Definition

For n1n\geq1, let the Sp(n)\operatorname{Sp}(n) act on Hn\mathbb H^n from the left and let its unit-quaternion subgroup Sp(1)\operatorname{Sp}(1) act from the right. The homomorphism

Sp(n)×Sp(1)SO(4n),(A,q)(vAvq1)\operatorname{Sp}(n)\times\operatorname{Sp}(1)\longrightarrow\operatorname{SO}(4n), \qquad (A,q)\longmapsto\bigl(v\mapsto Avq^{-1}\bigr)

has kernel {(I,1),(I,1)}\{(I,1),(-I,-1)\}. Its image is the group Sp(n)Sp(1)\operatorname{Sp}(n)\operatorname{Sp}(1). Hence

Sp(n)Sp(1)(Sp(n)×Sp(1))/{±(I,1)}.\operatorname{Sp}(n)\operatorname{Sp}(1) \cong \bigl(\operatorname{Sp}(n)\times\operatorname{Sp}(1)\bigr)/\{\pm(I,1)\}.

It is a compact connected of SO(4n)\operatorname{SO}(4n), not the direct product denoted by simply placing the two factors side by side.

Action on quaternionic structures

The left Sp(n)\operatorname{Sp}(n)-factor commutes with right quaternionic multiplication. The right Sp(1)\operatorname{Sp}(1)-factor conjugates the three-dimensional space ImH\operatorname{Im}\mathbb H of imaginary units, inducing the standard rotation action through Sp(1)/{±1}SO(3)\operatorname{Sp}(1)/\{\pm1\}\cong\operatorname{SO}(3). Thus the quotient preserves the rank-three family of complex structures while generally rotating its local basis I,J,KI,J,K. This is why the group, rather than Sp(n)\operatorname{Sp}(n) alone, is natural in quaternionic Kähler geometry Besse, §14.G.

Low-rank case and dimensions

Its is sp(n)sp(1)\mathfrak{sp}(n)\oplus\mathfrak{sp}(1), because quotienting by a finite central subgroup does not change the Lie algebra. Therefore

dimSp(n)Sp(1)=n(2n+1)+3.\dim\operatorname{Sp}(n)\operatorname{Sp}(1)=n(2n+1)+3.

For n=1n=1, the action identifies Sp(1)Sp(1)\operatorname{Sp}(1)\operatorname{Sp}(1) with SO(4)\operatorname{SO}(4). In quaternionic Kähler geometry the holonomy condition is normally stated for n2n\geq2; real dimension four is treated separately.

Relation to geometric structures

A Riemannian 4n4n-manifold whose frame bundle reduces to this subgroup has an almost quaternionic Hermitian structure. If its Levi–Civita lies in Sp(n)Sp(1)\operatorname{Sp}(n)\operatorname{Sp}(1), it is quaternionic Kähler under the standard higher-dimensional convention. By contrast, holonomy contained in the smaller subgroup Sp(n)\operatorname{Sp}(n) is the hyperkähler condition. The two conditions should not be conflated Salamon, pp. 143–145.

Conventions and scope

Authors variously print the middle operation as adjacency, a centered dot, or an explicit quotient. None of these denotes a direct product in this context. The expression {±(I,1)}\{\pm(I,1)\} abbreviates the two diagonal central elements (I,1)(I,1) and (I,1)(-I,-1), not four independently chosen signs.

References
  1. Arthur L. Besse, Einstein Manifolds, Springer, 1987. DOI record. Relevant: §14.G on quaternionic Kähler manifolds and their holonomy group.
  2. Simon Salamon, “Quaternionic Kähler Manifolds,” Inventiones Mathematicae 67 (1982), 143–171. DOI record. Relevant: pp. 143–145 on the groups Sp(n)Sp(1)\operatorname{Sp}(n)\operatorname{Sp}(1) and GL(n,H)Sp(1)\operatorname{GL}(n,\mathbb H)\operatorname{Sp}(1).