Taking a finite difference lowers the degree of a polynomial phase. For , expand by shifts and apply the Cauchy-Schwarz inequality to those shift sums. This gives , where enforces that lie in . Although individual terms can be complex, the entire sum is real and nonnegative because it equals a sum of squares. For , the phase is .
For a real degree- polynomial with leading coefficient , , and coprime integers satisfying , the displayed bound applies to its exponential sum over . Repeated Weyl differencing reduces the phase to slope . A geometric-sum estimate, the subpower bound for the divisor function and the reciprocal fractional-part sum near a rational complete the estimate. The arbitrary positive exponent absorbs divisor bounds and logarithms.
If and with , the displayed estimate holds. Twice applying Weyl differencing bounds by . Group by and use the subpower bound for the divisor function. The reciprocal fractional-part sum near a rational bounds the resulting sum by . Take fourth roots, absorbing logarithms into when ; for larger the trivial bound suffices. Leiden lecture notes, Section 7.2 develop this cubic differencing estimate.
For and every , the displayed estimate bounds a mean value of a polynomial exponential sum. For cubes its eighth-moment bound is . It complements pointwise Weyl differencing estimates: a ninth moment over a region is bounded by its supremum there times this eighth moment. Leiden lecture notes, Section 8.1 give the cubic formulation.
Write and . Character orthogonality gives . For , fix the difference . If , there are choices for the two equal pairs. If , any solution has ; fixing this divisor gives a quadratic equation for , hence at most two choices. The subpower bound for the divisor function yields .
The twice-differenced inequality in Weyl differencing reads , with counting triples for which and all four shifted arguments are in . Thus , and for : the product divides , and the remaining equation determines . The Fourier coefficients of are nonnegative counts, with and . Multiply the inequality by and integrate. It follows that , after choosing the divisor-bound exponents small enough.
Articles by others on the same topic
There are currently no matching articles.