We theoretically investigate an opportunity to implement a source of highly spin-polarized ac current on the basis of superconductor/weak ferromagnet/superconductor (SFS) voltage-biased junction in the regime of essential proximity effect and calculate the current flowing through the probe electrode tunnel coupled to the ferromagnetic interlayer region. It is shown that while the polarization of the dc current component is generally small in case of weak exchange field of the ferromagnet, there is an ac component of the current in the system. This ac current is highly spin-polarized and entirely originated from the non-equilibrium proximity effect in the interlayer. The frequency of the current is controlled by the voltage applied to SFS junction. We discuss a possibility to obtain a source of coherent ac currents with a certain phase shift between them by tunnel coupling two probe electrodes at different locations of the interlayer region. PACS numbers: 74.50.+r, 74.45.+c Various proximity and transport phenomena in hybrid structures containing superconducting and ferromagnetic elements are currently in the spotlight. The equilibrium transport and proximity effect in such structures have been theoretically and experimentally investigated recently in details as for the case of weak ferromagnetic alloys (see Ref. 1 and references therein) so as for halfmetals like CrO 2 2,3 .Spin-dependent properties of nonequilibrium systems are also actively investigated. In particular, the spin imbalance induced in a ferromagnet (F) in nonequilibrium conditions was studied in ferromagnet-superconductorferromagnet (FSF) junctions 4,5,6,7,8,9 . It was found that antiferromagnetic alignment of the exchange fields of the ferromagnets strongly suppresses superconductivity, which leads to large magnetoresistive effect. The influence of the interplay between Andreev reflection at the interface and spin accumulation close to the interface was investigated 10 . The effect of spin injection in Josephson junctions was considered 11 . The papers 9,12 have theoretically studied the spin relaxation due to spin-flip scattering.The authors of 13,14 propose the possibility of manipulating magnetization of a mesoscopic normal (N) region through the Zeeman splitting of superconducting density of states and applied voltage in voltage biased SNS or FSNSF tunnel junctions. Also, the spin-polarized transport through superconductor-normal metal hybrid structures, where the density of states in a superconductor is Zeeman-splitted, was investigated 13,14,15 . It was shown that, in alternative to half-metallic ferromagnets, such junction can be used to generate highly spin-polarized currents, which are tunable in magnitude and sign by the bias voltage and exchange field. In 13,14 the normal metal region between the superconducting leads has been considered to be long enough in order to suppress the proximity effect and, consequently, ac Josephson effect in it. However, if the junction length is of the order of superconducting coherence length ξ = D/∆,...