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Oriented smooth cobordism

Definition

Let M0 and M1 be closed oriented smooth n-manifolds, with orientations o0 and o1. An oriented bordism from M0 to M1 is a bordism (W,θ0,θ1) from M0 to M1 in the sense of Unoriented smooth cobordism of closed manifolds, together with an orientation of W, such that the induced boundary orientation (Induced boundary orientation) of the incoming face (∂W)0 is the negative of the supplied orientation o0 of M0, and the induced boundary orientation of the outgoing face (∂W)1 is the supplied orientation o1 of M1. Oriented manifolds are oriented cobordant when such data exist.

Equivalent collar formulation. The condition is equivalent to the requirement that, in the collar parametrisations, the embeddings θ0:[0,1)×M0→W and θ1:(−1,0]×M1→W are orientation-preserving (Orientation-preserving parametrizations) for the product orientations of [0,1)×M0 and (−1,0]×M1 (Product orientations), the intervals carrying their standard orientations. Indeed, at a point of the incoming collar the derivative of θ0 in the interval direction is an inward normal vector, so θ0 is orientation-preserving exactly when an outward vector followed by the image orientation of M0 is a negative determinant of TW, that is, exactly when the induced boundary orientation of (∂W)0 is −o0; at the outgoing collar the derivative in the interval direction is an outward normal vector, so θ1 is orientation-preserving exactly when the induced orientation of (∂W)1 is o1. The induced orientation is independent of the choice of outward vector field (Boundary orientation is independent of the outward vector field), so the condition is well posed. This is the same outward-normal-first convention that the relative fundamental class uses to define the induced boundary orientation (Relative fundamental class and boundary orientation).

Orientation reversal and empty manifolds. An orientation of a manifold is a smooth choice of a ray in each determinant line (Oriented smooth manifolds and oriented charts); the opposite orientation reverses every ray pointwise and the manifold with that orientation is written −M. For a disconnected oriented manifold the reversal is taken on every component. The empty manifold carries its unique orientation and is its own negative. The definition uses no choice principle: the orientation of W and the collar data are supplied, and the boundary orientation is determined by the outward-normal-first convention.

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