For the first time, the diffusion phase diagram in highly confined colloidal systems, predicted by Continuous Time Random Walk (CTRW), is experimentally obtained. Temporal and spatial fractional exponents, α and µ, introduced within the framework of CTRW, are simultaneously measured by Pulse Field Gradient Nuclear Magnetic Resonance technique in samples of microbeads dispersed in water. We find that α depends on the disorder degree of the system. Conversely, µ depends on both bead sizes and magnetic susceptibility differences within samples. Our findings fully match the CTRW predictions.PACS numbers: 82.56. Lz, 87.64.kj, 61.05.Qr, Anomalous diffusion (AD), that predicts the meansquare displacement (MSD) of a diffusing particle to grow nonlinearly in time, [x(t) − x(0)] 2 ∝ t ν (with ν = 1), is a property of many complex systems and its related phenomena have been observed in various physical fields [5,8,14,16,17]. As shown by Metzler and coworkers [10], the features of AD can be described using fractional calculus. According to these Authors, molecular AD in media can be described by defining the motion propagator (MP) as the solution of fractional diffusion equations, which arise from the continuous time random walk (CTRW) model. These equations involve two fractional exponents, α and µ, which are, the orders of the time and space fractional derivatives, respectively [15]. The theoretical framework of CTRW is well established and has been corroborated by huge amounts of Monte Carlo simulations (see for example [20]) together with several experimental evidences, mainly obtained by using fluorescent spectroscopy [13,19]. However, to our knowledge, an experimental α vs µ phase diagram, showing the competition between superdiffusion and subdiffusion of diffusing molecules in heterogeneous media, has never been carried out. In this Letter, we experimentally challenge the Metzler et al. prediction of the CTRW theory [10] by measuring the fractional exponents α and µ by means of Nuclear Magnetic Resonance (NMR) methods, based on Pulse Field Gradient (PFG) technique [18], and by providing their interplay for the first time.In the last few decades, NMR water diffusion measurements have been a topic of extensive research, having broad applications in biophysics [2] and medicine [7]. Translational self-diffusion in liquid systems can be measured using PFG techniques, by applying magnetic gradient pulses (named diffusion gradients) to the system, in addition to the static magnetic field of the instrument itself. The signal attenuation, that depends on both dif- * Corresponding author: silvia.capuani@roma1.infn.it fusion gradient strength and diffusion time, is simply the Fourier Transform (FT) of the MP. When MP is Gaussian, NMR signal attenuation follows a mono-exponential Stejskal-Tanner decay [18]. Conversely, when the motion is described by a non-Gaussian propagator, the signal attenuation deviates from a mono-exponential decay [9,12]. In the present study, we have measured the fractional exponent α collecting the PFG ...