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How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

A circle is the boundary of a disk

Example

Let D2=B‾2(0,1)⊂R2 be the closed unit disk. It is a compact smooth surface with boundary S1=S2(0,1), and with the orientation of D2 induced from the standard orientation of R2, its induced boundary orientation is the standard counterclockwise orientation of S1. Consequently S1 with that orientation is null-cobordant, so its class is zero in Ω1SO and in Ω1O; and the circle with the opposite orientation has the same zero class and is the inverse of [S1] in Ω1SO.

Facts & Assumptions

Given: The closed unit disk D2=B‾2(0,1)⊂R2, the sphere S1=S2(0,1), the standard orientation of R2 (the one for which the identity chart is positive), and the orientations induced on D2 and on its boundary.

[F1]

For n≥1, write Bn={x:ρ(x)≥0} with ρ(x)=1−∣x∣2. At each boundary point choose an index j with ∂jρ≠0, move that coordinate last, and apply the inverse function theorem to the remaining n−1 coordinates together with ρ. Its inverse is smooth: the derivative formula for the C1 inverse bootstraps inductively to every order when the original map is smooth. Restricting to ρ≥0 gives a half-space chart, and these charts have smooth transitions because they are restrictions of ambient diffeomorphisms (The Euclidean inverse function theorem, Euclidean upper half-space and its boundary, Smooth charts, atlases, and structures with boundary). The interior uses ordinary Euclidean charts (Euclidean spaces and Euclidean open subsets as smooth manifolds). Thus Bn is a smooth manifold with boundary Sn−1. Inward vectors have dρ>0 (Boundary-defining functions exist locally and detect inward vectors, Boundary-defining functions), and Euclidean balls and spheres are compact (For n≥1, every Euclidean closed ball and every Euclidean sphere of positive radius is compact, Euclidean spheres and closed balls as subspaces of Rn).

[F2]

The induced boundary orientation is outward-normal-first: an outward vector followed by a positive basis of the boundary is a positive basis of the ambient tangent space (Induced boundary orientation, Oriented smooth manifolds and oriented charts).

[F3]

A closed oriented manifold is null-cobordant when it is oriented cobordant to the empty manifold; reversing the orientation of an oriented bordism flips both induced boundary orientations (Null-cobordant closed manifolds, Oriented smooth cobordism), and the classes of closed oriented 1-manifolds form Ω1SO with operation [M]+[N]=[M⊔N] and zero the class of ∅ (Unoriented and oriented bordism groups).

[F4]

Orientation-preserving diffeomorphic closed oriented manifolds have the same class (Disjoint union makes bordism classes abelian groups). A nonempty connected orientable manifold has exactly two orientations: relative to one supplied determinant ray the sign of another is locally constant, hence constant on the connected manifold (Oriented smooth manifolds and oriented charts).

Verification

1.1F1

(D2 is a compact smooth surface with boundary S1.) By [F1] with n=2, D2=B2 is a smooth manifold with boundary S1, and ρ(x)=1−∣x∣2 is a boundary-defining function; by compactness of Euclidean balls D2 is compact, hence a compact surface with boundary.

1.2F1F2

(The induced boundary orientation is counterclockwise.) Let p∈S1. Since ρ(x)=1−∣x∣2 has gradient ∇ρ(p)=−2p, the function ρ decreases in the radial direction, so the outward normal of D2 at p is the radial vector p (unit length). Let Jp=(−p2,p1) be the counterclockwise rotation of p by 90∘. In the standard orientation of R2 the basis (p,Jp) is positive, because det⁡(p,Jp)=∣p∣2=1>0. The outward-normal-first rule of [F2] therefore says that (p,Jp) is a positive basis of TpD2 exactly when Jp is a positive basis of TpS1; the unit tangent Jp is the counterclockwise direction of S1, so the induced boundary orientation of S1=∂D2 is counterclockwise.

2.1F3step 1.2construct

(Null-cobordisms of the two circles.) Let o be the counterclockwise orientation of S1. The map θ:[0,1)×S1→D2, θ(s,p)=(1−s/2)p, is a smooth embedding onto the open annulus {x:1/2<∣x∣≤1} and satisfies θ(0,p)=p, so it is a supplied collar (Smooth collars of a manifold boundary). With the whole boundary incoming, the standard orientation on D2 gives induced orientation o by step 1.2, so it null-bords (S1,−o). Reversing the disk orientation gives induced boundary orientation −o and null-bords (S1,o). Thus both oriented classes and their underlying unoriented classes are zero by [F3].

2.2F3F4step 1.2

(The two classes are mutually inverse.) Let W:=(−D2)⊔D2 with the disjoint-union orientation, a compact oriented surface whose boundary is the disjoint union of the two circles, and whose induced boundary orientation on ∂W is (clockwise)⊔(counterclockwise). As a bordism from the closed oriented manifold S1⊔(−S1) to ∅ it realises [S1]+[−S1]=[∅]=0 in Ω1SO by [F3]: the incoming face carries the negative of o⊔(−o), namely (−o)⊔o, which is exactly the induced orientation of ∂W.

3.1step 1.1step 1.2step 2.1step 2.2∎

(Assembly.) Steps 1.1–1.2 identify D2 as a compact smooth surface with boundary S1 and compute its induced boundary orientation as counterclockwise; step 2.1 gives the null-cobordisms of both oriented circles, so [S1]=0 in Ω1SO and in Ω1O; step 2.2 shows that the class of the opposite orientation is also 0 and is the inverse of [S1]. This is the asserted example.

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