PSU⁡3(3)\operatorname{PSU}_{3}(3) is the following , with n=3n=3 and q=3q=3:

PSU⁡3(3)=SU⁡3(3)/{λI:λ3+1=1, λ3=1},SU⁡3(3)={A∈M3(F32):(A(3))TA=I, det⁡A=1}.\operatorname{PSU}_{3}(3)=\operatorname{SU}_{3}(3)/\{\lambda I:\lambda^{3+1}=1,\ \lambda^{3}=1\}, \quad \operatorname{SU}_{3}(3)=\{A\in M_{3}(\mathbb F_{3^2}): (A^{(3)})^{\mathsf T}A=I,\ \det A=1\}.

Here A(3)A^{(3)} is entrywise 33-th power. The has 323^2 elements; its involution has of size 33. The scalar λ\lambda belongs to F32×\mathbb F_{3^2}^\times; multiplication is multiplication of scalar cosets.

Order and simplicity

Its order is

∣PSU⁡3(3)∣=6048.|\operatorname{PSU}_{3}(3)|=6048.

It is a nonabelian . The exact order is 6,048.

Parameter convention

The parameter qq is the size of the fixed field, while matrices have entries in Fq2\mathbb F_{q^2}. The Hermitian form is h(v,w)=∑iviqwih(v,w)=\sum_i v_i^q w_i. All nondegenerate Hermitian forms of this dimension over the finite field give isomorphic groups. Type 2An−1{}^2A_{n-1} has absolute rank n−1n-1; it is not a unitary group over the real or complex numbers.

Small-group identification

This group is isomorphic to the index-two G2(2)′G_2(2)'.

References
  1. 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.
  2. Robert A. Wilson, Classical groups (lecture notes), §3.1.7, pp. 5–6; §§3.2–3.4, pp. 7–17.
  3. ATLAS of Finite Group Representations: U3(3) and G2(2) derived group, Heading and Standard generators: U3(3) = G2(2)′ has order 6048; U3(3):2 = G2(2).