Hitchin Fibration

In mathematics, the Hitchin integrable system is an integrable system depending on the choice of a complex reductive group and a compact Riemann surface, introduced by Nigel Hitchin in 1987. It lies on the crossroads of algebraic geometry, the theory of Lie algebras and integrable system theory. It also plays an important role in the geometric Langlands correspondence over the field of complex numbers through conformal field theory. A genus zero analogue of the Hitchin system, the Garnier system, was discovered by René Garnier somewhat earlier as a certain limit of the Schlesinger equations, and Garnier solved his system by defining spectral curves. (The Garnier system is the classical limit of the Gaudin model. In turn, the Schlesinger equations are the classical limit of the Knizhnik–Zamolodchikov equations). Almost all integrable systems of classical mechanics can be obtained as particular cases of the Hitchin system or their common generalization defined by Bottacin and Markman in 1994.

Description

Using the language of algebraic geometry, the phase space of the system is a partial compactification of the cotangent bundle to the moduli space of stable ''G''-bundles for some reductive group ''G'', on some compact algebraic curve. This space is endowed with a canonical symplectic form. Suppose for simplicity that ''G''=GL(''n'', ℂ), the general linear group; then the Hamiltonians can be described as follows: the tangent space to the moduli space of ''G''-bundles at the bundle ''F'' is

:$H^1(\operatorname(F)),$

which by Serre duality is dual to

:$\Phi \in H^0(\operatorname(F)\otimes K),$

where $K$ is the canonical bundle, so a pair

:$(F,\Phi)$

called a Hitchin pair or Higgs bundle, defines a point in the cotangent bundle. Taking

:$\operatorname(\Phi^k),\qquad k=1,\ldots,\operatorname(G)$

one obtains elements in

:$H^0( K^ ),$

which is a vector space which does not depend on $(F,\Phi)$. So taking any basis in these vector spaces we obtain functions ''H_i'', which are Hitchin's hamiltonians. The construction for general reductive group is similar and uses invariant polynomials on the Lie algebra of ''G''.

For trivial reasons these functions are algebraically independent, and some calculations show that their number is exactly half of the dimension of the phase space. The nontrivial part is a proof of Poisson commutativity of these functions. They therefore define an integrable system in the symplectic or Arnol'd–Liouville sense.

Hitchin fibration

The Hitchin fibration is the map from the moduli space of Hitchin pairs to characteristic polynomials, a higher genus analogue of the map Garnier used to define the spectral curves. used Hitchin fibrations over finite fields in his proof of the fundamental lemma.

See also

* Yang–Mills equations
* Higgs bundle
*Nonabelian Hodge correspondence
* Character variety
* Hitchin's equations

References

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{{Integrable systems
Algebraic geometry
Dynamical systems
Hamiltonian mechanics
Integrable systems
Lie groups
Differential geometry