Solution
= Solution
If an elliptic <function> has no poles, it is entire. It is bounded on the closure of a fundamental parallelogram, and periodicity transfers that bound to the whole plane. Liouville's theorem therefore makes it constant.
= Solution
If an elliptic <function> has no poles, it is entire. It is bounded on the closure of a fundamental parallelogram, and periodicity transfers that bound to the whole plane. Liouville's theorem therefore makes it constant.