Rosati involution

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In mathematics, a Rosati involution, named after Carlo Rosati, is an involution of the rational endomorphism ring of an abelian variety induced by a polarization.

Let A be an abelian variety, let {\hat  A}={\mathrm  {Pic}}^{0}(A) be the dual abelian variety, and for a\in A, let T_{a}:A\to A be the translation-by-a map, T_{a}(x)=x+a. Then each divisor D on A defines a map \phi _{D}:A\to {\hat  A} via \phi _{D}(a)=[T_{a}^{*}D-D]. The map \phi _{D} is a polarization, i.e., has finite kernel, if and only if D is ample. The Rosati involution of {\mathrm  {End}}(A)\otimes {\mathbb  {Q}} relative to the polarization \phi _{D} sends a map \psi \in {\mathrm  {End}}(A)\otimes {\mathbb  {Q}} to the map \psi '=\phi _{D}^{{-1}}\circ {\hat  \psi }\circ \phi _{D}, where {\hat  \psi }:{\hat  A}\to {\hat  A} is the dual map induced by the action of \psi ^{*} on {\mathrm  {Pic}}(A).

Let {\mathrm  {NS}}(A) denote the Néron–Severi group of A. The polarization \phi _{D} also induces an inclusion \Phi :{\mathrm  {NS}}(A)\otimes {\mathbb  {Q}}\to {\mathrm  {End}}(A)\otimes {\mathbb  {Q}} via \Phi _{E}=\phi _{D}^{{-1}}\circ \phi _{E}. The image of \Phi is equal to \{\psi \in {\mathrm  {End}}(A)\otimes {\mathbb  {Q}}:\psi '=\psi \}, i.e., the set of endomorphisms fixed by the Rosati involution. The operation E\star F={\frac  12}\Phi ^{{-1}}(\Phi _{E}\circ \Phi _{F}+\Phi _{F}\circ \Phi _{E}) then gives {\mathrm  {NS}}(A)\otimes {\mathbb  {Q}} the structure of a formally real Jordan algebra.


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