Omega groups
Ω(n,𝔽q) — written Ω(n,𝔽q) — is the index-2 subgroup of
SO(n,𝔽q) cut out by the spinor norm, and the last step down the
orthogonal chain
GO ⊇ SO ⊇ Ω
Like GO and SO it carries a Witt type in even dimension:
Ω+(2m,𝔽q) and Ω−(2m,𝔽q), with none in odd dimension.
- Order —
|Ω| = |GO| / 4over a field of odd order, and|GO| / 2over a field of even order, where the determinant is useless (it is identically1) and the Dickson invariant does the cutting instead. - Simplicity —
Ωitself need not be simple; its projective quotientPΩ = Ω / Z(Ω)is, apart from small exceptions.Z(Ω)is trivial or of order 2.
A naming caution
The ATLAS of Finite Groups
writes Onε(q) for the simple group
PΩε(n, q) — not for GO, and not for Ω. Three different
groups sit behind similar-looking symbols, so a name has to say which one it
means. Here Omega±(n, q) is the spinor kernel itself; where it differs from
its projective quotient, they differ by a center of order 2.
The exceptional isomorphisms
In dimension at most 6 every orthogonal group coincides with a member of another classical family — the classical exceptional isomorphisms:
Ω(3,𝔽q) | ≅ PSL(2,𝔽q) |
Ω(5,𝔽q) | ≅ PSp(4,𝔽q) |
Ω−(4,𝔽q) | ≅ PSL(2,𝔽q²) |
Ω+(4,𝔽q) | ≅ SL(2,𝔽q) ∘ SL(2,𝔽q) (a central product) |
Ω+(6,𝔽q) | ≅ SL(4,𝔽q) modulo its center |
Ω−(6,𝔽q) | ≅ SU(4,𝔽q) modulo its center |
So Ω(3,𝔽7) ≅ PSL(2,𝔽7) of order 168, Ω−(4,𝔽3) ≅ PSL(2,𝔽9) ≅ A₆, and
Ω+(6,𝔽2) ≅ A₈. In Lie-theoretic terms these are the coincidences
B₁ = A₁, B₂ = C₂, D₂ = A₁ × A₁, ²D₂ = ²A₁, D₃ = A₃ and ²D₃ = ²A₃.