The Montgomery--Taylor computation #
A(Q_0) = C_MT: the pair-correlation functional at the self-convolution of the extremal test
function is the Montgomery--Taylor constant. It is proved here rather than assumed.
The three preceding files supply the pieces: the functional is the integral of f_0 against G
(Reduction), G is constant (AffineKernel), and that constant is C_MT (Evaluation). With
f_0 of total mass one, the integral collapses to the constant.
The Montgomery--Taylor computation (lem_montgomery_taylor). See Montgomery,
Distribution of the zeros of the Riemann zeta function, Proc. ICM (Vancouver, 1974), Vol. 1,
379--381.