We present exact results on the dynamics of a biased, by an external force F, intruder (BI) in a two-dimensional lattice gas of unbiased, randomly moving hard-core particles. Going beyond the usual analysis of the force-velocity relation, we study the probability distribution P (Rn) of the BI displacement Rn at time n. We show that despite the fact that the BI drives the gas to a non-equilibrium steady-state, P (Rn) converges to a Gaussian distribution as n → ∞. We find that the variance σ 2 x of P (Rn) along F exhibits a weakly superdiffusive growth σ 2 x ∼ ν1 n ln(n), and a usual diffusive growth, σ 2 y ∼ ν2 n, in the perpendicular direction. We determine ν1 and ν2 exactly for arbitrary bias, in the lowest order in the density of vacancies, and show that ν1 ∼ |F| 2 for small bias, which signifies that superdiffusive behaviour emerges beyond the linear-response approximation. Monte Carlo simulations confirm our analytical results, and reveal a striking fieldinduced superdiffusive behavior σ 2 x ∼ n 3/2 for infinitely long 2D stripes and 3D capillaries. A biased intruder (BI) traveling through a quiescent medium, composed of bath particles which move randomly without any preferential direction, drives the medium to a non-equilibrium steady-state with an inhomogeneous particles' spatial distribution: the latter jam in front of and are depleted behind the BI. The BI can be a charge carrier biased by an electric field or a colloid moved with an optical tweezer. The bath particles may be colloids in a solvent or adatoms on a solid surface.Such microstructural changes of the medium (MCM) were experimentally observed, e.g., in microrheological studies of the drag force on a colloid driven through a λ-DNA solution [1] or for a BI in a monolayer of vibrated grains [2]. Brownian Dynamics simulations have revealed the MCM for a driven colloid in a λ-DNA solution [1,3], or for BIs in colloidal crystals [4]. Remarkably, the MCM not only enhance the drag force exerted on the BI, but also induce effective interactions between the BIs, when more than one BI is present [5][6][7][8].The MCM produced by a BI were studied analytically for quiescent baths modeled as hard-core lattice gases with symmetric simple exclusion dynamics [9][10][11][12][13][14][15]. Despite some simplifications (interactions are a mere hardcore, no momentum transfer and etc), this type of modeling captures quite well many qualitative features and reproduces a cooperative, essentially many-particle behavior present in realistic physical systems [16,17]. It is also often amenable to analytical analysis.It was found that in 1D the size of the inhomogeneity grows in proportion to the traveled distance, so that the jamming-induced contribution to the frictional drag force exhibits an unbounded growth with time n. In consequence, the BI velocity v n ∝ n −1/2 [9-11], ensuring the validity of the Einstein relation for anomalous tracer diffusion in 1D hard-core lattice gases [10][11][12]18]. In higher dimensions, the BI velocity approaches a terminal value v and th...