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In mathematics, the Schottky problem is a classical question of algebraic geometry, asking for a characterisation of Jacobian varieties amongst abelian varieties.
## Geometric formulation

## Period lattice formulation

## Riemann's matrix formulation

NB a Riemann matrix is quite different from any Riemann tensor## Geometry of the problem

## See also

## External links

More precisely, one should consider algebraic curves C of a given genus g, and their Jacobians J. There is a moduli space M_{g} of such curves, and a moduli space A_{g} of abelian varieties of dimension g, which are principally polarized. There is a morphism

- ι: M
_{g}→ A_{g}

which on points (geometric points, to be more accurate) takes C to J. The content of Torelli's theorem is that ι is injective (again, on points). The Schottky problem asks for a description of the image of ι.

It is discussed for g ≥ 4: the dimension of M_{g} is 3g − 3, for g ≥ 2, while the dimension of A_{g} is g(g + 1)/2. This means that the dimensions are the same (0, 1, 3, 6) for g = 0, 1, 2, 3. Therefore g = 4 is the first interesting case, and this was studied by W. Schottky in the 1880s. Schottky applied the theta constants, which are modular forms for the Siegel upper half-space, to define the Schottky locus in A_{g}. A more precise form of the question is to determine whether the image of ι essentially coincides with the Schottky locus (in other words, whether it is Zariski dense there).

If one describes the moduli space A_{g} in intuitive terms, as the parameters on which an abelian variety depends, then the Schottky problem asks simply what condition on the parameters implies that the abelian variety comes from a curve's Jacobian. The classical case, over the complex number field, has received most of the attention, and then an abelian variety A is simply a complex torus of a particular type, arising from a lattice in C^{g}. In relatively concrete terms, it is being asked which lattices are the period lattices of compact Riemann surfaces.

One of the major achievements of Bernhard Riemann was his theory of complex tori and theta functions. Using the Riemann theta function, necessary and sufficient conditions on a lattice were written down by Riemann for a lattice in C^{g} to have the corresponding torus embed into complex projective space. (The interpretation may have come later, with Solomon Lefschetz, but Riemann's theory was definitive.) The data is what is now called a Riemann matrix. Therefore the complex Schottky problem becomes the question of characterising the period matrices of compact Riemann surfaces of genus g, formed by integrating a basis for the abelian integrals round a basis for the first homology group, amongst all Riemann matrices.

There are a number of geometric approaches, and the question has also been shown to implicate the Kadomtsev-Petviashvili equation, related to soliton theory.

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Last updated on Thursday November 29, 2007 at 11:13:14 PST (GMT -0800)

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Last updated on Thursday November 29, 2007 at 11:13:14 PST (GMT -0800)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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