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Weingarten equation and adjointness of the shape operator

Statement

Assume ACω. For tangent fields X,Y and a normal field ν along an embedded Riemannian submanifold,

Xν=SνX+Xν

and

g(SνX,Y)=g(II(X,Y),ν).

Consequently every shape operator Sν is self-adjoint. The choice hypothesis is inherited exactly through the smooth normal-bundle projections.

Facts & Assumptions

Given: Countable choice, the embedded Riemannian submanifold, tangent fields X,Y, and a normal field ν.

[F1]

The shape operator is SνX=(Xν). Shape operator.

[F2]

The normal connection is Xν=(Xν). Normal connection.

[F3]

The Gauss decomposition is XY=XMY+II(X,Y). Induced connection and second fundamental form.

[F4]

The ambient Levi–Civita connection is compatible with g. Levi civita connection.

Proof

technique · direct
1.1

Split Xν into its tangential and normal components. By [F1] its tangential component is SνX, and by [F2] its normal component is Xν. This proves the first displayed identity.

F1F2algebra
2.1

Since g(ν,Y)=0 along M, differentiation in the tangent direction X and [F4] give 0=Xg(ν,Y)=g(Xν,Y)+g(ν,XY). By step 1.1 the first inner product is g(SνX,Y); by [F3] the second is g(ν,II(X,Y)), since ν is normal and XMY is tangent. Rearranging proves the second displayed identity.

F3F4step 1.1algebra
3.1

Using [F5] and the symmetry of the metric, g(SνX,Y)=g(II(X,Y),ν)=g(II(Y,X),ν)=g(SνY,X)=g(X,SνY). Thus Sν is self-adjoint.

F5step 2.1algebra
4.1

All identities are vacuous on the empty submanifold and reduce to the unique zero maps when tangent or normal rank is zero. They apply unchanged in rank one and at boundary points. Positive definiteness is used for the orthogonal splitting and for the usual self-adjoint interpretation. The stated ACω is inherited through [F1]–[F3], and no new selection occurs.

F1F2F3step 1.1step 2.1step 3.1

Depends on

Used by

Dependency tree · two levels

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Sources