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By pretending that the imaginery parts E m of the Riemann zeros are eigenvalues of a quantum Hamiltonian whose corresponding classical trajectories are chaotic and without time-reversal symmetry, it is possible to obtain by asymptotic arguments a formula for the mean square difference V(L;x) between the actual and average number of zeros near the xth zero in an interval where the expected number is L. This predicts that when L<<L max =ln(E/2 pi )/2 pi ln 2 (where x=(E/2 pi )(ln(E/2 pi )-1)+ 7 / 8 ), V is the variance of the Gaussian unitary ensemble (GUE) of random matrices, while when L>>L max , V will have quasirandom oscillations about the mean value pi -2 (lnln(E/2 pi )+1.4009). Comparisons with V(L;x) computed by Odlyzko (1987) from 10 5 zeros E m near x=10 12 confirm all details of the semiclassical predictions to within the limits of graphical precision.
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Michael Berry (1988) studied this question.
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