Schematic of the spatial pair-correlation method. The fluorescence intensity is rapidly sampled (compared with the motion of the particles) at several points in a grid (labeled 1, 2, 3, 4). As particles migrate, they appear at different points of the grid. Only the same particle will produce an average cross-correlation with a given time delay at two different points in the grid. For example, a fluctuation in intensity at position 1 will statistically correlate with a fluctuation of the intensity at position 2 if the same particle is moving (with some delay) to position 2. Fluctuations at position 3 in the grid (the other side of the barrier in blue) will never correlate with the fluctuations at position 1 or 2. If we map the amount of correlation between pairs of points (1,2 and 2,3), we see a discontinuity in the correlation between 2 and 3 but not between 1,2 and 3,4. If instead of an impenetrable barrier we have obstacles, as shown in the right panel, we could observe the same particle on the other side of the obstacle but with a delayed correlation. If we cross-correlate the intensity fluctuations at each point of the grid, we produce a map of molecular flow with a resolution given by the size of the PSF shown in light blue, which is ∼250 nm in the plane of the grid.