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Part (iii) gives at least ${\eta }^2|A{|}^3$ additive quadruples. By the Balog-Szemerédi-Gowers theorem, there is $A^{\prime }\subseteq A$ withThe Freiman-Ruzsa theorem places $A^{\prime }$ in a coset progression $P$ whose rank is bounded in terms of $\eta$ and which satisfiesThus $A^{\prime }$ has density at least $C_1(\eta {)}^{-1}$ inside $P$.

The Szemerédi theorem in a bounded-rank coset progression says that, for fixed rank and density, every sufficiently large such progression has a nontrivial four-term progression in every subset of that density. If $|A|\ge C(\eta )$ for a sufficiently large $C(\eta )$, then $|P|\ge |A^{\prime }|\ge c(\eta )|A|$ crosses this threshold. It gives a nontrivial four-term progression in $A^{\prime }$, which is also contained in $A$. This proves the claim with a constant depending only on $\eta$.

The hypothesis says that the normalized additive energy of $A$ is at least $\eta$. By the Balog-Szemerédi-Gowers theorem, for an absolute $C_0$ there is $A^{\prime }\subseteq A$ such thatThe finite-field Bogolyubov-Ruzsa consequence of the Freiman-Ruzsa theorem over a finite field says that a set of doubling at most $K$ has a vector subspacewith $|V|\ge p^{-K^{C_1}}|A^{\prime }|$ for an absolute $C_1$. Taking $K={\eta }^{-C_0}$ and enlarging the absolute exponent givesThis 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 $A$.