The Conway group Co2\mathrm{Co}_2 is the

Co2={g∈O(Λ):g(v)=v}\mathrm{Co}_2=\{g\in O(\Lambda):g(v)=v\}

of a vector vv of squared length ⟨v,v⟩=4\langle v,v\rangle=4 in the Λ\Lambda. Here O(Λ)O(\Lambda) is the group of real linear isometries preserving the lattice. These vectors form one orbit, so all choices give conjugate stabilizers.

Order and simplicity

This is a nonabelian , with

∣Co2∣=42 305 421 312 000=218⋅36⋅53⋅7⋅11⋅23.|\mathrm{Co}_2|=42\,305\,421\,312\,000 =2^{18}\cdot3^6\cdot5^3\cdot7\cdot11\cdot23.
A finite matrix model

The two matrices in Co2G1-f2r22B0.m1 and Co2G1-f2r22B0.m2 generate a faithful copy of this group in , the group of over the with two elements. The representation dimension 2222 is not the dimension 2424 of the original lattice.

Subgroup relationships

Projection to is injective on this vector stabilizer, since −I-I does not fix vv. Its image is a maximal subgroup of index 98 28098\,280.

The is isomorphic to a maximal subgroup of Co2\mathrm{Co}_2, of index 47 10447\,104.

References
  1. Robert A. Wilson, Finite Simple Groups, Chapter 5 notes, §5.3.4 and equation (5.16), for vector transitivity and the stabilizer.
  2. ATLAS: Co2, order and maximal-subgroup tables; ATLAS: Co1, Co2 maximal-subgroup row.
  3. Representation Co2G1-f2r22B0, “About this representation” and “Checks applied”; exact MeatAxe data generator a and generator b.