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. 2021 Oct 13;143(42):17395–17411. doi: 10.1021/jacs.1c05219

Figure 5.

Figure 5

T-Jump IR responses reflect sequence-dependent conformational heterogeneity. The final temperature for each measurement is AT-all, 320 K; GC-end, 319 K; GC-core, 327 K; and GC-mix, 326 K. (a) Mid-IR t-HDVE difference spectra for GC-core at time delays from 5 ns to 560 μs. Normalized time traces for each sequence are shown at (b) 1600 cm–1 and (c) 1660 cm–1. The signal at 1600 cm–1 corresponds to changes in A and T ring vibrations while the signal at 1660 cm–1 contains contributions from G and T carbonyl vibrations. Each time trace is fit to the sum of a stretched exponential with two exponentials (solid lines): S(t) = A exp(−(tfast)βfast) + B exp(−tslow) + C exp(−tcool). The stretched exponential describes the process from 5 ns to 1 μs, and the two exponentials describe the signal increase from 1 to 320 μs and signal decay from rehybridization induced by thermal relaxation back to the initial temperature. The stretch factor βfast for the fits at 1600 and 1660 cm–1 are reported directly on the plots in panels b and c.