With normalized averages on the finite abelian group , the Gowers U2 norm is defined byThe Gowers U3 norm is defined bywhere denotes complex conjugation.
WriteApply the Cauchy-Schwarz inequality first in the variable carrying and then in the variable carrying . After the invertible linear changes of variables permitted by , apply the assumed three-function estimate to the resulting multiplicative derivatives. The standard calculation givesBy the Derivative identity for the Gowers U3 norm, the last two factors are and . Taking eighth roots proves
If has density , write . Expanding , the constant term is , and the displayed inequality bounds every nonconstant term after translation of one factor by a norm of the balanced function . Thus sufficiently small makes the normalized number of four-term arithmetic progressions close to .
Put . By the Derivative identity for the Gowers U3 norm, the Fourier formula for the norm, and Parseval identity,because . Letand for every choose attaining . Thenfor every , and deleting the complement of from the preceding average leaves total mass at least .
Let . The box-norm inequality applied to the selected Fourier coefficients and the cocycle identity for multiplicative derivatives givesThe left side is at least . An additive quadruple in is exactly a tuple satisfyingTherefore there are at least such quadruples, which is the Frequency graph extracted from a large Gowers U3 norm.
Let have density at least and put . If has too few four-term progressions, part ii forces to be large. Part iii then produces a frequency graph with large additive energy. The Balog-Szemerédi-Gowers theorem extracts a large piece with small doubling, and a finite-field Freiman theorem makes the frequency selection approximately affine-linear there. Integrating these approximately linear derivative frequencies produces correlation of with a quadratic phase, as in the inverse theorem for the Gowers U3 norm over a finite field.
Restricting to a suitable level set of that quadratic phase produces a density increment on a structured affine subspace. Iterating these increments cannot continue indefinitely because density is at most one. Once is sufficiently large in terms of , the iteration must instead terminate with the expected nontrivial four-term progression. This is the density-increment proof of the finite-field four-term progression theorem.
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