For integers n≥4n\geq4 and prime powers q≥2q\geq 2, P⁡Ω2n−(q)\operatorname{P}\Omega_{2n}^{-}(q) is the of Q(x,y,z)=∑i=1n−1xiyi+zq+1Q(x,y,z)=\sum_{i=1}^{n-1}x_i y_i+z^{q+1}, with x,y∈Fqn−1x,y\in\mathbb F_q^{n-1} and z∈Fq2z\in\mathbb F_{q^2}:

Ω=O⁡(Q)′,P⁡Ω2n−(q)=Ω/(Ω∩{λI:λ∈Fq×}).\Omega=\operatorname O(Q)',\qquad \operatorname{P}\Omega_{2n}^{-}(q)=\Omega/(\Omega\cap\{\lambda I:\lambda\in\mathbb F_q^\times\}).

Here O⁡(Q)\operatorname O(Q) is the group of invertible preserving QQ, and its prime denotes the . Multiplication is multiplication of scalar cosets. The displayed , not merely its polar form, is part of the definition.

Order and simplicity

Its order is

∣P⁡Ω2n−(q)∣=qn(n−1)(qn+1)∏i=1n−1(q2i−1)gcd⁡(4,qn+1).|\operatorname{P}\Omega_{2n}^{-}(q)|=\frac{q^{n(n-1)}(q^{n}+1)\prod_{i=1}^{n-1}(q^{2i}-1)}{\gcd(4,q^{n}+1)}.

It is a nonabelian for every admitted parameter.

Rank and form convention

The ambient quadratic-space dimension is 2n2n, and the absolute rank is nn. This is type 2Dn{}^2D_{n}. The plus sign has Witt index nn; the minus sign has Witt index n−1n-1, because the norm plane is anisotropic. The order denominator is gcd⁡(4,qn−1)\gcd(4,q^n-1) in plus type and gcd⁡(4,qn+1)\gcd(4,q^n+1) in minus type. There is no additional irreducible D1D_1 family; the ranks two and three have the separate low-rank descriptions.

References
  1. Peter J. Cameron, Notes on Classical Groups, §6, pp. 64–74, especially Theorems 6.3 and 6.6; §7 introduction, p. 75.
  2. Robert A. Wilson, Classical groups (lecture notes), §3.1.7, pp. 5–6; §§3.2–3.4, pp. 7–17.