The Fourier density-increment proof of the Meshulam theorem controls three-term progressions through ordinary Fourier coefficients, equivalently the norm. Four-term progressions are controlled by the Gowers uniformity norm . A function can have small correlation with every linear character while correlating strongly with a quadratic phase; such a function can have small norm but large norm. Ordinary Fourier uniformity therefore does not make the four-term progression count pseudorandom, and a large linear Fourier coefficient need not exist when that count is deficient. Quadratic or higher-order Fourier structure is needed.
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