nLab Rokhlin's theorem

Context

Differential geometry

synthetic differential geometry

Introductions

from point-set topology to differentiable manifolds

geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry

Differentials

V-manifolds

smooth space

Tangency

The magic algebraic facts

Theorems

Axiomatics

cohesion

infinitesimal cohesion

tangent cohesion

differential cohesion

graded differential cohesion

singular cohesion

id id fermionic bosonic bosonic Rh rheonomic reduced infinitesimal infinitesimal & étale cohesive ʃ discrete discrete continuous * \array{ && id &\dashv& id \\ && \vee && \vee \\ &\stackrel{fermionic}{}& \rightrightarrows &\dashv& \rightsquigarrow & \stackrel{bosonic}{} \\ && \bot && \bot \\ &\stackrel{bosonic}{} & \rightsquigarrow &\dashv& \mathrm{R}\!\!\mathrm{h} & \stackrel{rheonomic}{} \\ && \vee && \vee \\ &\stackrel{reduced}{} & \Re &\dashv& \Im & \stackrel{infinitesimal}{} \\ && \bot && \bot \\ &\stackrel{infinitesimal}{}& \Im &\dashv& \& & \stackrel{\text{étale}}{} \\ && \vee && \vee \\ &\stackrel{cohesive}{}& \esh &\dashv& \flat & \stackrel{discrete}{} \\ && \bot && \bot \\ &\stackrel{discrete}{}& \flat &\dashv& \sharp & \stackrel{continuous}{} \\ && \vee && \vee \\ && \emptyset &\dashv& \ast }

Models

Lie theory, ∞-Lie theory

differential equations, variational calculus

Chern-Weil theory, ∞-Chern-Weil theory

Cartan geometry (super, higher)

Manifolds and cobordisms

Contents

Idea

Rokhlin’s theorem states that the signature of a smooth orientable closed spin 4-manifold is divisible by 1616. It therefore serves as an obstruction for the existence of smooth structures. A famous example is the E₈ manifold with intersection form the E₈ lattice and therefore signature 88. Since it is an orientable closed spin 4-manifold, Rokhlin’s theorem states that it cannot carry a smooth structure.

Formulation

For a smooth orientable closed spin 4-manifold MM, hence with vanishing second Stiefel-Whitney class w 2(M)=0w_2(M)=0, one has:

σ(M)0mod16. \sigma(M) \equiv 0 mod 16.

Generalizations

Kervaire-Milnor theorem

Proposition

(Kervaire-Milnor theorem) For a smooth compact 4-manifold MM and a characteristic sphere S 2MS^2\hookrightarrow M, one has:

σ(M)=S 2S 2mod16. \sigma(M) =S^2\cdot S^2 mod 16.

A characteristic sphere i:S 2Mi\colon S^2\hookrightarrow M represents the second Stiefel-Whitney class w 2(TM)=PD(i *[S 2])H 2(M, 2)w_2(TM)=PD(i_*[S^2])\in H^2(M,\mathbb{Z}_2) using Poincaré duality PD:H 2(M, 2)H 2(M, 2)PD\colon H_2(M,\mathbb{Z}_2)\rightarrow H^2(M,\mathbb{Z}_2) and the fundamental class [S 2]H 2(S 2, 2) 2[S^2]\in H_2(S^2,\mathbb{Z}_2)\cong\mathbb{Z}_2, which is the unique generator.

Freedman-Kirby theorem

Proposition

(Smooth Freedman-Kirby theorem) For a smooth compact 4-manifold MM and a characteristic surface ΣM\Sigma\hookrightarrow M, one has:

σ(M)=ΣΣ+8Arf(M,Σ)mod16 \sigma(M) =\Sigma\cdot\Sigma +8 Arf(M,\Sigma) mod 16

with the Arf invariant.

A characteristic surface i:ΣMi\colon\Sigma\hookrightarrow M represents the second Stiefel-Whitney class w 2(TM)=PD(i *[Σ])H 2(M, 2)w_2(TM)=PD(i_*[\Sigma])\in H^2(M,\mathbb{Z}_2) using Poincaré duality PD:H 2(M, 2)H 2(M, 2)PD\colon H_2(M,\mathbb{Z}_2)\rightarrow H^2(M,\mathbb{Z}_2) and the fundamental class [Σ]H 2(Σ, 2) 2[\Sigma]\in H_2(\Sigma,\mathbb{Z}_2)\cong\mathbb{Z}_2, which is the unique generator.
Proposition

(Topological Freedman-Kirby theorem) For a topological compact 4-manifold MM and a characteristic surface ΣM\Sigma\hookrightarrow M, one has:

σ(M)=ΣΣ+8Arf(M,Σ)+8KS(M)mod16 \sigma(M) =\Sigma\cdot\Sigma +8 Arf(M,\Sigma) +8 KS(M) mod 16

with the Arf invariant and Kirby-Siebenmann invariant.

References

See also:

Created on April 23, 2026 at 18:07:11. See the history of this page for a list of all contributions to it.