We report here on time-resolved x-ray diffraction measurements following femtosecond laser excitation in pure bulk chromium. Comparing the evolution of incommensurate charge-density-wave (CDW) and atomic lattice reflections, we show that, few nanoseconds after laser excitation, the CDW undergoes different structural changes than the atomic lattice. We give evidence for a transient CDW shear strain that breaks the lattice point symmetry. This strain is characteristic of sliding CDWs, as observed in other incommensurate CDW systems, suggesting the laser-induced CDW sliding capability in 3D systems. This first evidence opens perspectives for unconventional laser-assisted transport of correlated charges.Understanding the interplay between spin, charge and lattice is a major issue in condensed matter. Chromium is a typical system having complex electronic and magnetic ground states despite a basic crystallographic structure [1]. Below 311 K, a spin-density-wave appears with twice the period of a charge-density-wave (CDW)/strain wave modulation. In bulk chromium, the ratio of the atomic lattice and CDW periods is incommensurate. In principle, this implies that energetically equivalent states are found whatever the position of the CDW with respect to the atomic lattice. However, this translational invariance, inducing transport of correlated charges in low-dimensional systems, has never been observed in 3D systems like chromium [2].Systems submitted to an external driving force in disordered media share universal behaviours. For various systems, such as surfaces, vortices in type-II superconductors [3], or magnetic domain walls [4], similar regimes are sequentially observed -pinning, creep and flow -depending on the pinning strength compared to the applied force magnitude. The case of periodic systems, like CDWs, is peculiar. They are generally found in low dimensional materials, characterized by strong structural anisotropy, when a periodic lattice distortion allows a major decrease of the electron energy thanks to a gap opening, resulting in a static modulation of the electron density [5]. CDWs are pinned to the lattice either because of local impurity potentials or commensurability effects between the lattice and the CDW periodicities. Depinning thus requires the CDW and lattice periods to be incommensurate, i.e. to have an irrational ratio. When it takes place, the collective transport of charges is detectable through the non-ohmic behaviour of the current-voltage characteristics, as well as an additional ac voltage. This effect has been observed in several quasione dimensional systems like in NbSe3 [6] and in blue bronze [7]. More recently, quasi-2D CDW systems were also found to have this ability [8,9] but CDW sliding has never been observed in 3D materials so far.The presence of a CDW in an isotropic 3D metal like chromium is exceptional. In the bulk, this metal indeed displays incommensurate DWs although its structure is cubic and monoatomic, with hardly any anisotropy of its properties [1]. It was the first m...