nLab exceptional geometry

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Contents

Contents

Idea

The classification of Riemannian manifolds with special holonomy contains two “exceptional” cases: G₂-holonomy in dimension 7, and Spin(7)-holonomy in dimension 8. Their study is the topic of exceptional geometry.

Sometimes more generally, exceptional geometry is understood to study spaces controled by exceptional Lie groups in some way.


Properties

In terms of twisted Cohomotopy

coset space-structures on n-spheres:

standard:
S n1 diffSO(n)/SO(n1)S^{n-1} \simeq_{diff} SO(n)/SO(n-1)this Prop.
S 2n1 diffSU(n)/SU(n1)S^{2n-1} \simeq_{diff} SU(n)/SU(n-1)this Prop.
S 4n1 diffSp(n)/Sp(n1)S^{4n-1} \simeq_{diff} Sp(n)/Sp(n-1)this Prop.
exceptional:
S 7 diffSpin(7)/G 2S^7 \simeq_{diff} Spin(7)/G_2Spin(7)/G₂ is the 7-sphere
S 7 diffSpin(6)/SU(3)S^7 \simeq_{diff} Spin(6)/SU(3)since Spin(6) \simeq SU(4)
S 7 diffSpin(5)/SU(2)S^7 \simeq_{diff} Spin(5)/SU(2)since Sp(2) is Spin(5) and Sp(1) is SU(2), see Spin(5)/SU(2) is the 7-sphere
S 6 diffG 2/SU(3)S^6 \simeq_{diff} G_2/SU(3)G₂/SU(3) is the 6-sphere
S 15 diffSpin(9)/Spin(7)S^15 \simeq_{diff} Spin(9)/Spin(7)Spin(9)/Spin(7) is the 15-sphere

see also Spin(8)-subgroups and reductions

homotopy fibers of homotopy pullbacks of classifying spaces:

(from FSS 19, 3.4)

References

General

General discussion is in

Discussion of G₂ manifolds is in

  • Spiro Karigiannis, G 2G_2-manifolds – Exceptional structures in geometry arising from exceptional algebra (pdf)

In supergravity

Applications to U-duality-covariant formulations of 11d supergravity (exceptional field theory, see there for more)

For more along these lines see the references at exceptional generalized geometry.

As M-brane target space

Discusssion of M-brane sigma-models on exceptional geometry target spaces:

Last revised on September 17, 2024 at 10:22:52. See the history of this page for a list of all contributions to it.