Use normalized Fourier analysis on a finite abelian group, identifying with its indicator function on the cyclic group . The conventions are
The 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 gives
For the translation of a function , putting yields
The two transforms are therefore
The 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 give
For completeness, the character orthogonality used here is
which 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 bound
In 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 most
Adding the estimates proves
The 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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