  Hadrons in lattice QCD are usually created employing smeared interpolators.
We introduce a new quark smearing that allows us to maintain small statistical
errors and good overlaps of hadronic wavefunctions with the respective ground
states, also at high spatial momenta. The method is successfully tested for the
pion and the nucleon at a pion mass $m_{\pi}\approx 295$ MeV and momenta as
high as 2.8 GeV. We compare the results obtained to dispersion relations and
suggest further optimizations.
