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A root system is a finite set Φ\Phi of nonzero vectors (called roots) in a Euclidean space EE satisfying the following conditions.

  • The roots span EE.
  • For αΦ\alpha \in \Phi, the only scalar multiples of α\alpha in EE are ±α\pm \alpha.
  • For α,βΦ\alpha, \beta \in \Phi, the quantity 2αβαα2 \frac{\alpha \cdot \beta}{\alpha \cdot \alpha} is an integer.
  • For α,βΦ\alpha,\beta \in \Phi, we have β2αβαααΦ\beta - 2 \frac{\alpha \cdot \beta}{\alpha \cdot \alpha} \alpha \in \Phi. That is, Φ\Phi is stable under the reflection through the hyperplane perpendicular to α\alpha.

The lattice generated by Φ\Phi is a root lattice.

The product of two root systems is again a root system. Root systems which are irreducible for this product are classified by Dynkin diagrams, which have standard names (where the subscript is always the dimension of the lattice): An(n1),Bn(n2),Cn(n3),Dn(n4),E6,E7,E8,F4,G2. A_n \,(n \geq 1), \,B_n \,(n \geq 2), \,C_n\, (n \geq 3), \,D_n \,(n \geq 4), \,E_6,\, E_7, \,E_8, \,F_4,\, G_2. Some small indices are omitted due to exceptional equalities: B1=A1,C2=B2,D3=A3. B_1 = A_1, \,C_2 = B_2, \,D_3 = A_3. In addition, in some cases multiple root systems generate the same lattice. The names used for root lattices are: An(n1),Dn(n4),E6,E7,E8. A_n \,(n \geq 1), \,D_n \,(n \geq 4), \,E_6, \,E_7, \,E_8. For any root system, the reflections in the hyperplanes orthogonal to the roots generate a finite group, called the Weyl group. The Weyl group is a subgroup of the automorphism group of the root lattice.

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  • Review status: beta
  • Last edited by Kiran S. Kedlaya on 2018-06-26 12:47:50
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