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. 2020 Jan 22;11(8):2112–2120. doi: 10.1039/c9sc05717j

Fig. 4. 2D-IR spectra of c-P6·T6+˙ (a) and l-P2+˙ (b) at 400 fs delay, with pump (FWHM ∼80 cm−1) centered at 2080 cm−1. Black solid and blue dashed contour lines correspond to positive (ESA) and negative (GSB) signals, respectively. Vertical dashed lines correspond to different experimental spectra, where probe a was changed to cover region 1300 cm−1 to 1900 cm−1 and probe b was centered in the 1900–2150 cm−1 region for each experiment (see Fig. S14–S23 for time resolution of each probe window). Probe windows in 1300–1900 cm−1 were stitched together by normalizing all probe a spectra to probe. b (c) fit of on-diagonal slice for l-P2+˙ (red line in (b)) using the sum of two Voigt. (d) The peak–peak distance for each time delay, calculated from the fit in (c).

Fig. 4