There is a normalization omission in the printed conclusion: the discrepancy of a count of pairs must be bounded by a small function of the energy excess times . We prove this normalized result, then give a counterexample to the literal bound without . Write for the energy excess parameter to avoid confusing it with an element of the third set.
For Fourier analysis on a finite abelian group, use andCharacter orthogonality, for and zero otherwise, gives Fourier inversion and the Parseval identity on a finite group:Put , , . Expanding the constraint by the same character orthogonality gives the additive energy identityThus , and every nonconstant Fourier coefficient on a finite abelian group of has modulus at most . Expanding the constraint in the triple count givesThe Cauchy-Schwarz inequality yieldsThe first squared norm is by the Parseval identity on a finite group. For the second, multiplication by on has kernel size and every element of its image has exactly preimages. HenceThis proves that additive energy controls three-term progression mixing, including for even moduli:Thus the intended density-error function can be , which tends to zero. For odd moduli the factor can be replaced by one.
To see why the literal unnormalized conclusion is false, take and let all three sets be the subgroup of multiples of . Their densities are . Every choice of three entries of that subgroup determines the fourth entry of an additive quadruple, so its energy is . The excess parameter isEvery pair in the subgroup determines there, giving , whereas . Their difference is , which cannot be bounded by any function of tending to zero. The missing is therefore a genuine source defect, not an alternative Fourier transform normalization.
The positive-power length assertion is an asymptotic one: it requires sufficiently large in terms of the density. Read literally for every , it fails when , and , whose triple sumset is a singleton. We prove the intended result with this necessary qualification and an explicit positive exponent.
Embed the interval into the cyclic group with , and set , . Since all integer triple sums lie in , this embedding introduces no collisions between distinct sums. Use normalized Fourier coefficients on a finite abelian group and normalized convolution on a finite group, and putThe function is nonnegative and has mean , so some satisfies . We show that a whole translated Bohr set is contained in its positive support, hence in the triple sumset.
Put , , and define the large spectrumThe Parseval identity on a finite group gives , soAlso , and therefore . Using Fourier inversion and the convolution theorem on a finite group, for we obtainConsequently . This proves the translated Bohr neighborhood in a triple sumset:It remains to produce a long ordinary integer arithmetic progression in this translate; we supply the simultaneous approximation and the lifting argument. SetThus . Partition the -dimensional unit cube into boxes of side . The pointscontain two in the same box by the pigeonhole principle. Their index difference gives an integer with andIn particular . The identity on the unit circle now shows thatAll residues therefore lie in the triple sumset. Let be their actual integer representatives. Their successive differences are congruent to modulo , and each lies in , which is contained in . There is at most one integer in this interval in any specified residue class, so every difference is the same integer. It is nonzero because . Thus the form an ordinary integer arithmetic progression of distinct elements, even though is composite. Reversing it if necessary makes the common difference positive.
For sufficiently large , we have and , whenceAbsorb this fixed prefactor by decreasing the exponent: withthe last lower bound is at least once is sufficiently large in terms of . This proves a polynomial-length progression in by the polynomial-length progression in a dense triple sumset argument, without replacing the triple sumset by a fourfold difference set.
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