We predict the existence of chiral spin waves-collective modes in a two-dimensional Fermi liquid with the Rashba or Dresselhaus spin-orbit coupling. Starting from the phenomenological Landau theory, we show that the long-wavelength dynamics of magnetization is governed by the KleinGordon equations. The standing-wave solutions of these equations describe "particles" with effective masses, whose magnitudes and signs depend on the strength of the electron-electron interaction. The spectrum of the spin-chiral modes for arbitrary wavelengths is determined from the Dyson equation for the interaction vertex. We propose to observe spin-chiral modes via microwave absorption of standing waves confined by an in-plane profile of the spin-orbit splitting.Introduction.-The rapidly developing field of spintronics aims to manipulate electron spins by electric rather than magnetic fields. Since spin-orbit (SO) interaction allows for such a coupling, electron systems with SO interaction have been under intense study. A particularly interesting issue is the role of the electronelectron interaction in such systems [1,2]. SO-coupled Fermi liquids (FLs) are expected to exhibit a rich variety of effects, which arise only from a combination of the electron-electron and SO interactions, such as spinsplit and Rashba phases [3,4], unusual Friedel oscillations [5,6], and spin textures [7], to name just a few. The focus of this Letter is on the collective excitations in a SO-coupled FL.