G2 manifold explained

G2

is one of the five exceptional simple Lie groups. It can be described as the automorphism group of the octonions, or equivalently, as a proper subgroup of special orthogonal group SO(7) that preserves a spinor in the eight-dimensional spinor representation or lastly as the subgroup of the general linear group GL(7) which preserves the non-degenerate 3-form

\phi

, the associative form. The Hodge dual,

\psi=*\phi

is then a parallel 4-form, the coassociative form. These forms are calibrations in the sense of Reese Harvey and H. Blaine Lawson,[1] and thus define special classes of 3- and 4-dimensional submanifolds.

Properties

All

G2

-manifold are 7-dimensional, Ricci-flat, orientable spin manifolds. In addition, any compact manifold with holonomy equal to

G2

has finite fundamental group, non-zero first Pontryagin class, and non-zero third and fourth Betti numbers.

History

The fact that

G2

might possibly be the holonomy group of certain Riemannian 7-manifolds was first suggested by the 1955 classification theorem of Marcel Berger, and this remained consistent with the simplified proof later given by Jim Simons in 1962. Although not a single example of such a manifold had yet been discovered, Edmond Bonan nonetheless made a useful contribution by showing that, if such a manifold did in fact exist, it would carry both a parallel 3-form and a parallel 4-form, and that it would necessarily be Ricci-flat.[2]

The first local examples of 7-manifolds with holonomy

G2

were finally constructed around 1984 by Robert Bryant, and his full proof of their existence appeared in the Annals in 1987.[3] Next, complete (but still noncompact) 7-manifolds with holonomy

G2

were constructed by Bryant and Simon Salamon in 1989.[4] The first compact 7-manifolds with holonomy

G2

were constructed by Dominic Joyce in 1994. Compact

G2

manifolds are therefore sometimes known as "Joyce manifolds", especially in the physics literature.[5] In 2013, it was shown by M. Firat Arikan, Hyunjoo Cho, and Sema Salur that any manifold with a spin structure, and, hence, a

G2

-structure, admits a compatible almost contact metric structure, and an explicit compatible almost contact structure was constructed for manifolds with

G2

-structure.[6] In the same paper, it was shown that certain classes of

G2

-manifolds admit a contact structure.

In 2015, a new construction of compact

G2

manifolds, due to Alessio Corti, Mark Haskins, Johannes Nordstrőm, and Tommaso Pacini, combined a gluing idea suggested by Simon Donaldson with new algebro-geometric and analytic techniques for constructing Calabi–Yau manifolds with cylindrical ends, resulting in tens of thousands of diffeomorphism types of new examples.[7]

Connections to physics

These manifolds are important in string theory. They break the original supersymmetry to 1/8 of the original amount. For example, M-theory compactified on a

G2

manifold leads to a realistic four-dimensional (11-7=4) theory with N=1 supersymmetry. The resulting low energy effective supergravity contains a single supergravity supermultiplet, a number of chiral supermultiplets equal to the third Betti number of the

G2

manifold and a number of U(1) vector supermultiplets equal to the second Betti number. Recently it was shown that almost contact structures (constructed by Sema Salur et al.) play an important role in

G2

geometry".

See also

Further reading

Notes and References

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  7. Corti. Alessio. Alessio Corti. Haskins. Mark. Nordström. Johannes. Pacini. Tommaso . 2015. -manifolds and associative submanifolds via semi-Fano 3-folds. . 164. 10. 1971–2092. 10.1215/00127094-3120743. 119141666.