For n=2n=2 and prime powers q≥3q\geq 3, P⁡Ω4+(q)\operatorname{P}\Omega_{4}^{+}(q) is the of Q(x,y)=∑i=12xiyiQ(x,y)=\sum_{i=1}^{2}x_i y_i on Fq4\mathbb F_q^{4}:

Ω=O⁡(Q)′,P⁡Ω4+(q)=Ω/(Ω∩{λI:λ∈Fq×}).\Omega=\operatorname O(Q)',\qquad \operatorname{P}\Omega_{4}^{+}(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⁡Ω4+(q)∣=q2(2−1)(q2−1)∏i=12−1(q2i−1)gcd⁡(4,q2−1).|\operatorname{P}\Omega_{4}^{+}(q)|=\frac{q^{2(2-1)}(q^{2}-1)\prod_{i=1}^{2-1}(q^{2i}-1)}{\gcd(4,q^{2}-1)}.

It is never simple: it is a direct product of two nontrivial copies of PSL(2,q).

Rank and form convention

The ambient quadratic-space dimension is 44, and the absolute rank is 22. 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.

Low-rank identification

P⁡Ω4+(q)≅PSL⁡2(q)×PSL⁡2(q)\operatorname{P}\Omega_4^+(q)\cong\operatorname{PSL}_2(q)\times\operatorname{PSL}_2(q) for q≥3q\geq3. This is the reducible root-system case D2=A1⊔A1D_2=A_1\sqcup A_1. The lower parameters are excluded here because the full orthogonal commutator subgroup can differ from the usual small Chevalley-group convention.

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.