nLab exotic 7-sphere

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synthetic differential geometry

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

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cohesion

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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 }

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Lie theory, ∞-Lie theory

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Spheres

Contents

Idea

A topological 7-sphere equipped with an exotic smooth structure is called an exotic 7-sphere.

Milnor’s construction

Milnor (1956) gave the first examples of exotic smooth structures on the 7-sphere, finding at least seven.

The exotic 7-spheres constructed in Milnor 1956 are all examples of fibre bundles over the 4-sphere S 4S^4 with fibre the 3-sphere S 3S^3, with structure group the special orthogonal group SO(4) (see also at 8-manifold the section With exotic boundary 7-spheres):

By the classification of bundles on spheres via the clutching construction, these correspond to homotopy classes of maps S 3→SO(4)S^3 \to SO(4), i.e. elements of π 3(SO(4))\pi_3(SO(4)). From the table at orthogonal group – Homotopy groups, this latter group is ℤ⊕ℤ\mathbb{Z}\oplus\mathbb{Z}. Thus any such bundle can be described, up to isomorphism, by a pair of integers (n,m)(n,m).

Let E m,n↠S 4E_{m,n}\twoheadrightarrow S^4 denote the real vector bundle corresponding to the integer pair m,n∈ℤm,n\in\mathbb{Z}. There is an orientation-reversing vector bundle isomorphism E m,n≅E −m,−nE_{m,n}\cong E_{-m,-n}. (McEnroe 15, Lem. 6.14) Let α∈H 4(S 4)≅ℤ\alpha\in H^4(S^4)\cong\mathbb{Z} be a generator, then its Euler class and fractional first Pontryagin class are:

e(E m,n)=−(m+n)α; e(E_{m,n}) =-(m+n)\alpha;
p 1(E m,n)2=(n−m)α. \frac{p_1(E_{m,n})}{2} =(n-m)\alpha.

(McEnroe 15, Eq. (6.17) & Eq. (6.29))

With the choice of a Riemannian metric on it, one has a disk bundle D(E m,n)↠S 4D(E_{m,n})\twoheadrightarrow S^4 by taking the disks D 4⊂ℝ 4D^4\subset\mathbb{R}^4 of each fiber, a sphere bundle S(E m,n)=∂D(E m,n)↠S 4S(E_{m,n})=\partial D(E_{m,n})\twoheadrightarrow S^4 by taking the spheres S 3⊂ℝ 4S^3\subset\mathbb{R}^4 of each fiber as well as a Thom space Th(E m,n)=D(E m,n)/S(E m,n)Th(E_{m,n})=D(E_{m,n})/S(E_{m,n}). None of their topological or smooth structures depend on the choice of the Riemannian metric.

A special case is the quaternionic Hopf fibration h ℍ:ℍ 2⊃S 7↠S 4≅ℍP 1,[q,p]↦[q:p]h_\mathbb{H}\colon\mathbb{H}^2\supset S^7\twoheadrightarrow S^4\cong\mathbb{H}P^1,[q,p]\mapsto[q:p], which is a principal SU(2)-bundle and the sphere bundle of the real vector bundle (γ ℍ 1,1) ℝ↠S 4(\gamma_\mathbb{H}^{1,1})_\mathbb{R}\twoheadrightarrow S^4 represented by the continuous map:

S 4≅ℍP 1↪ℍP ∞≅BSU(2)↪BSO(4), S^4 \cong\mathbb{H}P^1 \hookrightarrow\mathbb{H}P^\infty \cong B SU(2) \hookrightarrow B SO(4),

which corresponds to m=0m=0 and n=1n=1. (McEnroe 15, p. 11)

More generally for n+m=1n+m=1, a Morse function with exactly two critical points on S(E m,n)S(E_{m,n}) exists, implying that it is homeomorphic to S 7S^7 according to the Reeb sphere theorem. If it is further diffeomorphic, then it is possible to glue the disk bundle D(E m,n)D(E_{m,n}) and the disk D 8D^8 together along their common boundary S(E m,n)≅S 7S(E_{m,n})\cong S^7 using a pullback to obtain the closed 8-manifold:

M m,n=D(E m,n)+ S 7D 8. M_{m,n} =D(E_{m,n})+_{S^7}D^8.

Due to H 4(M m,n,ℤ)≅ℤH^4(M_{m,n},\mathbb{Z})\cong\mathbb{Z} and H 8(M m,n,ℤ)≅ℤH^8(M_{m,n},\mathbb{Z})\cong\mathbb{Z}, the intersection form is described by a single integer and hence the signature can only be σ(M m,n)=1\sigma(M_{m,n})=1 with suitable orientation. According to Hirzebruch's signature theorem, the signature is also given by:

σ(M m,n)=145⟨7p 2(M m,n)−p 1 2(M m,n),[M m,n]⟩ \sigma(M_{m,n}) =\frac{1}{45}\langle 7p_2(M_{m,n})-p_1^2(M_{m,n}),[M_{m,n}]\rangle

(McEnroe 15, Thrm. 6.37)

Since the first Pontrjagin class is known, but the second Pontrjagin class is not, John Milnor eliminated it by projecting to the following modulo-7 diffeomorphism invariant:

4(m−n) 2mod7=−⟨p 1 2(M m,n),[M m,n]⟩mod7=45σ(M m,n)mod7=±45mod7=±3 ⇒(p 1(E m,n)2) 2=(m−n) 2mod7=1. \begin{aligned} 4(m-n)^2 mod 7 =-\langle p_1^2(M_{m,n}),[M_{m,n}]\rangle mod 7 =45\sigma(M_{m,n}) mod 7 =\pm 45 mod 7 =\pm 3 \\ \Rightarrow \left(\frac{p_1(E_{m,n})}{2}\right)^2 =(m-n)^2 mod 7 =1. \end{aligned}

(McEnroe 15, Thrm. 6.44)

S(E m,n)S(E_{m,n}) with m+n=1m+n=1 is then diffeomorphic to the standard 77-sphere S 7S^7 if and only if this equation holds and hence the modulo-7 diffeomorphism invariant (m−n) 2−1mod7(m-n)^2-1 mod 7 vanishes. Examples like m=1m=1 and n=2n=2 show, that this doesn’t have to be true. In this case, the contradiction in Hirzebruch's signature theorem is resolved by the previously used assumption of S(E m,n)S(E_{m,n}) and S 7S^7 to be diffeomorphic to obtain the glueing M m,nM_{m,n} to not be true. E m,nE_{m,n} with m+n=1m+n=1 and (m−n) 2mod7≠1(m-n)^2 mod 7\neq 1 is then homeomorphic but not diffeomorphic to the standard 77-sphere S 7S^7.

By using the connected sum operation, the set of smooth, non-diffeomorphic structures on the nn-sphere has the structure of an abelian group. For the 7-sphere, it is the cyclic group ℤ/28\mathbb{Z}/{28} and Brieskorn (1966) found the generator Σ\Sigma so that Σ#⋯#Σ⏟ 28\underbrace{\Sigma\#\cdots\#\Sigma}_28 is the standard sphere.

Review includes (Kreck 10, chapter 19, McEnroe 15, Joachim-Wraith).

Examples

Properties

As near-horizon geometries of black M2-branes

From the point of view of M-theory on 8-manifolds, these 8-manifolds XX with (exotic) 7-sphere boundaries in Milnor’s construction correspond to near horizon limits of black M2 brane spacetimes ℝ 2,1×X\mathbb{R}^{2,1} \times X, where the M2-branes themselves would be sitting at the center of the 7-spheres (if that were included in the spacetime, see also Dirac charge quantization).

(Morrison-Plesser 99, section 3.2, FSS 19, 3.8))

References

General

See also:

In relation to TQFT:

In M-theory

Last revised on July 15, 2026 at 07:24:51. See the history of this page for a list of all contributions to it.