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For functions bounded by one on a cyclic group of prime order greater than three, three applications of Cauchy-Schwarz bound the four-term arithmetic progression average by the smallest Gowers U3 norm of its factors. Zero extension yields the corresponding interval bound with an absolute factor. This makes Gowers U3 norm a measure of uniformity relevant to four-term arithmetic progression counts.

Normalize the conjugated cube average by the number of integer cubes whose vertices all lie in the interval. Equivalently, extend $f$ by zero to a cyclic group of order greater than $8N$ and divide its Gowers U3 norm by that of the interval's indicator function. A quadratic phase then has norm one. Omitting the denominator gives a different but uniformly equivalent interval normalization.

The proof of Szemerédi theorem for four-term progressions follows a uniformity-versus-density-increment iteration. Fix a positive starting density; the quantitative parameters below depend only on that density.

First apply the counting argument in part (i). A sufficiently long set with no nonconstant four-term arithmetic progression cannot have small balanced Gowers U3 norm. Thus its balanced function has a quantitatively large cube average. The Derivative identity for the Gowers U3 norm expresses this as an average of fourth Fourier moments of the multiplicative derivatives $x\mapsto f(x+h)\overline{f(x)}$. Many shifts therefore have a derivative with a large Fourier coefficient.

The next step is the inverse argument. Choose these frequencies as a function of the shifts. The relations between repeated derivatives force a large part of the resulting frequency graph to have many additive quadruples. A Balog-Szemerédi-Gowers theorem extraction followed by Freiman theorem for integer sets organizes this graph on a bounded-complexity additive model. Integrating the organized derivative frequencies yields correlation of $f$ with a locally quadratic phase on a structured region. On integer intervals this is generally a local quadratic phase on a Bohr-type region, or equivalent two-step structure; it need not be one global quadratic polynomial on the entire interval.

The quantitative density-increment lemma obtained from that inverse argument says that either the interval is bounded in size by a function of its density, or there is a nonempty integer progression of length at least $c(\delta )N^{c(\delta )}$ on which the density increases by at least $c(\delta )>0$. The passage from correlation to this increment partitions the structured region into progressions on which the phase varies very little, controls discarded boundaries, and uses the balanced function's zero mean to find a positive-density gain. Both the gain and the size exponent are bounded away from zero for densities above the fixed starting density.

Reidentify the new progression with an interval and repeat. The property of having no nonconstant four-term progression is preserved under this affine identification. Density can increase only finitely many times before it exceeds one. Starting with $N$ sufficiently large ensures that the successive power-type length losses never reach the exceptional bounded-size case during those finitely many steps. This contradiction proves that every fixed positive density has a threshold beyond which a four-term progression must occur. The counting lemma, inverse structural argument, density increment and final iteration are the main steps; the deep inverse step is only outlined here, as permitted by this part of the question.

The expectations use normalized counting measure on a finite abelian group $G$. This is the finite-group convention implicit in the averaging notation; an arbitrary infinite group has no normalized counting probability measure on all its points. For $h\in G$, define ${\Delta }_{h}f(x)=f(x)\overline{f(x+h)}$, and let $\mathcal{C}$ denote complex conjugation. The Gowers U3 norm isAveraging first over $h_3$ gives the Derivative identity for the Gowers U3 normIndeed, if $u(x)={\Delta }_{h_1}{\Delta }_{h_2}f(x)$, the average over $(x,h_3)$ is ${\mathbb{E}}_{x,h_3}u(x)\overline{u(x+h_3)}=|{\mathbb{E}}_{x}u(x){|}^2$. The eighth root is consequently well-defined. Homogeneity follows because the cube has four unconjugated and four conjugated factors, so $\Vert af{\Vert }_{U^3}=|a|\Vert f{\Vert }_{U^3}$. If the norm is zero, every squared term in the finite average vanishes. Taking $h_1=h_2=0$ gives ${\mathbb{E}}_x|f(x){|}^4=0$, so $f=0$ pointwise. This proves positive definiteness.

For the triangle inequality, we prove the needed Gowers-Cauchy-Schwarz inequality. For eight functions $F_{\omega }$ on a product of finite sets $X_1\times X_2\times X_3$, form the box norm multilinear averageFix a coordinate $j$. After averaging its two variables separately, this is $\mathbb{E}A\overline{B}$, where $A$ uses all vertices with ${\omega }_j=0$ and $B$ those with ${\omega }_j=1$, with the remaining parity conjugations. The Cauchy-Schwarz inequality giveswhere $S_j^b$ replaces the function at each vertex by the original function with its $j$th index set to $b$. Each right-hand average is a squared absolute value averaged over the other coordinates, hence nonnegative. Apply this operation successively for $j=1,2,3$, to every resulting factor. The eight final families each use one original $F_{\omega }$ at all vertices. Taking roots gives the box Cauchy-Schwarz inequalityNow take $X_j=G$ and $F_{\omega }(a,b,c)=f_{\omega }(a+b+c)$. With $x=a_0+b_0+c_0$ and $h_j=x_j^1-x_j^0$, these independent variables induce uniform $(x,h_1,h_2,h_3)$: each such tuple has exactly $|G{|}^2$ preimages. Therefore each box norm is the corresponding $U^3$ norm, and the mixed cube obeysExpand the eight factors in the cube expression for $f+g$. Its $2^8$ mixed terms are bounded by this inequality, and their bounds sum to $(\Vert f{\Vert }_{U^3}+\Vert g{\Vert }_{U^3}{)}^8$. Thus $\boxed{\Vert f+g{\Vert }_{U^3}\le \Vert f{\Vert }_{U^3}+\Vert g{\Vert }_{U^3}}$, completing the norm proof.

Two consequences will be useful below. Multiplication by a character of a finite abelian group leaves the norm unchanged, because the alternating character product around a three-dimensional cube equals one. Alsowhere the last inequality uses the $h=0$ term and $\Vert u{\Vert }_{U^2}^4={\sum }_{\chi }|\hat{u}(\chi ){|}^4\ge |\mathbb{E}u{|}^4$. Hence $\Vert f{\Vert }_{U^3}\ge |G{|}^{-1/8}\Vert f{\Vert }_2$.

The Gowers U3 norm derivative identity isLet $\kappa =\Vert F{\Vert }_{U^3(G)}^8$. Since $\Vert I{\Vert }_{U^3(G)}\ge \mathbb{E}I=N/M\ge 1/16$, by repeated Cauchy-Schwarz, the interval hypothesis gives $\kappa \ge 16^{-8}{\delta }^8$. Also $\Vert {\partial }_{h}F{\Vert }_{U^2}^4\le 1$. Therefore the sethas density at least $\kappa /2$ in $G$.

Use normalized Fourier coefficients on a finite abelian group $\hat{g}(k)={\mathbb{E}}_{x}g(x)e(-kx/M)$. The Gowers U2 norm and Parseval identity giveFor $g={\partial }_{h}F$, the final mean is at most one. Thus each $h\in H$ has a frequency $\theta (h)=k_h/M$ withThe derivative is identically zero unless $h$ is represented by an integer in $[-N+1,N-1]$, so $H$ lies in the requested interval of shifts. Its size is $\gg {\delta }^{8}M\gg {\delta }^{8}N$. Keep one such frequency for each shift; these same choices will satisfy the energy conclusion below.

We use the normalized Gowers U3 norm on an interval, for which a quadratic phase has norm one. Let ${\mathcal{C}}_N$ consist of integer tuples $(x,h_1,h_2,h_3)$ whose eight vertices $x+{\omega }_1{h}_1+{\omega }_2{h}_2+{\omega }_3{h}_3$, $\omega \in \{0,1{\}}^3$, all lie in $[1,N]$. If $\mathcal{C}$ denotes complex conjugation, defineEquivalently, choose a prime $8N<M<16N$, extend $f$ by zero to $G=\mathbb{Z}/M\mathbb{Z}$, call that extension $F$, and put $I=1_{[1,N]}$. ThenThe large ambient modulus prevents wraparound in cubes supported on the interval, so the ratio is independent of the chosen such $M$. This also proves nonnegativity and the norm properties by the Gowers uniformity norm on $G$. Some conventions omit the denominator; their interval norm differs by a fixed bounded factor, and the quadratic-phase norm is then $\Vert I{\Vert }_{U^3(G)}$.

For $f_0(x)=e(\alpha x^2)$, the exponent in every conjugated cube product is a third additive difference of a quadratic polynomial and is zero. Thus $\Vert f_0{\Vert }_{U^3(N)}=1$ in the normalized interval convention.

The generalized von Neumann inequality for four-term progressions connects this norm to counting arithmetic progressions. For functions bounded by one on a cyclic group of prime order greater than three,Three applications of Cauchy-Schwarz prove the bound. Zero extension and division by the number of interval progressions give the analogous interval estimate up to an absolute constant. In particular, if $g=1_A-\alpha 1_{[1,N]}$, where $\alpha =|A|/N$, has small Gowers U3 norm on an interval, expansion of the progression count shows that it differs from ${\alpha }^4$ times the count for $[1,N]$ by $O(\Vert g{\Vert }_{U^3(N)}{N}^2)$. A large Gowers U3 norm detects structure capable of changing four-term progression counts; quadratic phases are the basic example.

For the remaining proof use the ambient $G$ just specified, define ${\partial }_{h}F(x)=F(x+h)\overline{F(x)}$, and take averages uniformly on $G$. For frequencies not on the character grid, an exponential is evaluated at the chosen integer representatives; the general proof below selects actual characters $\theta =k/M$. The printed question does not define $G$ or the interval normalization, so these conventions make the assertion precise. If instead ${\partial }_{h}f(x)=f(x)\overline{f(x+h)}$ is used, conjugate the correlations and reverse every frequency sign; the quadratic example then has $\theta (h)=-2\alpha h$.

With normalized averages on the finite abelian group $G$, the Gowers U2 norm is defined byThe Gowers U3 norm is defined bywhere $\mathcal{C}$ denotes complex conjugation.

A subset $A$ of a finite abelian group $G$ with subset density $\eta =|A|/|G|$ is quadratically $\alpha$-uniform, in the norm convention, if its balanced subset indicator $g=1_A-\eta$ has Gowers U3 norm at most $\alpha$. This controls correlations on additive three-dimensional cubes after the subset density contribution is removed. If a convention instead bounds the eighth power of the norm by $\alpha$, its parameter corresponds to the norm parameter ${\alpha }^{1/8}$. The convention must therefore be stated when giving quantitative thresholds.

For $A\subseteq {\mathbb{Z}}_N$, $N\ge 16$, put $\eta =|A|/N$, $M=\lfloor N/16\rfloor$, $J=\{0,\dots ,M-1\}$, and $w=1_J\ast 1_J$ using normalized convolution on a finite group. The weights $w(x)w(d-M)$ are supported where $0\le x\le 2M-2$ and $M\le d\le 3M-2$, so $x,x+d,x+2d,x+3d$ are distinct integer points below $N$. If $t=M/N$, then $\mathbb{E}w=t^2$ and the sum of absolute values of its Fourier coefficients is $t$, by Parseval identity on a finite group. Expanding the four indicators around their subset density leaves four terms with one balanced factor. Expand both weights in Fourier series and absorb each character $e(rx+sd)$ into the factors at $x$ and $x+d$. Character multiplication preserves the Gowers U3 norm, and the cyclic four-term progression bound with torsion factors bounds every error by $6^{1/8}\alpha$. Thus the weighted count is at least ${\eta }^4{t}^4-4\cdot 6^{1/8}\alpha t^2$. Since $t\ge 1/32$, positivity follows from $\alpha <{\eta }^4/(4096\cdot 6^{1/8})$.

A bound tending to zero with one factor's Gowers U3 norm, uniformly over all finite abelian groups, is false. On $G={\mathbb{F}}_2^m$, choose a random independent sign at each point. A cube with eight distinct vertices has sign product of expectation zero. The probability of a collision among its vertices is at most $\left(\genfrac{}{}{0ex}{}{8}{2}\right)/|G|$, since each equality of distinct vertices imposes a nonzero linear equation in the increments. Thus some sign function $f$ has $\Vert f{\Vert }_{U^3}^8\le 28/|G|$. But the four-term arithmetic progression is $(x,x+d,x,x+d)$, so choosing factors $(f,1,f,1)$ gives correlation identically one. As $m\to \infty$, the norm tends to zero. Bounded torsion, as in cyclic groups, avoids this obstruction.