# G-structure on a manifold

(Redirected from G-structure)

In differential geometry, a G-structure on an n-manifold M, for a given structure group[1] G, is a G-subbundle of the tangent frame bundle FM (or GL(M)) of M.

The notion of G-structures includes various classical structures that can be defined on manifolds, which in some cases are tensor fields. For example, for the orthogonal group, an O(n)-structure defines a Riemannian metric, and for the special linear group an SL(n,R)-structure is the same as a volume form. For the trivial group, an {e}-structure consists of an absolute parallelism of the manifold.

In mathematics, in particular the theory of principal bundles, one can ask if a principal ${\displaystyle G}$-bundle over a group ${\displaystyle G}$ "comes from" a subgroup ${\displaystyle H}$ of ${\displaystyle G}$. This is called reduction of the structure group (to ${\displaystyle H}$).

Several structures on manifolds, such as a complex structure, a symplectic structure, or a Kähler structure, are G-structures with an additional integrability condition.

## Principal bundles and G-structures

Although the theory of principal bundles plays an important role in the study of G-structures, the two notions are different. A G-structure is a principal subbundle of the tangent frame bundle, but the fact that the G-structure bundle consists of tangent frames is regarded as part of the data. For example, consider two Riemannian metrics on Rn. The associated O(n)-structures are isomorphic if and only if the metrics are isometric. But, since Rn is contractible, the underlying O(n)-bundles are always going to be isomorphic as principal bundles because the only bundles over contractible spaces are trivial bundles.

This fundamental difference between the two theories can be captured by giving an additional piece of data on the underlying G-bundle of a G-structure: the solder form. The solder form is what ties the underlying principal bundle of the G-structure to the local geometry of the manifold itself by specifying a canonical isomorphism of the tangent bundle of M to an associated vector bundle. Although the solder form is not a connection form, it can sometimes be regarded as a precursor to one.

In detail, suppose that Q is the principal bundle of a G-structure. If Q is realized as a reduction of the frame bundle of M, then the solder form is given by the pullback of the tautological form of the frame bundle along the inclusion. Abstractly, if one regards Q as a principal bundle independently of its realization as a reduction of the frame bundle, then the solder form consists of a representation ρ of G on Rn and an isomorphism of bundles θ : TMQ ×ρ Rn.

## Integrability conditions

Several structures on manifolds, such as a complex structure, a symplectic structure, or a Kähler structure, are G-structures with an additional integrability condition. Without the corresponding integrability condition, the structure is instead called an "almost" structure, as in an almost complex structure, an almost symplectic structure, or an almost Kähler structure

Specifically, a symplectic manifold structure is a stronger concept than a G-structure for the symplectic group. A symplectic structure on a manifold is a two-form ω on M that is non-degenerate (which is an ${\displaystyle Sp}$-structure, or almost symplectic structure), together with the extra condition that dω = 0; this latter is called an integrability condition.

Similarly, foliations correspond to G-structures coming from block matrices, together with integrability conditions so that the Frobenius theorem applies.

## Isomorphism of G-structures

The set of diffeomorphisms of M that preserve a G-structure is called the automorphism group of that structure. For an O(n)-structure they are the group of isometries of the Riemannian metric and for an SL(n,R)-structure volume preserving maps.

Let P be a G-structure on a manifold M, and Q a G-structure on a manifold N. Then an isomorphism of the G-structures is a diffeomorphism f : MN such that the pushforward of linear frames f* : FMFN restricts to give a mapping of P into Q. (Note that it is sufficient that Q be contained within the image of f*.) The G-structures P and Q are locally isomorphic if M admits a covering by open sets U and a family of diffeomorphisms fU : Uf(U) ⊂ N such that fU induces an isomorphism of P|UQ|f(U).

An automorphism of a G-structure is an isomorphism of a G-structure P with itself. Automorphisms arise frequently[2] in the study of transformation groups of geometric structures, since many of the important geometric structures on a manifold can be realized as G-structures.

A flat G-structure is a G-structure P having a global section (V1,...,Vn) consisting of commuting vector fields. A G-structure is integrable (or locally flat) if it is locally isomorphic to a flat G-structure.

A wide class of equivalence problems can be formulated in the language of G-structures. For example, a pair of Riemannian manifolds are (locally) equivalent if and only if their bundles of orthonormal frames are (locally) isomorphic G-structures. In this view, the general procedure for solving an equivalence problem is to construct a system of invariants for the G-structure which are then sufficient to determine whether a pair of G-structures are locally isomorphic or not.

## Connections on G-structures

Let Q be a G-structure on M. A principal connection on the principal bundle Q induces a connection on any associated vector bundle: in particular on the tangent bundle. A linear connection ∇ on TM arising in this way is said to be compatible with Q. Connections compatible with Q are also called adapted connections.

Concretely speaking, adapted connections can be understood in terms of a moving frame.[3] Suppose that Vi is a basis of local sections of TM (i.e., a frame on M) which defines a section of Q. Any connection ∇ determines a system of basis-dependent 1-forms ω via

X Vi = ωij(X)Vj

where, as a matrix of 1-forms, ω ∈ Ω1(M)⊗gl(n). An adapted connection is one for which ω takes its values in the Lie algebra g of G.

### Torsion of a G-structure

Associated to any G-structure is a notion of torsion, related to the torsion of a connection. Note that a given G-structure may admit many different compatible connections which in turn can have different torsions, but in spite of this it is possible to give an independent notion of torsion of the G-structure as follows.[4]

The difference of two adapted connections is a 1-form on M with values in the adjoint bundle AdQ. That is to say, the space AQ of adapted connections is an affine space for Ω1(AdQ).

The torsion of an adapted connection defines a map

${\displaystyle A^{Q}\to \Omega ^{2}(TM)\,}$

to 2-forms with coefficients in TM. This map is linear; its linearization

${\displaystyle \tau :\Omega ^{1}(\mathrm {Ad} _{Q})\to \Omega ^{2}(TM)\,}$

is called the algebraic torsion map. Given two adapted connections ∇ and ∇′, their torsion tensors T, T∇′ differ by τ(∇−∇′). Therefore, the image of T in coker(τ) is independent from the choice of ∇.

The image of T in coker(τ) for any adapted connection ∇ is called the torsion of the G-structure. A G-structure is said to be torsion-free if its torsion vanishes. This happens precisely when Q admits a torsion-free adapted connection.

### Example: Torsion for almost complex structures

An example of a G-structure is an almost complex structure, that is, a reduction of a structure group of an even-dimensional manifold to GL(n,C). Such a reduction is uniquely determined by a C-linear endomorphism J ∈ End(TM) such that J2 = −1. In this situation, the torsion can be computed explicitly as follows.

An easy dimension count shows that

${\displaystyle \Omega ^{2}(TM)=\Omega ^{2,0}(TM)\oplus \mathrm {im} (\tau )}$,

where Ω2,0(TM) is a space of forms B ∈ Ω2(TM) which satisfy

${\displaystyle B(JX,Y)=B(X,JY)=-JB(X,Y).\,}$

Therefore, the torsion of an almost complex structure can be considered as an element in Ω2,0(TM). It is easy to check that the torsion of an almost complex structure is equal to its Nijenhuis tensor.

## Higher order G-structures

Imposing integrability conditions on a particular G-structure (for instance, with the case of a symplectic form) can be dealt with via the process of prolongation. In such cases, the prolonged G-structure cannot be identified with a G-subbundle of the bundle of linear frames. In many cases, however, the prolongation is a principal bundle in its own right, and its structure group can be identified with a subgroup of a higher-order jet group. In which case, it is called a higher order G-structure [Kobayashi]. In general, Cartan's equivalence method applies to such cases.

## Reduction of the structure group

One can ask if a principal ${\displaystyle G}$-bundle over a group ${\displaystyle G}$ "comes from" a subgroup ${\displaystyle H}$ of ${\displaystyle G}$. This is called reduction of the structure group (to ${\displaystyle H}$), and makes sense for any map ${\displaystyle H\to G}$, which need not be an inclusion map (despite the terminology).

The notion of G-structures includes many other structures on manifolds, some of them being defined by tensor fields. For example, for the orthogonal group, an O(n)-structure defines a Riemannian metric, and for the special linear group an SL(n,R)-structure is the same as a volume form. For the trivial group, an {e}-structure consists of an absolute parallelism of the manifold.

Formally, given a G-bundle B and a map HG, a reduction of the structure group (from G to H) is an H-bundle ${\displaystyle B_{H}}$ and an isomorphism of the associated bundle ${\displaystyle B_{H}\times ^{H}G}$ to B.

Note that these do not always exist, nor if they exist are they unique.

As a concrete example, every even-dimensional real vector space is isomorphic to the underlying real space of a complex vector space: it admits a linear complex structure. A real vector bundle admits an almost complex structure if and only if it is isomorphic to the underlying real bundle of a complex vector bundle. This is then a reduction along the inclusion GL(n,C) → GL(2n,R)

In terms of transition maps, a G-bundle can be reduced if and only if the transition maps can be taken to have values in H. Note that the term reduction is misleading: it suggests that H is a subgroup of G, which is often the case, but need not be (for example for spin structures): it's properly called a lifting.

More abstractly, "G-bundles over X" is a functor[5] in G: given a map HG, one gets a map from H-bundles to G-bundles by inducing (as above). Reduction of the structure group of a G-bundle B is choosing an H-bundle whose image is B.

The inducing map from H-bundles to G-bundles is in general neither onto nor one-to-one, so the structure group cannot always be reduced, and when it can, this reduction need not be unique. For example, not every manifold is orientable, and those that are orientable admit exactly two orientations.

If H is a closed subgroup of G, then there is a natural one-to-one correspondence between reductions of a G-bundle B to H and global sections of the fiber bundle B/H obtained by quotienting B by the right action of H. Specifically, the fibration BB/H is a principal H-bundle over B/H. If σ : XB/H is a section, then the pullback bundle BH = σ−1B is a reduction of B.[6]

### Examples

Examples for vector bundles, particularly the tangent bundle of a manifold:

• ${\displaystyle GL^{+} is an orientation, and this is possible if and only if the bundle is orientable
• ${\displaystyle SL is a volume form; since ${\displaystyle SL\to GL^{+}}$ is a deformation retract, a volume form exists if and only if a bundle is orientable
• ${\displaystyle SL^{\pm } is a pseudo-volume form, and this is always possible
• ${\displaystyle O(n) is a Riemannian metric; as ${\displaystyle O(n)}$ is the maximal compact subgroup (so the inclusion is a deformation retract), this is always possible
• ${\displaystyle O(1,n-1) is a pseudo-Riemannian metric;[7] there is the topological obstruction to this reduction
• ${\displaystyle GL(n,\mathbf {C} ) is an almost complex structure
• ${\displaystyle GL(n,\mathbf {H} )\cdot Sp(1) (where ${\displaystyle GL(n,\mathbf {H} )}$ is the group of n×n invertible quaternionic matrices acting on ${\displaystyle \mathbf {H} ^{n}\cong \mathbf {R} ^{4n}}$ on the left and Sp(1)=Spin(3) the group of unit quaternions acting on ${\displaystyle \mathbf {H} ^{n}}$ from the right) is an almost quaternionic structure[8]
• ${\displaystyle {\mbox{Spin}}(n)\to {\mbox{SO}}(n)}$ (which is not an inclusion: it's a 2-fold covering space) is a spin structure.
• ${\displaystyle GL(k)\times GL(n-k) decomposes a vector bundle as a Whitney sum (direct sum) of sub-bundles of rank k and n − k.

### Integrability

Many geometric structures are stronger than G-structures; they are G-structures with an integrability condition. Thus such a structure requires a reduction of the structure group (and can be obstructed, as below), but this is not sufficient. Examples include complex structure, symplectic structure (as opposed to almost complex structures and almost symplectic structures).

Another example is for a foliation, which requires a reduction of the tangent bundle to a block matrix subgroup, together with an integrability condition so that the Frobenius theorem applies.

## Notes

1. ^ Which is a Lie group ${\displaystyle G\to GL(n,\mathbf {R} )}$ mapping to the general linear group ${\displaystyle GL(n,\mathbf {R} )}$. This is often but not always a Lie subgroup; for instance, for a spin structure the map is a covering space onto its image.
2. ^ Kobayashi (1972).
3. ^ Kobayashi (1972) I.4.
4. ^ Gauduchon (1997).
5. ^ Indeed, it is a bifunctor in G and X.
6. ^ In classical field theory, such a section ${\displaystyle \sigma }$ describes a classical Higgs field (Sardanashvily, G. (2006). "Geometry of Classical Higgs Fields". International Journal of Geometric Methods in Modern Physics. 03: 139. arXiv:. doi:10.1142/S0219887806001065.).
7. ^ It is a gravitational field in gauge gravitation theory (Sardanashvily, G. (2006). "Gauge gravitation theory from the geometric viewpoint". Int.J.Geom.Methods Mod.Phys. 3 (1): v–xx. arXiv:.)
8. ^ Besse 1987, §14.61

## References

• Chern, S.S. (1966). "The geometry of G-structures". Bull. Amer. Math. Soc. 72 (2): 167–219. doi:10.1090/S0002-9904-1966-11473-8.
• Gauduchon, P. (1997). "Canonical connections for almost-hypercomplex structures". Complex Analysis and Geometry. Pitman Research Notes in Mathematics Series. Longman. pp. 123–136.
• Kobayashi, S. (1972). Transformation Groups in Differential Geometry. Classics in Mathematics. Springer. ISBN 3-540-58659-8. OCLC 31374337.
• Sternberg, S. (1983). Lectures on Differential Geometry ((2nd ed.) ed.). New York: Chelsea Publishing Co. ISBN 0-8218-1385-4. OCLC 43032711.
• Godina M. and Matteucci P. (2003). "Reductive G-structures and Lie derivatives". Journal of Geometry and Physics. 47: 66–86. doi:10.1016/S0393-0440(02)00174-2.