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Smooth Cobordism Relations Groups and Rings
1 · Prerequisites
- Abelian Categories
- Absolute and Conditional Convergence; Rearrangement; Products
- Binary Operations, Monoids, Groups and Subgroups
- Bocksteins Steenrod Squares and Cohomology Operations
- Cardinal Arithmetic, Cofinality and the Alephs
- Categories, Functors and Natural Transformations
- Chain Complexes and Homology
- Chain Homotopy and the Homotopy Category
- Chern and Pontryagin Classes by Splitting and Complexification
- Chern–Weil Theory and Characteristic Forms
- Classification of Covering Spaces
- Compactness
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Composition Series, the Jordan–Hölder Theorem and Solvable Groups
- Congruences, the Integers Modulo n and the Chinese Remainder Theorem
- Connectedness
- Connections Levi Civita and Parallel Transport
- Constant Rank, Submersions, Immersions and Regular Level Sets
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Countability Axioms and Cardinal Functions
- Covering Spaces and Lifting
- Cup Cap Cross Products and Cohomology Rings
- Cw Complexes and Cellular Homology
- Derived Functors
- Determinants of Matrices over a Commutative Ring
- Diagonalisation and the Minimal Polynomial
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Double Complexes Exact Couples and Convergence
- Dual Spaces, Bilinear and Quadratic Forms, and Sylvester's Law of Inertia
- Eigenvalues, Eigenvectors and the Characteristic Polynomial
- Euclidean Ordinary Differential Equations with Smooth Dependence
- Exactness and the Member Calculus
- Ext and Balanced Resolutions
- Exterior Powers, Orientation and Hodge Duality
- Fibrations Fiber Bundles and Homotopy Exact Sequences
- Filters and Ultrafilters
- Finite Counting, Factorials and Binomial Coefficients
- Foundations of the Real Numbers for Analysis
- Free Groups and Presentations
- Free Modules, Exact Sequences, Projective and Injective Modules
- Free Products and Amalgamation
- Fubini and Change of Variables
- Function Space Topologies and the Exponential Law
- Gaussian Elimination, Elementary Matrices and Reduced Row Echelon Form
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Hausdorff via the Diagonal
- Hereditary and Productive Behaviour of the Separation Axioms
- Higher Homotopy Groups and Cofiber Sequences
- Homology Axioms Degree and Classical Applications
- Homotopy and Homotopy Equivalence
- Hurewicz Whitehead Freudenthal and Cw Approximation
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Inner Product Spaces, Gram-Schmidt, Projections and Adjoints
- Kunneth Exactness and Splittings over Principal Ideal Domains
- Leray–Hirsch, the Thom Isomorphism, and Gysin Sequences
- Limits and Colimits
- Limits of Real Functions
- limsup, liminf, and Subsequential Limits
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Local Coefficients, Twisted Homology, and Duality
- Long Exact Sequences in Homology
- Manifolds with Boundary Collars and Orientations
- Matrices, the Matrix of a Linear Map, and Change of Basis
- Metric Spaces
- Mixed Partials, Taylor Formulae, and Extrema
- Modules, Submodules, Quotient Modules and the Isomorphism Theorems
- Monotone Functions, Discontinuities, and Continuity Sets
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Obstruction Theory, Postnikov Towers, and Classifying Spaces
- Order, Zorn's Lemma, and the Axiom of Choice
- Ordinal Arithmetic and the First Uncountable Ordinal
- Ordinals, Cardinals, and Transfinite Recursion
- Orientations Poincare Lefschetz and Alexander Duality
- Partitions of Unity and Paracompactness
- Picard-Lindelöf and First-Order Ordinary Differential Equations
- Polynomial Rings, the Division Algorithm and Roots
- Power Series and Real-Analytic Functions
- Preadditive and Additive Categories and Biproducts
- Projective and Injective Resolutions
- Properties of the Integral and the Working FTC
- Rank Theorems and Embedded Submanifolds
- Rees Modules Artin Rees and Hilbert Samuel Theory
- Reflective Subcategories and the Adjoint Functor Theorems
- Relations, Functions, and Quotients
- Relative Homology Excision and Mayer Vietoris
- Riemann Curvature and Riemannian Submanifolds
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Sard Theorem and Transversality
- Separation Axioms: the Hierarchy
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Simple Field Extensions and the Construction of the Complex Numbers
- Simplicial Complexes and Simplicial Homology
- Simplicial Subdivision and Simplicial Approximation
- Singular Chains and Singular Homology
- Singular Cohomology and Coefficient Theorems
- Smooth Manifolds and Smooth Maps
- Smooth Partitions of Unity and Exhaustions
- Smooth Vector Bundles and Sections
- Spectral Sequences
- Stiefel Whitney and Euler Classes by Universal Constructions
- Subobject Lattices Generators and the Grothendieck Axioms
- Subspaces, Products, and Quotients
- Suprema and Infima
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- Tangent Cotangent and the Differential
- Tensor Fields Exterior Algebra and Differential Forms
- Tensor Products of Modules
- The Cantor Set, Baire Category, and Measure Zero in ℝ
- The Derivative and the Mean Value Theorems
- The Determinant of a Linear Operator, Cofactors and Cramer's Rule
- The Diagram Lemmas in an Abelian Category
- The Exponential Function
- The Exterior Derivative and Cartan Calculus
- The Fundamental Group
- The Fundamental Group of the Circle
- The Fundamental Theorems of Calculus
- The Group Algebra and Representations of Finite Groups
- The Inverse and Implicit Function Theorems
- The Inverse Function Theorem Completed
- The Riemann Integral in Rᵐ and Jordan Content
- The Riemann Integral: Definition and Integrability
- The Seifert–van Kampen Theorem
- The Serre Spectral Sequence and Applications
- The Topology of Euclidean Space
- The Total Derivative in ℝᵐ → ℝⁿ
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topological Vector Bundles and Grassmannian Classification
- Topology of ℝ
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Uniform Spaces: the Three Definitions
- Universal Coefficients and Kunneth Theorems
- Universal Properties, Representables and the Yoneda Lemma
- Urysohn's Lemma and the Tietze Extension Theorem
- Vector Fields Flows and Lie Derivatives
- Vector Spaces, Linear Subspaces, Span and Direct Sums
- Whitney Embedding Tubular Neighbourhoods and Approximation
2 · Summary
This page builds geometric cobordism from the ground up: a bordism is a compact manifold with boundary carrying a decomposition of its boundary into an incoming and an outgoing part together with collar parametrisations, and cobordance is the equivalence relation of being joined by such data. The collars are part of the definition, so gluing and the geometric group and ring laws use the supplied data without a choice axiom; the optional comparison of different collar systems uses countable choice, and the characteristic-class constructions below inherit AC; the boundary conventions are fixed outward-normal-first, so the signs in the oriented theory are stated once and used consistently.
The first block proves that cobordism is an equivalence relation in both the unoriented and the oriented theory, via cylinders, dual bordisms and collar gluing, and derives the elementary computations attached to the relation: null-cobordism, zero-dimensional bordism groups, and the product boundary formula for products with at most one boundary factor. The second block equips the sets of cobordism classes with the disjoint-union group structure and the Cartesian-product ring structure, with the one-point class (positively oriented in the oriented theory) as unit and the Koszul sign in the oriented theory.
The page closes with the characteristic-number obstruction to bounding: the stable tangent bundle of a boundary splits off a trivial line, the fundamental class of a boundary pushes forward to zero, and consequently all Stiefel-Whitney numbers (respectively all Pontryagin numbers, for a boundary of an oriented manifold) of a closed boundary vanish. The final remark fixes the seam between these geometric constructions and the Thom-spectrum picture, which belongs to algebraic topology and to later pages.
3 · Logical flowchart
4 · Definitions, theorems and proofs
Unoriented smooth cobordism of closed manifolds
Definition
Fix an integer . In this library a manifold is Hausdorff and second-countable, and closed means compact without boundary (Smooth manifolds and their smooth charts, Open cover, subcover, and compact topological space; a compact subset is a subspace that is compact in its own right).
Let and be closed smooth -manifolds. A (unoriented) bordism from to is data consisting of
- a compact smooth -manifold with boundary (Smooth charts, atlases, and structures with boundary) whose boundary is decomposed as a disjoint union of boundary subsets that are both open and closed in ; and
- smooth embeddings and (Immersions and embeddings for manifolds with boundary) onto open collar neighbourhoods of and respectively, with for (Smooth collars of a manifold boundary).
Each is then a union of components of , of which there are finitely many because is compact; and is a closed embedded smooth -manifold (The boundary of a positive-dimensional manifold is a closed embedded smooth (n-1)-manifold). The two closed -manifolds and are cobordant when such data exist; we then also say that is a bordism from to and that bounds .
The collar embeddings are part of the data, not a choice made afterwards: every gluing argument on this page uses the supplied collars, which is why no choice principle is required for the cobordism relation. The parametrisation widths are fixed to the standard intervals and ; a collar supplied with a different width is rescaled to this form before it is used, and the rescaled embedding is again a smooth embedding onto the same collar neighbourhood.
The empty manifold is allowed as or and as , and is allowed; a bordism from the empty -manifold to the empty -manifold is exactly a compact smooth -manifold with empty boundary. The definition depends only on the smooth structures of , and and on the supplied data; it introduces no equivalence relation by itself, and the statement that cobordism is an equivalence relation is proved later.
Oriented smooth cobordism
Definition
Let and be closed oriented smooth -manifolds, with orientations and . An oriented bordism from to is a bordism from to in the sense of Unoriented smooth cobordism of closed manifolds, together with an orientation of , such that the induced boundary orientation (Induced boundary orientation) of the incoming face is the negative of the supplied orientation of , and the induced boundary orientation of the outgoing face is the supplied orientation of . 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 and are orientation-preserving (Orientation-preserving parametrizations) for the product orientations of and (Product orientations), the intervals carrying their standard orientations. Indeed, at a point of the incoming collar the derivative of in the interval direction is an inward normal vector, so is orientation-preserving exactly when an outward vector followed by the image orientation of is a negative determinant of , that is, exactly when the induced boundary orientation of is ; at the outgoing collar the derivative in the interval direction is an outward normal vector, so is orientation-preserving exactly when the induced orientation of is . 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 . 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 and the collar data are supplied, and the boundary orientation is determined by the outward-normal-first convention.
Cylinders give reflexivity of cobordism
Statement
For every closed smooth -manifold , the product with its product smooth structure and the collars is a bordism from to : take and (Unoriented smooth cobordism of closed manifolds).
If is oriented and carries its standard orientation, then with the product orientation of the induced boundary orientation (Induced boundary orientation) on is and that on is ; consequently oriented by is an oriented bordism from to (Oriented smooth cobordism). Hence is cobordant to itself in both theories.
Facts & Assumptions
Given: A closed smooth -manifold , the product with its product smooth structure, and the maps , . In the oriented case, orientations of and the standard orientation of .
The boundaryless product atlas is given by Products of smooth manifolds have a canonical product smooth structure. For , use the same product charts with interval charts in the interior, near , and near ; the last two take values in a half-space and their transitions extend smoothly, so Immersions and embeddings for manifolds with boundary supplies the usual product collars. The interval is compact by For , every Euclidean closed ball and every Euclidean sphere of positive radius is compact after affine rescaling, and is compact by A product of finitely many compact spaces is compact in the product topology.
If one factor of a product is closed, the boundary is the product of the other factor's boundary with the closed factor, and the orientation sign is of the closed factor: for oriented with one has with the product boundary orientation, while if then carries times the product orientation (Boundary orientation of a product with at most one boundary factor). On the interval with its standard orientation, (Boundary orientation is independent of the outward vector field).
The product orientation is the tensor product of the selected rays under the ordered determinant isomorphism, and the induced boundary orientation is the outward-normal-first one (Product orientations, Induced boundary orientation).
A bordism from to is data with a decomposition of into open and closed parts and collar embeddings onto open collar neighbourhoods; an oriented bordism additionally carries an orientation of whose induced boundary orientations are on the incoming and on the outgoing face (Unoriented smooth cobordism of closed manifolds, Oriented smooth cobordism).
The maps have injective differentials and are homeomorphisms onto their images, hence are smooth embeddings (Immersions and embeddings for manifolds with boundary, Diffeomorphisms and local diffeomorphisms of manifolds).
Proof
( with the two collars is a bordism.) The product charts and compactness in [F1] make a compact smooth manifold with boundary. The boundary of is by [F2] applied with the second factor ; the two parts are open and closed in the boundary. The maps and are smooth embeddings by [F5]; their images are and , which are open neighbourhoods of and in , and , . By [F4] the data are a bordism from to ; the construction uses no choice.
(Induced orientations of the two faces.) Suppose is oriented by . Apply the second clause of [F2] to , , and with its standard orientation: the boundary carries times the product orientation . Since by [F2], the face carries and the face carries .
( oriented by is an oriented bordism.) Reverse the orientation of when is odd; that is, orient by . Reversing an orientation reverses every induced boundary orientation, so by step 1.2 the face now carries and the face carries . With and , this is exactly the oriented bordism condition incoming, outgoing of [F4]: is an oriented bordism from to . For even the orientation is the product orientation itself.
(Reflexivity in both theories.) Step 1.1 exhibits the cylinder as a bordism from to , so is cobordant to itself in the unoriented theory; step 2.1 exhibits, for every orientation of a closed smooth , an oriented bordism from to , so is oriented cobordant to itself. The empty manifold is covered (, ). No choice principle is used anywhere: the data are the explicit collars of the product.
Reversing a cobordism gives symmetry
Statement
If is a bordism from a closed smooth manifold to a closed smooth manifold (Unoriented smooth cobordism of closed manifolds), then swapping the two boundary parts and the two collar parametrisations yields a bordism from to .
In the oriented theory, if and are oriented and with an orientation of is an oriented bordism from to (Oriented smooth cobordism), then the same manifold with the opposite orientation, again with the two boundary parts and the two collar parametrisations interchanged, is an oriented bordism from to : the induced boundary orientations match on the incoming face and on the outgoing face.
Facts & Assumptions
Given: A bordism from to with boundary decomposition and collars , ; in the oriented case, orientations and an orientation of with induced boundary orientations on and on .
A bordism is data with a decomposition of into open and closed parts and smooth embeddings onto open collar neighbourhoods with (Unoriented smooth cobordism of closed manifolds, Immersions and embeddings for manifolds with boundary).
An oriented bordism additionally carries an orientation of whose induced boundary orientation is on the incoming face and on the outgoing face; the opposite orientation of an oriented manifold reverses every determinant ray pointwise (Oriented smooth cobordism, Oriented smooth manifolds and oriented charts).
The induced boundary orientation is defined by the outward-normal-first rule: an outward vector followed by a positive basis of the boundary is a positive basis of the ambient tangent space; it is independent of the chosen outward vector field (Induced boundary orientation, Boundary orientation is independent of the outward vector field).
The reflection is a diffeomorphism of onto and of onto (Diffeomorphisms and local diffeomorphisms of manifolds, Orientation-preserving parametrizations).
Proof
(The dual bordism.) Keep the manifold and swap the roles of the two boundary parts, setting and ; these are again open and closed in and cover it. Define The reflection maps onto and onto by [F4], so the composites are defined; each is a smooth embedding, being a composite of the smooth embedding with a diffeomorphism of the interval factor, and its image is the same open collar neighbourhood as that of . Moreover and . By [F1], is a bordism from to . No choice is used.
(The oriented dual.) Suppose now that are oriented and carries an orientation making an oriented bordism from to . Keep the swapped data of step 1.1 and give the opposite orientation. By [F3], the induced boundary orientation of a face is computed from the ambient orientation by the outward-normal-first rule, so reversing the ambient orientation reverses the induced orientation of every boundary face: for a face with induced orientation under one orientation of , the same face has induced orientation under the opposite orientation. Hence the new incoming face carries and the new outgoing face carries . By [F2], with the opposite orientation is an oriented bordism from to .
(Assembly.) Step 1.1 gives symmetry of the unoriented cobordism relation; step 2.1 gives symmetry of the oriented relation with the reversed orientation on the dual bordism and the required boundary signs incoming and outgoing. The constructions are explicit and use no choice principle.
Collar gluing and seam smoothing give transitivity
Statement
Let be a bordism from a closed smooth -manifold to a closed smooth -manifold , and let be a bordism from to a closed smooth -manifold , with the same in both (Unoriented smooth cobordism of closed manifolds). The outgoing collar of the first and the incoming collar of the second agree on after the seam identification and combine to a bi-collar ; thereby they define a smooth structure on the glued space making it a compact smooth -manifold with boundary whose seam is interior. The structure is canonical for the given data: it is the maximal atlas generated by the two given smooth structures and the bi-collar, and, assuming (The Axiom of Countable Choice ()), a change of collar presentation changes it at most by a diffeomorphism fixed off a neighbourhood of the seam, by the collar-comparison argument in The double has a well-defined smooth structure. The boundary decomposes as , and the outer collars and make a bordism from to .
In the oriented theory, if both bordisms are oriented (Oriented smooth cobordism), the induced orientations on the common boundary component are opposite, the orientations glue to an orientation of , and with that orientation is an oriented bordism from to . The glued bordism and transitivity use only the supplied collars and require no choice principle. The additional comparison of different collar systems uses through the cited comparison theorem.
Facts & Assumptions
Given: Bordisms from to and from to , with and . In the oriented case, orientations of satisfying the oriented bordism conditions.
Each is a compact smooth manifold with boundary; the boundary parts are open and closed in , and the collars are smooth embeddings onto open collar neighbourhoods with (Unoriented smooth cobordism of closed manifolds, Smooth collars of a manifold boundary, Immersions and embeddings for manifolds with boundary).
An oriented bordism condition is equivalent to its collars being orientation-preserving for the interval-first product orientations; the induced boundary orientation is outward-normal-first and independent of the outward field (Oriented smooth cobordism, Induced boundary orientation, Boundary orientation is independent of the outward vector field).
A quotient of a topological space carries the quotient topology, characterised by the universal property for continuous maps out of it (The quotient topology of a surjection, quotient maps, saturated sets, and the quotient of a space by an equivalence relation with its canonical projection).
A smooth structure is a maximal smooth atlas; compatibility of charts is smoothness of transitions in the local-extension sense; smooth embeddings are smooth maps that are homeomorphisms onto their images, and open subsets carry restricted smooth structures (Smooth charts, atlases, and structures with boundary, Smooth manifolds and their smooth charts, Smooth maps between manifolds with boundary, Diffeomorphisms and local diffeomorphisms of manifolds, An open subset of a smooth manifold has a canonical restricted smooth structure); products carry the product smooth structure (Products of smooth manifolds have a canonical product smooth structure).
Assuming (The Axiom of Countable Choice ()), the double admits comparison diffeomorphisms for different collars (The double has a well-defined smooth structure, proof steps 4.1–9.1). That proof constructs on a labelled half a boundary-fixing diffeomorphism with near the boundary. Its cutoff can be supported in a chosen neighbourhood of the boundary. The same construction applies near an open-and-closed boundary part, leaving the other parts fixed; it is used only in step 3.2 below.
Continuous images of compact spaces are compact (A continuous image of a compact space is compact; a continuous real-valued map on a nonempty compact space attains a maximum and a minimum; and a continuous bijection from a compact space to a Hausdorff space is a homeomorphism), finite products of Hausdorff spaces are Hausdorff (Arbitrary products preserve , , and Hausdorffness), and subspaces of second-countable spaces are second-countable (Second countability is hereditary). A binary product of second-countable spaces needs no countable choice: instantiate one countable basis in each factor, and enumerate their products by pairs of natural numbers. A finite union of bases of an open cover is a basis of the whole space.
Proof
(The glued space and the bi-collar.) Let and let be the equivalence relation on generated by for ; put with the quotient topology. Define The two formulas agree at and each is continuous on its closed half, so is continuous; it is injective because are injective and their images meet exactly in the identified seam; and it is open onto its image: for a relatively open subset of the two half-images are open in the collar neighbourhoods of and , whose union is saturated. Hence is open in and is a homeomorphism onto . The images of and are open in and homeomorphic to those open submanifolds, and .
(The smooth atlas.) For a chart of define the seam chart Take the atlas consisting of the charts of with domain disjoint from , the charts of with domain disjoint from , and all seam charts . Its domains cover by step 1.1 and are open in . Transitions between two charts from the same half are smooth by the given structures; a chart of the first half and one of the second have disjoint domains; two seam charts have transition , smooth in coordinates; and a seam chart with a chart of (or ) has overlap in (or ), where it equals the smooth expression (or ) in the coordinates . Thus the generated maximal atlas is a smooth structure of dimension with boundary; each point of the seam lies in the seam chart and has a Euclidean neighbourhood.
(Boundary, outer collars and bordism structure.) The seam is , which every seam chart exhibits as an interior hypersurface ; hence the boundary of is the image of . Put and ; these are open and closed in and cover it. The outer collars and are unchanged smooth embeddings onto open collar neighbourhoods of these parts with the required normalisation, so is a bordism from to .
(Canonicity and conditional collar comparison.) The atlas of step 2.1 is determined by the supplied collars: changing a chart of changes a seam chart by , so the generated maximal atlas is unchanged. For the additional comparison assume . Normalize outgoing collars by and incoming collars by . Apply the boundary-fixing comparison construction [F5] separately in and , supported near their seam parts, to obtain intertwining the old and new collars near the seam. They descend to a bijection of the glued spaces because both fix the seam points; in the old source and new target seam coordinates the descended map is near . Away from the seam it and its inverse are the smooth maps . Thus it is a diffeomorphism fixed off a neighbourhood of the seam. Only this comparison uses [F5]; construction and transitivity use the given collars directly.
(The orientations glue.) Assume both bordisms oriented. By [F2], is orientation-preserving for the product orientation of , and is orientation-preserving for the product orientation of : both use the same orientation of the seam and the interval coordinate first. In the bi-collar coordinates of step 1.1 this says that a basis is positive in the orientation of for and in the orientation of for . Therefore the chart system that declares all charts of the first half positive for the orientation of and all charts of the second half positive for the orientation of is consistent on overlaps: the transition across the seam is the identity in the coordinates with Jacobian determinant . By step 2.1 this defines one orientation of . Equivalently, the induced orientations of the common boundary component are as the outgoing face of and as the incoming face of , so they are opposite and glue. On the outer faces the induced orientations are and , unchanged from the two bordisms, and the outer collars remain orientation-preserving; hence with this orientation is an oriented bordism from to .
(Compactness, Hausdorffness and second countability.) The finite disjoint union is compact Hausdorff: finite subcovers of its two summands combine, and separation is checked within a summand or by the disjoint summands. Let be the quotient. It is closed: the saturation of a closed adds only the images of its intersections with the two closed seam parts under the seam-identifying homeomorphism, hence is closed. For distinct , the fibres are finite and disjoint. Hausdorffness of gives disjoint open sets containing these two fibres (intersect and unite finitely many separating neighbourhoods). The open sets and contain and are disjoint, proving Hausdorffness. Compactness follows from [F6]. Choose countable bases of ; their restrictions give bases of , and the products of the basis of with rational intervals give a countable basis of . Their union is a countable basis of by [F6]. Together with steps 2.1, 3.1 and 4.1 this makes the required compact smooth bordism, oriented when the supplied bordisms are. No choice axiom is needed for transitivity.
Smooth cobordism is an equivalence relation
Statement
For every , unoriented cobordism of closed smooth -manifolds (Unoriented smooth cobordism of closed manifolds) and oriented cobordism of closed oriented smooth -manifolds (Oriented smooth cobordism) are reflexive by cylinders, symmetric by dual bordisms (orientation-reversed in the oriented case), and transitive by collar gluing. Restricted to any set of such manifolds in either theory, cobordism is therefore an equivalence relation (Equivalence relation, equivalence class, and the quotient set ) and partitions into classes . The collection of manifolds on arbitrary underlying sets is not itself a set; global bordism sets and the notation use the bounded models introduced in the subsequent bordism-group definition. No choice principle is used, and no claim about diffeomorphism classification is made.
Facts & Assumptions
Given: An integer , closed smooth -manifolds, and in the oriented theory closed oriented smooth -manifolds. A closed manifold is compact without boundary (Open cover, subcover, and compact topological space; a compact subset is a subspace that is compact in its own right, Smooth manifolds and their smooth charts).
For every closed smooth -manifold the cylinder with its product collars is a bordism from to , and in the oriented case it carries an orientation making it an oriented bordism from to ; hence is cobordant to itself in both theories (Cylinders give reflexivity of cobordism).
Swapping the boundary parts and collar parametrisations of a bordism from to yields a bordism from to ; in the oriented case the dual with the opposite orientation on the same manifold is an oriented bordism from to (Reversing a cobordism gives symmetry).
If is a bordism from to and a bordism from to , the collar gluing produces a bordism from to , and in the oriented case the orientations glue to an orientation making it an oriented bordism from to (Collar gluing and seam smoothing give transitivity).
A binary relation on a set is an equivalence relation when it is reflexive, symmetric and transitive; for an equivalence relation the equivalence classes form a partition of the set and denotes the class of (Equivalence relation, equivalence class, and the quotient set ).
Proof
(Reflexivity.) Let be a closed smooth -manifold, oriented by in the oriented theory. By [F1] the cylinder with its product collars is a bordism from to , and with the orientation it is an oriented bordism from to . Thus is cobordant to itself in both theories.
(Symmetry.) If is cobordant to , choose a bordism ; the dual data of [F2] give a bordism from to . If is an oriented bordism from to , the same manifold with the opposite orientation and the swapped collars is an oriented bordism from to , with induced orientations and on the incoming and outgoing faces.
(Transitivity.) If is cobordant to through and is cobordant to through , the collar gluing of [F3] gives a bordism from to ; if both bordisms are oriented, the glued orientation makes the result an oriented bordism from to .
(Equivalence relation on a set.) Let be any set of closed smooth -manifolds, with supplied orientations in the oriented theory. Restricted to , cobordism is reflexive by step 1.1, symmetric by step 1.2 and transitive by step 1.3. Thus [F4] gives an equivalence relation on and the quotient classes . The three properties hold for arbitrary manifolds, but the set-theoretic quotient is asserted only on a set of models; the subsequent definition constructs global bordism sets this way. The argument uses only supplied collar data and no choice principle.
Null-cobordant closed manifolds
Definition
A closed smooth -manifold is null-cobordant if it is cobordant to the empty -manifold, that is, if there is a bordism from to (Unoriented smooth cobordism of closed manifolds).
Unwinding the bordism data, this is equivalent to the following statement: there is a compact smooth -manifold whose boundary is carried by a collar onto all of , so that and restricts to a diffeomorphism (Smooth collars of a manifold boundary, Diffeomorphisms and local diffeomorphisms of manifolds). Indeed, for a bordism to the empty manifold the outgoing boundary part is empty, hence ; conversely such a collar gives a bordism from to by taking , and the empty map. Thus, informally, is null-cobordant exactly when is (diffeomorphic to) the whole boundary of a compact smooth -manifold.
In the oriented theory, a closed oriented -manifold is null-cobordant if it is oriented cobordant to the empty oriented manifold (Oriented smooth cobordism). Because the incoming face contributes the negative orientation, a null-cobordism satisfies: the induced boundary orientation of the whole boundary is . Thus is null-cobordant exactly when occurs as the orientation opposite to the induced boundary orientation of some compact oriented -manifold; reversing the orientation of presents as the induced boundary with its outward-normal-first orientation. The empty manifold carries its unique orientation and is null-cobordant in both theories, being cobordant to itself by the cylinder.
Null-cobordism depends only on the cobordism class: if is cobordant to and is null-cobordant, then is cobordant to and to , and transitivity of the cobordism relation (Smooth cobordism is an equivalence relation) gives that is null-cobordant; the same holds in the oriented theory. The definition uses no choice principle.
Unoriented and oriented bordism groups
Definition
Fix . By the cobordism equivalence relation (Smooth cobordism is an equivalence relation) the closed smooth -manifolds are partitioned into cobordism classes (Unoriented smooth cobordism of closed manifolds). Let be the set of these classes in the bounded model convention below, and let be the set of oriented cobordism classes (Oriented smooth cobordism).
Set-size convention. For each use the set of all closed smooth -manifold structures on subsets of , and in the oriented theory include the orientation datum, before taking the quotient by cobordism. Every closed smooth -manifold has such a model: compactness gives a finite chart cover , and the map , with the least index for which , is injective into . Transport the topology, maximal atlas, and supplied orientation along this injection; its image is diffeomorphic to the original manifold. This uses only a finite chart cover, not a choice of a model for every manifold simultaneously. Two transported models are diffeomorphic, and a cylinder of Cylinders give reflexivity of cobordism with outgoing collar composed with a diffeomorphism's inverse shows they are cobordant (orientation-preservingly in the oriented case). Thus means the unique class of any such model. Products and disjoint unions are returned to this set of models in the same way; their class is independent of the transport.
The operation. Disjoint union of manifolds defines operations where is the orientation of the disjoint union whose restriction to each summand is the given orientation, and finite disjoint unions carry the transported component atlases (Countable disjoint unions of fixed-dimensional smooth manifolds are smooth manifolds); for summands with boundary the same construction uses half-space charts. Finite union preserves compactness and combines finitely many countable bases, so this boundary extension requires no countable choice. The class of the empty -manifold is the displayed zero : it is null-cobordant and is a two-sided identity for the operation, since is canonically diffeomorphic to (Null-cobordant closed manifolds).
Well-definedness. The operations are independent of the chosen representatives. If is a bordism from to for , then the disjoint union carries the canonical smooth structure of a compact -manifold with boundary , the collars and are smooth embeddings onto collar neighbourhoods of the boundary parts, and the decomposition of the boundary into the two parts is again open and closed; hence is a bordism from to . In the oriented case, orienting the disjoint union by the given orientations makes the disjoint union of the oriented bordisms an oriented bordism between the disjoint unions, because the induced boundary orientation is computed componentwise and each summand carries its required sign. Thus whenever , and similarly in the oriented theory. The class of a finite disjoint union is computed from the canonical smooth structure on disjoint unions; no further choice is made.
Deferred axioms and the forgetful map. That these operations satisfy the group axioms (associativity, commutativity, identity and inverses) is not asserted here: it is proved in the following theorem, together with the finiteness of the inverse in the unoriented theory. The forgetful map sends the oriented class of a closed oriented -manifold to its underlying unoriented cobordism class; it is well defined because an oriented bordism between two oriented manifolds is in particular a bordism between their underlying manifolds, so oriented cobordant manifolds are cobordant.
Disjoint union makes bordism classes abelian groups
Statement
For each , the operations and make and abelian groups (Unoriented and oriented bordism groups, Group and abelian group). The operation is well defined: if is cobordant to for , the disjoint unions and are cobordant via the disjoint union of the two bordisms. It is associative and commutative, the canonical diffeomorphisms of finite disjoint unions identifying the two bracketings and the two orders, and the class of the empty manifold is a two-sided identity. Inverses: for every closed , in because is the boundary of ; for every closed oriented , in because is the boundary of the cylinder with the appropriate orientation. No choice principle is used.
Facts & Assumptions
Given: An integer , closed smooth -manifolds and closed oriented smooth -manifolds, and their classes in , with the operation .
The operation is well defined by disjoint unions of bordisms, the disjoint union of finitely many presented smooth manifolds carries its canonical smooth structure, and the empty class is the zero of the displayed operation (Unoriented and oriented bordism groups, Countable disjoint unions of fixed-dimensional smooth manifolds are smooth manifolds).
A map from a finite disjoint union with its canonical smooth structure is smooth exactly when each restriction to a summand is smooth, so the canonical bijections and that act as the identity on summands are diffeomorphisms, and they respect the disjoint-union orientations (A map from a disjoint union is smooth iff each restriction is smooth, Diffeomorphisms and local diffeomorphisms of manifolds).
The cylinder with its product structure and collars is a bordism from to , and with the orientation it is an oriented bordism from to ; the induced orientation on is and on is (Cylinders give reflexivity of cobordism, Products of smooth manifolds have a canonical product smooth structure, Product orientations, Boundary orientation of a product with at most one boundary factor, Induced boundary orientation).
Cobordism is an equivalence relation in both theories, and a closed manifold is null-cobordant exactly when it is cobordant to the empty manifold; the class of a null-cobordant manifold is zero in the corresponding bordism set (Smooth cobordism is an equivalence relation, Null-cobordant closed manifolds, Oriented smooth cobordism, Unoriented smooth cobordism of closed manifolds).
A group is a monoid in which every element is invertible; the axioms are associativity (G1), a two-sided identity (G2) and two-sided inverses (G3), and it is abelian when the operation is commutative (Group and abelian group).
Proof
(Diffeomorphic manifolds are cobordant; the class of a diffeomorphism type.) Let be a diffeomorphism of closed smooth -manifolds. Then with the collars and is a bordism from to , because and are smooth embeddings onto collar neighbourhoods of and (identified with by ) and the boundary parts cover . If is orientation-preserving between and , orient by ; by [F3] the incoming face carries and the outgoing face carries , so is an oriented bordism from to . Consequently diffeomorphic closed manifolds, respectively orientation-preserving diffeomorphic closed oriented manifolds, are cobordant.
(Identity.) The empty -manifold is a summand with and as smooth manifolds, and it is null-cobordant; hence in both theories.
(Unoriented inverses: exponent two.) Let be a closed smooth -manifold. Consider and view its whole boundary as the incoming part, with no outgoing part: the map given by on the first summand and on the second has disjoint open images and whose union is an open neighbourhood of , is a smooth embedding onto it, and satisfies . Hence is null-cobordant, so in .
(Associativity.) Let be closed smooth -manifolds. The canonical bijection which is the identity on each summand is a diffeomorphism by [F2]; in the oriented theory it preserves the disjoint-union orientations. By step 1.1 the two sides are cobordant (oriented cobordant), so by [F1].
(Commutativity.) The canonical bijection swapping the summands is a diffeomorphism by [F2] and preserves the disjoint-union orientations; by step 1.1 it gives in both theories.
(Oriented inverses.) Let be a closed oriented -manifold and orient by ; by [F3] the induced boundary orientations are on and on . View the whole boundary as the incoming part with the single collar of step 1.3; the incoming face is with the orientation of the source , and the required condition is that the induced orientation equal its negative, namely ; this is exactly what the two faces carry. Hence is null-cobordant and in .
(The group axioms.) By [F5], associativity (G1) is step 2.1, the two-sided identity (G2) is step 1.2, and two-sided inverses (G3) are steps 1.3 and 2.3; commutativity is step 2.2. Therefore and are abelian groups for every . The construction uses only the supplied smooth structures and collars, so no choice principle is used.
The fundamental class of a boundary pushes forward to zero
Statement
Let be a compact -oriented smooth -manifold with boundary , where is a commutative unital ring (Relative fundamental class and boundary orientation). The manifold carries the induced boundary orientation, and for the canonical mod-two orientation may be used, so that the statement applies to every compact smooth manifold (Every manifold is F2-orientable and orientability is componentwise). Let be the inclusion, a closed embedding of a smooth -manifold, and let be the fundamental class of the induced orientation (Fundamental class of a compact oriented manifold).
Then in , and consequently Empty boundary, dimension zero, disconnected manifolds and the empty manifold are included, and no choice principle is used.
Facts & Assumptions
Given: A compact -oriented smooth -manifold with boundary , the inclusion , the induced boundary orientation on , and the fundamental class .
The relative fundamental class is the unique class restricting to the prescribed local generators at interior points, the induced boundary orientation on is the one whose local generator at is the restriction of the connector , and consequently in ; the construction handles closed components, dimension zero and the empty case, and uses no AC (Relative fundamental class and boundary orientation, Fundamental class of a compact oriented manifold).
The singular homology of the pair is naturally long exact: , so at the image of equals the kernel of (Long exact sequence of a pair).
The Kronecker pairing descends through cocycle and cycle representatives, is additive in each variable, and satisfies for every continuous (Kronecker evaluation pairing, The kronecker pairing is independent of cocycle and cycle representatives).
For every topological manifold carries a canonical -orientation, and this construction is choice-free (Every manifold is F2-orientable and orientability is componentwise).
If is compact then its boundary , being a closed embedded submanifold and hence a closed subset of the compact space , is compact (The boundary of a positive-dimensional manifold is a closed embedded smooth (n-1)-manifold, A closed subspace of a compact space is compact, and a finite union of compact subspaces is compact).
Proof
(.) By the definition of the relative fundamental class and of the induced boundary orientation, the connector sends the relative fundamental class to the fundamental class of the boundary in that orientation: .
(.) The long exact homology sequence of the pair is exact at , so the image of equals the kernel of . By step 1.1 the class lies in that image, hence .
(Vanishing of all evaluations.) Let . Naturality of the Kronecker pairing gives by step 2.1 and additivity of the pairing.
(Degenerate cases and assembly.) If then , the fundamental class is the zero class of , and both assertions hold. If the formula of step 2.1 is the statement that the signed count of the boundary points of a compact oriented one-manifold is zero in , which is exactly followed by exactness; the earlier steps cover this case without change, as they make no positive-dimensional hypothesis. Disconnected reduces to the connected case: the finitely many components of are compact -oriented manifolds with boundary , the induced boundary orientation of each is the one induced by , and by the componentwise description of the relative and absolute fundamental classes the boundary class is the finite sum of the images of the classes under the inclusions; hence the vanishing proved on each component, together with additivity of and of the pairing, gives the assertion for . For the induced boundary orientation of the canonical mod-two orientation is the canonical mod-two orientation of , since over each component carries a unique orientation; [F4] and [F5] record the choice-freeness and compactness facts used for this case. No step used a choice principle: the relative fundamental class is unique, exactness and naturality are algebraic, and is already given as the boundary of .
Zero-dimensional bordism groups
Statement
, generated by the class of a one-point manifold, the invariant being the parity of the cardinality of a finite set of points; and , via the isomorphism that sends a positively oriented point to and a negatively oriented point to , with generator the positively oriented point. In particular a compact zero-manifold bounds a compact one-manifold exactly when its signed count is zero in the oriented theory, and exactly when its cardinality is even in the unoriented theory (Unoriented and oriented bordism groups, Null-cobordant closed manifolds). The proof is choice-free; it does not use the classification of compact one-manifolds.
Facts & Assumptions
Given: Closed zero-manifolds, i.e. finite sets of points with the discrete topology, oriented in the oriented theory; compact smooth one-manifolds with boundary, their path components, and the bordism classes of -manifolds in and .
For a compact -oriented -manifold with boundary , the fundamental class of the induced boundary orientation pushes forward to zero: in ; for the canonical mod-two orientation applies to every compact smooth manifold, and no AC is used (The fundamental class of a boundary pushes forward to zero, Every manifold is F2-orientable and orientability is componentwise, Fundamental class of a compact oriented manifold).
For every topological space , is free on the path components, with the class of any point of (Zero-th singular homology is free on path components).
An oriented bordism from to has induced boundary orientations on and on ; the fundamental class is additive over disjoint unions of components, and a closed oriented manifold diffeomorphic to is null-cobordant exactly when its class in the bordism group is zero (Oriented smooth cobordism, Null-cobordant closed manifolds, Induced boundary orientation, Fundamental class of a compact oriented manifold).
and are abelian groups under disjoint union with the class of the empty manifold as zero, a class is zero exactly when its representative is null-cobordant, and a bijective additive map of groups is an isomorphism (Disjoint union makes bordism classes abelian groups, Monoid homomorphism and group homomorphism, Group isomorphisms, automorphisms and the set ).
The closed ball is a compact smooth one-manifold with boundary by the half-space chart construction from the nonzero derivative of at the endpoints (The Euclidean inverse function theorem, Euclidean upper half-space and its boundary, Smooth charts, atlases, and structures with boundary, Boundary-defining functions, Euclidean spaces and Euclidean open subsets as smooth manifolds), and on an oriented interval the induced boundary orientation is (Boundary orientation is independent of the outward vector field, Induced boundary orientation).
Finitely many selections can be made without AC, and products of smooth manifolds carry product structures with the product boundary conventions (Every natural-number-indexed list of nonempty sets has a choice function on its family of values, Products of smooth manifolds have a canonical product smooth structure, Product orientations, Boundary orientation of a product with at most one boundary factor).
Proof
(The zeroth homology of a compact one-manifold, and the evaluation of the pushforward.) Let be a compact smooth one-manifold and let be or . By [F2] the group is free on the path components with generators , the classes of single points; for the same description holds: the augmentation that sums the coefficients of a -chain over each path component is surjective, and its kernel is exactly the image of , because every singular -simplex has its two endpoints in a single path component (so its boundary has componentwise coefficient sum ), while a finite -chain with componentwise sums is a finite sum of terms with in the same component, each of which is the boundary of a singular -simplex along a path from to ; the finitely many paths and basepoints are selected by finite choice [F6]. Consequently , and for a finite set with coefficients , the pushforward is .
(Invariance of the signed count.) Let be an oriented bordism from to between closed oriented -manifolds, and let be the signed count. The induced boundary orientation on is , so the boundary fundamental class is the sum of the classes of the points of with signs and of with signs . By [F1] with and step 1.1, gives for every path component of that the signed number of boundary points lying in is , and summing over gives . Hence is unchanged by oriented cobordism and descends to a map .
(Invariance of the parity.) Let be a bordism from to between closed (unoriented) -manifolds. Use the canonical mod-two orientation of and of its boundary ([F1] with ). By [F1] and step 1.1 over , every path component of contains an even number of boundary points, so the cardinality of is even; hence , and the parity descends to a map .
(Completeness: vanishing invariant implies null-cobordant.) (i) Let be a finite set of points of even cardinality. By [F6] pair the points of ; for each pair use a copy of , affinely diffeomorphic to , identify with and with , and give its whole boundary the collar , for ; the images and are disjoint open neighbourhoods of the endpoints; then is a compact smooth one-manifold whose whole boundary is , so the disjoint union over the pairs is a compact one-manifold with boundary . Hence is null-cobordant. (ii) Let be a finite oriented point set with signed count . Then the number of positively oriented points equals the number of negatively oriented points; by [F6] pair each positive point with a negative point . On the interval with its standard orientation, the collars and for , with disjoint images and , exhibit the whole boundary as the incoming part and induce on it the orientation , that is, the negative of the orientation with positive and negative ([F5]). Hence each pair, and therefore all of , is null-cobordant. In both cases the construction uses finitely many intervals and no infinite selection.
(The isomorphisms and the bounding criterion.) The signed count is additive under disjoint union and , so it is a surjective homomorphism ; by step 2.1 it is well defined and by step 2.3 its kernel is zero, so it is injective and hence an isomorphism of abelian groups with generator the positively oriented point. The parity is additive under disjoint union and equals on a one-point manifold, so it is a surjective homomorphism ; it is well defined by step 2.2, and step 2.3(i) makes its kernel zero, so it is an isomorphism with generator the class of a point. Finally, a compact zero-manifold bounds a compact one-manifold if and only if it is null-cobordant, which by [F3] and [F4] happens exactly when its invariant vanishes: the signed count is in the oriented theory, and the cardinality is even in the unoriented theory. The proof used only the boundary pushforward, the elementary description of , finitely many explicit intervals and finite choice, so it is choice-free and does not use the classification of compact one-manifolds.
Product boundary formula for oriented manifolds
Statement
Let and be compact oriented smooth manifolds with at most one of nonempty (the corner-free case), and give its product smooth structure (Products of smooth manifolds have a canonical product smooth structure) and product orientation (Product orientations). Then, up to a canonical orientation-preserving diffeomorphism (Diffeomorphisms and local diffeomorphisms of manifolds, Orientation-preserving parametrizations), the boundary with the outward-normal-first orientation (Induced boundary orientation) equals each summand carrying the product orientation of the induced boundary orientation of the factor and the supplied orientation of the other factor. In the unoriented theory the same identity of smooth manifolds with boundary holds without signs. If both factors are closed then is closed. The case where both boundaries are nonempty produces corners at and is excluded.
Facts & Assumptions
Given: Compact oriented smooth manifolds and with at most one of nonempty, and the product with its product smooth structure and product orientation.
If then carries the product boundary orientation; if then carries times the product orientation (Boundary orientation of a product with at most one boundary factor).
The boundaryless product atlas is Products of smooth manifolds have a canonical product smooth structure. When exactly one factor has boundary, products of its half-space charts with Euclidean charts of the other factor, followed by a coordinate permutation placing the boundary coordinate last, give half-space charts of the product. Transitions and their inverses extend smoothly as products of the extensions in the factors (Smooth charts, atlases, and structures with boundary). Product bases give second countability and product separation gives Hausdorffness, exactly as in the boundaryless proof. The product orientation is the ordered tensor product of determinant rays (Product orientations), and boundary orientation is outward-normal-first (Induced boundary orientation).
A finite product of compact spaces is compact, with no choice beyond finite choice (A product of finitely many compact spaces is compact in the product topology, Open cover, subcover, and compact topological space; a compact subset is a subspace that is compact in its own right).
Proof
(Case .) If , the first clause of [F1] with states that equals and carries the product boundary orientation: the induced boundary orientation on first, then the orientation of . In this case , so the displayed formula has a single summand, with sign as the first summand, and the identification is the canonical projection diffeomorphism.
(Case .) If , the second clause of [F1] with states that equals and carries times the product orientation, namely times (orientation of )(induced boundary orientation of ). In this case , so this is the second summand of the display.
(Both factors closed.) If and , then is a product of compact spaces, hence compact by [F3], and its boundary is empty; a compact smooth manifold with empty boundary is closed, so is closed and both summands of the display are empty.
(Unoriented theory.) The identifications of steps 1.1 and 1.2 are diffeomorphisms of the underlying smooth manifolds and do not depend on the orientations: the projection (when ) and (when ) are canonical diffeomorphisms, and reading them in the unoriented theory gives the same disjoint-union identity without the sign .
(Assembly and the excluded corner case.) In the two corner-free cases steps 1.1 and 1.2 identify the boundary with the two summands of the display with the stated orientations, and step 1.3 covers the closed case; step 1.4 covers the unoriented theory. If both boundaries are nonempty, then near a point of the space is locally a product of two half-spaces, a quadrant with a corner, and is not a smooth manifold with boundary in the sense fixed on this page; the formula is therefore asserted only in the corner-free case, exactly as stated.
Cartesian product makes bordism a graded ring
Statement
For both theories set . This is a well-defined biadditive associative product distributing over disjoint union, and the class of a one-point manifold (positively oriented in the oriented theory) is a two-sided unit. Hence is a nonnegatively graded commutative ring (Nonnegatively graded rings and modules, homogeneous elements, and twists, Commutative ring) with unit , and carries an associative, biadditive, unital product with the same unit (Unoriented and oriented bordism groups, Disjoint union makes bordism classes abelian groups).
In the oriented theory the product is graded-commutative: the canonical transposition diffeomorphism has orientation sign for , , so the Koszul sign rule; in the unoriented theory the product is commutative. The forgetful map is a ring homomorphism. No choice principle is used.
Facts & Assumptions
Given: Closed smooth manifolds of dimensions , closed oriented manifolds in the oriented theory, and their bordism classes.
If is a bordism from to and a bordism from to , the collar gluing yields a bordism from to , and in the oriented case the orientations glue when the induced orientations on the common component are opposite (Collar gluing and seam smoothing give transitivity).
Products of smooth manifolds carry the product smooth structure and the product orientation; if one factor is closed the boundary of the product is the product of the other factor's boundary with that closed factor, with the corner-free signs of the product-boundary formula (Products of smooth manifolds have a canonical product smooth structure, Product orientations, Product boundary formula for oriented manifolds, Induced boundary orientation).
The cylinder with its product collars is a bordism from to , and the product orientation makes it an oriented bordism from to (Cylinders give reflexivity of cobordism).
Disjoint union makes the bordism classes abelian groups with ; canonical bijections of finite disjoint unions that fix or permute summands are diffeomorphisms preserving the disjoint-union orientations, and diffeomorphic closed manifolds have equal unoriented classes, while orientation-preserving diffeomorphic closed oriented manifolds have equal oriented classes (Disjoint union makes bordism classes abelian groups, Countable disjoint unions of fixed-dimensional smooth manifolds are smooth manifolds, A map from a disjoint union is smooth iff each restriction is smooth, Unoriented and oriented bordism groups, Null-cobordant closed manifolds).
A nonnegatively graded ring is a commutative ring with ; a ring homomorphism preserves addition, multiplication and unit (Nonnegatively graded rings and modules, homogeneous elements, and twists, Commutative ring, Ring homomorphism: additive, multiplicative, and required to send to ).
Proof
(The product is well defined.) Let be a bordism from to of dimension and a bordism from to of dimension . By [F2] the products and are compact smooth manifolds with boundary, with boundary decompositions and , and with the collars and onto the corresponding parts. In the oriented case orient by its product orientation and by times its product orientation. The first piece has incoming orientation and outgoing orientation . The product-boundary formula [F2] contributes a further to both faces of the second piece, cancelling its selected orientation factor; thus those faces carry and . In particular the two induced orientations at the common component are opposite, and the outer faces have the required incoming and outgoing product orientations. Gluing along the common collars by [F1] gives a bordism from to , oriented when both given bordisms are. Hence cobordant representatives give cobordant products: the product is well defined on in both theories.
(Diffeomorphisms give cobordisms.) If is a diffeomorphism of closed smooth -manifolds, then with the collars and is a bordism from to ; if is orientation-preserving between and , the orientation of [F3] makes it an oriented bordism. Thus diffeomorphic closed manifolds represent the same class, and orientation-preserving diffeomorphic closed oriented manifolds represent the same oriented class.
(Biadditivity, associativity, distributivity, unit.) Let be closed -manifolds and a closed -manifold. The canonical diffeomorphism is orientation-preserving in the oriented theory, so by step 1.2 and [F4] ; the same argument in the second variable gives biadditivity (distributivity over disjoint union). The canonical diffeomorphism is orientation-preserving for the iterated product orientations and gives . Let carry the positive sign in the oriented theory. Then and as smooth (oriented) manifolds, so ; the product is graded in the sense .
(Graded commutativity; the unoriented commutative case.) Let , , be the transposition. Its differential interchanges the tangent directions of the first block with the of the second, so it multiplies the ordered determinant by the sign of that permutation, which is : is orientation-preserving from to . By step 1.2 the two oriented classes agree, so in . In the unoriented theory is a diffeomorphism, so and the product is commutative on the nose.
(Ring structure and the forgetful map.) By steps 2.1 and 2.2 the direct sum is a nonnegatively graded commutative ring with unit in the sense of [F5], and is a graded-commutative ring with the same unit and the Koszul sign rule; associativity, biadditivity, distributivity over the group operation, the grading and the unit are the assertions proved in step 2.1, and the commutativity statements are step 2.2. The forgetful map sends to and to the underlying class of , which is , and it preserves the unit; hence it is a ring homomorphism by [F5]. Everything is built from products of manifolds and supplied collars, so no choice principle is used.
Stiefel-Whitney numbers of a closed manifold
Definition
Assume AC (The Axiom of Choice). The assumption is inherited from the Stiefel-Whitney class construction and is used only there, through Stiefel–Whitney classes from the projective-bundle relation and the admissibility supplied by Smooth manifolds have CW homotopy type.
Let be a closed smooth -manifold (Smooth manifolds and their smooth charts), with tangent Stiefel-Whitney classes so that and for . Its canonical mod-two fundamental class is the fundamental class of the canonical -orientation (Every manifold is F2-orientable and orientability is componentwise), in the sense of Fundamental class of a compact oriented manifold.
Consider a monomial in the tangent classes, with non-negative exponents and total degree . If the total degree equals , the associated Stiefel-Whitney number of is the Kronecker evaluation (Kronecker evaluation pairing). A monomial of formal total degree defines a class in by the graded cup product. Its formal degree is determined by the exponents, even when that class vanishes; membership of the zero class in a homogeneous summand does not determine the formal degree. Monomials of formal total degree different from are assigned the value by convention. The Stiefel-Whitney numbers of are the values attached to all monomials of total degree . The evaluation is well defined on cohomology and homology classes by The kronecker pairing is independent of cocycle and cycle representatives.
Connected case. If is connected, then is path-connected: a manifold is locally path-connected (Topological manifolds are locally compact and locally path connected) and a connected locally path-connected space is path-connected (A connected, locally path-connected space is path-connected, because its path components are open). Hence is an admissible base and is a numerable smooth finite-rank real bundle (Smooth manifolds have CW homotopy type), so the classes are those of the Stiefel-Whitney class construction; for the rank-zero conventions , () are used. In particular the monomial of degree on a -manifold is the empty product , and is the parity of the cardinality of in .
General closed manifolds. Let be an arbitrary closed smooth -manifold. By the componentwise statement for compact manifolds, has finitely many connected components (Every manifold is F2-orientable and orientability is componentwise); each component is open (Components of a topological manifold are open and at most countable) and closed in the compact , hence compact, and open components carry the restricted smooth structure (An open subset of a smooth manifold has a canonical restricted smooth structure). Each is a closed smooth -manifold, and its canonical mod-two orientation is the restriction of the canonical orientation of . The definition of the number is extended to by the componentwise sum the sum of the componentwise Stiefel-Whitney numbers; for connected this is exactly the single evaluation displayed above.
The definitions are independent of all choices: the tangent bundle is determined by the smooth structure, its Stiefel-Whitney classes are determined by the bundle up to isomorphism (Naturality of Stiefel–Whitney classes), the canonical mod-two fundamental class is determined by the canonical mod-two orientation, and the pairing descends through both quotients. No orientation of is needed or used, and the numbers do not change when an orientation is supplied or reversed.
Behaviour under diffeomorphisms. Let be a diffeomorphism of closed smooth -manifolds (Diffeomorphisms and local diffeomorphisms of manifolds). Assume first that and are connected. The differential of identifies with the pullback , so naturality of Stiefel-Whitney classes gives , hence (Naturality of Stiefel–Whitney classes). The pushforward restricts at every to the image under of the canonical local generator at ; that local module is , so its unique nonzero element is carried to the unique nonzero element at , which is the canonical local generator there. By the characterisation of the fundamental class through its pointwise restrictions (Fundamental class of a compact oriented manifold) this gives . Naturality of the Kronecker pairing (The kronecker pairing is independent of cocycle and cycle representatives) therefore yields . For disconnected and the argument applies to each component and the componentwise sums agree; thus the Stiefel-Whitney numbers are invariants of diffeomorphism. No choice beyond the AC stated above is used.
Pontryagin numbers of a closed oriented manifold
Definition
Assume AC (The Axiom of Choice). The assumption is inherited from the Pontryagin class construction and is used only there, through Pontryagin classes by complexification its CW-type transport below, and the admissibility supplied by Smooth manifolds have CW homotopy type.
Let be a closed oriented smooth manifold of dimension for an integer , with orientation . Its fundamental class is the class determined by (Fundamental class of a compact oriented manifold). Its tangent Pontryagin classes, taken componentwise when is disconnected, are with the conventions and whenever .
Connected case. If is connected, then is path-connected: a manifold is locally path-connected (Topological manifolds are locally compact and locally path connected) and a connected locally path-connected space is path-connected (A connected, locally path-connected space is path-connected, because its path components are open). Hence is an admissible base for the characteristic-class construction: it is paracompact Hausdorff of CW homotopy type and its tangent bundle is a numerable smooth finite-rank real bundle (Smooth manifolds have CW homotopy type). For a partition of with (for the empty partition, with empty product ), the -th Pontryagin number of is the Kronecker evaluation of the cup product of the tangent Pontryagin classes on the fundamental class (Kronecker evaluation pairing); the value is well defined on cohomology and homology classes by The kronecker pairing is independent of cocycle and cycle representatives.
General closed oriented manifolds. Let be an arbitrary closed oriented manifold of dimension . By the componentwise statement for compact manifolds, has finitely many connected components ; each component is open (Components of a topological manifold are open and at most countable) and closed in the compact , hence compact, carries the restricted smooth structure as an open submanifold (An open subset of a smooth manifold has a canonical restricted smooth structure), and carries the orientation restricted to it; the family of these restricted orientations is the componentwise orientation of (Every manifold is F2-orientable and orientability is componentwise). Each is a closed oriented smooth -manifold and the connected case above applies. We set the sum of the componentwise Pontryagin numbers; for connected this is exactly the single evaluation displayed above. A manifold whose dimension is not is assigned the value by convention, and for a partition with never sees a class of index beyond the dimension.
The definition is independent of all choices: the complexification of is determined up to canonical isomorphism, so the even Chern classes, hence the classes , are determined; the fundamental class is determined by the orientation; and the Kronecker pairing descends through both quotients. The classes do not depend on the orientation. Replacing by negates the fundamental class on every component (Fundamental class of a compact oriented manifold) and therefore negates every Pontryagin number, by linearity of the pairing in its second variable (The kronecker pairing is independent of cocycle and cycle representatives).
Naturality and stability on CW-type bases. The cited Pontryagin theorem is stated for path-connected CW complexes, whereas smooth manifolds here are only known to have CW homotopy type. The needed extension is as follows. For a numerable complex bundle over a path-connected paracompact Hausdorff CGWH base of CW type, choose homotopy inverse maps and with a path-connected CW complex. Homotopy invariance of bundle pullback gives (Homotopy invariance of vector-bundle pullback). The Chern naturality theorem permits a CW-type source and a CW target, so (Naturality, normalization, and Whitney sum for Chern classes, Chern classes from the projective-bundle relation). For between such bases, , so the same theorem with target gives . Also ; Chern stability on and naturality along give . Complexification commutes with pullback and adjoining trivial summands, as seen from their transition matrices. The formula therefore proves naturality and stability of Pontryagin classes on these CW-type bases too. For a finite disjoint union define the classes componentwise: every singular simplex lies in one component, so cohomology is the finite product of the component rings, with pullbacks and cup products computed componentwise. This also handles maps whose different source components land in the same target component. For the empty base all classes and evaluations have their unique zero values. AC is inherited by this transport from the stated bundle-homotopy and characteristic-class suppliers.
Behaviour under diffeomorphisms. Let be a diffeomorphism of closed oriented -manifolds (Diffeomorphisms and local diffeomorphisms of manifolds). Assume first that and are connected and that is orientation-preserving (Orientation-preserving parametrizations). The differential of identifies with the pullback , so naturality of Pontryagin classes gives (by the CW-type derivation above). The pushforward restricts at every to the image under of the local generator of at , which is the local generator of at because is orientation-preserving; by the characterisation of the fundamental class through its pointwise restrictions (Fundamental class of a compact oriented manifold) this means . Naturality of the Kronecker pairing (The kronecker pairing is independent of cocycle and cycle representatives) therefore gives If is orientation-reversing, the same computation gives local generators that are negatives of those of , so and . For disconnected and the argument applies to each component, and the sum of the componentwise numbers transforms accordingly. In particular a nonzero Pontryagin number obstructs the existence of an orientation-reversing self-diffeomorphism. No choice beyond the AC stated above is used.
The boundary stable tangent bundle splits off a trivial line
Statement
Assume (The Axiom of Countable Choice ()), used exactly through the global inward vector field of A global inward-pointing boundary vector field exists. Let be a smooth manifold with boundary (Smooth maps between manifolds with boundary), let be the inclusion, which is a closed embedding of a smooth -manifold (The boundary of a positive-dimensional manifold is a closed embedded smooth (n-1)-manifold), and let be a smooth vector field on a neighbourhood of in that is inward at every point of (Inward, outward, and boundary-tangent vectors).
Then the map is an isomorphism of smooth real vector bundles over (Whitney sum, tensor, dual, Hom, and exterior-power bundles, Pullback vector bundles and sections). Consequently and the normal line is trivial. Since supplies such an for every smooth manifold with boundary, the splitting holds for every smooth manifold with boundary. In particular the stabilization of by one trivial line is identified with the restriction ; this is the identification used by the characteristic number propositions of this page.
Facts & Assumptions
Given: A smooth manifold with boundary , the inclusion , a neighbourhood of carrying a smooth vector field inward along , and the map , . Countable choice is assumed (The Axiom of Countable Choice ()).
A vector at is inward when its last coordinate in a boundary chart is positive, outward when negative, and boundary-tangent when zero; the alternatives are chart independent (Inward, outward, and boundary-tangent vectors).
For the differential identifies with the boundary-tangent hyperplane of (The boundary tangent space is the boundary-tangent hyperplane).
Here denotes the pullback , not restriction to an open subset (Pullback vector bundles and sections). In a boundary chart, the tangent-bundle trivialization restricts to its face and the bundle transitions are the ambient tangent transitions restricted to that face; they are smooth, so this gives a smooth bundle over (Tangent and cotangent bundles extend over a boundary). The inclusion differential and restricted section are smooth in these charts. With the Whitney sum and trivial line bundle, is therefore a smooth fibrewise-linear bundle map (Whitney sum, tensor, dual, Hom, and exterior-power bundles, Smooth vector bundles, rank, fibres, and trivial bundles).
A smooth vector bundle map over a diffeomorphism whose fibre maps are bijective is a vector bundle isomorphism (A fibrewise bijective smooth bundle map over a diffeomorphism is a bundle isomorphism).
Assuming , every smooth manifold with boundary admits a smooth vector field on a neighbourhood of its boundary that is inward at every boundary point (A global inward-pointing boundary vector field exists).
Proof
( is a smooth bundle map.) The differential is a smooth bundle map and is a smooth section by [F3], and the trivial line bundle is smooth; forming sums and scalar multiples fibrewise, is a smooth map of total spaces whose restriction to each fibre is linear and whose base map is the identity.
(Fibrewise bijectivity.) Fix . By [F2], is injective with image the boundary-tangent hyperplane , a linear subspace of dimension . By [F1], is inward at , so its last boundary-chart coordinate is positive and ; in particular , since elements of have last coordinate zero. Hence , and gives . Therefore , , is a linear isomorphism.
( is a bundle isomorphism.) The base map of is the identity, a diffeomorphism, and by step 1.2 every fibre map is bijective; step 1.1 makes a smooth bundle map. By [F4], is an isomorphism of smooth vector bundles. Hence . Moreover carries the subbundle isomorphically onto a line subbundle complementary to ; composing with the quotient projection identifies with , so the normal line is trivial and is spanned by .
(Every manifold with boundary; assembly.) Let be an arbitrary smooth manifold with boundary. By [F5] there is, under , a smooth vector field on a neighbourhood of inward at every boundary point, and steps 1.1–2.1 apply to it; hence for every smooth manifold with boundary . Applied to this is the asserted splitting, and it identifies the stabilization of by one trivial line with . The argument used only in the selection of the inward field in [F5]; no other choice is made.
Boundaries have zero Stiefel-Whitney numbers
Statement
Assume AC (The Axiom of Choice), used only through the Stiefel-Whitney class construction, its admissibility input, and the inward field used in the boundary tangent splitting (which requires ). Let be a closed smooth -manifold that is the boundary of a compact smooth -manifold , with canonical mod-two fundamental class (Stiefel-Whitney numbers of a closed manifold) and inclusion . Then for every monomial of total degree . Hence every Stiefel-Whitney number of a closed boundary vanishes, and a closed manifold with at least one nonzero Stiefel-Whitney number is not null-cobordant (Null-cobordant closed manifolds).
Facts & Assumptions
Given: A closed smooth -manifold that is the boundary of a compact smooth -manifold , its inclusion , and the monomials of total degree in the tangent classes of . AC is assumed.
The restriction of the tangent bundle of to the boundary splits off a trivial line: , under , which follows from AC (The boundary stable tangent bundle splits off a trivial line, The Axiom of Choice).
Stiefel-Whitney classes are natural, , and satisfy the Whitney sum formula with stability for trivial summands, ; the construction applies to because a closed smooth manifold is a paracompact Hausdorff CGWH base of CW homotopy type with numerable tangent bundle (Naturality of Stiefel–Whitney classes, Whitney sum formula for Stiefel–Whitney classes, Stiefel–Whitney classes from the projective-bundle relation, Smooth manifolds have CW homotopy type).
The Kronecker pairing is natural: , and is additive (Kronecker evaluation pairing, The kronecker pairing is independent of cocycle and cycle representatives).
The fundamental class of the boundary pushes forward to zero: in , where is the fundamental class of the canonical mod-two orientation (The fundamental class of a boundary pushes forward to zero, Every manifold is F2-orientable and orientability is componentwise, Fundamental class of a compact oriented manifold).
A Stiefel-Whitney number of a closed smooth -manifold is the evaluation of a degree- monomial, it is a diffeomorphism invariant, and is null-cobordant exactly when is diffeomorphic to the whole boundary of a compact smooth -manifold (Stiefel-Whitney numbers of a closed manifold, Null-cobordant closed manifolds).
Proof
(The tangent classes of are restrictions from .) By [F1], . Applying naturality and the Whitney sum formula with the trivial summand from [F2] gives and hence for every monomial.
(The evaluations vanish.) For a degree- monomial , naturality of the Kronecker pairing [F3] and the vanishing of the boundary pushforward [F4] give
(All numbers vanish; null-cobordism consequence.) Since the monomial of total degree was arbitrary, every Stiefel-Whitney number of the closed boundary vanishes. If a closed smooth -manifold is null-cobordant, then by [F5] it is diffeomorphic to the whole boundary of some compact smooth -manifold, and diffeomorphism invariance of the numbers transfers the vanishing to . Contrapositively, a closed manifold with at least one nonzero Stiefel-Whitney number is not null-cobordant.
Oriented boundaries have zero Pontryagin numbers
Statement
Assume AC (The Axiom of Choice), used only through the Pontryagin class construction, CW-type transport, admissibility input, and the inward field used in the boundary tangent splitting (which requires ). Let be a closed oriented smooth -manifold that is the boundary of a compact oriented smooth -manifold , in the orientation convention of the null-cobordism definition (Null-cobordant closed manifolds), with fundamental class and inclusion . Then for every partition of . Hence a closed oriented -manifold with a nonzero Pontryagin number is not an oriented boundary. The proof uses neither the signature nor the Hirzebruch signature theorem.
Facts & Assumptions
Given: A closed oriented smooth -manifold occurring as an oriented boundary of a compact oriented -manifold , the inclusion , and the partitions of . AC is assumed.
; the splitting is available under , which AC implies (The boundary stable tangent bundle splits off a trivial line, The Axiom of Choice).
On path-connected CW complexes, Pontryagin classes are natural and stable (Naturality, stability, and mod-two reduction of Pontryagin classes). The paragraph “Naturality and stability on CW-type bases” in Pontryagin numbers of a closed oriented manifold derives the same identities for admissible CW-type bases and finite disjoint unions. Both and are admissible smooth bases with numerable tangent bundles under AC (Smooth manifolds have CW homotopy type). Thus and apply here, including disconnected and empty cases.
The integral Kronecker pairing is natural and additive: (Kronecker evaluation pairing, The kronecker pairing is independent of cocycle and cycle representatives).
For the induced boundary orientation, whose fundamental class is the negative of by the null-cobordism convention, the boundary pushforward vanishes: in (The fundamental class of a boundary pushes forward to zero, Fundamental class of a compact oriented manifold, Null-cobordant closed manifolds).
The Pontryagin numbers are defined by for partitions of (Pontryagin numbers of a closed oriented manifold).
Proof
(The Pontryagin classes of are restrictions from .) By [F1] and stability in [F2], so for every partition.
(The evaluations vanish.) Let be a partition of . Naturality of the integral Kronecker pairing [F3], step 1.1, and the vanishing pushforward [F4] give the last step because , which follows from [F4] and linearity of .
(All numbers vanish; the boundary obstruction.) Since the partition of was arbitrary, every Pontryagin number of the closed oriented boundary vanishes. Contrapositively, if a closed oriented -manifold has some nonzero Pontryagin number, it cannot occur as such a boundary. The argument uses only the class naturality and stability, the Kronecker naturality and the boundary pushforward; neither the signature nor the Hirzebruch signature theorem is used.
Bordism groups here are geometric, not generalized homology constructions
Remark
The sets and defined on this page are geometric: their elements are bordism classes of closed smooth manifolds, their operation is disjoint union, and their product (taken up later on this page) is the Cartesian product of manifolds (Unoriented and oriented bordism groups). Every construction on this page is a statement about manifolds, bordisms and their boundary data.
This page constructs no Thom spectrum, no ring spectrum and no generalized homology theory, and it asserts no excision, suspension or Mayer-Vietoris property for bordism. In particular the identification of these groups with stable homotopy groups of Thom spectra, for instance together with the Pontryagin-Thom construction, the Thom transversality theorem and the bordism homology axioms, belongs to algebraic topology and to later pages of this library; the cited sources prove those statements, but nothing here depends on them. The remark fixes the seam so that consumers do not read a spectrum-level or homology-theoretic claim into the geometric definitions of this page.
5 · Examples, counterexamples and false statements
None yet.
Sources
- Daniel S. Freed, Bordism: Old and New (lecture notes, UT Austin, Fall 2012)
- C. T. C. Wall, Differential Topology (Cambridge Studies in Advanced Mathematics 156, 2016)
- John Milnor and James Stasheff, Characteristic Classes (original pagination)
- Andrew Ranicki, Algebraic and Geometric Surgery (Oxford Mathematical Monographs, 2002)