Understanding glasses and the glass transition is widely accepted as a deep, mysterious, and fundamental problem. However, the consensus does not extend much further. The topic is still hotly debated and progress toward a commonly accepted resolution seems slow for what is, after all, one of the oldest puzzles in physics. New theoretical tools and predictions do emerge, new phenomena are unveiled, and clever experiments are nonetheless carried out. In this vein, the two recent experimental papers in PNAS by Vivek et al. (1) and Illing et al. (2) convincingly address an issue at the junction of two fundamental questions in glass physics: the role of the dimensionality of space on the glass transition and the possible existence of long-wavelength fluctuations in 2D amorphous solids.Is the nature of the glass transition different in two and three dimensions? Contrary to many ordering transitions, such as crystallization, which are known to be different in 2D and in 3D, there has been for some time a loose form of consensus that the glass transition is similar in 2D and 3D. As summarized in a pithy sentence by P. Harrowell, "in Flatland, glasses reproduce all the behaviour of their three-dimensional relatives" (3). The rationale behind this is that the glass transition involves no obvious long-range order or spontaneous symmetry breaking. Actually, the experimentally observed glass transition is not even a true phase transition. It is a kinetic crossover, admittedly quite sharp, through which a liquid that, upon cooling, has become too viscous to flow and relax in a reasonable observation time (by anthropic standards) falls out of equilibrium. It then forms a glass, an "amorphous" solid the structure of which looks as disordered as that of the liquid before the crossover (4).However, a clear blow to this assumed similarity came from a recent comparative study of 2D and 3D model glass-forming liquids by computer simulation. Flenner and Szamel (5) showed that the dynamics of 2D glassformers is qualitatively different from that of their 3D counterparts. As illustrated in Fig. 1, the translational motion of the particles proceeds differently in 2D and 3D. Particles stay trapped for relatively long times in the "cage" formed by their neighbors in 3D, which gives rise to a plateau in the self-intermediate correlation function (Fig. 1, Upper). On the other hand, they can move sizable distances along with their neighbors with little change of their local structure in 2D (Fig. 1, Lower), which generates a strong dependence on the system size. Quite strikingly, in 2D but not in 3D, as one cools the system, the translational motion and the associated time-dependent correlation functions appear to decouple from the motion of the particles involving a rearrangement of the local environment. The latter can be detected through Fig. 1. Self-correlation function of the density modes F s (k,t) versus time (log scale) in a 3D (Upper) and a 2D (Lower) glass-former for several temperatures T (from left to right T decreases). (Inset) Tra...