“…[3][4][5][6][7][8][9][10] While it is widely accepted that the dynamics can be represented by a broad distribution of relaxation times or other nonexponential decay function, such as the Kolrausch-Williams-Watts ͑KWW͒ 11,12 stretched exponential, it is less clear whether this dispersion exhibits a uniform relaxation mechanism ͑homogeneous͒, or the net broadened relaxation is heterogeneous due to the response of slow and fast subensembles with independent mechanisms, which might be spatially distributed in the material. 3,[13][14][15] There has been a range of techniques used to test the heterogeneity of the relaxational dynamics, such as multidimensional nuclear magnetic resonance, 16 optical deep bleaching, 17 nonresonant spectral hole burning ͑NSHB͒ conducted in dielectric and magnetic fields, 5,14,15,[18][19][20][21][22] and recently, mechanical spectral hole burning ͑MSHB͒. 10 The fundamental assumption behind these spectral hole-burning techniques is that the spectrum of relaxation times can be locally altered rather than uniformly shifted by a strong impulse of given frequency.…”