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The signature is independent of the diagonalizing basis and unchanged by scalar extension from the rationals to the reals
Statement
Assume AC, inherited from finite generation and the coefficient-duality suppliers. Let be a closed oriented smooth -manifold. (1) Any basis of diagonalizing has the same number of positive entries and the same number of negative entries, and equals the intrinsic inertia difference of ; in particular the definition The signature of a closed oriented manifold of dimension divisible by four is well posed. (2) With and , the inertia data of and of agree; more generally, scalar extension of a finite-dimensional symmetric bilinear form along an ordered-field extension preserves inertia, so the signatures computed over and over coincide.
Facts & Assumptions
Given: AC; a closed oriented smooth -manifold with middle form (over ) and its rational counterpart on .
on , and the inertia of a symmetric bilinear form is the triple of counts of positive, negative and zero diagonal entries in a diagonalizing basis, with signature (The middle-dimensional intersection form of a closed oriented 4k-manifold, Positive and negative definiteness, the inertia , rank , and signature of a real symmetric bilinear or quadratic form).
Every symmetric bilinear form on a finite-dimensional real vector space is congruent to exactly one normal form , and the counts are independent of the diagonalizing basis (Sylvester's law of inertia: every real symmetric form is congruent to , and is unique).
Two symmetric forms of the same finite dimension are congruent exactly when they have the same inertia (Two real symmetric bilinear forms are congruent if and only if they have the same inertia); every symmetric bilinear form over a field of characteristic not two has an orthogonal basis (Every symmetric bilinear form on a finite-dimensional space over a field of characteristic not has an orthogonal basis).
If is a subfield of the ordered field with the order induced from (Ordered field, Subfield: a subring of a field closed under inverses of its nonzero elements, and therefore a field with the restricted operations), then for the sign of is the same in and in , since the positive cone of is the restriction of that of ; and if is an -basis of , then is a -basis of , with the same diagonal entries for a diagonal form (The elementary tensors of two bases form the product basis of the tensor product).
For a closed oriented -manifold, and are finitely generated, and for a divisible coefficient group evaluation gives a natural isomorphism (Finite generation from cap with a finite fundamental cycle, Cohomology with a divisible abelian coefficient group is Hom of homology).
Every finitely generated abelian group is with finite, and for torsion-free one has and (The fundamental theorem of finitely generated abelian groups from PID modules).
The Kronecker pairing evaluates representatives and is natural in the cohomology variable under coefficient homomorphisms : ; the cup product is the coefficientwise front/back cochain formula, so it commutes with coefficient change (The kronecker pairing is independent of cocycle and cycle representatives, Kronecker evaluation pairing, Singular cup product on cochains).
The fundamental class is the unique class restricting to the prescribed local generator at every point; for the real orientation obtained from the integral one by coefficient change, the image of is , because coefficient change carries the integral local generator to the real one and preserves local restrictions (Fundamental class of a compact oriented manifold).
Proof
Let be a symmetric form on a finite-dimensional space over an ordered field , and let carry an extending order. By [F3] choose an orthogonal -basis with diagonal entries . Write for its positive, negative and zero coordinate subspaces, of dimensions . The radical is . A positive-definite subspace projects injectively to : a vector with zero positive coordinates has , so cannot be a nonzero vector in such a subspace. Rank-nullity and the subspace dimension bound (Rank-nullity: , If and is a linear subspace of , then is finite-dimensional, , and if and only if ) give dimension at most , attained by . Similarly the maximal negative dimension is . Thus is intrinsic over any ordered field. By [F4], the extended basis has the same diagonal entries and signs over , so these intrinsic dimensions, and hence the signature, are preserved.
Basis independence and well-posedness: by [F2] the diagonal entries' sign counts of any diagonalizing basis of are intrinsic to , and by [F3] congruent forms have equal inertia, so , are the same for every diagonalizing basis; since is symmetric and nondegenerate by The middle-dimensional intersection form is symmetric and nondegenerate, and is the intrinsic inertia difference of as claimed in The signature of a closed oriented manifold of dimension divisible by four.
Coefficient bridge: by [F5] applied with the divisible groups and , evaluation gives natural isomorphisms and . Writing with finite by [F6], both groups are and , and the map induced by the coefficient inclusion is the natural inclusion . Hence the natural map is an isomorphism .
Form compatibility: for , with images under coefficient change, . Indeed the cup product formula is coefficientwise by [F7], so is the coefficient-change image of ; the real fundamental class is the coefficient-change image of the integral one by [F8], and the Kronecker pairing is natural in coefficients by [F7]; evaluating the rational cup class on the integral fundamental class gives the rational number , whose image in is the real evaluation. Since the span over by step 1.3, the real form is the scalar extension of the rational one.
Inertia agreement: by step 2.1 the real form is the scalar extension of the rational form along , so step 1.1 gives that their inertia triples agree; in particular the signatures over and over coincide.
Steps 1.1 and 2.1 prove the basis-independence and well-posedness clause, and steps 1.1, 1.3 and 2.1 prove the scalar-extension clause for ; the general statement for arbitrary finite-dimensional symmetric forms over an ordered field is exactly step 1.1. If the vector space of the form is zero, its diagonal data are empty and its signature is . For a zero-manifold the middle group need not vanish; both coefficient fields give its signed point count.
Depends on
- If $\dim_F V = n$ and $U$ is a linear subspace of $V$, then $U$ is finite-dimensional, $\dim_F U \le n$, and $\dim_F U = n$ if and only if $U = V$
- Rank-nullity: $\dim_F V=\operatorname{nullity}T+\operatorname{rank}T$
- Subfield: a subring of a field closed under inverses of its nonzero elements, and therefore a field with the restricted operations
- Ordered field
- The elementary tensors of two bases form the product basis of the tensor product
- The middle-dimensional intersection form is symmetric and nondegenerate
- Cohomology with a divisible abelian coefficient group is Hom of homology
- The fundamental theorem of finitely generated abelian groups from PID modules
- Two real symmetric bilinear forms are congruent if and only if they have the same inertia
- The Axiom of Choice
- Bilinear forms, and symmetric, skew-symmetric, and alternating bilinear forms
- Positive and negative definiteness, the inertia $(p,q,r)$, rank $p+q$, and signature $p-q$ of a real symmetric bilinear or quadratic form
- Kronecker evaluation pairing
- The middle-dimensional intersection form of a closed oriented 4k-manifold
- The signature of a closed oriented manifold of dimension divisible by four
- Singular cup product on cochains
- Fundamental class of a compact oriented manifold
- Finite generation from cap with a finite fundamental cycle
- The kronecker pairing is independent of cocycle and cycle representatives
- Sylvester's law of inertia: every real symmetric form is congruent to $\operatorname{diag}(I_p,-I_q,0_r)$, and $(p,q,r)$ is unique
- Every symmetric bilinear form on a finite-dimensional space over a field of characteristic not $2$ has an orthogonal basis
Used by
Cited to discharge well-definedness by The signature of a closed oriented manifold of dimension divisible by four.
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Sources
- John Milnor and James Stasheff, Characteristic Classes (re-typeset scan; original pagination) (standard reference, not scraped)
- Daniel S. Freed, Bordism: Old and New (lecture notes, UT Austin, Fall 2012) (standard reference, not scraped)
- Tom Weston, An Introduction to Cobordism Theory (lecture notes, Stanford) (standard reference, not scraped)