For prime powers qq and fixed matrix size 44, PSU⁡4(q)\operatorname{PSU}_{4}(q) is the defined by

PSU⁡4(q)=SU⁡4(q)/{λI:λq+1=1, λ4=1},SU⁡4(q)={A∈M4(Fq2):(A(q))TA=I, det⁡A=1}.\operatorname{PSU}_{4}(q)=\operatorname{SU}_{4}(q)/\{\lambda I:\lambda^{q+1}=1,\ \lambda^{4}=1\}, \quad \operatorname{SU}_{4}(q)=\{A\in M_{4}(\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⁡4(q)∣=q6(q2−1)(q3+1)(q4−1)gcd⁡(4,q+1).|\operatorname{PSU}_{4}(q)|=\frac{q^{6}(q^{2}-1)(q^{3}+1)(q^{4}-1)}{\gcd(4,q+1)}.

It is simple for every prime power q.

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.

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.