We present experimental evidence supported by simulations of a relativistic ionization wave launched into surrounding gas by the sheath field of a plasma filament with high energy electrons. Such filament is created by irradiating a clustering gas jet with a short pulse laser (∼115 fs) at a peak intensity of 5 × 10 17 W/cm 2 . We observe an ionization wave propagating radially through the gas for about 2 ps at 0.2-0.5 c after the laser has passed, doubling the initial radius of the filament. The gas is ionized by the sheath field, while the longevity of the wave is explained by a moving field structure that traps the high energy electrons near the boundary, maintaining a strong sheath field despite the significant expansion of the plasma.A sheath electric field is a ubiquitous phenomenon caused by electron motion that occurs at the plasma edge. It is employed in applications ranging from plasma discharges [1, 2] to ion acceleration [3,4]. In this paper, we present experimental evidence supported by simulations of a collisionless self-sustaining relativistic ionization wave that is launched into a surrounding un-ionized gas by a plasma sheath field.Suitable experimental conditions are achieved by irradiating a supersonic clustering argon gas jet with a moderate intensity laser pulse (5 × 10 17 W/cm 2 ). Enhanced absorption of the laser energy by such jet makes it possible to create a plasma with high energy electrons [5]. The expansion of such plasmas have been used to study phenomena ranging from nonlocal heat transport [6] to formation of electrostatic shocks [7] and blast waves [8]. The corresponding time-scale is in the range of tens of ps, because these phenomena either involve ion motion or electron collisions. In what follows, we focus on much faster phenomenon. We present direct measurements of a relativistic velocity ionization wave, launched by the radial sheath field of a laser-generated plasma with high energy electrons, that is sustained for up to 2 ps. The measured radial velocity of the wave after the laser pulse is 0.2-0.5 c, causing the plasma radius to double on a ps time scale. Our relatively short laser pulse (115 fs) makes it possible to clearly distinguish energy deposition into the plasma from the propagation of the ionization wave that follows.The measured increase of the plasma radius is clearly too fast to be attributed to hydrodynamic motion, and it is even too fast to be explained by free-streaming electrons ionizing the surrounding gas via impact ionization. Indeed, the velocity of these electrons has to be comparable to the speed of the wave front, v e ≈ 0.5 c, which leads to a collisional time τ e 10 ps at 3 × 10 18 cm −3 gas densities [9]. This is much too long for the observed ionization. In this paper, we also present particle-in-cell (PIC) simulations that reveal a new collisionless mechanism that can launch and maintain the observed fast ionization front. We show that a hot electron minor- ity produced by the laser-cluster interaction generates a strong sheath electric field at...