Landsberg–Schaar relation

In number theory and harmonic analysis, the Landsberg–Schaar relation (or identity) is the following equation, which is valid for arbitrary positive integers p and q:

${\frac {1}{\sqrt {p}}}\sum _{n=0}^{p-1}\exp \left({\frac {2\pi in^{2}q}{p}}\right)={\frac {e^{{\frac {1}{4}}\pi i}}{\sqrt {2q}}}\sum _{n=0}^{2q-1}\exp \left(-{\frac {\pi in^{2}p}{2q}}\right).$

The standard way to prove it is to put τ = ⁠2iq/p⁠ + ε, where ε > 0 in this identity due to Jacobi (which is essentially just a special case of the Poisson summation formula in classical harmonic analysis):

$\sum _{n=-\infty }^{+\infty }e^{-\pi n^{2}\tau }={\frac {1}{\sqrt {\tau }}}\sum _{n=-\infty }^{+\infty }e^{-\pi {\frac {n^{2}}{\tau }}}$

and then let ε → 0.

If we let q = 1, the identity reduces to a formula for the quadratic Gauss sum modulo p.

The Landsberg–Schaar identity can be rephrased more symmetrically as

${\frac {1}{\sqrt {p}}}\sum _{n=0}^{p-1}\exp \left({\frac {\pi in^{2}q}{p}}\right)={\frac {e^{{\frac {1}{4}}\pi i}}{\sqrt {q}}}\sum _{n=0}^{q-1}\exp \left(-{\frac {\pi in^{2}p}{q}}\right)$

provided that we add the hypothesis that pq is an even number.