For n=1n=1 and prime powers qq, PSp⁡2(q)\operatorname{PSp}_{2}(q) is the

PSp⁡2(q)=Sp⁡2(q)/{λI:λ∈Fq×,λ2=1},Sp⁡2(q)={A∈GL⁡2(Fq):ATJA=J},\operatorname{PSp}_{2}(q)=\operatorname{Sp}_{2}(q)/\{\lambda I:\lambda\in\mathbb F_{q}^\times,\lambda^2=1\}, \quad \operatorname{Sp}_{2}(q)=\{A\in\operatorname{GL}_{2}(\mathbb F_{q}):A^{\mathsf T}JA=J\},

where Fq\mathbb F_{q} is the . The matrix J=(0I1−I10)J=\begin{pmatrix}0&I_{1}\\-I_{1}&0\end{pmatrix} gives the B(v,w)=vTJwB(v,w)=v^{\mathsf T}Jw, which is alternating, meaning B(v,v)=0B(v,v)=0 for every vv, and nondegenerate. Multiplication is multiplication of scalar cosets.

Order and simplicity

Its order is

∣PSp⁡2(q)∣=q(q2−1)gcd⁡(2,q−1).|\operatorname{PSp}_{2}(q)|=\frac{q(q^{2}-1)}{\gcd(2,q-1)}.

It is simple exactly when q ≥ 4.

Parameter convention

Type CnC_n has rank nn and matrix dimension 2n2n. The center has size gcd⁡(2,q−1)\gcd(2,q-1), so the projective quotient does nothing when qq is even. Alternating means B(v,v)=0B(v,v)=0, also in characteristic two.

In dimension two, preservation of JJ is equivalent to determinant one, so PSp⁡2(q)≅PSL⁡2(q)\operatorname{PSp}_2(q)\cong\operatorname{PSL}_2(q). See .

References
  1. Peter J. Cameron, Notes on Classical Groups, §§4.2–4.3, pp. 49–54; the Sp(4,2) action on six quadratic forms, p. 51.