%0 journal article
%@ 1098-0121
%A Grigoriev, S.V.,Dyadkin, V.A.,Menzel, D.,Schoenes, J.,Chetverikov, Y.O.,Okorokov, A.I.,Eckerlebe, H.

%D 2007
%J Physical Review  B
%N 22
%P 224424 
%R doi:10.1103/PhysRevB.76.224424
%T Magnetic structure of Fe1−xCoxSi in a magnetic field studied via small-angle polarized neutron diffraction
%U https://doi.org/10.1103/PhysRevB.76.224424
22 
%X The magnetic structure of Fe1−xCoxSi single crystals with x=0.10,0.15,0.20,0.50 has been studied by small angle polarized neutron diffraction and superconducting quantum interference device measurements. Experiments have shown that in zero field the compounds with x=0.1,0.15 have a well-defined tendency to order in the one-handed spiral along <100> axes due to the anisotropic exchange, that, however, decreases with increasing Co concentration x. The magnetic structure of Fe1−xCoxSi with x=0.2,0.5 consists of spiral domains with randomly oriented spiral wave vector k. The applied magnetic field produces a single domain helix oriented along the field. The process of the reorientation starts at the field HC1. Further increase of the field leads to a magnetic phase transition from a conical to a ferromagnetic state near HC2. In the critical range near TC the integral intensity of the Bragg reflection shows a well-pronounced minimum at Hfl attributed to a k flop of the helix wave vector. On the basis of our experiments we built the H-T phase diagram for each compound. It is shown that the same set of the parameters governs the magnetic properties of these compounds k, HC1, Hfl, and HC2. Our experimental findings are well interpreted in the framework of a recently developed theory [Phys. Rev. B 73, 174402 (2006)] for cubic magnets with Dzyaloshinskii-Moriya (DM) interaction. In particular, the theory suggests an additional quantum term in the magnetic susceptibility caused by the DM interaction which is in good agreement with the experiment.