The Freiman-Ruzsa theorem over a finite field states that if and , then is contained in a vector subspace with
After translating , assume . Put , and choose maximal subject to the translates , , being pairwise disjoint. Since , the Plünnecke-Ruzsa inequality gives
so .
Maximality gives : if is not already in , then for some , whence . Inductively, for every positive integer . Because , every element of belongs to some in the finite vector space, and therefore
Finally, and by the Plünnecke-Ruzsa inequality, so
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Let be a subspace with much larger than , and choose linearly independent vectors whose images are independent modulo . Set
Then , while is the union of , the disjoint cosets , and at most exceptional sums . Hence
Every subspace containing must contain and all , so it has at least elements. Thus the exponential dependence on in the Freiman-Ruzsa theorem over a finite field cannot in general be replaced by a subexponential one.
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The hypothesis says that the normalized additive energy of is at least . By the Balog-Szemerédi-Gowers theorem, for an absolute there is such that
The finite-field Bogolyubov-Ruzsa consequence of the Freiman-Ruzsa theorem over a finite field says that a set of doubling at most has a vector subspace
with for an absolute . Taking and enlarging the absolute exponent gives
This is an energy form of the Bogolyubov lemma: the usual lemma assumes positive density in an ambient group, whereas the Balog-Szemerédi-Gowers theorem first extracts a dense structured model from the many additive quadruples. The resulting bound depends on the energy parameter rather than on the possibly tiny ambient density of .
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For and , the Bohr set is
Writing , the lower bound for the size of a Bohr set is
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Use normalized convolution and Fourier coefficients, and define the large spectrum
By the Parseval identity and ,
so .
The convolution theorem gives
If , the part over is at most
because . On the complementary spectrum, and , so the contribution is less than . The required difference is therefore less than .
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Apply the preceding Fourier argument to , retaining the frequencies needed to make the oscillation of strictly smaller than its mean . The standard optimized cutoff gives a set with
such that the nonnegative function cannot fall from a maximal value to zero under any shift in . If maximizes , then
The support of a convolution of indicator functions is the corresponding sumset, so
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Write and identify each character with a residue . Partition the -dimensional torus into cubes of side , where is comparable to . Applying the pigeonhole principle to the points
gives a nonzero residue satisfying
Consequently whenever . After allowing for integer parts and the small values of , this produces the centered arithmetic progression
of length at least .
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Part c gives with . By the arithmetic progression in a cyclic Bohr set, contains a centered progression of length at least
Its translate by is the required arithmetic progression in .
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One standard normalized form of the Croot-Sisask almost-periodicity theorem is this. Let be finite subsets of an abelian group with , let , let , and let be a complex function. There is with
such that every satisfies
For the proof, sample independent points of and approximate by the empirical average of the corresponding translates of . A moment inequality bounds the expected error, so many samples are good. The small size of lets a translation and pigeonhole argument find many shifts in producing the same good approximation. Subtracting two such shifts and applying the triangle inequality yields the almost periods in .
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Apply the assumed finite-field character approximation with error . We obtain characters and a function
such that . Let
Each character has a kernel of codimension at most one, so . For , , and translation invariance of the norm gives
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Put . Then , , and the Parseval identity gives
Set . If , the asserted integer lower bound is trivial. Otherwise take and in part b. The resulting subspace has
Thus , and we may choose a -dimensional subspace .
For , part b gives
Apply the supplied maximal inequality to . Since , it gives
Hence some satisfies , so for every . Since , this proves
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For functions on , the Gowers inner product is
where is the complex conjugate operator. The Gowers uniformity norm is
The Gowers-Cauchy-Schwarz inequality states
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Repeated Cauchy-Schwarz inequality shows that the norm dominates the absolute mean of a function:
Taking and using gives
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For , the product in the cube average is
The expression in parentheses is the third additive derivative of the quadratic form , so it vanishes. Every cube contributes one and therefore the quadratic phase satisfies
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Apply the Cauchy-Schwarz inequality successively in the three shift variables to the correlation with the quadratic phase . At the third step the third additive derivative of its phase vanishes, leaving
Thus implies
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Expand the cube product for
Whenever all eight -vertices of the cube lie in , the Freiman homomorphism property makes every second additive derivative of vanish. Consequently the coefficients of and of each of the three -direction increments in the phase cancel, so the phase product around the cube is one. It follows that
Part b(i), applied to , now gives
Since , one can apply the inverse theorem for the Gowers U3 norm over a finite field: has nontrivial correlation, quantitatively in and , with a quadratic phase on .
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