nLab Rokhlin 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 ℜ ⊣ ℑ infinitesimal ⊥ ⊥ infinitesimal ℑ ⊣ & 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 2↪MS^2\hookrightarrow M, one has:

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

A characteristic sphere i:S 2↪Mi\colon S^2\hookrightarrow M represents the second Stiefel-Whitney class w 2(TM)=PD(i *[S 2])∈H 2(M,ℤ 2)w_2(TM)=PD(i_*[S^2])\in H^2(M,\mathbb{Z}_2) using Poincaré duality PD:H 2(M,ℤ 2)→H 2(M,ℤ 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,ℤ 2)≅ℤ 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 Σ↪M\Sigma\hookrightarrow M, one has:

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

with the Arf invariant.

A characteristic surface i:Σ↪Mi\colon\Sigma\hookrightarrow M represents the second Stiefel-Whitney class w 2(TM)=PD(i *[Σ])∈H 2(M,ℤ 2)w_2(TM)=PD(i_*[\Sigma])\in H^2(M,\mathbb{Z}_2) using Poincaré duality PD:H 2(M,ℤ 2)→H 2(M,ℤ 2)PD\colon H_2(M,\mathbb{Z}_2)\rightarrow H^2(M,\mathbb{Z}_2) and the fundamental class [Σ]∈H 2(Σ,ℤ 2)≅ℤ 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 Σ↪M\Sigma\hookrightarrow M, one has:

σ(M)=Σ⋅Σ+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.

Articles on geometry and topology of 4-manifolds:

References

See also:

Last revised on May 16, 2026 at 14:33:36. See the history of this page for a list of all contributions to it.