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In differential geometry, a **quaternionic manifold** is a quaternionic analog of a complex manifold. The definition is more complicated and technical than the one for complex manifolds due in part to the noncommutativity of the quaternions and in part to the lack of a suitable calculus of holomorphic functions for quaternions. The most succinct definition uses the language of *G*-structures on a manifold. Specifically, a **quaternionic n-manifold** can be defined as a smooth manifold of real dimension 4

If we regard the quaternionic vector space as a right -module, we can identify the algebra of right -linear maps with the algebra of quaternionic matrices acting on *from the left*. The invertible right -linear maps then form a subgroup of . We can enhance this group with the group of nonzero quaternions acting by scalar multiplication on *from the right*. Since this scalar multiplication is -linear (but *not* -linear) we have another embedding of into . The group is then defined as the product of these subgroups in . Since the intersection of the subgroups and in is their mutual center (the group of scalar matrices with nonzero real coefficients), we have the isomorphism

An **almost quaternionic structure** on a smooth manifold is just a -structure on . Equivalently, it can be defined as a subbundle of the endomorphism bundle such that each fiber is isomorphic (as a real algebra) to the quaternion algebra . The subbundle is called the **almost quaternionic structure bundle**. A manifold equipped with an almost quaternionic structure is called an **almost quaternionic manifold**.

The quaternion structure bundle naturally admits a bundle metric coming from the quaternionic algebra structure, and, with this metric, splits into an orthogonal direct sum of vector bundles where is the trivial line bundle through the identity operator, and is a rank-3 vector bundle corresponding to the purely imaginary quaternions. Neither the bundles or are necessarily trivial.

The unit sphere bundle
inside corresponds to the pure unit imaginary quaternions. These are endomorphisms of the tangent spaces that square to −1. The bundle is called the **twistor space** of the manifold , and its properties are described in more detail below. Local sections of are (locally defined) almost complex structures. There exists a neighborhood of every point in an almost quaternionic manifold with an entire 2-sphere of almost complex structures defined on . One can always find such that

Note, however, that none of these operators may be extendable to all of . That is, the bundle may admit no *global* sections (e.g. this is the case with quaternionic projective space ). This is in marked contrast to the situation for complex manifolds, which always have a globally defined almost complex structure.

A **quaternionic structure** on a smooth manifold is an almost quaternionic structure which admits a torsion-free affine connection preserving . Such a connection is never unique, and is not considered to be part of the quaternionic structure. A **quaternionic manifold** is a smooth manifold together with a quaternionic structure on .

A **hypercomplex manifold** is a quaternionic manifold with a torsion-free -structure. The reduction of the structure group to is possible if and only if the almost quaternionic structure bundle is trivial (i.e. isomorphic to ). An almost hypercomplex structure corresponds to a global frame of , or, equivalently, triple of almost complex structures , and such that

A hypercomplex structure is an almost hypercomplex structure such that each of , and are integrable.

A **quaternionic Kähler manifold** is a quaternionic manifold with a torsion-free -structure.

A **hyperkähler manifold** is a quaternionic manifold with a torsion-free -structure. A hyperkähler manifold is simultaneously a hypercomplex manifold and a quaternionic Kähler manifold.

Given a quaternionic -manifold , the unit 2-sphere subbundle corresponding to the pure unit imaginary quaternions (or almost complex structures) is called the **twistor space** of . It turns out that, when , there exists a natural complex structure on such that the fibers of the projection are isomorphic to . When , the space admits a natural almost complex structure, but this structure is integrable only if the manifold is self-dual. It turns out that the quaternionic geometry on can be reconstructed entirely from holomorphic data on .

The twistor space theory gives a method of translating problems on quaternionic manifolds into problems on complex manifolds, which are much better understood, and amenable to methods from algebraic geometry. Unfortunately, the twistor space of a quaternionic manifold can be quite complicated, even for simple spaces like .

- Besse, Arthur L. (1987).
*Einstein Manifolds*. Berlin: Springer-Verlag. ISBN 3-540-15279-2. - Joyce, Dominic (2000).
*Compact Manifolds with Special Holonomy*. Oxford University Press. ISBN 0-19-850601-5.