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A class of morphisms among toric varieties are described by certain lattice morphisms.
Let $N_1$ and $N_2$ be lattices and $\Sigma_1$, $\Sigma_2$ fans in $N_1$ and $N_2$
respectively. A $\mathbb{Z}$-linear map
$$\overline{\phi} \colon N_1 \to N_2$$
is said to be compatible with the fans $\Sigma_1$ and $\Sigma_2$ if for every cone
$\sigma_1 \in \Sigma_1$, there exists a cone $\sigma_2 \in \Sigma_2$ such that
$\overline{\phi}_{\mathbb{R}}(\sigma_1) \subseteq \sigma_2$.
By theorem 3.3.4 CLS11, such a map $\overline{\phi}$ induces a morphism
$\phi \colon X_{\Sigma_1} \to X_{\Sigma_2}$ of the toric varieties, and those
morphisms are exactly the toric morphisms.
To every toric variety $v$ we can associate a special toric variety, the
Cox variety. By definition, the Cox variety is such that the mapping matrix of
the toric morphism from the Cox variety to the variety $v$ is simply
given by the ray generators of the variety $v$. Put differently,
if there are exactly $N$ ray generators for the fan of $v$, then the
Cox variety of $v$ has a fan for which the ray generators are the standard basis
of $\mathbb{R}^N$ and the maximal cones are one to one to the maximal cones of
the fan of $v$.