We numerically investigate the dynamical properties of the one-component Gaussian core model in supercooled states. We find that nucleation is increasingly suppressed with increasing density. The system concomitantly exhibits glassy, slow dynamics characterized by the two-step stretched exponential relaxation of the density correlation and a drastic increase of the relaxation time. We also find a weaker violation of the Stokes-Einstein relation and a smaller non-Gaussian parameter than in typical model glass formers, implying weaker dynamic heterogeneities. Additionally, the agreement of the simulation data with the prediction of mode-coupling theory is exceptionally good, indicating that the nature of the slow dynamics of this ultra-soft particle fluid is mean-field-like. This fact may be understood as a consequence of the long-range nature of the interaction. The nature of the glass transition is surrounded by controversy. Several scenarios have been proposed to explain the drastic slowing down of dynamics of supercooled fluids near the glass transition point [1][2][3]. Numerical simulation of simple model fluids is an ideal tool to test these competing scenarios. However, the typical model fluids studied so far, such as Lennard-Jones, soft-core, and hard-sphere mixtures, have short-ranged, strong repulsive interactions in common, which dictate their thermodynamic, structural, and dynamical properties and render the results of these models qualitatively similar [4]. A new class of model glass formers is desirable to diversify our pictures and perspectives on the glass transition within the limited accessible time windows of the simulations. Recently, ultra-soft particle fluids have attracted particular attention in soft-materials science [5]. They are systems composed of spherical particles interacting with bounded and weak repulsions and are a good model for various soft materials, such as star-polymers and dendrimers. The absence of the hard-core-like repulsion makes the thermodynamic and dynamic behaviors of this class of systems extremely rich compared with standard molecular systems. Their phase diagrams exhibit exotic and counterintuitive properties, including a stable fluid phase at high temperatures for arbitrary densities, re-melting of solids at higher densities, and complex crystalline phases at low temperatures [5]. The dynamics of the ultra-soft particles fluids also exhibits rich and nontrivial behaviors [6][7][8][9].In this Letter, we consider the simplest version of ultrasoft particles, i.e., the Gaussian core model (GCM) fluid originally introduced by Stillinger [10]. The GCM interaction is given bywhere ǫ and σ characterize the energy and length scales, respectively. The GCM is an ideal model to study glassy dynamics because its thermodynamic phase diagram is relatively simple. Other ultra-soft particles, such as Hertzian spheres and star-polymers, exhibit complex crystalline phases, which may affect the dynamics in the supercooled state [6,11]. We numerically study the monodisperse GCM in th...