Theorems
If H is a finite-dimensional space, then every basis of H is a Riesz basis.
Let φ be in the Lp space L2(R), let
and let denote the Fourier transform of φ. Define constants c and C with . Then the following are equivalent:
The first of the above conditions is the definition for (φn) to form a Riesz basis for the space it spans.
Read more about this topic: Riesz Sequence