Let \{\chi_1,\ldots,\chi_d\} be the irreducible representations of G. If

	V\otimes\chi_i = \sum_j n_{ij} \chi_j,

then define the McKay graph \Gamma_G of G as follow:

We can calculate the value of nij by considering the inner product. We have the following formula:

n_{ij} = \langle V\otimes\chi_i, \chi_j\rangle = \frac{1}{|G|}\sum_{g\in G} V(g)\chi_i(g)\overline{\chi_j(g)},

where \langle \cdot, \cdot \rangle denotes the inner product of the characters.

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 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 follow:

c_V = (d\delta_{ij} - n_{ij})_{ij},

where  \delta_{ij} is the Kronecker delta.

Some results

Examples

\chi_i\times\psi_j\quad 1\leq i \leq k,\,\, 1\leq j \leq l

are the irreducible representations of A\times B, where \chi_i\times\psi_j(a,b) = \chi_i(a)\psi_j(b), (a,b)\in A\times B. In this case, we have

\langle (c_A\times c_B)\otimes (\chi_i\times\psi_l), \chi_n\times\psi_p\rangle = \langle c_A\otimes \chi_k, \chi_n\rangle\cdot \langle c_B\otimes \psi_l, \psi_p\rangle.

Therefore, there is an arrow in the McKay graph of G between \chi_i\times\psi_j and \chi_k\times\psi_l if and only if there is an arrow in the McKay graph of A between \chi_i and \chi_k and there is an arrow in the McKay graph of B between \psi_j and \psi_l. 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 = \left( \begin{array}{cc}
i & 0 \\
0 & -i \end{array} \right) , 
V = \left( \begin{array}{cc}
0 & i \\
i & 0 \end{array} \right), 
U = \frac{1}{\sqrt{2}} \left( \begin{array}{cc}
\epsilon & \epsilon^3 \\
\epsilon & \epsilon^7 \end{array} \right),

where ε is a primitive eighth root of unity. Then, \overline{T} is generated by S, U, V. In fact, we have

\overline{T} = \{U^k, SU^k,VU^k,SVU^k | k = 0,\ldots, 5\}.

The conjugacy classes of \overline{T} are the following:

C_1 = \{U^0 = I\},
C_2 = \{U^3 = - I\},
C_3 = \{\pm S, \pm V, \pm SV\},
C_4 = \{U^2, SU^2, VU^2, SVU^2\},
C_5 = \{-U, SU, VU, SVU\},
C_6 = \{-U^2, -SU^2, -VU^2, -SVU^2\},
C_7 = \{U, -SU, -VU, -SVU\}.

The character table of \overline{T} is

Conjugacy Classes C_1 C_2 C_3 C_4 C_5 C_6 C_7
\chi_1 1 1 1 1 1 1 1
\chi_2 1 1 1 \omega \omega^2 \omega \omega^2
\chi_3 1 1 1 \omega^2 \omega \omega^2 \omega
\chi_4 3 3 -1 0 0 0 0
c 2 -2 0 -1 -1 1 1
\chi_5 2 -2 0 -\omega -\omega^2 \omega \omega^2
\chi_6 2 -2 0 -\omega^2 -\omega \omega^2 \omega

Here \omega = e^{2\pi i/3}. The canonical representation is represented by c. By using the inner product, we have that the McKay graph of \overline{T} is the extended Coxeter-Dynkin diagram of type \tilde{E}_6.

See also

References

This article is issued from Wikipedia - version of the Monday, June 29, 2015. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.