The lattice invariants are defined by
23.3.1 | ||||
23.3.2 | ||||
The lattice roots satisfy the cubic equation
23.3.3 | |||
and are denoted by . The discriminant (§1.11(ii)) is given by
23.3.4 | |||
In consequence,
23.3.5 | |||
23.3.6 | |||
23.3.7 | |||
Let , or equivalently be nonzero, or be distinct. Given and there is a unique lattice such that (23.3.1) and (23.3.2) are satisfied. We may therefore define
23.3.8 | |||
Similarly for and . As functions of and , and are meromorphic and is entire.
Conversely, , , and the set are determined uniquely by the lattice independently of the choice of generators. However, given any pair of generators , of , and with defined by (23.2.1), we can identify the individually, via
23.3.9 | |||
. | |||
In what follows, it will be assumed that (23.3.9) always applies.