PSU⁡4(2)\operatorname{PSU}_{4}(2) is the following , with n=4n=4 and q=2q=2:

PSU⁡4(2)=SU⁡4(2)/{λI:λ2+1=1, λ4=1},SU⁡4(2)={A∈M4(F22):(A(2))TA=I, det⁡A=1}.\operatorname{PSU}_{4}(2)=\operatorname{SU}_{4}(2)/\{\lambda I:\lambda^{2+1}=1,\ \lambda^{4}=1\}, \quad \operatorname{SU}_{4}(2)=\{A\in M_{4}(\mathbb F_{2^2}): (A^{(2)})^{\mathsf T}A=I,\ \det A=1\}.

Here A(2)A^{(2)} is entrywise 22-th power. The has 222^2 elements; its involution has of size 22. The scalar λ\lambda belongs to F22×\mathbb F_{2^2}^\times; multiplication is multiplication of scalar cosets.

Order and simplicity

Its order is

∣PSU⁡4(2)∣=25920.|\operatorname{PSU}_{4}(2)|=25920.

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

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

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

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.