Using an optical centrifuge to control molecular rotation in an extremely broad range of angular momenta, we study coherent rotational dynamics of nitrogen molecules in the presence of collisions. We cover the range of rotational quantum numbers between J = 8 and J = 66 at room temperature and study a cross-over between the adiabatic and non-adiabatic regimes of rotational relaxation, which cannot be easily accessed by thermal means. We demonstrate that the rate of rotational decoherence changes by more than an order of magnitude in this range of J values, and show that its dependence on J can be described by a simplified scaling law. 33.20.Sn, 33.20.Xx Rotational decoherence in dense gaseous media is an area of active research because of its importance in the fundamental understanding of the dissipative properties of gases, as well as in the practical aspects of thermochemistry and combustion research [1][2][3][4]. Laser control of molecular rotation has been successfully applied to numerous physical and chemical processes, in which long lived rotational coherence is essential (for a comprehensive review, see Ref.5).One of the most interesting aspects of the collisioninduced rotational decoherence is the question about its dependence on the speed of molecular rotation and temperature. From the very first experimental works on the topic [6,7], it was suggested that the rate of rotational relaxation should drop with increasing rotational quantum number J, i.e. that the faster molecular rotors are more robust with respect to collisions. This expectation stems from the intuitive "exponential-gap law" (EGL) according to which the decay rate decreases as exp[−∆E J /k B T ] with the increasing distance between the rotational levels ∆E J (here k B is the Boltzmann constant and T is the temperature of the gas). The refined version of EGL, known as the "energy corrected sudden" (ECS) approximation and introduced by DePristo et al. [8], is a popular model which successfully explained a large number of experimental observations [1,2,[9][10][11][12].The ECS theory describes the collisional decay rate in terms of an "adiabaticity parameter" a ≡ ω J τ c = ω J l c /v c , where ω J is the frequency of molecular rotation, τ c is the collision time, l c is a characteristic interaction length (usually determined empirically) and v c is the mean relative velocity between the collision partners. Since a = 2πτ c /T J (with T J being the rotation period), it may also be viewed as the angle, by which a molecule rotates during the collision process. When a π, the collision is sudden and the energy transfer does not depend on J. In the case of the finite duration of collisions, i.e. a π, the ECS model calls for scaling the decay rate with a J-and temperature-dependent correction factorwith '1/6' being specific to R −6 interaction potentials. In thermal ensembles, both the highest available ω J and the mean particle velocity v c scale equally with temperature. Hence, thermally accessible values of a do not increase with increasing T a...