We study inelastic gases in two dimensions using event-driven molecular dynamics simulations. Our focus is the nature of the stationary state attained by rare injection of large amounts of energy to balance the dissipation due to collisions. We find that under such extreme driving, with the injection rate much smaller than the collision rate, the velocity distribution has a power-law high energy tail. The numerically measured exponent characterizing this tail is in excellent agreement with predictions of kinetic theory over a wide range of system parameters. We conclude that driving by rare but powerful energy injection leads to a well-mixed gas and constitutes an alternative mechanism for agitating granular matter. In this distinct nonequilibrium steady-state, energy cascades from large to small scales. Our simulations also show that when the injection rate is comparable with the collision rate, the velocity distribution has a stretched exponential tail. Granular materials are ubiquitous in nature, but nevertheless, fundamental understanding of the properties of granular materials presents many challenges [1][2][3][4][5]. Underlying these challenges are structural inhomogeneities, macroscopic particle size, and energy dissipation, all of which are defining features of granular matter.Equilibrium gases have Maxwellian velocity distributions. Due to the irreversible nature of the dissipative collisions, granular gases are out of equilibrium. Indeed, non-Maxwellian velocity distributions are observed in a wide range of experiments in driven granular matter including in particular shaken grains [6][7][8][9][10][11][12][13][14][15][16][17]. In such experiments, energy is injected over a wide range of scales and the measured velocity distribution has a stretched exponential form. To a large extent, a kinetic theory where energy injection through the system boundary is modeled by a thermostat successfully describes these nonequilibrium steady-states [18][19][20][21].Furthermore, theoretical studies suggest that the steady-state is controlled primarily by the ratio between the energy injection rate and the collision rate [22,23]. When the injection rate is much larger than the collision rate, the velocity distribution is Maxwellian. However, when the injection rate is smaller than the collision rate, the velocity distribution is non-Maxwellian, and has a stretched-exponential tail.In this study, we focus on the limiting case where the injection rate is vanishingly small and energy is injected at extremely large velocity scales [24,25]. Under such extreme driving, the injected energy cascades down from large velocity scales to small scales and thereby counters the dissipation by collisions. Kinetic theory shows that in the stationary state, the velocity distribution has * Electronic address: wfkang@gmail.com † Electronic address: machta@physics.umass.edu ‡ Electronic address: ebn@lanl.gov a power-law high energy tail. These theoretical predictions were supplemented by Monte-Carlo simulations of the homogeneous Boltzmann...