An analytical dependence of the cross section for the small-angle scattering of polarized neutrons at spin waves in helimagnets formed because of Dzyaloshinskii—Moriya interaction in cubic crystals without an inversion center (the space group is P2₁3) is obtained. It is assumed that the dispersion of spin waves in helimagnets with the wave vector k_s polarized by a magnetic field is larger than the critical field H_C2 of the transition to the ferromagnetic phase and has the form E_q = A(q − k_s ) + gμ_B(H − H_С2). It is shown that the cross section for neutron scattering at the two-dimensional map of angles (θ_x, θ_y) is two circles of the radii θ_C with the centers ±θ_S, corresponding to the Bragg angle of diffraction by a helix oriented along the applied magnetic field H. The radii of these two circles θ_C are directly related to the stiffness of spin waves A of the magnetic system and depends on the applied magnetic field: θC2=θ02−gμBHEnθ0, where θ0=h22Amn and E_n and m_n are the neutron energy and mass. It is shown that the scattering cross section depends on the neutron polarization, which is evidence of the chiral character of spin waves in the Dzyaloshinskii—Moriya helimagnets even in the completely polarized phase. The cases of neutron scattering at magnons where θ₀ ≤ θ_S and θ_S ≥ θ₀ are considered. The case of neutron scattering at spin waves in helimagnets is compared with analogous scattering at ferromagnets where θ_S → 0.