EN
We investigate the behaviour of Fourier coefficients with respect to the system of ultraspherical polynomials. This leads us to the study of the "boundary" Lorentz space $ℒ_{λ}$ corresponding to the left endpoint of the mean convergence interval. The ultraspherical coefficients ${cₙ^{(λ)}(f)}$ of $ℒ_{λ}$-functions turn out to behave like the Fourier coefficients of functions in the real Hardy space ReH¹. Namely, we prove that for any $f ∈ ℒ_{λ}$ the series $∑_{n=1}^{∞} cₙ^{(λ)}(f) cos nθ $ is the Fourier series of some function φ ∈ ReH¹ with $||φ||_{ReH¹} ≤ c||f||_{ℒ_{λ}}$.