An exotic smooth structure is, roughly speaking, a smooth structure on a topological manifold $X$ which makes the resulting smooth manifold be non-diffeomorphic to the smooth manifold given by some evident ‘standard’ smooth structure on $X$.
Milnor (1956) gave the first examples of exotic smooth structures on the 7-sphere constructed via a $S^3$-bundle over the 4-sphere $S^4$, finding at least seven. Note that spheres inherit a canonical smooth structure from their canonical (topological) embedding into a Cartesian space $S^n \hookrightarrow \mathbb{R}^{n+1}$.
Via the celebrated h cobordism theorem of Smale (Smale 1962, Milnor 1965) one gets a relation between the number of smooth structures on the $n$-sphere $S^n$ (for $n \geq 5$) and the number of isotopy classes $\pi_0 (Diff(S^{n-1}))$ of the equator $S^{n-1}$. Then Kervaire and Milnor (1963) proved that there are only finitely many exotic smooth structures on all spheres in dimension 5 or higher. By using the connected sum operation, the set of smooth, non-diffeomorphic structures on the $n$-sphere has the structure of an abelian group. For the 7-sphere, it is the cyclic group $Z_{28}$ and Brieskorn (1966) found the generator $\Sigma$ so that $\underbrace{\Sigma\#\cdots\#\Sigma}_28$ is the standard sphere.
A complete classification of smooth, PL and topological structures on manifolds in dimension 5 and higher was established by Kirby and Siebenmann (1977) using obstruction theory.
Note that there exist uncountably many exotic smooth structures on $\mathbb{R}^4$ (Gompf 1985, Freedman/Taylor 1986, Taubes 1987), but a unique smooth structure on $\mathbb{R}^n$ for $n\neq 4$ (Stallings, Zeeman 1962). There is a unique maximal exotic $\mathbb{R}^4$ into which all other ‘versions’ of $\mathbb{R}^4$ smoothly embed as open subsets (Freedman/Taylor 1986, DeMichelis/Freedman 1992).
There are two classes of exotic $\mathbb{R}^4$‘s: large and small. A large exotic $\mathbb{R}^4$ cannot be embedded in the 4-sphere $S^4$ (Gompf 1985, Taubes 1987) whereas a small exotic $\mathbb{R}^4$ admits such an embedding (DeMichelis/Freedman 1992). A large exotic $\mathbb{R}^4$ is constructed by using the failure to smoothly split a smooth 4-manifold (the K3 surface for instance) as connected sum of some factors (where a topological splitting exits). The small exotic $\mathbb{R}^4$ (or ribbon $\mathbb{R}^4$) is constructed by using the failure of the smooth h cobordism theorem in dimension 4 (Donaldson 1987, 1990). Bizaca and Gompf (1996) are able to present an infinite handle body of a small exotic $\mathbb{R}^4$ which serve as a coordinate representation.
Moise (1952) proved that in dimension 3 there are no exotic differentiable structures, or to put in another way, 3-dimensional differentiable manifolds which are homeomorphic are diffeomorphic. In this way the 3-sphere $S^3$ inherits a unique differentiable structure, no matter which $\mathbb{R}^4$ it is considered to be embedded in.
Rado (1925) proved that in dimension 2 there are no exotic differentiable structures (or the uniqueness of the standard structure). The classification of 1-dimensional manifolds and the uniqueness of the smooth structure can be found in the Appendix of Milnor (1965b).
The 7-spheres constructed in Milnor 1956 are all examples of fibre bundles over $S^4$ with fibre $S^3$, with structure group $SO(4)$. By the classification of bundles on spheres, these correspond to homotopy classes of maps $S^3 \to SO(4)$, i.e. elements of $\pi_3(SO(4))$. From the table at orthogonal group, this latter group is $\mathbb{Z}\oplus\mathbb{Z}$. Thus any such bundle can be described up to isomorphism by a pair of integers $(n,m)$. When $n+m=1$, then one can show there is a Morse function with exactly two critical points on the total space of the bundle, and hence this 7-manifold is homeomorphic to a sphere.
The fractional first Pontryagin class $\frac{p_1}{2} \in H^4(S^4) \simeq \mathbb{Z}$ of the bundle is given by $n-m$. Milnor constructs, using cobordism theory and Hirzebruch's signature theorem? for 8-manifolds, a mod-7 diffeomorphism invariant of the manifold, so that it is standard 7-sphere precisely when $\frac{p_1}{2}^2 -1 = 0 (mod 7)$.
The first construction of exotic smooth structures was on the 7-sphere in
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Smale, Stephen (1962), “On the structure of manifolds” , Amer. J. of Math. 84 : 387-399 (#Smale)
John Milnor (1965), Lectures on the h-cobordism theorem (Princeton Univ. Press, Princeton)
(see Wikipedia (spheres, $R^4$) for more for now)
A survey of applications of the theory of exotic smooth structures in physics is in
below we list more references sorted by the kind of physical application they deal with.
The original argument that exotic spheres are to be regarded as instantons of gravity is on p. 12 of
Further discussion of exotic $4$-manifolds from the general relativity point of view is in
Carl Brans, Duane Randall, Exotic differentiable structures and general relativity Gen. Rel. Grav., 25 (1993) 205–220
Carl Brans Exotic smoothness and physics J. Math. Phys. 35, (1994), 5494–5506.
The following paper contained a first proof to localize exotic smoothness in an exotic $\mathbb{R}^4$:
A more philosophical discussion can be found in:
Brans conjectured in the papers above, that exotic smoothness should be a source of an additional gravitational field (Brans conjecture). This conjecture was confirmed for compact $4$-manifolds (using implicitly a mapping of basic classes):
Using the invariant of L. Taylor arXiv, Sladkowski confirmed the conjecture for the exotic $\mathbb{R}^4$ in:
Via a detailed analysis of the Casson handle (as the main object to construct exotic smoothness for $4$-manifolds via the Akbulut cork), it is possible to get the action of Dirac field and of the gauge bosons from the Einstein-Hilbert action (with a boundary term) in:
The first paper describes a construction of an exotic $\mathbb{R}^4$ via a codimension-$1$ foliation of a homology $3$-sphere in the interior (classified by the Godbillon–Vey invariant). One of the results is a charge quantization without a monopole:
Then one gets various relations to orbifolds and the WZW model (level of the conformal field theory)
The first real connection between exotic smoothness and quantum field theory is Witten’s TQFT:
and the whole work of Seiberg and Witten leading to the celebrated invariants.
The relation to particle physics by using the algebra of smooth functions can be found in
Jan Sładkowski, Exotic smoothness, noncommutative geometry and particle physics Int. J. Theor. Phys., 35, (1996), 2075–2083
Jan Sładkowski, Exotic smoothness and particle physics Acta Phys. Polon., B 27, (1996), 1649–1652
Jan Sładkowski, Exotic smoothness, fundamental interactions and noncommutative geometry arXiv
The relation between TQFT and differential-topological invariants of smooth manifolds was clarified in:
Hendryk Pfeiffer Quantum general relativity and the classification of smooth manifolds arXiv
Hendryk Pfeiffer Diffeomorphisms from finite triangulations and absence of ‘local’ degrees of freedom Phys.Lett. B, 591, (2004), 197-201
The first conjectured (direct) relation (identifying submanifolds with operators) to quantum mechanics (using singular connections) was established here:
Using the relation to foliations and noncommutative geometry for the leave space, one can reproduce the vacuum sector of a QFT (the factor $III_1$) via exotic smoothness as explained here:
An argument for interpreting exotic smooth spheres as gravitational instanton?s and to cancel the gravitational anomalies of string theory is in
The influence of exotic smoothness for Kaluza-Klein models was discussed here:
A discussion of topological effects (also of string theory) in relation to exotic smoothness is in
There are also some relations between string backgrounds, quantum D-branes and exotic $\mathbb{R}^4$
The first idea to use exotic smoothness to explain some cosmological anomalies (dark energy etc.) can be found here:
Then this idea was used to discuss a model of the cosmos including the cosmological constant (only the present value of the constant can be reproduced, no explanation of the scaling behavior!):
An overview can be also found in
A first calculation of the state sum in quantum gravity by inclusion of exotic smoothness
A semi-classical approach to the functional integral is discussed here:
A complete expression for the state sum in quantum gravity for compact $4$-manifolds by inclusion of exotic smoothness using the knot surgery a la Fintushel and Stern
The inclusion of singularities for asymptotically flat spacetimes is discussed here (with an example of a singularity coming from exotic smoothness):