A -structure on a manifold of dimension 7 is a choice of reduction of the structure group of the tangent bundle along the inclusion of G2 into .
Given that is the subgroup of the general linear group on the Cartesian space which preserves the associative 3-form on , a structre is a higher analog of an almost symplectic structure under lifting from symplectic geometry to 2-plectic geometry (Ibort).
A -manifold is a manifold equipped with an “integrable” or “parallel” -structure. This is equivalently a Riemannian manifold of dimension 7 with special holonomy group being the exceptional Lie group G2.
-manifolds may be understood as 7-dimensional analogs of real 6-dimensional Calabi-Yau manifolds.
For a smooth manifold of dimension a -structure on is a choice of differential 3-form such that there is an atlas over which this 3-form locally identifies with the associative 3-form on the Cartesian space .
Equivalently, this is a choice of reduction of the structure group of the tangent bundle along the inclusion
A -structure in particular implies an orthogonal structure, hence a Riemannian metric.
A manifold equipped with a -structure , def. 1, is called a -manifold if is “parallel” or “integrable” in that
(where is the de Rham differential and is the Hodge star operator of the canonical Riemannian metric of remark 1).
For instance (Joyce, p. 4).
The holonomy of the Levi-Civita connection on a -manifold is contained in .
There is a useful weakened notion of -holonomy.
A 7-dimensional manifold is said to be of weak -holonomy if it carries a 3-form with the relation of def. 2 generalized to
and hence
for . For this reduces to strict -holonomy, by 2.
(See for instance (Bilal-Derendinger-Sfetsos).)
A 7-manifold admits a -structure, def. 1, precisely if it admits a spin structure.
The canonical Riemannian metric manifold is Ricci flat?. More generally a manifold of weak -holonomy, def. 3, with weakness parameter is an Einstein manifold with cosmological constant .
In string phenomenology models obtained from compactification of 11-dimensional supergravity/M-theory on -manifolds (see for instance Duff) can have attractive phenomenological properties, see for instance the G2-MSSM.
classification of special holonomy manifolds by Berger's theorem:
Compact -manifolds were first found in
Surveys include
Spiro Karigiannis, What is… a -manifold (pdf)
Spiro Karigiannis, -manifolds – Exceptional structures in geometry arising from exceptional algebra (pdf)
The relation to multisymplectic geometry/2-plectic geometry is mentioned explicitly in
(but beware of some mistakes in that article…)
For more see the references at exceptional geometry.
The following references discuss the role of -manifolds in M-theory on G2-manifolds:
A survey of the corresponding string phenomenology for M-theory on G2-manifolds (see there for more) is in
Weak -holonomy is discussed in