nLab Barlow surface

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)

Contents

Idea

The Barlow surface is a simply connected complex surface of general type that is homeomorphic (Barlow 1984) but not diffeomorphic (Kotschick 1989) to P 2#8P 2¯\mathbb{C}P^2\# 8\overline{\mathbb{C}P^2} (the eight-fold blow-up of the complex projective plane), and thus the first known example of an exotic smooth structure on this topological manifold.

While it is now established that the underlying topological manifold P 2#8P 2¯\mathbb{C}P^2\# 8\overline{\mathbb{C}P^2} admits countably infinitely many non-diffeomorphic smooth structures, these infinite families are generally constructed via later techniques (such as rational blowdowns or knot surgery) and are not themselves “Barlow surfaces”.

(For context, the topological manifold obtained by one further blow-up is P 2#9P 2¯\mathbb{C}P^2\# 9\overline{\mathbb{C}P^2}, which is the space famously underlying the Dolgachev surfaces.)

Description

Freedman's classification provides:

Proposition

Every simply connected oriented closed smooth 4-manifold with intersection form [1]8[+1][-1]\oplus 8[+1] is homeomorphic to P 2#8P 2¯\mathbb{C}P^2\# 8\overline{\mathbb{C}P^2}.

(Instead of smoothness, a vanishing Kirby-Siebenmann invariant is also sufficient.)

For example with the E₈ form E 8E_8, the intersection form of the E₈ manifold, one has E 8[+1][+1]8[1]-E_8\oplus[+1]\cong [+1]\oplus 8[-1] from Serre’s classification theorem, with Freedman's classification translating it into a homeomorphism:

M E 8¯#*P 2P 2#8P 2¯. \overline{M_{E_8}}\#*\mathbb{C}P^2 \cong\mathbb{C}P^2\# 8\overline{\mathbb{C}P^2}.

(*P 2*\mathbb{C}P^2 is the fake second complex projective space, which is required instead of the second complex projective space P 2\mathbb{C}P^2 to make the connected sum on the left side have vanishing Kirby-Siebenmann invariant like the right side.)

As another example with the hyperbolic form H=[0 1 1 0]H=\begin{bmatrix} 0 & 1 \\ 1 & 0 \end{bmatrix}, the intersection form of the complex surface S 2×S 2P 1×P 1S^2\times S^2\cong\mathbb{C}P^1\times\mathbb{C}P^1, one has H[1][+1]2[1]H\oplus[-1]\cong[+1]\oplus 2[-1] from Serre’s classification, with Freedman's classification translating it into a homeomorphism:

(S 2×S 2)#P 2¯P 2#2P 2¯. (S^2\times S^2)\#\overline{\mathbb{C}P^2} \cong\mathbb{C}P^2\# 2\overline{\mathbb{C}P^2}.

It can be shown that it’s even a diffeomorphism, hence further gives a diffeomorphism:

(S 2×S 2)#7P 2¯P 2#8P 2¯. (S^2\times S^2)\# 7\overline{\mathbb{C}P^2} \cong\mathbb{C}P^2\# 8\overline{\mathbb{C}P^2}.

Articles on geometry and topology of 4-manifolds:

References

See also:

Last revised on May 22, 2026 at 09:22:20. See the history of this page for a list of all contributions to it.