Kosmann lift

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Template:Use dmy dates In differential geometry, the Kosmann lift,[1][2] named after Yvette Kosmann-Schwarzbach, of a vector field X on a Riemannian manifold (M,g) is the canonical projection XK on the orthonormal frame bundle of its natural lift X^ defined on the bundle of linear frames.[3]

Generalisations exist for any given reductive G-structure.

Introduction

In general, given a subbundle QE of a fiber bundle πE:EM over M and a vector field Z on E, its restriction Z|Q to Q is a vector field "along" Q not on (i.e., tangent to) Q. If one denotes by iQ:QE the canonical embedding, then Z|Q is a section of the pullback bundle iQ(TE)Q, where

iQ(TE)={(q,v)Q×TEi(q)=τE(v)}Q×TE,

and τE:TEE is the tangent bundle of the fiber bundle E. Let us assume that we are given a Kosmann decomposition of the pullback bundle iQ(TE)Q, such that

iQ(TE)=TQ(Q),

i.e., at each qQ one has TqE=TqQu, where u is a vector subspace of TqE and we assume (Q)Q to be a vector bundle over Q, called the transversal bundle of the Kosmann decomposition. It follows that the restriction Z|Q to Q splits into a tangent vector field ZK on Q and a transverse vector field ZG, being a section of the vector bundle (Q)Q.

Definition

Let FSO(M)M be the oriented orthonormal frame bundle of an oriented n-dimensional Riemannian manifold M with given metric g. This is a principal SO(n)-subbundle of FM, the tangent frame bundle of linear frames over M with structure group GL(n,). By definition, one may say that we are given with a classical reductive SO(n)-structure. The special orthogonal group SO(n) is a reductive Lie subgroup of GL(n,). In fact, there exists a direct sum decomposition 𝔤𝔩(n)=𝔰𝔬(n)𝔪, where 𝔤𝔩(n) is the Lie algebra of GL(n,), 𝔰𝔬(n) is the Lie algebra of SO(n), and 𝔪 is the AdSO-invariant vector subspace of symmetric matrices, i.e. Ada𝔪𝔪 for all aSO(n).

Let iFSO(M):FSO(M)FM be the canonical embedding.

One then can prove that there exists a canonical Kosmann decomposition of the pullback bundle iFSO(M)(TFM)FSO(M) such that

iFSO(M)(TFM)=TFSO(M)(FSO(M)),

i.e., at each uFSO(M) one has TuFM=TuFSO(M)u, u being the fiber over u of the subbundle (FSO(M))FSO(M) of iFSO(M)(VFM)FSO(M). Here, VFM is the vertical subbundle of TFM and at each uFSO(M) the fiber u is isomorphic to the vector space of symmetric matrices 𝔪.

From the above canonical and equivariant decomposition, it follows that the restriction Z|FSO(M) of an GL(n,)-invariant vector field Z on FM to FSO(M) splits into a SO(n)-invariant vector field ZK on FSO(M), called the Kosmann vector field associated with Z, and a transverse vector field ZG.

In particular, for a generic vector field X on the base manifold (M,g), it follows that the restriction X^|FSO(M) to FSO(M)M of its natural lift X^ onto FMM splits into a SO(n)-invariant vector field XK on FSO(M), called the Kosmann lift of X, and a transverse vector field XG.

See also

Notes

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References