In differential geometry the Hitchin - Thorpe inequality is a relation which restricts the topology of 4-manifolds that carry an Einstein metric.
Let M be a closed, oriented, four-dimensional smooth manifold. If there exists a Riemannian metric on M which is an Einstein metric, then
\chi(M)\geq
3 | |
2 |
|\tau(M)|,
This inequality was first stated by John Thorpe in a footnote to a 1969 paper focusing on manifolds of higher dimension.[1] Nigel Hitchin then rediscovered the inequality, and gave a complete characterization of the equality case in 1974;[2] he found that if is an Einstein manifold for which equality in the Hitchin-Thorpe inequality is obtained, then the Ricci curvature of is zero; if the sectional curvature is not identically equal to zero, then is a Calabi–Yau manifold whose universal cover is a K3 surface.
Already in 1961, Marcel Berger showed that the Euler characteristic is always non-negative.[3] [4]
Let be a four-dimensional smooth Riemannian manifold which is Einstein. Given any point of, there exists a -orthonormal basis of the tangent space such that the curvature operator, which is a symmetric linear map of into itself, has matrix
\begin{pmatrix}λ1&0&0&\mu1&0&0\ 0&λ2&0&0&\mu2&0\ 0&0&λ3&0&0&\mu3\ \mu1&0&0&λ1&0&0\ 0&\mu2&0&0&λ2&0\ 0&0&\mu3&0&0&λ3\end{pmatrix}
According to Chern-Weil theory, if is oriented then the Euler characteristic and signature of can be computed by
\begin{align} \chi(M)&= | 1 |
4\pi2 |
\intM(λ
2)d\mu | ||||
|
\intM(λ1\mu1+λ2\mu2+λ3\mu3)d\mug. \end{align}
2=\underbrace{(λ | |
λ | |
1-\mu |
2+(λ | |
2-\mu |
2+(λ | |
3-\mu |
2} | |
\geq0 |
+2(λ1\mu1+λ2\mu2+λ3\mu3).
A natural question to ask is whether the Hitchin - Thorpe inequality provides a sufficient condition for the existence of Einstein metrics. In 1995, Claude LeBrun and Andrea Sambusetti independently showed that the answer is no: there exist infinitely many non-homeomorphic compact, smooth, oriented 4-manifolds that carry no Einstein metrics but nevertheless satisfy
\chi(M)>
3 | |
2 |
|\tau(M)|.
LeBrun's examples are actually simply connected, and the relevant obstruction depends on the smooth structure of the manifold.[5] By contrast, Sambusetti's obstruction only applies to 4-manifolds with infinite fundamental group, but the volume-entropy estimate he uses to prove non-existence only depends on the homotopy type of the manifold.[6]