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. 2013 Nov 5;105(9):2182–2187. doi: 10.1016/j.bpj.2013.09.029

Figure 3.

Figure 3

(a and b) Comparison of normalized intensity at the boson peak energy, as a function of Q for hGFP and dGFP at 295 K for the dry and hydrated states, respectively. The spectra are overlaid (dashed lines) for ∝Q2, illustrating the expected spectra for random phase or out-of-phase collective motions. (Dotted line in panel a) Expected Q-dependence for a fully in-phase coherent motion, ∝S(Q)Q2. (c) Schematic of the fitting procedure used to decompose the random and coherent phase motions, shown here for the boson peak region of dry deuterated GFP at 295 K. To see this figure in color, go online.