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Statement and Proof of the Main Theorem

Let $ K$ be as in Section 2, and let $ \pi:J\rightarrow A$ be an optimal quotient. Assume that $ J$ is equipped with a symmetric principal polarization $ \lambda$, that $ J$ has semistable reduction, and that $ A$ has purely toric reduction. Let $ X_A$, $ X_{A^{\vee}}$, and $ X_J$ denote the character groups of the toric parts of the closed fibers of the abelian varieties $ A$, $ A^{\vee}$, and $ J$, respectively.

Let $ \pi:J\rightarrow A$ be an optimal quotient, and let $ \theta:A^{\vee}\rightarrow A$ denote the induced polarization. Let $ \pi_*$, $ \pi^*$, $ \theta_*$, and $ \theta^*$ be the maps induced on character groups by the various functorialities, as indicated in the following two key diagrams:

$\displaystyle \xymatrix @=3pc{A^{\vee} \ar@{^(->}[r]^{\pi^{\vee}}\ar[dr]_{\thet...
...*}
& X_J \ar@{-»}[d]^{\pi_*} \\
& X_{A^{\vee}}.\ar@/^1.5pc/[ul]^{\theta_*}}
$

The surjectivity of $ \pi_*$ is proved in Theorem 8.2. The injectivity of $ \pi^*$ follows because

$\displaystyle \theta_*\pi_*\pi^*=\theta_*\theta^*=\deg(\theta)\neq 0,$

and multiplication by a nonzero integer on a free abelian group is injective.

Let $ \mathcal{L}$ be the saturation of $ \pi^* X_A$ in $ X_J$; thus $ \pi^* X_A$ is a finite-index subgroup of  $ \mathcal{L}$ and the quotient $ X_J/\mathcal{L}$ is torsion free. Let

$\displaystyle \alpha :X_J\rightarrow \Hom(\pi^* X_A,\mathbf{Z})$

be the map defined by the monodromy pairing restricted to $ X_J\times \pi^* X_A$. For $ L$ of finite index in $ \mathcal{L}$, define the degree of $ L$ to be

$\displaystyle m_L = [\alpha (X_J):\alpha (L)],$

and the component group of $ L$ to be

$\displaystyle \Phi_L = \coker( X_J \rightarrow \Hom(L,\mathbf{Z})).$

When $ L=\mathcal{L}$ and $ A$ is fixed, for simplicity we write $ m_X=m_\mathcal{L}$ and $ \Phi_X=\Phi_\mathcal{L}$.

Recall that $ \Phi_A$ is the component group of $ A$ and $ m_A$ is the square root of the degree of the induced map $ A^{\vee}\rightarrow A$.

Theorem 6.1   For any subgroup $ L$ of finite index in $ \mathcal{L}$, the following relation holds:

$\displaystyle \frac{\char93 \Phi_A}{m_A} = \frac{\char93 \Phi_L}{m_L}.$



Subsections
next up previous
Next: Proof of the Main Up: Component Groups of Purely Previous: The Degree of a
William A Stein 2001-12-09