when
Thus
is periodic, with period 1, in
each element of
. More generally,
with
,
. This is the
quasi-periodicity property of the Riemann theta function. It determines
the Riemann theta function up to a constant factor. The set of points
form a
-dimensional lattice,
the period lattice of the Riemann theta function.
Again, with
,
Because of this property, the elements of
and
are usually restricted to
, without loss of generality.
For Riemann theta functions with half-period characteristics,
See also §20.2(iii) for the case
and classical theta
functions.