Spatial modulation (tagging) of the longitudinal magnetization allows diffusive displacements to be measured over times approximately as long as T 1 and over correspondingly long distances. Magnetization tagging is used here with hyperpolarized 3 He gas in canine lungs with unilateral elastase-induced emphysema. A new scheme for analyzing images subsequent to tagging determines the spatially-resolved fractional modulation and its decay rate, using a sliding window. The free diffusivity D o of 3 He, dilute in air or N 2 , is exceptionally large at 0.88 cm 2 /s. Thus, the root mean square (RMS) free displacement of a typical 3 He atom during several milliseconds is larger than the diameter of the acinar airways, with the result that the apparent diffusivity measured over such times is restricted by collisions with airway walls and is near 0.2 cm 2 /s in healthy lung (1-4). Airway expansion and destruction of airway and alveolar walls in emphysema (5) result in reduced restriction of diffusion (D Ϸ 0.55 cm 2 /s in a group of severely diseased subjects) (3). Nearly all of the work to date has measured D msec , taken from the decay of transverse magnetization measured at two b-values (that is, with and without a pulsed, diffusion-sensitizing field gradient) (3,4,6 -8). The experiment is sensitive to displacements during the gradient waveform that is typically several milliseconds in duration, corresponding to displacements of a few hundred microns. This time is limited by the short T* 2 of 3 He in lung (about 20 ms in 1.5 T) (9,10). The small length scale associated with this method limits the motion to individual acinar airways where 95% of the gas resides; the time is not sufficient for many of the atoms to move from one airway to the next. Multi-b-value measurements of the decay of transverse magnetization over times of milliseconds have been understood in terms of anisotropic diffusion, with different values longitudinal and transverse to the airways (D L and D T ) (1). Diffusion values so measured are sensitive indicators of the changes in localized lung morphology that accompany emphysema.However, by probing gas diffusion over longer times, one can examine the structure of the airway network over longer length scales. In the canonical description of lung (11), there are 24 levels of branching airways, where the trachea is Z ϭ 0 and the alveolar sacs are Z ϭ 23. The acinar units are the primary regions of gas exchange and comprise the highest-numbered eight airway levels. The mean linear size of an acinar unit is about 7 mm, with individual acinar airways having lengths of approximately 1 mm (11). Because the average acinar-airway length is small, and the acini contain the vast majority of gas in the lung, diffusion between arbitrary points that are centimeter(s) apart requires that atoms must travel from one acinus to another, connecting via a common conducting airway node. From the alveolar sacs, for example, this is a path through eight or more airway levels. The diffusion coefficient measured over such long ...