Superconducting cosmic strings naturally emit highly boosted charge carriers from cusps. This occurs when a cosmic string or a loop moves through a magnetic field and develops an electric current. The charge carriers and the products of their decay, including protons, photons and neutrinos, are emitted as narrow jets with opening angle θ ∼ 1/γ c , where γ c is the Lorentz factor of the cusp. The excitation of electric currents in strings occurs mostly in clusters of galaxies, which are characterized by magnetic fields B ∼ 10 −6 G and a filling factor f B ∼ 10 −3 .Two string parameters determine the emission of the particles: the symmetry breaking scale η, which for successful applications should be of order 10 9 -10 12 GeV, and the dimensionless parameter i c , which determines the maximum induced current as J max = i c eη and the energy of emitted charge carriers as ǫ X ∼ i c γ c η, where e is the electric charge of a particle. For the parameters η and B mentioned above, the Lorentz factor reaches γ c ∼ 10 12 and the maximum particle energy can be as high as γ c η ∼ 10 22 GeV. The diffuse fluxes of UHE neutrinos are close to the cascade upper limit, and can be detected by future neutrino observatories. The signatures of this model are: very high energies of neutrinos, in excess of 10 20 eV, correlation of neutrinos with clusters of galaxies, simultaneous appearance of several neutrino-produced showers in the field of view of very large detectors, such as JEM-EUSO, and 10 TeV gamma radiation from the Virgo cluster. The flux of UHE protons from cusps may account for a large fraction of the observed events at the highest energies.