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The family of Hodge structures is given concretely by matrices of integrals. To illustrate these ideas, consider an Elliptic Curve E with equation

:y^2 = x^3 + ax + b.\,

Let \delta and \gamma be an integral homology basis for E where the intersection number \delta . \gamma = 1. Consider the differential 1-form

:\omega = extrm{d}x/y.\,

It is a holomorphic 1-form ( Differential Of The First Kind ). Consider the integrals

:\int_\gamma \omega,\ \int_\delta \omega.\,

These integrals are called periods. The vector of periods whose coordinates are the given integrals is the Period Matrix in this example. Denote the period matrix by P. The matrix P depends holomorphically on the parameters a and b of the elliptic curve. The map which sends (a,b) to P is a concrete representation the period map of the given family of elliptic curves.

Let us now make the connecton with Hodge structures. The holomorphic 1-form \omega defines a one-dimensional subspace of the complex cohomology of E. Let us denote this subspace by H^{1,0}. Thus we have a line H^{1,0} in the two-dimensional complex vector space H^1(E,C). The choice of homology basis \delta, \gamma defines an isomorphism of H^1(E,C) with the standard two-dimensional complex vector space C^2. This isomorphism identifies H^{1,0} with a line L in C^2, namely, the line spanned by the vector P. The line L is determined by its slope, the ratio

: au = rac{\int_\gamma \omega}{\int_\delta \omega}.\,

The period map in this context is the map

:(a,b) o au

modulo the choice of homology basis subject to the constraint on the intersection number.


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