For prime powers qq and fixed matrix size 22, PSU⁡2(q)\operatorname{PSU}_{2}(q) is the defined by

PSU⁡2(q)=SU⁡2(q)/{λI:λq+1=1, λ2=1},SU⁡2(q)={A∈M2(Fq2):(A(q))TA=I, det⁡A=1}.\operatorname{PSU}_{2}(q)=\operatorname{SU}_{2}(q)/\{\lambda I:\lambda^{q+1}=1,\ \lambda^{2}=1\}, \quad \operatorname{SU}_{2}(q)=\{A\in M_{2}(\mathbb F_{q^2}): (A^{(q)})^{\mathsf T}A=I,\ \det A=1\}.

Here A(q)A^{(q)} is entrywise qq-th power. The has q2q^2 elements; its involution has of size qq. The scalar λ\lambda belongs to Fq2×\mathbb F_{q^2}^\times; multiplication is multiplication of scalar cosets.

Order and simplicity

Its order is

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

It is simple exactly when q ≥ 4, since PSU(2,q) is isomorphic to PSL(2,q).

Parameter convention

The matrices have entries in Fq2\mathbb F_{q^2}, with involution x↦xqx\mapsto x^q, but this rank-one group is isomorphic to PSL⁡2(q)\operatorname{PSL}_2(q). The A1A_1 diagram has no nontrivial symmetry, so this does not define an additional twisted 2A1{}^2A_1 family.

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.