# Atiyah–Singer index theorem

In differential geometry, the **Atiyah–Singer index theorem**, proved by Michael Atiyah and Isadore Singer (1963),^{[1]} states that for an elliptic differential operator on a compact manifold, the **analytical index** (related to the dimension of the space of solutions) is equal to the **topological index** (defined in terms of some topological data). It includes many other theorems, such as the Chern–Gauss–Bonnet theorem and Riemann–Roch theorem, as special cases, and has applications to theoretical physics.^{[2]}^{[3]}

The index problem for elliptic differential operators was posed by Israel Gel'fand.^{[4]} He noticed the homotopy invariance of the index, and asked for a formula for it by means of topological invariants. Some of the motivating examples included the Riemann–Roch theorem and its generalization the Hirzebruch–Riemann–Roch theorem, and the Hirzebruch signature theorem. Friedrich Hirzebruch and Armand Borel had proved the integrality of the Â genus of a spin manifold, and Atiyah suggested that this integrality could be explained if it were the index of the Dirac operator (which was rediscovered by Atiyah and Singer in 1961).

The Atiyah–Singer theorem was announced in 1963.^{[1]} The proof sketched in this announcement was never published by them, though it appears in the Palais's book.^{[5]} It appears also in the "Séminaire Cartan-Schwartz 1963/64"^{[6]} that was held in Paris simultaneously with the seminar led by Richard Palais at Princeton University. The last talk in Paris was by Atiyah on manifolds with boundary. Their first published proof^{[7]} replaced the cobordism theory of the first proof with K-theory, and they used this to give proofs of various generalizations in another sequence of papers.^{[8]}

The symbol of a differential operator of order *n* on a smooth manifold *X* is defined in much the same way using local coordinate charts, and is a function on the cotangent bundle of *X*, homogeneous of degree *n* on each cotangent space. (In general, differential operators transform in a rather complicated way under coordinate transforms (see jet bundle); however, the highest order terms transform like tensors so we get well defined homogeneous functions on the cotangent spaces that are independent of the choice of local charts.) More generally, the symbol of a differential operator between two vector bundles *E* and *F* is a section of the pullback of the bundle Hom(*E*, *F*) to the cotangent space of *X*. The differential operator is called *elliptic* if the element of Hom(*E _{x}*,

*F*) is invertible for all non-zero cotangent vectors at any point

_{x}*x*of

*X*.

A key property of elliptic operators is that they are almost invertible; this is closely related to the fact that their symbols are almost invertible. More precisely, an elliptic operator *D* on a compact manifold has a (non-unique) **parametrix** (or **pseudoinverse**) *D*′ such that *DD′ *^{−1} and *D′D*^{−1} are both compact operators. An important consequence is that the kernel of *D* is finite-dimensional, because all eigenspaces of compact operators, other than the kernel, are finite-dimensional. (The pseudoinverse of an elliptic differential operator is almost never a differential operator. However, it is an elliptic pseudodifferential operator.)

As the elliptic differential operator *D* has a pseudoinverse, it is a Fredholm operator. Any Fredholm operator has an *index*, defined as the difference between the (finite) dimension of the kernel of *D* (solutions of *Df* = 0), and the (finite) dimension of the cokernel of *D* (the constraints on the right-hand-side of an inhomogeneous equation like *Df* = *g*, or equivalently the kernel of the adjoint operator). In other words,

**Example:** Suppose that the manifold is the circle (thought of as **R**/**Z**), and *D* is the operator d/dx − λ for some complex constant λ. (This is the simplest example of an elliptic operator.) Then the kernel is the space of multiples of exp(λ*x*) if λ is an integral multiple of 2π*i* and is 0 otherwise, and the kernel of the adjoint is a similar space with λ replaced by its complex conjugate. So *D* has index 0. This example shows that the kernel and cokernel of elliptic operators can jump discontinuously as the elliptic operator varies, so there is no nice formula for their dimensions in terms of continuous topological data. However the jumps in the dimensions of the kernel and cokernel are the same, so the index, given by the difference of their dimensions, does indeed vary continuously, and can be given in terms of topological data by the index theorem.

One can also define the topological index using only K-theory (and this alternative definition is compatible in a certain sense with the Chern-character construction above). If *X* is a compact submanifold of a manifold *Y* then there is a pushforward (or "shriek") map from K(*TX*) to K(*TY*). The topological index of an element of K(*TX*) is defined to be the image of this operation with *Y* some Euclidean space, for which K(*TY*) can be naturally identified with the integers **Z** (as a consequence of Bott-periodicity). This map is independent of the embedding of *X* in Euclidean space. Now a differential operator as above naturally defines an element of K(*TX*), and the image in **Z** under this map "is" the topological index.

As usual, *D* is an elliptic differential operator between vector bundles *E* and *F* over a compact manifold *X*.

The *index problem* is the following: compute the (analytical) index of *D* using only the symbol *s* and *topological* data derived from the manifold and the vector bundle. The Atiyah–Singer index theorem solves this problem, and states:

In spite of its formidable definition, the topological index is usually straightforward to evaluate explicitly. So this makes it possible to evaluate the analytical index. (The cokernel and kernel of an elliptic operator are in general extremely hard to evaluate individually; the index theorem shows that we can usually at least evaluate their **difference**.) Many important invariants of a manifold (such as the signature) can be given as the index of suitable differential operators, so the index theorem allows us to evaluate these invariants in terms of topological data.

Although the analytical index is usually hard to evaluate directly, it is at least obviously an integer. The topological index is by definition a rational number, but it is usually not at all obvious from the definition that it is also integral. So the Atiyah–Singer index theorem implies some deep integrality properties, as it implies that the topological index is integral.

The index of an elliptic differential operator obviously vanishes if the operator is self adjoint. It also vanishes if the manifold *X* has odd dimension, though there are **pseudodifferential** elliptic operators whose index does not vanish in odd dimensions.

**For any abstract elliptic operator (Atiyah 1970) on a closed, oriented, topological manifold, the analytical index equals the topological index.**

The proof of this result goes through specific considerations, including the extension of Hodge theory on combinatorial and Lipschitz manifolds (Teleman 1980), (Teleman 1983), the extension of Atiyah–Singer's signature operator to Lipschitz manifolds (Teleman 1983), Kasparov's K-homology (Kasparov 1972) and topological cobordism (Kirby & Siebenmann 1977).

This result shows that the index theorem is not merely a differentiability statement, but rather a topological statement.

Due to (Donaldson & Sullivan 1989), (Connes, Sullivan & Teleman 1994):

**For any quasiconformal manifold there exists a local construction of the Hirzebruch–Thom characteristic classes.**

This theory is based on a signature operator *S*, defined on middle degree differential forms on even-dimensional quasiconformal manifolds (compare (Donaldson & Sullivan 1989)).

Using topological cobordism and K-homology one may provide a full statement of an index theorem on quasiconformal manifolds (see page 678 of (Connes, Sullivan & Teleman 1994)). The work (Connes, Sullivan & Teleman 1994) "provides local constructions for characteristic classes based on higher dimensional relatives of the measurable Riemann mapping in dimension two and the Yang–Mills theory in dimension four."

These results constitute significant advances along the lines of Singer's program *Prospects in Mathematics* (Singer 1971). At the same time, they provide, also, an effective construction of the rational Pontrjagin classes on topological manifolds. The paper (Teleman 1985) provides a link between Thom's original construction of the rational Pontrjagin classes (Thom 1956) and index theory.

It is important to mention that the index formula is a topological statement. The obstruction theories due to Milnor, Kervaire, Kirby, Siebenmann, Sullivan, Donaldson show that only a minority of topological manifolds possess differentiable structures and these are not necessarily unique. Sullivan's result on Lipschitz and quasiconformal structures (Sullivan 1979) shows that any topological manifold in dimension different from 4 possesses such a structure which is unique (up to isotopy close to identity).

The quasiconformal structures (Connes, Sullivan & Teleman 1994) and more generally the *L*^{p}-structures, *p* > *n(n+1)/2*, introduced by M. Hilsum (Hilsum 1999), are the weakest analytical structures on topological manifolds of dimension *n* for which the index theorem is known to hold.

Suppose that *M* is a compact oriented manifold. If we take *E* to be the sum of the even exterior powers of the cotangent bundle, and *F* to be the sum of the odd powers, define *D* = *d* + *d**, considered as a map from *E* to *F*. Then the topological index of *D* is the Euler characteristic of the Hodge cohomology of *M*, and the analytical index is the Euler class of the manifold. The index formula for this operator yields the Chern–Gauss–Bonnet theorem.

Take *X* to be a complex manifold with a holomorphic vector bundle *V*. We let the vector bundles *E* and *F* be the sums of the bundles of differential forms with coefficients in *V* of type (0,*i*) with *i* even or odd, and we let the differential operator *D* be the sum

restricted to *E*. Then the analytical index of *D* is the holomorphic Euler characteristic of *V*:

the product of the Chern character of *V* and the Todd class of *X* evaluated on the fundamental class of *X*.
By equating the topological and analytical indices we get the Hirzebruch–Riemann–Roch theorem. In fact we get a generalization of it to all complex manifolds: Hirzebruch's proof only worked for **projective** complex manifolds *X*.

This derivation of the Hirzebruch–Riemann–Roch theorem is more natural if we use the index theorem for elliptic complexes rather than elliptic operators. We can take the complex to be

The Hirzebruch signature theorem states that the signature of a compact oriented manifold *X* of dimension 4*k* is given by the L genus of the manifold. This follows from the Atiyah–Singer index theorem applied to the following signature operator.

The bundles *E* and *F* are given by the +1 and −1 eigenspaces of the operator on the bundle of differential forms of *X*, that acts on *k*-forms as

restricted to *E*, where **d** is the Cartan exterior derivative and **d*** is its adjoint.

The analytic index of *D* is the signature of the manifold *X*, and its topological index is the L genus of *X*, so these are equal.

The Â genus is a rational number defined for any manifold, but is in general not an integer. Borel and Hirzebruch showed that it is integral for spin manifolds, and an even integer if in addition the dimension is 4 mod 8. This can be deduced from the index theorem, which implies that the Â genus for spin manifolds is the index of a Dirac operator. The extra factor of 2 in dimensions 4 mod 8 comes from the fact that in this case the kernel and cokernel of the Dirac operator have a quaternionic structure, so as complex vector spaces they have even dimensions, so the index is even.

In dimension 4 this result implies Rochlin's theorem that the signature of a 4-dimensional spin manifold is divisible by 16: this follows because in dimension 4 the Â genus is minus one eighth of the signature.

Pseudodifferential operators can be explained easily in the case of constant coefficient operators on Euclidean space. In this case, constant coefficient differential operators are just the Fourier transforms of multiplication by polynomials, and constant coefficient pseudodifferential operators are just the Fourier transforms of multiplication by more general functions.

Many proofs of the index theorem use pseudodifferential operators rather than differential operators. The reason for this is that for many purposes there are not enough differential operators. For example, a pseudoinverse of an elliptic differential operator of positive order is not a differential operator, but is a pseudodifferential operator. Also, there is a direct correspondence between data representing elements of K(B(*X*), *S*(*X*)) (clutching functions) and symbols of elliptic pseudodifferential operators.

Pseudodifferential operators have an order, which can be any real number or even −∞, and have symbols (which are no longer polynomials on the cotangent space), and elliptic differential operators are those whose symbols are invertible for sufficiently large cotangent vectors. Most version of the index theorem can be extended from elliptic differential operators to elliptic pseudodifferential operators.

The initial proof was based on that of the Hirzebruch–Riemann–Roch theorem (1954), and involved cobordism theory and pseudodifferential operators.

The idea of this first proof is roughly as follows. Consider the ring generated by pairs (*X*, *V*) where *V* is a smooth vector bundle on the compact smooth oriented manifold *X*, with relations that the sum and product of the ring on these generators are given by disjoint union and product of manifolds (with the obvious operations on the vector bundles), and any boundary of a manifold with vector bundle is 0. This is similar to the cobordism ring of oriented manifolds, except that the manifolds also have a vector bundle. The topological and analytical indices are both reinterpreted as functions from this ring to the integers. Then one checks that these two functions are in fact both ring homomorphisms. In order to prove they are the same, it is then only necessary to check they are the same on a set of generators of this ring. Thom's cobordism theory gives a set of generators; for example, complex vector spaces with the trivial bundle together with certain bundles over even dimensional spheres. So the index theorem can be proved by checking it on these particularly simple cases.

Atiyah and Singer's first published proof used K-theory rather than cobordism. If *i* is any inclusion of compact manifolds from *X* to *Y*, they defined a 'pushforward' operation *i*_{!} on elliptic operators of *X* to elliptic operators of *Y* that preserves the index. By taking *Y* to be some sphere that *X* embeds in, this reduces the index theorem to the case of spheres. If *Y* is a sphere and *X* is some point embedded in *Y*, then any elliptic operator on *Y* is the image under *i*_{!} of some elliptic operator on the point. This reduces the index theorem to the case of a point, where it is trivial.

Atiyah, Bott, and Patodi (1973) gave a new proof of the index theorem using the heat equation, see e.g. Berline, Getzler & Vergne (1992). The proof is also published in (Melrose 1993) and (Gilkey 1994).

If *D* is a differential operator with adjoint *D**, then *D*D* and *DD** are self adjoint operators whose non-zero eigenvalues have the same multiplicities. However their zero eigenspaces may have different multiplicities, as these multiplicities are the dimensions of the kernels of *D* and *D**. Therefore, the index of *D* is given by

for any positive *t*. The right hand side is given by the trace of the difference of the kernels of two heat operators. These have an asymptotic expansion for small positive *t*, which can be used to evaluate the limit as *t* tends to 0, giving a proof of the Atiyah–Singer index theorem. The asymptotic expansions for small *t* appear very complicated, but invariant theory shows that there are huge cancellations between the terms, which makes it possible to find the leading terms explicitly. These cancellations were later explained using supersymmetry.

The papers by Atiyah are reprinted in volumes 3 and 4 of his collected works, (Atiyah 1988a, 1988b)