For n=2n=2 and q=3q=3, PSp⁡4(3)\operatorname{PSp}_{4}(3) is the

PSp⁡4(3)=Sp⁡4(3)/{λI:λ∈F3×,λ2=1},Sp⁡4(3)={A∈GL⁡4(F3):ATJA=J},\operatorname{PSp}_{4}(3)=\operatorname{Sp}_{4}(3)/\{\lambda I:\lambda\in\mathbb F_{3}^\times,\lambda^2=1\}, \quad \operatorname{Sp}_{4}(3)=\{A\in\operatorname{GL}_{4}(\mathbb F_{3}):A^{\mathsf T}JA=J\},

where F3\mathbb F_{3} is the . The matrix J=(0I2−I20)J=\begin{pmatrix}0&I_{2}\\-I_{2}&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⁡4(3)∣=25920.|\operatorname{PSp}_{4}(3)|=25920.

It is a nonabelian . The exact order is 25,920.

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.

Small-group identification

There is an exceptional isomorphism PSp⁡4(3)≅PSU⁡4(2)\operatorname{PSp}_4(3)\cong\operatorname{PSU}_4(2).

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.
  2. Peter J. Cameron, Notes on Classical Groups, §§5.2–5.3, pp. 59–63; PSU(2,q), PSU(3,2), and the PSU(4,2) identification.