Use normalized Fourier analysis on a finite abelian group, identifying with its indicator function on the cyclic group . The conventions areThe last operation is normalized convolution on a finite group. With these conventions the Fourier coefficients on a finite abelian group use a normalized average, while sums over frequencies use counting measure.
Expanding the normalized convolution on a finite group and putting givesFor the translation of a function , putting yieldsThe two transforms are thereforeThe negative sign in the translation factor follows from the negative sign in our Fourier coefficient on a finite abelian group convention.
Since is an indicator function of density of a finite subset , the triangle inequality gives for every frequency. Also, character orthogonality and the Parseval identity on a finite group giveFor completeness, the character orthogonality used here iswhich follows by summing a finite geometric series. Expanding the squared Fourier coefficients on a finite abelian group and using this identity proves the displayed Parseval identity on a finite group directly.
Combining the uniform bound with that identity gives the fourth-moment boundIn particular, the Lp norm on the frequency side here is a sum, not a normalized average. This is the fourth Fourier moment bound for an indicator function.
For the physical-space L2 norm use . By part (i) and the Parseval identity on a finite group,Split this sum into the large spectrum and its complement. Because belongs to the Bohr set in the question, for ,Consequently the contribution from is at most by part (ii). Outside , , and . Thus that contribution is at mostAdding the estimates provesThe argument also covers empty or empty . As usual the radius and threshold are nonnegative; a negative radius makes the premise empty whenever is nonempty. The estimate expresses Bohr-set almost periodicity of a convolution: a translation of a function by an element of the Bohr set barely changes the large Fourier coefficients on a finite abelian group, while the small ones have little total energy.
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